diff --git a/adv_lab.bib b/adv_lab.bib index 7bb499b..d46b03d 100644 --- a/adv_lab.bib +++ b/adv_lab.bib @@ -1,3 +1,64 @@ +@ARTICLE{2017arXiv170306889H, + author = {{Harrison}, C.~M.}, + title = "{Impact of supermassive black hole growth on star formation}", + journal = {ArXiv e-prints}, +archivePrefix = "arXiv", + eprint = {1703.06889}, + keywords = {Astrophysics - Astrophysics of Galaxies, Astrophysics - Cosmology and Nongalactic Astrophysics}, + year = 2017, + month = mar, + adsurl = {http://adsabs.harvard.edu/abs/2017arXiv170306889H}, + adsnote = {Provided by the SAO/NASA Astrophysics Data System} +} + +@ARTICLE{2006ApJS..163....1H, + author = {{Hopkins}, P.~F. and {Hernquist}, L. and {Cox}, T.~J. and {Di Matteo}, T. and + {Robertson}, B. and {Springel}, V.}, + title = "{A Unified, Merger-driven Model of the Origin of Starbursts, Quasars, the Cosmic X-Ray Background, Supermassive Black Holes, and Galaxy Spheroids}", + journal = {\apjs}, + eprint = {astro-ph/0506398}, + keywords = {Cosmology: Theory, Galaxies: Active, Galaxies: Evolution, Galaxies: Nuclei, Galaxies: Quasars: General}, + year = 2006, + month = mar, + volume = 163, + pages = {1-49}, + doi = {10.1086/499298}, + adsurl = {http://adsabs.harvard.edu/abs/2006ApJS..163....1H}, + adsnote = {Provided by the SAO/NASA Astrophysics Data System} +} + +@conference{springelfeedback, + author = {Volker Springel}, + month = 5, + year = 2006, + title = {Simulations of Quasar Feedback}, + organization = {The history of nuclear black holes in galaxies}, + publisher = {Harvard-CfA}, +} + + + +@unpublished{koristafeedback, + title = {Quasars and the Birth \& Evolution of Galaxies}, + year = 2016, + author = {Kirk Korista}, + month = 3, + organization = {Western Michigan University}, + note = {Conference presentation} +} + + +@book{maoz2007astrophysics, + title={Astrophysics in a Nutshell}, + author={Maoz, D.}, + isbn={9780691125848}, + lccn={2006050588}, + series={In a Nutshell}, + url={https://books.google.com/books?id=r88PAQAAMAAJ}, + year={2007}, + publisher={Princeton University Press} +} + @ARTICLE{2017ApJ...837..149G, author = {{Gaspari}, M. and {S{\c a}dowski}, A.}, diff --git a/feedback/papers/0506398.pdf b/feedback/papers/0506398.pdf new file mode 100644 index 0000000..5d8a6c6 Binary files /dev/null and b/feedback/papers/0506398.pdf differ diff --git a/feedback/papers/0506398/0506398.tar b/feedback/papers/0506398/0506398.tar new file mode 100644 index 0000000..b24c72e Binary files /dev/null and b/feedback/papers/0506398/0506398.tar differ diff --git a/feedback/papers/0506398/f1.ps b/feedback/papers/0506398/f1.ps new file mode 100644 index 0000000..76cd6dc --- /dev/null +++ b/feedback/papers/0506398/f1.ps @@ -0,0 +1,1878 @@ +%!PS-Adobe-3.0 EPSF-3.0 +%%BoundingBox: 0 0 644 424 +%%Pages: 0 +%%Creator: Sun Microsystems, Inc. +%%Title: none +%%CreationDate: none +%%LanguageLevel: 2 +%%EndComments +%%BeginProlog +%%BeginResource: SDRes +/b4_inc_state save def 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+1 1 s +0 14971 t +pom +count op_count sub {pop} repeat countdictstack dict_count sub {end} repeat b4_inc_state restore +%%PageTrailer +%%Trailer +%%EOF diff --git a/feedback/papers/0506398/f10.ps b/feedback/papers/0506398/f10.ps new file mode 100644 index 0000000..63da13a --- /dev/null +++ b/feedback/papers/0506398/f10.ps @@ -0,0 +1,1466 @@ +%!PS-Adobe-3.0 +%%BoundingBox: 54 360 558 720 +%%Title: Graphics produced by IDL +%%For: phopkins@net-93286, +%% /Users/phopkins/Documents/lars_galaxies/plots/lf_xr +%%Creator: IDL Student Edition 6.0, Mac OS X (darwin ppc m32) +%%CreationDate: Mon Apr 11 10:15:00 2005 +%%DocumentData: Clean7bit +%%Requirements: color +%%LanguageLevel: 1 +%%PageOrder: Ascend +%%Pages: (atend) +%%DocumentNeededResources: (atend) +%%EndComments +%%BeginProlog +save +%+ prolog.ps -- Prolog for IDL generated PostScript files +%+ Copyright (c) 1988-2003 Research Systems, Inc. All Rights Reserved. +%v 4 +/$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C +{currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint +stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} +bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show +grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 +setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 +{[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 +100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 +{[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef +/ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} +ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont +exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica +findfont exch scalefont setfont (\267) show currentpoint grestore moveto} +bdef end 2.5 setmiterlimit +%%EndProlog +%%Page: 0 1 +%%PageRequirements: color +%%PageResources: (atend) +%%PageOrientation: Portrait +%%PageBoundingBox: 54 360 558 720 +%%BeginPageSetup +save +$IDL_DICT begin 54 360 translate 0.0283465 dup scale +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +%%EndPageSetup +15 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 1794 7061 M 7545 0 R D +3221 7061 M 0 99 R D gsave 3221 6528 translate 0 0 M 1.01 dup scale +-58.8433 0 N +( ) show grestore 5260 7061 M 0 99 R D gsave 5260 6528 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 7299 7061 M 0 99 R D gsave 7299 6528 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 9339 7061 M 0 99 R D gsave 9339 6528 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 1794 7061 M 0 49 R D 1998 7061 M 0 49 R D 2202 7061 M +0 49 R D 2406 7061 M 0 49 R D 2609 7061 M 0 49 R D 2813 7061 M 0 49 R D +3017 7061 M 0 49 R D 3425 7061 M 0 49 R D 3629 7061 M 0 49 R D 3833 7061 M +0 49 R D 4037 7061 M 0 49 R D 4241 7061 M 0 49 R D 4445 7061 M 0 49 R D +4649 7061 M 0 49 R D 4853 7061 M 0 49 R D 5056 7061 M 0 49 R D 5464 7061 M +0 49 R D 5668 7061 M 0 49 R D 5872 7061 M 0 49 R D 6076 7061 M 0 49 R D +6280 7061 M 0 49 R D 6484 7061 M 0 49 R D 6688 7061 M 0 49 R D 6892 7061 M +0 49 R D 7096 7061 M 0 49 R D 7503 7061 M 0 49 R D 7707 7061 M 0 49 R D +7911 7061 M 0 49 R D 8115 7061 M 0 49 R D 8319 7061 M 0 49 R D 8523 7061 M +0 49 R D 8727 7061 M 0 49 R D 8931 7061 M 0 49 R D 9135 7061 M 0 49 R D +1794 11989 M 7545 0 R D 3221 11989 M 0 -99 R D 5260 11989 M 0 -99 R D +7299 11989 M 0 -99 R D 9339 11989 M 0 -99 R D 1794 11989 M 0 -49 R D +1998 11989 M 0 -49 R D 2202 11989 M 0 -49 R D 2406 11989 M 0 -49 R D +2609 11989 M 0 -49 R D 2813 11989 M 0 -49 R D 3017 11989 M 0 -49 R D +3425 11989 M 0 -49 R D 3629 11989 M 0 -49 R D 3833 11989 M 0 -49 R D +4037 11989 M 0 -49 R D 4241 11989 M 0 -49 R D 4445 11989 M 0 -49 R D +4649 11989 M 0 -49 R D 4853 11989 M 0 -49 R D 5056 11989 M 0 -49 R D +5464 11989 M 0 -49 R D 5668 11989 M 0 -49 R D 5872 11989 M 0 -49 R D +6076 11989 M 0 -49 R D 6280 11989 M 0 -49 R D 6484 11989 M 0 -49 R D +6688 11989 M 0 -49 R D 6892 11989 M 0 -49 R D 7096 11989 M 0 -49 R D +7503 11989 M 0 -49 R D 7707 11989 M 0 -49 R D 7911 11989 M 0 -49 R D +8115 11989 M 0 -49 R D 8319 11989 M 0 -49 R D 8523 11989 M 0 -49 R D +8727 11989 M 0 -49 R D 8931 11989 M 0 -49 R D 9135 11989 M 0 -49 R D +1794 7061 M 0 4928 R D 1794 7061 M 151 0 R D gsave 1682 7061 translate 0 0 M +1.01 dup scale -376.343 0 N +(-9) show grestore 1794 7991 M 151 0 R D gsave 1682 7849 translate 0 0 M +1.01 dup scale -376.343 0 N +(-8) show grestore 1794 8921 M 151 0 R D gsave 1682 8778 translate 0 0 M +1.01 dup scale -376.343 0 N +(-7) show grestore 1794 9850 M 151 0 R D gsave 1682 9708 translate 0 0 M +1.01 dup scale -376.343 0 N +(-6) show grestore 1794 10780 M 151 0 R D gsave 1682 10638 translate 0 0 M +1.01 dup scale -376.343 0 N +(-5) show grestore 1794 11710 M 151 0 R D gsave 1682 11568 translate 0 0 M +1.01 dup scale -376.343 0 N +(-4) show grestore 1794 7154 M 75 0 R D 1794 7247 M 75 0 R D 1794 7340 M +75 0 R D 1794 7433 M 75 0 R D 1794 7526 M 75 0 R D 1794 7619 M 75 0 R D +1794 7712 M 75 0 R D 1794 7805 M 75 0 R D 1794 7898 M 75 0 R D 1794 8084 M +75 0 R D 1794 8177 M 75 0 R D 1794 8270 M 75 0 R D 1794 8363 M 75 0 R D +1794 8456 M 75 0 R D 1794 8549 M 75 0 R D 1794 8642 M 75 0 R D 1794 8735 M +75 0 R D 1794 8828 M 75 0 R D 1794 9014 M 75 0 R D 1794 9107 M 75 0 R D +1794 9200 M 75 0 R D 1794 9293 M 75 0 R D 1794 9386 M 75 0 R D 1794 9479 M +75 0 R D 1794 9572 M 75 0 R D 1794 9665 M 75 0 R D 1794 9758 M 75 0 R D +1794 9943 M 75 0 R D 1794 10036 M 75 0 R D 1794 10129 M 75 0 R D +1794 10222 M 75 0 R D 1794 10315 M 75 0 R D 1794 10408 M 75 0 R D +1794 10501 M 75 0 R D 1794 10594 M 75 0 R D 1794 10687 M 75 0 R D +1794 10873 M 75 0 R D 1794 10966 M 75 0 R D 1794 11059 M 75 0 R D +1794 11152 M 75 0 R D 1794 11245 M 75 0 R D 1794 11338 M 75 0 R D +1794 11431 M 75 0 R D 1794 11524 M 75 0 R D 1794 11617 M 75 0 R D +1794 11803 M 75 0 R D 1794 11896 M 75 0 R D 1794 11989 M 75 0 R D +9339 7061 M 0 4928 R D 9339 7061 M -151 0 R D 9339 7991 M -151 0 R D +9339 8921 M -151 0 R D 9339 9850 M -151 0 R D 9339 10780 M -151 0 R D +9339 11710 M -151 0 R D 9339 7154 M -76 0 R D 9339 7247 M -76 0 R D +9339 7340 M -76 0 R D 9339 7433 M -76 0 R D 9339 7526 M -76 0 R D +9339 7619 M -76 0 R D 9339 7712 M -76 0 R D 9339 7805 M -76 0 R D +9339 7898 M -76 0 R D 9339 8084 M -76 0 R D 9339 8177 M -76 0 R D +9339 8270 M -76 0 R D 9339 8363 M -76 0 R D 9339 8456 M -76 0 R D +9339 8549 M -76 0 R D 9339 8642 M -76 0 R D 9339 8735 M -76 0 R D +9339 8828 M -76 0 R D 9339 9014 M -76 0 R D 9339 9107 M -76 0 R D +9339 9200 M -76 0 R D 9339 9293 M -76 0 R D 9339 9386 M -76 0 R D +9339 9479 M -76 0 R D 9339 9572 M -76 0 R D 9339 9665 M -76 0 R D +9339 9758 M -76 0 R D 9339 9943 M -76 0 R D 9339 10036 M -76 0 R D +9339 10129 M -76 0 R D 9339 10222 M -76 0 R D 9339 10315 M -76 0 R D +9339 10408 M -76 0 R D 9339 10501 M -76 0 R D 9339 10594 M -76 0 R D +9339 10687 M -76 0 R D 9339 10873 M -76 0 R D 9339 10966 M -76 0 R D +9339 11059 M -76 0 R D 9339 11152 M -76 0 R D 9339 11245 M -76 0 R D +9339 11338 M -76 0 R D 9339 11431 M -76 0 R D 9339 11524 M -76 0 R D +9339 11617 M -76 0 R D 9339 11803 M -76 0 R D 9339 11896 M -76 0 R D +9339 11989 M -76 0 R D gsave 2202 7526 translate 0 0 M 1.25 dup scale +(z = 0.3) show grestore 40 setlinewidth 3221 11495 M 167 -167 R -167 -166 R +-166 166 R 166 167 R D 4241 11076 M 166 -166 R -166 -167 R -167 167 R +167 166 R D 5260 10545 M 167 -167 R -167 -166 R -166 166 R 166 167 R D +6280 9891 M 166 -167 R -166 -166 R -167 166 R 167 167 R D 7299 9165 M +167 -167 R -167 -166 R -166 166 R 166 167 R D 8319 8414 M 166 -166 R +-166 -167 R -167 167 R 167 166 R D 1796 11840 M 10 0 R 0 -8 R 10 0 R 11 0 R +0 -8 R 10 0 R 10 0 R 0 -7 R 10 0 R 10 0 R 0 -8 R 11 0 R 10 0 R 0 -8 R 10 0 R +10 0 R 0 -7 R 10 0 R 10 0 R 0 -8 R 11 0 R 10 0 R 0 -7 R 10 0 R 10 0 R 0 -8 R +10 0 R 11 0 R 0 -8 R 10 0 R 10 0 R 0 -7 R 10 0 R 10 0 R 0 -8 R 11 0 R 10 0 R +0 -7 R 10 0 R 10 0 R 0 -8 R 10 0 R 11 0 R 0 -7 R 10 0 R 10 0 R 0 -8 R 10 0 R +10 0 R 0 -7 R 11 0 R 10 0 R 0 -8 R 10 0 R 10 0 R 0 -7 R 10 0 R 11 0 R 0 -8 R +10 0 R 10 0 R 0 -7 R 10 0 R 10 0 R 0 -7 R 11 0 R 10 0 R 0 -8 R 10 0 R 10 0 R +0 -7 R 10 0 R 11 0 R 0 -7 R 10 0 R 10 0 R 0 -8 R 10 0 R 10 0 R 0 -7 R 11 0 R +10 0 R 0 -8 R 10 0 R 10 0 R 0 -7 R 10 0 R 10 0 R 0 -7 R 11 0 R 10 0 R 0 -7 R +10 0 R 10 0 R 0 -8 R 10 0 R 11 0 R 0 -7 R 10 0 R 10 0 R 0 -7 R 10 0 R 10 0 R +0 -7 R 11 0 R 10 0 R 0 -8 R 10 0 R 10 0 R 0 -7 R 10 0 R 11 0 R 0 -7 R 10 0 R +10 0 R 0 -7 R 10 0 R 10 0 R 0 -7 R 11 0 R 10 0 R 0 -8 R 10 0 R 10 0 R 0 -7 R +10 0 R 11 0 R 0 -7 R 10 0 R 10 0 R 0 -7 R 10 0 R 10 0 R 0 -7 R 11 0 R 10 0 R +0 -7 R 10 0 R 10 0 R 0 -7 R 10 0 R 11 0 R 0 -7 R 10 0 R 10 0 R 0 -7 R 10 0 R +10 0 R 0 -7 R 11 0 R 10 0 R 0 -7 R 10 0 R 10 0 R 0 -7 R 10 0 R 10 0 R 0 -7 R +11 0 R 10 0 R 0 -7 R 10 0 R 10 0 R 0 -7 R 10 0 R 11 0 R 0 -7 R 10 0 R 10 0 R +0 -7 R 10 0 R 10 0 R 0 -7 R 11 0 R 10 0 R 0 -7 R 10 0 R 10 0 R 0 -7 R 10 0 R +11 0 R 0 -9 R 10 0 R 10 0 R 0 -7 R 10 0 R 10 0 R 0 -7 R 11 0 R 10 0 R 0 -7 R +10 0 R 10 0 R 0 -7 R 10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R 0 -7 R 10 0 R 10 0 R +0 -7 R 11 0 R 10 0 R 0 -7 R 10 0 R 10 0 R 0 -6 R 10 0 R 11 0 R 0 -17 R +10 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -7 R 10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R +0 -7 R 10 0 R 10 0 R 0 -7 R 11 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -7 R 10 0 R +11 0 R 0 -6 R 10 0 R 10 0 R 0 -7 R 10 0 R 10 0 R 0 -21 R 11 0 R 10 0 R +0 -6 R 10 0 R 10 0 R 0 -6 R 10 0 R 11 0 R 0 -7 R 10 0 R 10 0 R 0 -6 R 10 0 R +10 0 R 0 -6 R 11 0 R 10 0 R 0 -7 R 10 0 R 10 0 R 0 -6 R 10 0 R 11 0 R 0 -6 R +10 0 R 10 0 R 0 -7 R 10 0 R 10 0 R 0 -26 R 11 0 R 10 0 R 0 -6 R 10 0 R +10 0 R 0 -6 R 10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -6 R +10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R +0 -6 R 10 0 R 10 0 R 0 -32 R 10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R 0 -6 R +10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R +0 -6 R 10 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -39 R 10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -6 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 10 0 R 11 0 R 0 -5 R 10 0 R +10 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R +0 -45 R 10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R +10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -54 R +10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R +0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -63 R 10 0 R 10 0 R +0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R +10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -71 R 10 0 R 10 0 R 0 -4 R 10 0 R +11 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R +10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R +0 -4 R 11 0 R 10 0 R 0 -80 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -4 R +11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R +0 -3 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R +11 0 R 0 -88 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R +0 -4 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -3 R 10 0 R +10 0 R 0 -4 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R +0 -95 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -3 R +10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R +0 -4 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -103 R +11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R +0 -3 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -3 R 10 0 R +11 0 R 0 -3 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -108 R 11 0 R 10 0 R +0 -3 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R +10 0 R 0 -3 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R +11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -114 R 10 0 R 11 0 R 0 -2 R 10 0 R +10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R +10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R +0 -3 R 10 0 R 10 0 R 0 -117 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R +10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R +0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -3 R 10 0 R +10 0 R 0 -120 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R +0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R +10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R +0 -123 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R +10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R +0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R D 6894 9342 M 10 0 R +0 -124 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R +10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R +0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -125 R +10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R +0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R +10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -127 R 10 0 R 10 0 R +0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R +11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R +10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -127 R 10 0 R 10 0 R 0 -3 R 10 0 R +10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R +10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R +0 -3 R 10 0 R 11 0 R 0 -127 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R +11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R +0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R +10 0 R 0 -128 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R +0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R +10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R +0 -129 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R +10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R +0 -2 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -129 R +10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R +0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R +10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -129 R 10 0 R 11 0 R +0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R +10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R +11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -129 R 10 0 R 10 0 R 0 -3 R 11 0 R +10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R +10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R +0 -2 R 10 0 R 10 0 R 0 -129 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R +10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R +0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R +10 0 R 0 -130 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R +0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R +11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 8 0 R D +20 setlinewidth L3 3957 10425 M 11 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R +10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -38 R 10 0 R 11 0 R +0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R +10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -45 R 10 0 R 10 0 R 0 -5 R 11 0 R +10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R +0 -5 R 10 0 R 10 0 R 0 -53 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R +10 0 R 0 -62 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R +11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R +0 -71 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R +10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R +0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -80 R +10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R +0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R +10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -89 R 10 0 R 10 0 R +0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R +11 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R +10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -97 R 10 0 R 10 0 R 0 -4 R 10 0 R +10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R +11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R +0 -4 R 10 0 R 10 0 R 0 -105 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R +10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R +0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -110 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R +0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R +10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R +0 -116 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R +11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R +0 -4 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -119 R +10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R +10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -122 R 10 0 R 10 0 R +0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R +10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R +10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -124 R 10 0 R 10 0 R 0 -5 R 11 0 R +10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R +0 -5 R 10 0 R 10 0 R 0 -126 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R +10 0 R 0 -128 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R +11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R +0 -129 R 10 0 R 10 0 R 0 -6 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 11 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -130 R +10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R +0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R +10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -127 R 10 0 R 10 0 R +0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R +10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R +10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -128 R 11 0 R 10 0 R 0 -3 R 10 0 R +10 0 R 0 -2 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R +11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R +0 -2 R 10 0 R 10 0 R 0 -128 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R +10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R +0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R +10 0 R 0 -129 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R +0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -2 R 10 0 R +10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R +0 -129 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R +11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R +0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -104 R D L0 +1796 10446 M 10 0 R 0 43 R 10 0 R 11 0 R 0 39 R 10 0 R 10 0 R 0 34 R 10 0 R +10 0 R 0 32 R 11 0 R 10 0 R 0 29 R 10 0 R 10 0 R 0 26 R 10 0 R 10 0 R 0 23 R +11 0 R 10 0 R 0 22 R 10 0 R 10 0 R 0 20 R 10 0 R 11 0 R 0 17 R 10 0 R 10 0 R +0 17 R 10 0 R 10 0 R 0 15 R 11 0 R 10 0 R 0 13 R 10 0 R 10 0 R 0 13 R 10 0 R +11 0 R 0 11 R 10 0 R 10 0 R 0 11 R 10 0 R 10 0 R 0 9 R 11 0 R 10 0 R 0 9 R +10 0 R 10 0 R 0 8 R 10 0 R 11 0 R 0 7 R 10 0 R 10 0 R 0 6 R 10 0 R 10 0 R +0 6 R 11 0 R 10 0 R 0 5 R 10 0 R 10 0 R 0 5 R 10 0 R 11 0 R 0 4 R 10 0 R +10 0 R 0 3 R 10 0 R 10 0 R 0 4 R 11 0 R 10 0 R 0 2 R 10 0 R 10 0 R 0 3 R +10 0 R 10 0 R 0 2 R 11 0 R 10 0 R 0 1 R 10 0 R 10 0 R 0 1 R 10 0 R 11 0 R +0 1 R 10 0 R 10 0 R 0 1 R 10 0 R 10 0 R 11 0 R 10 0 R 10 0 R 10 0 R 10 0 R +11 0 R 0 -1 R 10 0 R 10 0 R 10 0 R 10 0 R 0 -1 R 11 0 R 10 0 R 0 -1 R 10 0 R +10 0 R 0 -2 R 10 0 R 11 0 R 0 -1 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R +11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R +0 -3 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R +10 0 R 0 -4 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -3 R +10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R +0 -4 R 10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 11 0 R +10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R +10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R +0 -14 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R +10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -19 R +11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 10 0 R +11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -25 R 11 0 R 10 0 R +0 -6 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -6 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R +11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -32 R 10 0 R 11 0 R 0 -5 R 10 0 R +10 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R +10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -39 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R +10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 10 0 R 11 0 R +0 -5 R 10 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -6 R 10 0 R +10 0 R 0 -46 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -6 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 11 0 R +10 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R +0 -54 R 10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R +10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -63 R +10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 10 0 R 11 0 R 0 -5 R 10 0 R +10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -72 R 10 0 R 10 0 R +0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R +10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -80 R 10 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 10 0 R 11 0 R 0 -89 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R +11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R +11 0 R 0 -97 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R +0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -104 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R +10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R +0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -110 R +11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -115 R 10 0 R 11 0 R +0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R +10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R +11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -119 R 10 0 R 11 0 R 0 -5 R 10 0 R +10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R +10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R +0 -4 R 10 0 R 10 0 R 0 -122 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R +10 0 R 0 -125 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R +0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R +10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R +0 -127 R 10 0 R 10 0 R D 6924 8542 M 0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R +10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R +10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R +0 -128 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 10 0 R 11 0 R +0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -129 R +10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 10 0 R 10 0 R +0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 11 0 R +10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -130 R 10 0 R 10 0 R +0 -6 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 10 0 R +11 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -6 R 10 0 R 11 0 R 0 -131 R 10 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -6 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R +11 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -132 R 11 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R +10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R +0 -6 R 10 0 R 10 0 R 0 -6 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 10 0 R +10 0 R 0 -132 R 11 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R +0 -6 R 10 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R 0 -6 R 10 0 R +10 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -6 R 10 0 R 10 0 R +0 -133 R 10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -6 R +11 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -6 R 10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R +0 -6 R 10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -132 R +10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R +0 -7 R 10 0 R 10 0 R 0 -6 R 10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R D +40 setlinewidth 3771 10292 M 333 0 R -167 0 R 0 166 R 0 -333 R D +4523 10025 M 333 0 R -166 0 R 0 167 R 0 -333 R D 5285 9623 M 333 0 R +-166 0 R 0 166 R 0 -333 R D 6056 8964 M 333 0 R -166 0 R 0 167 R 0 -333 R D +2454 10998 M 167 -333 R -333 0 R 166 333 R D 3458 10739 M 166 -333 R +-333 0 R 167 333 R D 4481 10314 M 166 -333 R -333 0 R 167 333 R D +5522 9720 M 167 -333 R -333 0 R 166 333 R D 6580 9031 M 166 -333 R -333 0 R +167 333 R D 7650 8221 M 166 -333 R -333 0 R 167 333 R D 15 setlinewidth +9339 7061 M 7544 0 R D 10766 7061 M 0 99 R D +gsave 10766 6528 translate 0 0 M 1.01 dup scale -58.8433 0 N +( ) show grestore 12805 7061 M 0 99 R D gsave 12805 6528 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 14844 7061 M 0 99 R D gsave 14844 6528 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 16883 7061 M 0 99 R D gsave 16883 6528 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 9339 7061 M 0 49 R D 9542 7061 M 0 49 R D 9746 7061 M +0 49 R D 9950 7061 M 0 49 R D 10154 7061 M 0 49 R D 10358 7061 M 0 49 R D +10562 7061 M 0 49 R D 10970 7061 M 0 49 R D 11174 7061 M 0 49 R D +11378 7061 M 0 49 R D 11582 7061 M 0 49 R D 11785 7061 M 0 49 R D +11989 7061 M 0 49 R D 12193 7061 M 0 49 R D 12397 7061 M 0 49 R D +12601 7061 M 0 49 R D 13009 7061 M 0 49 R D 13213 7061 M 0 49 R D +13417 7061 M 0 49 R D 13621 7061 M 0 49 R D 13825 7061 M 0 49 R D +14028 7061 M 0 49 R D 14232 7061 M 0 49 R D 14436 7061 M 0 49 R D +14640 7061 M 0 49 R D 15048 7061 M 0 49 R D 15252 7061 M 0 49 R D +15456 7061 M 0 49 R D 15660 7061 M 0 49 R D 15864 7061 M 0 49 R D +16068 7061 M 0 49 R D 16271 7061 M 0 49 R D 16475 7061 M 0 49 R D +16679 7061 M 0 49 R D 9339 11989 M 7544 0 R D 10766 11989 M 0 -99 R D +12805 11989 M 0 -99 R D 14844 11989 M 0 -99 R D 16883 11989 M 0 -99 R D +9339 11989 M 0 -49 R D 9542 11989 M 0 -49 R D 9746 11989 M 0 -49 R D +9950 11989 M 0 -49 R D 10154 11989 M 0 -49 R D 10358 11989 M 0 -49 R D +10562 11989 M 0 -49 R D 10970 11989 M 0 -49 R D 11174 11989 M 0 -49 R D +11378 11989 M 0 -49 R D 11582 11989 M 0 -49 R D 11785 11989 M 0 -49 R D +11989 11989 M 0 -49 R D 12193 11989 M 0 -49 R D 12397 11989 M 0 -49 R D +12601 11989 M 0 -49 R D 13009 11989 M 0 -49 R D 13213 11989 M 0 -49 R D +13417 11989 M 0 -49 R D 13621 11989 M 0 -49 R D 13825 11989 M 0 -49 R D +14028 11989 M 0 -49 R D 14232 11989 M 0 -49 R D 14436 11989 M 0 -49 R D +14640 11989 M 0 -49 R D 15048 11989 M 0 -49 R D 15252 11989 M 0 -49 R D +15456 11989 M 0 -49 R D 15660 11989 M 0 -49 R D 15864 11989 M 0 -49 R D +16068 11989 M 0 -49 R D 16271 11989 M 0 -49 R D 16475 11989 M 0 -49 R D +16679 11989 M 0 -49 R D 9339 7061 M 0 4928 R D 9339 7061 M 150 0 R D +gsave 9226 7061 translate 0 0 M 1.01 dup scale -117.687 0 N +( ) show grestore 9339 7991 M 150 0 R D gsave 9226 7849 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9339 8921 M 150 0 R D gsave 9226 8778 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9339 9850 M 150 0 R D gsave 9226 9708 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9339 10780 M 150 0 R D gsave 9226 10638 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9339 11710 M 150 0 R D gsave 9226 11568 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9339 7154 M 75 0 R D 9339 7247 M 75 0 R D 9339 7340 M +75 0 R D 9339 7433 M 75 0 R D 9339 7526 M 75 0 R D 9339 7619 M 75 0 R D +9339 7712 M 75 0 R D 9339 7805 M 75 0 R D 9339 7898 M 75 0 R D 9339 8084 M +75 0 R D 9339 8177 M 75 0 R D 9339 8270 M 75 0 R D 9339 8363 M 75 0 R D +9339 8456 M 75 0 R D 9339 8549 M 75 0 R D 9339 8642 M 75 0 R D 9339 8735 M +75 0 R D 9339 8828 M 75 0 R D 9339 9014 M 75 0 R D 9339 9107 M 75 0 R D +9339 9200 M 75 0 R D 9339 9293 M 75 0 R D 9339 9386 M 75 0 R D 9339 9479 M +75 0 R D 9339 9572 M 75 0 R D 9339 9665 M 75 0 R D 9339 9758 M 75 0 R D +9339 9943 M 75 0 R D 9339 10036 M 75 0 R D 9339 10129 M 75 0 R D +9339 10222 M 75 0 R D 9339 10315 M 75 0 R D 9339 10408 M 75 0 R D +9339 10501 M 75 0 R D 9339 10594 M 75 0 R D 9339 10687 M 75 0 R D +9339 10873 M 75 0 R D 9339 10966 M 75 0 R D 9339 11059 M 75 0 R D +9339 11152 M 75 0 R D 9339 11245 M 75 0 R D 9339 11338 M 75 0 R D +9339 11431 M 75 0 R D 9339 11524 M 75 0 R D 9339 11617 M 75 0 R D +9339 11803 M 75 0 R D 9339 11896 M 75 0 R D 9339 11989 M 75 0 R D +16883 7061 M 0 4928 R D 16883 7061 M -151 0 R D 16883 7991 M -151 0 R D +16883 8921 M -151 0 R D 16883 9850 M -151 0 R D 16883 10780 M -151 0 R D +16883 11710 M -151 0 R D 16883 7154 M -75 0 R D 16883 7247 M -75 0 R D +16883 7340 M -75 0 R D 16883 7433 M -75 0 R D 16883 7526 M -75 0 R D +16883 7619 M -75 0 R D 16883 7712 M -75 0 R D 16883 7805 M -75 0 R D +16883 7898 M -75 0 R D 16883 8084 M -75 0 R D 16883 8177 M -75 0 R D +16883 8270 M -75 0 R D 16883 8363 M -75 0 R D 16883 8456 M -75 0 R D +16883 8549 M -75 0 R D 16883 8642 M -75 0 R D 16883 8735 M -75 0 R D +16883 8828 M -75 0 R D 16883 9014 M -75 0 R D 16883 9107 M -75 0 R D +16883 9200 M -75 0 R D 16883 9293 M -75 0 R D 16883 9386 M -75 0 R D +16883 9479 M -75 0 R D 16883 9572 M -75 0 R D 16883 9665 M -75 0 R D +16883 9758 M -75 0 R D 16883 9943 M -75 0 R D 16883 10036 M -75 0 R D +16883 10129 M -75 0 R D 16883 10222 M -75 0 R D 16883 10315 M -75 0 R D +16883 10408 M -75 0 R D 16883 10501 M -75 0 R D 16883 10594 M -75 0 R D +16883 10687 M -75 0 R D 16883 10873 M -75 0 R D 16883 10966 M -75 0 R D +16883 11059 M -75 0 R D 16883 11152 M -75 0 R D 16883 11245 M -75 0 R D +16883 11338 M -75 0 R D 16883 11431 M -75 0 R D 16883 11524 M -75 0 R D +16883 11617 M -75 0 R D 16883 11803 M -75 0 R D 16883 11896 M -75 0 R D +16883 11989 M -75 0 R D gsave 9746 7526 translate 0 0 M 1.25 dup scale +(z = 0.5) show grestore 40 setlinewidth 10766 11739 M 166 -167 R -166 -166 R +-167 166 R 167 167 R D 11785 11321 M 167 -167 R -167 -166 R -166 166 R +166 167 R D 12805 10789 M 167 -166 R -167 -167 R -166 167 R 166 166 R D +13825 10135 M 166 -167 R -166 -166 R -167 166 R 167 167 R D 14844 9409 M +167 -166 R -167 -167 R -166 167 R 166 166 R D 15864 8659 M 166 -167 R +-166 -166 R -167 166 R 167 167 R D 9534 11989 M 0 -1 R 11 0 R 10 0 R 0 -7 R +10 0 R 10 0 R 0 -8 R 10 0 R 11 0 R 0 -7 R 10 0 R 10 0 R 0 -7 R 10 0 R 10 0 R +0 -8 R 10 0 R 11 0 R 0 -7 R 10 0 R 10 0 R 0 -7 R 10 0 R 10 0 R 0 -8 R 11 0 R +10 0 R 0 -7 R 10 0 R 10 0 R 0 -7 R 10 0 R 11 0 R 0 -7 R 10 0 R 10 0 R 0 -8 R +10 0 R 10 0 R 0 -7 R 11 0 R 10 0 R 0 -7 R 10 0 R 10 0 R 0 -7 R 10 0 R 11 0 R +0 -7 R 10 0 R 10 0 R 0 -8 R 10 0 R 10 0 R 0 -7 R 11 0 R 10 0 R 0 -7 R 10 0 R +10 0 R 0 -7 R 10 0 R 11 0 R 0 -7 R 10 0 R 10 0 R 0 -7 R 10 0 R 10 0 R 0 -7 R +11 0 R 10 0 R 0 -8 R 10 0 R 10 0 R 0 -7 R 10 0 R 11 0 R 0 -7 R 10 0 R 10 0 R +0 -7 R 10 0 R 10 0 R 0 -7 R 10 0 R 11 0 R 0 -7 R 10 0 R 10 0 R 0 -7 R 10 0 R +10 0 R 0 -7 R 11 0 R 10 0 R 0 -7 R 10 0 R 10 0 R 0 -7 R 10 0 R 11 0 R 0 -7 R +10 0 R 10 0 R 0 -7 R 10 0 R 10 0 R 0 -7 R 11 0 R 10 0 R 0 -7 R 10 0 R 10 0 R +0 -6 R 10 0 R 11 0 R 0 -7 R 10 0 R 10 0 R 0 -7 R 10 0 R 10 0 R 0 -7 R 11 0 R +10 0 R 0 -7 R 10 0 R 10 0 R 0 -7 R 10 0 R 11 0 R 0 -7 R 10 0 R 10 0 R 0 -7 R +10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R 0 -7 R 10 0 R 10 0 R 0 -7 R 10 0 R 11 0 R +0 -7 R 10 0 R 10 0 R 0 -7 R 10 0 R 10 0 R 0 -6 R 10 0 R 11 0 R 0 -7 R 10 0 R +10 0 R 0 -7 R 10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R 0 -7 R 10 0 R 10 0 R 0 -7 R +10 0 R 11 0 R 0 -7 R 10 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -7 R 11 0 R 10 0 R +0 -7 R 10 0 R 10 0 R 0 -6 R 10 0 R 11 0 R 0 -7 R 10 0 R 10 0 R 0 -6 R 10 0 R +10 0 R 0 -7 R 11 0 R 10 0 R 0 -7 R 10 0 R 10 0 R 0 -6 R 10 0 R 11 0 R 0 -7 R +10 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -7 R 11 0 R 10 0 R 0 -6 R 10 0 R 10 0 R +0 -18 R 10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R 0 -7 R 10 0 R 10 0 R 0 -6 R +10 0 R 11 0 R 0 -7 R 10 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R +0 -7 R 10 0 R 10 0 R 0 -6 R 10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R 0 -27 R +10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -6 R 10 0 R 11 0 R +0 -6 R 10 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R 0 -6 R 10 0 R +10 0 R 0 -6 R 10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R 0 -33 R 10 0 R 10 0 R +0 -6 R 11 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 11 0 R +10 0 R 0 -6 R 10 0 R 10 0 R 0 -6 R 10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R 0 -39 R 10 0 R 10 0 R 0 -6 R 10 0 R +11 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -6 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -6 R 11 0 R 10 0 R 0 -46 R 10 0 R 10 0 R 0 -6 R 10 0 R 11 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -6 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R +11 0 R 0 -54 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R +0 -63 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R +10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -71 R +11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R +0 -4 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R +11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -79 R 11 0 R 10 0 R +0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -3 R 10 0 R +10 0 R 0 -4 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -4 R +10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -88 R 10 0 R 11 0 R 0 -4 R 10 0 R +10 0 R 0 -3 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -4 R +10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R +0 -3 R 10 0 R 10 0 R 0 -96 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -3 R +10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R +0 -3 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -3 R 10 0 R +10 0 R 0 -103 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R +0 -3 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -3 R 11 0 R +10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R +0 -109 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R +10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R +0 -3 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -114 R +10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R +0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R +10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -117 R 10 0 R 10 0 R +0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R +10 0 R 0 -3 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R +10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -120 R 10 0 R 10 0 R 0 -3 R 10 0 R +11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R +10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R +0 -3 R 10 0 R 11 0 R 0 -122 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R +11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R +0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R +11 0 R 0 -124 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R +0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R +10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R D 14632 9442 M 0 -2 R +10 0 R 10 0 R 0 -125 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R +11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R +10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R +0 -126 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R +10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R +0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -127 R +11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R +0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R +10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -128 R 10 0 R 11 0 R +0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R +10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R +11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -129 R 10 0 R 11 0 R 0 -2 R 10 0 R +10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R +10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R +0 -3 R 10 0 R 10 0 R 0 -128 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R +10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R +0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R +10 0 R 0 -128 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R +0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R +11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R +0 -130 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R +10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R +0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -129 R +10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R +0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R +10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -129 R 10 0 R 10 0 R +0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R +11 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R +10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -129 R 10 0 R 10 0 R 0 -3 R 10 0 R +10 0 R 0 -2 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R +10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R +0 -3 R 8 0 R D 20 setlinewidth L3 11869 10425 M 10 0 R 0 -5 R 11 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -5 R 10 0 R 11 0 R 0 -54 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R +10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R +10 0 R 11 0 R 0 -63 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R +10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -71 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -80 R +11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R +11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -89 R 10 0 R 11 0 R +0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R +11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -97 R 10 0 R 11 0 R 0 -5 R 10 0 R +10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R +10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R +0 -4 R 10 0 R 10 0 R 0 -104 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R +10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R +10 0 R 0 -110 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R +0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R +10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R +0 -116 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R +10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R +0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -119 R +10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R +10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -122 R 10 0 R 10 0 R +0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R +10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -125 R 10 0 R 10 0 R 0 -4 R 10 0 R +10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 10 0 R 11 0 R 0 -126 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R +11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 10 0 R +10 0 R 0 -128 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R +0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R +10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R +0 -126 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R +10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R +0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -127 R +11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R +0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R +10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -128 R 10 0 R 11 0 R +0 -2 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R +10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R +11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -129 R 10 0 R 11 0 R 0 -2 R 10 0 R +10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R +10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R +0 -2 R 10 0 R 10 0 R 0 -129 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R +10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R +0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -2 R 10 0 R +10 0 R 0 -129 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R +0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R +11 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R +0 -129 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R +10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R +0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -130 R +10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R +0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -2 R 10 0 R +10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -129 R 10 0 R 10 0 R +0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R +11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -1 R +D L0 10136 10843 M 10 0 R 0 6 R 10 0 R 10 0 R 0 6 R 11 0 R 10 0 R 0 5 R +10 0 R 10 0 R 0 4 R 10 0 R 11 0 R 0 4 R 10 0 R 10 0 R 0 3 R 10 0 R 10 0 R +0 3 R 11 0 R 10 0 R 0 3 R 10 0 R 10 0 R 0 2 R 10 0 R 11 0 R 0 2 R 10 0 R +10 0 R 0 2 R 10 0 R 10 0 R 0 1 R 11 0 R 10 0 R 0 1 R 10 0 R 10 0 R 0 1 R +10 0 R 11 0 R 0 1 R 10 0 R 10 0 R 10 0 R 10 0 R 11 0 R 10 0 R 10 0 R 10 0 R +0 -1 R 10 0 R 11 0 R 10 0 R 10 0 R 0 -1 R 10 0 R 10 0 R 0 -1 R 10 0 R 11 0 R +0 -1 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -1 R 11 0 R 10 0 R 0 -2 R 10 0 R +10 0 R 0 -2 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R +11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R +0 -3 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -3 R 10 0 R +11 0 R 0 -4 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -4 R +10 0 R 10 0 R 0 -15 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -4 R 10 0 R +10 0 R 0 -4 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R +11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R +0 -24 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R +10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -31 R +10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R +10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -38 R 10 0 R 10 0 R +0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R +10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -46 R 10 0 R 10 0 R 0 -5 R 10 0 R +11 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 10 0 R 11 0 R 0 -55 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R +11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R +11 0 R 0 -63 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R +0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -72 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -80 R +11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R +0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R +11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -89 R 10 0 R 11 0 R +0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R +11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -97 R 10 0 R 11 0 R 0 -4 R 10 0 R +10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R +10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -104 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -4 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R +10 0 R 0 -111 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R +0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R +10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R +0 -116 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R +10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R +0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -119 R +10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R +10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -122 R 10 0 R 10 0 R +0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R +10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -125 R 10 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 10 0 R 11 0 R 0 -126 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R +11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -128 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R +0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -6 R 10 0 R +10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -129 R 11 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -130 R +11 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -6 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R D 15264 8124 M 0 -131 R +10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R +0 -6 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R 0 -6 R 10 0 R +10 0 R 0 -5 R 11 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -131 R 10 0 R 11 0 R +0 -6 R 10 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -6 R 10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -6 R +10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -132 R 10 0 R 10 0 R 0 -6 R 11 0 R +10 0 R 0 -6 R 10 0 R 10 0 R 0 -6 R 10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R 0 -6 R +10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -6 R 10 0 R 11 0 R +0 -6 R 10 0 R 10 0 R 0 -132 R 10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R 0 -6 R +10 0 R 10 0 R 0 -6 R 10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R 0 -6 R 10 0 R 10 0 R +0 -6 R 10 0 R 11 0 R 0 -7 R 10 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -6 R 11 0 R +10 0 R 0 -133 R 10 0 R 10 0 R 0 -6 R 10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R +0 -6 R 10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R 0 -7 R 10 0 R 10 0 R 0 -6 R 10 0 R +11 0 R 0 -6 R 10 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -7 R 11 0 R 10 0 R +0 -133 R 10 0 R 10 0 R 0 -3 R D 40 setlinewidth 11690 10306 M 333 0 R +-166 0 R 0 166 R 0 -333 R D 12448 10044 M 333 0 R -167 0 R 0 167 R 0 -333 R +D 13214 9657 M 333 0 R -166 0 R 0 166 R 0 -333 R D 13989 9017 M 333 0 R +-166 0 R 0 167 R 0 -333 R D 14771 8192 M 333 0 R -166 0 R 0 167 R 0 -333 R D +10123 11053 M 167 -333 R -333 0 R 166 333 R D 11129 10838 M 167 -333 R +-333 0 R 166 333 R D 12155 10449 M 166 -333 R -333 0 R 167 333 R D +13198 9900 M 167 -333 R -333 0 R 166 333 R D 14257 9236 M 167 -333 R +-333 0 R 166 333 R D 15329 8425 M 167 -333 R -333 0 R 166 333 R D +15 setlinewidth 1794 2133 M 7545 0 R D 3221 2133 M 0 99 R D +gsave 3221 1600 translate 0 0 M 1.01 dup scale -235.373 0 N +(11) show grestore 5260 2133 M 0 99 R D gsave 5260 1600 translate 0 0 M +1.01 dup scale -235.373 0 N +(12) show grestore 7299 2133 M 0 99 R D gsave 7299 1600 translate 0 0 M +1.01 dup scale -235.373 0 N +(13) show grestore 9339 2133 M 0 99 R D gsave 9339 1600 translate 0 0 M +1.01 dup scale -235.373 0 N +(14) show grestore 1794 2133 M 0 49 R D 1998 2133 M 0 49 R D 2202 2133 M +0 49 R D 2406 2133 M 0 49 R D 2609 2133 M 0 49 R D 2813 2133 M 0 49 R D +3017 2133 M 0 49 R D 3425 2133 M 0 49 R D 3629 2133 M 0 49 R D 3833 2133 M +0 49 R D 4037 2133 M 0 49 R D 4241 2133 M 0 49 R D 4445 2133 M 0 49 R D +4649 2133 M 0 49 R D 4853 2133 M 0 49 R D 5056 2133 M 0 49 R D 5464 2133 M +0 49 R D 5668 2133 M 0 49 R D 5872 2133 M 0 49 R D 6076 2133 M 0 49 R D +6280 2133 M 0 49 R D 6484 2133 M 0 49 R D 6688 2133 M 0 49 R D 6892 2133 M +0 49 R D 7096 2133 M 0 49 R D 7503 2133 M 0 49 R D 7707 2133 M 0 49 R D +7911 2133 M 0 49 R D 8115 2133 M 0 49 R D 8319 2133 M 0 49 R D 8523 2133 M +0 49 R D 8727 2133 M 0 49 R D 8931 2133 M 0 49 R D 9135 2133 M 0 49 R D +1794 7061 M 7545 0 R D 3221 7061 M 0 -98 R D 5260 7061 M 0 -98 R D +7299 7061 M 0 -98 R D 9339 7061 M 0 -98 R D 1794 7061 M 0 -49 R D +1998 7061 M 0 -49 R D 2202 7061 M 0 -49 R D 2406 7061 M 0 -49 R D +2609 7061 M 0 -49 R D 2813 7061 M 0 -49 R D 3017 7061 M 0 -49 R D +3425 7061 M 0 -49 R D 3629 7061 M 0 -49 R D 3833 7061 M 0 -49 R D +4037 7061 M 0 -49 R D 4241 7061 M 0 -49 R D 4445 7061 M 0 -49 R D +4649 7061 M 0 -49 R D 4853 7061 M 0 -49 R D 5056 7061 M 0 -49 R D +5464 7061 M 0 -49 R D 5668 7061 M 0 -49 R D 5872 7061 M 0 -49 R D +6076 7061 M 0 -49 R D 6280 7061 M 0 -49 R D 6484 7061 M 0 -49 R D +6688 7061 M 0 -49 R D 6892 7061 M 0 -49 R D 7096 7061 M 0 -49 R D +7503 7061 M 0 -49 R D 7707 7061 M 0 -49 R D 7911 7061 M 0 -49 R D +8115 7061 M 0 -49 R D 8319 7061 M 0 -49 R D 8523 7061 M 0 -49 R D +8727 7061 M 0 -49 R D 8931 7061 M 0 -49 R D 9135 7061 M 0 -49 R D +1794 2133 M 0 4928 R D 1794 2133 M 151 0 R D gsave 1682 2133 translate 0 0 M +1.01 dup scale -376.343 0 N +(-9) show grestore 1794 3063 M 151 0 R D gsave 1682 2921 translate 0 0 M +1.01 dup scale -376.343 0 N +(-8) show grestore 1794 3993 M 151 0 R D gsave 1682 3851 translate 0 0 M +1.01 dup scale -376.343 0 N +(-7) show grestore 1794 4923 M 151 0 R D gsave 1682 4780 translate 0 0 M +1.01 dup scale -376.343 0 N +(-6) show grestore 1794 5852 M 151 0 R D gsave 1682 5710 translate 0 0 M +1.01 dup scale -376.343 0 N +(-5) show grestore 1794 6782 M 151 0 R D gsave 1682 6640 translate 0 0 M +1.01 dup scale -376.343 0 N +(-4) show grestore 1794 2226 M 75 0 R D 1794 2319 M 75 0 R D 1794 2412 M +75 0 R D 1794 2505 M 75 0 R D 1794 2598 M 75 0 R D 1794 2691 M 75 0 R D +1794 2784 M 75 0 R D 1794 2877 M 75 0 R D 1794 2970 M 75 0 R D 1794 3156 M +75 0 R D 1794 3249 M 75 0 R D 1794 3342 M 75 0 R D 1794 3435 M 75 0 R D +1794 3528 M 75 0 R D 1794 3621 M 75 0 R D 1794 3714 M 75 0 R D 1794 3807 M +75 0 R D 1794 3900 M 75 0 R D 1794 4086 M 75 0 R D 1794 4179 M 75 0 R D +1794 4272 M 75 0 R D 1794 4365 M 75 0 R D 1794 4458 M 75 0 R D 1794 4551 M +75 0 R D 1794 4644 M 75 0 R D 1794 4737 M 75 0 R D 1794 4830 M 75 0 R D +1794 5016 M 75 0 R D 1794 5109 M 75 0 R D 1794 5202 M 75 0 R D 1794 5294 M +75 0 R D 1794 5387 M 75 0 R D 1794 5480 M 75 0 R D 1794 5573 M 75 0 R D +1794 5666 M 75 0 R D 1794 5759 M 75 0 R D 1794 5945 M 75 0 R D 1794 6038 M +75 0 R D 1794 6131 M 75 0 R D 1794 6224 M 75 0 R D 1794 6317 M 75 0 R D +1794 6410 M 75 0 R D 1794 6503 M 75 0 R D 1794 6596 M 75 0 R D 1794 6689 M +75 0 R D 1794 6875 M 75 0 R D 1794 6968 M 75 0 R D 1794 7061 M 75 0 R D +9339 2133 M 0 4928 R D 9339 2133 M -151 0 R D 9339 3063 M -151 0 R D +9339 3993 M -151 0 R D 9339 4923 M -151 0 R D 9339 5852 M -151 0 R D +9339 6782 M -151 0 R D 9339 2226 M -76 0 R D 9339 2319 M -76 0 R D +9339 2412 M -76 0 R D 9339 2505 M -76 0 R D 9339 2598 M -76 0 R D +9339 2691 M -76 0 R D 9339 2784 M -76 0 R D 9339 2877 M -76 0 R D +9339 2970 M -76 0 R D 9339 3156 M -76 0 R D 9339 3249 M -76 0 R D +9339 3342 M -76 0 R D 9339 3435 M -76 0 R D 9339 3528 M -76 0 R D +9339 3621 M -76 0 R D 9339 3714 M -76 0 R D 9339 3807 M -76 0 R D +9339 3900 M -76 0 R D 9339 4086 M -76 0 R D 9339 4179 M -76 0 R D +9339 4272 M -76 0 R D 9339 4365 M -76 0 R D 9339 4458 M -76 0 R D +9339 4551 M -76 0 R D 9339 4644 M -76 0 R D 9339 4737 M -76 0 R D +9339 4830 M -76 0 R D 9339 5016 M -76 0 R D 9339 5109 M -76 0 R D +9339 5202 M -76 0 R D 9339 5294 M -76 0 R D 9339 5387 M -76 0 R D +9339 5480 M -76 0 R D 9339 5573 M -76 0 R D 9339 5666 M -76 0 R D +9339 5759 M -76 0 R D 9339 5945 M -76 0 R D 9339 6038 M -76 0 R D +9339 6131 M -76 0 R D 9339 6224 M -76 0 R D 9339 6317 M -76 0 R D +9339 6410 M -76 0 R D 9339 6503 M -76 0 R D 9339 6596 M -76 0 R D +9339 6689 M -76 0 R D 9339 6875 M -76 0 R D 9339 6968 M -76 0 R D +9339 7061 M -76 0 R D gsave 2202 2598 translate 0 0 M 1.25 dup scale +(z = 0.8) show grestore 40 setlinewidth 3221 6976 M 167 -166 R -167 -167 R +-166 167 R 166 166 R D 4241 6704 M 166 -166 R -166 -167 R -167 167 R +167 166 R D 5260 6173 M 167 -167 R -167 -166 R -166 166 R 166 167 R D +6280 5518 M 166 -166 R -166 -167 R -167 167 R 167 166 R D 7299 4793 M +167 -167 R -167 -166 R -166 166 R 166 167 R D 8319 4042 M 166 -166 R +-166 -167 R -167 167 R 167 166 R D 1888 7061 M 0 -2 R 10 0 R 10 0 R 0 -6 R +10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R +0 -6 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -6 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R +11 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R +11 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -6 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 11 0 R +10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R +0 -5 R 10 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -5 R 10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R +11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -6 R +10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R +10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R +10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R +10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 10 0 R +10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R +10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R +11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R +10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R +10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R +0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R +11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R +11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -16 R 10 0 R +10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R +11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -85 R 10 0 R 10 0 R 0 -4 R +10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R +0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -4 R 11 0 R 10 0 R 0 -91 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R +0 -4 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -4 R 10 0 R +10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R +10 0 R 11 0 R 0 -96 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 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10 0 R +0 -3 R 10 0 R 10 0 R 0 -117 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R +10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R +0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -3 R 10 0 R +10 0 R 0 -120 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R +0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R +10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R +0 -123 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R +10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R +0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -124 R +10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R +D 6985 4838 M 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R +0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -125 R +10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R +0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R +10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -127 R 10 0 R 10 0 R +0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R +11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R +10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -127 R 10 0 R 10 0 R 0 -3 R 10 0 R +10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R +10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R +0 -3 R 10 0 R 11 0 R 0 -128 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R +11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R +0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R +10 0 R 0 -128 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R +0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R +10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R +0 -129 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R +10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R +0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -129 R +10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R +0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R +10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -129 R 10 0 R 11 0 R +0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R +10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R +11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -129 R 10 0 R 10 0 R 0 -3 R 11 0 R +10 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R +10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R +0 -2 R 10 0 R 10 0 R 0 -129 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R +10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R +0 -2 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R +10 0 R 0 -130 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R +0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R +11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R 8 0 R D +20 setlinewidth L3 4324 5758 M 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R +0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R +10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R +0 -16 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R +0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -86 R +10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R +10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -92 R 10 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R +11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -98 R 10 0 R 10 0 R 0 -4 R 10 0 R +10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R +10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 10 0 R 11 0 R 0 -103 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R +11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -108 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R +0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R +10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -113 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R +10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -117 R +10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R +0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R +10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -119 R 10 0 R 11 0 R +0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R +10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -122 R 10 0 R 10 0 R 0 -5 R 11 0 R +10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R +0 -5 R 10 0 R 10 0 R 0 -124 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R +10 0 R 0 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10 0 R 0 -2 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R +0 -3 R 10 0 R 10 0 R 0 -128 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R +10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R +0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R +10 0 R 0 -128 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R +0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R +10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R +0 -129 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R +11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R +0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -129 R +10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R +0 -2 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R +10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -129 R 10 0 R 10 0 R +0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R +10 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R +10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -129 R 10 0 R 10 0 R 0 -2 R 11 0 R +10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R +10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R +0 -2 R 10 0 R 10 0 R 0 -130 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R +10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R +0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R 8 0 R +D L0 3346 6105 M 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R +10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R +0 -3 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R +10 0 R 0 -3 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -3 R +10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R +0 -3 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -4 R 10 0 R +10 0 R 0 -3 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -3 R +10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R +0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R +10 0 R 0 -4 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -4 R +10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -4 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R +11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R +0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R +10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R +10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -15 R +10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R +10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -85 R 10 0 R 10 0 R +0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R +10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R +10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -92 R 10 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 10 0 R 11 0 R 0 -97 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R +11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R +0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R +11 0 R 0 -103 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R +0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -4 R 10 0 R +10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R +0 -108 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -4 R +10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R +0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -112 R +11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R +0 -4 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R +10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -116 R 10 0 R 11 0 R +0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -4 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R +11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -119 R 10 0 R 11 0 R 0 -4 R 10 0 R +10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R +10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R +0 -4 R 10 0 R 10 0 R 0 -122 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R +10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -4 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R +10 0 R 0 -125 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R +10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R +0 -126 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R +10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R +0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -127 R +10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R +10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -129 R 10 0 R 10 0 R +0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R +11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -130 R 10 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -6 R +10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -5 R 10 0 R 11 0 R 0 -131 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R +11 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R +0 -6 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 10 0 R +10 0 R 0 -131 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 10 0 R 11 0 R +0 -5 R 10 0 R 10 0 R 0 -6 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -6 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -6 R 10 0 R 10 0 R +0 -132 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R +10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R +0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -129 R +10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R +0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R D 8443 2980 M 11 0 R 0 -3 R 10 0 R 10 0 R +0 -2 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -129 R +10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R +0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R 10 0 R +10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -129 R 10 0 R 10 0 R +0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R +10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R +10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -129 R 10 0 R 10 0 R 0 -3 R 11 0 R +10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R +10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R +0 -3 R 10 0 R 10 0 R 0 -129 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R +10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R +0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 8 0 R +D 40 setlinewidth 4146 5548 M 333 0 R -167 0 R 0 167 R 0 -333 R D +4903 5315 M 333 0 R -166 0 R 0 167 R 0 -333 R D 5670 5036 M 333 0 R -167 0 R +0 167 R 0 -333 R D 6445 4595 M 333 0 R -167 0 R 0 167 R 0 -333 R D +7226 3897 M 333 0 R -166 0 R 0 167 R 0 -333 R D 8014 3050 M 333 0 R -166 0 R +0 166 R 0 -332 R D 3331 6138 M 167 -333 R -333 0 R 166 333 R D 4352 5873 M +166 -333 R -333 0 R 167 333 R D 5391 5433 M 167 -333 R -333 0 R 166 333 R D +6447 4899 M 166 -333 R -333 0 R 167 333 R D 7516 4091 M 166 -333 R -333 0 R +167 333 R D 8595 3276 M 166 -333 R -333 0 R 167 333 R D 15 setlinewidth +9339 2133 M 7544 0 R D 10766 2133 M 0 99 R D +gsave 10766 1600 translate 0 0 M 1.01 dup scale -235.373 0 N +(11) show grestore 12805 2133 M 0 99 R D gsave 12805 1600 translate 0 0 M +1.01 dup scale -235.373 0 N +(12) show grestore 14844 2133 M 0 99 R D gsave 14844 1600 translate 0 0 M +1.01 dup scale -235.373 0 N +(13) show grestore 16883 2133 M 0 99 R D gsave 16883 1600 translate 0 0 M +1.01 dup scale -235.373 0 N +(14) show grestore 9339 2133 M 0 49 R D 9542 2133 M 0 49 R D 9746 2133 M +0 49 R D 9950 2133 M 0 49 R D 10154 2133 M 0 49 R D 10358 2133 M 0 49 R D +10562 2133 M 0 49 R D 10970 2133 M 0 49 R D 11174 2133 M 0 49 R D +11378 2133 M 0 49 R D 11582 2133 M 0 49 R D 11785 2133 M 0 49 R D +11989 2133 M 0 49 R D 12193 2133 M 0 49 R D 12397 2133 M 0 49 R D +12601 2133 M 0 49 R D 13009 2133 M 0 49 R D 13213 2133 M 0 49 R D +13417 2133 M 0 49 R D 13621 2133 M 0 49 R D 13825 2133 M 0 49 R D +14028 2133 M 0 49 R D 14232 2133 M 0 49 R D 14436 2133 M 0 49 R D +14640 2133 M 0 49 R D 15048 2133 M 0 49 R D 15252 2133 M 0 49 R D +15456 2133 M 0 49 R D 15660 2133 M 0 49 R D 15864 2133 M 0 49 R D +16068 2133 M 0 49 R D 16271 2133 M 0 49 R D 16475 2133 M 0 49 R D +16679 2133 M 0 49 R D 9339 7061 M 7544 0 R D 10766 7061 M 0 -98 R D +12805 7061 M 0 -98 R D 14844 7061 M 0 -98 R D 16883 7061 M 0 -98 R D +9339 7061 M 0 -49 R D 9542 7061 M 0 -49 R D 9746 7061 M 0 -49 R D +9950 7061 M 0 -49 R D 10154 7061 M 0 -49 R D 10358 7061 M 0 -49 R D +10562 7061 M 0 -49 R D 10970 7061 M 0 -49 R D 11174 7061 M 0 -49 R D +11378 7061 M 0 -49 R D 11582 7061 M 0 -49 R D 11785 7061 M 0 -49 R D +11989 7061 M 0 -49 R D 12193 7061 M 0 -49 R D 12397 7061 M 0 -49 R D +12601 7061 M 0 -49 R D 13009 7061 M 0 -49 R D 13213 7061 M 0 -49 R D +13417 7061 M 0 -49 R D 13621 7061 M 0 -49 R D 13825 7061 M 0 -49 R D +14028 7061 M 0 -49 R D 14232 7061 M 0 -49 R D 14436 7061 M 0 -49 R D +14640 7061 M 0 -49 R D 15048 7061 M 0 -49 R D 15252 7061 M 0 -49 R D +15456 7061 M 0 -49 R D 15660 7061 M 0 -49 R D 15864 7061 M 0 -49 R D +16068 7061 M 0 -49 R D 16271 7061 M 0 -49 R D 16475 7061 M 0 -49 R D +16679 7061 M 0 -49 R D 9339 2133 M 0 4928 R D 9339 2133 M 150 0 R D +gsave 9226 2133 translate 0 0 M 1.01 dup scale -117.687 0 N +( ) show grestore 9339 3063 M 150 0 R D gsave 9226 2921 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9339 3993 M 150 0 R D gsave 9226 3851 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9339 4923 M 150 0 R D gsave 9226 4780 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9339 5852 M 150 0 R D gsave 9226 5710 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9339 6782 M 150 0 R D gsave 9226 6640 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9339 2226 M 75 0 R D 9339 2319 M 75 0 R D 9339 2412 M +75 0 R D 9339 2505 M 75 0 R D 9339 2598 M 75 0 R D 9339 2691 M 75 0 R D +9339 2784 M 75 0 R D 9339 2877 M 75 0 R D 9339 2970 M 75 0 R D 9339 3156 M +75 0 R D 9339 3249 M 75 0 R D 9339 3342 M 75 0 R D 9339 3435 M 75 0 R D +9339 3528 M 75 0 R D 9339 3621 M 75 0 R D 9339 3714 M 75 0 R D 9339 3807 M +75 0 R D 9339 3900 M 75 0 R D 9339 4086 M 75 0 R D 9339 4179 M 75 0 R D +9339 4272 M 75 0 R D 9339 4365 M 75 0 R D 9339 4458 M 75 0 R D 9339 4551 M +75 0 R D 9339 4644 M 75 0 R D 9339 4737 M 75 0 R D 9339 4830 M 75 0 R D +9339 5016 M 75 0 R D 9339 5109 M 75 0 R D 9339 5202 M 75 0 R D 9339 5294 M +75 0 R D 9339 5387 M 75 0 R D 9339 5480 M 75 0 R D 9339 5573 M 75 0 R D +9339 5666 M 75 0 R D 9339 5759 M 75 0 R D 9339 5945 M 75 0 R D 9339 6038 M +75 0 R D 9339 6131 M 75 0 R D 9339 6224 M 75 0 R D 9339 6317 M 75 0 R D +9339 6410 M 75 0 R D 9339 6503 M 75 0 R D 9339 6596 M 75 0 R D 9339 6689 M +75 0 R D 9339 6875 M 75 0 R D 9339 6968 M 75 0 R D 9339 7061 M 75 0 R D +16883 2133 M 0 4928 R D 16883 2133 M -151 0 R D 16883 3063 M -151 0 R D +16883 3993 M -151 0 R D 16883 4923 M -151 0 R D 16883 5852 M -151 0 R D +16883 6782 M -151 0 R D 16883 2226 M -75 0 R D 16883 2319 M -75 0 R D +16883 2412 M -75 0 R D 16883 2505 M -75 0 R D 16883 2598 M -75 0 R D +16883 2691 M -75 0 R D 16883 2784 M -75 0 R D 16883 2877 M -75 0 R D +16883 2970 M -75 0 R D 16883 3156 M -75 0 R D 16883 3249 M -75 0 R D +16883 3342 M -75 0 R D 16883 3435 M -75 0 R D 16883 3528 M -75 0 R D +16883 3621 M -75 0 R D 16883 3714 M -75 0 R D 16883 3807 M -75 0 R D +16883 3900 M -75 0 R D 16883 4086 M -75 0 R D 16883 4179 M -75 0 R D +16883 4272 M -75 0 R D 16883 4365 M -75 0 R D 16883 4458 M -75 0 R D +16883 4551 M -75 0 R D 16883 4644 M -75 0 R D 16883 4737 M -75 0 R D +16883 4830 M -75 0 R D 16883 5016 M -75 0 R D 16883 5109 M -75 0 R D +16883 5202 M -75 0 R D 16883 5294 M -75 0 R D 16883 5387 M -75 0 R D +16883 5480 M -75 0 R D 16883 5573 M -75 0 R D 16883 5666 M -75 0 R D +16883 5759 M -75 0 R D 16883 5945 M -75 0 R D 16883 6038 M -75 0 R D +16883 6131 M -75 0 R D 16883 6224 M -75 0 R D 16883 6317 M -75 0 R D +16883 6410 M -75 0 R D 16883 6503 M -75 0 R D 16883 6596 M -75 0 R D +16883 6689 M -75 0 R D 16883 6875 M -75 0 R D 16883 6968 M -75 0 R D +16883 7061 M -75 0 R D gsave 9746 2598 translate 0 0 M 1.25 dup scale +(z = 1.0) show grestore 40 setlinewidth 10766 6912 M 166 -166 R -166 -167 R +-167 167 R 167 166 R D 11785 6804 M 167 -166 R -167 -167 R -166 167 R +166 166 R D 12805 6353 M 167 -167 R -167 -166 R -166 166 R 166 167 R D +13825 5698 M 166 -166 R -166 -167 R -167 167 R 167 166 R D 14844 4973 M +167 -167 R -167 -166 R -166 166 R 166 167 R D 15864 4222 M 166 -166 R +-166 -167 R -167 167 R 167 166 R D 9341 7012 M 10 0 R 0 -5 R 10 0 R 10 0 R +0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R +10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R +0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R +10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R +10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R +0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R +10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R +10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R +11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R +0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R +10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R +10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R +0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R +10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R +11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -5 R 10 0 R 10 0 R +0 -4 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R +11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -4 R +10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R +0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 11 0 R +10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R +10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R +0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -4 R 10 0 R +10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R +11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R +0 -4 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R +10 0 R 0 -4 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -4 R +10 0 R 10 0 R 0 -5 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R +0 -4 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R +10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R +10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R +0 -5 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -4 R 10 0 R +10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R +10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R +0 -4 R 10 0 R 10 0 R 0 -5 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R +10 0 R 0 -4 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -4 R +10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R +0 -4 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 11 0 R +10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R 0 -4 R +10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R +0 -4 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -4 R 10 0 R +10 0 R 0 -4 R 10 0 R 10 0 R 0 -5 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R +10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 11 0 R 10 0 R +0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -4 R 10 0 R 10 0 R 0 -3 R 10 0 R +10 0 R 0 -110 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -4 R 10 0 R 10 0 R +0 -3 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -3 R 10 0 R +10 0 R 0 -4 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -4 R 10 0 R 10 0 R +0 -112 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -3 R +11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -4 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R +0 -3 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -114 R +10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R +0 -3 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -3 R 10 0 R +10 0 R 0 -3 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -116 R 10 0 R 10 0 R +0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R +10 0 R 0 -3 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R +10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -118 R 10 0 R 10 0 R 0 -2 R 11 0 R +10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -3 R +10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R +0 -3 R 11 0 R 10 0 R 0 -120 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R +10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R +0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R +10 0 R 0 -120 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R +0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R +10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R +0 -123 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R +10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R +0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R D 14438 5150 M +11 0 R 0 -124 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R +0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R +10 0 R 0 -3 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R +0 -125 R 11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R +10 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R +0 -2 R 10 0 R 11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -127 R +11 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -3 R 10 0 R 11 0 R 0 -2 R 10 0 R 10 0 R +0 -3 R 10 0 R 10 0 R 0 -2 R 11 0 R 10 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R +11 0 R 0 -3 R 10 0 R 10 0 R 0 -2 R 10 0 R 10 0 R 0 -127 R 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+423.333 /Helvetica STDFONT +( \)) show grestore +%%PageTrailer +end +restore +showpage +%%PageResources: font Helvetica +%%+ font Symbol +%%+ font AvantGarde-Book +%%Trailer +restore +%%Pages: 1 +%%DocumentNeededResources: font Helvetica +%%+ font Symbol +%%+ font AvantGarde-Book +%%EOF diff --git a/feedback/papers/0506398/f11.ps b/feedback/papers/0506398/f11.ps new file mode 100644 index 0000000..50292f7 --- /dev/null +++ b/feedback/papers/0506398/f11.ps @@ -0,0 +1,890 @@ +%!PS-Adobe-3.0 +%%BoundingBox: 54 360 558 720 +%%Title: Graphics produced by IDL +%%For: phopkins@Philip-Hopkins-Computer.local, +%% /Users/phopkins/Documents/lars_galaxies/plots/LF_massive +%%Creator: IDL Student Edition 6.0.3, Mac OS X (darwin ppc m32) +%%CreationDate: Thu Nov 3 08:22:53 2005 +%%DocumentData: Clean7bit +%%Requirements: color +%%LanguageLevel: 1 +%%PageOrder: Ascend +%%Pages: (atend) +%%DocumentNeededResources: (atend) +%%EndComments +%%BeginProlog +save +%+ prolog.ps -- Prolog for IDL generated PostScript files +%+ Copyright (c) 1988-2003 Research Systems, Inc. All Rights Reserved. +%v 4 +/$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C +{currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint +stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} +bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show +grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 +setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 +{[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 +100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 +{[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef +/ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} +ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont +exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica +findfont exch scalefont setfont (\267) show currentpoint grestore moveto} +bdef end 2.5 setmiterlimit +%%EndProlog +%%Page: 0 1 +%%PageRequirements: color +%%PageResources: (atend) +%%PageOrientation: Portrait +%%PageBoundingBox: 54 360 558 720 +%%BeginPageSetup +save +$IDL_DICT begin 54 360 translate 0.0283465 dup scale +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +%%EndPageSetup +15 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 2242 6706 M 4955 0 R D +3220 6706 M 0 105 R D gsave 3220 6172 translate 0 0 M 1.01 dup scale +-58.8433 0 N +( ) show grestore 4524 6706 M 0 105 R D gsave 4524 6172 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 5828 6706 M 0 105 R D gsave 5828 6172 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 7132 6706 M 0 105 R D gsave 7132 6172 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 2242 6706 M 0 52 R D 2568 6706 M 0 52 R D 2894 6706 M +0 52 R D 3546 6706 M 0 52 R D 3872 6706 M 0 52 R D 4198 6706 M 0 52 R D +4850 6706 M 0 52 R D 5176 6706 M 0 52 R D 5502 6706 M 0 52 R D 6154 6706 M +0 52 R D 6480 6706 M 0 52 R D 6806 6706 M 0 52 R D 2242 11989 M 4955 0 R D +3220 11989 M 0 -106 R D 4524 11989 M 0 -106 R D 5828 11989 M 0 -106 R D +7132 11989 M 0 -106 R D 2242 11989 M 0 -53 R D 2568 11989 M 0 -53 R D +2894 11989 M 0 -53 R D 3546 11989 M 0 -53 R D 3872 11989 M 0 -53 R D +4198 11989 M 0 -53 R D 4850 11989 M 0 -53 R D 5176 11989 M 0 -53 R D +5502 11989 M 0 -53 R D 6154 11989 M 0 -53 R D 6480 11989 M 0 -53 R D +6806 11989 M 0 -53 R D 2242 6706 M 0 5283 R D 2242 7036 M 99 0 R D +gsave 2130 6894 translate 0 0 M 1.01 dup scale -376.343 0 N +(-8) show grestore 2242 8687 M 99 0 R D gsave 2130 8545 translate 0 0 M +1.01 dup scale -376.343 0 N +(-7) show grestore 2242 10338 M 99 0 R D gsave 2130 10196 translate 0 0 M +1.01 dup scale -376.343 0 N +(-6) show grestore 2242 11989 M 99 0 R D gsave 2130 11740 translate 0 0 M +1.01 dup scale -376.343 0 N +(-5) show grestore 2242 6706 M 50 0 R D 2242 6871 M 50 0 R D 2242 7201 M +50 0 R D 2242 7366 M 50 0 R D 2242 7531 M 50 0 R D 2242 7696 M 50 0 R D +2242 7861 M 50 0 R D 2242 8026 M 50 0 R D 2242 8192 M 50 0 R D 2242 8357 M +50 0 R D 2242 8522 M 50 0 R D 2242 8852 M 50 0 R D 2242 9017 M 50 0 R D +2242 9182 M 50 0 R D 2242 9347 M 50 0 R D 2242 9512 M 50 0 R D 2242 9678 M +50 0 R D 2242 9843 M 50 0 R D 2242 10008 M 50 0 R D 2242 10173 M 50 0 R D +2242 10503 M 50 0 R D 2242 10668 M 50 0 R D 2242 10833 M 50 0 R D +2242 10998 M 50 0 R D 2242 11163 M 50 0 R D 2242 11329 M 50 0 R D +2242 11494 M 50 0 R D 2242 11659 M 50 0 R D 2242 11824 M 50 0 R D +7197 6706 M 0 5283 R D 7197 7036 M -99 0 R D 7197 8687 M -99 0 R D +7197 10338 M -99 0 R D 7197 11989 M -99 0 R D 7197 6706 M -49 0 R D +7197 6871 M -49 0 R D 7197 7201 M -49 0 R D 7197 7366 M -49 0 R D +7197 7531 M -49 0 R D 7197 7696 M -49 0 R D 7197 7861 M -49 0 R D +7197 8026 M -49 0 R D 7197 8192 M -49 0 R D 7197 8357 M -49 0 R D +7197 8522 M -49 0 R D 7197 8852 M -49 0 R D 7197 9017 M -49 0 R D +7197 9182 M -49 0 R D 7197 9347 M -49 0 R D 7197 9512 M -49 0 R D +7197 9678 M -49 0 R D 7197 9843 M -49 0 R D 7197 10008 M -49 0 R D +7197 10173 M -49 0 R D 7197 10503 M -49 0 R D 7197 10668 M -49 0 R D +7197 10833 M -49 0 R D 7197 10998 M -49 0 R D 7197 11163 M -49 0 R D +7197 11329 M -49 0 R D 7197 11494 M -49 0 R D 7197 11659 M -49 0 R D +7197 11824 M -49 0 R D 2588 10590 M 0 222 R 222 0 R 0 -222 R -222 0 R F +3240 10920 M 0 222 R 222 0 R 0 -222 R -222 0 R F +3892 10739 M 0 222 R 222 0 R 0 -222 R -222 0 R F +4544 10194 M 0 222 R 222 0 R 0 -222 R -222 0 R F +5196 10062 M 0 222 R 222 0 R 0 -222 R -222 0 R F +5848 8906 M 0 222 R 222 0 R 0 -222 R -222 0 R F +20 setlinewidth 2674 10499 M 49 0 R -24 0 R 0 360 R -25 0 R 49 0 R D +3326 10876 M 49 0 R -24 0 R 0 283 R -25 0 R 49 0 R D 3978 10670 M 49 0 R +-24 0 R 0 323 R -25 0 R 49 0 R D 4630 10025 M 49 0 R -24 0 R 0 481 R -25 0 R +49 0 R D 5282 9859 M 49 0 R -24 0 R 0 532 R -25 0 R 49 0 R D 5934 7883 M +49 0 R -24 0 R 0 1553 R -25 0 R 49 0 R D 2553 6960 M 0 178 R 178 0 R +0 -178 R -178 0 R F +gsave 2908 6944 translate 0 0 M 0.8 dup scale +(z = 1.2 - 1.8 \(W03\)) show grestore 0.000 0.514 1.000 setrgbcolor +2553 7373 M 0 178 R 178 0 R 0 -178 R -178 0 R F +0.000 0.000 0.000 setrgbcolor gsave 2908 7356 translate 0 0 M 0.8 dup scale +(z = 1.39 \(R05\)) show grestore 10 setlinewidth +0.000 0.514 1.000 setrgbcolor 2553 7786 M 0 178 R 178 0 R 0 -178 R -178 0 R +D 0.000 0.000 0.000 setrgbcolor gsave 2908 7769 translate 0 0 M +0.8 dup scale +(z = 1.67 \(R05\)) show grestore 0.000 0.514 1.000 setrgbcolor 5636 9410 M +0 222 R 222 0 R 0 -222 R -222 0 R F +5473 9359 M 0 222 R 222 0 R 0 -222 R -222 0 R F +5310 9687 M 0 222 R 222 0 R 0 -222 R -222 0 R F +5147 10110 M 0 222 R 222 0 R 0 -222 R -222 0 R F +4984 10232 M 0 222 R 222 0 R 0 -222 R -222 0 R F +4821 10342 M 0 222 R 222 0 R 0 -222 R -222 0 R F +4658 10558 M 0 222 R 222 0 R 0 -222 R -222 0 R F +4495 10755 M 0 222 R 222 0 R 0 -222 R -222 0 R F +4332 10774 M 0 222 R 222 0 R 0 -222 R -222 0 R F +4169 10841 M 0 222 R 222 0 R 0 -222 R -222 0 R F +4006 11095 M 0 222 R 222 0 R 0 -222 R -222 0 R F +5962 8635 M 0 222 R 222 0 R 0 -222 R -222 0 R F +5799 8820 M 0 222 R 222 0 R 0 -222 R -222 0 R F +3843 11061 M 0 222 R 222 0 R 0 -222 R -222 0 R F +3680 10975 M 0 222 R 222 0 R 0 -222 R -222 0 R F +3517 10816 M 0 222 R 222 0 R 0 -222 R -222 0 R F +20 setlinewidth 6048 8321 M 49 0 R -24 0 R 0 690 R -25 0 R 49 0 R D +5885 8640 M 49 0 R -24 0 R 0 497 R -25 0 R 49 0 R D 5722 9340 M 49 0 R +-24 0 R 0 326 R -25 0 R 49 0 R D 5559 9277 M 49 0 R -24 0 R 0 345 R -25 0 R +49 0 R D 5396 9641 M 49 0 R -24 0 R 0 285 R -25 0 R 49 0 R D 5233 10102 M +49 0 R -24 0 R 0 221 R -25 0 R 49 0 R D 5070 10227 M 49 0 R -24 0 R 0 216 R +-25 0 R 49 0 R D 4907 10341 M 49 0 R -24 0 R 0 209 R -25 0 R 49 0 R D +4744 10567 M 49 0 R -24 0 R 0 192 R -25 0 R 49 0 R D 4581 10778 M 49 0 R +-24 0 R 0 166 R -25 0 R 49 0 R D 4418 10803 M 49 0 R -24 0 R 0 155 R -25 0 R +49 0 R D 4255 10874 M 50 0 R -25 0 R 0 148 R -25 0 R 50 0 R D 4092 11134 M +50 0 R -25 0 R 0 137 R -25 0 R 50 0 R D 3929 11093 M 50 0 R -25 0 R 0 150 R +-25 0 R 50 0 R D 3766 10978 M 50 0 R -25 0 R 0 202 R -25 0 R 50 0 R D +3603 10614 M 50 0 R -25 0 R 0 530 R -25 0 R 50 0 R D 10 setlinewidth +5962 9031 M 0 222 R 222 0 R 0 -222 R -222 0 R D 5799 9463 M 0 222 R 222 0 R +0 -222 R -222 0 R D 5636 9786 M 0 222 R 222 0 R 0 -222 R -222 0 R D +5473 10037 M 0 222 R 222 0 R 0 -222 R -222 0 R D 5310 10274 M 0 222 R +222 0 R 0 -222 R -222 0 R D 5147 10375 M 0 222 R 222 0 R 0 -222 R -222 0 R D +4984 10462 M 0 222 R 222 0 R 0 -222 R -222 0 R D 4821 10540 M 0 222 R +222 0 R 0 -222 R -222 0 R D 4658 10720 M 0 222 R 222 0 R 0 -222 R -222 0 R D +4495 10956 M 0 222 R 222 0 R 0 -222 R -222 0 R D 4332 10893 M 0 222 R +222 0 R 0 -222 R -222 0 R D 4169 11150 M 0 222 R 222 0 R 0 -222 R -222 0 R D +6451 9352 M 0 222 R 222 0 R 0 -222 R -222 0 R D 6288 8597 M 0 222 R 222 0 R +0 -222 R -222 0 R D 6125 8356 M 0 222 R 222 0 R 0 -222 R -222 0 R D +4006 11096 M 0 222 R 222 0 R 0 -222 R -222 0 R D 3843 11152 M 0 222 R +222 0 R 0 -222 R -222 0 R D 20 setlinewidth 6562 6705 M 0 3256 R -25 0 R +49 0 R D 6374 8211 M 49 0 R -24 0 R 0 789 R -25 0 R 49 0 R D 6211 8042 M +49 0 R -24 0 R 0 690 R -25 0 R 49 0 R D 6048 8910 M 49 0 R -24 0 R 0 408 R +-25 0 R 49 0 R D 5885 9406 M 49 0 R -24 0 R 0 304 R -25 0 R 49 0 R D +5722 9762 M 49 0 R -24 0 R 0 248 R -25 0 R 49 0 R D 5559 10031 M 49 0 R +-24 0 R 0 218 R -25 0 R 49 0 R D 5396 10279 M 49 0 R -24 0 R 0 199 R -25 0 R +49 0 R D 5233 10383 M 49 0 R -24 0 R 0 193 R -25 0 R 49 0 R D 5070 10471 M +49 0 R -24 0 R 0 192 R -25 0 R 49 0 R D 4907 10552 M 49 0 R -24 0 R 0 186 R +-25 0 R 49 0 R D 4744 10749 M 49 0 R -24 0 R 0 156 R -25 0 R 49 0 R D +4581 11000 M 49 0 R -24 0 R 0 129 R -25 0 R 49 0 R D 4418 10929 M 49 0 R +-24 0 R 0 142 R -25 0 R 49 0 R D 4255 11195 M 50 0 R -25 0 R 0 126 R -25 0 R +50 0 R D 4092 11125 M 50 0 R -25 0 R 0 155 R -25 0 R 50 0 R D 3929 11085 M +50 0 R -25 0 R 0 320 R -25 0 R 50 0 R D L2 0.000 0.000 0.000 setrgbcolor +2242 11540 M 10 0 R 90 -10 R 90 -12 R 90 -14 R 89 -17 R 90 -18 R 89 -21 R +89 -23 R 89 -25 R 89 -27 R 88 -29 R 89 -32 R 88 -33 R 88 -36 R 88 -37 R +88 -40 R 87 -42 R 88 -44 R 87 -47 R 87 -48 R 87 -51 R 87 -52 R 87 -55 R +86 -57 R 87 -59 R 86 -61 R 87 -63 R 86 -66 R 86 -67 R 86 -70 R 85 -71 R +86 -74 R 86 -76 R 85 -78 R 85 -81 R 86 -82 R 85 -84 R 85 -87 R 85 -89 R +85 -90 R 84 -93 R 85 -95 R 85 -97 R 84 -100 R 85 -101 R 84 -103 R 85 -106 R +84 -108 R 84 -110 R 84 -111 R 84 -115 R 84 -116 R 84 -118 R 84 -120 R +84 -123 R 84 -124 R 84 -127 R 84 -129 R 28 -45 R D L0 2242 11540 M 10 0 R +90 -10 R 90 -12 R 90 -14 R 89 -17 R 90 -18 R 89 -21 R 89 -23 R 89 -25 R +89 -27 R 88 -29 R 89 -32 R 88 -33 R 88 -36 R 88 -37 R 88 -40 R 87 -42 R +88 -44 R 87 -47 R 87 -48 R 87 -51 R 87 -52 R 87 -55 R 86 -57 R 87 -59 R +86 -61 R 87 -63 R 86 -66 R 86 -67 R 86 -70 R 85 -71 R 86 -74 R 86 -76 R +85 -78 R 85 -81 R 86 -82 R 85 -84 R 85 -87 R 85 -89 R 85 -90 R 84 -93 R +85 -95 R 85 -97 R 84 -100 R 85 -101 R 84 -103 R 85 -106 R 84 -108 R +84 -110 R 84 -111 R 84 -115 R 84 -116 R 84 -118 R 84 -120 R 84 -123 R +84 -124 R 84 -127 R 84 -129 R 28 -45 R D L2 2242 11519 M 10 1 R 90 1 R +90 -1 R 90 -4 R 89 -5 R 90 -8 R 89 -10 R 89 -12 R 89 -14 R 89 -17 R 88 -18 R +89 -21 R 88 -22 R 88 -25 R 88 -27 R 88 -29 R 87 -31 R 88 -34 R 87 -35 R +87 -38 R 87 -40 R 87 -41 R 87 -44 R 86 -47 R 87 -48 R 86 -50 R 87 -53 R +86 -54 R 86 -57 R 86 -59 R 85 -61 R 86 -63 R 86 -65 R 85 -67 R 85 -70 R +86 -71 R 85 -74 R 85 -76 R 85 -78 R 85 -80 R 84 -82 R 85 -84 R 85 -87 R +84 -88 R 85 -91 R 84 -93 R 85 -95 R 84 -97 R 84 -99 R 84 -101 R 84 -103 R +84 -106 R 84 -107 R 84 -110 R 84 -112 R 84 -114 R 84 -116 R 84 -118 R +28 -41 R D L0 2242 11519 M 10 1 R 90 1 R 90 -1 R 90 -4 R 89 -5 R 90 -8 R +89 -10 R 89 -12 R 89 -14 R 89 -17 R 88 -18 R 89 -21 R 88 -22 R 88 -25 R +88 -27 R 88 -29 R 87 -31 R 88 -34 R 87 -35 R 87 -38 R 87 -40 R 87 -41 R +87 -44 R 86 -47 R 87 -48 R 86 -50 R 87 -53 R 86 -54 R 86 -57 R 86 -59 R +85 -61 R 86 -63 R 86 -65 R 85 -67 R 85 -70 R 86 -71 R 85 -74 R 85 -76 R +85 -78 R 85 -80 R 84 -82 R 85 -84 R 85 -87 R 84 -88 R 85 -91 R 84 -93 R +85 -95 R 84 -97 R 84 -99 R 84 -101 R 84 -103 R 84 -106 R 84 -107 R 84 -110 R +84 -112 R 84 -114 R 84 -116 R 84 -118 R 28 -41 R D 15 setlinewidth +7197 6706 M 4955 0 R D 8175 6706 M 0 105 R D gsave 8175 6172 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 9479 6706 M 0 105 R D gsave 9479 6172 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 10783 6706 M 0 105 R D gsave 10783 6172 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 12087 6706 M 0 105 R D gsave 12087 6172 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 7197 6706 M 0 52 R D 7523 6706 M 0 52 R D 7849 6706 M +0 52 R D 8501 6706 M 0 52 R D 8827 6706 M 0 52 R D 9153 6706 M 0 52 R D +9805 6706 M 0 52 R D 10131 6706 M 0 52 R D 10457 6706 M 0 52 R D +11109 6706 M 0 52 R D 11435 6706 M 0 52 R D 11761 6706 M 0 52 R D +7197 11989 M 4955 0 R D 8175 11989 M 0 -106 R D 9479 11989 M 0 -106 R D +10783 11989 M 0 -106 R D 12087 11989 M 0 -106 R D 7197 11989 M 0 -53 R D +7523 11989 M 0 -53 R D 7849 11989 M 0 -53 R D 8501 11989 M 0 -53 R D +8827 11989 M 0 -53 R D 9153 11989 M 0 -53 R D 9805 11989 M 0 -53 R D +10131 11989 M 0 -53 R D 10457 11989 M 0 -53 R D 11109 11989 M 0 -53 R D +11435 11989 M 0 -53 R D 11761 11989 M 0 -53 R D 7197 6706 M 0 5283 R D +7197 7036 M 99 0 R D gsave 7085 6894 translate 0 0 M 1.01 dup scale +-117.687 0 N +( ) show grestore 7197 8687 M 99 0 R D gsave 7085 8545 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 10338 M 99 0 R D gsave 7085 10196 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 11989 M 99 0 R D gsave 7085 11740 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 6706 M 50 0 R D 7197 6871 M 50 0 R D 7197 7201 M +50 0 R D 7197 7366 M 50 0 R D 7197 7531 M 50 0 R D 7197 7696 M 50 0 R D +7197 7861 M 50 0 R D 7197 8026 M 50 0 R D 7197 8192 M 50 0 R D 7197 8357 M +50 0 R D 7197 8522 M 50 0 R D 7197 8852 M 50 0 R D 7197 9017 M 50 0 R D +7197 9182 M 50 0 R D 7197 9347 M 50 0 R D 7197 9512 M 50 0 R D 7197 9678 M +50 0 R D 7197 9843 M 50 0 R D 7197 10008 M 50 0 R D 7197 10173 M 50 0 R D +7197 10503 M 50 0 R D 7197 10668 M 50 0 R D 7197 10833 M 50 0 R D +7197 10998 M 50 0 R D 7197 11163 M 50 0 R D 7197 11329 M 50 0 R D +7197 11494 M 50 0 R D 7197 11659 M 50 0 R D 7197 11824 M 50 0 R D +12152 6706 M 0 5283 R D 12152 7036 M -99 0 R D 12152 8687 M -99 0 R D +12152 10338 M -99 0 R D 12152 11989 M -99 0 R D 12152 6706 M -49 0 R D +12152 6871 M -49 0 R D 12152 7201 M -49 0 R D 12152 7366 M -49 0 R D +12152 7531 M -49 0 R D 12152 7696 M -49 0 R D 12152 7861 M -49 0 R D +12152 8026 M -49 0 R D 12152 8192 M -49 0 R D 12152 8357 M -49 0 R D +12152 8522 M -49 0 R D 12152 8852 M -49 0 R D 12152 9017 M -49 0 R D +12152 9182 M -49 0 R D 12152 9347 M -49 0 R D 12152 9512 M -49 0 R D +12152 9678 M -49 0 R D 12152 9843 M -49 0 R D 12152 10008 M -49 0 R D +12152 10173 M -49 0 R D 12152 10503 M -49 0 R D 12152 10668 M -49 0 R D +12152 10833 M -49 0 R D 12152 10998 M -49 0 R D 12152 11163 M -49 0 R D +12152 11329 M -49 0 R D 12152 11494 M -49 0 R D 12152 11659 M -49 0 R D +12152 11824 M -49 0 R D 7543 11003 M 0 222 R 222 0 R 0 -222 R -222 0 R F +8195 11284 M 0 222 R 222 0 R 0 -222 R -222 0 R F +8847 10887 M 0 222 R 222 0 R 0 -222 R -222 0 R F +9499 10475 M 0 222 R 222 0 R 0 -222 R -222 0 R F +10151 9979 M 0 222 R 222 0 R 0 -222 R -222 0 R F +10803 8824 M 0 222 R 222 0 R 0 -222 R -222 0 R F +20 setlinewidth 7629 10968 M 49 0 R -24 0 R 0 267 R -25 0 R 49 0 R D +8281 11277 M 49 0 R -24 0 R 0 219 R -25 0 R 49 0 R D 8933 10839 M 49 0 R +-24 0 R 0 290 R -25 0 R 49 0 R D 9585 10364 M 49 0 R -24 0 R 0 391 R -25 0 R +49 0 R D 10237 9752 M 49 0 R -24 0 R 0 567 R -25 0 R 49 0 R D 10889 7614 M +49 0 R -24 0 R 0 1758 R -25 0 R 49 0 R D 0.000 1.000 0.580 setrgbcolor +9805 11552 M -40 -126 R -132 0 R 106 -77 R -40 -125 R 106 77 R 107 -77 R +-41 125 R 107 77 R -132 0 R -41 126 R F +10457 11126 M -40 -126 R -132 0 R 106 -77 R -40 -125 R 106 77 R 107 -77 R +-41 125 R 107 77 R -132 0 R -41 126 R F +11109 9639 M -40 -125 R -132 0 R 106 -78 R -40 -125 R 106 77 R 107 -77 R +-41 125 R 107 78 R -132 0 R -41 125 R F +11761 7567 M -41 -125 R -131 0 R 106 -77 R -40 -126 R 106 78 R 107 -78 R +-41 126 R 107 77 R -132 0 R -41 125 R F +9780 11197 M 50 0 R -25 0 R 0 313 R -25 0 R 50 0 R D 10432 10735 M 50 0 R +-25 0 R 0 371 R -25 0 R 50 0 R D 11084 9356 M 50 0 R -25 0 R 0 191 R -25 0 R +50 0 R D 11736 6891 M 50 0 R -25 0 R 0 786 R -25 0 R 50 0 R D +0.000 0.000 0.000 setrgbcolor 7508 6960 M 0 178 R 178 0 R 0 -178 R -178 0 R +F +gsave 7863 6944 translate 0 0 M 0.8 dup scale +(z = 1.8 - 2.4 \(W03\)) show grestore 0.000 0.514 1.000 setrgbcolor +7508 7373 M 0 178 R 178 0 R 0 -178 R -178 0 R F +0.000 0.000 0.000 setrgbcolor gsave 7863 7356 translate 0 0 M 0.8 dup scale +(z = 1.955 \(R05\)) show grestore 0.000 1.000 0.580 setrgbcolor 7597 8020 M +-33 -100 R -105 0 R 85 -62 R -32 -101 R 85 62 R 85 -62 R -32 101 R 85 62 R +-106 0 R -32 100 R F +0.000 0.000 0.000 setrgbcolor gsave 7863 7769 translate 0 0 M 0.8 dup scale +(z = 2.0 - 2.2 \(WHO\)) show grestore 0.000 0.514 1.000 setrgbcolor +11243 8915 M 0 222 R 222 0 R 0 -222 R -222 0 R F +11080 9249 M 0 222 R 222 0 R 0 -222 R -222 0 R F +10917 9544 M 0 222 R 222 0 R 0 -222 R -222 0 R F +10754 9752 M 0 222 R 222 0 R 0 -222 R -222 0 R F +10591 9856 M 0 222 R 222 0 R 0 -222 R -222 0 R F +10428 10096 M 0 222 R 222 0 R 0 -222 R -222 0 R F +10265 10310 M 0 222 R 222 0 R 0 -222 R -222 0 R F +10102 10537 M 0 222 R 222 0 R 0 -222 R -222 0 R F +9939 10517 M 0 222 R 222 0 R 0 -222 R -222 0 R F +9776 10779 M 0 222 R 222 0 R 0 -222 R -222 0 R F +9613 10871 M 0 222 R 222 0 R 0 -222 R -222 0 R F +9450 10880 M 0 222 R 222 0 R 0 -222 R -222 0 R F +11569 7891 M 0 222 R 222 0 R 0 -222 R -222 0 R F +11406 8543 M 0 222 R 222 0 R 0 -222 R -222 0 R F +9287 11016 M 0 222 R 222 0 R 0 -222 R -222 0 R F +9124 10968 M 0 222 R 222 0 R 0 -222 R -222 0 R F +8961 11317 M 0 222 R 222 0 R 0 -222 R -222 0 R F +11680 6705 M 0 1794 R -25 0 R 49 0 R D 11492 8314 M 49 0 R -24 0 R 0 571 R +-25 0 R 49 0 R D 11329 8782 M 49 0 R -24 0 R 0 426 R -25 0 R 49 0 R D +11166 9173 M 49 0 R -24 0 R 0 335 R -25 0 R 49 0 R D 11003 9502 M 49 0 R +-24 0 R 0 279 R -25 0 R 49 0 R D 10840 9726 M 49 0 R -24 0 R 0 253 R -25 0 R +49 0 R D 10677 9832 M 50 0 R -25 0 R 0 249 R -25 0 R 50 0 R D 10514 10088 M +50 0 R -25 0 R 0 221 R -25 0 R 50 0 R D 10351 10315 M 50 0 R -25 0 R 0 198 R +-25 0 R 50 0 R D 10188 10553 M 50 0 R -25 0 R 0 180 R -25 0 R 50 0 R D +10025 10533 M 50 0 R -25 0 R 0 178 R -25 0 R 50 0 R D 9862 10816 M 50 0 R +-25 0 R 0 140 R -25 0 R 50 0 R D 9699 10911 M 50 0 R -25 0 R 0 135 R -25 0 R +50 0 R D 9536 10918 M 50 0 R -25 0 R 0 140 R -25 0 R 50 0 R D 9373 11057 M +50 0 R -25 0 R 0 134 R -25 0 R 50 0 R D 9210 10965 M 50 0 R -25 0 R 0 213 R +-25 0 R 50 0 R D 9047 10548 M 50 0 R -25 0 R 0 1264 R -25 0 R 50 0 R D L2 +0.000 0.000 0.000 setrgbcolor 7197 11519 M 10 1 R 90 1 R 90 -1 R 90 -4 R +89 -5 R 90 -8 R 89 -10 R 89 -12 R 89 -14 R 89 -17 R 88 -18 R 89 -21 R +88 -22 R 88 -25 R 88 -27 R 88 -29 R 87 -31 R 88 -34 R 87 -35 R 87 -38 R +87 -40 R 87 -41 R 87 -44 R 87 -47 R 86 -48 R 86 -50 R 87 -53 R 86 -54 R +86 -57 R 86 -59 R 85 -61 R 86 -63 R 86 -65 R 85 -67 R 85 -70 R 86 -71 R +85 -74 R 85 -76 R 85 -78 R 85 -80 R 84 -82 R 85 -84 R 85 -87 R 84 -88 R +85 -91 R 84 -93 R 85 -95 R 84 -97 R 84 -99 R 84 -101 R 84 -103 R 84 -106 R +84 -107 R 84 -110 R 84 -112 R 84 -114 R 84 -116 R 84 -118 R 28 -41 R D L0 +7197 11519 M 10 1 R 90 1 R 90 -1 R 90 -4 R 89 -5 R 90 -8 R 89 -10 R 89 -12 R +89 -14 R 89 -17 R 88 -18 R 89 -21 R 88 -22 R 88 -25 R 88 -27 R 88 -29 R +87 -31 R 88 -34 R 87 -35 R 87 -38 R 87 -40 R 87 -41 R 87 -44 R 87 -47 R +86 -48 R 86 -50 R 87 -53 R 86 -54 R 86 -57 R 86 -59 R 85 -61 R 86 -63 R +86 -65 R 85 -67 R 85 -70 R 86 -71 R 85 -74 R 85 -76 R 85 -78 R 85 -80 R +84 -82 R 85 -84 R 85 -87 R 84 -88 R 85 -91 R 84 -93 R 85 -95 R 84 -97 R +84 -99 R 84 -101 R 84 -103 R 84 -106 R 84 -107 R 84 -110 R 84 -112 R +84 -114 R 84 -116 R 84 -118 R 28 -41 R D L2 7197 11051 M 10 1 R 90 8 R +90 5 R 90 3 R 89 0 R 90 -1 R 89 -3 R 89 -6 R 89 -7 R 89 -10 R 88 -12 R +89 -14 R 88 -16 R 88 -19 R 88 -20 R 88 -23 R 87 -25 R 88 -26 R 87 -29 R +87 -32 R 87 -33 R 87 -35 R 87 -38 R 87 -39 R 86 -42 R 86 -44 R 87 -46 R +86 -48 R 86 -50 R 86 -53 R 85 -54 R 86 -57 R 86 -59 R 85 -61 R 85 -63 R +86 -65 R 85 -67 R 85 -69 R 85 -72 R 85 -73 R 84 -76 R 85 -78 R 85 -80 R +84 -82 R 85 -84 R 84 -87 R 85 -88 R 84 -91 R 84 -92 R 84 -95 R 84 -97 R +84 -99 R 84 -101 R 84 -103 R 84 -106 R 84 -107 R 84 -110 R 84 -111 R +28 -39 R D L0 7197 11531 M 10 0 R 90 -2 R 90 -4 R 90 -7 R 89 -8 R 90 -11 R +89 -12 R 89 -15 R 89 -17 R 89 -19 R 88 -22 R 89 -23 R 88 -25 R 88 -28 R +88 -30 R 88 -32 R 87 -34 R 88 -36 R 87 -38 R 87 -40 R 87 -43 R 87 -45 R +87 -46 R 87 -49 R 86 -51 R 86 -53 R 87 -56 R 86 -57 R 86 -60 R 86 -61 R +85 -64 R 86 -66 R 86 -68 R 85 -70 R 85 -72 R 86 -75 R 85 -76 R 85 -79 R +85 -80 R 85 -83 R 84 -85 R 85 -87 R 85 -89 R 84 -92 R 85 -93 R 84 -96 R +85 -97 R 84 -100 R 84 -102 R 84 -104 R 84 -106 R 84 -108 R 84 -110 R +84 -113 R 84 -114 R 84 -117 R 84 -119 R 84 -121 R 28 -42 R D 15 setlinewidth +12152 6706 M 4955 0 R D 13130 6706 M 0 105 R D +gsave 13130 6172 translate 0 0 M 1.01 dup scale -58.8433 0 N +( ) show grestore 14434 6706 M 0 105 R D gsave 14434 6172 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 15738 6706 M 0 105 R D gsave 15738 6172 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 17042 6706 M 0 105 R D gsave 17042 6172 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 12152 6706 M 0 52 R D 12478 6706 M 0 52 R D 12804 6706 M +0 52 R D 13456 6706 M 0 52 R D 13782 6706 M 0 52 R D 14108 6706 M 0 52 R D +14760 6706 M 0 52 R D 15086 6706 M 0 52 R D 15412 6706 M 0 52 R D +16064 6706 M 0 52 R D 16390 6706 M 0 52 R D 16716 6706 M 0 52 R D +12152 11989 M 4955 0 R D 13130 11989 M 0 -106 R D 14434 11989 M 0 -106 R D +15738 11989 M 0 -106 R D 17042 11989 M 0 -106 R D 12152 11989 M 0 -53 R D +12478 11989 M 0 -53 R D 12804 11989 M 0 -53 R D 13456 11989 M 0 -53 R D +13782 11989 M 0 -53 R D 14108 11989 M 0 -53 R D 14760 11989 M 0 -53 R D +15086 11989 M 0 -53 R D 15412 11989 M 0 -53 R D 16064 11989 M 0 -53 R D +16390 11989 M 0 -53 R D 16716 11989 M 0 -53 R D 12152 6706 M 0 5283 R D +12152 7036 M 99 0 R D gsave 12040 6894 translate 0 0 M 1.01 dup scale +-117.687 0 N +( ) show grestore 12152 8687 M 99 0 R D gsave 12040 8545 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 10338 M 99 0 R D gsave 12040 10196 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 11989 M 99 0 R D gsave 12040 11740 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 6706 M 50 0 R D 12152 6871 M 50 0 R D 12152 7201 M +50 0 R D 12152 7366 M 50 0 R D 12152 7531 M 50 0 R D 12152 7696 M 50 0 R D +12152 7861 M 50 0 R D 12152 8026 M 50 0 R D 12152 8192 M 50 0 R D +12152 8357 M 50 0 R D 12152 8522 M 50 0 R D 12152 8852 M 50 0 R D +12152 9017 M 50 0 R D 12152 9182 M 50 0 R D 12152 9347 M 50 0 R D +12152 9512 M 50 0 R D 12152 9678 M 50 0 R D 12152 9843 M 50 0 R D +12152 10008 M 50 0 R D 12152 10173 M 50 0 R D 12152 10503 M 50 0 R D +12152 10668 M 50 0 R D 12152 10833 M 50 0 R D 12152 10998 M 50 0 R D +12152 11163 M 50 0 R D 12152 11329 M 50 0 R D 12152 11494 M 50 0 R D +12152 11659 M 50 0 R D 12152 11824 M 50 0 R D 17107 6706 M 0 5283 R D +17107 7036 M -99 0 R D 17107 8687 M -99 0 R D 17107 10338 M -99 0 R D +17107 11989 M -99 0 R D 17107 6706 M -49 0 R D 17107 6871 M -49 0 R D +17107 7201 M -49 0 R D 17107 7366 M -49 0 R D 17107 7531 M -49 0 R D +17107 7696 M -49 0 R D 17107 7861 M -49 0 R D 17107 8026 M -49 0 R D +17107 8192 M -49 0 R D 17107 8357 M -49 0 R D 17107 8522 M -49 0 R D +17107 8852 M -49 0 R D 17107 9017 M -49 0 R D 17107 9182 M -49 0 R D +17107 9347 M -49 0 R D 17107 9512 M -49 0 R D 17107 9678 M -49 0 R D +17107 9843 M -49 0 R D 17107 10008 M -49 0 R D 17107 10173 M -49 0 R D +17107 10503 M -49 0 R D 17107 10668 M -49 0 R D 17107 10833 M -49 0 R D +17107 10998 M -49 0 R D 17107 11163 M -49 0 R D 17107 11329 M -49 0 R D +17107 11494 M -49 0 R D 17107 11659 M -49 0 R D 17107 11824 M -49 0 R D +13150 11185 M 0 222 R 222 0 R 0 -222 R -222 0 R F +13802 10739 M 0 222 R 222 0 R 0 -222 R -222 0 R F +14454 10210 M 0 222 R 222 0 R 0 -222 R -222 0 R F +15106 9600 M 0 222 R 222 0 R 0 -222 R -222 0 R F +15758 9600 M 0 222 R 222 0 R 0 -222 R -222 0 R F +20 setlinewidth 13236 11169 M 50 0 R -25 0 R 0 234 R -25 0 R 50 0 R D +13888 10670 M 50 0 R -25 0 R 0 323 R -25 0 R 50 0 R D 14540 10045 M 49 0 R +-24 0 R 0 475 R -25 0 R 49 0 R D 15192 9228 M 49 0 R -24 0 R 0 768 R -25 0 R +49 0 R D 15844 9228 M 49 0 R -24 0 R 0 768 R -25 0 R 49 0 R D +0.000 1.000 0.580 setrgbcolor 14760 11942 M -40 -126 R -132 0 R 106 -77 R +-40 -125 R 106 77 R 107 -77 R -41 125 R 107 77 R -132 0 R -41 126 R F +15412 10870 M -40 -126 R -132 0 R 106 -77 R -40 -125 R 106 77 R 107 -77 R +-41 125 R 107 77 R -132 0 R -41 126 R F +16064 10156 M -40 -125 R -132 0 R 106 -77 R -40 -125 R 106 77 R 107 -77 R +-41 125 R 107 77 R -132 0 R -41 125 R F +16716 7545 M -40 -125 R -132 0 R 106 -78 R -40 -125 R 106 78 R 107 -78 R +-41 125 R 107 78 R -132 0 R -41 125 R F +14736 11288 M 49 0 R -25 0 R 0 701 R D 15388 10491 M 49 0 R -25 0 R 0 352 R +-24 0 R 49 0 R D 16039 9753 M 50 0 R -25 0 R 0 392 R -25 0 R 50 0 R D +16691 7059 M 50 0 R -25 0 R 0 518 R -25 0 R 50 0 R D +0.000 0.000 0.000 setrgbcolor 12463 6960 M 0 178 R 178 0 R 0 -178 R -178 0 R +F +gsave 12818 6944 translate 0 0 M 0.8 dup scale +(z = 2.4 - 3.0 \(W03\)) show grestore 0.000 1.000 0.580 setrgbcolor +12552 7607 M -33 -100 R -105 0 R 85 -62 R -32 -100 R 85 62 R 85 -62 R +-32 100 R 85 62 R -105 0 R -33 100 R F +0.000 0.000 0.000 setrgbcolor gsave 12818 7356 translate 0 0 M 0.8 dup scale +(z = 2.2 - 3.0 \(WHO\)) show grestore L2 12152 11051 M 10 1 R 90 8 R 90 5 R +90 3 R 89 0 R 90 -1 R 89 -3 R 89 -6 R 89 -7 R 89 -10 R 88 -12 R 89 -14 R +88 -16 R 88 -19 R 88 -20 R 88 -23 R 87 -25 R 88 -26 R 87 -29 R 87 -32 R +87 -33 R 87 -35 R 87 -38 R 87 -39 R 86 -42 R 86 -44 R 87 -46 R 86 -48 R +86 -50 R 86 -53 R 85 -54 R 86 -57 R 86 -59 R 85 -61 R 85 -63 R 86 -65 R +85 -67 R 85 -69 R 85 -72 R 85 -73 R 84 -76 R 85 -78 R 85 -80 R 84 -82 R +85 -84 R 84 -87 R 85 -88 R 84 -91 R 84 -92 R 84 -95 R 84 -97 R 84 -99 R +84 -101 R 84 -103 R 84 -106 R 84 -107 R 84 -110 R 84 -111 R 28 -39 R D L0 +12152 11531 M 10 0 R 90 -2 R 90 -4 R 90 -7 R 89 -8 R 90 -11 R 89 -12 R +89 -15 R 89 -17 R 89 -19 R 88 -22 R 89 -23 R 88 -25 R 88 -28 R 88 -30 R +88 -32 R 87 -34 R 88 -36 R 87 -38 R 87 -40 R 87 -43 R 87 -45 R 87 -46 R +87 -49 R 86 -51 R 86 -53 R 87 -56 R 86 -57 R 86 -60 R 86 -61 R 85 -64 R +86 -66 R 86 -68 R 85 -70 R 85 -72 R 86 -75 R 85 -76 R 85 -79 R 85 -80 R +85 -83 R 84 -85 R 85 -87 R 85 -89 R 84 -92 R 85 -93 R 84 -96 R 85 -97 R +84 -100 R 84 -102 R 84 -104 R 84 -106 R 84 -108 R 84 -110 R 84 -113 R +84 -114 R 84 -117 R 84 -119 R 84 -121 R 28 -42 R D L2 12152 10370 M 10 2 R +90 12 R 90 9 R 90 7 R 89 6 R 90 3 R 89 0 R 89 -1 R 89 -3 R 89 -6 R 88 -8 R +89 -10 R 88 -12 R 88 -14 R 88 -16 R 88 -18 R 87 -21 R 88 -23 R 87 -24 R +87 -27 R 87 -29 R 87 -31 R 87 -34 R 87 -35 R 86 -38 R 86 -39 R 87 -42 R +86 -44 R 86 -46 R 86 -48 R 85 -51 R 86 -52 R 86 -55 R 85 -56 R 85 -59 R +86 -61 R 85 -63 R 85 -65 R 85 -67 R 85 -70 R 84 -71 R 85 -74 R 85 -76 R +84 -78 R 85 -80 R 84 -82 R 85 -84 R 84 -87 R 84 -88 R 84 -91 R 84 -92 R +84 -95 R 84 -97 R 84 -99 R 84 -101 R 84 -104 R 84 -105 R 84 -108 R 28 -37 R +D L0 12152 11539 M 10 0 R 90 -12 R 90 -14 R 90 -16 R 89 -18 R 90 -21 R +89 -22 R 89 -24 R 89 -27 R 89 -29 R 88 -31 R 89 -33 R 88 -35 R 88 -37 R +88 -40 R 88 -41 R 87 -44 R 88 -46 R 87 -48 R 87 -50 R 87 -52 R 87 -54 R +87 -57 R 87 -58 R 86 -61 R 86 -63 R 87 -65 R 86 -67 R 86 -69 R 86 -71 R +85 -74 R 86 -75 R 86 -78 R 85 -80 R 85 -82 R 86 -84 R 85 -86 R 85 -88 R +85 -90 R 85 -93 R 84 -94 R 85 -97 R 85 -99 R 84 -101 R 85 -103 R 84 -105 R +85 -107 R 84 -110 R 84 -111 R 84 -114 R 84 -115 R 84 -118 R 84 -120 R +84 -122 R 84 -124 R 84 -126 R 84 -129 R 84 -130 R 28 -45 R D 15 setlinewidth +2242 1422 M 4955 0 R D 3220 1422 M 0 106 R D gsave 3220 889 translate 0 0 M +1.01 dup scale -305.858 0 N +(-22) show grestore 4524 1422 M 0 106 R D gsave 4524 889 translate 0 0 M +1.01 dup scale -305.858 0 N +(-24) show grestore 5828 1422 M 0 106 R D gsave 5828 889 translate 0 0 M +1.01 dup scale -305.858 0 N +(-26) show grestore 7132 1422 M 0 106 R D gsave 7132 889 translate 0 0 M +1.01 dup scale -305.858 0 N +(-28) show grestore 2242 1422 M 0 53 R D 2568 1422 M 0 53 R D 2894 1422 M +0 53 R D 3546 1422 M 0 53 R D 3872 1422 M 0 53 R D 4198 1422 M 0 53 R D +4850 1422 M 0 53 R D 5176 1422 M 0 53 R D 5502 1422 M 0 53 R D 6154 1422 M +0 53 R D 6480 1422 M 0 53 R D 6806 1422 M 0 53 R D 2242 6706 M 4955 0 R D +3220 6706 M 0 -106 R D 4524 6706 M 0 -106 R D 5828 6706 M 0 -106 R D +7132 6706 M 0 -106 R D 2242 6706 M 0 -53 R D 2568 6706 M 0 -53 R D +2894 6706 M 0 -53 R D 3546 6706 M 0 -53 R D 3872 6706 M 0 -53 R D +4198 6706 M 0 -53 R D 4850 6706 M 0 -53 R D 5176 6706 M 0 -53 R D +5502 6706 M 0 -53 R D 6154 6706 M 0 -53 R D 6480 6706 M 0 -53 R D +6806 6706 M 0 -53 R D 2242 1422 M 0 5284 R D 2242 2100 M 99 0 R D +gsave 2130 1957 translate 0 0 M 1.01 dup scale -376.343 0 N +(-9) show grestore 2242 3454 M 99 0 R D gsave 2130 3312 translate 0 0 M +1.01 dup scale -376.343 0 N +(-8) show grestore 2242 4809 M 99 0 R D gsave 2130 4667 translate 0 0 M +1.01 dup scale -376.343 0 N +(-7) show grestore 2242 6164 M 99 0 R D gsave 2130 6021 translate 0 0 M +1.01 dup scale -376.343 0 N +(-6) show grestore 2242 1422 M 50 0 R D 2242 1558 M 50 0 R D 2242 1693 M +50 0 R D 2242 1829 M 50 0 R D 2242 1964 M 50 0 R D 2242 2235 M 50 0 R D +2242 2370 M 50 0 R D 2242 2506 M 50 0 R D 2242 2641 M 50 0 R D 2242 2777 M +50 0 R D 2242 2912 M 50 0 R D 2242 3048 M 50 0 R D 2242 3183 M 50 0 R D +2242 3319 M 50 0 R D 2242 3590 M 50 0 R D 2242 3725 M 50 0 R D 2242 3861 M +50 0 R D 2242 3996 M 50 0 R D 2242 4132 M 50 0 R D 2242 4267 M 50 0 R D +2242 4403 M 50 0 R D 2242 4538 M 50 0 R D 2242 4673 M 50 0 R D 2242 4944 M +50 0 R D 2242 5080 M 50 0 R D 2242 5215 M 50 0 R D 2242 5351 M 50 0 R D +2242 5486 M 50 0 R D 2242 5622 M 50 0 R D 2242 5757 M 50 0 R D 2242 5893 M +50 0 R D 2242 6028 M 50 0 R D 2242 6299 M 50 0 R D 2242 6435 M 50 0 R D +2242 6570 M 50 0 R D 2242 6706 M 50 0 R D 7197 1422 M 0 5284 R D 7197 2100 M +-99 0 R D 7197 3454 M -99 0 R D 7197 4809 M -99 0 R D 7197 6164 M -99 0 R D +7197 1422 M -49 0 R D 7197 1558 M -49 0 R D 7197 1693 M -49 0 R D +7197 1829 M -49 0 R D 7197 1964 M -49 0 R D 7197 2235 M -49 0 R D +7197 2370 M -49 0 R D 7197 2506 M -49 0 R D 7197 2641 M -49 0 R D +7197 2777 M -49 0 R D 7197 2912 M -49 0 R D 7197 3048 M -49 0 R D +7197 3183 M -49 0 R D 7197 3319 M -49 0 R D 7197 3590 M -49 0 R D +7197 3725 M -49 0 R D 7197 3861 M -49 0 R D 7197 3996 M -49 0 R D +7197 4132 M -49 0 R D 7197 4267 M -49 0 R D 7197 4403 M -49 0 R D +7197 4538 M -49 0 R D 7197 4673 M -49 0 R D 7197 4944 M -49 0 R D +7197 5080 M -49 0 R D 7197 5215 M -49 0 R D 7197 5351 M -49 0 R D +7197 5486 M -49 0 R D 7197 5622 M -49 0 R D 7197 5757 M -49 0 R D +7197 5893 M -49 0 R D 7197 6028 M -49 0 R D 7197 6299 M -49 0 R D +7197 6435 M -49 0 R D 7197 6570 M -49 0 R D 7197 6706 M -49 0 R D +3240 6256 M 0 222 R 222 0 R 0 -222 R -222 0 R F +3892 5917 M 0 222 R 222 0 R 0 -222 R -222 0 R F +4544 5565 M 0 222 R 222 0 R 0 -222 R -222 0 R F +5196 5565 M 0 222 R 222 0 R 0 -222 R -222 0 R F +20 setlinewidth 3326 6185 M 49 0 R -24 0 R 0 321 R -25 0 R 49 0 R D +3978 5770 M 49 0 R -24 0 R 0 437 R -25 0 R 49 0 R D 4630 5293 M 49 0 R +-24 0 R 0 613 R -25 0 R 49 0 R D 5282 5293 M 49 0 R -24 0 R 0 613 R -25 0 R +49 0 R D 0.000 1.000 0.580 setrgbcolor 5502 6599 M -41 -125 R -131 0 R +106 -78 R -40 -125 R 106 77 R 107 -77 R -41 125 R 107 78 R -132 0 R +-41 125 R F +6154 5934 M -41 -126 R -131 0 R 106 -77 R -40 -125 R 106 77 R 107 -77 R +-41 125 R 107 77 R -132 0 R -41 126 R F +6806 4892 M -41 -125 R -131 0 R 106 -78 R -40 -125 R 106 77 R 107 -77 R +-41 125 R 107 78 R -132 0 R -41 125 R F +5477 6201 M 50 0 R -25 0 R 0 375 R -25 0 R 50 0 R D 6129 5549 M 50 0 R +-25 0 R 0 354 R -25 0 R 50 0 R D 6781 4382 M 50 0 R -25 0 R 0 538 R -25 0 R +50 0 R D 0.000 0.000 0.000 setrgbcolor 2553 1694 M 0 178 R 178 0 R 0 -178 R +-178 0 R F +gsave 2908 1677 translate 0 0 M 0.8 dup scale +(z = 3.0 - 3.6 \(W03\)) show grestore 0.000 1.000 0.580 setrgbcolor +2642 2266 M -33 -100 R -105 0 R 85 -62 R -32 -100 R 85 62 R 85 -62 R +-32 100 R 85 62 R -106 0 R -32 100 R F +0.000 0.000 0.000 setrgbcolor gsave 2908 2016 translate 0 0 M 0.8 dup scale +(z = 3.0 - 3.5 \(WHO\)) show grestore gsave 1264 6841 translate 0 0 M +90 rotate 1.01 dup scale -2768.03 0 N +(Log\( d) show +%%IncludeResource: font Symbol +423.333 /Symbol STDFONT +(F) show +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( / dM) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(B) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( \) [Mpc) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(-3) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( mag) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(-1) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(]) show grestore L2 2242 6190 M 10 2 R 90 9 R 90 8 R 90 6 R 89 4 R 90 3 R +89 0 R 89 -1 R 89 -3 R 89 -4 R 88 -7 R 89 -8 R 88 -10 R 88 -11 R 88 -13 R +88 -16 R 87 -16 R 88 -19 R 87 -20 R 87 -22 R 87 -24 R 87 -26 R 87 -27 R +86 -29 R 87 -31 R 86 -32 R 87 -35 R 86 -36 R 86 -38 R 86 -39 R 85 -41 R +86 -43 R 86 -45 R 85 -47 R 85 -48 R 86 -50 R 85 -52 R 85 -53 R 85 -55 R +85 -57 R 84 -59 R 85 -60 R 85 -63 R 84 -64 R 85 -65 R 84 -68 R 85 -69 R +84 -71 R 84 -72 R 84 -74 R 84 -77 R 84 -77 R 84 -80 R 84 -81 R 84 -83 R +84 -85 R 84 -86 R 84 -89 R 28 -31 R D L0 3854 6705 M 81 -38 R 87 -43 R +87 -45 R 87 -46 R 86 -48 R 87 -50 R 86 -51 R 87 -54 R 86 -55 R 86 -56 R +86 -59 R 85 -60 R 86 -62 R 86 -64 R 85 -65 R 85 -67 R 86 -69 R 85 -71 R +85 -72 R 85 -74 R 85 -76 R 84 -78 R 85 -79 R 85 -81 R 84 -83 R 85 -85 R +84 -86 R 85 -88 R 84 -90 R 84 -91 R 84 -93 R 84 -95 R 84 -97 R 84 -98 R +84 -100 R 84 -102 R 84 -104 R 84 -105 R 84 -107 R 28 -37 R D L2 2242 5637 M +10 2 R 90 12 R 90 10 R 90 8 R 89 7 R 90 5 R 89 3 R 89 1 R 89 0 R 89 -2 R +88 -4 R 89 -6 R 88 -8 R 88 -9 R 88 -11 R 88 -12 R 87 -15 R 88 -16 R 87 -18 R +87 -20 R 87 -21 R 87 -23 R 87 -25 R 86 -27 R 87 -28 R 86 -30 R 87 -32 R +86 -34 R 86 -35 R 86 -38 R 85 -38 R 86 -41 R 86 -42 R 85 -45 R 85 -45 R +86 -48 R 85 -49 R 85 -51 R 85 -53 R 85 -55 R 84 -56 R 85 -58 R 85 -60 R +84 -62 R 85 -63 R 84 -65 R 85 -67 R 84 -68 R 84 -70 R 84 -72 R 84 -74 R +84 -75 R 84 -78 R 84 -79 R 84 -80 R 84 -83 R 84 -84 R 84 -86 R 28 -30 R D L0 +3468 6705 M 30 -14 R 88 -43 R 87 -45 R 88 -46 R 87 -49 R 87 -50 R 87 -52 R +87 -53 R 87 -55 R 86 -58 R 87 -58 R 86 -61 R 87 -62 R 86 -64 R 86 -66 R +86 -67 R 85 -69 R 86 -71 R 86 -73 R 85 -74 R 85 -77 R 86 -77 R 85 -80 R +85 -81 R 85 -84 R 85 -84 R 84 -87 R 85 -88 R 85 -90 R 84 -92 R 85 -93 R +84 -96 R 85 -97 R 84 -98 R 84 -101 R 84 -102 R 84 -104 R 84 -105 R 84 -108 R +84 -109 R 84 -110 R 84 -113 R 84 -114 R 84 -116 R 28 -40 R D 15 setlinewidth +7197 1422 M 4955 0 R D 8175 1422 M 0 106 R D gsave 8175 889 translate 0 0 M +1.01 dup scale -305.858 0 N +(-22) show grestore 9479 1422 M 0 106 R D gsave 9479 889 translate 0 0 M +1.01 dup scale -305.858 0 N +(-24) show grestore 10783 1422 M 0 106 R D gsave 10783 889 translate 0 0 M +1.01 dup scale -305.858 0 N +(-26) show grestore 12087 1422 M 0 106 R D gsave 12087 889 translate 0 0 M +1.01 dup scale -305.858 0 N +(-28) show grestore 7197 1422 M 0 53 R D 7523 1422 M 0 53 R D 7849 1422 M +0 53 R D 8501 1422 M 0 53 R D 8827 1422 M 0 53 R D 9153 1422 M 0 53 R D +9805 1422 M 0 53 R D 10131 1422 M 0 53 R D 10457 1422 M 0 53 R D +11109 1422 M 0 53 R D 11435 1422 M 0 53 R D 11761 1422 M 0 53 R D +7197 6706 M 4955 0 R D 8175 6706 M 0 -106 R D 9479 6706 M 0 -106 R D +10783 6706 M 0 -106 R D 12087 6706 M 0 -106 R D 7197 6706 M 0 -53 R D +7523 6706 M 0 -53 R D 7849 6706 M 0 -53 R D 8501 6706 M 0 -53 R D +8827 6706 M 0 -53 R D 9153 6706 M 0 -53 R D 9805 6706 M 0 -53 R D +10131 6706 M 0 -53 R D 10457 6706 M 0 -53 R D 11109 6706 M 0 -53 R D +11435 6706 M 0 -53 R D 11761 6706 M 0 -53 R D 7197 1422 M 0 5284 R D +7197 2100 M 99 0 R D gsave 7085 1957 translate 0 0 M 1.01 dup scale +-117.687 0 N +( ) show grestore 7197 3454 M 99 0 R D gsave 7085 3312 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 4809 M 99 0 R D gsave 7085 4667 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 6164 M 99 0 R D gsave 7085 6021 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 1422 M 50 0 R D 7197 1558 M 50 0 R D 7197 1693 M +50 0 R D 7197 1829 M 50 0 R D 7197 1964 M 50 0 R D 7197 2235 M 50 0 R D +7197 2370 M 50 0 R D 7197 2506 M 50 0 R D 7197 2641 M 50 0 R D 7197 2777 M +50 0 R D 7197 2912 M 50 0 R D 7197 3048 M 50 0 R D 7197 3183 M 50 0 R D +7197 3319 M 50 0 R D 7197 3590 M 50 0 R D 7197 3725 M 50 0 R D 7197 3861 M +50 0 R D 7197 3996 M 50 0 R D 7197 4132 M 50 0 R D 7197 4267 M 50 0 R D +7197 4403 M 50 0 R D 7197 4538 M 50 0 R D 7197 4673 M 50 0 R D 7197 4944 M +50 0 R D 7197 5080 M 50 0 R D 7197 5215 M 50 0 R D 7197 5351 M 50 0 R D +7197 5486 M 50 0 R D 7197 5622 M 50 0 R D 7197 5757 M 50 0 R D 7197 5893 M +50 0 R D 7197 6028 M 50 0 R D 7197 6299 M 50 0 R D 7197 6435 M 50 0 R D +7197 6570 M 50 0 R D 7197 6706 M 50 0 R D 12152 1422 M 0 5284 R D +12152 2100 M -99 0 R D 12152 3454 M -99 0 R D 12152 4809 M -99 0 R D +12152 6164 M -99 0 R D 12152 1422 M -49 0 R D 12152 1558 M -49 0 R D +12152 1693 M -49 0 R D 12152 1829 M -49 0 R D 12152 1964 M -49 0 R D +12152 2235 M -49 0 R D 12152 2370 M -49 0 R D 12152 2506 M -49 0 R D +12152 2641 M -49 0 R D 12152 2777 M -49 0 R D 12152 2912 M -49 0 R D +12152 3048 M -49 0 R D 12152 3183 M -49 0 R D 12152 3319 M -49 0 R D +12152 3590 M -49 0 R D 12152 3725 M -49 0 R D 12152 3861 M -49 0 R D +12152 3996 M -49 0 R D 12152 4132 M -49 0 R D 12152 4267 M -49 0 R D +12152 4403 M -49 0 R D 12152 4538 M -49 0 R D 12152 4673 M -49 0 R D +12152 4944 M -49 0 R D 12152 5080 M -49 0 R D 12152 5215 M -49 0 R D +12152 5351 M -49 0 R D 12152 5486 M -49 0 R D 12152 5622 M -49 0 R D +12152 5757 M -49 0 R D 12152 5893 M -49 0 R D 12152 6028 M -49 0 R D +12152 6299 M -49 0 R D 12152 6435 M -49 0 R D 12152 6570 M -49 0 R D +12152 6706 M -49 0 R D 8195 6026 M 0 222 R 222 0 R 0 -222 R -222 0 R F +8847 6026 M 0 222 R 222 0 R 0 -222 R -222 0 R F +9499 4955 M 0 222 R 222 0 R 0 -222 R -222 0 R F +10151 4955 M 0 222 R 222 0 R 0 -222 R -222 0 R F +20 setlinewidth 8281 5907 M 49 0 R -24 0 R 0 395 R -25 0 R 49 0 R D +8933 5907 M 49 0 R -24 0 R 0 395 R -25 0 R 49 0 R D 9585 4109 M 49 0 R +-24 0 R 0 1304 R -25 0 R 49 0 R D 10237 4109 M 49 0 R -24 0 R 0 1304 R +-25 0 R 49 0 R D 1.000 0.780 0.000 setrgbcolor 10764 4944 M -1 15 R -3 14 R +-5 14 R -6 13 R -8 12 R -10 11 R -11 9 R -12 9 R -13 6 R -13 5 R -15 2 R +-14 1 R -15 -1 R -14 -2 R -14 -5 R -13 -6 R -12 -9 R -11 -9 R -9 -11 R +-8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -14 R 4 -14 R 7 -13 R +8 -12 R 9 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R 15 -1 R 14 1 R +15 3 R 13 5 R 13 6 R 12 8 R 11 10 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R +1 14 R F +11090 4403 M -1 14 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 10 R +-12 8 R -13 6 R -13 5 R -15 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R -13 -6 R +-12 -8 R -11 -10 R -9 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -14 R +1 -15 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -10 R 12 -8 R 13 -6 R +14 -5 R 14 -3 R 15 0 R 14 0 R 15 3 R 13 5 R 13 6 R 12 8 R 11 10 R 10 11 R +8 12 R 6 13 R 5 14 R 3 14 R 1 15 R F +11416 4199 M -1 15 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 9 R +-12 8 R -13 7 R -13 5 R -15 2 R -14 1 R -15 -1 R -14 -2 R -14 -5 R -13 -7 R +-12 -8 R -11 -9 R -9 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -15 R +1 -14 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -10 R 12 -8 R 13 -6 R +14 -5 R 14 -3 R 15 -1 R 14 1 R 15 3 R 13 5 R 13 6 R 12 8 R 11 10 R 10 11 R +8 12 R 6 13 R 5 14 R 3 14 R 1 14 R F +11872 3183 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -9 11 R -11 9 R -12 8 R +-13 7 R -14 5 R -14 2 R -15 1 R -14 -1 R -15 -2 R -13 -5 R -13 -7 R -12 -8 R +-11 -9 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -15 R 1 -14 R +3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -10 R 12 -8 R 13 -6 R 13 -5 R +15 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 9 11 R 8 12 R +7 13 R 4 14 R 3 14 R 1 14 R F +10628 4741 M 50 0 R -25 0 R 0 339 R -25 0 R 50 0 R D 10954 4267 M 50 0 R +-25 0 R 0 271 R -25 0 R 50 0 R D 11280 4064 M 50 0 R -25 0 R 0 237 R -25 0 R +50 0 R D 11736 2912 M 50 0 R -25 0 R 0 474 R -25 0 R 50 0 R D +1.000 0.000 0.000 setrgbcolor 11096 4508 M -1 15 R -2 14 R -5 14 R -7 13 R +-8 12 R -9 11 R -11 9 R -12 9 R -13 6 R -14 5 R -14 2 R -15 1 R -14 -1 R +-14 -2 R -14 -5 R -13 -6 R -12 -9 R -11 -9 R -10 -11 R -8 -12 R -6 -13 R +-5 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R +11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R +12 8 R 11 10 R 9 11 R 8 12 R 7 13 R 5 14 R 2 14 R 1 14 R F +11403 3993 M -1 15 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 9 R +-12 8 R -13 7 R -14 5 R -14 2 R -14 1 R -15 -1 R -14 -2 R -14 -5 R -13 -7 R +-12 -8 R -11 -9 R -9 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -15 R +1 -14 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -10 R 12 -8 R 13 -6 R +14 -5 R 14 -3 R 15 -1 R 14 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 10 11 R +8 12 R 6 13 R 5 14 R 3 14 R 1 14 R F +11729 3300 M -1 15 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 10 R +-12 8 R -13 6 R -14 5 R -14 3 R -14 0 R -15 0 R -14 -3 R -14 -5 R -13 -6 R +-12 -8 R -11 -10 R -9 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -15 R +1 -14 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -10 R 12 -8 R 13 -6 R +14 -5 R 14 -3 R 15 -1 R 14 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 10 11 R +8 12 R 6 13 R 5 14 R 3 14 R 1 14 R F +10961 3969 M 49 0 R -25 0 R 0 791 R -24 0 R 49 0 R D 11267 3693 M 50 0 R +-25 0 R 0 498 R -25 0 R 50 0 R D 11593 2971 M 50 0 R -25 0 R 0 539 R -25 0 R +50 0 R D 10 setlinewidth 11207 3993 M -1 15 R -3 14 R -4 14 R -7 13 R +-8 12 R -9 11 R -11 9 R -12 8 R -13 7 R -14 5 R -14 2 R -15 1 R -14 -1 R +-15 -2 R -13 -5 R -13 -7 R -12 -8 R -11 -9 R -10 -11 R -8 -12 R -6 -13 R +-5 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R +11 -10 R 12 -8 R 13 -6 R 13 -5 R 15 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R +12 8 R 11 10 R 9 11 R 8 12 R 7 13 R 4 14 R 3 14 R 1 14 R D 11501 3510 M +-1 15 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 9 R -12 8 R -13 7 R +-14 5 R -14 2 R -14 1 R -15 -1 R -14 -2 R -14 -5 R -13 -7 R -12 -8 R +-11 -9 R -9 -11 R -9 -12 R -6 -13 R -5 -14 R -2 -14 R -1 -15 R 1 -14 R +2 -14 R 5 -14 R 6 -13 R 9 -12 R 9 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R +14 -3 R 15 -1 R 14 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 10 11 R 8 12 R +6 13 R 5 14 R 3 14 R 1 14 R D 11977 3154 M -1 14 R -3 14 R -5 14 R -6 13 R +-8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -14 1 R -15 -1 R +-14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -10 -11 R -8 -12 R -6 -13 R +-5 -14 R -3 -14 R 0 -14 R 0 -15 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R +11 -9 R 12 -8 R 13 -7 R 14 -5 R 14 -2 R 15 -1 R 14 1 R 14 2 R 14 5 R 13 7 R +12 8 R 11 9 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 15 R D 20 setlinewidth +11071 3454 M 50 0 R -25 0 R 0 816 R -25 0 R 50 0 R D 11365 3323 M 49 0 R +-24 0 R 0 443 R -25 0 R 49 0 R D 11841 2784 M 49 0 R -24 0 R 0 608 R -25 0 R +49 0 R D 0.000 1.000 0.580 setrgbcolor 10457 4955 M -40 -125 R -132 0 R +106 -78 R -40 -125 R 106 78 R 107 -78 R -41 125 R 107 78 R -132 0 R +-41 125 R F +11109 5067 M -40 -125 R -132 0 R 106 -77 R -40 -126 R 106 78 R 107 -78 R +-41 126 R 107 77 R -132 0 R -41 125 R F +11761 3971 M -41 -125 R -131 0 R 106 -77 R -40 -125 R 106 77 R 107 -77 R +-41 125 R 107 77 R -132 0 R -41 125 R F +10457 1422 M 0 3760 R -25 0 R 50 0 R D 11084 4317 M 50 0 R -25 0 R 0 853 R +-25 0 R 50 0 R D 11736 3372 M 50 0 R -25 0 R 0 660 R -25 0 R 50 0 R D +0.000 0.000 0.000 setrgbcolor 7508 1694 M 0 178 R 178 0 R 0 -178 R -178 0 R +F +gsave 7863 1677 translate 0 0 M 0.8 dup scale +(z = 3.6 - 4.2 \(W03\)) show grestore 0.000 1.000 0.580 setrgbcolor +7597 2266 M -33 -100 R -105 0 R 85 -62 R -32 -100 R 85 62 R 85 -62 R +-32 100 R 85 62 R -106 0 R -32 100 R F +0.000 0.000 0.000 setrgbcolor gsave 7863 2016 translate 0 0 M 0.8 dup scale +(z = 3.5 - 4.5 \(WHO\)) show grestore 1.000 0.780 0.000 setrgbcolor +7686 2460 M -1 12 R -2 11 R -4 11 R -5 10 R -7 10 R -7 9 R -9 8 R -10 6 R +-10 5 R -11 4 R -11 2 R -12 1 R -12 -1 R -11 -2 R -11 -4 R -10 -5 R -10 -6 R +-9 -8 R -8 -9 R -6 -10 R -5 -10 R -4 -11 R -2 -11 R -1 -12 R 1 -12 R 2 -11 R +4 -11 R 5 -10 R 6 -10 R 8 -9 R 9 -7 R 10 -7 R 10 -5 R 11 -4 R 11 -2 R +12 -1 R 12 1 R 11 2 R 11 4 R 10 5 R 10 7 R 9 7 R 7 9 R 7 10 R 5 10 R 4 11 R +2 11 R 1 12 R F +0.000 0.000 0.000 setrgbcolor gsave 7863 2354 translate 0 0 M 0.8 dup scale +(z ~ 4 \(SSG\)) show grestore 1.000 0.000 0.000 setrgbcolor 7686 2799 M +-1 11 R -2 12 R -4 11 R -5 10 R -7 10 R -7 9 R -9 7 R -10 7 R -10 5 R +-11 4 R -11 2 R -12 1 R -12 -1 R -11 -2 R -11 -4 R -10 -5 R -10 -7 R -9 -7 R +-8 -9 R -6 -10 R -5 -10 R -4 -11 R -2 -12 R -1 -11 R 1 -12 R 2 -11 R 4 -11 R +5 -11 R 6 -9 R 8 -9 R 9 -8 R 10 -6 R 10 -5 R 11 -4 R 11 -2 R 12 -1 R 12 1 R +11 2 R 11 4 R 10 5 R 10 6 R 9 8 R 7 9 R 7 9 R 5 11 R 4 11 R 2 11 R 1 12 R F +0.000 0.000 0.000 setrgbcolor gsave 7863 2693 translate 0 0 M 0.8 dup scale +(z = 3.6 - 3.9 \(F01\)) show grestore 10 setlinewidth +1.000 0.000 0.000 setrgbcolor 7686 3137 M -1 12 R -2 11 R -4 11 R -5 11 R +-7 9 R -7 9 R -9 8 R -10 6 R -10 5 R -11 4 R -11 2 R -12 1 R -12 -1 R +-11 -2 R -11 -4 R -10 -5 R -10 -6 R -9 -8 R -8 -9 R -6 -9 R -5 -11 R +-4 -11 R -2 -11 R -1 -12 R 1 -11 R 2 -12 R 4 -11 R 5 -10 R 6 -10 R 8 -8 R +9 -8 R 10 -6 R 10 -6 R 11 -3 R 11 -3 R 12 0 R 12 0 R 11 3 R 11 3 R 10 6 R +10 6 R 9 8 R 7 8 R 7 10 R 5 10 R 4 11 R 2 12 R 1 11 R D +0.000 0.000 0.000 setrgbcolor gsave 7863 3032 translate 0 0 M 0.8 dup scale +(z = 3.9 - 4.4 \(F01\)) show grestore gsave 9675 406 translate 0 0 M +1.01 dup scale -263.851 0 N +(M) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(B) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 20 setlinewidth L2 7197 5637 M 10 2 R 90 12 R +90 10 R 90 8 R 89 7 R 90 5 R 89 3 R 89 1 R 89 0 R 89 -2 R 88 -4 R 89 -6 R +88 -8 R 88 -9 R 88 -11 R 88 -12 R 87 -15 R 88 -16 R 87 -18 R 87 -20 R +87 -21 R 87 -23 R 87 -25 R 87 -27 R 86 -28 R 86 -30 R 87 -32 R 86 -34 R +86 -35 R 86 -38 R 85 -38 R 86 -41 R 86 -42 R 85 -45 R 85 -45 R 86 -48 R +85 -49 R 85 -51 R 85 -53 R 85 -55 R 84 -56 R 85 -58 R 85 -60 R 84 -62 R +85 -63 R 84 -65 R 85 -67 R 84 -68 R 84 -70 R 84 -72 R 84 -74 R 84 -75 R +84 -78 R 84 -79 R 84 -80 R 84 -83 R 84 -84 R 84 -86 R 28 -30 R D L0 +8423 6705 M 30 -14 R 88 -43 R 87 -45 R 88 -46 R 87 -49 R 87 -50 R 87 -52 R +87 -53 R 87 -55 R 87 -58 R 86 -58 R 86 -61 R 87 -62 R 86 -64 R 86 -66 R +86 -67 R 85 -69 R 86 -71 R 86 -73 R 85 -74 R 85 -77 R 86 -77 R 85 -80 R +85 -81 R 85 -84 R 85 -84 R 84 -87 R 85 -88 R 85 -90 R 84 -92 R 85 -93 R +84 -96 R 85 -97 R 84 -98 R 84 -101 R 84 -102 R 84 -104 R 84 -105 R 84 -108 R +84 -109 R 84 -110 R 84 -113 R 84 -114 R 84 -116 R 28 -40 R D L2 7197 5089 M +10 2 R 90 14 R 90 11 R 90 11 R 89 8 R 90 6 R 89 5 R 89 3 R 89 2 R 89 -1 R +88 -2 R 89 -4 R 88 -6 R 88 -7 R 88 -9 R 88 -11 R 87 -13 R 88 -15 R 87 -16 R +87 -18 R 87 -19 R 87 -22 R 87 -23 R 87 -25 R 86 -27 R 86 -28 R 87 -30 R +86 -32 R 86 -34 R 86 -35 R 85 -38 R 86 -38 R 86 -41 R 85 -43 R 85 -44 R +86 -46 R 85 -47 R 85 -50 R 85 -51 R 85 -53 R 84 -54 R 85 -56 R 85 -59 R +84 -59 R 85 -62 R 84 -63 R 85 -65 R 84 -67 R 84 -69 R 84 -70 R 84 -72 R +84 -73 R 84 -76 R 84 -77 R 84 -79 R 84 -81 R 84 -82 R 84 -84 R 28 -30 R D L0 +8003 6705 M 9 -4 R 88 -44 R 89 -46 R 88 -47 R 88 -49 R 88 -52 R 88 -52 R +87 -55 R 88 -56 R 87 -58 R 87 -60 R 87 -61 R 87 -63 R 87 -65 R 87 -67 R +86 -68 R 86 -71 R 87 -71 R 86 -74 R 86 -75 R 86 -77 R 85 -79 R 86 -81 R +86 -82 R 85 -84 R 85 -86 R 86 -87 R 85 -90 R 85 -91 R 85 -92 R 85 -95 R +84 -96 R 85 -98 R 85 -99 R 84 -102 R 85 -103 R 84 -104 R 85 -107 R 84 -108 R +84 -110 R 84 -112 R 84 -113 R 84 -115 R 84 -117 R 84 -119 R 84 -120 R +84 -122 R 84 -124 R 84 -126 R 28 -43 R D 15 setlinewidth 12152 1422 M +4955 0 R D 13130 1422 M 0 106 R D gsave 13130 889 translate 0 0 M +1.01 dup scale -305.858 0 N +(-22) show grestore 14434 1422 M 0 106 R D gsave 14434 889 translate 0 0 M +1.01 dup scale -305.858 0 N +(-24) show grestore 15738 1422 M 0 106 R D gsave 15738 889 translate 0 0 M +1.01 dup scale -305.858 0 N +(-26) show grestore 17042 1422 M 0 106 R D gsave 17042 889 translate 0 0 M +1.01 dup scale -305.858 0 N +(-28) show grestore 12152 1422 M 0 53 R D 12478 1422 M 0 53 R D 12804 1422 M +0 53 R D 13456 1422 M 0 53 R D 13782 1422 M 0 53 R D 14108 1422 M 0 53 R D +14760 1422 M 0 53 R D 15086 1422 M 0 53 R D 15412 1422 M 0 53 R D +16064 1422 M 0 53 R D 16390 1422 M 0 53 R D 16716 1422 M 0 53 R D +12152 6706 M 4955 0 R D 13130 6706 M 0 -106 R D 14434 6706 M 0 -106 R D +15738 6706 M 0 -106 R D 17042 6706 M 0 -106 R D 12152 6706 M 0 -53 R D +12478 6706 M 0 -53 R D 12804 6706 M 0 -53 R D 13456 6706 M 0 -53 R D +13782 6706 M 0 -53 R D 14108 6706 M 0 -53 R D 14760 6706 M 0 -53 R D +15086 6706 M 0 -53 R D 15412 6706 M 0 -53 R D 16064 6706 M 0 -53 R D +16390 6706 M 0 -53 R D 16716 6706 M 0 -53 R D 12152 1422 M 0 5284 R D +12152 2100 M 99 0 R D gsave 12040 1957 translate 0 0 M 1.01 dup scale +-117.687 0 N +( ) show grestore 12152 3454 M 99 0 R D gsave 12040 3312 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 4809 M 99 0 R D gsave 12040 4667 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 6164 M 99 0 R D gsave 12040 6021 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 1422 M 50 0 R D 12152 1558 M 50 0 R D 12152 1693 M +50 0 R D 12152 1829 M 50 0 R D 12152 1964 M 50 0 R D 12152 2235 M 50 0 R D +12152 2370 M 50 0 R D 12152 2506 M 50 0 R D 12152 2641 M 50 0 R D +12152 2777 M 50 0 R D 12152 2912 M 50 0 R D 12152 3048 M 50 0 R D +12152 3183 M 50 0 R D 12152 3319 M 50 0 R D 12152 3590 M 50 0 R D +12152 3725 M 50 0 R D 12152 3861 M 50 0 R D 12152 3996 M 50 0 R D +12152 4132 M 50 0 R D 12152 4267 M 50 0 R D 12152 4403 M 50 0 R D +12152 4538 M 50 0 R D 12152 4673 M 50 0 R D 12152 4944 M 50 0 R D +12152 5080 M 50 0 R D 12152 5215 M 50 0 R D 12152 5351 M 50 0 R D +12152 5486 M 50 0 R D 12152 5622 M 50 0 R D 12152 5757 M 50 0 R D +12152 5893 M 50 0 R D 12152 6028 M 50 0 R D 12152 6299 M 50 0 R D +12152 6435 M 50 0 R D 12152 6570 M 50 0 R D 12152 6706 M 50 0 R D +17107 1422 M 0 5284 R D 17107 2100 M -99 0 R D 17107 3454 M -99 0 R D +17107 4809 M -99 0 R D 17107 6164 M -99 0 R D 17107 1422 M -49 0 R D +17107 1558 M -49 0 R D 17107 1693 M -49 0 R D 17107 1829 M -49 0 R D +17107 1964 M -49 0 R D 17107 2235 M -49 0 R D 17107 2370 M -49 0 R D +17107 2506 M -49 0 R D 17107 2641 M -49 0 R D 17107 2777 M -49 0 R D +17107 2912 M -49 0 R D 17107 3048 M -49 0 R D 17107 3183 M -49 0 R D +17107 3319 M -49 0 R D 17107 3590 M -49 0 R D 17107 3725 M -49 0 R D +17107 3861 M -49 0 R D 17107 3996 M -49 0 R D 17107 4132 M -49 0 R D +17107 4267 M -49 0 R D 17107 4403 M -49 0 R D 17107 4538 M -49 0 R D +17107 4673 M -49 0 R D 17107 4944 M -49 0 R D 17107 5080 M -49 0 R D +17107 5215 M -49 0 R D 17107 5351 M -49 0 R D 17107 5486 M -49 0 R D +17107 5622 M -49 0 R D 17107 5757 M -49 0 R D 17107 5893 M -49 0 R D +17107 6028 M -49 0 R D 17107 6299 M -49 0 R D 17107 6435 M -49 0 R D +17107 6570 M -49 0 R D 17107 6706 M -49 0 R D 14454 5606 M 0 222 R 222 0 R +0 -222 R -222 0 R F +15106 4982 M 0 222 R 222 0 R 0 -222 R -222 0 R F +20 setlinewidth 14540 5351 M 49 0 R -24 0 R 0 589 R -25 0 R 49 0 R D +15192 4188 M 49 0 R -24 0 R 0 1246 R -25 0 R 49 0 R D +0.082 1.000 0.000 setrgbcolor 16279 3606 M 111 222 R 111 -222 R -222 0 R F +16931 2231 M 111 222 R 65 -130 R 0 -92 R -176 0 R F +16365 3359 M 50 0 R -25 0 R 0 580 R -25 0 R 50 0 R D 17017 1716 M 50 0 R +-25 0 R 0 922 R -25 0 R 50 0 R D 1.000 0.000 0.000 setrgbcolor 16456 3069 M +-1 15 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R +-14 5 R -14 3 R -14 0 R -15 0 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R +-11 -10 R -9 -11 R -9 -12 R -6 -13 R -5 -14 R -2 -14 R -1 -15 R 1 -14 R +2 -14 R 5 -14 R 6 -13 R 9 -12 R 9 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R +14 -3 R 15 -1 R 14 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 10 11 R 8 12 R +6 13 R 5 14 R 3 14 R 1 14 R F +16866 2563 M -1 15 R -2 14 R -5 14 R -7 13 R -8 12 R -9 11 R -11 9 R -12 9 R +-13 6 R -14 5 R -14 2 R -15 1 R -14 -1 R -14 -2 R -14 -5 R -13 -6 R -12 -9 R +-11 -9 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -15 R 1 -14 R +3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R +14 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 9 11 R 8 12 R +7 13 R 5 14 R 2 14 R 1 14 R F +16320 2662 M 49 0 R -24 0 R 0 661 R -25 0 R 49 0 R D 16731 2038 M 49 0 R +-25 0 R 0 799 R -24 0 R 49 0 R D 0.000 0.000 0.000 setrgbcolor 12463 1694 M +0 178 R 178 0 R 0 -178 R -178 0 R F +gsave 12818 1677 translate 0 0 M 0.8 dup scale +(z = 4.2 - 4.8 \(W03\)) show grestore 1.000 0.000 0.000 setrgbcolor +12641 2121 M -1 12 R -2 11 R -4 11 R -5 11 R -7 9 R -7 9 R -9 8 R -10 6 R +-10 5 R -11 4 R -11 2 R -12 1 R -12 -1 R -11 -2 R -11 -4 R -10 -5 R -10 -6 R +-9 -8 R -7 -9 R -7 -9 R -5 -11 R -4 -11 R -2 -11 R -1 -12 R 1 -11 R 2 -12 R +4 -11 R 5 -10 R 7 -10 R 7 -8 R 9 -8 R 10 -7 R 10 -5 R 11 -3 R 11 -3 R 12 0 R +12 0 R 11 3 R 11 3 R 10 5 R 10 7 R 9 8 R 7 8 R 7 10 R 5 10 R 4 11 R 2 12 R +1 11 R F +0.000 0.000 0.000 setrgbcolor gsave 12818 2016 translate 0 0 M 0.8 dup scale +(z = 4.4 - 5.0 \(F01\)) show grestore 0.082 1.000 0.000 setrgbcolor +12463 2371 M 89 178 R 89 -178 R -178 0 R F +0.000 0.000 0.000 setrgbcolor gsave 12818 2354 translate 0 0 M 0.8 dup scale +(z = 4.0 - 4.5 \(KDC\)) show grestore L2 12152 5089 M 10 2 R 90 14 R 90 11 R +90 11 R 89 8 R 90 6 R 89 5 R 89 3 R 89 2 R 89 -1 R 88 -2 R 89 -4 R 88 -6 R +88 -7 R 88 -9 R 88 -11 R 87 -13 R 88 -15 R 87 -16 R 87 -18 R 87 -19 R +87 -22 R 87 -23 R 87 -25 R 86 -27 R 86 -28 R 87 -30 R 86 -32 R 86 -34 R +86 -35 R 85 -38 R 86 -38 R 86 -41 R 85 -43 R 85 -44 R 86 -46 R 85 -47 R +85 -50 R 85 -51 R 85 -53 R 84 -54 R 85 -56 R 85 -59 R 84 -59 R 85 -62 R +84 -63 R 85 -65 R 84 -67 R 84 -69 R 84 -70 R 84 -72 R 84 -73 R 84 -76 R +84 -77 R 84 -79 R 84 -81 R 84 -82 R 84 -84 R 28 -30 R D L0 12958 6705 M +9 -4 R 88 -44 R 89 -46 R 88 -47 R 88 -49 R 88 -52 R 88 -52 R 87 -55 R +88 -56 R 87 -58 R 87 -60 R 87 -61 R 87 -63 R 87 -65 R 87 -67 R 86 -68 R +86 -71 R 87 -71 R 86 -74 R 86 -75 R 86 -77 R 85 -79 R 86 -81 R 86 -82 R +85 -84 R 85 -86 R 86 -87 R 85 -90 R 85 -91 R 85 -92 R 85 -95 R 84 -96 R +85 -98 R 85 -99 R 84 -102 R 85 -103 R 84 -104 R 85 -107 R 84 -108 R +84 -110 R 84 -112 R 84 -113 R 84 -115 R 84 -117 R 84 -119 R 84 -120 R +84 -122 R 84 -124 R 84 -126 R 28 -43 R D L2 12152 4545 M 10 2 R 90 15 R +90 13 R 90 11 R 89 10 R 90 8 R 89 6 R 89 4 R 89 3 R 89 0 R 88 0 R 89 -3 R +88 -4 R 88 -7 R 88 -8 R 88 -9 R 87 -12 R 88 -13 R 87 -15 R 87 -16 R 87 -19 R +87 -20 R 87 -22 R 87 -23 R 86 -26 R 86 -27 R 87 -29 R 86 -30 R 86 -33 R +86 -34 R 85 -36 R 86 -37 R 86 -40 R 85 -41 R 85 -43 R 86 -44 R 85 -47 R +85 -48 R 85 -50 R 85 -51 R 84 -53 R 85 -56 R 85 -56 R 84 -59 R 85 -60 R +84 -62 R 85 -64 R 84 -65 R 84 -68 R 84 -69 R 84 -70 R 84 -73 R 84 -74 R +84 -76 R 84 -77 R 84 -80 R 84 -81 R 84 -83 R 28 -29 R D L0 12512 6705 M +9 -4 R 90 -46 R 89 -47 R 89 -49 R 89 -51 R 89 -52 R 88 -54 R 89 -56 R +88 -58 R 88 -59 R 88 -61 R 88 -63 R 87 -64 R 88 -67 R 87 -68 R 87 -70 R +87 -71 R 87 -73 R 87 -75 R 87 -77 R 86 -79 R 86 -80 R 87 -82 R 86 -83 R +86 -86 R 86 -87 R 85 -89 R 86 -90 R 86 -92 R 85 -95 R 85 -95 R 86 -98 R +85 -99 R 85 -101 R 85 -103 R 85 -104 R 84 -106 R 85 -108 R 85 -110 R +84 -111 R 85 -113 R 84 -115 R 85 -116 R 84 -119 R 84 -120 R 84 -121 R +84 -124 R 84 -125 R 84 -127 R 84 -128 R 84 -130 R 84 -132 R 84 -134 R +84 -136 R 28 -47 R D +%%PageTrailer +end +restore +showpage +%%PageResources: font Helvetica +%%+ font Symbol +%%Trailer +restore +%%Pages: 1 +%%DocumentNeededResources: font Helvetica +%%+ font Symbol +%%EOF diff --git a/feedback/papers/0506398/f12.ps b/feedback/papers/0506398/f12.ps new file mode 100644 index 0000000..7601429 --- /dev/null +++ b/feedback/papers/0506398/f12.ps @@ -0,0 +1,471 @@ +%!PS-Adobe-3.0 +%%BoundingBox: 54 360 620 643 +%%Title: Graphics produced by IDL +%%For: phopkins@Philip-Hopkins-Computer.local, +%% /Users/phopkins/Documents/lars_galaxies/plots/LF_massive/from_zeus +%%Creator: IDL Student Edition 6.0.3, Mac OS X (darwin ppc m32) +%%CreationDate: Wed Aug 17 15:13:19 2005 +%%DocumentData: Clean7bit +%%Requirements: color +%%LanguageLevel: 1 +%%PageOrder: Ascend +%%Pages: (atend) +%%DocumentNeededResources: (atend) +%%EndComments +%%BeginProlog +save +%+ prolog.ps -- Prolog for IDL generated PostScript files +%+ Copyright (c) 1988-2003 Research Systems, Inc. All Rights Reserved. +%v 4 +/$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C +{currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint +stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} +bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show +grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 +setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 +{[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 +100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 +{[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef +/ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} +ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont +exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica +findfont exch scalefont setfont (\267) show currentpoint grestore moveto} +bdef end 2.5 setmiterlimit +%%EndProlog +%%Page: 0 1 +%%PageRequirements: color +%%PageResources: (atend) +%%PageOrientation: Portrait +%%PageBoundingBox: 54 360 620 643 +%%BeginPageSetup +save +$IDL_DICT begin 54 360 translate 0.0283465 dup scale +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +%%EndPageSetup +15 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 1345 1422 M 9104 0 R D +1345 1422 M 0 157 R D gsave 1345 889 translate 0 0 M 1.01 dup scale +-117.687 0 N +(0) show grestore 3874 1422 M 0 157 R D gsave 3874 889 translate 0 0 M +1.01 dup scale -117.687 0 N +(1) show grestore 6403 1422 M 0 157 R D gsave 6403 889 translate 0 0 M +1.01 dup scale -117.687 0 N +(2) show grestore 8931 1422 M 0 157 R D gsave 8931 889 translate 0 0 M +1.01 dup scale -117.687 0 N +(3) show grestore 1598 1422 M 0 79 R D 1851 1422 M 0 79 R D 2104 1422 M +0 79 R D 2357 1422 M 0 79 R D 2610 1422 M 0 79 R D 2863 1422 M 0 79 R D +3115 1422 M 0 79 R D 3368 1422 M 0 79 R D 3621 1422 M 0 79 R D 4127 1422 M +0 79 R D 4380 1422 M 0 79 R D 4633 1422 M 0 79 R D 4886 1422 M 0 79 R D +5138 1422 M 0 79 R D 5391 1422 M 0 79 R D 5644 1422 M 0 79 R D 5897 1422 M +0 79 R D 6150 1422 M 0 79 R D 6656 1422 M 0 79 R D 6908 1422 M 0 79 R D +7161 1422 M 0 79 R D 7414 1422 M 0 79 R D 7667 1422 M 0 79 R D 7920 1422 M +0 79 R D 8173 1422 M 0 79 R D 8426 1422 M 0 79 R D 8678 1422 M 0 79 R D +9184 1422 M 0 79 R D 9437 1422 M 0 79 R D 9690 1422 M 0 79 R D 9943 1422 M +0 79 R D 10196 1422 M 0 79 R D 10449 1422 M 0 79 R D +gsave 5897 427 translate 0 0 M 1.01 dup scale -1336.04 0 N +(N) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(H I) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( [10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(21) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( cm) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(-2) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(]) show grestore 1345 9289 M 9104 0 R D 1345 9289 M 0 -157 R D 3874 9289 M +0 -157 R D 6403 9289 M 0 -157 R D 8931 9289 M 0 -157 R D 1598 9289 M 0 -79 R +D 1851 9289 M 0 -79 R D 2104 9289 M 0 -79 R D 2357 9289 M 0 -79 R D +2610 9289 M 0 -79 R D 2863 9289 M 0 -79 R D 3115 9289 M 0 -79 R D +3368 9289 M 0 -79 R D 3621 9289 M 0 -79 R D 4127 9289 M 0 -79 R D +4380 9289 M 0 -79 R D 4633 9289 M 0 -79 R D 4886 9289 M 0 -79 R D +5138 9289 M 0 -79 R D 5391 9289 M 0 -79 R D 5644 9289 M 0 -79 R D +5897 9289 M 0 -79 R D 6150 9289 M 0 -79 R D 6656 9289 M 0 -79 R D +6908 9289 M 0 -79 R D 7161 9289 M 0 -79 R D 7414 9289 M 0 -79 R D +7667 9289 M 0 -79 R D 7920 9289 M 0 -79 R D 8173 9289 M 0 -79 R D +8426 9289 M 0 -79 R D 8678 9289 M 0 -79 R D 9184 9289 M 0 -79 R D +9437 9289 M 0 -79 R D 9690 9289 M 0 -79 R D 9943 9289 M 0 -79 R D +10196 9289 M 0 -79 R D 10449 9289 M 0 -79 R D 1345 1422 M 0 7867 R D +1345 1422 M 182 0 R D gsave 1233 1422 translate 0 0 M 1.01 dup scale +-117.687 0 N +( ) show grestore 1345 2996 M 182 0 R D gsave 1233 2853 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 1345 4569 M 182 0 R D gsave 1233 4427 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 1345 6142 M 182 0 R D gsave 1233 6000 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 1345 7716 M 182 0 R D gsave 1233 7573 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 1345 9289 M 182 0 R D gsave 1233 9040 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 1345 1737 M 91 0 R D 1345 2051 M 91 0 R D 1345 2366 M +91 0 R D 1345 2681 M 91 0 R D 1345 3310 M 91 0 R D 1345 3625 M 91 0 R D +1345 3940 M 91 0 R D 1345 4254 M 91 0 R D 1345 4884 M 91 0 R D 1345 5198 M +91 0 R D 1345 5513 M 91 0 R D 1345 5828 M 91 0 R D 1345 6457 M 91 0 R D +1345 6772 M 91 0 R D 1345 7086 M 91 0 R D 1345 7401 M 91 0 R D 1345 8030 M +91 0 R D 1345 8345 M 91 0 R D 1345 8660 M 91 0 R D 1345 8974 M 91 0 R D +gsave 779 5356 translate 0 0 M 90 rotate 1.01 dup scale -2575.77 0 N +(Probability \(Arbitrary Scale\)) show grestore 10449 1422 M 0 7867 R D +10449 1422 M -183 0 R D 10449 2996 M -183 0 R D 10449 4569 M -183 0 R D +10449 6142 M -183 0 R D 10449 7716 M -183 0 R D 10449 9289 M -183 0 R D +10449 1737 M -91 0 R D 10449 2051 M -91 0 R D 10449 2366 M -91 0 R D +10449 2681 M -91 0 R D 10449 3310 M -91 0 R D 10449 3625 M -91 0 R D +10449 3940 M -91 0 R D 10449 4254 M -91 0 R D 10449 4884 M -91 0 R D +10449 5198 M -91 0 R D 10449 5513 M -91 0 R D 10449 5828 M -91 0 R D +10449 6457 M -91 0 R D 10449 6772 M -91 0 R D 10449 7086 M -91 0 R D +10449 7401 M -91 0 R D 10449 8030 M -91 0 R D 10449 8345 M -91 0 R D +10449 8660 M -91 0 R D 10449 8974 M -91 0 R D 40 setlinewidth 1472 1422 M +126 0 R 0 11 R 127 0 R 126 0 R 0 717 R 127 0 R 126 0 R 0 2822 R 126 0 R +127 0 R 0 -829 R 126 0 R 127 0 R 0 -1253 R 126 0 R 127 0 R 0 1064 R 126 0 R +126 0 R 0 -136 R 127 0 R 126 0 R 0 -395 R 127 0 R 126 0 R 0 -257 R 127 0 R +126 0 R 0 -263 R 126 0 R 127 0 R 0 -157 R 126 0 R 127 0 R 0 -162 R 126 0 R +127 0 R 0 -243 R 126 0 R 127 0 R 0 60 R 126 0 R 126 0 R 0 -236 R 127 0 R +126 0 R 0 -91 R 127 0 R 126 0 R 0 40 R 127 0 R 126 0 R 0 -18 R 126 0 R +127 0 R 0 -18 R 126 0 R 127 0 R 0 -6 R 126 0 R 127 0 R 0 -102 R 126 0 R +126 0 R 0 60 R 127 0 R 126 0 R 0 -98 R 127 0 R 126 0 R 0 -38 R 127 0 R +126 0 R 0 -20 R 126 0 R 127 0 R 0 -35 R 126 0 R 127 0 R 0 -40 R 126 0 R +127 0 R 0 -87 R 126 0 R 126 0 R 0 -55 R 127 0 R 126 0 R 0 -57 R 127 0 R +126 0 R 0 -45 R 127 0 R 126 0 R 0 -38 R 127 0 R 126 0 R 0 -38 R 126 0 R +127 0 R 0 -41 R 126 0 R 127 0 R 0 -16 R 126 0 R 126 0 R D 20 setlinewidth +1.000 0.000 0.000 setrgbcolor 1472 1552 M 253 308 R 253 686 R 252 1080 R +253 1097 R 253 475 R 253 -238 R 253 -563 R 253 -624 R 253 -533 R 252 -411 R +253 -304 R 253 -224 R 253 -168 R 253 -126 R 253 -97 R 253 -75 R 253 -60 R +252 -48 R 253 -39 R 253 -32 R 253 -27 R 253 -22 R 253 -19 R 253 -17 R +252 -14 R 253 -12 R 253 -10 R 253 -10 R 253 -8 R 253 -7 R 253 -7 R 253 -5 R +252 -6 R 253 -4 R 253 -5 R 126 -2 R D 0.000 0.000 0.000 setrgbcolor +gsave 2104 8660 translate 0 0 M 1.2 dup scale +(Optical) show grestore gsave 6150 8691 translate 0 0 M 1.15 dup scale +(\(L) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(B, obs) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( > 10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(11) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( L) show CP X -101.051 M +%%IncludeResource: font AvantGarde-Book +262.467 /AvantGarde-Book STDFONT +(O) show M X -58.3193 M +%%IncludeResource: font AvantGarde-Book +186.267 /AvantGarde-Book STDFONT +( \267) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(\)) show grestore L2 3741 7949 M 1998 0 R D gsave 6072 7817 translate 0 0 M +1.01 dup scale +(Standard Torus) show grestore L1 3741 7421 M 1998 0 R D +gsave 6072 7289 translate 0 0 M 1.01 dup scale +(Receding Torus) show grestore L0 3741 6893 M 1998 0 R D +gsave 6072 6761 translate 0 0 M 1.01 dup scale +(Full Model) show grestore L2 1662 9289 M 0 -7867 R 316 0 R 316 0 R 316 0 R +316 0 R 316 0 R 316 0 R 316 0 R 316 0 R 316 0 R 316 0 R 316 0 R 316 0 R +317 0 R 316 0 R 316 0 R 316 0 R 316 0 R 316 0 R 316 0 R 316 0 R 316 0 R +316 0 R 316 0 R 316 0 R 317 0 R 316 0 R 316 0 R 252 0 R D L1 1788 9289 M +0 -7867 R 316 0 R 316 0 R 316 0 R 316 0 R 316 0 R 316 0 R 316 0 R 317 0 R +316 0 R 316 0 R 316 0 R 316 0 R 316 0 R 316 0 R 316 0 R 316 0 R 316 0 R +316 0 R 316 0 R 317 0 R 316 0 R 316 0 R 316 0 R 316 0 R 316 0 R 316 0 R +316 0 R 126 0 R D 15 setlinewidth L0 10449 1422 M 9103 0 R D 10449 1422 M +0 157 R D gsave 10449 889 translate 0 0 M 1.01 dup scale -381.305 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(19) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 11749 1422 M 0 157 R D +gsave 11749 889 translate 0 0 M 1.01 dup scale -381.305 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(20) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 13049 1422 M 0 157 R D +gsave 13049 889 translate 0 0 M 1.01 dup scale -381.305 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(21) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 14350 1422 M 0 157 R D +gsave 14350 889 translate 0 0 M 1.01 dup scale -381.305 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(22) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 15650 1422 M 0 157 R D +gsave 15650 889 translate 0 0 M 1.01 dup scale -381.305 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(23) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 16951 1422 M 0 157 R D +gsave 16951 889 translate 0 0 M 1.01 dup scale -381.305 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(24) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 18251 1422 M 0 157 R D +gsave 18251 889 translate 0 0 M 1.01 dup scale -381.305 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(25) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 19552 1422 M 0 157 R D +gsave 19552 889 translate 0 0 M 1.01 dup scale -381.305 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(26) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT gsave 15000 427 translate 0 0 M 1.01 dup scale +-822.922 0 N +(N) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(H) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( [cm) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(-2) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(]) show grestore 10449 9289 M 9103 0 R D 10449 9289 M 0 -157 R D +11749 9289 M 0 -157 R D 13049 9289 M 0 -157 R D 14350 9289 M 0 -157 R D +15650 9289 M 0 -157 R D 16951 9289 M 0 -157 R D 18251 9289 M 0 -157 R D +19552 9289 M 0 -157 R D 10449 1422 M 0 7867 R D 10449 1422 M 182 0 R D +gsave 10336 1422 translate 0 0 M 1.01 dup scale -117.687 0 N +( ) show grestore 10449 2996 M 182 0 R D gsave 10336 2853 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 10449 4569 M 182 0 R D gsave 10336 4427 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 10449 6142 M 182 0 R D gsave 10336 6000 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 10449 7716 M 182 0 R D gsave 10336 7573 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 10449 9289 M 182 0 R D gsave 10336 9040 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 10449 1737 M 91 0 R D 10449 2051 M 91 0 R D 10449 2366 M +91 0 R D 10449 2681 M 91 0 R D 10449 3310 M 91 0 R D 10449 3625 M 91 0 R D +10449 3940 M 91 0 R D 10449 4254 M 91 0 R D 10449 4884 M 91 0 R D +10449 5198 M 91 0 R D 10449 5513 M 91 0 R D 10449 5828 M 91 0 R D +10449 6457 M 91 0 R D 10449 6772 M 91 0 R D 10449 7086 M 91 0 R D +10449 7401 M 91 0 R D 10449 8030 M 91 0 R D 10449 8345 M 91 0 R D +10449 8660 M 91 0 R D 10449 8974 M 91 0 R D gsave 9882 5356 translate 0 0 M +90 rotate 1.01 dup scale -58.8433 0 N +( ) show grestore 19552 1422 M 0 7867 R D 19552 1422 M -182 0 R D +19552 2996 M -182 0 R D 19552 4569 M -182 0 R D 19552 6142 M -182 0 R D +19552 7716 M -182 0 R D 19552 9289 M -182 0 R D 19552 1737 M -91 0 R D +19552 2051 M -91 0 R D 19552 2366 M -91 0 R D 19552 2681 M -91 0 R D +19552 3310 M -91 0 R D 19552 3625 M -91 0 R D 19552 3940 M -91 0 R D +19552 4254 M -91 0 R D 19552 4884 M -91 0 R D 19552 5198 M -91 0 R D +19552 5513 M -91 0 R D 19552 5828 M -91 0 R D 19552 6457 M -91 0 R D +19552 6772 M -91 0 R D 19552 7086 M -91 0 R D 19552 7401 M -91 0 R D +19552 8030 M -91 0 R D 19552 8345 M -91 0 R D 19552 8660 M -91 0 R D +19552 8974 M -91 0 R D 40 setlinewidth 10449 1422 M 229 0 R 162 0 R 229 0 R +162 0 R 229 0 R 0 2199 R 163 0 R 229 0 R 0 -2199 R 162 0 R 229 0 R 163 0 R +229 0 R 162 0 R 229 0 R 0 1449 R 163 0 R 229 0 R 0 580 R 162 0 R 229 0 R +0 606 R 163 0 R 229 0 R 0 538 R 162 0 R 229 0 R 0 372 R 163 0 R 229 0 R +0 130 R 162 0 R 229 0 R 0 -140 R 163 0 R 229 0 R 0 -379 R 162 0 R 229 0 R +0 -541 R 163 0 R 229 0 R 0 -603 R 162 0 R 229 0 R 0 -575 R 163 0 R 229 0 R +0 -484 R 162 0 R 229 0 R 0 -366 R 163 0 R 229 0 R 0 -252 R 162 0 R 229 0 R +0 -157 R 162 0 R 229 0 R 0 -90 R 163 0 R 229 0 R 0 -48 R 162 0 R 99 0 R D +20 setlinewidth L3 10449 1438 M 229 0 R 0 23 R 162 0 R 229 0 R 0 47 R +162 0 R 229 0 R 0 90 R 163 0 R 229 0 R 0 159 R 162 0 R 229 0 R 0 253 R +163 0 R 229 0 R 0 371 R 162 0 R 229 0 R 0 490 R 163 0 R 229 0 R 0 580 R +162 0 R 229 0 R 0 606 R 163 0 R 229 0 R 0 538 R 162 0 R 229 0 R 0 372 R +163 0 R 229 0 R 0 130 R 162 0 R 229 0 R 0 -140 R 163 0 R 229 0 R 0 -379 R +162 0 R 229 0 R 0 -541 R 163 0 R 229 0 R 0 -603 R 162 0 R 229 0 R 0 -575 R +163 0 R 229 0 R 0 -484 R 162 0 R 229 0 R 0 -366 R 163 0 R 229 0 R 0 -252 R +162 0 R 229 0 R 0 -157 R 162 0 R 229 0 R 0 -90 R 163 0 R 229 0 R 0 -48 R +162 0 R 99 0 R D 1.000 0.000 0.000 setrgbcolor 11972 4578 M -2 22 R -4 21 R +-7 21 R -10 20 R -12 18 R -14 16 R -16 14 R -18 13 R -20 9 R -21 7 R -21 4 R +-22 2 R -21 -2 R -22 -4 R -20 -7 R -20 -9 R -18 -13 R -16 -14 R -15 -16 R +-12 -18 R -10 -20 R -7 -21 R -4 -21 R -1 -22 R 1 -21 R 4 -22 R 7 -20 R +10 -20 R 12 -18 R 15 -16 R 16 -15 R 18 -12 R 20 -9 R 20 -7 R 22 -5 R 21 -1 R +22 1 R 21 5 R 21 7 R 20 9 R 18 12 R 16 15 R 14 16 R 12 18 R 10 20 R 7 20 R +4 22 R 2 21 R F +12363 1422 M -1 22 R -4 21 R -7 21 R -10 19 R -12 18 R -14 17 R -17 14 R +-18 12 R -20 10 R -20 7 R -21 4 R -22 2 R -22 -2 R -21 -4 R -21 -7 R +-19 -10 R -19 -12 R -16 -14 R -14 -17 R -12 -18 R -10 -19 R -7 -21 R +-4 -21 R -2 -22 R 333 0 R F +12755 1422 M -2 22 R -4 21 R -7 21 R -10 19 R -12 18 R -14 17 R -16 14 R +-19 12 R -19 10 R -21 7 R -21 4 R -22 2 R -21 -2 R -22 -4 R -20 -7 R +-20 -10 R -18 -12 R -16 -14 R -15 -17 R -12 -18 R -10 -19 R -7 -21 R +-4 -21 R -1 -22 R 333 0 R F +13146 1422 M -1 22 R -4 21 R -7 21 R -10 19 R -12 18 R -15 17 R -16 14 R +-18 12 R -20 10 R -20 7 R -22 4 R -21 2 R -22 -2 R -21 -4 R -21 -7 R +-20 -10 R -18 -12 R -16 -14 R -14 -17 R -12 -18 R -10 -19 R -7 -21 R +-4 -21 R -2 -22 R 333 0 R F +13538 2116 M -2 22 R -4 22 R -7 20 R -10 20 R -12 18 R -14 16 R -16 15 R +-19 12 R -19 9 R -21 7 R -21 5 R -22 1 R -22 -1 R -21 -5 R -21 -7 R -19 -9 R +-18 -12 R -17 -15 R -14 -16 R -12 -18 R -10 -20 R -7 -20 R -4 -22 R -1 -22 R +1 -21 R 4 -22 R 7 -20 R 10 -20 R 12 -18 R 14 -16 R 17 -15 R 18 -12 R 19 -9 R +21 -7 R 21 -5 R 22 -1 R 22 1 R 21 5 R 21 7 R 19 9 R 19 12 R 16 15 R 14 16 R +12 18 R 10 20 R 7 20 R 4 22 R 2 21 R F +13929 2842 M -1 22 R -5 22 R -7 20 R -9 20 R -12 18 R -15 16 R -16 15 R +-18 12 R -20 9 R -20 7 R -22 5 R -21 1 R -22 -1 R -21 -5 R -21 -7 R -20 -9 R +-18 -12 R -16 -15 R -14 -16 R -13 -18 R -9 -20 R -7 -20 R -4 -22 R -2 -22 R +2 -21 R 4 -22 R 7 -20 R 9 -20 R 13 -18 R 14 -16 R 16 -15 R 18 -12 R 20 -9 R +21 -7 R 21 -5 R 22 -1 R 21 1 R 22 5 R 20 7 R 20 9 R 18 12 R 16 15 R 15 16 R +12 18 R 9 20 R 7 20 R 5 22 R 1 21 R F +14321 3631 M -2 22 R -4 22 R -7 20 R -10 20 R -12 18 R -14 16 R -16 15 R +-19 12 R -19 9 R -21 7 R -21 5 R -22 1 R -22 -1 R -21 -5 R -21 -7 R -19 -9 R +-18 -12 R -17 -15 R -14 -16 R -12 -18 R -10 -20 R -7 -20 R -4 -22 R -1 -22 R +1 -21 R 4 -22 R 7 -20 R 10 -20 R 12 -18 R 14 -16 R 17 -15 R 18 -12 R 19 -9 R +21 -7 R 21 -5 R 22 -1 R 22 1 R 21 5 R 21 7 R 19 9 R 19 12 R 16 15 R 14 16 R +12 18 R 10 20 R 7 20 R 4 22 R 2 21 R F +14712 2842 M -1 22 R -5 22 R -7 20 R -9 20 R -12 18 R -15 16 R -16 15 R +-18 12 R -20 9 R -20 7 R -22 5 R -21 1 R -22 -1 R -21 -5 R -21 -7 R -20 -9 R +-18 -12 R -16 -15 R -14 -16 R -13 -18 R -9 -20 R -7 -20 R -4 -22 R -2 -22 R +2 -21 R 4 -22 R 7 -20 R 9 -20 R 13 -18 R 14 -16 R 16 -15 R 18 -12 R 20 -9 R +21 -7 R 21 -5 R 22 -1 R 21 1 R 22 5 R 20 7 R 20 9 R 18 12 R 16 15 R 15 16 R +12 18 R 9 20 R 7 20 R 5 22 R 1 21 R F +15104 5367 M -2 22 R -4 21 R -7 21 R -10 20 R -12 18 R -14 16 R -17 14 R +-18 13 R -19 9 R -21 7 R -21 4 R -22 2 R -22 -2 R -21 -4 R -21 -7 R -19 -9 R +-18 -13 R -17 -14 R -14 -16 R -12 -18 R -10 -20 R -7 -21 R -4 -21 R -1 -22 R +1 -21 R 4 -22 R 7 -20 R 10 -20 R 12 -18 R 14 -16 R 17 -15 R 18 -12 R 19 -9 R +21 -7 R 21 -5 R 22 -1 R 22 1 R 21 5 R 21 7 R 19 9 R 18 12 R 17 15 R 14 16 R +12 18 R 10 20 R 7 20 R 4 22 R 2 21 R F +15495 5052 M -1 22 R -5 21 R -7 21 R -9 19 R -12 18 R -15 17 R -16 14 R +-18 12 R -20 10 R -20 7 R -22 4 R -21 1 R -22 -1 R -22 -4 R -20 -7 R +-20 -10 R -18 -12 R -16 -14 R -15 -17 R -12 -18 R -9 -19 R -7 -21 R -5 -21 R +-1 -22 R 1 -22 R 5 -21 R 7 -21 R 9 -19 R 12 -19 R 15 -16 R 16 -14 R 18 -12 R +20 -10 R 20 -7 R 22 -4 R 22 -2 R 21 2 R 22 4 R 20 7 R 20 10 R 18 12 R +16 14 R 15 16 R 12 19 R 9 19 R 7 21 R 5 21 R 1 22 R F +15887 5367 M -2 22 R -4 21 R -7 21 R -10 20 R -12 18 R -14 16 R -17 14 R +-18 13 R -19 9 R -21 7 R -21 4 R -22 2 R -22 -2 R -21 -4 R -21 -7 R -19 -9 R +-18 -13 R -17 -14 R -14 -16 R -12 -18 R -10 -20 R -7 -21 R -4 -21 R -1 -22 R +1 -21 R 4 -22 R 7 -20 R 10 -20 R 12 -18 R 14 -16 R 17 -15 R 18 -12 R 19 -9 R +21 -7 R 21 -5 R 22 -1 R 22 1 R 21 5 R 21 7 R 19 9 R 18 12 R 17 15 R 14 16 R +12 18 R 10 20 R 7 20 R 4 22 R 2 21 R F +16278 5367 M -1 22 R -5 21 R -7 21 R -9 20 R -12 18 R -15 16 R -16 14 R +-18 13 R -20 9 R -20 7 R -22 4 R -21 2 R -22 -2 R -22 -4 R -20 -7 R -20 -9 R +-18 -13 R -16 -14 R -15 -16 R -12 -18 R -9 -20 R -7 -21 R -5 -21 R -1 -22 R +1 -21 R 5 -22 R 7 -20 R 9 -20 R 12 -18 R 15 -16 R 16 -15 R 18 -12 R 20 -9 R +20 -7 R 22 -5 R 22 -1 R 21 1 R 22 5 R 20 7 R 20 9 R 18 12 R 16 15 R 15 16 R +12 18 R 9 20 R 7 20 R 5 22 R 1 21 R F +16669 2527 M -1 22 R -4 21 R -7 21 R -10 19 R -12 18 R -14 17 R -17 14 R +-18 12 R -19 10 R -21 7 R -21 4 R -22 1 R -22 -1 R -21 -4 R -21 -7 R +-19 -10 R -18 -12 R -17 -14 R -14 -17 R -12 -18 R -10 -19 R -7 -21 R +-4 -21 R -2 -22 R 2 -22 R 4 -21 R 7 -21 R 10 -19 R 12 -19 R 14 -16 R +17 -14 R 18 -12 R 19 -10 R 21 -7 R 21 -4 R 22 -2 R 22 2 R 21 4 R 21 7 R +19 10 R 18 12 R 17 14 R 14 16 R 12 19 R 10 19 R 7 21 R 4 21 R 1 22 R F +17061 4263 M -1 21 R -5 22 R -7 20 R -9 20 R -12 18 R -15 16 R -16 15 R +-18 12 R -20 10 R -20 7 R -22 4 R -22 1 R -21 -1 R -22 -4 R -20 -7 R +-20 -10 R -18 -12 R -16 -15 R -15 -16 R -12 -18 R -9 -20 R -7 -20 R -5 -22 R +-1 -21 R 1 -22 R 5 -21 R 7 -21 R 9 -20 R 12 -18 R 15 -16 R 16 -14 R 18 -12 R +20 -10 R 20 -7 R 22 -4 R 21 -2 R 22 2 R 22 4 R 20 7 R 20 10 R 18 12 R +16 14 R 15 16 R 12 18 R 9 20 R 7 21 R 5 21 R 1 22 R F +17452 4263 M -1 21 R -4 22 R -7 20 R -10 20 R -12 18 R -14 16 R -17 15 R +-18 12 R -19 10 R -21 7 R -21 4 R -22 1 R -22 -1 R -21 -4 R -21 -7 R +-19 -10 R -18 -12 R -17 -15 R -14 -16 R -12 -18 R -10 -20 R -7 -20 R +-4 -22 R -2 -21 R 2 -22 R 4 -21 R 7 -21 R 10 -20 R 12 -18 R 14 -16 R +17 -14 R 18 -12 R 19 -10 R 21 -7 R 21 -4 R 22 -2 R 22 2 R 21 4 R 21 7 R +19 10 R 18 12 R 17 14 R 14 16 R 12 18 R 10 20 R 7 21 R 4 21 R 1 22 R F +17844 1422 M -2 22 R -4 21 R -7 21 R -9 19 R -13 18 R -14 17 R -16 14 R +-18 12 R -20 10 R -21 7 R -21 4 R -22 2 R -21 -2 R -22 -4 R -20 -7 R +-20 -10 R -18 -12 R -16 -14 R -15 -17 R -12 -18 R -9 -19 R -7 -21 R -5 -21 R +-1 -22 R 333 0 R F +18235 1738 M -1 21 R -4 22 R -7 20 R -10 20 R -12 18 R -14 16 R -17 15 R +-18 12 R -19 10 R -21 7 R -21 4 R -22 1 R -22 -1 R -21 -4 R -21 -7 R +-19 -10 R -18 -12 R -17 -15 R -14 -16 R -12 -18 R -10 -20 R -7 -20 R +-4 -22 R -2 -21 R 2 -22 R 4 -21 R 7 -21 R 10 -19 R 12 -19 R 14 -16 R +17 -14 R 18 -12 R 19 -10 R 21 -7 R 21 -4 R 22 -2 R 22 2 R 21 4 R 21 7 R +19 10 R 18 12 R 17 14 R 14 16 R 12 19 R 10 19 R 7 21 R 4 21 R 1 22 R F +L0 11760 4002 M 91 0 R -46 0 R 0 1153 R -45 0 R 91 0 R D 12151 1422 M 91 0 R +-45 0 R -46 0 R 91 0 R D 12543 1422 M 91 0 R -46 0 R -45 0 R 91 0 R D +12934 1422 M 91 0 R -45 0 R -46 0 R 91 0 R D 13326 1846 M 91 0 R -46 0 R +0 541 R -45 0 R 91 0 R D 13717 2456 M 91 0 R -45 0 R 0 773 R -46 0 R 91 0 R +D 14109 3149 M 91 0 R -46 0 R 0 965 R -45 0 R 91 0 R D 14500 2456 M 91 0 R +-45 0 R 0 773 R -46 0 R 91 0 R D 14892 4723 M 91 0 R -46 0 R 0 1289 R +-45 0 R 91 0 R D 15283 4434 M 91 0 R -45 0 R 0 1236 R -46 0 R 91 0 R D +15675 4723 M 91 0 R -46 0 R 0 1289 R -45 0 R 91 0 R D 16066 4723 M 91 0 R +-45 0 R 0 1289 R -46 0 R 91 0 R D 16457 2186 M 91 0 R -45 0 R 0 682 R +-46 0 R 91 0 R D 16849 3716 M 91 0 R -46 0 R 0 1093 R -45 0 R 91 0 R D +17240 3716 M 91 0 R -45 0 R 0 1093 R -46 0 R 91 0 R D 17632 1422 M 91 0 R +-46 0 R -45 0 R 91 0 R D 18023 1556 M 91 0 R -45 0 R 0 364 R -46 0 R 91 0 R +D 0.000 0.282 1.000 setrgbcolor 11582 3714 M 0 333 R 333 0 R 0 -333 R +-333 0 R F +12233 1422 M 0 261 R 333 0 R 0 -261 R F +12883 2201 M 0 333 R 333 0 R 0 -333 R -333 0 R F +13533 2768 M 0 333 R 333 0 R 0 -333 R -333 0 R F +14183 4300 M 0 333 R 333 0 R 0 -333 R -333 0 R F +14834 5377 M 0 333 R 333 0 R 0 -333 R -333 0 R F +15484 6701 M 0 333 R 333 0 R 0 -333 R -333 0 R F +16134 2390 M 0 333 R 333 0 R 0 -333 R -333 0 R F +16784 1445 M 0 333 R 333 0 R 0 -333 R -333 0 R F +11703 3379 M 92 0 R -46 0 R 0 1002 R -46 0 R 92 0 R D 12399 1422 M 0 193 R +-45 0 R 91 0 R D 13004 2057 M 91 0 R -46 0 R 0 621 R -45 0 R 91 0 R D +13654 2542 M 91 0 R -45 0 R 0 786 R -46 0 R 91 0 R D 14304 3908 M 91 0 R +-45 0 R 0 1116 R -46 0 R 91 0 R D 14955 4895 M 91 0 R -46 0 R 0 1298 R +-45 0 R 91 0 R D 15605 6121 M 91 0 R -46 0 R 0 1493 R -45 0 R 91 0 R D +16255 2216 M 91 0 R -45 0 R 0 681 R -46 0 R 91 0 R D 16905 1472 M 91 0 R +-45 0 R 0 278 R -46 0 R 91 0 R D 10 setlinewidth 11523 5761 M 0 333 R +333 0 R 0 -333 R -333 0 R D 12173 1422 M 0 167 R 333 0 R 0 -167 R D +12823 2047 M 0 333 R 333 0 R 0 -333 R -333 0 R D 13474 3103 M 0 333 R +333 0 R 0 -333 R -333 0 R D 14124 4140 M 0 333 R 333 0 R 0 -333 R -333 0 R D +14774 4234 M 0 333 R 333 0 R 0 -333 R -333 0 R D 15424 6157 M 0 333 R +333 0 R 0 -333 R -333 0 R D 16075 2198 M 0 333 R 333 0 R 0 -333 R -333 0 R D +16725 1422 M 0 261 R 333 0 R 0 -261 R D 20 setlinewidth 11644 5250 M 91 0 R +-46 0 R 0 1355 R -45 0 R 91 0 R D 12294 1422 M 91 0 R -45 0 R -46 0 R 91 0 R +D 12944 1930 M 91 0 R -45 0 R 0 568 R -46 0 R 91 0 R D 13595 2836 M 91 0 R +-46 0 R 0 867 R -45 0 R 91 0 R D 14245 3764 M 91 0 R -46 0 R 0 1084 R +-45 0 R 91 0 R D 14895 3850 M 91 0 R -45 0 R 0 1102 R -46 0 R 91 0 R D +15545 5617 M 91 0 R -45 0 R 0 1413 R -46 0 R 91 0 R D 16196 2055 M 91 0 R +-46 0 R 0 620 R -45 0 R 91 0 R D 16891 1422 M 0 192 R -45 0 R 91 0 R D +0.000 0.000 0.000 setrgbcolor gsave 12140 8660 translate 0 0 M 1.2 dup scale +(X-ray) show grestore L2 11619 1422 M 69 0 R 0 7867 R D 11818 9289 M +0 -7858 R 61 0 R 69 0 R 0 8 R 61 0 R 69 0 R 0 8 R 61 0 R 69 0 R 0 9 R 61 0 R +69 0 R 0 1 R 61 0 R 69 0 R 0 -1 R 61 0 R 69 0 R 0 -2 R 61 0 R 69 0 R 0 -1 R +61 0 R 69 0 R 0 -2 R 61 0 R 69 0 R 0 -1 R 61 0 R 69 0 R 0 -2 R 61 0 R 69 0 R +0 13 R 62 0 R 68 0 R 0 84 R 62 0 R 68 0 R 0 84 R 62 0 R 68 0 R 0 85 R 62 0 R +68 0 R 0 185 R 62 0 R 68 0 R 0 246 R 62 0 R 69 0 R 0 337 R 61 0 R 69 0 R +0 420 R 61 0 R 69 0 R 0 490 R 61 0 R 69 0 R 0 532 R 61 0 R 69 0 R 0 538 R +61 0 R 69 0 R 0 513 R 61 0 R 69 0 R 0 471 R 61 0 R 69 0 R 0 419 R 61 0 R +69 0 R 0 367 R 61 0 R 69 0 R 0 320 R 61 0 R 69 0 R 0 278 R 61 0 R 69 0 R +0 242 R 61 0 R 69 0 R 0 213 R 61 0 R 69 0 R 0 188 R 61 0 R 69 0 R 0 170 R +61 0 R 69 0 R 0 154 R 61 0 R 69 0 R 0 141 R 62 0 R 68 0 R 0 133 R 62 0 R +68 0 R 0 126 R 62 0 R 68 0 R 0 123 R 62 0 R 68 0 R 0 121 R 62 0 R 68 0 R +0 122 R 62 0 R 68 0 R 0 126 R 62 0 R 69 0 R 0 -7267 R 61 0 R D L1 +11619 1422 M 69 0 R 61 0 R 69 0 R 0 1 R 61 0 R 69 0 R 61 0 R 69 0 R 61 0 R +69 0 R 0 1 R 61 0 R 69 0 R 61 0 R 69 0 R 0 1 R 61 0 R 69 0 R 0 1 R 61 0 R +69 0 R 0 1 R 61 0 R 69 0 R 0 3 R 61 0 R 69 0 R 0 3 R 61 0 R 69 0 R 0 5 R +61 0 R 69 0 R 0 10 R 62 0 R 68 0 R 0 20 R 62 0 R 68 0 R 0 28 R 62 0 R 68 0 R +0 41 R 62 0 R 68 0 R 0 64 R 62 0 R 68 0 R 0 81 R 62 0 R 69 0 R 0 104 R +61 0 R 69 0 R 0 129 R 61 0 R 69 0 R 0 171 R 61 0 R 69 0 R 0 208 R 61 0 R +69 0 R 0 226 R 61 0 R 69 0 R 0 245 R 61 0 R 69 0 R 0 279 R 61 0 R 69 0 R +0 309 R 61 0 R 69 0 R 0 325 R 61 0 R 69 0 R 0 343 R 61 0 R 69 0 R 0 371 R +61 0 R 69 0 R 0 375 R 61 0 R 69 0 R 0 401 R 61 0 R 69 0 R 0 412 R 61 0 R +69 0 R 0 421 R 61 0 R 69 0 R 0 431 R 61 0 R 69 0 R 0 442 R 62 0 R 68 0 R +0 453 R 62 0 R 68 0 R 0 464 R 62 0 R 68 0 R 0 487 R 62 0 R 68 0 R 0 531 R +62 0 R 68 0 R 0 480 R D 17020 9289 M 0 -7867 R 61 0 R D +%%PageTrailer +end +restore +showpage +%%PageResources: font Helvetica +%%+ font AvantGarde-Book +%%Trailer +restore +%%Pages: 1 +%%DocumentNeededResources: font Helvetica +%%+ font AvantGarde-Book +%%EOF diff --git a/feedback/papers/0506398/f13.ps b/feedback/papers/0506398/f13.ps new file mode 100644 index 0000000..2031ac2 --- /dev/null +++ b/feedback/papers/0506398/f13.ps @@ -0,0 +1,822 @@ +%!PS-Adobe-3.0 +%%BoundingBox: 54 360 558 720 +%%Title: Graphics produced by IDL +%%For: phopkins@dhcp152-235.cfa.harvard.edu, +%% /Users/phopkins/Documents/lars_galaxies/plots/LF_massive +%%Creator: IDL Student Edition 6.0.3, Mac OS X (darwin ppc m32) +%%CreationDate: Sun Aug 28 22:28:04 2005 +%%DocumentData: Clean7bit +%%Requirements: color +%%LanguageLevel: 1 +%%PageOrder: Ascend +%%Pages: (atend) +%%DocumentNeededResources: (atend) +%%EndComments +%%BeginProlog +save +%+ prolog.ps -- Prolog for IDL generated PostScript files +%+ Copyright (c) 1988-2003 Research Systems, Inc. All Rights Reserved. +%v 4 +/$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C +{currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint +stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} +bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show +grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 +setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 +{[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 +100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 +{[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef +/ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} +ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont +exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica +findfont exch scalefont setfont (\267) show currentpoint grestore moveto} +bdef end 2.5 setmiterlimit +%%EndProlog +%%Page: 0 1 +%%PageRequirements: color +%%PageResources: (atend) +%%PageOrientation: Portrait +%%PageBoundingBox: 54 360 558 720 +%%BeginPageSetup +save +$IDL_DICT begin 54 360 translate 0.0283465 dup scale +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +%%EndPageSetup +15 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 2242 8467 M 7433 0 R D +3304 8467 M 0 70 R D gsave 3304 7933 translate 0 0 M 1.01 dup scale +-58.8433 0 N +( ) show grestore 5428 8467 M 0 70 R D gsave 5428 7933 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 7551 8467 M 0 70 R D gsave 7551 7933 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 9675 8467 M 0 70 R D gsave 9675 7933 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 2455 8467 M 0 35 R D 2879 8467 M 0 35 R D 3729 8467 M +0 35 R D 4154 8467 M 0 35 R D 4578 8467 M 0 35 R D 5003 8467 M 0 35 R D +5852 8467 M 0 35 R D 6277 8467 M 0 35 R D 6702 8467 M 0 35 R D 7127 8467 M +0 35 R D 7976 8467 M 0 35 R D 8401 8467 M 0 35 R D 8825 8467 M 0 35 R D +9250 8467 M 0 35 R D gsave 5959 7471 translate 0 0 M 1.01 dup scale +-58.8433 0 N +( ) show grestore 2242 11989 M 7433 0 R D 3304 11989 M 0 -70 R D +5428 11989 M 0 -70 R D 7551 11989 M 0 -70 R D 9675 11989 M 0 -70 R D +2455 11989 M 0 -35 R D 2879 11989 M 0 -35 R D 3729 11989 M 0 -35 R D +4154 11989 M 0 -35 R D 4578 11989 M 0 -35 R D 5003 11989 M 0 -35 R D +5852 11989 M 0 -35 R D 6277 11989 M 0 -35 R D 6702 11989 M 0 -35 R D +7127 11989 M 0 -35 R D 7976 11989 M 0 -35 R D 8401 11989 M 0 -35 R D +8825 11989 M 0 -35 R D 9250 11989 M 0 -35 R D 2242 8467 M 0 3522 R D +2242 8846 M 149 0 R D gsave 2130 8703 translate 0 0 M 1.01 dup scale +-616.678 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(8) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 2242 9798 M 149 0 R D +gsave 2130 9656 translate 0 0 M 1.01 dup scale -616.678 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(9) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 2242 10750 M 149 0 R D +gsave 2130 10608 translate 0 0 M 1.01 dup scale -762.61 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(10) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 2242 11702 M 149 0 R D +gsave 2130 11560 translate 0 0 M 1.01 dup scale -762.61 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(11) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 2242 8467 M 75 0 R D 2242 8559 M 75 0 R D +2242 8634 M 75 0 R D 2242 8698 M 75 0 R D 2242 8753 M 75 0 R D 2242 8802 M +75 0 R D 2242 9132 M 75 0 R D 2242 9300 M 75 0 R D 2242 9419 M 75 0 R D +2242 9511 M 75 0 R D 2242 9587 M 75 0 R D 2242 9650 M 75 0 R D 2242 9706 M +75 0 R D 2242 9754 M 75 0 R D 2242 10085 M 75 0 R D 2242 10252 M 75 0 R D +2242 10371 M 75 0 R D 2242 10463 M 75 0 R D 2242 10539 M 75 0 R D +2242 10603 M 75 0 R D 2242 10658 M 75 0 R D 2242 10707 M 75 0 R D +2242 11037 M 75 0 R D 2242 11204 M 75 0 R D 2242 11323 M 75 0 R D +2242 11416 M 75 0 R D 2242 11491 M 75 0 R D 2242 11555 M 75 0 R D +2242 11610 M 75 0 R D 2242 11659 M 75 0 R D 2242 11989 M 75 0 R D +gsave 1024 10228 translate 0 0 M 90 rotate 1.01 dup scale -58.8433 0 N +( ) show grestore 9675 8467 M 0 3522 R D 9675 8846 M -149 0 R D 9675 9798 M +-149 0 R D 9675 10750 M -149 0 R D 9675 11702 M -149 0 R D 9675 8467 M +-74 0 R D 9675 8559 M -74 0 R D 9675 8634 M -74 0 R D 9675 8698 M -74 0 R D +9675 8753 M -74 0 R D 9675 8802 M -74 0 R D 9675 9132 M -74 0 R D +9675 9300 M -74 0 R D 9675 9419 M -74 0 R D 9675 9511 M -74 0 R D +9675 9587 M -74 0 R D 9675 9650 M -74 0 R D 9675 9706 M -74 0 R D +9675 9754 M -74 0 R D 9675 10085 M -74 0 R D 9675 10252 M -74 0 R D +9675 10371 M -74 0 R D 9675 10463 M -74 0 R D 9675 10539 M -74 0 R D +9675 10603 M -74 0 R D 9675 10658 M -74 0 R D 9675 10707 M -74 0 R D +9675 11037 M -74 0 R D 9675 11204 M -74 0 R D 9675 11323 M -74 0 R D +9675 11416 M -74 0 R D 9675 11491 M -74 0 R D 9675 11555 M -74 0 R D +9675 11610 M -74 0 R D 9675 11659 M -74 0 R D 9675 11989 M -74 0 R D +40 setlinewidth 2242 8915 M 152 17 R 607 120 R 606 261 R 607 103 R 607 182 R +607 24 R 303 132 R 303 -35 R 122 7 R 121 6 R 61 39 R 60 -115 R 61 100 R +61 23 R 60 -71 R 61 -26 R 31 -89 R 30 151 R 30 -25 R 31 24 R 30 -81 R +30 43 R 30 15 R 31 -47 R 30 -75 R 31 32 R 30 271 R 30 148 R 31 -45 R 30 50 R +30 -172 R 31 -57 R 30 -145 R 30 254 R 31 292 R 30 95 R 30 -386 R 31 216 R +30 -117 R 30 399 R 31 135 R 30 -52 R 30 -192 R 31 195 R 30 -236 R 30 264 R +31 152 R 30 -207 R 30 -117 R 31 -12 R 30 155 R 30 2 R 31 -278 R 30 141 R +30 -214 R 31 168 R 30 204 R 30 -385 R 31 -21 R 30 -97 R 30 -135 R 31 127 R +30 -54 R 30 -71 R 31 58 R 30 -34 R 30 -174 R 31 39 R 30 -49 R 30 28 R +31 -77 R 30 -96 R 30 100 R 31 -98 R 30 -112 R 30 78 R 31 -34 R 30 11 R +30 21 R 31 -91 R 30 -151 R 30 72 R 31 -86 R 30 -76 R 30 20 R 31 -46 R +30 18 R 30 42 R 31 -98 R 30 -35 R 30 107 R 31 -43 R 30 -36 R 30 -50 R +31 59 R 30 64 R 61 -174 R 60 -4 R 61 86 R 61 -91 R 60 -114 R 61 -28 R +61 -29 R 61 41 R 60 -78 R 60 90 R D 10 setlinewidth 2242 11248 M 152 -28 R +607 -137 R 606 -111 R 607 -78 R 607 -85 R 607 -80 R 303 -31 R 303 78 R +122 -56 R 121 31 R 61 -23 R 60 -30 R 61 -12 R 61 8 R 60 30 R 61 -46 R +31 96 R 30 -23 R 30 -50 R 31 44 R 30 -55 R 30 158 R 30 -5 R 31 -109 R +30 -55 R 31 -43 R 30 -11 R 30 63 R 31 134 R 30 -2 R 30 19 R 31 -7 R 30 -14 R +30 -13 R 31 -2 R 30 52 R 30 -43 R 31 -15 R 30 9 R 30 -20 R 31 -34 R 30 8 R +30 -8 R 31 40 R 30 27 R 30 -54 R 31 -26 R 30 40 R 30 -10 R 31 -38 R 30 -7 R +30 -21 R 31 -9 R 30 7 R 30 21 R 31 31 R 30 -20 R 30 -14 R 31 5 R 30 -5 R +30 -3 R 31 -4 R 30 13 R 30 14 R 31 11 R 30 -34 R 30 -4 R 31 53 R 30 -23 R +30 11 R 31 -17 R 30 30 R 30 -14 R 31 93 R 30 -27 R 30 -42 R 31 -12 R +30 -16 R 30 49 R 31 24 R 30 -5 R 30 -12 R 31 -6 R 30 -12 R 30 25 R 31 20 R +30 -11 R 30 -40 R 31 -7 R 30 0 R 30 1 R 31 -1 R 30 34 R 30 14 R 31 -31 R +30 8 R 61 -16 R 60 10 R 61 -19 R 61 8 R 60 -2 R 61 6 R 61 8 R 61 23 R +60 -37 R 60 -43 R D L1 2242 10971 M 152 0 R 607 -108 R 606 -90 R 607 -59 R +607 -75 R 607 -121 R 303 -23 R 303 136 R 122 -72 R 121 50 R 61 -32 R +60 -38 R 61 -13 R 61 2 R 60 52 R 61 -60 R 31 134 R 30 -33 R 30 -69 R 31 62 R +30 -72 R 30 214 R 30 -8 R 31 -142 R 30 -64 R 31 -57 R 30 -7 R 30 85 R +31 146 R 30 -1 R 30 18 R 31 -9 R 30 -22 R 30 -12 R 31 4 R 30 70 R 30 -63 R +31 -13 R 30 13 R 30 -32 R 31 -34 R 30 5 R 30 -7 R 31 50 R 30 36 R 30 -67 R +31 -32 R 30 52 R 30 -11 R 31 -48 R 30 -14 R 30 -20 R 31 -8 R 30 2 R 30 24 R +31 42 R 30 -31 R 30 -15 R 31 8 R 30 -7 R 30 -2 R 31 -14 R 30 20 R 30 20 R +31 14 R 30 -49 R 30 0 R 31 62 R 30 -33 R 30 11 R 31 -17 R 30 43 R 30 -23 R +31 127 R 30 -39 R 30 -57 R 31 -14 R 30 -18 R 30 60 R 31 24 R 30 -8 R +30 -18 R 31 -1 R 30 -14 R 30 32 R 31 23 R 30 -15 R 30 -51 R 31 -9 R 30 -5 R +30 2 R 31 -3 R 30 46 R 30 15 R 31 -31 R 30 1 R 61 -23 R 60 6 R 61 -21 R +61 9 R 60 0 R 61 10 R 61 1 R 61 32 R 60 -48 R 60 -49 R D +gsave 2455 11416 translate 0 0 M 1.1 dup scale +(M) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(BH) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(=3) show +%%IncludeResource: font Symbol +423.333 /Symbol STDFONT +(\264) show +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(7) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( M) show CP X -101.051 M +%%IncludeResource: font AvantGarde-Book +262.467 /AvantGarde-Book STDFONT +(O) show M X -58.3193 M +%%IncludeResource: font AvantGarde-Book +186.267 /AvantGarde-Book STDFONT +( \267) show +%%IncludeResource: font Helvetica +186.267 /Helvetica STDFONT grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT L0 1.000 0.000 0.000 setrgbcolor 2242 10247 M +213 54 R 424 165 R 425 -24 R 425 -87 R 425 -138 R 424 79 R 425 -66 R +425 35 R 424 105 R 425 -60 R 425 -15 R 425 -69 R 424 -74 R 425 -61 R +425 -51 R 424 -45 R 425 -35 R 424 -34 R D 0.000 0.514 1.000 setrgbcolor +2242 10562 M 152 -40 R 303 121 R 304 5 R 303 26 R 303 2 R 304 -10 R +303 -130 R 304 10 R 303 79 R 303 -34 R 304 25 R 303 -64 R 303 24 R 304 -97 R +303 173 R 304 9 R 303 -47 R 303 -108 R 304 -40 R 303 -10 R 303 29 R 304 37 R +303 21 R 303 50 R 303 -7 R D 15 setlinewidth 0.000 0.000 0.000 setrgbcolor +9675 8467 M 7432 0 R D 10737 8467 M 0 70 R D +gsave 10737 7933 translate 0 0 M 1.01 dup scale -58.8433 0 N +( ) show grestore 12860 8467 M 0 70 R D gsave 12860 7933 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 14984 8467 M 0 70 R D gsave 14984 7933 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 17107 8467 M 0 70 R D gsave 17107 7933 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 9887 8467 M 0 35 R D 10312 8467 M 0 35 R D 11161 8467 M +0 35 R D 11586 8467 M 0 35 R D 12011 8467 M 0 35 R D 12436 8467 M 0 35 R D +13285 8467 M 0 35 R D 13710 8467 M 0 35 R D 14134 8467 M 0 35 R D +14559 8467 M 0 35 R D 15409 8467 M 0 35 R D 15833 8467 M 0 35 R D +16258 8467 M 0 35 R D 16683 8467 M 0 35 R D gsave 13391 7471 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 9675 11989 M 7432 0 R D 10737 11989 M 0 -70 R D +12860 11989 M 0 -70 R D 14984 11989 M 0 -70 R D 17107 11989 M 0 -70 R D +9887 11989 M 0 -35 R D 10312 11989 M 0 -35 R D 11161 11989 M 0 -35 R D +11586 11989 M 0 -35 R D 12011 11989 M 0 -35 R D 12436 11989 M 0 -35 R D +13285 11989 M 0 -35 R D 13710 11989 M 0 -35 R D 14134 11989 M 0 -35 R D +14559 11989 M 0 -35 R D 15409 11989 M 0 -35 R D 15833 11989 M 0 -35 R D +16258 11989 M 0 -35 R D 16683 11989 M 0 -35 R D 9675 8467 M 0 3522 R D +9675 8846 M 149 0 R D gsave 9563 8703 translate 0 0 M 1.01 dup scale +-117.687 0 N +( ) show grestore 9675 9798 M 149 0 R D gsave 9563 9656 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9675 10750 M 149 0 R D gsave 9563 10608 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9675 11702 M 149 0 R D gsave 9563 11560 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9675 8467 M 74 0 R D 9675 8559 M 74 0 R D 9675 8634 M +74 0 R D 9675 8698 M 74 0 R D 9675 8753 M 74 0 R D 9675 8802 M 74 0 R D +9675 9132 M 74 0 R D 9675 9300 M 74 0 R D 9675 9419 M 74 0 R D 9675 9511 M +74 0 R D 9675 9587 M 74 0 R D 9675 9650 M 74 0 R D 9675 9706 M 74 0 R D +9675 9754 M 74 0 R D 9675 10085 M 74 0 R D 9675 10252 M 74 0 R D +9675 10371 M 74 0 R D 9675 10463 M 74 0 R D 9675 10539 M 74 0 R D +9675 10603 M 74 0 R D 9675 10658 M 74 0 R D 9675 10707 M 74 0 R D +9675 11037 M 74 0 R D 9675 11204 M 74 0 R D 9675 11323 M 74 0 R D +9675 11416 M 74 0 R D 9675 11491 M 74 0 R D 9675 11555 M 74 0 R D +9675 11610 M 74 0 R D 9675 11659 M 74 0 R D 9675 11989 M 74 0 R D +gsave 9108 10228 translate 0 0 M 90 rotate 1.01 dup scale -58.8433 0 N +( ) show grestore 17107 8467 M 0 3522 R D 17107 8846 M -148 0 R D +17107 9798 M -148 0 R D 17107 10750 M -148 0 R D 17107 11702 M -148 0 R D +17107 8467 M -74 0 R D 17107 8559 M -74 0 R D 17107 8634 M -74 0 R D +17107 8698 M -74 0 R D 17107 8753 M -74 0 R D 17107 8802 M -74 0 R D +17107 9132 M -74 0 R D 17107 9300 M -74 0 R D 17107 9419 M -74 0 R D +17107 9511 M -74 0 R D 17107 9587 M -74 0 R D 17107 9650 M -74 0 R D +17107 9706 M -74 0 R D 17107 9754 M -74 0 R D 17107 10085 M -74 0 R D +17107 10252 M -74 0 R D 17107 10371 M -74 0 R D 17107 10463 M -74 0 R D +17107 10539 M -74 0 R D 17107 10603 M -74 0 R D 17107 10658 M -74 0 R D +17107 10707 M -74 0 R D 17107 11037 M -74 0 R D 17107 11204 M -74 0 R D +17107 11323 M -74 0 R D 17107 11416 M -74 0 R D 17107 11491 M -74 0 R D +17107 11555 M -74 0 R D 17107 11610 M -74 0 R D 17107 11659 M -74 0 R D +17107 11989 M -74 0 R D 40 setlinewidth 9674 9179 M 153 61 R 606 195 R +607 305 R 607 73 R 607 152 R 606 -13 R 304 135 R 303 -98 R 121 29 R 122 29 R +60 64 R 61 -195 R 61 28 R 60 40 R 61 -60 R 61 6 R 30 -121 R 30 163 R +31 -42 R 30 52 R 30 -115 R 31 68 R 30 -12 R 30 -59 R 31 -64 R 30 78 R +30 354 R 31 133 R 30 259 R 30 25 R 31 -107 R 30 39 R 30 -14 R 31 132 R +30 365 R 30 83 R 31 -40 R 30 109 R 30 -256 R 31 263 R 30 130 R 30 -181 R +31 -103 R 30 120 R 31 -378 R 30 164 R 30 165 R 31 -235 R 30 -94 R 30 -69 R +31 123 R 30 6 R 30 -317 R 31 130 R 30 -233 R 30 142 R 31 186 R 30 -421 R +30 -29 R 31 -122 R 30 -167 R 30 127 R 31 -50 R 30 -59 R 30 51 R 31 -69 R +30 -156 R 30 32 R 31 -75 R 30 37 R 30 -81 R 31 -111 R 30 110 R 30 -116 R +31 -96 R 30 84 R 30 -54 R 31 20 R 30 15 R 30 -94 R 31 -148 R 30 53 R +30 -83 R 31 -68 R 30 19 R 30 -46 R 31 6 R 30 46 R 30 -79 R 31 -43 R 30 94 R +30 -34 R 31 -18 R 30 -58 R 30 33 R 31 67 R 60 -168 R 61 -8 R 61 87 R +60 -112 R 61 -125 R 61 -21 R 60 -30 R 61 31 R 61 -72 R 60 82 R D +10 setlinewidth 9674 11752 M 153 -5 R 606 -44 R 607 -13 R 607 -15 R +607 -57 R 606 -56 R 304 -40 R 303 45 R 121 -46 R 122 40 R 60 -24 R 61 -28 R +61 -5 R 60 3 R 61 9 R 61 -29 R 30 69 R 30 -22 R 31 -34 R 30 64 R 30 -49 R +31 111 R 30 1 R 30 -75 R 31 -13 R 30 -24 R 30 21 R 31 39 R 30 109 R 30 -14 R +31 -26 R 30 -50 R 30 -15 R 31 -9 R 30 70 R 30 128 R 31 -88 R 30 -21 R +30 -18 R 31 41 R 30 -62 R 30 69 R 31 -50 R 30 32 R 31 35 R 30 -53 R 30 -10 R +31 18 R 30 -15 R 30 -43 R 31 12 R 30 -37 R 30 5 R 31 -5 R 30 -10 R 30 34 R +31 -28 R 30 -28 R 30 1 R 31 -19 R 30 -2 R 30 -13 R 31 15 R 30 13 R 30 9 R +31 -37 R 30 -4 R 30 50 R 31 -42 R 30 -14 R 30 -16 R 31 33 R 30 -11 R +30 120 R 31 -56 R 30 -52 R 30 -19 R 31 -11 R 30 38 R 30 16 R 31 -9 R +30 -20 R 30 -14 R 31 0 R 30 29 R 30 2 R 31 -4 R 30 -40 R 30 -16 R 31 -5 R +30 -6 R 30 -10 R 31 21 R 30 8 R 30 -29 R 31 3 R 60 -25 R 61 -12 R 61 -10 R +60 -9 R 61 -1 R 61 27 R 60 -15 R 61 19 R 61 -40 R 60 -14 R D L1 9674 11446 M +153 22 R 606 13 R 607 25 R 607 17 R 607 -57 R 606 -75 R 304 -41 R 303 85 R +121 -60 R 122 59 R 60 -31 R 61 -37 R 61 -5 R 60 5 R 61 15 R 61 -39 R 30 95 R +30 -29 R 31 -46 R 30 88 R 30 -66 R 31 147 R 30 1 R 30 -96 R 31 -17 R +30 -32 R 30 29 R 31 52 R 30 137 R 30 -16 R 31 -33 R 30 -62 R 30 -19 R +31 -11 R 30 89 R 30 154 R 31 -104 R 30 -25 R 30 -21 R 31 50 R 30 -76 R +30 85 R 31 -60 R 30 40 R 31 42 R 30 -63 R 30 -11 R 31 22 R 30 -18 R 30 -52 R +31 16 R 30 -45 R 30 7 R 31 -5 R 30 -13 R 30 43 R 31 -33 R 30 -34 R 30 2 R +31 -24 R 30 -2 R 30 -17 R 31 20 R 30 18 R 30 11 R 31 -46 R 30 -5 R 30 62 R +31 -51 R 30 -17 R 30 -20 R 31 41 R 30 -13 R 30 147 R 31 -67 R 30 -64 R +30 -24 R 31 -13 R 30 49 R 30 20 R 31 -11 R 30 -25 R 30 -17 R 31 0 R 30 37 R +30 2 R 31 -4 R 30 -51 R 30 -19 R 31 -7 R 30 -7 R 30 -12 R 31 27 R 30 10 R +30 -36 R 31 4 R 60 -32 R 61 -16 R 61 -12 R 60 -12 R 61 0 R 61 37 R 60 -20 R +61 25 R 61 -51 R 60 -19 R D L0 1.000 0.000 0.000 setrgbcolor 9674 10277 M +213 67 R 425 244 R 425 219 R 424 61 R 425 -219 R 425 -103 R 425 -139 R +424 -24 R 425 211 R 425 -143 R 424 -127 R 425 -90 R 425 -77 R 425 -61 R +424 -53 R 425 -44 R 425 -34 R 424 -36 R D 0.000 0.514 1.000 setrgbcolor +9674 10594 M 153 -36 R 303 140 R 303 27 R 304 53 R 303 23 R 303 -6 R +304 -100 R 303 42 R 304 93 R 303 -7 R 303 45 R 304 -12 R 303 37 R 303 -92 R +304 119 R 303 183 R 303 290 R 304 -120 R 303 -66 R 304 -117 R 303 -51 R +303 -90 R 304 -60 R 303 -56 R 303 -53 R 0 1 R D 15 setlinewidth +0.000 0.000 0.000 setrgbcolor 2242 4944 M 7433 0 R D 3304 4944 M 0 71 R D +gsave 3304 4411 translate 0 0 M 1.01 dup scale -58.8433 0 N +( ) show grestore 5428 4944 M 0 71 R D gsave 5428 4411 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 7551 4944 M 0 71 R D gsave 7551 4411 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 9675 4944 M 0 71 R D gsave 9675 4411 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 2455 4944 M 0 36 R D 2879 4944 M 0 36 R D 3729 4944 M +0 36 R D 4154 4944 M 0 36 R D 4578 4944 M 0 36 R D 5003 4944 M 0 36 R D +5852 4944 M 0 36 R D 6277 4944 M 0 36 R D 6702 4944 M 0 36 R D 7127 4944 M +0 36 R D 7976 4944 M 0 36 R D 8401 4944 M 0 36 R D 8825 4944 M 0 36 R D +9250 4944 M 0 36 R D gsave 5959 3949 translate 0 0 M 1.01 dup scale +-58.8433 0 N +( ) show grestore 2242 8467 M 7433 0 R D 3304 8467 M 0 -71 R D 5428 8467 M +0 -71 R D 7551 8467 M 0 -71 R D 9675 8467 M 0 -71 R D 2455 8467 M 0 -35 R D +2879 8467 M 0 -35 R D 3729 8467 M 0 -35 R D 4154 8467 M 0 -35 R D +4578 8467 M 0 -35 R D 5003 8467 M 0 -35 R D 5852 8467 M 0 -35 R D +6277 8467 M 0 -35 R D 6702 8467 M 0 -35 R D 7127 8467 M 0 -35 R D +7976 8467 M 0 -35 R D 8401 8467 M 0 -35 R D 8825 8467 M 0 -35 R D +9250 8467 M 0 -35 R D 2242 4944 M 0 3523 R D 2242 5560 M 149 0 R D +gsave 2130 5418 translate 0 0 M 1.01 dup scale -616.678 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(9) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 2242 6441 M 149 0 R D +gsave 2130 6298 translate 0 0 M 1.01 dup scale -762.61 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(10) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 2242 7321 M 149 0 R D +gsave 2130 7179 translate 0 0 M 1.01 dup scale -762.61 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(11) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 2242 8202 M 149 0 R D +gsave 2130 8059 translate 0 0 M 1.01 dup scale -762.61 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(12) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 2242 4944 M 75 0 R D 2242 5099 M 75 0 R D +2242 5210 M 75 0 R D 2242 5295 M 75 0 R D 2242 5365 M 75 0 R D 2242 5424 M +75 0 R D 2242 5475 M 75 0 R D 2242 5520 M 75 0 R D 2242 5825 M 75 0 R D +2242 5980 M 75 0 R D 2242 6090 M 75 0 R D 2242 6175 M 75 0 R D 2242 6245 M +75 0 R D 2242 6304 M 75 0 R D 2242 6355 M 75 0 R D 2242 6400 M 75 0 R D +2242 6706 M 75 0 R D 2242 6861 M 75 0 R D 2242 6971 M 75 0 R D 2242 7056 M +75 0 R D 2242 7126 M 75 0 R D 2242 7185 M 75 0 R D 2242 7236 M 75 0 R D +2242 7281 M 75 0 R D 2242 7586 M 75 0 R D 2242 7741 M 75 0 R D 2242 7851 M +75 0 R D 2242 7937 M 75 0 R D 2242 8006 M 75 0 R D 2242 8065 M 75 0 R D +2242 8116 M 75 0 R D 2242 8161 M 75 0 R D 2242 8467 M 75 0 R D +gsave 1024 6706 translate 0 0 M 90 rotate 1.01 dup scale -1588.99 0 N +(Observed L) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(B) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( \(L) show CP X -101.051 M +%%IncludeResource: font AvantGarde-Book +262.467 /AvantGarde-Book STDFONT +(O) show M X -58.3193 M +%%IncludeResource: font AvantGarde-Book +186.267 /AvantGarde-Book STDFONT +( \267) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(\)) show grestore 9675 4944 M 0 3523 R D 9675 5560 M -149 0 R D 9675 6441 M +-149 0 R D 9675 7321 M -149 0 R D 9675 8202 M -149 0 R D 9675 4944 M -74 0 R +D 9675 5099 M -74 0 R D 9675 5210 M -74 0 R D 9675 5295 M -74 0 R D +9675 5365 M -74 0 R D 9675 5424 M -74 0 R D 9675 5475 M -74 0 R D +9675 5520 M -74 0 R D 9675 5825 M -74 0 R D 9675 5980 M -74 0 R D +9675 6090 M -74 0 R D 9675 6175 M -74 0 R D 9675 6245 M -74 0 R D +9675 6304 M -74 0 R D 9675 6355 M -74 0 R D 9675 6400 M -74 0 R D +9675 6706 M -74 0 R D 9675 6861 M -74 0 R D 9675 6971 M -74 0 R D +9675 7056 M -74 0 R D 9675 7126 M -74 0 R D 9675 7185 M -74 0 R D +9675 7236 M -74 0 R D 9675 7281 M -74 0 R D 9675 7586 M -74 0 R D +9675 7741 M -74 0 R D 9675 7851 M -74 0 R D 9675 7937 M -74 0 R D +9675 8006 M -74 0 R D 9675 8065 M -74 0 R D 9675 8116 M -74 0 R D +9675 8161 M -74 0 R D 9675 8467 M -74 0 R D 40 setlinewidth 2242 5746 M +152 51 R 607 338 R 606 213 R 607 26 R 607 -130 R 61 -197 R 60 22 R 61 115 R +61 75 R 60 203 R 61 739 R 61 -246 R 60 -524 R 61 -308 R 61 12 R 60 -132 R +61 -177 R 61 58 R 60 38 R 61 -87 R 61 -132 R 60 -88 R 61 11 R 61 228 R +60 -135 R 31 -129 R 30 46 R 30 -22 R 31 129 R 30 -92 R 30 -39 R 31 78 R +30 -133 R 30 14 R 31 -109 R 30 326 R 30 99 R 31 -200 R 30 -32 R 30 102 R +31 -79 R 30 99 R 30 592 R 31 312 R 30 288 R 31 -1390 R 13 -635 R D +6790 4944 M 3 1008 R 30 1224 R 30 -283 R 31 -507 R 30 1146 R 31 -413 R +30 29 R 30 -195 R 31 -317 R 30 18 R 30 -68 R 31 -305 R 30 37 R 30 -283 R +31 -41 R 30 -138 R 30 -152 R 31 -27 R 30 -77 R 30 -4 R 31 -22 R 30 46 R +30 44 R 31 0 R 30 34 R 30 -13 R 31 252 R 30 133 R 30 18 R 31 -42 R 30 -12 R +30 -16 R 31 -57 R 30 -17 R 30 -83 R 31 51 R 30 -28 R 30 51 R 31 -62 R +30 37 R 30 -11 R 31 -94 R 30 -138 R 30 63 R 31 120 R 30 -155 R 30 -85 R +31 157 R 30 -44 R 30 94 R 31 -164 R 30 -26 R 30 -73 R 31 243 R 30 -30 R +30 -62 R 61 -331 R 61 62 R 60 -25 R 61 4 R 61 388 R 60 -458 R 61 65 R +61 -140 R 60 114 R 61 -150 R 61 184 R 60 -239 R 61 -55 R 61 311 R 60 -64 R +61 53 R 61 -287 R 61 351 R 60 -421 R 29 -123 R D 10 setlinewidth 2242 7405 M +152 -14 R 607 -126 R 606 88 R 607 -154 R 607 -20 R 61 10 R 60 -18 R 61 4 R +61 -23 R 60 29 R 61 -9 R 61 13 R 60 5 R 61 -11 R 61 21 R 60 2 R 61 -28 R +61 12 R 60 -11 R 61 2 R 61 -22 R 60 -10 R 61 -12 R 61 -24 R 60 -11 R 31 4 R +30 -3 R 30 49 R 31 -7 R 30 -15 R 30 11 R 31 -10 R 30 17 R 30 2 R 31 -10 R +30 -16 R 30 -4 R 31 4 R 30 45 R 30 -40 R 31 -5 R 30 -24 R 30 -34 R 31 -61 R +30 32 R 31 38 R 30 35 R 30 12 R 31 8 R 30 -4 R 30 -15 R 30 32 R 31 35 R +30 -39 R 31 30 R 30 -6 R 30 -51 R 31 60 R 30 -11 R 30 -5 R 31 16 R 30 9 R +30 1 R 31 -22 R 30 7 R 30 5 R 31 -4 R 30 -11 R 30 14 R 31 -6 R 30 -20 R +30 7 R 31 3 R 30 -3 R 30 -7 R 31 -28 R 30 24 R 30 -7 R 31 10 R 30 -1 R +30 2 R 31 -1 R 30 -5 R 30 -8 R 31 8 R 30 -10 R 30 0 R 31 5 R 30 -11 R +30 22 R 31 -12 R 30 3 R 30 -14 R 31 1 R 30 6 R 30 8 R 31 -16 R 30 -15 R +30 10 R 31 -1 R 30 15 R 30 -19 R 31 -11 R 30 15 R 30 -6 R 61 -23 R 61 -1 R +60 -16 R 61 2 R 61 4 R 60 -20 R 61 1 R 61 26 R 60 -16 R 61 -3 R 61 -22 R +60 6 R 61 15 R 61 -19 R 60 5 R 61 -6 R 61 -11 R 61 -11 R 60 9 R 60 -4 R D L1 +2242 7194 M 152 12 R 607 -112 R 606 147 R 607 -192 R 607 -8 R 61 10 R +60 -27 R 61 8 R 61 -33 R 60 34 R 61 -17 R 61 30 R 60 2 R 61 -19 R 61 32 R +60 -2 R 61 -34 R 61 19 R 60 -14 R 61 12 R 61 -32 R 60 -12 R 61 -7 R 61 -32 R +60 -12 R 31 6 R 30 -3 R 30 67 R 31 -7 R 30 -22 R 30 15 R 31 -13 R 30 25 R +30 5 R 31 -12 R 30 -23 R 30 -2 R 31 3 R 30 63 R 30 -41 R 31 -17 R 30 -29 R +30 -35 R 31 -68 R 30 32 R 31 51 R 30 32 R 30 8 R 31 8 R 30 -10 R 30 -14 R +30 57 R 31 39 R 30 -46 R 31 35 R 30 -8 R 30 -66 R 31 89 R 30 -25 R 30 -1 R +31 17 R 30 4 R 30 5 R 31 -24 R 30 3 R 30 6 R 31 -4 R 30 -17 R 30 22 R +31 -1 R 30 -31 R 30 14 R 31 3 R 30 -2 R 30 -12 R 31 -35 R 30 30 R 30 -6 R +31 12 R 30 1 R 30 2 R 31 1 R 30 -11 R 30 -7 R 31 9 R 30 -10 R 30 0 R 31 8 R +30 -12 R 30 26 R 31 -12 R 30 1 R 30 -18 R 31 4 R 30 4 R 30 9 R 31 -18 R +30 -18 R 30 13 R 31 -1 R 30 17 R 30 -20 R 31 -13 R 30 17 R 30 -9 R 61 -28 R +61 1 R 60 -22 R 61 3 R 61 5 R 60 -25 R 61 -3 R 61 38 R 60 -21 R 61 -3 R +61 -28 R 60 9 R 61 16 R 61 -24 R 60 10 R 61 -9 R 61 -13 R 61 -18 R 60 13 R +60 -4 R D gsave 2455 7851 translate 0 0 M 1.1 dup scale +(M) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(BH) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(=3) show +%%IncludeResource: font Symbol +423.333 /Symbol STDFONT +(\264) show +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(8) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( M) show CP X -101.051 M +%%IncludeResource: font AvantGarde-Book +262.467 /AvantGarde-Book STDFONT +(O) show M X -58.3193 M +%%IncludeResource: font AvantGarde-Book +186.267 /AvantGarde-Book STDFONT +( \267) show +%%IncludeResource: font Helvetica +186.267 /Helvetica STDFONT grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT L0 1.000 0.000 0.000 setrgbcolor 2242 6338 M +213 106 R 424 191 R 425 -176 R 425 -16 R 425 -40 R 424 15 R 425 81 R +425 -37 R 424 -49 R 425 37 R 425 -36 R 425 -82 R 424 -62 R 425 -47 R +425 -44 R 424 -42 R 425 -25 R 424 -22 R D 0.000 0.514 1.000 setrgbcolor +2242 6616 M 152 136 R 303 -55 R 304 62 R 303 -36 R 303 -33 R 304 113 R +303 -152 R 304 68 R 303 -67 R 303 -21 R 304 -24 R 303 -16 R 303 -52 R +304 -3 R 303 112 R 304 26 R 303 -136 R 303 280 R 304 -44 R 303 -63 R +303 -52 R 304 -19 R 303 -43 R 303 -14 R 303 3 R D 15 setlinewidth +0.000 0.000 0.000 setrgbcolor 9675 4944 M 7432 0 R D 10737 4944 M 0 71 R D +gsave 10737 4411 translate 0 0 M 1.01 dup scale -58.8433 0 N +( ) show grestore 12860 4944 M 0 71 R D gsave 12860 4411 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 14984 4944 M 0 71 R D gsave 14984 4411 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 17107 4944 M 0 71 R D gsave 17107 4411 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 9887 4944 M 0 36 R D 10312 4944 M 0 36 R D 11161 4944 M +0 36 R D 11586 4944 M 0 36 R D 12011 4944 M 0 36 R D 12436 4944 M 0 36 R D +13285 4944 M 0 36 R D 13710 4944 M 0 36 R D 14134 4944 M 0 36 R D +14559 4944 M 0 36 R D 15409 4944 M 0 36 R D 15833 4944 M 0 36 R D +16258 4944 M 0 36 R D 16683 4944 M 0 36 R D gsave 13391 3949 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 9675 8467 M 7432 0 R D 10737 8467 M 0 -71 R D 12860 8467 M +0 -71 R D 14984 8467 M 0 -71 R D 17107 8467 M 0 -71 R D 9887 8467 M 0 -35 R +D 10312 8467 M 0 -35 R D 11161 8467 M 0 -35 R D 11586 8467 M 0 -35 R D +12011 8467 M 0 -35 R D 12436 8467 M 0 -35 R D 13285 8467 M 0 -35 R D +13710 8467 M 0 -35 R D 14134 8467 M 0 -35 R D 14559 8467 M 0 -35 R D +15409 8467 M 0 -35 R D 15833 8467 M 0 -35 R D 16258 8467 M 0 -35 R D +16683 8467 M 0 -35 R D 9675 4944 M 0 3523 R D 9675 5560 M 149 0 R D +gsave 9563 5418 translate 0 0 M 1.01 dup scale -117.687 0 N +( ) show grestore 9675 6441 M 149 0 R D gsave 9563 6298 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9675 7321 M 149 0 R D gsave 9563 7179 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9675 8202 M 149 0 R D gsave 9563 8059 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9675 4944 M 74 0 R D 9675 5099 M 74 0 R D 9675 5210 M +74 0 R D 9675 5295 M 74 0 R D 9675 5365 M 74 0 R D 9675 5424 M 74 0 R D +9675 5475 M 74 0 R D 9675 5520 M 74 0 R D 9675 5825 M 74 0 R D 9675 5980 M +74 0 R D 9675 6090 M 74 0 R D 9675 6175 M 74 0 R D 9675 6245 M 74 0 R D +9675 6304 M 74 0 R D 9675 6355 M 74 0 R D 9675 6400 M 74 0 R D 9675 6706 M +74 0 R D 9675 6861 M 74 0 R D 9675 6971 M 74 0 R D 9675 7056 M 74 0 R D +9675 7126 M 74 0 R D 9675 7185 M 74 0 R D 9675 7236 M 74 0 R D 9675 7281 M +74 0 R D 9675 7586 M 74 0 R D 9675 7741 M 74 0 R D 9675 7851 M 74 0 R D +9675 7937 M 74 0 R D 9675 8006 M 74 0 R D 9675 8065 M 74 0 R D 9675 8116 M +74 0 R D 9675 8161 M 74 0 R D 9675 8467 M 74 0 R D +gsave 9108 6706 translate 0 0 M 90 rotate 1.01 dup scale -58.8433 0 N +( ) show grestore 17107 4944 M 0 3523 R D 17107 5560 M -148 0 R D +17107 6441 M -148 0 R D 17107 7321 M -148 0 R D 17107 8202 M -148 0 R D +17107 4944 M -74 0 R D 17107 5099 M -74 0 R D 17107 5210 M -74 0 R D +17107 5295 M -74 0 R D 17107 5365 M -74 0 R D 17107 5424 M -74 0 R D +17107 5475 M -74 0 R D 17107 5520 M -74 0 R D 17107 5825 M -74 0 R D +17107 5980 M -74 0 R D 17107 6090 M -74 0 R D 17107 6175 M -74 0 R D +17107 6245 M -74 0 R D 17107 6304 M -74 0 R D 17107 6355 M -74 0 R D +17107 6400 M -74 0 R D 17107 6706 M -74 0 R D 17107 6861 M -74 0 R D +17107 6971 M -74 0 R D 17107 7056 M -74 0 R D 17107 7126 M -74 0 R D +17107 7185 M -74 0 R D 17107 7236 M -74 0 R D 17107 7281 M -74 0 R D +17107 7586 M -74 0 R D 17107 7741 M -74 0 R D 17107 7851 M -74 0 R D +17107 7937 M -74 0 R D 17107 8006 M -74 0 R D 17107 8065 M -74 0 R D +17107 8116 M -74 0 R D 17107 8161 M -74 0 R D 17107 8467 M -74 0 R D +40 setlinewidth 9674 6098 M 153 86 R 606 540 R 607 624 R 607 -748 R +607 -162 R 60 -229 R 61 -15 R 61 113 R 60 67 R 61 196 R 61 749 R 60 -269 R +61 -543 R 61 -299 R 60 7 R 61 -140 R 61 -176 R 60 41 R 61 33 R 61 -80 R +60 -149 R 61 -75 R 61 16 R 60 242 R 61 -159 R 30 -116 R 31 38 R 30 -23 R +30 145 R 31 -108 R 30 -32 R 30 81 R 31 -116 R 30 4 R 30 -110 R 31 324 R +30 104 R 30 -179 R 31 -41 R 30 100 R 30 -89 R 31 101 R 30 621 R 30 714 R +31 626 R 30 101 R 30 128 R 31 -66 R 30 18 R 30 99 R 31 -111 R 30 -807 R +30 -638 R 31 1206 R 30 -442 R 30 84 R 31 783 R 30 -1263 R 30 -50 R 31 -132 R +30 -317 R 30 9 R 31 -303 R 30 -46 R 30 -141 R 31 -161 R 30 -35 R 30 -71 R +31 -4 R 30 -20 R 30 39 R 31 35 R 30 2 R 31 32 R 30 -12 R 30 258 R 31 141 R +30 35 R 30 -55 R 31 -26 R 30 -18 R 30 -44 R 31 -25 R 30 -83 R 30 47 R +31 -9 R 30 32 R 30 -65 R 31 33 R 30 5 R 30 -121 R 31 -137 R 30 74 R 30 116 R +31 -177 R 30 -82 R 30 167 R 31 -40 R 30 84 R 30 -168 R 31 -26 R 30 -69 R +30 267 R 31 -44 R 30 -74 R 61 -337 R 60 64 R 61 -18 R 61 -7 R 60 384 R +61 -453 R 61 63 R 60 -138 R 61 110 R 61 -149 R 60 182 R 61 -235 R 61 -60 R +60 313 R 61 -64 R 61 51 R 60 -287 R 61 352 R 61 -419 R 30 -133 R D +10 setlinewidth 9674 7849 M 153 4 R 606 -18 R 607 197 R 607 -207 R 607 -55 R +60 2 R 61 -32 R 61 -1 R 60 -10 R 61 8 R 61 -13 R 60 5 R 61 -19 R 61 -25 R +60 12 R 61 -4 R 61 -23 R 60 7 R 61 -20 R 61 0 R 60 -17 R 61 -18 R 61 -2 R +60 -19 R 61 -9 R 30 -5 R 31 -5 R 30 45 R 30 -7 R 31 -23 R 30 12 R 30 -20 R +31 20 R 30 -6 R 30 -1 R 31 -14 R 30 -14 R 30 -2 R 31 38 R 30 -20 R 30 -20 R +31 -8 R 30 13 R 30 3 R 31 12 R 30 52 R 30 120 R 31 101 R 30 -33 R 30 -65 R +31 -37 R 30 -2 R 30 -2 R 31 4 R 30 21 R 30 51 R 31 -42 R 30 -56 R 30 -26 R +31 -9 R 30 -16 R 30 -7 R 31 -10 R 30 -11 R 30 -7 R 31 -8 R 30 -2 R 30 -9 R +31 5 R 30 4 R 30 -18 R 31 4 R 30 -3 R 31 -6 R 30 -6 R 30 -12 R 31 9 R +30 -2 R 30 -14 R 31 -3 R 30 -4 R 30 -3 R 31 -6 R 30 -5 R 30 -8 R 31 -5 R +30 -4 R 30 4 R 31 -3 R 30 3 R 30 -14 R 31 -6 R 30 2 R 30 2 R 31 -11 R +30 -1 R 30 0 R 31 -7 R 30 0 R 30 -9 R 31 21 R 30 -16 R 30 -7 R 31 1 R +30 -2 R 61 -15 R 60 -7 R 61 -5 R 61 -7 R 60 1 R 61 -8 R 61 -8 R 60 16 R +61 -9 R 61 -7 R 60 -12 R 61 -2 R 61 1 R 60 -10 R 61 -3 R 61 -6 R 60 -6 R +61 -3 R 61 -1 R 60 0 R D L1 9674 7638 M 153 28 R 606 28 R 607 274 R +607 -238 R 607 -55 R 60 4 R 61 -41 R 61 0 R 60 -13 R 61 11 R 61 -17 R 60 6 R +61 -24 R 61 -33 R 60 16 R 61 -6 R 61 -28 R 60 12 R 61 -23 R 61 3 R 60 -19 R +61 -23 R 61 2 R 60 -23 R 61 -10 R 30 -6 R 31 -6 R 30 61 R 30 -8 R 31 -30 R +30 17 R 30 -26 R 31 27 R 30 -6 R 30 -1 R 31 -19 R 30 -18 R 30 -1 R 31 51 R +30 -26 R 30 -26 R 31 -10 R 30 18 R 30 5 R 31 17 R 30 68 R 30 147 R 31 117 R +30 -37 R 30 -75 R 31 -45 R 30 -2 R 30 -2 R 31 6 R 30 25 R 30 60 R 31 -49 R +30 -67 R 30 -32 R 31 -10 R 30 -19 R 30 -9 R 31 -11 R 30 -14 R 30 -9 R +31 -10 R 30 -1 R 30 -11 R 31 7 R 30 6 R 30 -23 R 31 6 R 30 -3 R 31 -7 R +30 -7 R 30 -15 R 31 12 R 30 0 R 30 -18 R 31 -3 R 30 -5 R 30 -3 R 31 -7 R +30 -5 R 30 -11 R 31 -6 R 30 -3 R 30 5 R 31 -3 R 30 5 R 30 -17 R 31 -8 R +30 3 R 30 3 R 31 -15 R 30 0 R 30 0 R 31 -8 R 30 0 R 30 -11 R 31 27 R +30 -19 R 30 -10 R 31 2 R 30 -2 R 61 -20 R 60 -9 R 61 -6 R 61 -8 R 60 1 R +61 -9 R 61 -11 R 60 24 R 61 -12 R 61 -9 R 60 -16 R 61 -2 R 61 2 R 60 -13 R +61 -3 R 61 -7 R 60 -8 R 61 -5 R 61 1 R 60 0 R D L0 +1.000 0.000 0.000 setrgbcolor 9674 6390 M 213 131 R 425 406 R 425 97 R +424 -229 R 425 -146 R 425 -85 R 425 5 R 424 -43 R 425 129 R 425 -115 R +424 -111 R 425 -87 R 425 -59 R 425 -50 R 424 -44 R 425 -40 R 425 -26 R +424 -22 R D 0.000 0.514 1.000 setrgbcolor 9674 6659 M 153 140 R 303 -40 R +303 102 R 304 17 R 303 27 R 303 187 R 304 -92 R 303 122 R 304 13 R 303 -54 R +303 -18 R 304 -64 R 303 -78 R 303 -40 R 304 51 R 303 278 R 303 6 R +304 -165 R 303 -84 R 304 -61 R 303 -52 R 303 -40 R 304 -41 R 303 -34 R +303 -11 R D 15 setlinewidth 0.000 0.000 0.000 setrgbcolor 2242 1422 M +7433 0 R D 3304 1422 M 0 71 R D gsave 3304 889 translate 0 0 M +1.01 dup scale -294.217 0 N +(0.5) show grestore 5428 1422 M 0 71 R D gsave 5428 889 translate 0 0 M +1.01 dup scale -294.217 0 N +(1.0) show grestore 7551 1422 M 0 71 R D gsave 7551 889 translate 0 0 M +1.01 dup scale -294.217 0 N +(1.5) show grestore 9675 1422 M 0 71 R D gsave 9675 889 translate 0 0 M +1.01 dup scale -294.217 0 N +(2.0) show grestore 2455 1422 M 0 35 R D 2879 1422 M 0 35 R D 3729 1422 M +0 35 R D 4154 1422 M 0 35 R D 4578 1422 M 0 35 R D 5003 1422 M 0 35 R D +5852 1422 M 0 35 R D 6277 1422 M 0 35 R D 6702 1422 M 0 35 R D 7127 1422 M +0 35 R D 7976 1422 M 0 35 R D 8401 1422 M 0 35 R D 8825 1422 M 0 35 R D +9250 1422 M 0 35 R D gsave 5959 427 translate 0 0 M 1.01 dup scale +-1011.13 0 N +(Time \(Gyr\)) show grestore 2242 4944 M 7433 0 R D 3304 4944 M 0 -70 R D +5428 4944 M 0 -70 R D 7551 4944 M 0 -70 R D 9675 4944 M 0 -70 R D +2455 4944 M 0 -35 R D 2879 4944 M 0 -35 R D 3729 4944 M 0 -35 R D +4154 4944 M 0 -35 R D 4578 4944 M 0 -35 R D 5003 4944 M 0 -35 R D +5852 4944 M 0 -35 R D 6277 4944 M 0 -35 R D 6702 4944 M 0 -35 R D +7127 4944 M 0 -35 R D 7976 4944 M 0 -35 R D 8401 4944 M 0 -35 R D +8825 4944 M 0 -35 R D 9250 4944 M 0 -35 R D 2242 1422 M 0 3522 R D +2242 1422 M 149 0 R D gsave 2130 1422 translate 0 0 M 1.01 dup scale +-616.678 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(9) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 2242 2374 M 149 0 R D +gsave 2130 2232 translate 0 0 M 1.01 dup scale -762.61 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(10) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 2242 3327 M 149 0 R D +gsave 2130 3184 translate 0 0 M 1.01 dup scale -762.61 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(11) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 2242 4279 M 149 0 R D +gsave 2130 4137 translate 0 0 M 1.01 dup scale -762.61 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(12) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 2242 1709 M 75 0 R D 2242 1876 M 75 0 R D +2242 1995 M 75 0 R D 2242 2088 M 75 0 R D 2242 2163 M 75 0 R D 2242 2227 M +75 0 R D 2242 2282 M 75 0 R D 2242 2331 M 75 0 R D 2242 2661 M 75 0 R D +2242 2829 M 75 0 R D 2242 2948 M 75 0 R D 2242 3040 M 75 0 R D 2242 3115 M +75 0 R D 2242 3179 M 75 0 R D 2242 3234 M 75 0 R D 2242 3283 M 75 0 R D +2242 3613 M 75 0 R D 2242 3781 M 75 0 R D 2242 3900 M 75 0 R D 2242 3992 M +75 0 R D 2242 4068 M 75 0 R D 2242 4131 M 75 0 R D 2242 4187 M 75 0 R D +2242 4235 M 75 0 R D 2242 4566 M 75 0 R D 2242 4733 M 75 0 R D 2242 4852 M +75 0 R D 2242 4944 M 75 0 R D gsave 1024 3183 translate 0 0 M 90 rotate +1.01 dup scale -58.8433 0 N +( ) show grestore 9675 1422 M 0 3522 R D 9675 1422 M -149 0 R D 9675 2374 M +-149 0 R D 9675 3327 M -149 0 R D 9675 4279 M -149 0 R D 9675 1709 M -74 0 R +D 9675 1876 M -74 0 R D 9675 1995 M -74 0 R D 9675 2088 M -74 0 R D +9675 2163 M -74 0 R D 9675 2227 M -74 0 R D 9675 2282 M -74 0 R D +9675 2331 M -74 0 R D 9675 2661 M -74 0 R D 9675 2829 M -74 0 R D +9675 2948 M -74 0 R D 9675 3040 M -74 0 R D 9675 3115 M -74 0 R D +9675 3179 M -74 0 R D 9675 3234 M -74 0 R D 9675 3283 M -74 0 R D +9675 3613 M -74 0 R D 9675 3781 M -74 0 R D 9675 3900 M -74 0 R D +9675 3992 M -74 0 R D 9675 4068 M -74 0 R D 9675 4131 M -74 0 R D +9675 4187 M -74 0 R D 9675 4235 M -74 0 R D 9675 4566 M -74 0 R D +9675 4733 M -74 0 R D 9675 4852 M -74 0 R D 9675 4944 M -74 0 R D +40 setlinewidth 2242 1629 M 152 134 R 607 678 R 606 -71 R 607 195 R 607 79 R +607 -67 R 303 211 R 303 -338 R 122 51 R 121 116 R 61 -129 R 60 -102 R +61 79 R 61 -118 R 60 67 R 61 -82 R 31 -91 R 30 -45 R 30 140 R 31 84 R +30 -78 R 30 -133 R 30 -51 R 31 202 R 30 -7 R 31 -69 R 30 -41 R 30 -85 R +31 28 R 30 111 R 30 -38 R 31 -34 R 30 -35 R 30 -75 R 31 64 R 30 -31 R +30 -74 R 31 71 R 30 20 R 30 -57 R 31 -35 R 30 -33 R 30 16 R 31 -16 R 30 43 R +30 50 R 31 -27 R 30 45 R 30 754 R 31 -125 R 30 -124 R 30 -22 R 31 -122 R +30 32 R 30 -61 R 31 -122 R 30 -26 R 30 137 R 31 -195 R 30 124 R 30 -171 R +31 403 R 30 609 R 15 -1820 R D 8298 1422 M 12 81 R 30 948 R 30 298 R +31 601 R 30 359 R 30 -422 R 31 -374 R 30 -6 R 30 -62 R 31 -217 R 30 -28 R +30 45 R 31 -78 R 30 2 R 30 -57 R 31 -25 R 30 -46 R 30 -25 R 31 1 R 30 110 R +30 -186 R 31 -11 R 30 151 R 30 -100 R 31 -220 R 30 28 R 61 75 R 60 -66 R +61 18 R 61 26 R 60 -328 R 61 187 R 61 -39 R 61 -257 R 60 293 R 60 -120 R D +10 setlinewidth 2242 3514 M 152 -34 R 607 -181 R 606 -78 R 607 102 R +607 -256 R 607 -20 R 303 -1 R 303 -42 R 122 22 R 121 44 R 61 58 R 60 -89 R +61 18 R 61 54 R 60 -20 R 61 -71 R 31 16 R 30 -1 R 30 2 R 31 0 R 30 -11 R +30 -6 R 30 10 R 31 -20 R 30 0 R 31 -2 R 30 4 R 30 15 R 31 2 R 30 -8 R +30 -10 R 31 -37 R 30 -1 R 30 -29 R 31 19 R 30 -18 R 30 15 R 31 -21 R 30 8 R +30 -20 R 31 -39 R 30 86 R 30 -57 R 31 -6 R 30 -14 R 30 -40 R 31 43 R +30 102 R 30 -128 R 31 -37 R 30 98 R 30 83 R 31 29 R 30 76 R 30 12 R 31 30 R +30 29 R 30 -23 R 31 25 R 30 -30 R 30 22 R 31 3 R 30 -21 R 30 -23 R 31 19 R +30 18 R 30 -1 R 31 18 R 30 24 R 30 -7 R 31 -13 R 30 -54 R 30 -51 R 31 -58 R +30 17 R 30 35 R 31 35 R 30 -16 R 30 58 R 31 -26 R 30 39 R 30 -26 R 31 35 R +30 -12 R 30 -3 R 31 -18 R 30 48 R 30 8 R 31 -31 R 30 -17 R 30 76 R 31 -29 R +30 10 R 30 -14 R 31 -33 R 30 66 R 61 -50 R 60 26 R 61 23 R 61 -22 R 60 7 R +61 9 R 61 2 R 61 37 R 60 -40 R 60 -13 R D L1 2242 3090 M 152 -26 R +607 -135 R 606 7 R 607 247 R 607 -336 R 607 -62 R 303 14 R 303 -41 R +122 42 R 121 69 R 61 105 R 60 -141 R 61 20 R 61 84 R 60 -19 R 61 -110 R +31 5 R 30 4 R 30 2 R 31 -1 R 30 -17 R 30 -8 R 30 7 R 31 -25 R 30 -6 R +31 -2 R 30 11 R 30 24 R 31 -4 R 30 -15 R 30 -16 R 31 -41 R 30 7 R 30 -41 R +31 18 R 30 -21 R 30 19 R 31 -33 R 30 13 R 30 -26 R 31 -41 R 30 157 R +30 -87 R 31 -18 R 30 -6 R 30 -65 R 31 84 R 30 169 R 30 -161 R 31 -41 R +30 97 R 30 96 R 31 24 R 30 98 R 30 13 R 31 28 R 30 31 R 30 -12 R 31 12 R +30 -19 R 30 15 R 31 20 R 30 -29 R 30 -22 R 31 15 R 30 15 R 30 5 R 31 10 R +30 32 R 30 -10 R 31 -7 R 30 -56 R 30 -53 R 31 -62 R 30 10 R 30 34 R 31 34 R +30 -16 R 30 66 R 31 -33 R 30 41 R 30 -30 R 31 39 R 30 -19 R 30 -1 R 31 -20 R +30 64 R 30 9 R 31 -39 R 30 -17 R 30 80 R 31 -19 R 30 2 R 30 -12 R 31 -43 R +30 76 R 61 -62 R 60 31 R 61 27 R 61 -28 R 60 3 R 61 7 R 61 13 R 61 50 R +60 -63 R 60 -15 R D gsave 2455 4279 translate 0 0 M 1.1 dup scale +(M) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(BH) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(=2) show +%%IncludeResource: font Symbol +423.333 /Symbol STDFONT +(\264) show +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(9) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( M) show CP X -101.051 M +%%IncludeResource: font AvantGarde-Book +262.467 /AvantGarde-Book STDFONT +(O) show M X -58.3193 M +%%IncludeResource: font AvantGarde-Book +186.267 /AvantGarde-Book STDFONT +( \267) show +%%IncludeResource: font Helvetica +186.267 /Helvetica STDFONT grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT L0 1.000 0.000 0.000 setrgbcolor 2242 2980 M +213 65 R 424 -117 R 425 4 R 425 -12 R 425 -153 R 424 40 R 425 68 R 425 86 R +424 -87 R 425 -57 R 425 -13 R 425 -54 R 424 -54 R 425 -39 R 425 -35 R +424 -57 R 425 -31 R 424 -47 R D 0.000 0.514 1.000 setrgbcolor 2242 3002 M +152 17 R 303 12 R 304 -70 R 303 105 R 303 18 R 304 -61 R 303 35 R 304 -65 R +303 51 R 303 64 R 304 -112 R 303 -54 R 303 40 R 304 -62 R 303 -5 R 304 -14 R +303 48 R 303 -44 R 304 -32 R 303 32 R 303 -23 R 304 96 R 303 -64 R 303 1 R +303 -41 R D 15 setlinewidth 0.000 0.000 0.000 setrgbcolor 9675 1422 M +7432 0 R D 10737 1422 M 0 71 R D gsave 10737 889 translate 0 0 M +1.01 dup scale -294.217 0 N +(0.5) show grestore 12860 1422 M 0 71 R D gsave 12860 889 translate 0 0 M +1.01 dup scale -294.217 0 N +(1.0) show grestore 14984 1422 M 0 71 R D gsave 14984 889 translate 0 0 M +1.01 dup scale -294.217 0 N +(1.5) show grestore 17107 1422 M 0 71 R D gsave 17107 889 translate 0 0 M +1.01 dup scale -294.217 0 N +(2.0) show grestore 9887 1422 M 0 35 R D 10312 1422 M 0 35 R D 11161 1422 M +0 35 R D 11586 1422 M 0 35 R D 12011 1422 M 0 35 R D 12436 1422 M 0 35 R D +13285 1422 M 0 35 R D 13710 1422 M 0 35 R D 14134 1422 M 0 35 R D +14559 1422 M 0 35 R D 15409 1422 M 0 35 R D 15833 1422 M 0 35 R D +16258 1422 M 0 35 R D 16683 1422 M 0 35 R D gsave 13391 427 translate 0 0 M +1.01 dup scale -1011.13 0 N +(Time \(Gyr\)) show grestore 9675 4944 M 7432 0 R D 10737 4944 M 0 -70 R D +12860 4944 M 0 -70 R D 14984 4944 M 0 -70 R D 17107 4944 M 0 -70 R D +9887 4944 M 0 -35 R D 10312 4944 M 0 -35 R D 11161 4944 M 0 -35 R D +11586 4944 M 0 -35 R D 12011 4944 M 0 -35 R D 12436 4944 M 0 -35 R D +13285 4944 M 0 -35 R D 13710 4944 M 0 -35 R D 14134 4944 M 0 -35 R D +14559 4944 M 0 -35 R D 15409 4944 M 0 -35 R D 15833 4944 M 0 -35 R D +16258 4944 M 0 -35 R D 16683 4944 M 0 -35 R D 9675 1422 M 0 3522 R D +9675 1422 M 149 0 R D gsave 9563 1422 translate 0 0 M 1.01 dup scale +-117.687 0 N +( ) show grestore 9675 2374 M 149 0 R D gsave 9563 2232 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9675 3327 M 149 0 R D gsave 9563 3184 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9675 4279 M 149 0 R D gsave 9563 4137 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9675 1709 M 74 0 R D 9675 1876 M 74 0 R D 9675 1995 M +74 0 R D 9675 2088 M 74 0 R D 9675 2163 M 74 0 R D 9675 2227 M 74 0 R D +9675 2282 M 74 0 R D 9675 2331 M 74 0 R D 9675 2661 M 74 0 R D 9675 2829 M +74 0 R D 9675 2948 M 74 0 R D 9675 3040 M 74 0 R D 9675 3115 M 74 0 R D +9675 3179 M 74 0 R D 9675 3234 M 74 0 R D 9675 3283 M 74 0 R D 9675 3613 M +74 0 R D 9675 3781 M 74 0 R D 9675 3900 M 74 0 R D 9675 3992 M 74 0 R D +9675 4068 M 74 0 R D 9675 4131 M 74 0 R D 9675 4187 M 74 0 R D 9675 4235 M +74 0 R D 9675 4566 M 74 0 R D 9675 4733 M 74 0 R D 9675 4852 M 74 0 R D +9675 4944 M 74 0 R D gsave 9108 3183 translate 0 0 M 90 rotate +1.01 dup scale -58.8433 0 N +( ) show grestore 17107 1422 M 0 3522 R D 17107 1422 M -148 0 R D +17107 2374 M -148 0 R D 17107 3327 M -148 0 R D 17107 4279 M -148 0 R D +17107 1709 M -74 0 R D 17107 1876 M -74 0 R D 17107 1995 M -74 0 R D +17107 2088 M -74 0 R D 17107 2163 M -74 0 R D 17107 2227 M -74 0 R D +17107 2282 M -74 0 R D 17107 2331 M -74 0 R D 17107 2661 M -74 0 R D +17107 2829 M -74 0 R D 17107 2948 M -74 0 R D 17107 3040 M -74 0 R D +17107 3115 M -74 0 R D 17107 3179 M -74 0 R D 17107 3234 M -74 0 R D +17107 3283 M -74 0 R D 17107 3613 M -74 0 R D 17107 3781 M -74 0 R D +17107 3900 M -74 0 R D 17107 3992 M -74 0 R D 17107 4068 M -74 0 R D +17107 4131 M -74 0 R D 17107 4187 M -74 0 R D 17107 4235 M -74 0 R D +17107 4566 M -74 0 R D 17107 4733 M -74 0 R D 17107 4852 M -74 0 R D +17107 4944 M -74 0 R D 40 setlinewidth 9674 2153 M 153 204 R 606 519 R +607 -105 R 607 40 R 607 271 R 606 -196 R 304 113 R 303 -342 R 121 54 R +122 46 R 60 -106 R 61 -130 R 61 92 R 60 -86 R 61 43 R 61 -90 R 30 -85 R +30 -61 R 31 160 R 30 61 R 30 -70 R 31 -133 R 30 -50 R 30 196 R 31 0 R +30 -54 R 30 -68 R 31 -68 R 30 3 R 30 147 R 31 -44 R 30 -49 R 30 -27 R +31 -94 R 30 71 R 30 -3 R 31 -52 R 30 18 R 30 40 R 31 -59 R 30 0 R 30 -39 R +31 -21 R 30 -7 R 31 44 R 30 65 R 30 -18 R 31 49 R 30 962 R 30 33 R 31 -401 R +30 -71 R 30 -148 R 31 16 R 30 -126 R 30 -110 R 31 -29 R 30 131 R 30 -187 R +31 125 R 30 -151 R 30 428 R 31 580 R 30 843 R 30 -52 R 31 79 R 30 56 R +30 286 R 31 -159 R 30 53 R 30 53 R 31 -35 R 30 206 R 30 -352 R 31 -47 R +30 -682 R 30 -443 R 31 -46 R 30 -101 R 30 -236 R 31 -49 R 30 54 R 30 -110 R +31 -3 R 30 -33 R 30 -14 R 31 -64 R 30 -40 R 30 20 R 31 119 R 30 -237 R +30 3 R 31 127 R 30 -86 R 30 -239 R 31 10 R 60 76 R 61 -90 R 61 55 R 60 17 R +61 -348 R 61 180 R 60 -58 R 61 -246 R 61 288 R 60 -133 R D 10 setlinewidth +9674 4230 M 153 0 R 606 -46 R 607 17 R 607 178 R 607 -205 R 606 -82 R +304 -20 R 303 -45 R 121 5 R 122 47 R 60 65 R 61 -105 R 61 15 R 60 36 R +61 0 R 61 -79 R 30 -9 R 30 -10 R 31 22 R 30 -27 R 30 -7 R 31 -8 R 30 -4 R +30 -6 R 31 -9 R 30 -5 R 30 2 R 31 7 R 30 -2 R 30 -14 R 31 -9 R 30 -4 R +30 11 R 31 -2 R 30 -17 R 30 -2 R 31 9 R 30 -15 R 30 -8 R 31 -6 R 30 -4 R +30 81 R 31 -59 R 30 -15 R 31 15 R 30 -18 R 30 73 R 31 98 R 30 -80 R 30 -21 R +31 -15 R 30 -27 R 30 6 R 31 67 R 30 -28 R 30 36 R 31 83 R 30 -60 R 30 117 R +31 118 R 30 -3 R 30 59 R 31 -18 R 30 26 R 30 -44 R 31 -8 R 30 42 R 30 -13 R +31 22 R 30 -5 R 30 -14 R 31 -5 R 30 -61 R 30 -8 R 31 -47 R 30 -15 R 30 -17 R +31 -21 R 30 1 R 30 -23 R 31 -8 R 30 -12 R 30 -12 R 31 -8 R 30 -2 R 30 -15 R +31 -2 R 30 -8 R 30 -10 R 31 -9 R 30 -9 R 30 -6 R 31 -7 R 30 -7 R 30 -7 R +31 -6 R 60 -6 R 61 -4 R 61 -20 R 60 -10 R 61 -11 R 61 -11 R 60 -7 R 61 -4 R +61 -14 R 60 -8 R D L1 9674 3912 M 153 37 R 606 10 R 607 73 R 607 264 R +607 -246 R 606 -108 R 304 -12 R 303 -44 R 121 10 R 122 68 R 60 85 R +61 -136 R 61 23 R 60 48 R 61 0 R 61 -103 R 30 -11 R 30 -14 R 31 32 R +30 -37 R 30 -9 R 31 -11 R 30 -5 R 30 -7 R 31 -12 R 30 -7 R 30 4 R 31 10 R +30 -2 R 30 -20 R 31 -11 R 30 -5 R 30 16 R 31 -2 R 30 -24 R 30 -3 R 31 14 R +30 -20 R 30 -10 R 31 -8 R 30 -5 R 30 116 R 31 -81 R 30 -20 R 31 22 R +30 -23 R 30 101 R 31 128 R 30 -102 R 30 -27 R 31 -18 R 30 -37 R 30 10 R +31 90 R 30 -36 R 30 48 R 31 104 R 30 -74 R 30 143 R 31 136 R 30 -2 R 30 65 R +31 -20 R 30 30 R 30 -49 R 31 -9 R 30 47 R 30 -14 R 31 25 R 30 -5 R 30 -16 R +31 -6 R 30 -68 R 30 -9 R 31 -52 R 30 -18 R 30 -20 R 31 -24 R 30 2 R 30 -27 R +31 -9 R 30 -15 R 30 -14 R 31 -9 R 30 -2 R 30 -18 R 31 -2 R 30 -10 R 30 -12 R +31 -11 R 30 -10 R 30 -8 R 31 -8 R 30 -8 R 30 -8 R 31 -8 R 60 -6 R 61 -5 R +61 -25 R 60 -13 R 61 -13 R 61 -13 R 60 -9 R 61 -5 R 61 -17 R 60 -11 R D L0 +1.000 0.000 0.000 setrgbcolor 9674 3520 M 213 122 R 425 47 R 425 53 R +424 17 R 425 -180 R 425 -20 R 425 185 R 424 -212 R 425 -119 R 425 -84 R +424 -81 R 425 -69 R 425 -57 R 425 -44 R 424 -38 R 425 -54 R 425 -33 R +424 -36 R D 0.000 0.514 1.000 setrgbcolor 9674 3502 M 153 38 R 303 118 R +303 119 R 304 294 R 303 -92 R 303 -111 R 304 -15 R 303 -87 R 304 20 R +303 25 R 303 -85 R 304 2 R 303 25 R 303 -40 R 304 -32 R 303 -17 R 303 -4 R +304 -54 R 303 -24 R 304 16 R 303 -13 R 303 65 R 304 -38 R 303 -14 R +303 342 R D +%%PageTrailer +end +restore +showpage +%%PageResources: font Helvetica +%%+ font Symbol +%%+ font AvantGarde-Book +%%Trailer +restore +%%Pages: 1 +%%DocumentNeededResources: font Helvetica +%%+ font Symbol +%%+ font AvantGarde-Book +%%EOF diff --git a/feedback/papers/0506398/f14.ps b/feedback/papers/0506398/f14.ps new file mode 100644 index 0000000..58290ed --- /dev/null +++ b/feedback/papers/0506398/f14.ps @@ -0,0 +1,4122 @@ +%!PS-Adobe-3.0 +%%BoundingBox: 54 360 558 720 +%%Title: Graphics produced by IDL +%%For: phopkins@dhcp152-235.cfa.harvard.edu, +%% /Users/phopkins/Documents/lars_galaxies/plots/LF_massive +%%Creator: IDL Student Edition 6.0.3, Mac OS X (darwin ppc m32) +%%CreationDate: Mon Aug 29 02:31:18 2005 +%%DocumentData: Clean7bit +%%Requirements: color +%%LanguageLevel: 1 +%%PageOrder: Ascend +%%Pages: (atend) +%%DocumentNeededResources: (atend) +%%EndComments +%%BeginProlog +save +%+ prolog.ps -- Prolog for IDL generated PostScript files +%+ Copyright (c) 1988-2003 Research Systems, Inc. All Rights Reserved. +%v 4 +/$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C +{currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint +stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} +bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show +grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 +setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 +{[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 +100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 +{[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef +/ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} +ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont +exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica +findfont exch scalefont setfont (\267) show currentpoint grestore moveto} +bdef end 2.5 setmiterlimit +%%EndProlog +%%Page: 0 1 +%%PageRequirements: color +%%PageResources: (atend) +%%PageOrientation: Portrait +%%PageBoundingBox: 54 360 558 720 +%%BeginPageSetup +save +$IDL_DICT begin 54 360 translate 0.0283465 dup scale +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +%%EndPageSetup +15 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 1794 6706 M 7881 0 R D +2888 6706 M 0 112 R D gsave 2888 6172 translate 0 0 M 1.01 dup scale +-58.8433 0 N +( ) show grestore 5078 6706 M 0 112 R D gsave 5078 6172 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 7267 6706 M 0 112 R D gsave 7267 6172 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 9456 6706 M 0 112 R D gsave 9456 6172 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 1794 6706 M 0 56 R D 2013 6706 M 0 56 R D 2232 6706 M +0 56 R D 2451 6706 M 0 56 R D 2670 6706 M 0 56 R D 3107 6706 M 0 56 R D +3326 6706 M 0 56 R D 3545 6706 M 0 56 R D 3764 6706 M 0 56 R D 3983 6706 M +0 56 R D 4202 6706 M 0 56 R D 4421 6706 M 0 56 R D 4640 6706 M 0 56 R D +4859 6706 M 0 56 R D 5297 6706 M 0 56 R D 5515 6706 M 0 56 R D 5734 6706 M +0 56 R D 5953 6706 M 0 56 R D 6172 6706 M 0 56 R D 6391 6706 M 0 56 R D +6610 6706 M 0 56 R D 6829 6706 M 0 56 R D 7048 6706 M 0 56 R D 7486 6706 M +0 56 R D 7705 6706 M 0 56 R D 7924 6706 M 0 56 R D 8142 6706 M 0 56 R D +8361 6706 M 0 56 R D 8580 6706 M 0 56 R D 8799 6706 M 0 56 R D 9018 6706 M +0 56 R D 9237 6706 M 0 56 R D 9675 6706 M 0 56 R D +gsave 5734 5710 translate 0 0 M 1.01 dup scale -58.8433 0 N +( ) show grestore 1794 12345 M 7881 0 R D 2888 12345 M 0 -113 R D +5078 12345 M 0 -113 R D 7267 12345 M 0 -113 R D 9456 12345 M 0 -113 R D +1794 12345 M 0 -57 R D 2013 12345 M 0 -57 R D 2232 12345 M 0 -57 R D +2451 12345 M 0 -57 R D 2670 12345 M 0 -57 R D 3107 12345 M 0 -57 R D +3326 12345 M 0 -57 R D 3545 12345 M 0 -57 R D 3764 12345 M 0 -57 R D +3983 12345 M 0 -57 R D 4202 12345 M 0 -57 R D 4421 12345 M 0 -57 R D +4640 12345 M 0 -57 R D 4859 12345 M 0 -57 R D 5297 12345 M 0 -57 R D +5515 12345 M 0 -57 R D 5734 12345 M 0 -57 R D 5953 12345 M 0 -57 R D +6172 12345 M 0 -57 R D 6391 12345 M 0 -57 R D 6610 12345 M 0 -57 R D +6829 12345 M 0 -57 R D 7048 12345 M 0 -57 R D 7486 12345 M 0 -57 R D +7705 12345 M 0 -57 R D 7924 12345 M 0 -57 R D 8142 12345 M 0 -57 R D +8361 12345 M 0 -57 R D 8580 12345 M 0 -57 R D 8799 12345 M 0 -57 R D +9018 12345 M 0 -57 R D 9237 12345 M 0 -57 R D 9675 12345 M 0 -57 R D +1794 6706 M 0 5639 R D 1794 7010 M 157 0 R D gsave 1682 6868 translate 0 0 M +1.01 dup scale -376.343 0 N +(-3) show grestore 1794 8534 M 157 0 R D gsave 1682 8392 translate 0 0 M +1.01 dup scale -376.343 0 N +(-2) show grestore 1794 10058 M 157 0 R D gsave 1682 9916 translate 0 0 M +1.01 dup scale -376.343 0 N +(-1) show grestore 1794 11583 M 157 0 R D gsave 1682 11440 translate 0 0 M +1.01 dup scale -235.373 0 N +(0) show grestore 1794 6706 M 79 0 R D 1794 6858 M 79 0 R D 1794 7163 M +79 0 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0 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 9 11 R +8 12 R 7 13 R 4 14 R 3 14 R 1 15 R F +5491 9882 M -1 14 R -3 15 R -5 13 R -6 13 R -8 12 R -10 11 R -11 10 R +-12 8 R -13 6 R -13 5 R -15 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R -13 -6 R +-12 -8 R -11 -10 R -9 -11 R -8 -12 R -7 -13 R -4 -13 R -3 -15 R -1 -14 R +1 -15 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -9 R 12 -8 R 13 -7 R +14 -4 R 14 -3 R 15 -1 R 14 1 R 15 3 R 13 4 R 13 7 R 12 8 R 11 9 R 10 11 R +8 12 R 6 13 R 5 14 R 3 14 R 1 15 R F +5417 9828 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -9 11 R -11 9 R -12 8 R +-13 7 R -14 4 R -14 3 R -15 1 R -14 -1 R -15 -3 R -13 -4 R -13 -7 R -12 -8 R +-11 -9 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -15 R 1 -14 R +3 -15 R 5 -13 R 6 -13 R 8 -12 R 10 -11 R 11 -10 R 12 -8 R 13 -6 R 13 -5 R +15 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 9 11 R 8 12 R +7 13 R 4 13 R 3 15 R 1 14 R F +5180 9660 M -1 15 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 10 R +-12 8 R -13 6 R -14 5 R -14 3 R -14 0 R -15 0 R -14 -3 R -14 -5 R -13 -6 R +-12 -8 R -11 -10 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R 0 -15 R +0 -14 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -10 R 12 -8 R 13 -6 R +14 -5 R 14 -3 R 15 -1 R 14 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 10 11 R +8 12 R 6 13 R 5 14 R 3 14 R 1 14 R F +3852 8642 M -1 14 R -3 15 R -5 13 R -6 13 R -8 13 R -10 10 R -11 10 R +-12 8 R -13 7 R -14 4 R -14 3 R -14 1 R -15 -1 R -14 -3 R -14 -4 R -13 -7 R +-12 -8 R -11 -10 R -10 -10 R -8 -13 R -6 -13 R -5 -13 R -3 -15 R 0 -14 R +0 -14 R 3 -15 R 5 -13 R 6 -14 R 8 -12 R 10 -10 R 11 -10 R 12 -8 R 13 -7 R +14 -4 R 14 -3 R 15 -1 R 14 1 R 14 3 R 14 4 R 13 7 R 12 8 R 11 10 R 10 10 R +8 12 R 6 14 R 5 13 R 3 15 R 1 14 R F +2038 7165 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -9 11 R -11 9 R -12 9 R +-13 6 R -14 5 R -14 2 R -15 1 R -14 -1 R -15 -2 R -13 -5 R -13 -6 R -12 -9 R +-11 -9 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -15 R 1 -14 R +3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -10 R 12 -8 R 13 -6 R 13 -5 R +15 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 9 11 R 8 12 R +7 13 R 4 14 R 3 14 R 1 14 R F +2358 7440 M -1 14 R -2 14 R -5 14 R -7 13 R -8 12 R -9 11 R -11 10 R -12 8 R +-13 6 R -14 5 R -14 3 R -15 1 R -14 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R +-11 -10 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -14 R 1 -15 R +3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -9 R 12 -9 R 13 -6 R 14 -5 R +14 -2 R 14 -1 R 15 1 R 14 2 R 14 5 R 13 6 R 12 9 R 11 9 R 9 11 R 8 12 R +7 13 R 5 14 R 2 14 R 1 15 R F +2355 7447 M -1 14 R -3 15 R -5 13 R -6 14 R -8 12 R -10 10 R -11 10 R +-12 8 R -13 7 R -14 4 R -14 3 R -14 1 R -15 -1 R -14 -3 R -14 -4 R -13 -7 R +-12 -8 R -11 -10 R -9 -10 R -8 -12 R -7 -14 R -4 -13 R -3 -15 R -1 -14 R +1 -14 R 3 -15 R 4 -13 R 7 -13 R 8 -13 R 9 -10 R 11 -10 R 12 -8 R 13 -7 R +14 -4 R 14 -3 R 15 -1 R 14 1 R 14 3 R 14 4 R 13 7 R 12 8 R 11 10 R 10 10 R +8 13 R 6 13 R 5 13 R 3 15 R 1 14 R F +2185 7311 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R 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R 219 153 R 219 152 R 219 152 R 218 153 R +219 152 R 219 153 R 219 152 R 219 152 R 219 153 R 219 152 R 219 153 R +219 152 R 219 152 R 219 153 R 219 152 R 218 153 R 219 152 R 219 152 R +219 153 R 219 152 R 219 153 R 219 152 R 219 152 R 219 153 R 219 152 R +219 153 R 219 152 R 218 152 R 219 153 R 219 152 R 219 153 R 38 27 R D +0.000 0.000 0.000 setrgbcolor gsave 2232 11583 translate 0 0 M 1.2 dup scale +(f) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(gas) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( = 0.2) show grestore 1.000 0.000 0.000 setrgbcolor 1794 8000 M -1 -1 R D +1793 7779 M 1 -1 R D 2101 8222 M -222 -222 R 111 111 R -111 111 R 222 -222 R +D 2757 8710 M -222 -222 R 111 111 R -111 111 R 222 -222 R D 3099 8963 M +-222 -222 R 111 111 R -111 111 R 222 -222 R D 3193 9040 M -222 -222 R +111 111 R -111 111 R 222 -222 R D 3294 9121 M -222 -222 R 111 111 R +-111 111 R 222 -222 R D 3410 9212 M -222 -222 R 111 111 R -111 111 R +222 -222 R D 3311 9156 M -222 -222 R 111 111 R -111 111 R 222 -222 R D +3428 9247 M -222 -222 R 111 111 R -111 111 R 222 -222 R D 3454 9276 M +-222 -222 R 111 111 R -111 111 R 222 -222 R D 3732 9475 M -222 -222 R +111 111 R -111 111 R 222 -222 R D 3898 9596 M -222 -222 R 111 111 R +-111 111 R 222 -222 R D 3872 9581 M -222 -222 R 111 111 R -111 111 R +222 -222 R D 4060 9707 M -222 -222 R 111 111 R -111 111 R 222 -222 R D +4130 9755 M -222 -222 R 111 111 R -111 111 R 222 -222 R D 4270 9847 M +-222 -222 R 111 111 R -111 111 R 222 -222 R D 4437 9956 M -222 -222 R +111 111 R -111 111 R 222 -222 R D 4550 10028 M -222 -222 R 111 111 R +-111 111 R 222 -222 R D 4546 10028 M -222 -222 R 111 111 R -111 111 R +222 -222 R D 4791 10180 M -222 -222 R 111 111 R -111 111 R 222 -222 R D +4406 9948 M -222 -222 R 111 111 R -111 111 R 222 -222 R D 4590 10065 M +-222 -222 R 111 111 R -111 111 R 222 -222 R D 4547 10041 M -222 -222 R +111 111 R -111 111 R 222 -222 R D 4754 10170 M -222 -222 R 111 111 R +-111 111 R 222 -222 R D 4554 10053 M -222 -222 R 111 111 R -111 111 R +222 -222 R D 4551 10052 M -222 -222 R 111 111 R -111 111 R 222 -222 R D +4835 10229 M -222 -222 R 111 111 R -111 111 R 222 -222 R D 4495 10026 M +-222 -222 R 111 111 R -111 111 R 222 -222 R D 4725 10169 M -222 -222 R +111 111 R -111 111 R 222 -222 R D 4693 10153 M -222 -222 R 111 111 R +-111 111 R 222 -222 R D 4614 10108 M -222 -222 R 111 111 R -111 111 R +222 -222 R D 4766 10202 M -222 -222 R 111 111 R -111 111 R 222 -222 R D +4713 10191 M -222 -222 R 111 111 R -111 111 R 222 -222 R D 5086 10431 M +-222 -222 R 111 111 R -111 111 R 222 -222 R D 4898 10340 M -222 -222 R +111 111 R -111 111 R 222 -222 R D 4689 10235 M -222 -222 R 111 111 R +-111 111 R 222 -222 R D 5039 10462 M -222 -222 R 111 111 R -111 111 R +222 -222 R D 4446 10126 M -222 -222 R 111 111 R -111 111 R 222 -222 R D +5654 10842 M -222 -222 R 111 111 R -111 111 R 222 -222 R D 5967 11021 M +-222 -222 R 111 111 R -111 111 R 222 -222 R D 5849 10982 M 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R D 8255 11786 M +-222 -222 R 111 111 R -111 111 R 222 -222 R D 8470 11803 M -222 -222 R +111 111 R -111 111 R 222 -222 R D 8879 11814 M -222 -222 R 111 111 R +-111 111 R 222 -222 R D 6879 11377 M -222 -222 R 111 111 R -111 111 R +222 -222 R D 6069 11014 M -222 -222 R 111 111 R -111 111 R 222 -222 R D +5172 10528 M -222 -222 R 111 111 R -111 111 R 222 -222 R D 4915 10368 M +-222 -222 R 111 111 R -111 111 R 222 -222 R D 3934 9745 M -222 -222 R +111 111 R -111 111 R 222 -222 R D 3004 9104 M -222 -222 R 111 111 R +-111 111 R 222 -222 R D 2906 9023 M -222 -222 R 111 111 R -111 111 R +222 -222 R D 2979 9063 M -222 -222 R 111 111 R -111 111 R 222 -222 R D +2995 9063 M -222 -222 R 111 111 R -111 111 R 222 -222 R D 2974 9036 M +-222 -222 R 111 111 R -111 111 R 222 -222 R D 2883 8961 M -222 -222 R +111 111 R -111 111 R 222 -222 R D 3119 9116 M -222 -222 R 111 111 R +-111 111 R 222 -222 R D 2869 8952 M -222 -222 R 111 111 R -111 111 R +222 -222 R D 2878 8971 M -222 -222 R 111 111 R -111 111 R 222 -222 R D +2822 8944 M -222 -222 R 111 111 R -111 111 R 222 -222 R D 2811 8949 M +-222 -222 R 111 111 R -111 111 R 222 -222 R D 2804 8957 M -222 -222 R +111 111 R -111 111 R 222 -222 R D 2830 8988 M -222 -222 R 111 111 R +-111 111 R 222 -222 R D 2854 9018 M -222 -222 R 111 111 R -111 111 R +222 -222 R D 2854 9031 M -222 -222 R 111 111 R -111 111 R 222 -222 R D +2869 9054 M -222 -222 R 111 111 R -111 111 R 222 -222 R D 2908 9095 M +-222 -222 R 111 111 R -111 111 R 222 -222 R D 3145 9271 M -222 -222 R +111 111 R -111 111 R 222 -222 R D 3193 9314 M -222 -222 R 111 111 R +-111 111 R 222 -222 R D 3225 9347 M -222 -222 R 111 111 R -111 111 R +222 -222 R D 3201 9340 M -222 -222 R 111 111 R -111 111 R 222 -222 R D +2920 9154 M -222 -222 R 111 111 R -111 111 R 222 -222 R D 3037 9246 M +-222 -222 R 111 111 R -111 111 R 222 -222 R D 3175 9352 M -222 -222 R +111 111 R -111 111 R 222 -222 R D 3314 9458 M -222 -222 R 111 111 R +-111 111 R 222 -222 R D 3330 9480 M -222 -222 R 111 111 R -111 111 R +222 -222 R D 3292 9463 M -222 -222 R 111 111 R -111 111 R 222 -222 R D +3153 9370 M -222 -222 R 111 111 R -111 111 R 222 -222 R D 2737 9083 M +-222 -222 R 111 111 R -111 111 R 222 -222 R D 2333 8794 M -222 -222 R +111 111 R -111 111 R 222 -222 R D 2382 8834 M -222 -222 R 111 111 R +-111 111 R 222 -222 R D 2053 8595 M -222 -222 R 111 111 R -111 111 R +222 -222 R D 2706 9091 M -222 -222 R 111 111 R -111 111 R 222 -222 R D +1829 8453 M -36 -36 R D 1793 8267 M 36 -36 R D 1837 8472 M -44 -44 R D +1793 8294 M 44 -44 R D 1793 7995 M 1 1 R 219 153 R 219 152 R 219 152 R +219 153 R 218 152 R 219 153 R 219 152 R 219 152 R 219 153 R 219 152 R +219 153 R 219 152 R 219 152 R 219 153 R 219 152 R 219 153 R 218 152 R +219 152 R 219 153 R 219 152 R 219 153 R 219 152 R 219 152 R 219 153 R +219 152 R 219 153 R 219 152 R 219 152 R 115 81 R D +0.000 0.000 0.000 setrgbcolor gsave 2232 11583 translate 0 0 M 1.2 dup scale +(f) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(gas) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( = 0.2) show grestore 15 setlinewidth 9675 6706 M 7881 0 R D 10769 6706 M +0 112 R D gsave 10769 6172 translate 0 0 M 1.01 dup scale -58.8433 0 N +( ) show grestore 12959 6706 M 0 112 R D gsave 12959 6172 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 15148 6706 M 0 112 R D gsave 15148 6172 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 17337 6706 M 0 112 R D gsave 17337 6172 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 9675 6706 M 0 56 R D 9894 6706 M 0 56 R D 10113 6706 M +0 56 R D 10332 6706 M 0 56 R D 10551 6706 M 0 56 R D 10988 6706 M 0 56 R D +11207 6706 M 0 56 R D 11426 6706 M 0 56 R D 11645 6706 M 0 56 R D +11864 6706 M 0 56 R D 12083 6706 M 0 56 R D 12302 6706 M 0 56 R D +12521 6706 M 0 56 R D 12740 6706 M 0 56 R D 13178 6706 M 0 56 R D +13396 6706 M 0 56 R D 13615 6706 M 0 56 R D 13834 6706 M 0 56 R D +14053 6706 M 0 56 R D 14272 6706 M 0 56 R D 14491 6706 M 0 56 R D +14710 6706 M 0 56 R D 14929 6706 M 0 56 R D 15367 6706 M 0 56 R D +15586 6706 M 0 56 R D 15805 6706 M 0 56 R D 16023 6706 M 0 56 R D +16242 6706 M 0 56 R D 16461 6706 M 0 56 R D 16680 6706 M 0 56 R D +16899 6706 M 0 56 R D 17118 6706 M 0 56 R D 17556 6706 M 0 56 R D +gsave 13615 5710 translate 0 0 M 1.01 dup scale -58.8433 0 N +( ) show grestore 9675 12345 M 7881 0 R D 10769 12345 M 0 -113 R D +12959 12345 M 0 -113 R D 15148 12345 M 0 -113 R D 17337 12345 M 0 -113 R D +9675 12345 M 0 -57 R D 9894 12345 M 0 -57 R D 10113 12345 M 0 -57 R D +10332 12345 M 0 -57 R D 10551 12345 M 0 -57 R D 10988 12345 M 0 -57 R D +11207 12345 M 0 -57 R D 11426 12345 M 0 -57 R D 11645 12345 M 0 -57 R D +11864 12345 M 0 -57 R D 12083 12345 M 0 -57 R D 12302 12345 M 0 -57 R D +12521 12345 M 0 -57 R D 12740 12345 M 0 -57 R D 13178 12345 M 0 -57 R D +13396 12345 M 0 -57 R D 13615 12345 M 0 -57 R D 13834 12345 M 0 -57 R D +14053 12345 M 0 -57 R D 14272 12345 M 0 -57 R D 14491 12345 M 0 -57 R D +14710 12345 M 0 -57 R D 14929 12345 M 0 -57 R D 15367 12345 M 0 -57 R D +15586 12345 M 0 -57 R D 15805 12345 M 0 -57 R D 16023 12345 M 0 -57 R D +16242 12345 M 0 -57 R D 16461 12345 M 0 -57 R D 16680 12345 M 0 -57 R D +16899 12345 M 0 -57 R D 17118 12345 M 0 -57 R D 17556 12345 M 0 -57 R D +9675 6706 M 0 5639 R D 9675 7010 M 157 0 R D gsave 9563 6868 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9675 8534 M 157 0 R D gsave 9563 8392 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9675 10058 M 157 0 R D gsave 9563 9916 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9675 11583 M 157 0 R D gsave 9563 11440 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9675 6706 M 79 0 R D 9675 6858 M 79 0 R D 9675 7163 M +79 0 R D 9675 7315 M 79 0 R D 9675 7468 M 79 0 R D 9675 7620 M 79 0 R D +9675 7772 M 79 0 R D 9675 7925 M 79 0 R D 9675 8077 M 79 0 R D 9675 8230 M +79 0 R D 9675 8382 M 79 0 R D 9675 8687 M 79 0 R D 9675 8839 M 79 0 R D +9675 8992 M 79 0 R D 9675 9144 M 79 0 R D 9675 9296 M 79 0 R D 9675 9449 M +79 0 R D 9675 9601 M 79 0 R D 9675 9754 M 79 0 R D 9675 9906 M 79 0 R D +9675 10211 M 79 0 R D 9675 10363 M 79 0 R D 9675 10516 M 79 0 R D +9675 10668 M 79 0 R D 9675 10821 M 79 0 R D 9675 10973 M 79 0 R D +9675 11125 M 79 0 R D 9675 11278 M 79 0 R D 9675 11430 M 79 0 R D +9675 11735 M 79 0 R D 9675 11887 M 79 0 R D 9675 12040 M 79 0 R D +9675 12192 M 79 0 R D 9675 12345 M 79 0 R D gsave 9108 9525 translate 0 0 M +90 rotate 1.01 dup scale -58.8433 0 N +( ) show grestore 17556 6706 M 0 5639 R D 17556 7010 M -158 0 R D +17556 8534 M -158 0 R D 17556 10058 M -158 0 R D 17556 11583 M -158 0 R D +17556 6706 M -79 0 R D 17556 6858 M -79 0 R D 17556 7163 M -79 0 R D +17556 7315 M -79 0 R D 17556 7468 M -79 0 R D 17556 7620 M -79 0 R D +17556 7772 M -79 0 R D 17556 7925 M -79 0 R D 17556 8077 M -79 0 R D +17556 8230 M -79 0 R D 17556 8382 M -79 0 R D 17556 8687 M -79 0 R D +17556 8839 M -79 0 R D 17556 8992 M -79 0 R D 17556 9144 M -79 0 R D +17556 9296 M -79 0 R D 17556 9449 M -79 0 R D 17556 9601 M -79 0 R D +17556 9754 M -79 0 R D 17556 9906 M -79 0 R D 17556 10211 M -79 0 R D +17556 10363 M -79 0 R D 17556 10516 M -79 0 R D 17556 10668 M -79 0 R D +17556 10821 M -79 0 R D 17556 10973 M -79 0 R D 17556 11125 M -79 0 R D +17556 11278 M -79 0 R D 17556 11430 M -79 0 R D 17556 11735 M -79 0 R D +17556 11887 M -79 0 R D 17556 12040 M -79 0 R D 17556 12192 M -79 0 R D +17556 12345 M -79 0 R D 20 setlinewidth 13383 8297 M 111 -111 R -111 -111 R +-111 111 R 111 111 R D 11123 6764 M 59 -59 R D 11064 6705 M 59 59 R D +11055 6710 M 5 -5 R D 11050 6705 M 5 5 R D 11075 6730 M 25 -25 R D +11050 6705 M 25 25 R D 11074 6739 M 34 -34 R D 11040 6705 M 34 34 R D +11237 6881 M 111 -111 R -65 -65 R D 11191 6705 M -65 65 R 111 111 R D +11178 6838 M 111 -111 R -22 -22 R D 11089 6705 M -22 22 R 111 111 R D +11245 6900 M 111 -111 R -84 -84 R D 11218 6705 M -84 84 R 111 111 R D +11129 6810 M 105 -105 R D 11024 6705 M 105 105 R D 11138 6824 M 111 -111 R +-8 -8 R D 11035 6705 M -8 8 R 111 111 R D 11251 6942 M 111 -111 R +-111 -111 R -111 111 R 111 111 R D 10981 6743 M 38 -38 R D 10943 6705 M +38 38 R D 11273 7011 M 111 -111 R -111 -111 R -111 111 R 111 111 R D +11320 7075 M 111 -111 R -111 -111 R -111 111 R 111 111 R D 11415 7176 M +111 -111 R -111 -111 R -111 111 R 111 111 R D 11435 7196 M 111 -111 R +-111 -111 R -111 111 R 111 111 R D 11246 7041 M 111 -111 R -111 -111 R +-111 111 R 111 111 R D 11394 7165 M 111 -111 R -111 -111 R -111 111 R +111 111 R D 11339 7121 M 111 -111 R -111 -111 R -111 111 R 111 111 R D +11444 7207 M 111 -111 R -111 -111 R -111 111 R 111 111 R D 11392 7151 M +111 -111 R -111 -111 R -111 111 R 111 111 R D 11342 7100 M 111 -111 R +-111 -111 R -111 111 R 111 111 R D 11369 7107 M 111 -111 R -111 -111 R +-111 111 R 111 111 R D 11445 7160 M 111 -111 R -111 -111 R -111 111 R +111 111 R D 11268 7004 M 111 -111 R -111 -111 R -111 111 R 111 111 R D +11366 7089 M 111 -111 R -111 -111 R -111 111 R 111 111 R D 11755 7412 M +111 -111 R -111 -111 R -111 111 R 111 111 R D 11576 7277 M 111 -111 R +-111 -111 R -111 111 R 111 111 R D 11600 7304 M 111 -111 R -111 -111 R +-111 111 R 111 111 R D 11452 7191 M 111 -111 R -111 -111 R -111 111 R +111 111 R D 11642 7340 M 111 -111 R -111 -111 R -111 111 R 111 111 R D +11696 7379 M 111 -111 R -111 -111 R -111 111 R 111 111 R D 11562 7266 M +111 -111 R -111 -111 R -111 111 R 111 111 R D 11677 7353 M 111 -111 R +-111 -111 R -111 111 R 111 111 R D 11590 7278 M 111 -111 R -111 -111 R +-111 111 R 111 111 R D 11595 7294 M 111 -111 R -111 -111 R -111 111 R +111 111 R D 11640 7344 M 111 -111 R -111 -111 R -111 111 R 111 111 R D +11630 7350 M 111 -111 R -111 -111 R -111 111 R 111 111 R D 11747 7457 M +111 -111 R -111 -111 R -111 111 R 111 111 R D 11373 7167 M 111 -111 R +-111 -111 R -111 111 R 111 111 R D 11526 7289 M 111 -111 R -111 -111 R +-111 111 R 111 111 R D 11754 7469 M 111 -111 R -111 -111 R -111 111 R +111 111 R D 11795 7498 M 111 -111 R -111 -111 R -111 111 R 111 111 R D +11621 7356 M 111 -111 R -111 -111 R -111 111 R 111 111 R D 11806 7504 M +111 -111 R -111 -111 R -111 111 R 111 111 R D 11848 7559 M 111 -111 R +-111 -111 R -111 111 R 111 111 R D 11761 7514 M 111 -111 R -111 -111 R +-111 111 R 111 111 R D 11779 7553 M 111 -111 R -111 -111 R -111 111 R +111 111 R D 11727 7535 M 111 -111 R -111 -111 R -111 111 R 111 111 R D +11877 7674 M 111 -111 R -111 -111 R -111 111 R 111 111 R D 12157 7869 M +111 -111 R -111 -111 R -111 111 R 111 111 R D 11893 7632 M 111 -111 R +-111 -111 R -111 111 R 111 111 R D 12056 7728 M 111 -111 R -111 -111 R +-111 111 R 111 111 R D 12031 7682 M 111 -111 R -111 -111 R -111 111 R +111 111 R D 12200 7786 M 111 -111 R -111 -111 R -111 111 R 111 111 R D +12410 7946 M 111 -111 R -111 -111 R -111 111 R 111 111 R D 12692 8158 M +111 -111 R -111 -111 R -111 111 R 111 111 R D 12897 8309 M 111 -111 R +-111 -111 R -111 111 R 111 111 R D 12683 8150 M 111 -111 R -111 -111 R +-111 111 R 111 111 R D 13803 8945 M 111 -111 R -111 -111 R -111 111 R +111 111 R D 14511 9407 M 111 -111 R -111 -111 R -111 111 R 111 111 R D +14735 9550 M 111 -111 R -111 -111 R -111 111 R 111 111 R D 15064 9746 M +111 -111 R -111 -111 R -111 111 R 111 111 R D 15192 9824 M 111 -111 R +-111 -111 R -111 111 R 111 111 R D 14882 9660 M 111 -111 R -111 -111 R +-111 111 R 111 111 R D 15354 9944 M 111 -111 R -111 -111 R -111 111 R +111 111 R D 15432 10009 M 111 -111 R -111 -111 R -111 111 R 111 111 R D +15239 9932 M 111 -111 R -111 -111 R -111 111 R 111 111 R D 15474 10080 M +111 -111 R -111 -111 R -111 111 R 111 111 R D 15564 10146 M 111 -111 R +-111 -111 R -111 111 R 111 111 R D 15100 9916 M 111 -111 R -111 -111 R +-111 111 R 111 111 R D 15897 10289 M 111 -111 R -111 -111 R -111 111 R +111 111 R D 15918 10326 M 111 -111 R -111 -111 R -111 111 R 111 111 R D +14803 9767 M 111 -111 R -111 -111 R -111 111 R 111 111 R D 14823 9789 M +111 -111 R -111 -111 R -111 111 R 111 111 R D 16280 10493 M 111 -111 R +-111 -111 R -111 111 R 111 111 R D 16233 10500 M 111 -111 R -111 -111 R +-111 111 R 111 111 R D 15537 10092 M 111 -111 R -111 -111 R -111 111 R +111 111 R D 14188 9421 M 111 -111 R -111 -111 R -111 111 R 111 111 R D +15491 10139 M 111 -111 R -111 -111 R -111 111 R 111 111 R D 14266 9459 M +111 -111 R -111 -111 R -111 111 R 111 111 R D 14393 9524 M 111 -111 R +-111 -111 R -111 111 R 111 111 R D 15351 10047 M 111 -111 R -111 -111 R +-111 111 R 111 111 R D 14565 9576 M 111 -111 R -111 -111 R -111 111 R +111 111 R D 14313 9416 M 111 -111 R -111 -111 R -111 111 R 111 111 R D +14114 9298 M 111 -111 R -111 -111 R -111 111 R 111 111 R D 14137 9309 M +111 -111 R -111 -111 R -111 111 R 111 111 R D 14047 9247 M 111 -111 R +-111 -111 R -111 111 R 111 111 R D 14493 9522 M 111 -111 R -111 -111 R +-111 111 R 111 111 R D 13820 9089 M 111 -111 R -111 -111 R -111 111 R +111 111 R D 13842 9093 M 111 -111 R -111 -111 R -111 111 R 111 111 R D +13638 8939 M 111 -111 R -111 -111 R -111 111 R 111 111 R D 13547 8870 M +111 -111 R -111 -111 R -111 111 R 111 111 R D 13489 8819 M 111 -111 R +-111 -111 R -111 111 R 111 111 R D 12937 8414 M 111 -111 R -111 -111 R +-111 111 R 111 111 R D 13389 8739 M 111 -111 R -111 -111 R -111 111 R +111 111 R D 13808 9030 M 111 -111 R -111 -111 R -111 111 R 111 111 R D +14474 9344 M 111 -111 R -111 -111 R -111 111 R 111 111 R D 13524 8828 M +111 -111 R -111 -111 R -111 111 R 111 111 R D 13251 8651 M 111 -111 R +-111 -111 R -111 111 R 111 111 R D 12813 8335 M 111 -111 R -111 -111 R +-111 111 R 111 111 R D 13037 8501 M 111 -111 R -111 -111 R -111 111 R +111 111 R D 13100 8548 M 111 -111 R -111 -111 R -111 111 R 111 111 R D +12984 8466 M 111 -111 R -111 -111 R -111 111 R 111 111 R D 14458 9509 M +111 -111 R -111 -111 R -111 111 R 111 111 R D 10600 6705 M 169 118 R +219 152 R 219 152 R 219 153 R 219 152 R 219 153 R 219 152 R 219 152 R +219 153 R 219 152 R 219 153 R 219 152 R 218 152 R 219 153 R 219 152 R +219 153 R 219 152 R 219 152 R 219 153 R 219 152 R 219 153 R 219 152 R +219 152 R 219 153 R 218 152 R 219 153 R 219 152 R 219 153 R 219 152 R +219 152 R 219 153 R 218 151 R D gsave 10113 11583 translate 0 0 M +1.2 dup scale +(f) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(gas) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( = 0.4) show grestore 0.000 0.514 1.000 setrgbcolor 11028 6881 M -1 14 R +-3 15 R -5 13 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -14 5 R +-14 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R +-9 -11 R -9 -12 R -6 -13 R -5 -13 R -2 -15 R -1 -14 R 1 -15 R 2 -14 R +5 -14 R 6 -13 R 9 -12 R 9 -11 R 11 -9 R 12 -8 R 13 -7 R 14 -4 R 14 -3 R +15 -1 R 14 1 R 14 3 R 14 4 R 13 7 R 12 8 R 11 9 R 10 11 R 8 12 R 6 13 R +5 14 R 3 14 R 1 15 R F +10637 6705 M -6 4 R -13 6 R -14 5 R -14 3 R -15 1 R -14 -1 R -14 -3 R +-14 -5 R -13 -6 R -6 -4 R F +10493 6705 M -10 2 R -14 1 R -15 -1 R -10 -2 R F +10507 6705 M -4 1 R -14 1 R -15 -1 R -5 -1 R F +10587 6705 M -1 1 R -12 8 R -13 6 R -14 5 R -14 3 R -15 0 R -14 0 R -15 -3 R +-13 -5 R -13 -6 R -12 -8 R -2 -1 R F +10569 6705 M -7 5 R -13 6 R -14 5 R -14 3 R -14 0 R -15 0 R -14 -3 R +-14 -5 R -13 -6 R -8 -5 R F +10842 6809 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -10 11 R -10 9 R +-13 8 R -13 7 R -13 4 R -15 3 R -14 1 R -14 -1 R -15 -3 R -13 -4 R -14 -7 R +-12 -8 R -10 -9 R -10 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -15 R +1 -14 R 3 -15 R 4 -13 R 7 -13 R 8 -12 R 10 -11 R 10 -10 R 12 -8 R 14 -6 R +5 -2 R 73 0 R 6 2 R 13 6 R 13 8 R 10 10 R 10 11 R 8 12 R 7 13 R 4 13 R +3 15 R 1 14 R F +11046 6987 M -1 14 R -2 14 R -5 14 R -6 13 R -9 12 R -9 11 R -11 10 R +-12 8 R -13 6 R -14 5 R -14 3 R -15 1 R -14 -1 R -14 -3 R -14 -5 R -13 -6 R +-12 -8 R -11 -10 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -14 R +1 -15 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -9 R 12 -9 R 13 -6 R +14 -5 R 14 -2 R 14 -1 R 15 1 R 14 2 R 14 5 R 13 6 R 12 9 R 11 9 R 9 11 R +9 12 R 6 13 R 5 14 R 2 14 R 1 15 R F +11072 7018 M -1 15 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 9 R +-12 8 R -13 7 R -14 4 R -14 3 R -14 1 R -15 -1 R -14 -3 R -14 -4 R -13 -7 R +-12 -8 R -11 -9 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R 0 -15 R +0 -14 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -10 R 12 -8 R 13 -6 R +14 -5 R 14 -3 R 15 -1 R 14 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 10 11 R +8 12 R 6 13 R 5 14 R 3 14 R 1 14 R F +11216 7145 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -9 11 R -11 9 R -12 8 R +-13 7 R -14 4 R -14 3 R -15 1 R -14 -1 R -15 -3 R -13 -4 R -13 -7 R -12 -8 R +-11 -9 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -15 R 1 -14 R +3 -15 R 5 -13 R 6 -13 R 8 -12 R 10 -11 R 11 -10 R 12 -8 R 13 -6 R 13 -5 R +15 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 9 11 R 8 12 R +7 13 R 4 13 R 3 15 R 1 14 R F +11299 7220 M -1 14 R -3 14 R -4 14 R -7 13 R -8 12 R -9 11 R -11 10 R +-12 8 R -13 6 R -14 5 R -14 3 R -15 1 R -14 -1 R -15 -3 R -13 -5 R -13 -6 R +-12 -8 R -11 -10 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -14 R +1 -15 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -10 R 12 -8 R 13 -6 R +13 -5 R 15 -3 R 14 0 R 15 0 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 9 11 R +8 12 R 7 13 R 4 14 R 3 14 R 1 15 R F +11383 7294 M 0 14 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 10 R +-12 8 R -13 6 R -14 5 R -14 3 R -15 1 R -14 -1 R -14 -3 R -14 -5 R -13 -6 R +-12 -8 R -11 -10 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -14 R +1 -15 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -9 R 12 -8 R 13 -7 R +14 -4 R 14 -3 R 14 -1 R 15 1 R 14 3 R 14 4 R 13 7 R 12 8 R 11 9 R 10 11 R +8 12 R 6 13 R 5 14 R 3 14 R 0 15 R F +11539 7424 M -1 14 R -3 15 R -4 13 R -7 13 R -8 12 R -9 11 R -11 10 R +-12 8 R -13 6 R -14 5 R -14 3 R -15 1 R -14 -1 R -14 -3 R -14 -5 R -13 -6 R +-12 -8 R -11 -10 R -10 -11 R -8 -12 R -6 -13 R -5 -13 R -3 -15 R -1 -14 R +1 -15 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -9 R 12 -8 R 13 -7 R +14 -4 R 14 -3 R 14 -1 R 15 1 R 14 3 R 14 4 R 13 7 R 12 8 R 11 9 R 9 11 R +8 12 R 7 13 R 4 14 R 3 14 R 1 15 R F +11554 7443 M -1 15 R -2 14 R -5 14 R -6 13 R -9 12 R -9 11 R -11 9 R -12 8 R +-13 7 R -14 4 R -14 3 R -15 1 R -14 -1 R -14 -3 R -14 -4 R -13 -7 R -12 -8 R +-11 -9 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -15 R 1 -14 R +3 -15 R 5 -13 R 6 -13 R 8 -12 R 10 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R +14 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 9 11 R 9 12 R +6 13 R 5 13 R 2 15 R 1 14 R F +11609 7489 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -9 11 R -11 9 R -12 8 R +-13 7 R -14 4 R -14 3 R -15 1 R -14 -1 R -15 -3 R -13 -4 R -13 -7 R -13 -8 R +-10 -9 R -10 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -15 R 1 -14 R +3 -15 R 4 -13 R 7 -13 R 8 -12 R 10 -11 R 10 -10 R 13 -8 R 13 -6 R 13 -5 R +15 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 9 11 R 8 12 R +7 13 R 4 13 R 3 15 R 1 14 R F +11481 7371 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -10 11 R -10 9 R +-12 8 R -14 7 R -13 4 R -15 3 R -14 1 R -14 -1 R -15 -3 R -13 -4 R -13 -7 R +-13 -8 R -10 -9 R -10 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -15 R +1 -14 R 3 -15 R 4 -13 R 7 -13 R 8 -12 R 10 -11 R 10 -10 R 13 -8 R 13 -6 R +13 -5 R 15 -3 R 14 -1 R 14 1 R 15 3 R 13 5 R 14 6 R 12 8 R 10 10 R 10 11 R +8 12 R 7 13 R 4 13 R 3 15 R 1 14 R F +11676 7502 M -1 14 R -3 15 R -5 13 R -6 13 R -8 12 R -10 11 R -11 10 R +-12 8 R -13 6 R -14 5 R -14 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R -13 -6 R +-12 -8 R -11 -10 R -9 -11 R -8 -12 R -7 -13 R -5 -13 R -2 -15 R -1 -14 R +1 -15 R 2 -14 R 5 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -9 R 12 -8 R 13 -7 R +14 -4 R 14 -3 R 15 -1 R 14 1 R 14 3 R 14 4 R 13 7 R 12 8 R 11 9 R 10 11 R +8 12 R 6 13 R 5 14 R 3 14 R 1 15 R F +11853 7618 M 0 14 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 10 R +-12 8 R -13 6 R -14 5 R -14 3 R -15 1 R -14 -1 R -14 -3 R -14 -5 R -13 -6 R +-12 -8 R -11 -10 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -14 R +1 -15 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -10 R 12 -8 R 13 -6 R +14 -5 R 14 -2 R 14 -1 R 15 1 R 14 2 R 14 5 R 13 6 R 12 8 R 11 10 R 10 11 R +8 12 R 6 13 R 5 14 R 3 14 R 0 15 R F +12015 7719 M -1 15 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -10 9 R +-13 8 R -13 7 R -13 5 R -15 2 R -14 1 R -15 -1 R -14 -2 R -14 -5 R -13 -7 R +-12 -8 R -11 -9 R -9 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -15 R +1 -14 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -10 R 12 -8 R 13 -6 R +14 -5 R 14 -3 R 15 -1 R 14 1 R 15 3 R 13 5 R 13 6 R 13 8 R 10 10 R 10 11 R +8 12 R 6 13 R 5 14 R 3 14 R 1 14 R F +11922 7632 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -9 11 R -11 9 R -12 9 R +-13 6 R -14 5 R -14 2 R -15 1 R -14 -1 R -15 -2 R -13 -5 R -13 -6 R -12 -9 R +-11 -9 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -15 R 1 -14 R +3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -10 R 12 -8 R 13 -6 R 13 -5 R +15 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 9 11 R 8 12 R +7 13 R 4 14 R 3 14 R 1 14 R F +12113 7807 M -1 14 R -3 15 R -5 13 R -6 13 R -8 12 R -10 11 R -11 10 R +-12 8 R 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15 setlinewidth 1794 1067 M 7881 0 R D 2888 1067 M +0 112 R D gsave 2888 533 translate 0 0 M 1.01 dup scale -188.172 0 N +(-3) show grestore 5078 1067 M 0 112 R D gsave 5078 533 translate 0 0 M +1.01 dup scale -188.172 0 N +(-2) show grestore 7267 1067 M 0 112 R D gsave 7267 533 translate 0 0 M +1.01 dup scale -188.172 0 N +(-1) show grestore 9456 1067 M 0 112 R D gsave 9456 533 translate 0 0 M +1.01 dup scale -117.687 0 N +(0) show grestore 1794 1067 M 0 56 R D 2013 1067 M 0 56 R D 2232 1067 M +0 56 R D 2451 1067 M 0 56 R D 2670 1067 M 0 56 R D 3107 1067 M 0 56 R D +3326 1067 M 0 56 R D 3545 1067 M 0 56 R D 3764 1067 M 0 56 R D 3983 1067 M +0 56 R D 4202 1067 M 0 56 R D 4421 1067 M 0 56 R D 4640 1067 M 0 56 R D +4859 1067 M 0 56 R D 5297 1067 M 0 56 R D 5515 1067 M 0 56 R D 5734 1067 M +0 56 R D 5953 1067 M 0 56 R D 6172 1067 M 0 56 R D 6391 1067 M 0 56 R D +6610 1067 M 0 56 R D 6829 1067 M 0 56 R D 7048 1067 M 0 56 R D 7486 1067 M +0 56 R D 7705 1067 M 0 56 R D 7924 1067 M 0 56 R D 8142 1067 M 0 56 R D +8361 1067 M 0 56 R D 8580 1067 M 0 56 R D 8799 1067 M 0 56 R D 9018 1067 M +0 56 R D 9237 1067 M 0 56 R D 9675 1067 M 0 56 R D +gsave 5734 71 translate 0 0 M 1.01 dup scale -58.8433 0 N +( ) show grestore 1794 6706 M 7881 0 R D 2888 6706 M 0 -113 R D 5078 6706 M +0 -113 R D 7267 6706 M 0 -113 R D 9456 6706 M 0 -113 R D 1794 6706 M 0 -57 R +D 2013 6706 M 0 -57 R D 2232 6706 M 0 -57 R D 2451 6706 M 0 -57 R D +2670 6706 M 0 -57 R D 3107 6706 M 0 -57 R D 3326 6706 M 0 -57 R D +3545 6706 M 0 -57 R D 3764 6706 M 0 -57 R D 3983 6706 M 0 -57 R D +4202 6706 M 0 -57 R D 4421 6706 M 0 -57 R D 4640 6706 M 0 -57 R D +4859 6706 M 0 -57 R D 5297 6706 M 0 -57 R D 5515 6706 M 0 -57 R D +5734 6706 M 0 -57 R D 5953 6706 M 0 -57 R D 6172 6706 M 0 -57 R D +6391 6706 M 0 -57 R D 6610 6706 M 0 -57 R D 6829 6706 M 0 -57 R D +7048 6706 M 0 -57 R D 7486 6706 M 0 -57 R D 7705 6706 M 0 -57 R D +7924 6706 M 0 -57 R D 8142 6706 M 0 -57 R D 8361 6706 M 0 -57 R D +8580 6706 M 0 -57 R D 8799 6706 M 0 -57 R D 9018 6706 M 0 -57 R D +9237 6706 M 0 -57 R D 9675 6706 M 0 -57 R D 1794 1067 M 0 5639 R D +1794 1371 M 157 0 R D gsave 1682 1229 translate 0 0 M 1.01 dup scale +-376.343 0 N +(-3) show grestore 1794 2895 M 157 0 R D gsave 1682 2753 translate 0 0 M +1.01 dup scale -376.343 0 N +(-2) show grestore 1794 4420 M 157 0 R D gsave 1682 4277 translate 0 0 M +1.01 dup scale -376.343 0 N +(-1) show grestore 1794 5944 M 157 0 R D gsave 1682 5801 translate 0 0 M +1.01 dup scale -235.373 0 N +(0) show grestore 1794 1067 M 79 0 R D 1794 1219 M 79 0 R D 1794 1524 M +79 0 R D 1794 1676 M 79 0 R D 1794 1829 M 79 0 R D 1794 1981 M 79 0 R D +1794 2133 M 79 0 R D 1794 2286 M 79 0 R D 1794 2438 M 79 0 R D 1794 2591 M +79 0 R D 1794 2743 M 79 0 R D 1794 3048 M 79 0 R D 1794 3200 M 79 0 R D +1794 3353 M 79 0 R D 1794 3505 M 79 0 R D 1794 3657 M 79 0 R D 1794 3810 M +79 0 R D 1794 3962 M 79 0 R D 1794 4115 M 79 0 R D 1794 4267 M 79 0 R D +1794 4572 M 79 0 R D 1794 4724 M 79 0 R D 1794 4877 M 79 0 R 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All Rights Reserved. +%v 4 +/$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C +{currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint +stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} +bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show +grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 +setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 +{[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 +100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 +{[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef +/ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} +ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont +exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica +findfont exch scalefont setfont (\267) show currentpoint grestore moveto} +bdef end 2.5 setmiterlimit +%%EndProlog +%%Page: 0 1 +%%PageRequirements: color +%%PageResources: (atend) +%%PageOrientation: Portrait +%%PageBoundingBox: 54 360 558 720 +%%BeginPageSetup +save +$IDL_DICT begin 54 360 translate 0.0283465 dup scale +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +%%EndPageSetup +15 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 2242 6706 M 4955 0 R D +3247 6706 M 0 105 R D gsave 3247 6172 translate 0 0 M 1.01 dup scale +-58.8433 0 N +( ) show grestore 4586 6706 M 0 105 R D gsave 4586 6172 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 5925 6706 M 0 105 R D gsave 5925 6172 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 2242 6706 M 0 52 R D 2577 6706 M 0 52 R D 2912 6706 M +0 52 R D 3581 6706 M 0 52 R D 3916 6706 M 0 52 R D 4251 6706 M 0 52 R D +4921 6706 M 0 52 R D 5255 6706 M 0 52 R D 5590 6706 M 0 52 R D 6260 6706 M +0 52 R D 6595 6706 M 0 52 R D 6929 6706 M 0 52 R D 2242 11989 M 4955 0 R D +3247 11989 M 0 -106 R D 4586 11989 M 0 -106 R D 5925 11989 M 0 -106 R D +2242 11989 M 0 -53 R D 2577 11989 M 0 -53 R D 2912 11989 M 0 -53 R D +3581 11989 M 0 -53 R D 3916 11989 M 0 -53 R D 4251 11989 M 0 -53 R D +4921 11989 M 0 -53 R D 5255 11989 M 0 -53 R D 5590 11989 M 0 -53 R D +6260 11989 M 0 -53 R D 6595 11989 M 0 -53 R D 6929 11989 M 0 -53 R D +2242 6706 M 0 5283 R D 2242 7201 M 99 0 R D gsave 2130 7059 translate 0 0 M +1.01 dup scale -729.403 0 N +(-7.5) show grestore 2242 8026 M 99 0 R D gsave 2130 7884 translate 0 0 M +1.01 dup scale -729.403 0 N +(-7.0) show grestore 2242 8852 M 99 0 R D gsave 2130 8710 translate 0 0 M +1.01 dup scale -729.403 0 N +(-6.5) show grestore 2242 9678 M 99 0 R D gsave 2130 9535 translate 0 0 M +1.01 dup scale -729.403 0 N +(-6.0) show grestore 2242 10503 M 99 0 R D gsave 2130 10361 translate 0 0 M +1.01 dup scale -729.403 0 N +(-5.5) show grestore 2242 11329 M 99 0 R D gsave 2130 11186 translate 0 0 M +1.01 dup scale -729.403 0 N +(-5.0) show grestore 2242 6706 M 50 0 R D 2242 6871 M 50 0 R D 2242 7036 M +50 0 R D 2242 7366 M 50 0 R D 2242 7531 M 50 0 R D 2242 7696 M 50 0 R D +2242 7861 M 50 0 R D 2242 8192 M 50 0 R D 2242 8357 M 50 0 R D 2242 8522 M +50 0 R D 2242 8687 M 50 0 R D 2242 9017 M 50 0 R D 2242 9182 M 50 0 R D +2242 9347 M 50 0 R D 2242 9512 M 50 0 R D 2242 9843 M 50 0 R D 2242 10008 M +50 0 R D 2242 10173 M 50 0 R D 2242 10338 M 50 0 R D 2242 10668 M 50 0 R D +2242 10833 M 50 0 R D 2242 10998 M 50 0 R D 2242 11163 M 50 0 R D +2242 11494 M 50 0 R D 2242 11659 M 50 0 R D 2242 11824 M 50 0 R D +2242 11989 M 50 0 R D 7197 6706 M 0 5283 R D 7197 7201 M -99 0 R D +7197 8026 M -99 0 R D 7197 8852 M -99 0 R D 7197 9678 M -99 0 R D +7197 10503 M -99 0 R D 7197 11329 M -99 0 R D 7197 6706 M -49 0 R D +7197 6871 M -49 0 R D 7197 7036 M -49 0 R D 7197 7366 M -49 0 R D +7197 7531 M -49 0 R D 7197 7696 M -49 0 R D 7197 7861 M -49 0 R D +7197 8192 M -49 0 R D 7197 8357 M -49 0 R D 7197 8522 M -49 0 R D +7197 8687 M -49 0 R D 7197 9017 M -49 0 R D 7197 9182 M -49 0 R D +7197 9347 M -49 0 R D 7197 9512 M -49 0 R D 7197 9843 M -49 0 R D +7197 10008 M -49 0 R D 7197 10173 M -49 0 R D 7197 10338 M -49 0 R D +7197 10668 M -49 0 R D 7197 10833 M -49 0 R D 7197 10998 M -49 0 R D +7197 11163 M -49 0 R D 7197 11494 M -49 0 R D 7197 11659 M -49 0 R D +7197 11824 M -49 0 R D 7197 11989 M -49 0 R D 3889 9590 M 0 222 R 222 0 R +0 -222 R -222 0 R F +3722 9587 M 0 222 R 222 0 R 0 -222 R -222 0 R F +3554 9396 M 0 222 R 222 0 R 0 -222 R -222 0 R F +3387 9865 M 0 222 R 222 0 R 0 -222 R -222 0 R F +3219 10152 M 0 222 R 222 0 R 0 -222 R -222 0 R F +3052 10049 M 0 222 R 222 0 R 0 -222 R -222 0 R F +2885 10237 M 0 222 R 222 0 R 0 -222 R -222 0 R F +2717 10130 M 0 222 R 222 0 R 0 -222 R -222 0 R F +2550 10106 M 0 222 R 222 0 R 0 -222 R -222 0 R F +10 setlinewidth 4726 8352 M 0 222 R 222 0 R 0 -222 R -222 0 R D 4559 8527 M +0 222 R 222 0 R 0 -222 R -222 0 R D 4391 8728 M 0 222 R 222 0 R 0 -222 R +-222 0 R D 4224 8858 M 0 222 R 222 0 R 0 -222 R -222 0 R D 4056 9057 M +0 222 R 222 0 R 0 -222 R -222 0 R D 20 setlinewidth 4837 6705 M 0 2255 R +-25 0 R 50 0 R D 4645 8015 M 49 0 R -24 0 R 0 952 R -25 0 R 49 0 R D +4477 8414 M 50 0 R -25 0 R 0 690 R -25 0 R 50 0 R D 4310 8627 M 50 0 R +-25 0 R 0 572 R -25 0 R 50 0 R D 4143 8893 M 49 0 R -25 0 R 0 473 R -24 0 R +49 0 R D 3975 9517 M 50 0 R -25 0 R 0 330 R -25 0 R 50 0 R D 3808 9514 M +49 0 R -24 0 R 0 330 R -25 0 R 49 0 R D 3640 9280 M 50 0 R -25 0 R 0 399 R +-25 0 R 50 0 R D 3473 9809 M 50 0 R -25 0 R 0 302 R -25 0 R 50 0 R D +3306 10122 M 49 0 R -25 0 R 0 259 R -24 0 R 49 0 R D 3138 10009 M 50 0 R +-25 0 R 0 276 R -25 0 R 50 0 R D 2971 10217 M 49 0 R -24 0 R 0 242 R -25 0 R +49 0 R D 2803 10098 M 50 0 R -25 0 R 0 262 R -25 0 R 50 0 R D 2636 10069 M +50 0 R -25 0 R 0 271 R -25 0 R 50 0 R D 0.082 1.000 0.000 setrgbcolor +2510 10305 M -1 13 R -3 13 R -4 12 R -6 12 R -7 11 R -9 10 R -9 8 R -11 7 R +-12 6 R -12 4 R -13 3 R -13 1 R -13 -1 R -13 -3 R -13 -4 R -11 -6 R -11 -7 R +-10 -8 R -9 -10 R -7 -11 R -6 -12 R -4 -12 R -2 -13 R -1 -13 R 1 -13 R +2 -13 R 4 -12 R 6 -12 R 7 -11 R 9 -10 R 10 -8 R 11 -8 R 11 -5 R 13 -5 R +13 -2 R 13 -1 R 13 1 R 13 2 R 12 5 R 12 5 R 11 8 R 9 8 R 9 10 R 7 11 R +6 12 R 4 12 R 3 13 R 1 13 R F +2844 10255 M 0 13 R -3 13 R -4 13 R -6 11 R -7 11 R -9 10 R -10 9 R -11 7 R +-11 6 R -13 4 R -12 2 R -14 1 R -13 -1 R -12 -2 R -13 -4 R -11 -6 R -11 -7 R +-10 -9 R -9 -10 R -7 -11 R -6 -11 R -4 -13 R -3 -13 R 0 -13 R 0 -13 R +3 -12 R 4 -13 R 6 -12 R 7 -10 R 9 -10 R 10 -9 R 11 -7 R 11 -6 R 13 -4 R +12 -3 R 13 -1 R 14 1 R 12 3 R 13 4 R 11 6 R 11 7 R 10 9 R 9 10 R 7 10 R +6 12 R 4 13 R 3 12 R 0 13 R F +3179 10222 M -1 13 R -2 13 R -4 13 R -6 11 R -7 11 R -9 10 R -10 9 R -11 7 R +-11 6 R -13 4 R -13 2 R -13 1 R -13 -1 R -13 -2 R -12 -4 R -12 -6 R -11 -7 R +-9 -9 R -9 -10 R -7 -11 R -6 -11 R -4 -13 R -3 -13 R -1 -13 R 1 -13 R +3 -12 R 4 -13 R 6 -12 R 7 -10 R 9 -10 R 9 -9 R 11 -7 R 12 -6 R 12 -4 R +13 -3 R 13 -1 R 13 1 R 13 3 R 13 4 R 11 6 R 11 7 R 10 9 R 9 10 R 7 10 R +6 12 R 4 13 R 2 12 R 1 13 R F +3514 10123 M -1 13 R -2 13 R -5 13 R -5 11 R -8 11 R -8 10 R -10 9 R -11 7 R +-12 6 R -12 4 R -13 2 R -13 1 R -13 -1 R -13 -2 R -12 -4 R -12 -6 R -11 -7 R +-10 -9 R -8 -10 R -7 -11 R -6 -11 R -4 -13 R -3 -13 R -1 -13 R 1 -13 R +3 -13 R 4 -12 R 6 -12 R 7 -11 R 8 -9 R 10 -9 R 11 -7 R 12 -6 R 12 -4 R +13 -3 R 13 -1 R 13 1 R 13 3 R 12 4 R 12 6 R 11 7 R 10 9 R 8 9 R 8 11 R +5 12 R 5 12 R 2 13 R 1 13 R F +3849 9810 M -1 13 R -3 12 R -4 13 R -6 12 R -7 10 R -8 10 R -10 9 R -11 7 R +-12 6 R -12 4 R -13 3 R -13 1 R -13 -1 R -13 -3 R -12 -4 R -12 -6 R -11 -7 R +-10 -9 R -8 -10 R -8 -10 R -5 -12 R -5 -13 R -2 -12 R -1 -13 R 1 -13 R +2 -13 R 5 -13 R 5 -11 R 8 -11 R 8 -10 R 10 -9 R 11 -7 R 12 -6 R 12 -4 R +13 -2 R 13 -1 R 13 1 R 13 2 R 12 4 R 12 6 R 11 7 R 10 9 R 8 10 R 7 11 R +6 11 R 4 13 R 3 13 R 1 13 R F +4184 9611 M -1 14 R -3 12 R -4 13 R -6 11 R -7 11 R -9 10 R -9 9 R -11 7 R +-12 6 R -12 4 R -13 3 R -13 0 R -13 0 R -13 -3 R -13 -4 R -11 -6 R -11 -7 R +-10 -9 R -9 -10 R -7 -11 R -6 -11 R -4 -13 R -2 -12 R -1 -14 R 1 -13 R +2 -12 R 4 -13 R 6 -11 R 7 -11 R 9 -10 R 10 -9 R 11 -7 R 11 -6 R 13 -4 R +13 -3 R 13 0 R 13 0 R 13 3 R 12 4 R 12 6 R 11 7 R 9 9 R 9 10 R 7 11 R 6 11 R +4 13 R 3 12 R 1 13 R F +4518 9215 M 0 13 R -3 13 R -4 12 R -6 12 R -7 11 R -9 10 R -10 8 R -11 8 R +-11 6 R -13 4 R -12 2 R -14 1 R -13 -1 R -12 -2 R -13 -4 R -11 -6 R -11 -8 R +-10 -8 R -9 -10 R -7 -11 R -6 -12 R -4 -12 R -3 -13 R 0 -13 R 0 -13 R +3 -13 R 4 -12 R 6 -12 R 7 -11 R 9 -9 R 10 -9 R 11 -7 R 11 -6 R 13 -4 R +12 -3 R 13 -1 R 14 1 R 12 3 R 13 4 R 11 6 R 11 7 R 10 9 R 9 9 R 7 11 R +6 12 R 4 12 R 3 13 R 0 13 R F +4853 8753 M -1 13 R -2 13 R -4 12 R -6 12 R -7 11 R -9 10 R -10 8 R -11 7 R +-11 6 R -13 4 R -13 3 R -13 1 R -13 -1 R -13 -3 R -12 -4 R -12 -6 R -11 -7 R +-9 -8 R -9 -10 R -7 -11 R -6 -12 R -4 -12 R -3 -13 R -1 -13 R 1 -13 R +3 -13 R 4 -12 R 6 -12 R 7 -11 R 9 -10 R 9 -8 R 11 -8 R 12 -5 R 12 -5 R +13 -2 R 13 -1 R 13 1 R 13 2 R 13 5 R 11 5 R 11 8 R 10 8 R 9 10 R 7 11 R +6 12 R 4 12 R 2 13 R 1 13 R F +5188 8026 M -1 13 R -2 13 R -5 13 R -5 11 R -8 11 R -8 10 R -10 9 R -11 7 R +-12 6 R -12 4 R -13 2 R -13 1 R -13 -1 R -13 -2 R -12 -4 R -12 -6 R -11 -7 R +-10 -9 R -8 -10 R -7 -11 R -6 -11 R -4 -13 R -3 -13 R -1 -13 R 1 -13 R +3 -12 R 4 -13 R 6 -12 R 7 -10 R 8 -10 R 10 -9 R 11 -7 R 12 -6 R 12 -4 R +13 -3 R 13 0 R 13 0 R 13 3 R 12 4 R 12 6 R 11 7 R 10 9 R 8 10 R 8 10 R +5 12 R 5 13 R 2 12 R 1 13 R F +5523 7135 M -1 13 R -3 13 R -4 12 R -6 12 R -7 11 R -8 10 R -10 8 R -11 7 R +-12 6 R -12 4 R -13 3 R -13 1 R -13 -1 R -13 -3 R -12 -4 R -12 -6 R -11 -7 R +-10 -8 R -8 -10 R -8 -11 R -5 -12 R -5 -12 R -2 -13 R -1 -13 R 1 -13 R +2 -13 R 5 -12 R 5 -12 R 8 -11 R 8 -10 R 10 -8 R 11 -8 R 12 -5 R 12 -5 R +13 -2 R 13 -1 R 13 1 R 13 2 R 12 5 R 12 5 R 11 8 R 10 8 R 8 10 R 7 11 R +6 12 R 4 12 R 3 13 R 1 13 R F +5858 7234 M -1 13 R -3 13 R -4 12 R -6 12 R -7 11 R -9 10 R -9 8 R -11 7 R +-12 6 R -12 4 R -13 3 R -13 1 R -13 -1 R -13 -3 R -13 -4 R -11 -6 R -11 -7 R +-10 -8 R -9 -10 R -7 -11 R -6 -12 R -4 -12 R -2 -13 R -1 -13 R 1 -13 R +2 -13 R 4 -12 R 6 -12 R 7 -11 R 9 -10 R 10 -8 R 11 -8 R 11 -5 R 13 -5 R +13 -2 R 13 -1 R 13 1 R 13 2 R 12 5 R 12 5 R 11 8 R 9 8 R 9 10 R 7 11 R +6 12 R 4 12 R 3 13 R 1 13 R F +2385 10156 M 49 0 R -24 0 R 0 265 R -25 0 R 49 0 R D 2720 10189 M 49 0 R +-25 0 R 0 116 R -24 0 R 49 0 R D 3055 10189 M 49 0 R -25 0 R 0 66 R -24 0 R +49 0 R D 3389 10090 M 50 0 R -25 0 R 0 66 R -25 0 R 50 0 R D 3724 9777 M +50 0 R -25 0 R 0 66 R -25 0 R 50 0 R D 4059 9562 M 49 0 R -24 0 R 0 99 R +-25 0 R 49 0 R D 4394 9149 M 49 0 R -25 0 R 0 132 R -24 0 R 49 0 R D +4729 8654 M 49 0 R -25 0 R 0 181 R -24 0 R 49 0 R D 5063 7828 M 50 0 R +-25 0 R 0 380 R -25 0 R 50 0 R D 5398 6739 M 50 0 R -25 0 R 0 759 R -25 0 R +50 0 R D 5733 6838 M 49 0 R -24 0 R 0 759 R -25 0 R 49 0 R D 6092 6705 M +0 562 R -24 0 R 49 0 R D 0.000 0.000 0.000 setrgbcolor 2242 10227 M 10 4 R +92 -53 R 93 -56 R 92 -58 R 92 -60 R 92 4 R 92 -65 R 91 -68 R 92 -69 R +91 -72 R 91 -20 R 90 -77 R 91 -79 R 90 -81 R 91 -40 R 90 -86 R 90 -88 R +90 -90 R 89 -92 R 90 -61 R 89 -97 R 90 -99 R 89 -101 R 89 -103 R 88 -81 R +89 -107 R 89 -110 R 88 -112 R 88 -95 R 89 -117 R 88 -118 R 88 -120 R +88 -122 R 87 -112 R 88 -126 R 88 -129 R 87 -130 R 87 -124 R 88 -135 R +87 -137 R 25 -40 R D 2242 10628 M 10 8 R 92 -28 R 93 -30 R 92 -32 R 92 -34 R +92 46 R 92 -40 R 91 -41 R 92 -44 R 91 -46 R 91 20 R 90 -51 R 91 -53 R +90 -55 R 91 -2 R 90 -60 R 90 -63 R 90 -65 R 89 -66 R 90 -25 R 89 -71 R +90 -74 R 89 -76 R 89 -78 R 88 -45 R 89 -83 R 89 -85 R 88 -87 R 88 -62 R +89 -91 R 88 -94 R 88 -95 R 88 -98 R 87 -80 R 88 -102 R 88 -104 R 87 -106 R +87 -93 R 88 -111 R 87 -112 R 87 -115 R 87 -116 R 87 -109 R 87 -120 R +86 -123 R 87 -125 R 87 -126 R 86 -122 R 87 -131 R 86 -133 R 87 -134 R +86 -132 R 17 -29 R D L1 2242 11291 M 10 -4 R 92 -41 R 93 -19 R 92 -46 R +92 -48 R 92 -50 R 92 -33 R 91 -54 R 92 -57 R 91 -58 R 91 -60 R 90 -48 R +91 -65 R 90 -66 R 91 -68 R 90 -70 R 90 -62 R 90 -74 R 89 -76 R 90 -78 R +89 -72 R 90 -82 R 89 -84 R 89 -85 R 88 -87 R 89 -85 R 89 -91 R 88 -93 R +88 -95 R 89 -94 R 88 -99 R 88 -100 R 88 -102 R 87 -105 R 88 -104 R 88 -108 R +87 -110 R 87 -111 R 88 -114 R 87 -114 R 87 -117 R 87 -119 R 87 -121 R +87 -122 R 86 -125 R 87 -127 R 87 -128 R 86 -130 R 87 -132 R 86 -134 R +87 -136 R 86 -138 R 27 -45 R D 2242 9503 M 10 -1 R 92 -15 R 93 174 R +92 -21 R 92 -24 R 92 -25 R 92 -28 R 91 135 R 92 -33 R 91 -36 R 91 -38 R +90 103 R 91 -44 R 90 -46 R 91 -47 R 90 -51 R 90 69 R 90 -56 R 89 -58 R +90 -60 R 89 40 R 90 -65 R 89 -68 R 89 -70 R 88 -72 R 89 10 R 89 -77 R +88 -80 R 88 -82 R 89 -83 R 88 -18 R 88 -89 R 88 -91 R 87 -94 R 88 -40 R +88 -98 R 87 -101 R 87 -103 R 88 -104 R 87 -64 R 87 -110 R 87 -112 R +87 -114 R 87 -116 R 86 -85 R 87 -121 R 87 -123 R 86 -125 R 87 -102 R +86 -129 R 87 -132 R 50 -78 R D gsave 2577 7036 translate 0 0 M 1.1 dup scale +(z = 0.28 - 0.8) show grestore 15 setlinewidth L0 7197 6706 M 4955 0 R D +8202 6706 M 0 105 R D gsave 8202 6172 translate 0 0 M 1.01 dup scale +-58.8433 0 N +( ) show grestore 9541 6706 M 0 105 R D gsave 9541 6172 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 10880 6706 M 0 105 R D gsave 10880 6172 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 7197 6706 M 0 52 R D 7532 6706 M 0 52 R D 7867 6706 M +0 52 R D 8537 6706 M 0 52 R D 8871 6706 M 0 52 R D 9206 6706 M 0 52 R D +9876 6706 M 0 52 R D 10211 6706 M 0 52 R D 10545 6706 M 0 52 R D +11215 6706 M 0 52 R D 11550 6706 M 0 52 R D 11885 6706 M 0 52 R D +7197 11989 M 4955 0 R D 8202 11989 M 0 -106 R D 9541 11989 M 0 -106 R D +10880 11989 M 0 -106 R D 7197 11989 M 0 -53 R D 7532 11989 M 0 -53 R D +7867 11989 M 0 -53 R D 8537 11989 M 0 -53 R D 8871 11989 M 0 -53 R D +9206 11989 M 0 -53 R D 9876 11989 M 0 -53 R D 10211 11989 M 0 -53 R D +10545 11989 M 0 -53 R D 11215 11989 M 0 -53 R D 11550 11989 M 0 -53 R D +11885 11989 M 0 -53 R D 7197 6706 M 0 5283 R D 7197 7201 M 99 0 R D +gsave 7085 7059 translate 0 0 M 1.01 dup scale -117.687 0 N +( ) show grestore 7197 8026 M 99 0 R D gsave 7085 7884 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 8852 M 99 0 R D gsave 7085 8710 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 9678 M 99 0 R D gsave 7085 9535 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 10503 M 99 0 R D gsave 7085 10361 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 11329 M 99 0 R D gsave 7085 11186 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 6706 M 50 0 R D 7197 6871 M 50 0 R D 7197 7036 M +50 0 R D 7197 7366 M 50 0 R D 7197 7531 M 50 0 R D 7197 7696 M 50 0 R D +7197 7861 M 50 0 R D 7197 8192 M 50 0 R D 7197 8357 M 50 0 R D 7197 8522 M +50 0 R D 7197 8687 M 50 0 R D 7197 9017 M 50 0 R D 7197 9182 M 50 0 R D +7197 9347 M 50 0 R D 7197 9512 M 50 0 R D 7197 9843 M 50 0 R D 7197 10008 M +50 0 R D 7197 10173 M 50 0 R D 7197 10338 M 50 0 R D 7197 10668 M 50 0 R D +7197 10833 M 50 0 R D 7197 10998 M 50 0 R D 7197 11163 M 50 0 R D +7197 11494 M 50 0 R D 7197 11659 M 50 0 R D 7197 11824 M 50 0 R D +7197 11989 M 50 0 R D 12152 6706 M 0 5283 R D 12152 7201 M -99 0 R D +12152 8026 M -99 0 R D 12152 8852 M -99 0 R D 12152 9678 M -99 0 R D +12152 10503 M -99 0 R D 12152 11329 M -99 0 R D 12152 6706 M -49 0 R D +12152 6871 M -49 0 R D 12152 7036 M -49 0 R D 12152 7366 M -49 0 R D +12152 7531 M -49 0 R D 12152 7696 M -49 0 R D 12152 7861 M -49 0 R D +12152 8192 M -49 0 R D 12152 8357 M -49 0 R D 12152 8522 M -49 0 R D +12152 8687 M -49 0 R D 12152 9017 M -49 0 R D 12152 9182 M -49 0 R D +12152 9347 M -49 0 R D 12152 9512 M -49 0 R D 12152 9843 M -49 0 R D +12152 10008 M -49 0 R D 12152 10173 M -49 0 R D 12152 10338 M -49 0 R D +12152 10668 M -49 0 R D 12152 10833 M -49 0 R D 12152 10998 M -49 0 R D +12152 11163 M -49 0 R D 12152 11494 M -49 0 R D 12152 11659 M -49 0 R D +12152 11824 M -49 0 R D 12152 11989 M -49 0 R D 9681 8954 M 0 222 R 222 0 R +0 -222 R -222 0 R F +9514 9438 M 0 222 R 222 0 R 0 -222 R -222 0 R F +9346 9359 M 0 222 R 222 0 R 0 -222 R -222 0 R F +9179 9573 M 0 222 R 222 0 R 0 -222 R -222 0 R F +9011 9844 M 0 222 R 222 0 R 0 -222 R -222 0 R F +8844 10107 M 0 222 R 222 0 R 0 -222 R -222 0 R F +8677 10066 M 0 222 R 222 0 R 0 -222 R -222 0 R F +8509 10190 M 0 222 R 222 0 R 0 -222 R -222 0 R F +8342 10330 M 0 222 R 222 0 R 0 -222 R -222 0 R F +8174 10448 M 0 222 R 222 0 R 0 -222 R -222 0 R F +10 setlinewidth 10351 7916 M 0 222 R 222 0 R 0 -222 R -222 0 R D +10183 8147 M 0 222 R 222 0 R 0 -222 R -222 0 R D 10016 8654 M 0 222 R +222 0 R 0 -222 R -222 0 R D 9848 8950 M 0 222 R 222 0 R 0 -222 R -222 0 R D +8007 10321 M 0 222 R 222 0 R 0 -222 R -222 0 R D 7840 10440 M 0 222 R +222 0 R 0 -222 R -222 0 R D 7672 10352 M 0 222 R 222 0 R 0 -222 R -222 0 R D +7505 10592 M 0 222 R 222 0 R 0 -222 R -222 0 R D 20 setlinewidth +10462 6705 M 0 1819 R -25 0 R 49 0 R D 10269 7642 M 50 0 R -25 0 R 0 943 R +-25 0 R 50 0 R D 10102 8474 M 50 0 R -25 0 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13 2 R 12 4 R 12 6 R 11 7 R 10 9 R 8 10 R 7 11 R +6 11 R 4 13 R 3 13 R 1 13 R F +10813 7663 M -1 13 R -3 13 R -4 12 R -6 12 R -7 11 R -9 10 R -9 8 R -11 8 R +-12 6 R -12 4 R -13 2 R -13 1 R -13 -1 R -13 -2 R -12 -4 R -12 -6 R -11 -8 R +-10 -8 R -9 -10 R -7 -11 R -6 -12 R -4 -12 R -2 -13 R -1 -13 R 1 -13 R +2 -13 R 4 -12 R 6 -12 R 7 -11 R 9 -9 R 10 -9 R 11 -7 R 12 -6 R 12 -4 R +13 -3 R 13 -1 R 13 1 R 13 3 R 12 4 R 12 6 R 11 7 R 9 9 R 9 9 R 7 11 R 6 12 R +4 12 R 3 13 R 1 13 R F +8010 9826 M 49 0 R -25 0 R 0 1337 R -24 0 R 49 0 R D 8344 10123 M 50 0 R +-25 0 R 0 99 R -25 0 R 50 0 R D 8679 9991 M 50 0 R -25 0 R 0 66 R -25 0 R +50 0 R D 9014 9925 M 50 0 R -25 0 R 0 66 R -25 0 R 50 0 R D 9349 9661 M +49 0 R -24 0 R 0 66 R -25 0 R 49 0 R D 9684 9347 M 49 0 R -25 0 R 0 66 R +-24 0 R 49 0 R D 10018 8786 M 50 0 R -25 0 R 0 116 R -25 0 R 50 0 R D +10353 8258 M 50 0 R -25 0 R 0 181 R -25 0 R 50 0 R D 10688 7465 M 50 0 R +-25 0 R 0 380 R -25 0 R 50 0 R D 11048 6705 M 0 298 R -25 0 R 49 0 R D +11382 6705 M 0 182 R -24 0 R 49 0 R D 0.000 0.000 0.000 setrgbcolor +7197 10538 M 10 7 R 93 -36 R 92 -38 R 92 -40 R 92 -42 R 92 33 R 92 -48 R +91 -49 R 92 -52 R 91 -54 R 91 7 R 90 -59 R 91 -61 R 91 -63 R 90 -14 R +90 -69 R 90 -70 R 90 -73 R 89 -74 R 90 -36 R 89 -80 R 90 -82 R 89 -83 R +89 -86 R 88 -57 R 89 -90 R 89 -93 R 88 -94 R 89 -73 R 88 -99 R 88 -101 R +88 -103 R 88 -106 R 87 -89 R 88 -110 R 88 -112 R 87 -114 R 87 -103 R +88 -118 R 87 -120 R 87 -122 R 87 -124 R 87 -117 R 87 -129 R 86 -130 R +87 -132 R 87 -134 R 86 -130 R 44 -71 R D 7197 10684 M 10 10 R 93 -19 R +92 -22 R 92 -24 R 92 -26 R 92 60 R 92 -32 R 91 -33 R 92 -36 R 91 -38 R +91 33 R 90 -43 R 91 -45 R 91 -47 R 90 10 R 90 -52 R 90 -55 R 90 -56 R +89 -59 R 90 -13 R 89 -63 R 90 -66 R 89 -68 R 89 -70 R 88 -34 R 89 -75 R +89 -77 R 88 -79 R 89 -51 R 88 -84 R 88 -86 R 88 -88 R 88 -90 R 87 -69 R +88 -95 R 88 -96 R 87 -99 R 87 -83 R 88 -103 R 87 -105 R 87 -107 R 87 -109 R +87 -99 R 87 -113 R 86 -116 R 87 -117 R 87 -119 R 86 -113 R 87 -123 R +86 -125 R 87 -127 R 86 -124 R 86 -131 R 86 -134 R 86 -135 R 75 -119 R D L1 +7197 11404 M 10 -3 R 93 -34 R 92 -8 R 92 -38 R 92 -41 R 92 -43 R 92 -22 R +91 -47 R 92 -49 R 91 -51 R 91 -53 R 90 -39 R 91 -57 R 91 -59 R 90 -61 R +90 -62 R 90 -54 R 90 -67 R 89 -68 R 90 -71 R 89 -64 R 90 -75 R 89 -77 R +89 -78 R 88 -80 R 89 -77 R 89 -84 R 88 -86 R 89 -88 R 88 -86 R 88 -91 R +88 -94 R 88 -95 R 87 -97 R 88 -97 R 88 -101 R 87 -102 R 87 -105 R 88 -106 R +87 -107 R 87 -110 R 87 -112 R 87 -114 R 87 -115 R 86 -117 R 87 -120 R +87 -121 R 86 -123 R 87 -125 R 86 -126 R 87 -129 R 86 -131 R 86 -132 R +86 -134 R 86 -137 R 85 -136 R D 7197 9512 M 10 0 R 93 -7 R 92 189 R 92 -13 R +92 -15 R 92 -17 R 92 -20 R 91 150 R 92 -25 R 91 -27 R 91 -30 R 90 117 R +91 -35 R 91 -38 R 90 -40 R 90 -41 R 90 82 R 90 -47 R 89 -50 R 90 -52 R +89 54 R 90 -58 R 89 -59 R 89 -62 R 88 -64 R 89 24 R 89 -70 R 88 -71 R +89 -74 R 88 -76 R 88 -4 R 88 -81 R 88 -84 R 87 -85 R 88 -28 R 88 -90 R +87 -93 R 87 -94 R 88 -97 R 87 -52 R 87 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0 -53 R D +12822 11989 M 0 -53 R D 13492 11989 M 0 -53 R D 13826 11989 M 0 -53 R D +14161 11989 M 0 -53 R D 14831 11989 M 0 -53 R D 15166 11989 M 0 -53 R D +15500 11989 M 0 -53 R D 16170 11989 M 0 -53 R D 16505 11989 M 0 -53 R D +16840 11989 M 0 -53 R D 12152 6706 M 0 5283 R D 12152 7201 M 99 0 R D +gsave 12040 7059 translate 0 0 M 1.01 dup scale -117.687 0 N +( ) show grestore 12152 8026 M 99 0 R D gsave 12040 7884 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 8852 M 99 0 R D gsave 12040 8710 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 9678 M 99 0 R D gsave 12040 9535 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 10503 M 99 0 R D gsave 12040 10361 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 11329 M 99 0 R D gsave 12040 11186 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 6706 M 50 0 R D 12152 6871 M 50 0 R D 12152 7036 M +50 0 R D 12152 7366 M 50 0 R D 12152 7531 M 50 0 R D 12152 7696 M 50 0 R D +12152 7861 M 50 0 R D 12152 8192 M 50 0 R D 12152 8357 M 50 0 R D +12152 8522 M 50 0 R D 12152 8687 M 50 0 R D 12152 9017 M 50 0 R D +12152 9182 M 50 0 R D 12152 9347 M 50 0 R D 12152 9512 M 50 0 R D +12152 9843 M 50 0 R D 12152 10008 M 50 0 R D 12152 10173 M 50 0 R D +12152 10338 M 50 0 R D 12152 10668 M 50 0 R D 12152 10833 M 50 0 R D +12152 10998 M 50 0 R D 12152 11163 M 50 0 R D 12152 11494 M 50 0 R D +12152 11659 M 50 0 R D 12152 11824 M 50 0 R D 12152 11989 M 50 0 R D +17107 6706 M 0 5283 R D 17107 7201 M -99 0 R D 17107 8026 M -99 0 R D +17107 8852 M -99 0 R D 17107 9678 M -99 0 R D 17107 10503 M -99 0 R D +17107 11329 M -99 0 R D 17107 6706 M -49 0 R D 17107 6871 M -49 0 R D +17107 7036 M -49 0 R D 17107 7366 M -49 0 R D 17107 7531 M -49 0 R D +17107 7696 M -49 0 R D 17107 7861 M -49 0 R D 17107 8192 M -49 0 R D +17107 8357 M -49 0 R D 17107 8522 M -49 0 R D 17107 8687 M -49 0 R D +17107 9017 M -49 0 R D 17107 9182 M -49 0 R D 17107 9347 M -49 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10567 M 0 222 R +222 0 R 0 -222 R -222 0 R D 13297 10235 M 0 222 R 222 0 R 0 -222 R -222 0 R +D 13129 10639 M 0 222 R 222 0 R 0 -222 R -222 0 R D 12962 10995 M 0 222 R +222 0 R 0 -222 R -222 0 R D 20 setlinewidth 15727 7355 M 49 0 R -25 0 R +0 946 R -24 0 R 49 0 R D 15559 8423 M 50 0 R -25 0 R 0 426 R -25 0 R 50 0 R +D 15392 8656 M 49 0 R -24 0 R 0 354 R -25 0 R 49 0 R D 15225 8729 M 49 0 R +-25 0 R 0 345 R -24 0 R 49 0 R D 15057 9005 M 50 0 R -25 0 R 0 298 R -25 0 R +50 0 R D 14890 9492 M 49 0 R -25 0 R 0 227 R -24 0 R 49 0 R D 14722 9435 M +50 0 R -25 0 R 0 250 R -25 0 R 50 0 R D 14555 9732 M 49 0 R -24 0 R 0 217 R +-25 0 R 49 0 R D 14388 10011 M 49 0 R -25 0 R 0 192 R -24 0 R 49 0 R D +14220 10090 M 50 0 R -25 0 R 0 180 R -25 0 R 50 0 R D 14053 10170 M 49 0 R +-25 0 R 0 167 R -24 0 R 49 0 R D 13885 10365 M 50 0 R -25 0 R 0 145 R +-25 0 R 50 0 R D 13718 10404 M 49 0 R -24 0 R 0 147 R -25 0 R 49 0 R D +13551 10604 M 49 0 R -25 0 R 0 141 R -24 0 R 49 0 R D 13383 10222 M 50 0 R +-25 0 R 0 230 R -25 0 R 50 0 R D 13216 10602 M 49 0 R -25 0 R 0 270 R +-24 0 R 49 0 R D 13048 10488 M 50 0 R -25 0 R 0 945 R -25 0 R 50 0 R D +0.082 1.000 0.000 setrgbcolor 13759 10206 M -1 13 R -3 13 R -4 12 R -5 12 R +-8 11 R -8 10 R -10 8 R -11 7 R -12 6 R -12 4 R -13 3 R -13 1 R -13 -1 R +-13 -3 R -12 -4 R -12 -6 R -11 -7 R -10 -8 R -8 -10 R -8 -11 R -5 -12 R +-5 -12 R -2 -13 R -1 -13 R 1 -13 R 2 -13 R 5 -12 R 5 -12 R 8 -11 R 8 -10 R +10 -8 R 11 -8 R 12 -5 R 12 -5 R 13 -2 R 13 -1 R 13 1 R 13 2 R 12 5 R 12 5 R +11 8 R 10 8 R 8 10 R 8 11 R 5 12 R 4 12 R 3 13 R 1 13 R F +14094 9991 M -1 13 R -3 13 R -4 12 R -6 12 R -7 11 R -9 10 R -9 8 R -11 8 R +-12 6 R -12 4 R -13 2 R -13 1 R -13 -1 R -13 -2 R -12 -4 R -12 -6 R -11 -8 R +-10 -8 R -8 -10 R -8 -11 R -6 -12 R -4 -12 R -2 -13 R -1 -13 R 1 -13 R +2 -13 R 4 -12 R 6 -12 R 8 -11 R 8 -9 R 10 -9 R 11 -7 R 12 -6 R 12 -4 R +13 -3 R 13 -1 R 13 1 R 13 3 R 12 4 R 12 6 R 11 7 R 9 9 R 9 9 R 7 11 R 6 12 R +4 12 R 3 13 R 1 13 R F +14428 9909 M 0 13 R -3 13 R 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M 0 13 R -3 13 R -4 12 R -6 12 R -7 10 R -9 10 R -10 9 R -10 7 R +-12 6 R -13 4 R -12 3 R -13 1 R -13 -1 R -13 -3 R -13 -4 R -11 -6 R -11 -7 R +-10 -9 R -9 -10 R -7 -10 R -6 -12 R -4 -12 R -2 -13 R -1 -13 R 1 -13 R +2 -13 R 4 -13 R 6 -11 R 7 -11 R 9 -10 R 10 -9 R 11 -7 R 11 -6 R 13 -4 R +13 -2 R 13 -1 R 13 1 R 12 2 R 13 4 R 12 6 R 10 7 R 10 9 R 9 10 R 7 11 R +6 11 R 4 13 R 3 13 R 0 13 R F +16437 7052 M -1 13 R -2 13 R -4 13 R -6 11 R -7 11 R -9 10 R -10 9 R -11 7 R +-11 6 R -13 4 R -13 2 R -13 1 R -13 -1 R -12 -2 R -13 -4 R -12 -6 R -10 -7 R +-10 -9 R -9 -10 R -7 -11 R -6 -11 R -4 -13 R -3 -13 R -1 -13 R 1 -13 R +3 -13 R 4 -12 R 6 -12 R 7 -11 R 9 -9 R 10 -9 R 10 -7 R 12 -6 R 13 -4 R +12 -3 R 13 -1 R 13 1 R 13 3 R 13 4 R 11 6 R 11 7 R 10 9 R 9 9 R 7 11 R +6 12 R 4 12 R 2 13 R 1 13 R F +13634 10008 M 50 0 R -25 0 R 0 379 R -25 0 R 50 0 R D 13969 9958 M 50 0 R +-25 0 R 0 66 R -25 0 R 50 0 R D 14304 9876 M 49 0 R -24 0 R 0 49 R -25 0 R +49 0 R D 14639 9744 M 49 0 R -25 0 R 0 66 R -24 0 R 49 0 R D 14973 9347 M +50 0 R -25 0 R 0 66 R -25 0 R 50 0 R D 15308 8819 M 50 0 R -25 0 R 0 99 R +-25 0 R 50 0 R D 15643 8159 M 50 0 R -25 0 R 0 165 R -25 0 R 50 0 R D +15978 7449 M 49 0 R -24 0 R 0 297 R -25 0 R 49 0 R D 16313 6788 M 49 0 R +-25 0 R 0 512 R -24 0 R 49 0 R D 0.000 0.000 0.000 setrgbcolor 12152 10628 M +10 8 R 93 -28 R 92 -30 R 92 -32 R 92 -34 R 92 46 R 92 -40 R 91 -41 R +92 -44 R 91 -46 R 91 20 R 91 -51 R 90 -53 R 91 -55 R 90 -2 R 90 -60 R +90 -63 R 90 -65 R 89 -66 R 90 -25 R 89 -71 R 90 -74 R 89 -76 R 89 -78 R +89 -45 R 88 -83 R 89 -85 R 88 -87 R 89 -62 R 88 -91 R 88 -94 R 88 -95 R +88 -98 R 87 -80 R 88 -102 R 88 -104 R 87 -106 R 87 -93 R 88 -111 R 87 -112 R +87 -115 R 87 -116 R 87 -109 R 87 -120 R 86 -123 R 87 -125 R 87 -126 R +86 -122 R 87 -131 R 86 -133 R 87 -134 R 86 -132 R 17 -29 R D 12152 10711 M +10 11 R 93 -12 R 92 -13 R 92 -16 R 92 -18 R 92 73 R 92 -23 R 91 -26 R +92 -27 R 91 -30 R 91 46 R 91 -35 R 90 -37 R 91 -40 R 90 24 R 90 -44 R +90 -47 R 90 -49 R 89 -51 R 90 0 R 89 -56 R 90 -58 R 89 -60 R 89 -62 R +89 -22 R 88 -68 R 89 -69 R 88 -71 R 89 -40 R 88 -76 R 88 -78 R 88 -80 R +88 -82 R 87 -59 R 88 -87 R 88 -89 R 87 -91 R 87 -73 R 88 -96 R 87 -97 R +87 -100 R 87 -101 R 87 -89 R 87 -106 R 86 -108 R 87 -109 R 87 -112 R +86 -104 R 87 -116 R 86 -117 R 87 -120 R 86 -115 R 86 -124 R 86 -126 R +87 -128 R 86 -129 R 67 -100 R D L1 12152 11489 M 10 -2 R 93 -27 R 92 3 R +92 -31 R 92 -34 R 92 -35 R 92 -12 R 91 -40 R 92 -41 R 91 -44 R 91 -45 R +91 -29 R 90 -50 R 91 -52 R 90 -53 R 90 -56 R 90 -44 R 90 -60 R 89 -61 R +90 -64 R 89 -55 R 90 -68 R 89 -69 R 89 -72 R 89 -73 R 88 -68 R 89 -77 R +88 -79 R 89 -81 R 88 -78 R 88 -85 R 88 -86 R 88 -88 R 87 -90 R 88 -89 R +88 -94 R 87 -96 R 87 -97 R 88 -100 R 87 -99 R 87 -103 R 87 -105 R 87 -107 R +87 -107 R 86 -111 R 87 -112 R 87 -114 R 86 -116 R 87 -117 R 86 -120 R +87 -121 R 86 -124 R 86 -125 R 86 -127 R 87 -129 R 86 -131 R 67 -103 R D +12152 9488 M 10 1 R 93 1 R 92 205 R 92 -5 R 92 -7 R 92 -9 R 92 -11 R +91 165 R 92 -17 R 91 -19 R 91 -21 R 91 131 R 90 -27 R 91 -29 R 90 -32 R +90 -33 R 90 96 R 90 -39 R 89 -41 R 90 -44 R 89 68 R 90 -50 R 89 -51 R +89 -54 R 89 -55 R 88 37 R 89 -62 R 88 -63 R 89 -65 R 88 -68 R 88 8 R +88 -73 R 88 -75 R 87 -77 R 88 -15 R 88 -83 R 87 -84 R 87 -87 R 88 -89 R +87 -40 R 87 -93 R 87 -96 R 87 -98 R 87 -100 R 86 -63 R 87 -105 R 87 -107 R +86 -109 R 87 -81 R 86 -114 R 87 -116 R 86 -118 R 86 -120 R 86 -100 R +87 -125 R 86 -126 R 67 -101 R D gsave 12487 7036 translate 0 0 M +1.1 dup scale +(z = 0.8 - 1.42) show grestore 15 setlinewidth L0 2242 1422 M 4955 0 R D +3247 1422 M 0 106 R D gsave 3247 889 translate 0 0 M 1.01 dup scale +-305.858 0 N +(-22) show grestore 4586 1422 M 0 106 R D gsave 4586 889 translate 0 0 M +1.01 dup scale -305.858 0 N +(-24) show grestore 5925 1422 M 0 106 R D gsave 5925 889 translate 0 0 M +1.01 dup scale -305.858 0 N +(-26) show grestore 2242 1422 M 0 53 R D 2577 1422 M 0 53 R D 2912 1422 M +0 53 R D 3581 1422 M 0 53 R D 3916 1422 M 0 53 R D 4251 1422 M 0 53 R D +4921 1422 M 0 53 R D 5255 1422 M 0 53 R D 5590 1422 M 0 53 R D 6260 1422 M +0 53 R D 6595 1422 M 0 53 R D 6929 1422 M 0 53 R D 2242 6706 M 4955 0 R D +3247 6706 M 0 -106 R D 4586 6706 M 0 -106 R D 5925 6706 M 0 -106 R D +2242 6706 M 0 -53 R D 2577 6706 M 0 -53 R D 2912 6706 M 0 -53 R D +3581 6706 M 0 -53 R D 3916 6706 M 0 -53 R D 4251 6706 M 0 -53 R D +4921 6706 M 0 -53 R D 5255 6706 M 0 -53 R D 5590 6706 M 0 -53 R D +6260 6706 M 0 -53 R D 6595 6706 M 0 -53 R D 6929 6706 M 0 -53 R D +2242 1422 M 0 5284 R D 2242 1917 M 99 0 R D gsave 2130 1775 translate 0 0 M +1.01 dup scale -729.403 0 N +(-7.5) show grestore 2242 2743 M 99 0 R D gsave 2130 2601 translate 0 0 M +1.01 dup scale -729.403 0 N +(-7.0) show grestore 2242 3569 M 99 0 R D gsave 2130 3426 translate 0 0 M +1.01 dup scale -729.403 0 N +(-6.5) show grestore 2242 4394 M 99 0 R D gsave 2130 4252 translate 0 0 M +1.01 dup scale -729.403 0 N +(-6.0) show grestore 2242 5220 M 99 0 R D gsave 2130 5077 translate 0 0 M +1.01 dup scale -729.403 0 N +(-5.5) show grestore 2242 6045 M 99 0 R D gsave 2130 5903 translate 0 0 M +1.01 dup scale -729.403 0 N +(-5.0) show grestore 2242 1422 M 50 0 R D 2242 1587 M 50 0 R D 2242 1752 M +50 0 R D 2242 2083 M 50 0 R D 2242 2248 M 50 0 R D 2242 2413 M 50 0 R D +2242 2578 M 50 0 R D 2242 2908 M 50 0 R D 2242 3073 M 50 0 R D 2242 3238 M +50 0 R D 2242 3403 M 50 0 R D 2242 3734 M 50 0 R D 2242 3899 M 50 0 R D +2242 4064 M 50 0 R D 2242 4229 M 50 0 R D 2242 4559 M 50 0 R D 2242 4724 M +50 0 R D 2242 4889 M 50 0 R D 2242 5055 M 50 0 R D 2242 5385 M 50 0 R D +2242 5550 M 50 0 R D 2242 5715 M 50 0 R D 2242 5880 M 50 0 R D 2242 6210 M +50 0 R D 2242 6375 M 50 0 R D 2242 6540 M 50 0 R D 2242 6706 M 50 0 R D +7197 1422 M 0 5284 R D 7197 1917 M -99 0 R D 7197 2743 M -99 0 R D +7197 3569 M -99 0 R D 7197 4394 M -99 0 R D 7197 5220 M -99 0 R D +7197 6045 M -99 0 R D 7197 1422 M -49 0 R D 7197 1587 M -49 0 R D +7197 1752 M -49 0 R D 7197 2083 M -49 0 R D 7197 2248 M -49 0 R D +7197 2413 M -49 0 R D 7197 2578 M -49 0 R D 7197 2908 M -49 0 R D +7197 3073 M -49 0 R D 7197 3238 M -49 0 R D 7197 3403 M -49 0 R D +7197 3734 M -49 0 R D 7197 3899 M -49 0 R D 7197 4064 M -49 0 R D +7197 4229 M -49 0 R D 7197 4559 M -49 0 R D 7197 4724 M -49 0 R D +7197 4889 M -49 0 R D 7197 5055 M -49 0 R D 7197 5385 M -49 0 R D +7197 5550 M -49 0 R D 7197 5715 M -49 0 R D 7197 5880 M -49 0 R D +7197 6210 M -49 0 R D 7197 6375 M -49 0 R D 7197 6540 M -49 0 R D +7197 6706 M -49 0 R D 5730 3466 M 0 222 R 222 0 R 0 -222 R -222 0 R F +5563 3415 M 0 222 R 222 0 R 0 -222 R -222 0 R F +5396 3743 M 0 222 R 222 0 R 0 -222 R -222 0 R F +5228 4166 M 0 222 R 222 0 R 0 -222 R -222 0 R F +5061 4288 M 0 222 R 222 0 R 0 -222 R -222 0 R F +4893 4398 M 0 222 R 222 0 R 0 -222 R -222 0 R F +4726 4614 M 0 222 R 222 0 R 0 -222 R -222 0 R F +4559 4811 M 0 222 R 222 0 R 0 -222 R -222 0 R F +4391 4830 M 0 222 R 222 0 R 0 -222 R -222 0 R F +4224 4897 M 0 222 R 222 0 R 0 -222 R -222 0 R F +4056 5151 M 0 222 R 222 0 R 0 -222 R -222 0 R F +10 setlinewidth 6065 2691 M 0 222 R 222 0 R 0 -222 R -222 0 R D 5898 2876 M +0 222 R 222 0 R 0 -222 R -222 0 R D 3889 5117 M 0 222 R 222 0 R 0 -222 R +-222 0 R D 3722 5031 M 0 222 R 222 0 R 0 -222 R -222 0 R D 3554 4872 M +0 222 R 222 0 R 0 -222 R -222 0 R D 20 setlinewidth 6151 2377 M 50 0 R +-25 0 R 0 690 R -25 0 R 50 0 R D 5984 2697 M 50 0 R -25 0 R 0 496 R -25 0 R +50 0 R D 5817 3396 M 49 0 R -25 0 R 0 326 R -24 0 R 49 0 R D 5649 3333 M +50 0 R -25 0 R 0 345 R -25 0 R 50 0 R D 5482 3697 M 49 0 R -24 0 R 0 286 R +-25 0 R 49 0 R D 5314 4158 M 50 0 R -25 0 R 0 221 R -25 0 R 50 0 R D +5147 4283 M 50 0 R -25 0 R 0 216 R -25 0 R 50 0 R D 4980 4397 M 49 0 R +-25 0 R 0 209 R -24 0 R 49 0 R D 4812 4623 M 50 0 R -25 0 R 0 192 R -25 0 R +50 0 R D 4645 4835 M 49 0 R -24 0 R 0 165 R -25 0 R 49 0 R D 4477 4859 M +50 0 R -25 0 R 0 155 R -25 0 R 50 0 R D 4310 4931 M 50 0 R -25 0 R 0 147 R +-25 0 R 50 0 R D 4143 5191 M 49 0 R -25 0 R 0 136 R -24 0 R 49 0 R D +3975 5149 M 50 0 R -25 0 R 0 150 R -25 0 R 50 0 R D 3808 5034 M 49 0 R +-24 0 R 0 203 R -25 0 R 49 0 R D 3640 4670 M 50 0 R -25 0 R 0 531 R -25 0 R +50 0 R D 0.082 1.000 0.000 setrgbcolor 4518 4724 M 0 13 R -3 13 R -4 13 R +-6 11 R -7 11 R -9 10 R -10 9 R -11 7 R -11 6 R -13 4 R -12 2 R -14 1 R +-13 -1 R -12 -2 R -13 -4 R -11 -6 R -11 -7 R -10 -9 R -9 -10 R -7 -11 R +-6 -11 R -4 -13 R -3 -13 R 0 -13 R 0 -13 R 3 -13 R 4 -12 R 6 -12 R 7 -11 R +9 -9 R 10 -9 R 11 -7 R 11 -6 R 13 -4 R 12 -3 R 13 -1 R 14 1 R 12 3 R 13 4 R +11 6 R 11 7 R 10 9 R 9 9 R 7 11 R 6 12 R 4 12 R 3 13 R 0 13 R F +4853 4708 M -1 13 R -2 13 R -4 12 R -6 12 R -7 11 R -9 9 R -10 9 R -11 7 R +-11 6 R -13 4 R -13 3 R -13 1 R -13 -1 R -13 -3 R -12 -4 R -12 -6 R -11 -7 R +-9 -9 R -9 -9 R -7 -11 R -6 -12 R -4 -12 R -3 -13 R -1 -13 R 1 -13 R 3 -13 R +4 -12 R 6 -12 R 7 -11 R 9 -10 R 9 -8 R 11 -8 R 12 -6 R 12 -4 R 13 -2 R +13 -1 R 13 1 R 13 2 R 13 4 R 11 6 R 11 8 R 10 8 R 9 10 R 7 11 R 6 12 R +4 12 R 2 13 R 1 13 R F +5188 4510 M -1 13 R -2 13 R -5 12 R -5 12 R -8 10 R -8 10 R -10 9 R -11 7 R +-12 6 R -12 4 R -13 3 R -13 1 R -13 -1 R -13 -3 R -12 -4 R -12 -6 R -11 -7 R +-10 -9 R -8 -10 R -7 -10 R -6 -12 R -4 -12 R -3 -13 R -1 -13 R 1 -13 R +3 -13 R 4 -13 R 6 -11 R 7 -11 R 8 -10 R 10 -9 R 11 -7 R 12 -6 R 12 -4 R +13 -2 R 13 -1 R 13 1 R 13 2 R 12 4 R 12 6 R 11 7 R 10 9 R 8 10 R 8 11 R +5 11 R 5 13 R 2 13 R 1 13 R F +5523 4064 M -1 13 R -3 13 R -4 12 R -6 12 R -7 11 R -8 10 R -10 8 R -11 7 R +-12 6 R -12 4 R -13 3 R -13 1 R -13 -1 R -13 -3 R -12 -4 R -12 -6 R -11 -7 R +-10 -8 R -8 -10 R -8 -11 R -5 -12 R -5 -12 R -2 -13 R -1 -13 R 1 -13 R +2 -13 R 5 -12 R 5 -12 R 8 -11 R 8 -10 R 10 -8 R 11 -8 R 12 -5 R 12 -5 R +13 -2 R 13 -1 R 13 1 R 13 2 R 12 5 R 12 5 R 11 8 R 10 8 R 8 10 R 7 11 R +6 12 R 4 12 R 3 13 R 1 13 R F +5858 3486 M -1 13 R -3 13 R -4 12 R -6 12 R -7 11 R -9 10 R -9 8 R -11 8 R +-12 5 R -12 4 R -13 3 R -13 1 R -13 -1 R -13 -3 R -13 -4 R -11 -5 R -11 -8 R +-10 -8 R -9 -10 R -7 -11 R -6 -12 R -4 -12 R -2 -13 R -1 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4691 M 49 0 R -25 0 R 0 66 R -24 0 R 49 0 R D 4729 4691 M 49 0 R +-25 0 R 0 33 R -24 0 R 49 0 R D 5063 4493 M 50 0 R -25 0 R 0 33 R -25 0 R +50 0 R D 5398 4031 M 50 0 R -25 0 R 0 66 R -25 0 R 50 0 R D 5733 3436 M +49 0 R -24 0 R 0 100 R -25 0 R 49 0 R D 6068 2842 M 49 0 R -25 0 R 0 149 R +-24 0 R 49 0 R D 6403 2083 M 49 0 R -25 0 R 0 297 R -24 0 R 49 0 R D +0.000 0.000 0.000 setrgbcolor 2242 5416 M 10 11 R 92 -16 R 93 -19 R 92 -20 R +92 -22 R 92 65 R 92 -28 R 91 -30 R 92 -32 R 91 -34 R 91 38 R 90 -40 R +91 -41 R 90 -44 R 91 16 R 90 -49 R 90 -51 R 90 -53 R 89 -56 R 90 -7 R +89 -60 R 90 -63 R 89 -64 R 89 -67 R 88 -29 R 89 -72 R 89 -73 R 88 -76 R +88 -46 R 89 -81 R 88 -82 R 88 -85 R 88 -86 R 87 -65 R 88 -91 R 88 -94 R +87 -95 R 87 -79 R 88 -100 R 87 -101 R 87 -104 R 87 -106 R 87 -95 R 87 -110 R +86 -111 R 87 -114 R 87 -116 R 86 -109 R 87 -120 R 86 -122 R 87 -124 R +86 -120 R 86 -128 R 86 -130 R 86 -132 R 87 -134 R 67 -103 R D 2242 5428 M +10 12 R 92 -9 R 93 -10 R 92 -13 R 92 -15 R 92 78 R 92 -21 R 91 -23 R +92 -24 R 91 -27 R 91 50 R 90 -32 R 91 -35 R 90 -36 R 91 28 R 90 -42 R +90 -44 R 90 -46 R 89 -48 R 90 4 R 89 -53 R 90 -55 R 89 -58 R 89 -59 R +88 -18 R 89 -65 R 89 -66 R 88 -69 R 88 -36 R 89 -73 R 88 -76 R 88 -77 R +88 -80 R 87 -55 R 88 -84 R 88 -86 R 87 -88 R 87 -71 R 88 -92 R 87 -95 R +87 -97 R 87 -99 R 87 -86 R 87 -103 R 86 -105 R 87 -107 R 87 -109 R 86 -101 R +87 -113 R 86 -115 R 87 -117 R 86 -112 R 86 -122 R 86 -123 R 86 -125 R +87 -127 R 67 -98 R D L1 2242 6228 M 10 -2 R 92 -24 R 93 7 R 92 -29 R +92 -31 R 92 -32 R 92 -9 R 91 -37 R 92 -39 R 91 -41 R 91 -43 R 90 -26 R +91 -47 R 90 -49 R 91 -52 R 90 -53 R 90 -40 R 90 -58 R 89 -59 R 90 -61 R +89 -52 R 90 -65 R 89 -68 R 89 -68 R 88 -71 R 89 -65 R 89 -75 R 88 -77 R +88 -78 R 89 -75 R 88 -82 R 88 -84 R 88 -86 R 87 -88 R 88 -86 R 88 -92 R +87 -93 R 87 -95 R 88 -97 R 87 -97 R 87 -100 R 87 -103 R 87 -104 R 87 -105 R +86 -108 R 87 -110 R 87 -112 R 86 -113 R 87 -115 R 86 -117 R 87 -119 R +86 -121 R 86 -123 R 86 -124 R 86 -127 R 87 -128 R 67 -102 R D 2242 4189 M +10 1 R 92 4 R 93 210 R 92 -2 R 92 -4 R 92 -6 R 92 -8 R 91 170 R 92 -14 R +91 -17 R 91 -18 R 90 137 R 91 -25 R 90 -26 R 91 -29 R 90 -30 R 90 101 R +90 -36 R 89 -39 R 90 -41 R 89 73 R 90 -47 R 89 -48 R 89 -51 R 88 -53 R +89 42 R 89 -59 R 88 -60 R 88 -63 R 89 -65 R 88 13 R 88 -70 R 88 -73 R +87 -74 R 88 -11 R 88 -80 R 87 -81 R 87 -84 R 88 -86 R 87 -36 R 87 -91 R +87 -93 R 87 -96 R 87 -97 R 86 -59 R 87 -102 R 87 -104 R 86 -107 R 87 -77 R +86 -111 R 87 -113 R 86 -116 R 86 -117 R 86 -96 R 86 -122 R 87 -124 R +67 -99 R D gsave 2577 1752 translate 0 0 M 1.1 dup scale +(z = 1.2 - 1.58) show grestore gsave 836 6706 translate 0 0 M 90 rotate +1.01 dup scale -2734.43 0 N +(Log\( d) show +%%IncludeResource: font Symbol +423.333 /Symbol STDFONT +(F) show +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( / dM) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(g) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( \) [Mpc) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(-3) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( mag) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(-1) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(]) show grestore 15 setlinewidth L0 7197 1422 M 4955 0 R D 8202 1422 M +0 106 R D gsave 8202 889 translate 0 0 M 1.01 dup scale -305.858 0 N +(-22) show grestore 9541 1422 M 0 106 R D gsave 9541 889 translate 0 0 M +1.01 dup scale -305.858 0 N +(-24) show grestore 10880 1422 M 0 106 R D gsave 10880 889 translate 0 0 M +1.01 dup scale -305.858 0 N +(-26) show grestore 7197 1422 M 0 53 R D 7532 1422 M 0 53 R D 7867 1422 M +0 53 R D 8537 1422 M 0 53 R D 8871 1422 M 0 53 R D 9206 1422 M 0 53 R D +9876 1422 M 0 53 R D 10211 1422 M 0 53 R D 10545 1422 M 0 53 R D +11215 1422 M 0 53 R D 11550 1422 M 0 53 R D 11885 1422 M 0 53 R D +7197 6706 M 4955 0 R D 8202 6706 M 0 -106 R D 9541 6706 M 0 -106 R D +10880 6706 M 0 -106 R D 7197 6706 M 0 -53 R D 7532 6706 M 0 -53 R D +7867 6706 M 0 -53 R D 8537 6706 M 0 -53 R D 8871 6706 M 0 -53 R D +9206 6706 M 0 -53 R D 9876 6706 M 0 -53 R D 10211 6706 M 0 -53 R D +10545 6706 M 0 -53 R D 11215 6706 M 0 -53 R D 11550 6706 M 0 -53 R D +11885 6706 M 0 -53 R D 7197 1422 M 0 5284 R D 7197 1917 M 99 0 R D +gsave 7085 1775 translate 0 0 M 1.01 dup scale -117.687 0 N +( ) show grestore 7197 2743 M 99 0 R D gsave 7085 2601 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 3569 M 99 0 R D gsave 7085 3426 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 4394 M 99 0 R D gsave 7085 4252 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 5220 M 99 0 R D gsave 7085 5077 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 6045 M 99 0 R D gsave 7085 5903 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 1422 M 50 0 R D 7197 1587 M 50 0 R D 7197 1752 M +50 0 R D 7197 2083 M 50 0 R D 7197 2248 M 50 0 R D 7197 2413 M 50 0 R D +7197 2578 M 50 0 R D 7197 2908 M 50 0 R D 7197 3073 M 50 0 R D 7197 3238 M +50 0 R D 7197 3403 M 50 0 R D 7197 3734 M 50 0 R D 7197 3899 M 50 0 R D +7197 4064 M 50 0 R D 7197 4229 M 50 0 R D 7197 4559 M 50 0 R D 7197 4724 M +50 0 R D 7197 4889 M 50 0 R D 7197 5055 M 50 0 R D 7197 5385 M 50 0 R D +7197 5550 M 50 0 R D 7197 5715 M 50 0 R D 7197 5880 M 50 0 R D 7197 6210 M +50 0 R D 7197 6375 M 50 0 R D 7197 6540 M 50 0 R D 7197 6706 M 50 0 R D +12152 1422 M 0 5284 R D 12152 1917 M -99 0 R D 12152 2743 M -99 0 R D +12152 3569 M -99 0 R D 12152 4394 M -99 0 R D 12152 5220 M -99 0 R D +12152 6045 M -99 0 R D 12152 1422 M -49 0 R D 12152 1587 M -49 0 R D +12152 1752 M -49 0 R D 12152 2083 M -49 0 R D 12152 2248 M -49 0 R D +12152 2413 M -49 0 R D 12152 2578 M -49 0 R D 12152 2908 M -49 0 R D +12152 3073 M -49 0 R D 12152 3238 M -49 0 R D 12152 3403 M -49 0 R D 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222 R 222 0 R 0 -222 R -222 0 R D +11355 2654 M 0 222 R 222 0 R 0 -222 R -222 0 R D 11188 2412 M 0 222 R +222 0 R 0 -222 R -222 0 R D 9011 5152 M 0 222 R 222 0 R 0 -222 R -222 0 R D +8844 5208 M 0 222 R 222 0 R 0 -222 R -222 0 R D 20 setlinewidth 11633 1422 M +0 2595 R -24 0 R 49 0 R D 11441 2267 M 50 0 R -25 0 R 0 789 R -25 0 R 50 0 R +D 11274 2098 M 49 0 R -24 0 R 0 690 R -25 0 R 49 0 R D 11106 2966 M 50 0 R +-25 0 R 0 408 R -25 0 R 50 0 R D 10939 3463 M 50 0 R -25 0 R 0 303 R -25 0 R +50 0 R D 10772 3818 M 49 0 R -25 0 R 0 249 R -24 0 R 49 0 R D 10604 4087 M +50 0 R -25 0 R 0 218 R -25 0 R 50 0 R D 10437 4335 M 49 0 R -24 0 R 0 199 R +-25 0 R 49 0 R D 10269 4439 M 50 0 R -25 0 R 0 193 R -25 0 R 50 0 R D +10102 4528 M 50 0 R -25 0 R 0 191 R -25 0 R 50 0 R D 9935 4608 M 49 0 R +-25 0 R 0 187 R -24 0 R 49 0 R D 9767 4805 M 50 0 R -25 0 R 0 156 R -25 0 R +50 0 R D 9600 5056 M 49 0 R -24 0 R 0 129 R -25 0 R 49 0 R D 9432 4986 M +50 0 R -25 0 R 0 141 R -25 0 R 50 0 R D 9265 5252 M 50 0 R 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R -5 12 R -5 12 R -8 11 R -8 9 R -10 9 R -11 7 R +-12 6 R -12 4 R -13 3 R -13 1 R -13 -1 R -13 -3 R -12 -4 R -12 -6 R -11 -7 R +-9 -9 R -9 -9 R -7 -11 R -6 -12 R -4 -12 R -3 -13 R -1 -13 R 1 -13 R 3 -13 R +4 -12 R 6 -12 R 7 -11 R 9 -10 R 9 -9 R 11 -7 R 12 -6 R 12 -4 R 13 -2 R +13 -1 R 13 1 R 13 2 R 12 4 R 12 6 R 11 7 R 10 9 R 8 10 R 8 11 R 5 12 R +5 12 R 2 13 R 1 13 R F +10478 4361 M -1 13 R -3 13 R -4 12 R -6 12 R -7 11 R -8 10 R -10 8 R -11 8 R +-12 5 R -12 5 R -13 2 R -13 1 R -13 -1 R -13 -2 R -12 -5 R -12 -5 R -11 -8 R +-10 -8 R -8 -10 R -8 -11 R -5 -12 R -5 -12 R -2 -13 R -1 -13 R 1 -13 R +2 -13 R 5 -12 R 5 -12 R 8 -11 R 8 -10 R 10 -8 R 11 -7 R 12 -6 R 12 -4 R +13 -3 R 13 -1 R 13 1 R 13 3 R 12 4 R 12 6 R 11 7 R 10 8 R 8 10 R 7 11 R +6 12 R 4 12 R 3 13 R 1 13 R F +10813 3948 M -1 13 R -3 13 R -4 13 R -6 11 R -7 11 R -9 10 R -9 9 R -11 7 R +-12 6 R -12 4 R -13 2 R -13 1 R -13 -1 R -13 -2 R -12 -4 R -12 -6 R -11 -7 R +-10 -9 R -9 -10 R -7 -11 R -6 -11 R -4 -13 R -2 -13 R -1 -13 R 1 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-1 14 R -2 12 R -5 13 R -5 11 R -8 11 R -8 10 R -10 9 R -11 7 R +-12 6 R -12 4 R -13 3 R -13 0 R -13 0 R -13 -3 R -12 -4 R -12 -6 R -11 -7 R +-9 -9 R -9 -10 R -7 -11 R -6 -11 R -4 -13 R -3 -12 R -1 -14 R 1 -13 R +3 -12 R 4 -13 R 6 -11 R 7 -11 R 9 -10 R 9 -9 R 11 -7 R 12 -6 R 12 -4 R +13 -3 R 13 0 R 13 0 R 13 3 R 12 4 R 12 6 R 11 7 R 10 9 R 8 10 R 8 11 R +5 11 R 5 13 R 2 12 R 1 13 R F +9349 4328 M 49 0 R -24 0 R 0 1040 R -25 0 R 49 0 R D 9684 4741 M 49 0 R +-25 0 R 0 66 R -24 0 R 49 0 R D 10018 4625 M 50 0 R -25 0 R 0 33 R -25 0 R +50 0 R D 10353 4328 M 50 0 R -25 0 R 0 50 R -25 0 R 50 0 R D 10688 3915 M +50 0 R -25 0 R 0 66 R -25 0 R 50 0 R D 11023 3354 M 49 0 R -24 0 R 0 99 R +-25 0 R 49 0 R D 11358 2693 M 49 0 R -25 0 R 0 166 R -24 0 R 49 0 R D +11692 1719 M 50 0 R -25 0 R 0 397 R -25 0 R 50 0 R D 12052 1422 M 0 33 R +-25 0 R 50 0 R D 0.000 0.000 0.000 setrgbcolor 7197 5428 M 10 12 R 93 -10 R +92 -12 R 92 -14 R 92 -16 R 92 75 R 92 -21 R 91 -24 R 92 -26 R 91 -28 R +91 49 R 90 -34 R 91 -36 R 91 -37 R 90 26 R 90 -43 R 90 -45 R 90 -47 R +89 -49 R 90 2 R 89 -54 R 90 -57 R 89 -58 R 89 -61 R 88 -20 R 89 -66 R +89 -67 R 88 -70 R 89 -38 R 88 -74 R 88 -77 R 88 -78 R 88 -81 R 87 -57 R +88 -85 R 88 -87 R 87 -90 R 87 -71 R 88 -94 R 87 -96 R 87 -98 R 87 -99 R +87 -88 R 87 -104 R 86 -106 R 87 -108 R 87 -110 R 86 -103 R 87 -114 R +86 -116 R 87 -118 R 86 -114 R 86 -122 R 86 -124 R 86 -127 R 87 -128 R +67 -99 R D 7197 5424 M 10 13 R 93 -5 R 92 -7 R 92 -9 R 92 -12 R 92 84 R +92 -17 R 91 -19 R 92 -21 R 91 -23 R 91 56 R 90 -28 R 91 -31 R 91 -33 R +90 34 R 90 -38 R 90 -41 R 90 -42 R 89 -45 R 90 10 R 89 -50 R 90 -51 R +89 -54 R 89 -56 R 88 -13 R 89 -61 R 89 -63 R 88 -65 R 89 -31 R 88 -70 R +88 -72 R 88 -74 R 88 -76 R 87 -50 R 88 -81 R 88 -83 R 87 -85 R 87 -65 R +88 -89 R 87 -92 R 87 -93 R 87 -95 R 87 -82 R 87 -100 R 86 -102 R 87 -103 R +87 -106 R 86 -97 R 87 -110 R 86 -111 R 87 -114 R 86 -108 R 86 -118 R +86 -120 R 86 -122 R 87 -124 R 67 -94 R D L1 7197 6251 M 10 -1 R 93 -21 R +92 12 R 92 -25 R 92 -28 R 92 -29 R 92 -3 R 91 -34 R 92 -36 R 91 -38 R +91 -40 R 90 -20 R 91 -45 R 91 -46 R 90 -48 R 90 -49 R 90 -37 R 90 -54 R +89 -56 R 90 -58 R 89 -48 R 90 -62 R 89 -64 R 89 -66 R 88 -67 R 89 -62 R +89 -71 R 88 -74 R 89 -75 R 88 -71 R 88 -79 R 88 -81 R 88 -83 R 87 -85 R +88 -82 R 88 -89 R 87 -90 R 87 -92 R 88 -94 R 87 -93 R 87 -97 R 87 -100 R +87 -101 R 87 -102 R 86 -104 R 87 -107 R 87 -109 R 86 -110 R 87 -111 R +86 -114 R 87 -116 R 86 -118 R 86 -120 R 86 -121 R 86 -123 R 87 -125 R +67 -99 R D 7197 4162 M 10 2 R 93 8 R 92 216 R 92 2 R 92 0 R 92 -2 R 92 -5 R +91 177 R 92 -10 R 91 -13 R 91 -15 R 90 143 R 91 -20 R 91 -23 R 90 -25 R +90 -27 R 90 108 R 90 -32 R 89 -35 R 90 -37 R 89 78 R 90 -43 R 89 -45 R +89 -47 R 88 -49 R 89 48 R 89 -55 R 88 -57 R 89 -59 R 88 -61 R 88 19 R +88 -67 R 88 -68 R 87 -71 R 88 -5 R 88 -76 R 87 -79 R 87 -80 R 88 -82 R +87 -31 R 87 -87 R 87 -90 R 87 -91 R 87 -94 R 86 -54 R 87 -98 R 87 -101 R +86 -103 R 87 -72 R 86 -108 R 87 -110 R 86 -111 R 86 -114 R 86 -92 R +86 -118 R 87 -121 R 67 -96 R D gsave 7532 1752 translate 0 0 M 1.1 dup scale +(z = 1.51 - 1.83) show grestore gsave 9675 266 translate 0 0 M +1.01 dup scale -249.284 0 N +(M) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(g) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 15 setlinewidth L0 12152 1422 M 4955 0 R D +13157 1422 M 0 106 R D gsave 13157 889 translate 0 0 M 1.01 dup scale +-305.858 0 N +(-22) show grestore 14496 1422 M 0 106 R D gsave 14496 889 translate 0 0 M +1.01 dup scale -305.858 0 N +(-24) show grestore 15835 1422 M 0 106 R D gsave 15835 889 translate 0 0 M +1.01 dup scale -305.858 0 N +(-26) show grestore 12152 1422 M 0 53 R D 12487 1422 M 0 53 R D 12822 1422 M +0 53 R D 13492 1422 M 0 53 R D 13826 1422 M 0 53 R D 14161 1422 M 0 53 R D +14831 1422 M 0 53 R D 15166 1422 M 0 53 R D 15500 1422 M 0 53 R D +16170 1422 M 0 53 R D 16505 1422 M 0 53 R D 16840 1422 M 0 53 R D +12152 6706 M 4955 0 R D 13157 6706 M 0 -106 R D 14496 6706 M 0 -106 R D +15835 6706 M 0 -106 R D 12152 6706 M 0 -53 R D 12487 6706 M 0 -53 R D +12822 6706 M 0 -53 R D 13492 6706 M 0 -53 R D 13826 6706 M 0 -53 R D +14161 6706 M 0 -53 R D 14831 6706 M 0 -53 R D 15166 6706 M 0 -53 R D +15500 6706 M 0 -53 R D 16170 6706 M 0 -53 R D 16505 6706 M 0 -53 R D +16840 6706 M 0 -53 R D 12152 1422 M 0 5284 R D 12152 1917 M 99 0 R D +gsave 12040 1775 translate 0 0 M 1.01 dup scale -117.687 0 N +( ) show grestore 12152 2743 M 99 0 R D gsave 12040 2601 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 3569 M 99 0 R D gsave 12040 3426 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 4394 M 99 0 R D gsave 12040 4252 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 5220 M 99 0 R D gsave 12040 5077 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 6045 M 99 0 R D gsave 12040 5903 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 1422 M 50 0 R D 12152 1587 M 50 0 R D 12152 1752 M +50 0 R D 12152 2083 M 50 0 R D 12152 2248 M 50 0 R D 12152 2413 M 50 0 R D +12152 2578 M 50 0 R D 12152 2908 M 50 0 R D 12152 3073 M 50 0 R D +12152 3238 M 50 0 R D 12152 3403 M 50 0 R D 12152 3734 M 50 0 R D +12152 3899 M 50 0 R D 12152 4064 M 50 0 R D 12152 4229 M 50 0 R D +12152 4559 M 50 0 R D 12152 4724 M 50 0 R D 12152 4889 M 50 0 R D +12152 5055 M 50 0 R D 12152 5385 M 50 0 R D 12152 5550 M 50 0 R D +12152 5715 M 50 0 R D 12152 5880 M 50 0 R D 12152 6210 M 50 0 R D +12152 6375 M 50 0 R D 12152 6540 M 50 0 R D 12152 6706 M 50 0 R D +17107 1422 M 0 5284 R D 17107 1917 M -99 0 R D 17107 2743 M -99 0 R D +17107 3569 M -99 0 R D 17107 4394 M -99 0 R D 17107 5220 M -99 0 R D +17107 6045 M -99 0 R D 17107 1422 M -49 0 R D 17107 1587 M -49 0 R D +17107 1752 M -49 0 R D 17107 2083 M -49 0 R D 17107 2248 M -49 0 R D +17107 2413 M -49 0 R D 17107 2578 M -49 0 R D 17107 2908 M -49 0 R D +17107 3073 M -49 0 R D 17107 3238 M -49 0 R D 17107 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setlinewidth 16645 1947 M 0 222 R 222 0 R 0 -222 R -222 0 R D +16477 2599 M 0 222 R 222 0 R 0 -222 R -222 0 R D 14301 5073 M 0 222 R +222 0 R 0 -222 R -222 0 R D 14134 5024 M 0 222 R 222 0 R 0 -222 R -222 0 R D +13966 5374 M 0 222 R 222 0 R 0 -222 R -222 0 R D 20 setlinewidth +16756 1422 M 0 1133 R -25 0 R 50 0 R D 16564 2370 M 49 0 R -25 0 R 0 571 R +-24 0 R 49 0 R D 16396 2838 M 50 0 R -25 0 R 0 426 R -25 0 R 50 0 R D +16229 3230 M 49 0 R -24 0 R 0 334 R -25 0 R 49 0 R D 16062 3558 M 49 0 R +-25 0 R 0 280 R -24 0 R 49 0 R D 15894 3782 M 50 0 R -25 0 R 0 253 R -25 0 R +50 0 R D 15727 3888 M 49 0 R -25 0 R 0 249 R -24 0 R 49 0 R D 15559 4144 M +50 0 R -25 0 R 0 221 R -25 0 R 50 0 R D 15392 4371 M 49 0 R -24 0 R 0 199 R +-25 0 R 49 0 R D 15225 4609 M 49 0 R -25 0 R 0 180 R -24 0 R 49 0 R D +15057 4589 M 50 0 R -25 0 R 0 179 R -25 0 R 50 0 R D 14890 4872 M 49 0 R +-25 0 R 0 140 R -24 0 R 49 0 R D 14722 4968 M 50 0 R -25 0 R 0 134 R -25 0 R +50 0 R D 14555 4974 M 49 0 R -24 0 R 0 140 R -25 0 R 49 0 R D 14388 5113 M +49 0 R -25 0 R 0 134 R -24 0 R 49 0 R D 14220 5021 M 50 0 R -25 0 R 0 213 R +-25 0 R 50 0 R D 14053 4604 M 49 0 R -25 0 R 0 1264 R -24 0 R 49 0 R D +0.082 1.000 0.000 setrgbcolor 14763 4790 M -1 13 R -2 13 R -4 13 R -6 11 R +-7 11 R -9 10 R -10 9 R -11 7 R -11 6 R -13 4 R -13 2 R -13 1 R -13 -1 R +-12 -2 R -13 -4 R -12 -6 R -10 -7 R -10 -9 R -9 -10 R -7 -11 R -6 -11 R +-4 -13 R -3 -13 R -1 -13 R 1 -13 R 3 -13 R 4 -12 R 6 -12 R 7 -10 R 9 -10 R +10 -9 R 10 -7 R 12 -6 R 13 -4 R 12 -3 R 13 -1 R 13 1 R 13 3 R 13 4 R 11 6 R +11 7 R 10 9 R 9 10 R 7 10 R 6 12 R 4 12 R 2 13 R 1 13 R F +15098 4642 M -1 13 R -2 13 R -5 12 R -5 12 R -8 11 R -8 9 R -10 9 R -11 7 R +-12 6 R -12 4 R -13 3 R -13 1 R -13 -1 R -13 -3 R -12 -4 R -12 -6 R -11 -7 R +-9 -9 R -9 -9 R -7 -11 R -6 -12 R -4 -12 R -3 -13 R -1 -13 R 1 -13 R 3 -13 R +4 -12 R 6 -12 R 7 -11 R 9 -10 R 9 -9 R 11 -7 R 12 -6 R 12 -4 R 13 -2 R +13 -1 R 13 1 R 13 2 R 12 4 R 12 6 R 11 7 R 10 9 R 8 10 R 8 11 R 5 12 R +5 12 R 2 13 R 1 13 R F +15433 4394 M -1 13 R -3 13 R -4 12 R -5 12 R -8 11 R -8 10 R -10 8 R -11 8 R +-12 5 R -12 5 R -13 2 R -13 1 R -13 -1 R -13 -2 R -12 -5 R -12 -5 R -11 -8 R +-10 -8 R -8 -10 R -8 -11 R -5 -12 R -5 -12 R -2 -13 R -1 -13 R 1 -13 R +2 -13 R 5 -12 R 5 -12 R 8 -11 R 8 -10 R 10 -8 R 11 -7 R 12 -6 R 12 -4 R +13 -3 R 13 -1 R 13 1 R 13 3 R 12 4 R 12 6 R 11 7 R 10 8 R 8 10 R 8 11 R +5 12 R 4 12 R 3 13 R 1 13 R F +15768 4097 M -1 13 R -3 13 R -4 12 R -6 12 R -7 11 R -9 10 R -9 8 R -11 7 R +-12 6 R -12 4 R -13 3 R -13 1 R -13 -1 R -13 -3 R -12 -4 R -12 -6 R -11 -7 R +-10 -8 R -8 -10 R -8 -11 R -6 -12 R -4 -12 R -2 -13 R -1 -13 R 1 -13 R +2 -13 R 4 -12 R 6 -12 R 8 -11 R 8 -10 R 10 -8 R 11 -8 R 12 -5 R 12 -5 R +13 -2 R 13 -1 R 13 1 R 13 2 R 12 5 R 12 5 R 11 8 R 9 8 R 9 10 R 7 11 R +6 12 R 4 12 R 3 13 R 1 13 R F +16102 3651 M 0 13 R -3 13 R -4 12 R -6 12 R -7 11 R -9 10 R -10 8 R -10 8 R +-12 5 R -13 5 R -12 2 R -13 1 R -13 -1 R -13 -2 R -13 -5 R -11 -5 R -11 -8 R +-10 -8 R -9 -10 R -7 -11 R -6 -12 R -4 -12 R -2 -13 R -1 -13 R 1 -13 R +2 -13 R 4 -12 R 6 -12 R 7 -11 R 9 -10 R 10 -8 R 11 -7 R 11 -6 R 13 -4 R +13 -3 R 13 -1 R 13 1 R 12 3 R 13 4 R 12 6 R 10 7 R 10 8 R 9 10 R 7 11 R +6 12 R 4 12 R 3 13 R 0 13 R F +16437 2908 M -1 13 R -2 13 R -4 12 R -6 12 R -7 11 R -9 10 R -10 8 R -11 8 R +-11 5 R -13 5 R -13 2 R -13 1 R -13 -1 R -12 -2 R -13 -5 R -12 -5 R -10 -8 R +-10 -8 R -9 -10 R -7 -11 R -6 -12 R -4 -12 R -3 -13 R -1 -13 R 1 -13 R +3 -13 R 4 -12 R 6 -12 R 7 -11 R 9 -10 R 10 -8 R 10 -7 R 12 -6 R 13 -4 R +12 -3 R 13 -1 R 13 1 R 13 3 R 13 4 R 11 6 R 11 7 R 10 8 R 9 10 R 7 11 R +6 12 R 4 12 R 2 13 R 1 13 R F +16772 2347 M -1 13 R -2 13 R -5 12 R -5 12 R -8 11 R -8 9 R -10 9 R -11 7 R +-12 6 R -12 4 R -13 3 R -13 1 R -13 -1 R -13 -3 R -12 -4 R -12 -6 R -11 -7 R +-9 -9 R -9 -9 R -7 -11 R -6 -12 R -4 -12 R -3 -13 R -1 -13 R 1 -13 R 3 -13 R +4 -12 R 6 -12 R 7 -11 R 9 -10 R 9 -9 R 11 -7 R 12 -6 R 12 -4 R 13 -2 R +13 -1 R 13 1 R 13 2 R 12 4 R 12 6 R 11 7 R 10 9 R 8 10 R 8 11 R 5 12 R +5 12 R 2 13 R 1 13 R F +14639 4642 M 49 0 R -25 0 R 0 280 R -24 0 R 49 0 R D 14973 4625 M 50 0 R +-25 0 R 0 33 R -25 0 R 50 0 R D 15308 4378 M 50 0 R -25 0 R 0 33 R -25 0 R +50 0 R D 15643 4064 M 50 0 R -25 0 R 0 66 R -25 0 R 50 0 R D 15978 3618 M +49 0 R -24 0 R 0 66 R -25 0 R 49 0 R D 16313 2842 M 49 0 R -25 0 R 0 132 R +-24 0 R 49 0 R D 16647 2231 M 50 0 R -25 0 R 0 215 R -25 0 R 50 0 R D +0.000 0.000 0.000 setrgbcolor 12152 5427 M 10 12 R 93 -6 R 92 -9 R 92 -11 R +92 -13 R 92 80 R 92 -18 R 91 -21 R 92 -23 R 91 -25 R 91 53 R 91 -30 R +90 -33 R 91 -34 R 90 31 R 90 -40 R 90 -42 R 90 -45 R 89 -46 R 90 7 R +89 -51 R 90 -54 R 89 -56 R 89 -57 R 89 -16 R 88 -62 R 89 -65 R 88 -67 R +89 -33 R 88 -72 R 88 -74 R 88 -75 R 88 -78 R 87 -53 R 88 -82 R 88 -85 R +87 -86 R 87 -68 R 88 -91 R 87 -93 R 87 -95 R 87 -97 R 87 -84 R 87 -102 R +86 -103 R 87 -105 R 87 -107 R 86 -99 R 87 -112 R 86 -113 R 87 -116 R +86 -110 R 86 -119 R 86 -122 R 87 -123 R 86 -126 R 67 -96 R D 12152 5412 M +10 13 R 93 -1 R 92 -2 R 92 -5 R 92 -7 R 92 91 R 92 -13 R 91 -15 R 92 -16 R +91 -19 R 91 63 R 91 -24 R 90 -27 R 91 -29 R 90 41 R 90 -34 R 90 -36 R +90 -38 R 89 -40 R 90 16 R 89 -46 R 90 -47 R 89 -50 R 89 -52 R 89 -6 R +88 -57 R 89 -59 R 88 -61 R 89 -25 R 88 -66 R 88 -67 R 88 -70 R 88 -72 R +87 -45 R 88 -77 R 88 -78 R 87 -81 R 87 -60 R 88 -86 R 87 -87 R 87 -89 R +87 -91 R 87 -77 R 87 -96 R 86 -98 R 87 -99 R 87 -102 R 86 -92 R 87 -106 R +86 -108 R 87 -109 R 86 -104 R 86 -114 R 86 -116 R 87 -118 R 86 -120 R +67 -91 R D L1 12152 6271 M 10 -1 R 93 -16 R 92 18 R 92 -22 R 92 -23 R +92 -25 R 92 2 R 91 -30 R 92 -32 R 91 -34 R 91 -36 R 91 -15 R 90 -40 R +91 -43 R 90 -44 R 90 -46 R 90 -31 R 90 -51 R 89 -52 R 90 -54 R 89 -43 R +90 -59 R 89 -60 R 89 -62 R 89 -64 R 88 -57 R 89 -67 R 88 -70 R 89 -72 R +88 -67 R 88 -75 R 88 -77 R 88 -79 R 87 -81 R 88 -79 R 88 -85 R 87 -86 R +87 -88 R 88 -90 R 87 -90 R 87 -94 R 87 -95 R 87 -98 R 87 -97 R 86 -102 R +87 -103 R 87 -104 R 86 -107 R 87 -108 R 86 -110 R 87 -112 R 86 -114 R +86 -116 R 86 -117 R 87 -120 R 86 -121 R 67 -96 R D 12152 4123 M 10 2 R +93 13 R 92 224 R 92 6 R 92 5 R 92 2 R 92 0 R 91 184 R 92 -6 R 91 -8 R +91 -11 R 91 151 R 90 -16 R 91 -18 R 90 -21 R 90 -22 R 90 115 R 90 -28 R +89 -31 R 90 -33 R 89 86 R 90 -38 R 89 -41 R 89 -42 R 89 -45 R 88 55 R +89 -51 R 88 -52 R 89 -55 R 88 -57 R 88 26 R 88 -63 R 88 -64 R 87 -66 R +88 1 R 88 -72 R 87 -74 R 87 -76 R 88 -78 R 87 -24 R 87 -83 R 87 -85 R +87 -88 R 87 -89 R 86 -48 R 87 -94 R 87 -97 R 86 -99 R 87 -66 R 86 -103 R +87 -106 R 86 -108 R 86 -110 R 86 -85 R 87 -115 R 86 -116 R 67 -93 R D +gsave 12487 1752 translate 0 0 M 1.1 dup scale +(z = 1.7 - 2.21) show grestore +%%PageTrailer +end +restore +showpage +%%PageResources: font Helvetica +%%+ font Symbol +%%Trailer +restore +%%Pages: 1 +%%DocumentNeededResources: font Helvetica +%%+ font Symbol +%%EOF diff --git a/feedback/papers/0506398/f16.ps b/feedback/papers/0506398/f16.ps new file mode 100644 index 0000000..ea7092a --- /dev/null +++ b/feedback/papers/0506398/f16.ps @@ -0,0 +1,1090 @@ +%!PS-Adobe-3.0 +%%BoundingBox: 54 360 558 720 +%%Title: Graphics produced by IDL +%%For: phopkins@dhcp152-235.cfa.harvard.edu, +%% /Users/phopkins/Documents/lars_galaxies/plots/LF_massive +%%Creator: IDL Student Edition 6.0.3, Mac OS X (darwin ppc m32) +%%CreationDate: Mon Aug 29 03:57:10 2005 +%%DocumentData: Clean7bit +%%Requirements: color +%%LanguageLevel: 1 +%%PageOrder: Ascend +%%Pages: (atend) +%%DocumentNeededResources: (atend) +%%EndComments +%%BeginProlog +save +%+ prolog.ps -- Prolog for IDL generated PostScript files +%+ Copyright (c) 1988-2003 Research Systems, Inc. All Rights Reserved. +%v 4 +/$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C +{currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint +stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} +bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show +grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 +setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 +{[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 +100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 +{[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef +/ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} +ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont +exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica +findfont exch scalefont setfont (\267) show currentpoint grestore moveto} +bdef end 2.5 setmiterlimit +%%EndProlog +%%Page: 0 1 +%%PageRequirements: color +%%PageResources: (atend) +%%PageOrientation: Portrait +%%PageBoundingBox: 54 360 558 720 +%%BeginPageSetup +save +$IDL_DICT begin 54 360 translate 0.0283465 dup scale +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +%%EndPageSetup +15 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 2242 1422 M 14865 0 R D +2242 1422 M 0 211 R D gsave 2242 889 translate 0 0 M 1.01 dup scale +-235.373 0 N +(41) show grestore 4720 1422 M 0 211 R D gsave 4720 889 translate 0 0 M +1.01 dup scale -235.373 0 N +(42) show grestore 7197 1422 M 0 211 R D gsave 7197 889 translate 0 0 M +1.01 dup scale -235.373 0 N +(43) show grestore 9675 1422 M 0 211 R D gsave 9675 889 translate 0 0 M +1.01 dup scale -235.373 0 N +(44) show grestore 12152 1422 M 0 211 R D gsave 12152 889 translate 0 0 M +1.01 dup scale -235.373 0 N +(45) show grestore 14630 1422 M 0 211 R D gsave 14630 889 translate 0 0 M +1.01 dup scale -235.373 0 N +(46) show grestore 17107 1422 M 0 211 R D gsave 17107 889 translate 0 0 M +1.01 dup scale -235.373 0 N +(47) show grestore 2490 1422 M 0 106 R D 2738 1422 M 0 106 R D 2986 1422 M +0 106 R D 3233 1422 M 0 106 R D 3481 1422 M 0 106 R D 3729 1422 M 0 106 R D +3977 1422 M 0 106 R D 4224 1422 M 0 106 R D 4472 1422 M 0 106 R D +4968 1422 M 0 106 R D 5215 1422 M 0 106 R D 5463 1422 M 0 106 R D +5711 1422 M 0 106 R D 5959 1422 M 0 106 R D 6206 1422 M 0 106 R D +6454 1422 M 0 106 R D 6702 1422 M 0 106 R D 6950 1422 M 0 106 R D +7445 1422 M 0 106 R D 7693 1422 M 0 106 R D 7941 1422 M 0 106 R D +8188 1422 M 0 106 R D 8436 1422 M 0 106 R D 8684 1422 M 0 106 R D +8932 1422 M 0 106 R D 9179 1422 M 0 106 R D 9427 1422 M 0 106 R D +9923 1422 M 0 106 R D 10170 1422 M 0 106 R D 10418 1422 M 0 106 R D +10666 1422 M 0 106 R D 10914 1422 M 0 106 R D 11161 1422 M 0 106 R D +11409 1422 M 0 106 R D 11657 1422 M 0 106 R D 11905 1422 M 0 106 R D +12400 1422 M 0 106 R D 12648 1422 M 0 106 R D 12896 1422 M 0 106 R D +13143 1422 M 0 106 R D 13391 1422 M 0 106 R D 13639 1422 M 0 106 R D +13887 1422 M 0 106 R D 14134 1422 M 0 106 R D 14382 1422 M 0 106 R D +14878 1422 M 0 106 R D 15125 1422 M 0 106 R D 15373 1422 M 0 106 R D +15621 1422 M 0 106 R D 15869 1422 M 0 106 R D 16116 1422 M 0 106 R D +16364 1422 M 0 106 R D 16612 1422 M 0 106 R D 16860 1422 M 0 106 R D +gsave 9675 427 translate 0 0 M 1.01 dup scale -1960.51 0 N +(Log\( L) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(2-10 keV) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( \) [erg/s]) show grestore 2242 11989 M 14865 0 R D 2242 11989 M 0 -211 R +D 4720 11989 M 0 -211 R D 7197 11989 M 0 -211 R D 9675 11989 M 0 -211 R D +12152 11989 M 0 -211 R D 14630 11989 M 0 -211 R D 17107 11989 M 0 -211 R D +2490 11989 M 0 -106 R D 2738 11989 M 0 -106 R D 2986 11989 M 0 -106 R D +3233 11989 M 0 -106 R D 3481 11989 M 0 -106 R D 3729 11989 M 0 -106 R D +3977 11989 M 0 -106 R D 4224 11989 M 0 -106 R D 4472 11989 M 0 -106 R D +4968 11989 M 0 -106 R D 5215 11989 M 0 -106 R D 5463 11989 M 0 -106 R D +5711 11989 M 0 -106 R D 5959 11989 M 0 -106 R D 6206 11989 M 0 -106 R D +6454 11989 M 0 -106 R D 6702 11989 M 0 -106 R D 6950 11989 M 0 -106 R D +7445 11989 M 0 -106 R D 7693 11989 M 0 -106 R D 7941 11989 M 0 -106 R D +8188 11989 M 0 -106 R D 8436 11989 M 0 -106 R D 8684 11989 M 0 -106 R D +8932 11989 M 0 -106 R D 9179 11989 M 0 -106 R D 9427 11989 M 0 -106 R D +9923 11989 M 0 -106 R D 10170 11989 M 0 -106 R D 10418 11989 M 0 -106 R D +10666 11989 M 0 -106 R D 10914 11989 M 0 -106 R D 11161 11989 M 0 -106 R D +11409 11989 M 0 -106 R D 11657 11989 M 0 -106 R D 11905 11989 M 0 -106 R D +12400 11989 M 0 -106 R D 12648 11989 M 0 -106 R D 12896 11989 M 0 -106 R D +13143 11989 M 0 -106 R D 13391 11989 M 0 -106 R D 13639 11989 M 0 -106 R D +13887 11989 M 0 -106 R D 14134 11989 M 0 -106 R D 14382 11989 M 0 -106 R D +14878 11989 M 0 -106 R D 15125 11989 M 0 -106 R D 15373 11989 M 0 -106 R D +15621 11989 M 0 -106 R D 15869 11989 M 0 -106 R D 16116 11989 M 0 -106 R D +16364 11989 M 0 -106 R D 16612 11989 M 0 -106 R D 16860 11989 M 0 -106 R D +2242 1422 M 0 10567 R D 2242 1422 M 298 0 R D +gsave 2130 1422 translate 0 0 M 1.01 dup scale -588.433 0 N +(0.0) show grestore 2242 3536 M 298 0 R D gsave 2130 3393 translate 0 0 M +1.01 dup scale -588.433 0 N +(0.2) show grestore 2242 5649 M 298 0 R D gsave 2130 5507 translate 0 0 M +1.01 dup scale -588.433 0 N +(0.4) show grestore 2242 7762 M 298 0 R D gsave 2130 7620 translate 0 0 M +1.01 dup scale -588.433 0 N +(0.6) show grestore 2242 9876 M 298 0 R D gsave 2130 9733 translate 0 0 M +1.01 dup scale -588.433 0 N +(0.8) show grestore 2242 11989 M 298 0 R D gsave 2130 11740 translate 0 0 M +1.01 dup scale -588.433 0 N +(1.0) show grestore 2242 1950 M 149 0 R D 2242 2479 M 149 0 R D 2242 3007 M +149 0 R D 2242 4064 M 149 0 R D 2242 4592 M 149 0 R D 2242 5121 M 149 0 R D +2242 6177 M 149 0 R D 2242 6706 M 149 0 R D 2242 7234 M 149 0 R D +2242 8291 M 149 0 R D 2242 8819 M 149 0 R D 2242 9347 M 149 0 R D +2242 10404 M 149 0 R D 2242 10932 M 149 0 R D 2242 11461 M 149 0 R D +gsave 1200 6706 translate 0 0 M 90 rotate 1.01 dup scale -1858.65 0 N +(Broad-Line Fraction) show grestore 17107 1422 M 0 10567 R D 17107 1422 M +-297 0 R D 17107 3536 M -297 0 R D 17107 5649 M -297 0 R D 17107 7762 M +-297 0 R D 17107 9876 M -297 0 R D 17107 11989 M -297 0 R D 17107 1950 M +-148 0 R D 17107 2479 M -148 0 R D 17107 3007 M -148 0 R D 17107 4064 M +-148 0 R D 17107 4592 M -148 0 R D 17107 5121 M -148 0 R D 17107 6177 M +-148 0 R D 17107 6706 M -148 0 R D 17107 7234 M -148 0 R D 17107 8291 M +-148 0 R D 17107 8819 M -148 0 R D 17107 9347 M -148 0 R D 17107 10404 M +-148 0 R D 17107 10932 M -148 0 R D 17107 11461 M -148 0 R D 40 setlinewidth +2242 1497 M 2 1 R 11 0 R 12 1 R 11 0 R 11 3 R 11 1 R 12 0 R 11 1 R 11 0 R +11 1 R 12 0 R 11 1 R 11 0 R 11 4 R 12 0 R 11 1 R 11 0 R 11 1 R 12 0 R 11 1 R +11 0 R 11 1 R 11 4 R 12 0 R 11 1 R 11 0 R 11 1 R 11 0 R 12 1 R 11 1 R 11 0 R +11 4 R 11 1 R 11 0 R 12 1 R 11 0 R 11 1 R 11 1 R 11 0 R 11 1 R 12 4 R 11 1 R +11 0 R 11 1 R 11 1 R 11 0 R 11 1 R 12 1 R 11 0 R 11 5 R 11 1 R 11 0 R 11 1 R +11 1 R 11 1 R 11 0 R 11 1 R 12 1 R 11 4 R 11 1 R 11 1 R 11 1 R 11 0 R 11 1 R +11 1 R 11 1 R 11 1 R 11 5 R 11 1 R 11 0 R 11 1 R 11 1 R 11 1 R 12 1 R 11 0 R +11 1 R 11 6 R 11 1 R 11 0 R 11 1 R 11 1 R 11 1 R 11 1 R 11 1 R 11 1 R 11 5 R +11 1 R 11 1 R 11 1 R 11 1 R 11 1 R 11 1 R 11 1 R 11 1 R 10 6 R 11 1 R 11 1 R +11 1 R 11 1 R 11 1 R 11 1 R 11 1 R 11 1 R 11 7 R 11 1 R 11 1 R 11 1 R 11 1 R +11 1 R 11 1 R 10 1 R 11 1 R 11 7 R 11 1 R 11 1 R 11 1 R 11 1 R 11 1 R 11 1 R +11 2 R 10 1 R 11 7 R 11 1 R 11 2 R 11 1 R 11 1 R 11 1 R 10 1 R 11 1 R 11 2 R +11 8 R 11 1 R 11 1 R 11 1 R 10 1 R 11 2 R 11 1 R 11 1 R 11 1 R 11 9 R 10 1 R +11 1 R 11 2 R 11 1 R 11 1 R 10 2 R 11 1 R 11 1 R 11 9 R 11 2 R 10 1 R 11 1 R +11 2 R 11 1 R 10 1 R 11 2 R 11 1 R 11 10 R 10 1 R 11 2 R 11 1 R 11 2 R +10 1 R 11 1 R 11 2 R 11 1 R 10 10 R 11 2 R 11 1 R 11 2 R 10 1 R 11 2 R +11 1 R 10 2 R 11 2 R 11 10 R 11 2 R 10 1 R 11 2 R 11 2 R 10 1 R 11 2 R +11 1 R 10 2 R 11 11 R 11 2 R 10 2 R 11 1 R 11 2 R 10 2 R 11 1 R 11 2 R +10 2 R 11 12 R 11 1 R 10 2 R 11 2 R 11 2 R 10 1 R 11 2 R 11 2 R 10 2 R +11 12 R 10 2 R 11 2 R 11 2 R 10 1 R 11 2 R 11 2 R 10 2 R 11 2 R 10 13 R +11 2 R 11 2 R 10 2 R 11 2 R 10 2 R 11 1 R 10 2 R 11 2 R 11 14 R 10 2 R +11 2 R 10 2 R 11 2 R 10 2 R 11 2 R 11 2 R 10 2 R 11 15 R 10 2 R 11 2 R +10 2 R 11 2 R 10 2 R 11 2 R 10 3 R 11 2 R 10 15 R 11 2 R 10 2 R 11 2 R +10 3 R 11 2 R 10 2 R 11 2 R 10 3 R 11 15 R 10 3 R 11 2 R 10 2 R 11 3 R +10 2 R 11 2 R 10 2 R 11 3 R 10 16 R 11 3 R 10 2 R 11 3 R 10 2 R 11 2 R +10 3 R 10 2 R 11 3 R 10 17 R 11 2 R 10 3 R 11 2 R 10 3 R 10 2 R 11 3 R +10 2 R 11 3 R 10 18 R 11 3 R 10 2 R 10 3 R 11 2 R 10 3 R 11 3 R 10 2 R +10 3 R 11 19 R 10 2 R 11 3 R 10 3 R 10 3 R 11 2 R 10 3 R 10 3 R 11 2 R +10 20 R 11 3 R 10 3 R 10 2 R 11 3 R 10 3 R 10 3 R 11 3 R 10 3 R 10 20 R +11 3 R 10 3 R 10 3 R 11 3 R 10 3 R 10 2 R 11 3 R 10 3 R 10 22 R 11 3 R +10 3 R 10 3 R 11 3 R 10 3 R 10 3 R 11 3 R 10 3 R 10 22 R 10 3 R 11 3 R +10 3 R 10 3 R 11 4 R 10 3 R 10 3 R 10 3 R 11 23 R 10 3 R 10 3 R 10 4 R +11 3 R 10 3 R 10 3 R 10 4 R 11 3 R 10 24 R 10 3 R 10 3 R 11 4 R 10 3 R +10 3 R 10 4 R 11 3 R 10 3 R 10 25 R 10 4 R 10 3 R 11 3 R 10 4 R 10 3 R +10 4 R 11 3 R 10 4 R 10 25 R 10 4 R 10 3 R 11 4 R 10 3 R 10 4 R 10 4 R +10 3 R 10 4 R 11 26 R 10 4 R 10 4 R 10 3 R 10 4 R 10 4 R 11 3 R 10 4 R +10 4 R 10 27 R 10 4 R 10 3 R 11 4 R 10 4 R 10 4 R 10 4 R 10 3 R 10 4 R +10 28 R 10 4 R 11 4 R 10 4 R 10 4 R 10 4 R 10 4 R 10 4 R 10 4 R 10 29 R +11 4 R 10 4 R 10 4 R 10 4 R 10 4 R 10 4 R 10 4 R 10 4 R 10 30 R 10 4 R +10 4 R 11 4 R 10 4 R 10 4 R 10 4 R 10 5 R 10 4 R 10 31 R 10 4 R 10 4 R +10 4 R 10 5 R 10 4 R 10 4 R 10 4 R 10 5 R 10 31 R 11 5 R 10 4 R 10 4 R +10 5 R 10 4 R 10 4 R 10 5 R 10 4 R 10 33 R 10 4 R 10 5 R 10 4 R 10 4 R +10 5 R 10 4 R 10 5 R 10 4 R 10 34 R 10 4 R 10 5 R 10 4 R 10 5 R 10 5 R +10 4 R 10 5 R 10 4 R 10 35 R 10 4 R 10 5 R 10 5 R 10 4 R 10 5 R 10 5 R +10 4 R 10 5 R 9 35 R 10 5 R 10 5 R 10 5 R 10 4 R 10 5 R 10 5 R 10 5 R 10 5 R +10 36 R 10 5 R 10 4 R 10 5 R 10 5 R 10 5 R 10 5 R 10 5 R 9 5 R 10 37 R +10 5 R 10 5 R 10 5 R 10 5 R 10 5 R 10 5 R 10 5 R 10 5 R 10 38 R 9 5 R 10 5 R +10 5 R 10 5 R 10 5 R 10 5 R 10 5 R 10 5 R 10 39 R 9 5 R 10 5 R 10 6 R 10 5 R +10 5 R 10 5 R 10 5 R 9 6 R 10 39 R 10 5 R 10 6 R 10 5 R 10 5 R 10 5 R 9 6 R +10 5 R 10 5 R 10 41 R 10 5 R 10 5 R 9 6 R 10 5 R 10 6 R 10 5 R 10 5 R 10 6 R +9 41 R 10 5 R 10 6 R 10 5 R 10 6 R 9 5 R 10 6 R 10 5 R 10 6 R 10 42 R 10 5 R +9 6 R 10 5 R 10 6 R 10 5 R 9 6 R 10 6 R 10 5 R 10 43 R 10 5 R 9 6 R 10 6 R +10 5 R 10 6 R 9 6 R 10 5 R 10 6 R 10 43 R 10 6 R 9 6 R 10 6 R 10 5 R 10 6 R +9 6 R 10 6 R 10 6 R 10 44 R 9 5 R 10 6 R 10 6 R 10 6 R 9 6 R 10 6 R 10 5 R +9 6 R 10 45 R 10 6 R 10 6 R 9 6 R 10 6 R 10 6 R 10 6 R 9 5 R 10 6 R 10 46 R +9 6 R 10 6 R 10 6 R 9 6 R 10 6 R 10 6 R 10 6 R 9 6 R 10 46 R 10 6 R 9 6 R +10 6 R 10 6 R 9 6 R 10 6 R 10 6 R 9 6 R 10 47 R 10 6 R 9 6 R 10 7 R 10 6 R +9 6 R 10 6 R 10 6 R 9 6 R 10 48 R 10 6 R 9 6 R 10 6 R 10 6 R 9 7 R 10 6 R +10 6 R 9 6 R 10 48 R 10 6 R 9 7 R 10 6 R 10 6 R 9 6 R 10 7 R 9 6 R 10 6 R +10 49 R 9 6 R 10 6 R 10 7 R 9 6 R 10 6 R 9 7 R 10 6 R 10 6 R 9 49 R 10 7 R +9 6 R 10 6 R 10 7 R 9 6 R 10 7 R 9 6 R 10 6 R 10 50 R 9 6 R 10 7 R 9 6 R +10 7 R 10 6 R 9 7 R 10 6 R 9 6 R 10 50 R 9 7 R 10 6 R 10 7 R 9 6 R 10 7 R +9 6 R 10 7 R 9 6 R 10 51 R 10 6 R 9 7 R 10 6 R 9 7 R 10 6 R 9 7 R 10 6 R +9 7 R 10 51 R 9 6 R 10 7 R 10 6 R 9 7 R 10 6 R 9 7 R 10 7 R 9 6 R 10 51 R +9 7 R 10 6 R 9 7 R 10 7 R 9 6 R 10 7 R 9 6 R 10 7 R 9 52 R 10 6 R 9 7 R +10 6 R 9 7 R 10 7 R 9 6 R 10 7 R 9 7 R 10 51 R 9 7 R 10 7 R 9 6 R 10 7 R +9 7 R 10 6 R 9 7 R 10 7 R 9 52 R 10 6 R 9 7 R 10 7 R 9 7 R 10 6 R 9 7 R +10 7 R 9 6 R 10 53 R 9 6 R 10 7 R 9 7 R 10 6 R 9 7 R 9 7 R 10 7 R 9 6 R +10 53 R 9 6 R 10 7 R 9 7 R 10 7 R 9 6 R 10 7 R 9 7 R 9 6 R 10 53 R 9 7 R +10 7 R 9 6 R 10 7 R 9 7 R 10 7 R 9 6 R 9 7 R 10 53 R 9 6 R 10 7 R 9 7 R +10 7 R 9 6 R 9 7 R 10 7 R 9 7 R 10 52 R 9 7 R 9 7 R 10 7 R 9 6 R 10 7 R +9 7 R 9 7 R D 9894 6307 M 10 6 R 9 53 R 10 7 R 9 7 R 9 7 R 10 6 R 9 7 R +10 7 R 9 7 R 9 6 R 10 53 R 9 7 R 10 7 R 9 6 R 9 7 R 10 7 R 9 7 R 10 6 R +9 7 R 9 53 R 10 7 R 9 7 R 9 6 R 10 7 R 9 7 R 10 6 R 9 7 R 9 7 R 10 53 R +9 7 R 9 6 R 10 7 R 9 7 R 9 6 R 10 7 R 9 7 R 9 7 R 10 52 R 9 7 R 10 7 R 9 6 R +9 7 R 10 7 R 9 7 R 9 6 R 10 7 R 9 53 R 9 6 R 10 7 R 9 7 R 9 6 R 10 7 R 9 7 R +9 6 R 10 7 R 9 53 R 9 6 R 10 7 R 9 7 R 9 6 R 10 7 R 9 6 R 9 7 R 9 7 R +10 52 R 9 7 R 9 6 R 10 7 R 9 7 R 9 6 R 10 7 R 9 6 R 9 7 R 10 52 R 9 7 R +9 6 R 9 7 R 10 7 R 9 6 R 9 7 R 10 6 R 9 7 R 9 52 R 10 6 R 9 7 R 9 7 R 9 6 R +10 7 R 9 6 R 9 7 R 10 6 R 9 52 R 9 6 R 9 7 R 10 6 R 9 7 R 9 6 R 9 7 R 10 6 R +9 7 R 9 51 R 10 7 R 9 6 R 9 7 R 9 6 R 10 7 R 9 6 R 9 7 R 9 6 R 10 51 R 9 7 R +9 6 R 9 6 R 10 7 R 9 6 R 9 7 R 9 6 R 10 6 R 9 51 R 9 6 R 9 7 R 10 6 R 9 7 R +9 6 R 9 6 R 10 7 R 9 6 R 9 50 R 9 7 R 10 6 R 9 6 R 9 7 R 9 6 R 10 6 R 9 6 R +9 7 R 9 50 R 10 6 R 9 6 R 9 6 R 9 7 R 9 6 R 10 6 R 9 6 R 9 7 R 9 49 R 10 6 R +9 7 R 9 6 R 9 6 R 9 6 R 10 6 R 9 6 R 9 7 R 9 49 R 9 6 R 10 6 R 9 6 R 9 6 R +9 6 R 9 6 R 10 7 R 9 6 R 9 48 R 9 6 R 9 6 R 10 6 R 9 6 R 9 7 R 9 6 R 9 6 R +10 6 R 9 48 R 9 6 R 9 6 R 9 6 R 10 6 R 9 6 R 9 6 R 9 6 R 9 6 R 10 47 R 9 6 R +9 6 R 9 6 R 9 6 R 9 6 R 10 6 R 9 5 R 9 6 R 9 47 R 9 6 R 10 6 R 9 6 R 9 6 R +9 6 R 9 5 R 9 6 R 10 6 R 9 46 R 9 6 R 9 6 R 9 6 R 9 6 R 10 5 R 9 6 R 9 6 R +9 5 R 9 46 R 9 6 R 9 6 R 10 5 R 9 6 R 9 6 R 9 5 R 9 6 R 9 6 R 10 45 R 9 6 R +9 5 R 9 6 R 9 5 R 9 6 R 9 6 R 10 5 R 9 6 R 9 44 R 9 6 R 9 5 R 9 6 R 9 5 R +10 6 R 9 5 R 9 6 R 9 5 R 9 44 R 9 6 R 9 5 R 10 6 R 9 5 R 9 6 R 9 5 R 9 5 R +9 6 R 9 43 R 9 6 R 10 5 R 9 5 R 9 6 R 9 5 R 9 5 R 9 6 R 9 5 R 9 43 R 10 5 R +9 5 R 9 5 R 9 6 R 9 5 R 9 5 R 9 5 R 9 6 R 10 41 R 9 6 R 9 5 R 9 5 R 9 5 R +9 5 R 9 6 R 9 5 R 9 5 R 10 41 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 6 R 9 5 R +9 5 R 9 40 R 10 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 40 R 9 5 R +10 5 R 9 5 R 9 4 R 9 5 R 9 5 R 9 5 R 9 5 R 9 39 R 9 5 R 9 5 R 9 5 R 10 4 R +9 5 R 9 5 R 9 5 R 9 4 R 9 39 R 9 5 R 9 4 R 9 5 R 9 5 R 9 4 R 9 5 R 10 5 R +9 4 R 9 38 R 9 5 R 9 4 R 9 5 R 9 5 R 9 4 R 9 5 R 9 4 R 9 5 R 9 37 R 9 4 R +10 5 R 9 4 R 9 5 R 9 4 R 9 5 R 9 4 R 9 5 R 9 36 R 9 4 R 9 5 R 9 4 R 9 5 R +9 4 R 9 5 R 10 4 R 9 4 R 9 36 R 9 4 R 9 4 R 9 5 R 9 4 R 9 4 R 9 5 R 9 4 R +9 4 R 9 35 R 9 4 R 9 4 R 9 5 R 9 4 R 10 4 R 9 4 R 9 5 R 9 4 R 9 34 R 9 4 R +9 4 R 9 4 R 9 4 R 9 4 R 9 4 R 9 4 R 9 5 R 9 33 R 9 4 R 9 4 R 9 4 R 9 4 R +9 4 R 10 4 R 9 4 R 9 4 R 9 32 R 9 4 R 9 4 R 9 4 R 9 4 R 9 4 R 9 4 R 9 4 R +9 4 R 9 31 R 9 4 R 9 4 R 9 4 R 9 4 R 9 4 R 9 3 R 9 4 R 9 4 R 9 31 R 10 4 R +9 4 R 9 3 R 9 4 R 9 4 R 9 4 R 9 3 R 9 4 R 9 30 R 9 4 R 9 3 R 9 4 R 9 4 R +9 3 R 9 4 R 9 4 R 9 3 R 9 30 R 9 3 R 9 4 R 9 3 R 9 4 R 9 3 R 9 4 R 9 4 R +9 3 R 9 29 R 9 3 R 10 4 R 9 3 R 9 4 R 9 3 R 9 4 R 9 3 R 9 3 R 9 28 R 9 4 R +9 3 R 9 3 R 9 4 R 9 3 R 9 4 R 9 3 R 9 3 R 9 27 R 9 4 R 9 3 R 9 3 R 9 4 R +9 3 R 9 3 R 9 3 R 9 4 R 9 26 R 9 3 R 9 4 R 9 3 R 9 3 R 9 3 R 9 3 R 9 4 R +9 3 R 9 25 R 9 4 R 10 3 R 9 3 R 9 3 R 9 3 R 9 3 R 9 3 R 9 3 R 9 25 R 9 3 R +9 3 R 9 3 R 9 3 R 9 3 R 9 3 R 9 3 R 9 3 R 9 25 R 9 3 R 9 3 R 9 3 R 9 3 R +9 2 R 9 3 R 9 3 R 9 3 R 9 24 R 9 3 R 9 3 R 9 2 R 9 3 R 9 3 R 9 3 R 9 3 R +9 3 R 9 23 R 9 2 R 9 3 R 9 3 R 9 3 R 9 3 R 9 2 R 9 3 R 9 3 R 9 22 R 9 3 R +9 3 R 9 2 R 9 3 R 10 3 R 9 2 R 9 3 R 9 3 R 9 21 R 9 3 R 9 3 R 9 2 R 9 3 R +9 3 R 9 2 R 9 3 R 9 2 R 9 21 R 9 3 R 9 2 R 9 3 R 9 3 R 9 2 R 9 3 R 9 2 R +9 3 R 9 20 R 9 3 R 9 2 R 9 3 R 9 2 R 9 3 R 9 2 R 9 3 R 9 2 R 9 20 R 9 2 R +9 3 R 9 2 R 9 3 R 9 2 R 9 2 R 9 3 R 9 2 R 9 19 R 9 3 R 9 2 R 9 2 R 9 3 R +9 2 R 9 3 R 9 2 R 9 2 R 9 19 R 9 2 R 9 2 R 9 3 R 9 2 R 10 2 R 9 3 R 9 2 R +9 2 R 9 18 R 9 3 R 9 2 R 9 2 R 9 2 R 9 3 R 9 2 R 9 2 R 9 3 R 9 17 R 9 2 R +9 2 R 9 3 R 9 2 R 9 2 R 9 2 R 9 3 R 9 2 R 9 17 R 9 2 R 9 2 R 9 2 R 9 3 R +9 2 R 9 2 R 9 2 R 9 3 R 9 16 R 9 2 R 9 2 R 9 2 R 9 3 R 9 2 R 9 2 R 9 2 R +9 3 R 9 15 R 9 2 R 9 3 R 10 2 R 9 2 R 9 2 R 9 3 R 9 2 R 9 2 R 9 15 R 9 2 R +9 3 R 9 2 R 9 2 R 9 2 R 9 3 R 9 2 R 9 2 R 9 15 R 9 2 R 9 2 R 9 3 R 9 2 R +9 2 R 9 2 R 9 3 R 9 2 R 9 14 R 9 3 R 9 2 R 9 2 R 9 3 R 9 2 R 9 2 R 9 3 R +10 2 R 9 14 R 9 2 R 9 3 R 9 2 R 9 2 R 9 3 R 9 2 R 9 3 R 9 2 R 9 14 R 9 2 R +9 3 R 9 2 R 9 3 R 9 2 R 9 3 R 9 2 R 9 3 R 9 13 R 9 3 R 9 2 R 9 3 R 9 3 R +10 2 R 9 3 R 9 3 R 9 2 R 9 14 R 9 2 R 9 3 R 9 3 R 9 3 R 9 3 R 9 2 R 9 3 R +9 3 R 9 13 R 9 3 R 9 3 R 9 3 R 9 3 R 9 3 R 9 4 R 9 3 R 10 3 R 9 13 R 9 3 R +9 3 R 9 4 R 9 3 R 9 3 R 9 4 R 9 3 R 9 4 R 9 13 R 9 3 R 9 4 R 9 4 R 9 3 R +9 4 R 9 4 R 9 4 R 10 4 R 9 13 R 9 4 R 9 4 R 9 4 R 9 4 R 9 5 R 9 4 R 9 4 R +9 5 R 9 13 R 9 4 R 9 5 R 9 5 R 9 5 R 10 4 R 9 5 R 9 5 R 9 6 R 9 13 R 9 5 R +9 5 R 9 6 R 9 5 R 9 6 R 9 6 R 9 5 R 9 6 R 9 14 R 10 6 R 9 6 R 9 7 R 9 6 R +9 6 R 9 7 R 9 7 R 9 7 R 9 14 R 9 7 R 9 7 R 9 8 R 10 7 R 9 0 R 9 0 R 9 0 R +9 0 R 9 0 R 9 0 R D 16731 11989 M 9 0 R 9 0 R 9 0 R 9 0 R 9 0 R 10 0 R 9 0 R +9 0 R 9 0 R 9 0 R 9 0 R 9 0 R 9 0 R 9 0 R 9 0 R 10 0 R 9 0 R 9 0 R 9 0 R +9 0 R 9 0 R 9 0 R 9 0 R 9 0 R 9 0 R 10 0 R 9 0 R 9 0 R 9 0 R 9 0 R 9 0 R +9 0 R 9 0 R 9 0 R 10 0 R 9 0 R 9 0 R 9 0 R 9 0 R 9 0 R 9 0 R 3 0 R D +20 setlinewidth L1 2242 1427 M 2 0 R 11 0 R 12 0 R 11 1 R 11 0 R 11 0 R +12 0 R 11 0 R 11 0 R 11 0 R 12 0 R 11 0 R 11 0 R 11 0 R 12 0 R 11 0 R 11 0 R +11 0 R 12 0 R 11 0 R 11 0 R 11 0 R 11 0 R 12 0 R 11 1 R 11 0 R 11 0 R 11 0 R +12 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 12 0 R 11 0 R 11 0 R 11 0 R 11 0 R +11 0 R 12 0 R 11 1 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 12 0 R 11 0 R 11 0 R +11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 12 1 R 11 0 R 11 0 R 11 0 R +11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R +11 1 R 12 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R +11 0 R 11 0 R 11 1 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R +10 0 R 11 0 R 11 0 R 11 1 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R +11 0 R 11 0 R 11 0 R 11 1 R 11 0 R 10 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R +11 0 R 11 0 R 11 1 R 11 0 R 10 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R +10 0 R 11 1 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 10 0 R 11 0 R 11 0 R 11 1 R +11 0 R 11 0 R 10 0 R 11 0 R 11 0 R 11 0 R 11 0 R 10 0 R 11 1 R 11 0 R 11 0 R +11 0 R 10 0 R 11 0 R 11 0 R 11 0 R 10 1 R 11 0 R 11 0 R 11 0 R 10 0 R 11 0 R +11 0 R 11 0 R 10 1 R 11 0 R 11 0 R 11 0 R 10 0 R 11 0 R 11 0 R 11 1 R 10 0 R +11 0 R 11 0 R 10 0 R 11 0 R 11 0 R 11 0 R 10 1 R 11 0 R 11 0 R 10 0 R 11 0 R +11 0 R 10 0 R 11 1 R 11 0 R 10 0 R 11 0 R 11 0 R 10 0 R 11 1 R 11 0 R 10 0 R +11 0 R 11 0 R 10 0 R 11 1 R 11 0 R 10 0 R 11 0 R 11 0 R 10 0 R 11 0 R 10 1 R +11 0 R 11 0 R 10 0 R 11 0 R 11 1 R 10 0 R 11 0 R 10 0 R 11 0 R 11 0 R 10 1 R +11 0 R 10 0 R 11 0 R 10 0 R 11 0 R 11 1 R 10 0 R 11 0 R 10 0 R 11 0 R 10 1 R +11 0 R 11 0 R 10 0 R 11 0 R 10 1 R 11 0 R 10 0 R 11 0 R 10 0 R 11 1 R 10 0 R +11 0 R 10 0 R 11 0 R 10 1 R 11 0 R 10 0 R 11 0 R 10 0 R 11 1 R 10 0 R 11 0 R +10 0 R 11 0 R 10 1 R 11 0 R 10 0 R 11 0 R 10 1 R 11 0 R 10 0 R 11 0 R 10 1 R +11 0 R 10 0 R 11 0 R 10 0 R 10 1 R 11 0 R 10 0 R 11 0 R 10 1 R 11 0 R 10 0 R +10 0 R 11 1 R 10 0 R 11 0 R 10 0 R 11 1 R 10 0 R 10 0 R 11 0 R 10 1 R 11 0 R +10 0 R 10 0 R 11 1 R 10 0 R 11 0 R 10 0 R 10 1 R 11 0 R 10 0 R 10 1 R 11 0 R +10 0 R 11 0 R 10 1 R 10 0 R 11 0 R 10 0 R 10 1 R 11 0 R 10 0 R 10 1 R 11 0 R +10 0 R 10 1 R 11 0 R 10 0 R 10 0 R 11 1 R 10 0 R 10 0 R 11 1 R 10 0 R 10 0 R +11 1 R 10 0 R 10 0 R 11 0 R 10 1 R 10 0 R 10 0 R 11 1 R 10 0 R 10 0 R 11 1 R +10 0 R 10 0 R 10 1 R 11 0 R 10 0 R 10 1 R 10 0 R 11 0 R 10 1 R 10 0 R 10 0 R +11 1 R 10 0 R 10 1 R 10 0 R 11 0 R 10 1 R 10 0 R 10 0 R 11 1 R 10 0 R 10 0 R +10 1 R 10 0 R 11 1 R 10 0 R 10 0 R 10 1 R 11 0 R 10 0 R 10 1 R 10 0 R 10 1 R +11 0 R 10 0 R 10 1 R 10 0 R 10 1 R 10 0 R 11 0 R 10 1 R 10 0 R 10 1 R 10 0 R +10 0 R 11 1 R 10 0 R 10 1 R 10 0 R 10 0 R 10 1 R 11 0 R 10 1 R 10 0 R 10 1 R +10 0 R 10 0 R 10 1 R 10 0 R 11 1 R 10 0 R 10 1 R 10 0 R 10 1 R 10 0 R 10 1 R +10 0 R 11 0 R 10 1 R 10 0 R 10 1 R 10 0 R 10 1 R 10 0 R 10 1 R 10 0 R 10 1 R +10 0 R 11 1 R 10 0 R 10 1 R 10 0 R 10 1 R 10 0 R 10 1 R 10 0 R 10 1 R 10 0 R +10 1 R 10 0 R 10 1 R 10 0 R 10 1 R 10 0 R 11 1 R 10 0 R 10 1 R 10 0 R 10 1 R +10 1 R 10 0 R 10 1 R 10 0 R 10 1 R 10 0 R 10 1 R 10 0 R 10 1 R 10 1 R 10 0 R +10 1 R 10 0 R 10 1 R 10 0 R 10 1 R 10 1 R 10 0 R 10 1 R 10 0 R 10 1 R 10 1 R +10 0 R 10 1 R 10 0 R 10 1 R 10 1 R 10 0 R 10 1 R 10 0 R 9 1 R 10 1 R 10 0 R +10 1 R 10 1 R 10 0 R 10 1 R 10 0 R 10 1 R 10 1 R 10 0 R 10 1 R 10 1 R 10 0 R +10 1 R 10 1 R 10 0 R 9 1 R 10 1 R 10 0 R 10 1 R 10 1 R 10 1 R 10 0 R 10 1 R +10 1 R 10 0 R 10 1 R 9 1 R 10 0 R 10 1 R 10 1 R 10 1 R 10 0 R 10 1 R 10 1 R +10 1 R 9 0 R 10 1 R 10 1 R 10 1 R 10 0 R 10 1 R 10 1 R 9 1 R 10 0 R 10 1 R +10 1 R 10 1 R 10 0 R 10 1 R 9 1 R 10 1 R 10 1 R 10 0 R 10 1 R 10 1 R 9 1 R +10 1 R 10 0 R 10 1 R 10 1 R 10 1 R 9 1 R 10 1 R 10 0 R 10 1 R 10 1 R 9 1 R +10 1 R 10 1 R 10 1 R 10 0 R 10 1 R 9 1 R 10 1 R 10 1 R 10 1 R 9 1 R 10 1 R +10 1 R 10 0 R 10 1 R 9 1 R 10 1 R 10 1 R 10 1 R 9 1 R 10 1 R 10 1 R 10 1 R +10 1 R 9 1 R 10 1 R 10 1 R 10 1 R 9 1 R 10 1 R 10 0 R 10 1 R 9 1 R 10 1 R +10 1 R 10 1 R 9 1 R 10 1 R 10 1 R 9 1 R 10 1 R 10 2 R 10 1 R 9 1 R 10 1 R +10 1 R 10 1 R 9 1 R 10 1 R 10 1 R 9 1 R 10 1 R 10 1 R 9 1 R 10 1 R 10 1 R +10 1 R 9 1 R 10 2 R 10 1 R 9 1 R 10 1 R 10 1 R 9 1 R 10 1 R 10 1 R 9 2 R +10 1 R 10 1 R 9 1 R 10 1 R 10 1 R 9 2 R 10 1 R 10 1 R 9 1 R 10 1 R 10 1 R +9 2 R 10 1 R 10 1 R 9 1 R 10 1 R 10 2 R 9 1 R 10 1 R 10 1 R 9 2 R 10 1 R +10 1 R 9 1 R 10 2 R 9 1 R 10 1 R 10 2 R 9 1 R 10 1 R 10 1 R 9 2 R 10 1 R +9 1 R 10 2 R 10 1 R 9 1 R 10 2 R 9 1 R 10 1 R 10 2 R 9 1 R 10 1 R 9 2 R +10 1 R 10 2 R 9 1 R 10 1 R 9 2 R 10 1 R 10 2 R 9 1 R 10 1 R 9 2 R 10 1 R +9 2 R 10 1 R 10 2 R 9 1 R 10 2 R 9 1 R 10 1 R 9 2 R 10 1 R 10 2 R 9 1 R +10 2 R 9 1 R 10 2 R 9 2 R 10 1 R 9 2 R 10 1 R 9 2 R 10 1 R 10 2 R 9 1 R +10 2 R 9 2 R 10 1 R 9 2 R 10 1 R 9 2 R 10 2 R 9 1 R 10 2 R 9 1 R 10 2 R +9 2 R 10 1 R 9 2 R 10 2 R 9 1 R 10 2 R 9 2 R 10 1 R 9 2 R 10 2 R 9 2 R +10 1 R 9 2 R 10 2 R 9 2 R 10 1 R 9 2 R 10 2 R 9 2 R 10 1 R 9 2 R 10 2 R +9 2 R 10 2 R 9 1 R 10 2 R 9 2 R 10 2 R 9 2 R 10 2 R 9 1 R 10 2 R 9 2 R +10 2 R 9 2 R 9 2 R 10 2 R 9 2 R 10 2 R 9 1 R 10 2 R 9 2 R 10 2 R 9 2 R +10 2 R 9 2 R 9 2 R 10 2 R 9 2 R 10 2 R 9 2 R 10 2 R 9 2 R 10 2 R 9 2 R 9 2 R +10 2 R 9 2 R 10 3 R 9 2 R 10 2 R 9 2 R 9 2 R 10 2 R 9 2 R 10 2 R 9 2 R 9 3 R +10 2 R 9 2 R 10 2 R 9 2 R 9 2 R D 9894 1912 M 10 3 R 9 2 R 10 2 R 9 2 R +9 3 R 10 2 R 9 2 R 10 2 R 9 3 R 9 2 R 10 2 R 9 2 R 10 3 R 9 2 R 9 2 R 10 3 R +9 2 R 10 2 R 9 3 R 9 2 R 10 2 R 9 3 R 9 2 R 10 3 R 9 2 R 10 2 R 9 3 R 9 2 R +10 3 R 9 2 R 9 3 R 10 2 R 9 3 R 9 2 R 10 3 R 9 2 R 9 3 R 10 2 R 9 3 R 10 2 R +9 3 R 9 2 R 10 3 R 9 3 R 9 2 R 10 3 R 9 2 R 9 3 R 10 3 R 9 2 R 9 3 R 10 3 R +9 2 R 9 3 R 10 3 R 9 2 R 9 3 R 10 3 R 9 3 R 9 2 R 10 3 R 9 3 R 9 3 R 9 2 R +10 3 R 9 3 R 9 3 R 10 3 R 9 3 R 9 2 R 10 3 R 9 3 R 9 3 R 10 3 R 9 3 R 9 3 R +9 3 R 10 3 R 9 3 R 9 3 R 10 2 R 9 3 R 9 3 R 10 3 R 9 3 R 9 3 R 9 4 R 10 3 R +9 3 R 9 3 R 10 3 R 9 3 R 9 3 R 9 3 R 10 3 R 9 3 R 9 4 R 9 3 R 10 3 R 9 3 R +9 3 R 10 3 R 9 4 R 9 3 R 9 3 R 10 3 R 9 4 R 9 3 R 9 3 R 10 4 R 9 3 R 9 3 R +9 3 R 10 4 R 9 3 R 9 4 R 9 3 R 10 3 R 9 4 R 9 3 R 9 4 R 10 3 R 9 4 R 9 3 R +9 3 R 10 4 R 9 3 R 9 4 R 9 4 R 10 3 R 9 4 R 9 3 R 9 4 R 10 3 R 9 4 R 9 4 R +9 3 R 10 4 R 9 4 R 9 3 R 9 4 R 9 4 R 10 3 R 9 4 R 9 4 R 9 4 R 10 3 R 9 4 R +9 4 R 9 4 R 9 4 R 10 3 R 9 4 R 9 4 R 9 4 R 9 4 R 10 4 R 9 4 R 9 4 R 9 4 R +9 4 R 10 3 R 9 4 R 9 4 R 9 4 R 9 5 R 10 4 R 9 4 R 9 4 R 9 4 R 9 4 R 10 4 R +9 4 R 9 4 R 9 4 R 9 5 R 10 4 R 9 4 R 9 4 R 9 4 R 9 5 R 10 4 R 9 4 R 9 4 R +9 5 R 9 4 R 9 4 R 10 5 R 9 4 R 9 5 R 9 4 R 9 4 R 10 5 R 9 4 R 9 5 R 9 4 R +9 5 R 9 4 R 10 5 R 9 4 R 9 5 R 9 4 R 9 5 R 9 4 R 10 5 R 9 5 R 9 4 R 9 5 R +9 5 R 9 4 R 9 5 R 10 5 R 9 4 R 9 5 R 9 5 R 9 5 R 9 5 R 10 4 R 9 5 R 9 5 R +9 5 R 9 5 R 9 5 R 9 5 R 10 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 10 5 R +9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 10 5 R 9 6 R 9 5 R 9 5 R 9 5 R 9 6 R +9 5 R 9 5 R 10 6 R 9 5 R 9 5 R 9 6 R 9 5 R 9 5 R 9 6 R 9 5 R 10 6 R 9 5 R +9 6 R 9 5 R 9 6 R 9 5 R 9 6 R 9 5 R 10 6 R 9 6 R 9 5 R 9 6 R 9 6 R 9 5 R +9 6 R 9 6 R 9 6 R 10 5 R 9 6 R 9 6 R 9 6 R 9 6 R 9 5 R 9 6 R 9 6 R 9 6 R +9 6 R 10 6 R 9 6 R 9 6 R 9 6 R 9 6 R 9 6 R 9 6 R 9 6 R 9 7 R 9 6 R 10 6 R +9 6 R 9 6 R 9 7 R 9 6 R 9 6 R 9 6 R 9 7 R 9 6 R 9 6 R 9 7 R 10 6 R 9 7 R +9 6 R 9 6 R 9 7 R 9 6 R 9 7 R 9 6 R 9 7 R 9 7 R 9 6 R 9 7 R 10 6 R 9 7 R +9 7 R 9 7 R 9 6 R 9 7 R 9 7 R 9 7 R 9 6 R 9 7 R 9 7 R 9 7 R 9 7 R 10 7 R +9 7 R 9 7 R 9 7 R 9 7 R 9 7 R 9 7 R 9 7 R 9 7 R 9 7 R 9 7 R 9 8 R 9 7 R +9 7 R 10 7 R 9 8 R 9 7 R 9 7 R 9 8 R 9 7 R 9 7 R 9 8 R 9 7 R 9 8 R 9 7 R +9 8 R 9 7 R 9 8 R 9 7 R 9 8 R 10 7 R 9 8 R 9 8 R 9 7 R 9 8 R 9 8 R 9 8 R +9 8 R 9 7 R 9 8 R 9 8 R 9 8 R 9 8 R 9 8 R 9 8 R 9 8 R 9 8 R 9 8 R 9 8 R +10 8 R 9 8 R 9 8 R 9 8 R 9 9 R 9 8 R 9 8 R 9 8 R 9 9 R 9 8 R 9 8 R 9 9 R +9 8 R 9 9 R 9 8 R 9 9 R 9 8 R 9 9 R 9 8 R 9 9 R 9 8 R 9 9 R 10 9 R 9 8 R +9 9 R 9 9 R 9 9 R 9 9 R 9 8 R 9 9 R 9 9 R 9 9 R 9 9 R 9 9 R 9 9 R 9 9 R +9 9 R 9 9 R 9 9 R 9 9 R 9 10 R 9 9 R 9 9 R 9 9 R 9 9 R 9 10 R 9 9 R 9 9 R +9 10 R 9 9 R 10 10 R 9 9 R 9 10 R 9 9 R 9 10 R 9 9 R 9 10 R 9 10 R 9 9 R +9 10 R 9 10 R 9 10 R 9 9 R 9 10 R 9 10 R 9 10 R 9 10 R 9 10 R 9 10 R 9 10 R +9 10 R 9 10 R 9 10 R 9 10 R 9 11 R 9 10 R 9 10 R 9 10 R 9 11 R 9 10 R 9 10 R +9 11 R 9 10 R 9 10 R 9 11 R 9 10 R 10 11 R 9 11 R 9 10 R 9 11 R 9 11 R +9 10 R 9 11 R 9 11 R 9 11 R 9 10 R 9 11 R 9 11 R 9 11 R 9 11 R 9 11 R 9 11 R +9 11 R 9 11 R 9 11 R 9 12 R 9 11 R 9 11 R 9 11 R 9 12 R 9 11 R 9 11 R 9 12 R +9 11 R 9 12 R 9 11 R 9 12 R 9 11 R 9 12 R 9 11 R 9 12 R 9 12 R 9 12 R 9 11 R +9 12 R 9 12 R 9 12 R 9 12 R 9 12 R 9 12 R 9 12 R 9 12 R 9 12 R 9 12 R +10 12 R 9 13 R 9 12 R 9 12 R 9 12 R 9 13 R 9 12 R 9 13 R 9 12 R 9 13 R +9 12 R 9 13 R 9 12 R 9 13 R 9 13 R 9 12 R 9 13 R 9 13 R 9 13 R 9 13 R 9 13 R +9 13 R 9 13 R 9 13 R 9 13 R 9 13 R 9 13 R 9 13 R 9 13 R 9 14 R 9 13 R 9 13 R +9 14 R 9 13 R 9 14 R 9 13 R 9 14 R 9 13 R 9 14 R 9 13 R 9 14 R 9 14 R 9 14 R +9 14 R 9 13 R 9 14 R 9 14 R 9 14 R 9 14 R 9 14 R 9 15 R 9 14 R 9 14 R 9 14 R +10 14 R 9 15 R 9 14 R 9 15 R 9 14 R 9 15 R 9 14 R 9 15 R 9 14 R 9 15 R +9 15 R 9 14 R 9 15 R 9 15 R 9 15 R 9 15 R 9 15 R 9 15 R 9 15 R 9 15 R 9 15 R +9 16 R 9 15 R 9 15 R 9 15 R 9 16 R 9 15 R 9 16 R 9 15 R 9 16 R 9 16 R 9 15 R +9 16 R 9 16 R 9 16 R 9 15 R 9 16 R 9 16 R 9 16 R 9 16 R 9 17 R 9 16 R 9 16 R +10 16 R 9 17 R 9 16 R 9 16 R 9 17 R 9 16 R 9 17 R 9 17 R 9 16 R 9 17 R +9 17 R 9 17 R 9 16 R 9 17 R 9 17 R 9 17 R 9 18 R 9 17 R 9 17 R 9 17 R 9 17 R +9 18 R 9 17 R 9 18 R 9 17 R 9 18 R 9 18 R 9 17 R 9 18 R 9 18 R 9 18 R 9 18 R +10 18 R 9 18 R 9 18 R 9 18 R 9 18 R 9 19 R 9 18 R 9 18 R 9 19 R 9 19 R +9 18 R 9 19 R 9 19 R 9 18 R 9 19 R 9 19 R 9 19 R 9 19 R 9 19 R 9 20 R 9 19 R +9 19 R 9 20 R 9 19 R 10 20 R 9 19 R 9 20 R 9 20 R 9 20 R 9 20 R 9 20 R +9 20 R 9 20 R 9 20 R 9 20 R 9 21 R 9 20 R 9 21 R 9 20 R 9 21 R 9 21 R 9 20 R +9 21 R 9 21 R 9 22 R 10 21 R 9 21 R 9 21 R 9 22 R 9 21 R 9 22 R 9 22 R +9 21 R 9 22 R 9 22 R 9 22 R 9 23 R 9 22 R 9 22 R 9 23 R 9 22 R 9 23 R 9 23 R +10 23 R 9 23 R 9 23 R 9 23 R 9 23 R 9 24 R 9 23 R 9 24 R 9 24 R 9 23 R +9 24 R 9 25 R 9 24 R 9 24 R 9 25 R 10 24 R 9 25 R 9 25 R 9 25 R 9 25 R +9 25 R 9 26 R 9 25 R 9 26 R 9 26 R 9 26 R 9 26 R 9 26 R 9 26 R 10 27 R +9 27 R 9 27 R 9 27 R 9 27 R 9 27 R 9 28 R 9 28 R 9 28 R 9 28 R 9 28 R 9 28 R +10 29 R 9 29 R 9 29 R 9 29 R 9 30 R 9 29 R 9 30 R D 16731 9419 M 9 30 R +9 31 R 9 30 R 9 31 R 9 31 R 10 31 R 9 31 R 9 32 R 9 32 R 9 32 R 9 32 R +9 33 R 9 33 R 9 33 R 9 34 R 10 33 R 9 34 R 9 35 R 9 34 R 9 35 R 9 36 R +9 35 R 9 36 R 9 36 R 9 37 R 10 36 R 9 38 R 9 37 R 9 38 R 9 38 R 9 39 R +9 39 R 9 40 R 9 39 R 10 41 R 9 40 R 9 41 R 9 42 R 9 42 R 9 42 R 9 43 R +3 14 R D L2 2242 1422 M 2 0 R 11 0 R 12 0 R 11 0 R 11 0 R 11 0 R 12 0 R +11 0 R 11 0 R 11 0 R 12 0 R 11 0 R 11 0 R 11 0 R 12 0 R 11 0 R 11 0 R 11 0 R +12 0 R 11 0 R 11 0 R 11 0 R 11 0 R 12 0 R 11 0 R 11 0 R 11 0 R 11 0 R 12 0 R +11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 12 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R +12 0 R 11 1 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 12 0 R 11 0 R 11 0 R 11 0 R +11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 12 0 R 11 0 R 11 0 R 11 0 R 11 0 R +11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R +12 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R +11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 10 0 R +11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R +11 0 R 11 0 R 11 0 R 11 0 R 10 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R +11 0 R 11 0 R 11 0 R 10 0 R 11 0 R 11 1 R 11 0 R 11 0 R 11 0 R 11 0 R 10 0 R +11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 11 0 R 10 0 R 11 0 R 11 0 R 11 0 R 11 0 R +11 0 R 10 0 R 11 0 R 11 0 R 11 0 R 11 0 R 10 0 R 11 0 R 11 0 R 11 0 R 11 0 R +10 0 R 11 0 R 11 0 R 11 0 R 10 0 R 11 0 R 11 0 R 11 0 R 10 0 R 11 1 R 11 0 R +11 0 R 10 0 R 11 0 R 11 0 R 11 0 R 10 0 R 11 0 R 11 0 R 11 0 R 10 0 R 11 0 R +11 0 R 10 0 R 11 0 R 11 0 R 11 0 R 10 0 R 11 0 R 11 0 R 10 0 R 11 0 R 11 0 R +10 0 R 11 0 R 11 1 R 10 0 R 11 0 R 11 0 R 10 0 R 11 0 R 11 0 R 10 0 R 11 0 R +11 0 R 10 0 R 11 0 R 11 0 R 10 0 R 11 0 R 11 0 R 10 0 R 11 0 R 10 1 R 11 0 R +11 0 R 10 0 R 11 0 R 11 0 R 10 0 R 11 0 R 10 0 R 11 0 R 11 0 R 10 0 R 11 0 R +10 0 R 11 0 R 10 0 R 11 0 R 11 0 R 10 1 R 11 0 R 10 0 R 11 0 R 10 0 R 11 0 R +11 0 R 10 0 R 11 0 R 10 0 R 11 0 R 10 0 R 11 1 R 10 0 R 11 0 R 10 0 R 11 0 R +10 0 R 11 0 R 10 0 R 11 0 R 10 0 R 11 0 R 10 0 R 11 0 R 10 0 R 11 0 R 10 1 R +11 0 R 10 0 R 11 0 R 10 0 R 11 0 R 10 0 R 11 0 R 10 0 R 11 1 R 10 0 R 11 0 R +10 0 R 11 0 R 10 0 R 10 0 R 11 0 R 10 0 R 11 1 R 10 0 R 11 0 R 10 0 R 10 0 R +11 0 R 10 0 R 11 0 R 10 0 R 11 1 R 10 0 R 10 0 R 11 0 R 10 0 R 11 0 R 10 0 R +10 1 R 11 0 R 10 0 R 11 0 R 10 1 R 10 0 R 11 0 R 10 0 R 10 0 R 11 0 R 10 0 R +11 1 R 10 0 R 10 0 R 11 0 R 10 0 R 10 0 R 11 0 R 10 0 R 10 0 R 11 1 R 10 0 R +10 0 R 11 1 R 10 0 R 10 0 R 11 0 R 10 0 R 10 0 R 11 1 R 10 0 R 10 0 R 11 0 R +10 0 R 10 0 R 11 1 R 10 0 R 10 0 R 10 1 R 11 0 R 10 0 R 10 0 R 11 0 R 10 0 R +10 0 R 10 1 R 11 0 R 10 1 R 10 0 R 10 0 R 11 0 R 10 0 R 10 0 R 10 0 R 11 1 R +10 0 R 10 1 R 10 0 R 11 0 R 10 0 R 10 1 R 10 0 R 11 0 R 10 0 R 10 0 R 10 1 R +10 1 R 11 0 R 10 0 R 10 0 R 10 0 R 11 0 R 10 0 R 10 0 R 10 2 R 10 0 R 11 0 R +10 0 R 10 1 R 10 0 R 10 0 R 10 0 R 11 0 R 10 2 R 10 0 R 10 0 R 10 0 R 10 1 R +11 0 R 10 0 R 10 0 R 10 0 R 10 2 R 10 0 R 11 0 R 10 1 R 10 0 R 10 0 R 10 0 R +10 0 R 10 0 R 10 2 R 11 1 R 10 0 R 10 0 R 10 0 R 10 0 R 10 0 R 10 1 R 10 0 R +11 2 R 10 0 R 10 0 R 10 1 R 10 0 R 10 0 R 10 0 R 10 0 R 10 1 R 10 2 R 10 0 R +11 0 R 10 1 R 10 0 R 10 0 R 10 0 R 10 0 R 10 1 R 10 2 R 10 1 R 10 0 R 10 0 R +10 0 R 10 0 R 10 1 R 10 0 R 10 0 R 11 3 R 10 0 R 10 0 R 10 1 R 10 0 R 10 0 R +10 0 R 10 1 R 10 0 R 10 3 R 10 0 R 10 0 R 10 1 R 10 0 R 10 0 R 10 0 R 10 1 R +10 0 R 10 3 R 10 1 R 10 0 R 10 0 R 10 0 R 10 1 R 10 0 R 10 0 R 10 1 R 10 3 R +10 0 R 10 1 R 10 0 R 10 0 R 10 1 R 10 0 R 10 0 R 9 0 R 10 4 R 10 1 R 10 0 R +10 0 R 10 1 R 10 0 R 10 0 R 10 1 R 10 0 R 10 4 R 10 0 R 10 1 R 10 0 R 10 0 R +10 1 R 10 0 R 9 0 R 10 1 R 10 4 R 10 1 R 10 0 R 10 0 R 10 1 R 10 0 R 10 1 R +10 0 R 10 0 R 9 5 R 10 0 R 10 1 R 10 0 R 10 1 R 10 0 R 10 0 R 10 1 R 10 0 R +9 5 R 10 1 R 10 0 R 10 1 R 10 0 R 10 0 R 10 1 R 9 0 R 10 1 R 10 5 R 10 1 R +10 0 R 10 1 R 10 0 R 9 0 R 10 1 R 10 0 R 10 1 R 10 6 R 10 0 R 9 1 R 10 0 R +10 1 R 10 0 R 10 1 R 10 0 R 9 0 R 10 7 R 10 0 R 10 1 R 10 0 R 9 1 R 10 0 R +10 1 R 10 0 R 10 1 R 10 7 R 9 0 R 10 1 R 10 0 R 10 1 R 9 0 R 10 1 R 10 0 R +10 1 R 10 7 R 9 1 R 10 0 R 10 1 R 10 0 R 9 1 R 10 0 R 10 1 R 10 1 R 10 7 R +9 1 R 10 1 R 10 0 R 10 1 R 9 0 R 10 1 R 10 1 R 10 0 R 9 8 R 10 1 R 10 1 R +10 0 R 9 1 R 10 0 R 10 1 R 9 1 R 10 0 R 10 9 R 10 1 R 9 0 R 10 1 R 10 1 R +10 0 R 9 1 R 10 1 R 10 1 R 9 9 R 10 0 R 10 1 R 9 1 R 10 1 R 10 0 R 10 1 R +9 1 R 10 1 R 10 9 R 9 1 R 10 1 R 10 1 R 9 0 R 10 1 R 10 1 R 9 1 R 10 0 R +10 11 R 9 0 R 10 1 R 10 1 R 9 1 R 10 1 R 10 0 R 9 1 R 10 1 R 10 11 R 9 1 R +10 1 R 10 1 R 9 0 R 10 1 R 10 1 R 9 1 R 10 1 R 10 11 R 9 1 R 10 1 R 10 1 R +9 1 R 10 1 R 9 1 R 10 1 R 10 1 R 9 12 R 10 1 R 10 1 R 9 1 R 10 1 R 9 0 R +10 1 R 10 1 R 9 1 R 10 13 R 9 1 R 10 1 R 10 1 R 9 1 R 10 1 R 9 1 R 10 1 R +10 1 R 9 14 R 10 1 R 9 1 R 10 1 R 10 1 R 9 1 R 10 1 R 9 1 R 10 1 R 9 14 R +10 1 R 10 1 R 9 2 R 10 1 R 9 1 R 10 1 R 9 1 R 10 1 R 10 15 R 9 1 R 10 1 R +9 2 R 10 1 R 9 1 R 10 1 R 9 1 R 10 1 R 9 16 R 10 1 R 10 2 R 9 1 R 10 1 R +9 1 R 10 1 R 9 2 R 10 1 R 9 16 R 10 2 R 9 1 R 10 1 R 9 1 R 10 2 R 9 1 R +10 1 R 9 2 R 10 17 R 9 1 R 10 2 R 9 1 R 10 1 R 9 2 R 10 1 R 9 1 R 10 2 R +9 18 R 10 1 R 9 1 R 10 2 R 9 1 R 10 2 R 9 1 R 10 2 R 9 1 R 10 19 R 9 1 R +10 2 R 9 1 R 10 2 R 9 1 R 10 2 R 9 1 R 10 2 R 9 19 R 10 2 R 9 1 R 10 2 R +9 2 R 9 1 R 10 2 R 9 1 R 10 2 R 9 20 R 10 2 R 9 2 R 10 1 R 9 2 R 10 1 R +9 2 R 9 2 R 10 1 R 9 22 R 10 1 R 9 2 R 10 2 R 9 1 R 10 2 R 9 2 R 9 1 R +10 2 R 9 23 R 10 1 R 9 2 R 10 2 R 9 2 R 9 1 R 10 2 R 9 2 R 10 2 R 9 23 R +9 2 R 10 2 R 9 1 R 10 2 R 9 2 R 9 2 R D 9894 2129 M 10 2 R 9 2 R 10 24 R +9 2 R 9 2 R 10 1 R 9 2 R 10 2 R 9 2 R 9 2 R 10 2 R 9 25 R 10 2 R 9 2 R 9 2 R +10 2 R 9 2 R 10 2 R 9 2 R 9 2 R 10 26 R 9 2 R 9 2 R 10 2 R 9 2 R 10 2 R +9 3 R 9 2 R 10 2 R 9 27 R 9 2 R 10 2 R 9 2 R 9 2 R 10 2 R 9 3 R 9 2 R 10 2 R +9 28 R 10 2 R 9 2 R 9 3 R 10 2 R 9 2 R 9 2 R 10 3 R 9 2 R 9 29 R 10 2 R +9 3 R 9 2 R 10 2 R 9 2 R 9 3 R 10 2 R 9 2 R 9 31 R 10 2 R 9 2 R 9 3 R 10 2 R +9 2 R 9 3 R 9 2 R 10 3 R 9 31 R 9 2 R 10 3 R 9 2 R 9 3 R 10 2 R 9 3 R 9 2 R +10 2 R 9 33 R 9 2 R 9 3 R 10 2 R 9 3 R 9 2 R 10 3 R 9 3 R 9 2 R 10 33 R +9 3 R 9 3 R 9 2 R 10 3 R 9 3 R 9 2 R 10 3 R 9 2 R 9 35 R 9 3 R 10 2 R 9 3 R +9 3 R 9 2 R 10 3 R 9 3 R 9 3 R 10 35 R 9 3 R 9 3 R 9 2 R 10 3 R 9 3 R 9 3 R +9 3 R 10 2 R 9 37 R 9 3 R 9 3 R 10 2 R 9 3 R 9 3 R 9 3 R 10 3 R 9 3 R 9 37 R +9 3 R 10 3 R 9 3 R 9 3 R 9 3 R 10 3 R 9 3 R 9 3 R 9 39 R 10 3 R 9 3 R 9 3 R +9 3 R 10 3 R 9 3 R 9 3 R 9 3 R 10 40 R 9 3 R 9 3 R 9 3 R 9 3 R 10 4 R 9 3 R +9 3 R 9 3 R 10 41 R 9 3 R 9 3 R 9 3 R 9 4 R 10 3 R 9 3 R 9 3 R 9 4 R 9 41 R +10 4 R 9 3 R 9 3 R 9 4 R 9 3 R 10 3 R 9 4 R 9 3 R 9 43 R 9 3 R 10 3 R 9 4 R +9 3 R 9 4 R 9 3 R 10 3 R 9 4 R 9 44 R 9 3 R 9 4 R 10 3 R 9 4 R 9 3 R 9 4 R +9 3 R 10 4 R 9 45 R 9 3 R 9 4 R 9 3 R 9 4 R 10 3 R 9 4 R 9 3 R 9 4 R 9 46 R +10 4 R 9 3 R 9 4 R 9 4 R 9 3 R 9 4 R 10 3 R 9 4 R 9 47 R 9 4 R 9 4 R 9 3 R +10 4 R 9 4 R 9 3 R 9 4 R 9 4 R 9 48 R 9 4 R 10 3 R 9 4 R 9 4 R 9 4 R 9 4 R +9 4 R 10 3 R 9 49 R 9 4 R 9 4 R 9 4 R 9 4 R 9 4 R 10 4 R 9 3 R 9 4 R 9 50 R +9 4 R 9 4 R 9 4 R 10 4 R 9 4 R 9 4 R 9 4 R 9 4 R 9 51 R 9 4 R 10 4 R 9 4 R +9 4 R 9 4 R 9 4 R 9 4 R 9 4 R 9 52 R 10 4 R 9 4 R 9 4 R 9 4 R 9 5 R 9 4 R +9 4 R 9 4 R 10 53 R 9 4 R 9 4 R 9 4 R 9 4 R 9 5 R 9 4 R 9 4 R 10 4 R 9 54 R +9 4 R 9 4 R 9 5 R 9 4 R 9 4 R 9 4 R 9 5 R 10 4 R 9 54 R 9 5 R 9 4 R 9 4 R +9 5 R 9 4 R 9 4 R 9 5 R 9 4 R 10 55 R 9 5 R 9 4 R 9 4 R 9 5 R 9 4 R 9 5 R +9 4 R 9 4 R 9 57 R 10 4 R 9 4 R 9 5 R 9 4 R 9 5 R 9 4 R 9 5 R 9 4 R 9 57 R +9 5 R 9 4 R 10 5 R 9 4 R 9 5 R 9 4 R 9 5 R 9 4 R 9 58 R 9 5 R 9 4 R 9 5 R +9 4 R 9 5 R 10 4 R 9 5 R 9 5 R 9 58 R 9 5 R 9 4 R 9 5 R 9 5 R 9 4 R 9 5 R +9 5 R 9 4 R 9 59 R 10 5 R 9 5 R 9 4 R 9 5 R 9 5 R 9 4 R 9 5 R 9 5 R 9 59 R +9 5 R 9 5 R 9 5 R 9 5 R 9 4 R 10 5 R 9 5 R 9 5 R 9 60 R 9 5 R 9 4 R 9 5 R +9 5 R 9 5 R 9 5 R 9 5 R 9 4 R 9 61 R 9 5 R 9 5 R 9 5 R 10 5 R 9 4 R 9 5 R +9 5 R 9 5 R 9 61 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 62 R +9 5 R 9 4 R 9 5 R 9 5 R 10 5 R 9 5 R 9 5 R 9 5 R 9 63 R 9 5 R 9 5 R 9 5 R +9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 62 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R +9 5 R 9 6 R 10 63 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 64 R +9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 64 R 9 5 R 9 6 R 9 5 R +9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 64 R 10 5 R 9 6 R 9 5 R 9 5 R 9 5 R 9 5 R +9 5 R 9 6 R 9 64 R 9 5 R 9 5 R 9 5 R 9 6 R 9 5 R 9 5 R 9 5 R 9 5 R 9 65 R +9 5 R 9 5 R 9 5 R 9 5 R 9 6 R 9 5 R 9 5 R 9 5 R 9 65 R 9 5 R 9 5 R 9 5 R +9 6 R 9 5 R 9 5 R 9 5 R 9 5 R 9 65 R 10 5 R 9 6 R 9 5 R 9 5 R 9 5 R 9 6 R +9 5 R 9 5 R 9 65 R 9 5 R 9 5 R 9 5 R 9 6 R 9 5 R 9 5 R 9 5 R 9 6 R 9 64 R +9 6 R 9 5 R 9 5 R 9 5 R 9 6 R 9 5 R 9 5 R 9 5 R 9 65 R 9 5 R 9 6 R 9 5 R +9 5 R 9 5 R 9 6 R 9 5 R 9 5 R 9 65 R 9 5 R 9 5 R 9 6 R 9 5 R 9 5 R 9 5 R +9 6 R 9 5 R 9 64 R 9 6 R 9 5 R 9 5 R 10 5 R 9 6 R 9 5 R 9 5 R 9 5 R 9 65 R +9 5 R 9 5 R 9 6 R 9 5 R 9 5 R 9 5 R 9 6 R 9 5 R 9 64 R 9 5 R 9 6 R 9 5 R +9 5 R 9 5 R 9 6 R 9 5 R 9 5 R 9 64 R 9 6 R 9 5 R 9 5 R 9 5 R 9 5 R 9 6 R +9 5 R 9 5 R 9 64 R 9 5 R 9 6 R 9 5 R 9 5 R 9 5 R 9 5 R 9 6 R 9 5 R 9 63 R +9 6 R 9 5 R 9 5 R 9 5 R 9 6 R 9 5 R 9 5 R 9 5 R 9 64 R 9 5 R 9 5 R 9 5 R +10 5 R 9 6 R 9 5 R 9 5 R 9 5 R 9 63 R 9 5 R 9 6 R 9 5 R 9 5 R 9 5 R 9 6 R +9 5 R 9 5 R 9 62 R 9 6 R 9 5 R 9 5 R 9 5 R 9 6 R 9 5 R 9 5 R 9 5 R 9 62 R +9 6 R 9 5 R 9 5 R 9 5 R 9 5 R 9 6 R 9 5 R 9 5 R 9 62 R 9 5 R 9 5 R 9 5 R +9 6 R 9 5 R 9 5 R 9 5 R 9 5 R 9 62 R 9 5 R 10 5 R 9 5 R 9 6 R 9 5 R 9 5 R +9 5 R 9 5 R 9 61 R 9 5 R 9 6 R 9 5 R 9 5 R 9 5 R 9 6 R 9 5 R 9 5 R 9 60 R +9 6 R 9 5 R 9 5 R 9 6 R 9 5 R 9 5 R 9 5 R 9 6 R 9 59 R 9 6 R 9 5 R 9 5 R +9 6 R 9 5 R 9 5 R 10 6 R 9 5 R 9 59 R 9 6 R 9 5 R 9 5 R 9 6 R 9 5 R 9 5 R +9 6 R 9 5 R 9 59 R 9 5 R 9 6 R 9 5 R 9 6 R 9 5 R 9 6 R 9 5 R 9 6 R 9 58 R +9 5 R 9 6 R 9 5 R 10 6 R 9 5 R 9 6 R 9 6 R 9 5 R 9 58 R 9 6 R 9 5 R 9 6 R +9 6 R 9 5 R 9 6 R 9 6 R 9 6 R 9 57 R 9 6 R 9 6 R 9 5 R 9 6 R 9 6 R 9 6 R +10 6 R 9 6 R 9 57 R 9 6 R 9 6 R 9 6 R 9 6 R 9 6 R 9 6 R 9 6 R 9 7 R 9 56 R +9 6 R 9 7 R 9 6 R 9 6 R 9 7 R 9 6 R 10 7 R 9 6 R 9 56 R 9 7 R 9 7 R 9 6 R +9 7 R 9 7 R 9 7 R 9 6 R 9 7 R 9 56 R 9 7 R 9 7 R 9 8 R 10 7 R 9 7 R 9 7 R +9 7 R 9 8 R 9 56 R 9 7 R 9 8 R 9 8 R 9 7 R 9 8 R 9 8 R 9 8 R 9 8 R 10 56 R +9 8 R 9 8 R 9 8 R 9 9 R 9 8 R 9 9 R 9 9 R 9 8 R 9 56 R 9 9 R 9 9 R 10 9 R +9 10 R 9 9 R 9 10 R 9 9 R 9 10 R 9 56 R D 16731 9619 M 9 10 R 9 10 R 9 10 R +9 11 R 9 10 R 10 11 R 9 10 R 9 11 R 9 57 R 9 11 R 9 12 R 9 11 R 9 12 R +9 11 R 9 12 R 10 12 R 9 12 R 9 59 R 9 12 R 9 13 R 9 13 R 9 13 R 9 13 R +9 14 R 9 14 R 10 14 R 9 59 R 9 14 R 9 15 R 9 15 R 9 15 R 9 15 R 9 16 R +9 15 R 10 17 R 9 61 R 9 16 R 9 17 R 9 17 R 9 18 R 9 17 R 3 6 R D 2242 2436 M +2 1 R 11 4 R 12 5 R 11 19 R 11 5 R 11 5 R 12 5 R 11 5 R 11 5 R 11 5 R 12 4 R +11 5 R 11 20 R 11 5 R 12 5 R 11 5 R 11 5 R 11 6 R 12 5 R 11 5 R 11 5 R +11 21 R 11 5 R 12 5 R 11 5 R 11 5 R 11 6 R 11 5 R 12 5 R 11 5 R 11 22 R +11 5 R 11 6 R 11 5 R 12 5 R 11 6 R 11 5 R 11 5 R 11 6 R 11 22 R 12 6 R +11 5 R 11 6 R 11 5 R 11 6 R 11 6 R 11 5 R 12 6 R 11 23 R 11 6 R 11 5 R +11 6 R 11 6 R 11 5 R 11 6 R 11 6 R 11 6 R 12 24 R 11 6 R 11 5 R 11 6 R +11 6 R 11 6 R 11 6 R 11 6 R 11 6 R 11 25 R 11 6 R 11 6 R 11 6 R 11 6 R +11 6 R 11 6 R 12 6 R 11 6 R 11 26 R 11 6 R 11 6 R 11 6 R 11 6 R 11 7 R +11 6 R 11 6 R 11 6 R 11 27 R 11 6 R 11 6 R 11 7 R 11 6 R 11 7 R 11 6 R +11 6 R 11 7 R 11 27 R 10 7 R 11 6 R 11 7 R 11 6 R 11 7 R 11 6 R 11 7 R +11 6 R 11 28 R 11 7 R 11 7 R 11 6 R 11 7 R 11 7 R 11 6 R 11 7 R 10 7 R +11 29 R 11 7 R 11 6 R 11 7 R 11 7 R 11 7 R 11 7 R 11 6 R 11 7 R 10 30 R +11 7 R 11 7 R 11 7 R 11 7 R 11 7 R 11 7 R 10 7 R 11 7 R 11 30 R 11 7 R +11 8 R 11 7 R 11 7 R 10 7 R 11 7 R 11 7 R 11 7 R 11 32 R 11 7 R 10 7 R +11 7 R 11 8 R 11 7 R 11 7 R 10 8 R 11 7 R 11 32 R 11 7 R 11 8 R 10 7 R +11 7 R 11 8 R 11 7 R 10 8 R 11 7 R 11 33 R 11 7 R 10 8 R 11 7 R 11 8 R +11 7 R 10 8 R 11 8 R 11 7 R 11 34 R 10 7 R 11 8 R 11 8 R 11 7 R 10 8 R +11 8 R 11 7 R 10 8 R 11 34 R 11 8 R 11 8 R 10 7 R 11 8 R 11 8 R 10 8 R +11 8 R 11 8 R 10 34 R 11 8 R 11 8 R 10 8 R 11 8 R 11 8 R 10 8 R 11 8 R +11 8 R 10 35 R 11 8 R 11 8 R 10 8 R 11 8 R 11 8 R 10 8 R 11 8 R 11 8 R +10 37 R 11 8 R 10 8 R 11 8 R 11 8 R 10 8 R 11 8 R 11 9 R 10 8 R 11 36 R +10 9 R 11 8 R 11 8 R 10 8 R 11 9 R 10 8 R 11 8 R 10 8 R 11 38 R 11 8 R +10 8 R 11 9 R 10 8 R 11 8 R 10 9 R 11 8 R 11 8 R 10 38 R 11 9 R 10 8 R +11 9 R 10 8 R 11 9 R 10 8 R 11 8 R 10 9 R 11 38 R 10 9 R 11 8 R 10 9 R +11 8 R 10 9 R 11 8 R 10 9 R 11 8 R 10 39 R 11 9 R 10 9 R 11 8 R 10 9 R +11 8 R 10 9 R 11 9 R 10 8 R 11 40 R 10 8 R 11 9 R 10 9 R 11 8 R 10 9 R +11 9 R 10 8 R 10 9 R 11 40 R 10 9 R 11 8 R 10 9 R 11 9 R 10 9 R 10 8 R +11 9 R 10 9 R 11 40 R 10 9 R 11 9 R 10 9 R 10 8 R 11 9 R 10 9 R 11 9 R +10 9 R 10 40 R 11 9 R 10 9 R 11 9 R 10 9 R 10 9 R 11 9 R 10 8 R 10 9 R +11 41 R 10 9 R 11 9 R 10 9 R 10 9 R 11 9 R 10 9 R 10 9 R 11 9 R 10 41 R +10 9 R 11 9 R 10 9 R 10 9 R 11 9 R 10 9 R 10 9 R 11 9 R 10 41 R 10 9 R +11 9 R 10 9 R 10 9 R 11 9 R 10 9 R 10 9 R 11 9 R 10 42 R 10 9 R 10 9 R +11 9 R 10 9 R 10 9 R 11 9 R 10 9 R 10 9 R 10 43 R 11 9 R 10 9 R 10 9 R +10 9 R 11 9 R 10 9 R 10 9 R 10 9 R 11 42 R 10 9 R 10 9 R 10 9 R 11 9 R +10 10 R 10 9 R 10 9 R 11 9 R 10 42 R 10 9 R 10 9 R 10 9 R 11 10 R 10 9 R +10 9 R 10 9 R 11 9 R 10 43 R 10 9 R 10 9 R 10 9 R 11 9 R 10 9 R 10 9 R +10 9 R 10 9 R 10 43 R 11 9 R 10 9 R 10 9 R 10 9 R 10 9 R 10 9 R 11 9 R +10 9 R 10 43 R 10 9 R 10 9 R 10 9 R 11 9 R 10 9 R 10 9 R 10 9 R 10 9 R +10 43 R 10 9 R 10 9 R 11 9 R 10 9 R 10 9 R 10 9 R 10 9 R 10 9 R 10 44 R +10 9 R 11 9 R 10 8 R 10 9 R 10 9 R 10 9 R 10 9 R 10 9 R 10 43 R 10 9 R +10 9 R 10 9 R 11 9 R 10 9 R 10 9 R 10 9 R 10 9 R 10 43 R 10 9 R 10 9 R 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9 42 R 9 5 R 9 6 R +9 6 R 9 5 R 9 6 R 10 6 R 9 5 R 9 6 R 9 41 R 9 6 R 9 5 R 9 6 R 9 6 R 9 5 R +9 6 R 9 5 R 9 6 R 9 40 R 9 6 R 9 6 R 9 5 R 9 6 R 9 5 R 9 6 R 9 5 R 9 6 R +9 39 R 10 6 R 9 5 R 9 6 R 9 5 R 9 5 R 9 6 R 9 5 R 9 6 R 9 39 R 9 5 R 9 5 R +9 6 R 9 5 R 9 5 R 9 6 R 9 5 R 9 5 R 9 39 R 9 5 R 9 5 R 9 6 R 9 5 R 9 5 R +9 5 R 9 5 R 9 6 R 9 37 R 9 6 R 10 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R +9 37 R 9 6 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 36 R 9 5 R 9 5 R +9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 35 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R +9 5 R 9 4 R 9 5 R 9 35 R 9 5 R 10 5 R 9 5 R 9 4 R 9 5 R 9 5 R 9 5 R 9 4 R +9 35 R 9 4 R 9 5 R 9 5 R 9 4 R 9 5 R 9 5 R 9 4 R 9 5 R 9 33 R 9 5 R 9 5 R +9 4 R 9 5 R 9 4 R 9 5 R 9 5 R 9 4 R 9 33 R 9 5 R 9 4 R 9 5 R 9 4 R 9 5 R +9 4 R 9 5 R 9 4 R 9 32 R 9 5 R 9 4 R 9 4 R 9 5 R 9 4 R 9 5 R 9 4 R 9 4 R +9 32 R 9 4 R 9 5 R 9 4 R 9 4 R 10 5 R 9 4 R 9 4 R 9 5 R 9 30 R 9 5 R 9 4 R +9 4 R 9 5 R 9 4 R 9 4 R 9 4 R 9 5 R 9 30 R 9 4 R 9 4 R 9 4 R 9 4 R 9 5 R +9 4 R 9 4 R 9 4 R 9 30 R 9 4 R 9 4 R 9 4 R 9 4 R 9 4 R 9 4 R 9 5 R 9 4 R +9 28 R 9 4 R 9 5 R 9 4 R 9 4 R 9 4 R 9 4 R 9 4 R 9 4 R 9 28 R 9 4 R 9 4 R +9 4 R 9 4 R 9 4 R 9 4 R 9 4 R 9 4 R 9 28 R 9 4 R 9 4 R 9 4 R 9 4 R 10 4 R +9 4 R 9 4 R 9 4 R 9 27 R 9 4 R 9 4 R 9 4 R 9 4 R 9 4 R 9 4 R 9 4 R 9 4 R +9 26 R 9 4 R 9 4 R 9 4 R 9 4 R 9 3 R 9 4 R 9 4 R 9 4 R 9 26 R 9 4 R 9 4 R +9 4 R 9 4 R 9 4 R 9 4 R 9 4 R 9 4 R 9 25 R 9 4 R 9 4 R 9 4 R 9 4 R 9 4 R +9 4 R 9 4 R 9 4 R 9 24 R 9 4 R 9 4 R 10 4 R 9 5 R 9 4 R 9 4 R 9 4 R 9 4 R +9 24 R 9 4 R 9 4 R 9 4 R 9 4 R 9 4 R 9 5 R 9 4 R 9 4 R 9 23 R 9 5 R 9 4 R +9 4 R 9 4 R 9 4 R 9 5 R 9 4 R 9 4 R 9 23 R 9 5 R 9 4 R 9 4 R 9 5 R 9 4 R +9 5 R 9 4 R 10 4 R 9 23 R 9 5 R 9 4 R 9 5 R 9 4 R 9 5 R 9 4 R 9 5 R 9 5 R +9 22 R 9 5 R 9 4 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 4 R 9 23 R 9 4 R 9 5 R +9 6 R 9 5 R 10 5 R 9 5 R 9 5 R 9 5 R 9 22 R 9 6 R 9 5 R 9 5 R 9 6 R 9 5 R +9 6 R 9 5 R 9 6 R 9 22 R 9 5 R 9 6 R 9 6 R 9 6 R 9 6 R 9 6 R 9 6 R 10 6 R +9 22 R 9 6 R 9 6 R 9 7 R 9 6 R 9 7 R 9 6 R 9 7 R 9 6 R 9 22 R 9 7 R 9 7 R +9 7 R 9 7 R 9 7 R 9 8 R 9 7 R 10 7 R 9 22 R 9 8 R 9 8 R 9 7 R 9 8 R 9 8 R +9 8 R 9 8 R 9 9 R 9 22 R 9 9 R 9 8 R 9 9 R 9 9 R 10 8 R 9 9 R 9 10 R 9 9 R +9 23 R 9 10 R 9 9 R 9 10 R 9 10 R 9 10 R 9 10 R 9 10 R 9 11 R 9 24 R 10 11 R +9 11 R 9 11 R 9 11 R 9 11 R 9 12 R 9 12 R 9 12 R 9 25 R 9 12 R 9 13 R 9 12 R +10 13 R 9 0 R 9 0 R 9 0 R 9 0 R 9 0 R 9 0 R D 16731 11989 M 9 0 R 9 0 R +9 0 R 9 0 R 9 0 R 10 0 R 9 0 R 9 0 R 9 0 R 9 0 R 9 0 R 9 0 R 9 0 R 9 0 R +9 0 R 10 0 R 9 0 R 9 0 R 9 0 R 9 0 R 9 0 R 9 0 R 9 0 R 9 0 R 9 0 R 10 0 R +9 0 R 9 0 R 9 0 R 9 0 R 9 0 R 9 0 R 9 0 R 9 0 R 10 0 R 9 0 R 9 0 R 9 0 R +9 0 R 9 0 R 9 0 R 3 0 R D L0 0.000 0.965 1.000 setrgbcolor 2242 1452 M 2 0 R +11 0 R 12 1 R 11 0 R 11 0 R 11 1 R 12 0 R 11 0 R 11 1 R 11 0 R 12 0 R 11 1 R +11 0 R 11 0 R 12 1 R 11 0 R 11 0 R 11 1 R 12 0 R 11 1 R 11 0 R 11 0 R 11 1 R +12 0 R 11 0 R 11 1 R 11 0 R 11 1 R 12 0 R 11 0 R 11 1 R 11 0 R 11 1 R 11 0 R +12 1 R 11 0 R 11 1 R 11 0 R 11 0 R 11 1 R 12 0 R 11 1 R 11 0 R 11 1 R 11 0 R +11 1 R 11 0 R 12 1 R 11 0 R 11 1 R 11 0 R 11 1 R 11 0 R 11 1 R 11 0 R 11 1 R +11 0 R 12 1 R 11 1 R 11 0 R 11 1 R 11 0 R 11 1 R 11 0 R 11 1 R 11 1 R 11 0 R +11 1 R 11 0 R 11 1 R 11 1 R 11 0 R 11 1 R 12 0 R 11 1 R 11 1 R 11 0 R 11 1 R +11 1 R 11 0 R 11 1 R 11 1 R 11 1 R 11 0 R 11 1 R 11 1 R 11 0 R 11 1 R 11 1 R +11 1 R 11 0 R 11 1 R 11 1 R 11 1 R 10 0 R 11 1 R 11 1 R 11 1 R 11 1 R 11 1 R +11 0 R 11 1 R 11 1 R 11 1 R 11 1 R 11 1 R 11 1 R 11 0 R 11 1 R 11 1 R 10 1 R +11 1 R 11 1 R 11 1 R 11 1 R 11 1 R 11 1 R 11 1 R 11 1 R 11 1 R 10 1 R 11 1 R +11 1 R 11 1 R 11 1 R 11 1 R 11 1 R 10 1 R 11 1 R 11 1 R 11 1 R 11 2 R 11 1 R +11 1 R 10 1 R 11 1 R 11 1 R 11 1 R 11 2 R 11 1 R 10 1 R 11 1 R 11 2 R 11 1 R +11 1 R 10 1 R 11 2 R 11 1 R 11 1 R 11 2 R 10 1 R 11 1 R 11 2 R 11 1 R 10 1 R +11 2 R 11 1 R 11 2 R 10 1 R 11 2 R 11 1 R 11 2 R 10 1 R 11 2 R 11 1 R 11 2 R +10 1 R 11 2 R 11 1 R 11 2 R 10 1 R 11 2 R 11 2 R 10 1 R 11 2 R 11 2 R 11 1 R +10 2 R 11 2 R 11 2 R 10 1 R 11 2 R 11 2 R 10 2 R 11 2 R 11 2 R 10 1 R 11 2 R +11 2 R 10 2 R 11 2 R 11 2 R 10 2 R 11 2 R 11 2 R 10 2 R 11 2 R 11 2 R 10 2 R +11 2 R 11 2 R 10 2 R 11 3 R 10 2 R 11 2 R 11 2 R 10 2 R 11 3 R 11 2 R 10 2 R +11 3 R 10 2 R 11 2 R 11 3 R 10 2 R 11 2 R 10 3 R 11 2 R 10 3 R 11 2 R 11 3 R +10 2 R 11 3 R 10 3 R 11 2 R 10 3 R 11 3 R 11 2 R 10 3 R 11 3 R 10 2 R 11 3 R +10 3 R 11 3 R 10 3 R 11 3 R 10 3 R 11 2 R 10 3 R 11 3 R 10 3 R 11 3 R 10 4 R +11 3 R 10 3 R 11 3 R 10 3 R 11 3 R 10 3 R 11 4 R 10 3 R 11 3 R 10 4 R 11 3 R +10 3 R 11 4 R 10 3 R 11 4 R 10 3 R 11 4 R 10 3 R 11 4 R 10 4 R 10 3 R 11 4 R +10 4 R 11 3 R 10 4 R 11 4 R 10 4 R 10 4 R 11 4 R 10 4 R 11 4 R 10 4 R 11 4 R +10 4 R 10 4 R 11 4 R 10 4 R 11 4 R 10 5 R 10 4 R 11 4 R 10 5 R 11 4 R 10 4 R +10 5 R 11 4 R 10 5 R 10 4 R 11 5 R 10 5 R 11 4 R 10 5 R 10 5 R 11 5 R 10 4 R +10 5 R 11 5 R 10 5 R 10 5 R 11 5 R 10 5 R 10 5 R 11 5 R 10 6 R 10 5 R 11 5 R +10 5 R 10 6 R 11 5 R 10 6 R 10 5 R 11 6 R 10 5 R 10 6 R 11 5 R 10 6 R 10 6 R +10 5 R 11 6 R 10 6 R 10 6 R 11 6 R 10 6 R 10 6 R 10 6 R 11 6 R 10 6 R 10 7 R +10 6 R 11 6 R 10 7 R 10 6 R 10 6 R 11 7 R 10 6 R 10 7 R 10 7 R 11 6 R 10 7 R +10 7 R 10 7 R 11 7 R 10 6 R 10 7 R 10 8 R 10 7 R 11 7 R 10 7 R 10 7 R 10 7 R +11 8 R 10 7 R 10 8 R 10 7 R 10 8 R 11 7 R 10 8 R 10 8 R 10 7 R 10 8 R 10 8 R +11 8 R 10 8 R 10 8 R 10 8 R 10 8 R 10 8 R 11 8 R 10 9 R 10 8 R 10 8 R 10 9 R +10 8 R 11 9 R 10 9 R 10 8 R 10 9 R 10 9 R 10 9 R 10 8 R 10 9 R 11 9 R 10 9 R +10 10 R 10 9 R 10 9 R 10 9 R 10 10 R 10 9 R 11 10 R 10 9 R 10 10 R 10 9 R +10 10 R 10 10 R 10 10 R 10 9 R 10 10 R 10 10 R 10 10 R 11 10 R 10 11 R +10 10 R 10 10 R 10 11 R 10 10 R 10 10 R 10 11 R 10 11 R 10 10 R 10 11 R +10 11 R 10 10 R 10 11 R 10 11 R 10 11 R 11 11 R 10 11 R 10 12 R 10 11 R +10 11 R 10 12 R 10 11 R 10 12 R 10 11 R 10 12 R 10 11 R 10 12 R 10 12 R +10 12 R 10 12 R 10 12 R 10 12 R 10 12 R 10 12 R 10 12 R 10 12 R 10 13 R +10 12 R 10 13 R 10 12 R 10 13 R 10 12 R 10 13 R 10 13 R 10 12 R 10 13 R +10 13 R 10 13 R 10 13 R 10 13 R 9 14 R 10 13 R 10 13 R 10 13 R 10 14 R +10 13 R 10 14 R 10 13 R 10 14 R 10 14 R 10 13 R 10 14 R 10 14 R 10 14 R +10 14 R 10 14 R 10 14 R 9 14 R 10 14 R 10 15 R 10 14 R 10 14 R 10 15 R +10 14 R 10 15 R 10 14 R 10 15 R 10 15 R 9 14 R 10 15 R 10 15 R 10 15 R +10 15 R 10 15 R 10 15 R 10 15 R 10 15 R 9 16 R 10 15 R 10 15 R 10 15 R +10 16 R 10 15 R 10 16 R 9 15 R 10 16 R 10 16 R 10 15 R 10 16 R 10 16 R +10 16 R 9 16 R 10 16 R 10 16 R 10 16 R 10 16 R 10 16 R 9 16 R 10 16 R +10 17 R 10 16 R 10 16 R 10 17 R 9 16 R 10 16 R 10 17 R 10 16 R 10 17 R +9 17 R 10 16 R 10 17 R 10 17 R 10 17 R 10 16 R 9 17 R 10 17 R 10 17 R +10 17 R 9 17 R 10 17 R 10 17 R 10 17 R 10 17 R 9 18 R 10 17 R 10 17 R +10 17 R 9 18 R 10 17 R 10 17 R 10 18 R 10 17 R 9 17 R 10 18 R 10 17 R +10 18 R 9 17 R 10 18 R 10 18 R 10 17 R 9 18 R 10 18 R 10 17 R 10 18 R 9 18 R +10 18 R 10 17 R 9 18 R 10 18 R 10 18 R 10 18 R 9 18 R 10 18 R 10 17 R +10 18 R 9 18 R 10 18 R 10 18 R 9 18 R 10 18 R 10 18 R 9 18 R 10 19 R 10 18 R +10 18 R 9 18 R 10 18 R 10 18 R 9 18 R 10 18 R 10 18 R 9 19 R 10 18 R 10 18 R +9 18 R 10 18 R 10 19 R 9 18 R 10 18 R 10 18 R 9 18 R 10 19 R 10 18 R 9 18 R +10 18 R 10 18 R 9 19 R 10 18 R 10 18 R 9 18 R 10 19 R 10 18 R 9 18 R 10 18 R +10 18 R 9 19 R 10 18 R 10 18 R 9 18 R 10 19 R 9 18 R 10 18 R 10 18 R 9 18 R +10 18 R 10 19 R 9 18 R 10 18 R 9 18 R 10 18 R 10 18 R 9 18 R 10 18 R 9 18 R +10 19 R 10 18 R 9 18 R 10 18 R 9 18 R 10 18 R 10 18 R 9 18 R 10 18 R 9 17 R +10 18 R 10 18 R 9 18 R 10 18 R 9 18 R 10 18 R 9 18 R 10 17 R 10 18 R 9 18 R +10 18 R 9 17 R 10 18 R 9 18 R 10 17 R 10 18 R 9 18 R 10 17 R 9 18 R 10 17 R +9 18 R 10 17 R 9 18 R 10 17 R 9 17 R 10 18 R 10 17 R 9 18 R 10 17 R 9 17 R +10 17 R 9 18 R 10 17 R 9 17 R 10 17 R 9 17 R 10 17 R 9 17 R 10 17 R 9 17 R +10 17 R 9 17 R 10 17 R 9 17 R 10 17 R 9 17 R 10 16 R 9 17 R 10 17 R 9 17 R +10 16 R 9 17 R 10 16 R 9 17 R 10 17 R 9 16 R 10 16 R 9 17 R 10 16 R 9 17 R +10 16 R 9 16 R 10 16 R 9 17 R 10 16 R 9 16 R 10 16 R 9 16 R 10 16 R 9 16 R +10 16 R 9 16 R 10 16 R 9 16 R 9 15 R 10 16 R 9 16 R 10 16 R 9 15 R 10 16 R +9 16 R 10 15 R 9 16 R 10 15 R 9 15 R 9 16 R 10 15 R 9 15 R 10 16 R 9 15 R +10 15 R 9 15 R 10 15 R 9 15 R 9 16 R 10 15 R 9 14 R 10 15 R 9 15 R 10 15 R +9 15 R 9 15 R 10 14 R 9 15 R 10 15 R 9 14 R 9 15 R 10 14 R 9 15 R 10 14 R +9 15 R 9 14 R D 9894 8241 M 10 14 R 9 14 R 10 15 R 9 14 R 9 14 R 10 14 R +9 14 R 10 14 R 9 14 R 9 14 R 10 14 R 9 14 R 10 14 R 9 13 R 9 14 R 10 14 R +9 13 R 10 14 R 9 13 R 9 14 R 10 13 R 9 14 R 9 13 R 10 14 R 9 13 R 10 13 R +9 13 R 9 14 R 10 13 R 9 13 R 9 13 R 10 13 R 9 13 R 9 13 R 10 13 R 9 12 R +9 13 R 10 13 R 9 13 R 10 12 R 9 13 R 9 13 R 10 12 R 9 13 R 9 12 R 10 13 R +9 12 R 9 12 R 10 13 R 9 12 R 9 12 R 10 12 R 9 12 R 9 12 R 10 12 R 9 12 R +9 12 R 10 12 R 9 12 R 9 12 R 10 12 R 9 12 R 9 11 R 9 12 R 10 12 R 9 11 R +9 12 R 10 11 R 9 12 R 9 11 R 10 12 R 9 11 R 9 11 R 10 12 R 9 11 R 9 11 R +9 11 R 10 11 R 9 12 R 9 11 R 10 11 R 9 11 R 9 11 R 10 10 R 9 11 R 9 11 R +9 11 R 10 11 R 9 10 R 9 11 R 10 11 R 9 10 R 9 11 R 9 10 R 10 11 R 9 10 R +9 10 R 9 11 R 10 10 R 9 10 R 9 11 R 10 10 R 9 10 R 9 10 R 9 10 R 10 10 R +9 10 R 9 10 R 9 10 R 10 10 R 9 10 R 9 10 R 9 9 R 10 10 R 9 10 R 9 9 R 9 10 R +10 10 R 9 9 R 9 10 R 9 9 R 10 10 R 9 9 R 9 10 R 9 9 R 10 9 R 9 10 R 9 9 R +9 9 R 10 9 R 9 9 R 9 9 R 9 9 R 10 9 R 9 9 R 9 9 R 9 9 R 10 9 R 9 9 R 9 9 R +9 9 R 9 8 R 10 9 R 9 9 R 9 9 R 9 8 R 10 9 R 9 8 R 9 9 R 9 8 R 9 9 R 10 8 R +9 9 R 9 8 R 9 8 R 9 9 R 10 8 R 9 8 R 9 8 R 9 8 R 9 8 R 10 9 R 9 8 R 9 8 R +9 8 R 9 8 R 10 8 R 9 7 R 9 8 R 9 8 R 9 8 R 10 8 R 9 8 R 9 7 R 9 8 R 9 8 R +10 7 R 9 8 R 9 7 R 9 8 R 9 7 R 10 8 R 9 7 R 9 8 R 9 7 R 9 8 R 9 7 R 10 7 R +9 7 R 9 8 R 9 7 R 9 7 R 10 7 R 9 7 R 9 7 R 9 8 R 9 7 R 9 7 R 10 7 R 9 7 R +9 6 R 9 7 R 9 7 R 9 7 R 10 7 R 9 7 R 9 6 R 9 7 R 9 7 R 9 7 R 9 6 R 10 7 R +9 6 R 9 7 R 9 7 R 9 6 R 9 7 R 10 6 R 9 6 R 9 7 R 9 6 R 9 7 R 9 6 R 9 6 R +10 7 R 9 6 R 9 6 R 9 6 R 9 6 R 9 7 R 9 6 R 10 6 R 9 6 R 9 6 R 9 6 R 9 6 R +9 6 R 9 6 R 10 6 R 9 6 R 9 6 R 9 6 R 9 5 R 9 6 R 9 6 R 9 6 R 10 6 R 9 5 R +9 6 R 9 6 R 9 5 R 9 6 R 9 5 R 9 6 R 10 6 R 9 5 R 9 6 R 9 5 R 9 6 R 9 5 R +9 5 R 9 6 R 10 5 R 9 6 R 9 5 R 9 5 R 9 6 R 9 5 R 9 5 R 9 5 R 9 5 R 10 6 R +9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 10 5 R 9 5 R 9 5 R +9 5 R 9 5 R 9 5 R 9 5 R 9 5 R 9 4 R 9 5 R 10 5 R 9 5 R 9 4 R 9 5 R 9 5 R +9 4 R 9 5 R 9 5 R 9 4 R 9 5 R 9 4 R 10 5 R 9 5 R 9 4 R 9 5 R 9 4 R 9 5 R +9 4 R 9 4 R 9 5 R 9 4 R 9 5 R 9 4 R 10 4 R 9 5 R 9 4 R 9 4 R 9 4 R 9 5 R +9 4 R 9 4 R 9 4 R 9 4 R 9 5 R 9 4 R 9 4 R 10 4 R 9 4 R 9 4 R 9 4 R 9 4 R +9 4 R 9 4 R 9 4 R 9 4 R 9 4 R 9 4 R 9 4 R 9 4 R 9 4 R 10 4 R 9 4 R 9 3 R +9 4 R 9 4 R 9 4 R 9 4 R 9 3 R 9 4 R 9 4 R 9 4 R 9 3 R 9 4 R 9 4 R 9 3 R +9 4 R 10 3 R 9 4 R 9 4 R 9 3 R 9 4 R 9 3 R 9 4 R 9 3 R 9 4 R 9 3 R 9 4 R +9 3 R 9 4 R 9 3 R 9 4 R 9 3 R 9 3 R 9 4 R 9 3 R 10 4 R 9 3 R 9 3 R 9 3 R +9 4 R 9 3 R 9 3 R 9 4 R 9 3 R 9 3 R 9 3 R 9 3 R 9 4 R 9 3 R 9 3 R 9 3 R +9 3 R 9 3 R 9 3 R 9 3 R 9 4 R 9 3 R 10 3 R 9 3 R 9 3 R 9 3 R 9 3 R 9 3 R +9 3 R 9 3 R 9 3 R 9 3 R 9 3 R 9 2 R 9 3 R 9 3 R 9 3 R 9 3 R 9 3 R 9 3 R +9 2 R 9 3 R 9 3 R 9 3 R 9 3 R 9 2 R 9 3 R 9 3 R 9 3 R 9 2 R 10 3 R 9 3 R +9 3 R 9 2 R 9 3 R 9 3 R 9 2 R 9 3 R 9 2 R 9 3 R 9 3 R 9 2 R 9 3 R 9 2 R +9 3 R 9 3 R 9 2 R 9 3 R 9 2 R 9 3 R 9 2 R 9 3 R 9 2 R 9 3 R 9 2 R 9 2 R +9 3 R 9 2 R 9 3 R 9 2 R 9 3 R 9 2 R 9 2 R 9 3 R 9 2 R 9 2 R 10 3 R 9 2 R +9 2 R 9 3 R 9 2 R 9 2 R 9 3 R 9 2 R 9 2 R 9 2 R 9 3 R 9 2 R 9 2 R 9 2 R +9 2 R 9 3 R 9 2 R 9 2 R 9 2 R 9 2 R 9 2 R 9 3 R 9 2 R 9 2 R 9 2 R 9 2 R +9 2 R 9 2 R 9 2 R 9 2 R 9 2 R 9 2 R 9 3 R 9 2 R 9 2 R 9 2 R 9 2 R 9 2 R +9 2 R 9 2 R 9 2 R 9 2 R 9 1 R 9 2 R 9 2 R 9 2 R 9 2 R 9 2 R 10 2 R 9 2 R +9 2 R 9 2 R 9 2 R 9 2 R 9 1 R 9 2 R 9 2 R 9 2 R 9 2 R 9 2 R 9 1 R 9 2 R +9 2 R 9 2 R 9 2 R 9 1 R 9 2 R 9 2 R 9 2 R 9 1 R 9 2 R 9 2 R 9 2 R 9 1 R +9 2 R 9 2 R 9 1 R 9 2 R 9 2 R 9 2 R 9 1 R 9 2 R 9 2 R 9 1 R 9 2 R 9 1 R +9 2 R 9 2 R 9 1 R 9 2 R 9 2 R 9 1 R 9 2 R 9 1 R 9 2 R 9 1 R 9 2 R 9 2 R +9 1 R 9 2 R 9 1 R 9 2 R 10 1 R 9 2 R 9 1 R 9 2 R 9 1 R 9 2 R 9 1 R 9 2 R +9 1 R 9 2 R 9 1 R 9 2 R 9 1 R 9 2 R 9 1 R 9 1 R 9 2 R 9 1 R 9 2 R 9 1 R +9 2 R 9 1 R 9 1 R 9 2 R 9 1 R 9 1 R 9 2 R 9 1 R 9 2 R 9 1 R 9 1 R 9 2 R +9 1 R 9 1 R 9 2 R 9 1 R 9 1 R 9 2 R 9 1 R 9 1 R 9 1 R 9 2 R 9 1 R 10 1 R +9 2 R 9 1 R 9 1 R 9 1 R 9 2 R 9 1 R 9 1 R 9 1 R 9 1 R 9 2 R 9 1 R 9 1 R +9 1 R 9 2 R 9 1 R 9 1 R 9 1 R 9 1 R 9 2 R 9 1 R 9 1 R 9 1 R 9 1 R 9 1 R +9 1 R 9 2 R 9 1 R 9 1 R 9 1 R 9 1 R 9 1 R 10 1 R 9 2 R 9 1 R 9 1 R 9 1 R +9 1 R 9 1 R 9 1 R 9 1 R 9 1 R 9 1 R 9 1 R 9 1 R 9 2 R 9 1 R 9 1 R 9 1 R +9 1 R 9 1 R 9 1 R 9 1 R 9 1 R 9 1 R 9 1 R 10 1 R 9 1 R 9 1 R 9 1 R 9 1 R +9 1 R 9 1 R 9 1 R 9 1 R 9 1 R 9 1 R 9 1 R 9 1 R 9 1 R 9 1 R 9 1 R 9 0 R +9 1 R 9 1 R 9 1 R 9 1 R 10 1 R 9 1 R 9 1 R 9 1 R 9 1 R 9 1 R 9 1 R 9 1 R +9 0 R 9 1 R 9 1 R 9 1 R 9 1 R 9 1 R 9 1 R 9 1 R 9 0 R 9 1 R 10 1 R 9 1 R +9 1 R 9 1 R 9 1 R 9 0 R 9 1 R 9 1 R 9 1 R 9 1 R 9 1 R 9 0 R 9 1 R 9 1 R +9 1 R 10 1 R 9 0 R 9 1 R 9 1 R 9 1 R 9 1 R 9 0 R 9 1 R 9 1 R 9 1 R 9 1 R +9 0 R 9 1 R 9 1 R 10 1 R 9 0 R 9 1 R 9 1 R 9 1 R 9 0 R 9 1 R 9 1 R 9 1 R +9 0 R 9 1 R 9 1 R 10 1 R 9 0 R 9 1 R 9 1 R 9 0 R 9 1 R 9 1 R D 16731 11822 M +9 1 R 9 0 R 9 1 R 9 1 R 9 0 R 10 1 R 9 1 R 9 0 R 9 1 R 9 1 R 9 0 R 9 1 R +9 1 R 9 0 R 9 1 R 10 1 R 9 0 R 9 1 R 9 1 R 9 0 R 9 1 R 9 1 R 9 0 R 9 1 R +9 1 R 10 0 R 9 1 R 9 0 R 9 1 R 9 1 R 9 0 R 9 1 R 9 1 R 9 0 R 10 1 R 9 0 R +9 1 R 9 1 R 9 0 R 9 1 R 9 0 R 3 0 R D 10 setlinewidth +0.000 0.000 0.000 setrgbcolor 7641 5644 M 0 222 R 222 0 R 0 -222 R -222 0 R +D 11407 6595 M 0 222 R 222 0 R 0 -222 R -222 0 R D 16362 8391 M 0 222 R +222 0 R 0 -222 R -222 0 R D 20 setlinewidth 7752 5543 M 0 423 R D +5968 5755 M 3568 0 R D 7663 5543 M 178 0 R D 7663 5966 M 178 0 R D +5968 5666 M 0 177 R D 9536 5666 M 0 177 R D 11518 6283 M 0 845 R D +9709 6706 M 3617 0 R D 11429 6283 M 178 0 R D 11429 7128 M 178 0 R D +9709 6617 M 0 177 R D 13327 6617 M 0 177 R D 16473 7868 M 0 1268 R D +13450 8502 M 3657 0 R D 16384 7868 M 178 0 R D 16384 9136 M 178 0 R D +13450 8413 M 0 178 R D 10 setlinewidth 3149 11032 M 0 224 R 224 0 R 0 -224 R +-224 0 R D gsave 3528 11038 translate 0 0 M 1.01 dup scale +(Ueda et al. \(2003\)) show grestore 2934 1945 M 111 222 R 111 -222 R +-222 0 R D 5466 1422 M 56 111 R 55 -111 R D 7889 2791 M 111 222 R 111 -222 R +-222 0 R D 10366 4059 M 111 222 R 111 -222 R -222 0 R D 12844 7123 M +111 222 R 111 -222 R -222 0 R D 20 setlinewidth 3045 1422 M 0 1480 R D +2242 2056 M 2042 0 R D 2956 2902 M 178 0 R D 4284 1967 M 0 178 R D +5522 1422 M 0 528 R D 4284 1422 M 2477 0 R D 5433 1950 M 178 0 R D +4284 1422 M 0 89 R D 6761 1422 M 0 89 R D 8000 2267 M 0 1269 R D 6761 2902 M +2478 0 R D 7911 2267 M 178 0 R D 7911 3536 M 178 0 R D 6761 2813 M 0 177 R D +9239 2813 M 0 177 R D 10477 3324 M 0 1691 R D 9239 4170 M 2477 0 R D +10388 3324 M 178 0 R D 10388 5015 M 178 0 R D 9239 4081 M 0 177 R D +11716 4081 M 0 177 R D 12955 5649 M 0 3170 R D 11716 7234 M 2478 0 R D +12866 5649 M 178 0 R D 12866 8819 M 178 0 R D 11716 7145 M 0 178 R D +14194 7145 M 0 178 R D 10 setlinewidth 3149 10503 M 112 225 R 112 -225 R +-224 0 R D gsave 3528 10510 translate 0 0 M 1.01 dup scale +(Grimes et al. \(2004\)) show grestore 20 setlinewidth 6018 3118 M +111 -111 R -111 -111 R -111 111 R 111 111 R D 6513 3435 M 111 -111 R +-111 -111 R -111 111 R 111 111 R D 7009 3858 M 111 -111 R -111 -111 R +-111 111 R 111 111 R D 7504 4281 M 111 -111 R -111 -111 R -111 111 R +111 111 R D 8000 5337 M 111 -111 R -111 -111 R -111 111 R 111 111 R D +8495 5496 M 111 -111 R -111 -111 R -111 111 R 111 111 R D 8991 4809 M +111 -111 R -111 -111 R -111 111 R 111 111 R D 9486 5549 M 111 -111 R +-111 -111 R -111 111 R 111 111 R D 9982 7345 M 111 -111 R -111 -111 R +-111 111 R 111 111 R D 10725 6869 M 111 -111 R -111 -111 R -111 111 R +111 111 R D 6018 2796 M 0 423 R D 5770 3007 M 496 0 R D 5929 2796 M 178 0 R +D 5929 3219 M 178 0 R D 5770 2918 M 0 178 R D 6266 2918 M 0 178 R D +6513 3113 M 0 423 R D 6266 3324 M 495 0 R D 6424 3113 M 178 0 R D +6424 3536 M 178 0 R D 6266 3235 M 0 178 R D 6761 3235 M 0 178 R D +7009 3536 M 0 422 R D 6761 3747 M 496 0 R D 6920 3536 M 178 0 R D +6920 3958 M 178 0 R D 6761 3658 M 0 178 R D 7257 3658 M 0 178 R D +7504 3958 M 0 423 R D 7257 4170 M 495 0 R D 7415 3958 M 178 0 R D +7415 4381 M 178 0 R D 7257 4081 M 0 177 R D 7752 4081 M 0 177 R D +8000 4962 M 0 528 R D 7752 5226 M 496 0 R D 7911 4962 M 178 0 R D +7911 5490 M 178 0 R D 7752 5137 M 0 178 R D 8248 5137 M 0 178 R D +8495 5068 M 0 634 R D 8248 5385 M 495 0 R D 8406 5068 M 178 0 R D +8406 5702 M 178 0 R D 8248 5296 M 0 178 R D 8743 5296 M 0 178 R D +8991 4328 M 0 740 R D 8743 4698 M 496 0 R D 8902 4328 M 178 0 R D +8902 5068 M 178 0 R D 8743 4609 M 0 178 R D 9239 4609 M 0 178 R D +9486 4909 M 0 1057 R D 9239 5438 M 495 0 R D 9397 4909 M 178 0 R D +9397 5966 M 178 0 R D 9239 5349 M 0 177 R D 9734 5349 M 0 177 R D +9982 6283 M 0 1902 R D 9734 7234 M 496 0 R D 9893 6283 M 178 0 R D +9893 8185 M 178 0 R D 9734 7145 M 0 178 R D 10230 7145 M 0 178 R D +10725 5649 M 0 2219 R D 10230 6758 M 991 0 R D 10636 5649 M 178 0 R D +10636 7868 M 178 0 R D 10230 6670 M 0 177 R D 11221 6670 M 0 177 R D +3261 9671 M 112 -112 R -112 -112 R -112 112 R 112 112 R D +gsave 3528 9453 translate 0 0 M 1.01 dup scale +(Simpson \(2005\)) show grestore 10 setlinewidth 6689 4909 M -1 15 R -3 14 R +-4 14 R -7 13 R -8 12 R -10 11 R -10 9 R -13 8 R -13 7 R -13 4 R -15 3 R +-14 1 R -15 -1 R -14 -3 R -14 -4 R -13 -7 R -12 -8 R -11 -9 R -9 -11 R +-8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -15 R 4 -13 R 7 -13 R +8 -12 R 9 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R 15 -1 R 14 1 R +15 3 R 13 5 R 13 6 R 13 8 R 10 10 R 10 11 R 8 12 R 7 13 R 4 13 R 3 15 R +1 14 R D 7928 4117 M -1 14 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R +-11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R +-13 -6 R -12 -8 R -11 -10 R -9 -11 R -8 -12 R -7 -13 R -5 -14 R -2 -14 R +-1 -14 R 1 -15 R 2 -14 R 5 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -9 R 12 -8 R +13 -7 R 14 -5 R 14 -2 R 15 -1 R 14 1 R 14 2 R 14 5 R 13 7 R 12 8 R 11 9 R +10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 15 R D 9166 5755 M 0 14 R -3 14 R +-5 14 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R +-15 1 R -14 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -10 -11 R +-8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -14 R 1 -15 R 3 -14 R 5 -14 R 6 -13 R +8 -12 R 10 -11 R 11 -9 R 12 -9 R 13 -6 R 14 -5 R 14 -2 R 14 -1 R 15 1 R +14 2 R 14 5 R 13 6 R 12 9 R 11 9 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R +0 15 R D 10405 6600 M -1 14 R -3 15 R -4 13 R -7 13 R -8 12 R -9 11 R +-11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -15 1 R -14 -1 R -14 -3 R -14 -5 R +-13 -6 R -12 -8 R -11 -10 R -10 -11 R -8 -12 R -6 -13 R -5 -13 R -3 -15 R +-1 -14 R 1 -15 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -9 R 12 -8 R +13 -7 R 14 -4 R 14 -3 R 14 -1 R 15 1 R 14 3 R 14 4 R 13 7 R 12 8 R 11 9 R +9 11 R 8 12 R 7 13 R 4 14 R 3 14 R 1 15 R D 11644 6336 M -1 14 R -3 14 R +-4 14 R -7 13 R -8 12 R -10 11 R -10 10 R -12 8 R -14 6 R -13 5 R -15 3 R +-14 1 R -14 -1 R -15 -3 R -13 -5 R -13 -6 R -13 -8 R -10 -10 R -10 -11 R +-8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -14 R 1 -15 R 3 -14 R 4 -14 R 7 -13 R +8 -12 R 10 -11 R 10 -9 R 13 -8 R 13 -7 R 13 -4 R 15 -3 R 14 -1 R 14 1 R +15 3 R 13 4 R 14 7 R 12 8 R 10 9 R 10 11 R 8 12 R 7 13 R 4 14 R 3 14 R +1 15 R D 12883 8291 M -1 14 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R +-11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R +-13 -6 R -12 -8 R -11 -10 R -9 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R +-1 -14 R 1 -15 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -9 R 12 -9 R +13 -6 R 14 -5 R 14 -2 R 15 -1 R 14 1 R 14 2 R 14 5 R 13 6 R 12 9 R 11 9 R +10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 15 R D 14122 7974 M -1 14 R -3 14 R +-5 14 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R +-14 1 R -15 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -10 -11 R +-8 -12 R -6 -13 R -5 -14 R -3 -14 R 0 -14 R 0 -15 R 3 -14 R 5 -14 R 6 -13 R +8 -12 R 10 -11 R 11 -9 R 12 -9 R 13 -6 R 14 -5 R 14 -2 R 15 -1 R 14 1 R +14 2 R 14 5 R 13 6 R 12 9 R 11 9 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R +1 15 R D 20 setlinewidth 6578 3219 M 0 3381 R D 5959 4909 M 1238 0 R D +6489 3219 M 178 0 R D 6489 6600 M 178 0 R D 5959 4820 M 0 178 R D +7197 4820 M 0 178 R D 7817 3536 M 0 1162 R D 7197 4117 M 1239 0 R D +7728 3536 M 178 0 R D 7728 4698 M 178 0 R D 7197 4028 M 0 178 R D +8436 4028 M 0 178 R D 9055 5226 M 0 1057 R D 8436 5755 M 1239 0 R D +8967 5226 M 177 0 R D 8967 6283 M 177 0 R D 8436 5666 M 0 177 R D +9675 5666 M 0 177 R D 10294 6019 M 0 1162 R D 9675 6600 M 1239 0 R D +10205 6019 M 178 0 R D 10205 7181 M 178 0 R D 9675 6511 M 0 178 R D +10914 6511 M 0 178 R D 11533 5702 M 0 1268 R D 10914 6336 M 1238 0 R D +11444 5702 M 178 0 R D 11444 6970 M 178 0 R D 10914 6247 M 0 178 R D +12152 6247 M 0 178 R D 12772 7445 M 0 1691 R D 12152 8291 M 1239 0 R D +12683 7445 M 178 0 R D 12683 9136 M 178 0 R D 12152 8202 M 0 178 R D +13391 8202 M 0 178 R D 14011 6600 M 0 2747 R D 13391 7974 M 1239 0 R D +13922 6600 M 177 0 R D 13922 9347 M 177 0 R D 13391 7885 M 0 178 R D +14630 7885 M 0 178 R D 10 setlinewidth 3373 10087 M -1 15 R -2 14 R -5 14 R +-7 13 R -8 12 R -9 11 R -11 10 R -13 8 R -13 7 R -14 4 R -14 3 R -15 1 R +-14 -1 R -15 -3 R -14 -4 R -13 -7 R -12 -8 R -11 -10 R -10 -11 R -8 -12 R +-6 -13 R -5 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -15 R 5 -14 R 6 -13 R 8 -12 R +10 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 15 -3 R 14 -1 R 15 1 R 14 3 R +14 5 R 13 6 R 13 8 R 11 10 R 9 11 R 8 12 R 7 13 R 5 14 R 2 15 R 1 14 R D +gsave 3528 9982 translate 0 0 M 1.01 dup scale +(Hasinger \(2004\)) show grestore +%%PageTrailer +end +restore +showpage +%%PageResources: font Helvetica +%%Trailer +restore +%%Pages: 1 +%%DocumentNeededResources: font Helvetica +%%EOF diff --git a/feedback/papers/0506398/f17.ps b/feedback/papers/0506398/f17.ps new file mode 100644 index 0000000..b12a1cb --- /dev/null +++ b/feedback/papers/0506398/f17.ps @@ -0,0 +1,205 @@ +%!PS-Adobe-3.0 +%%BoundingBox: 54 360 558 720 +%%Title: Graphics produced by IDL +%%For: phopkins@zeus, /home/phopkins/montecarlo_runs +%%Creator: IDL Version 6.1.1 (linux x86 m32) +%%CreationDate: Mon Aug 29 03:50:20 2005 +%%DocumentData: Clean7bit +%%Requirements: color +%%LanguageLevel: 1 +%%PageOrder: Ascend +%%Pages: (atend) +%%DocumentNeededResources: (atend) +%%EndComments +%%BeginProlog +save +%+ prolog.ps -- Prolog for IDL generated PostScript files +%+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. +%v 5 +/$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C +{currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint +stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} +bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show +grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 +setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 +{[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 +100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 +{[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef +/ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} +ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont +exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica +findfont exch scalefont setfont (\267) show currentpoint grestore moveto} +bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end +%%EndProlog +%%Page: 0 1 +%%PageRequirements: color +%%PageResources: (atend) +%%PageOrientation: Portrait +%%PageBoundingBox: 54 360 558 720 +%%BeginPageSetup +save +$IDL_DICT begin 54 360 translate 0.0283465 dup scale MITERLIMIT +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +%%EndPageSetup +15 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 2242 1422 M 14865 0 R D +2242 1422 M 0 211 R D gsave 2242 889 translate 0 0 M 1.01 dup scale +-235.373 0 N +(41) show grestore 4720 1422 M 0 211 R D gsave 4720 889 translate 0 0 M +1.01 dup scale -235.373 0 N +(42) show grestore 7197 1422 M 0 211 R D gsave 7197 889 translate 0 0 M +1.01 dup scale -235.373 0 N +(43) show grestore 9675 1422 M 0 211 R D gsave 9675 889 translate 0 0 M +1.01 dup scale -235.373 0 N +(44) show grestore 12152 1422 M 0 211 R D gsave 12152 889 translate 0 0 M +1.01 dup scale -235.373 0 N +(45) show grestore 14630 1422 M 0 211 R D gsave 14630 889 translate 0 0 M +1.01 dup scale -235.373 0 N +(46) show grestore 17107 1422 M 0 211 R D gsave 17107 889 translate 0 0 M +1.01 dup scale -235.373 0 N +(47) show grestore 2490 1422 M 0 106 R D 2738 1422 M 0 106 R D 2986 1422 M +0 106 R D 3233 1422 M 0 106 R D 3481 1422 M 0 106 R D 3729 1422 M 0 106 R D +3977 1422 M 0 106 R D 4224 1422 M 0 106 R D 4472 1422 M 0 106 R D +4968 1422 M 0 106 R D 5215 1422 M 0 106 R D 5463 1422 M 0 106 R D +5711 1422 M 0 106 R D 5959 1422 M 0 106 R D 6206 1422 M 0 106 R D +6454 1422 M 0 106 R D 6702 1422 M 0 106 R D 6950 1422 M 0 106 R D +7445 1422 M 0 106 R D 7693 1422 M 0 106 R D 7941 1422 M 0 106 R D +8188 1422 M 0 106 R D 8436 1422 M 0 106 R D 8684 1422 M 0 106 R D +8932 1422 M 0 106 R D 9179 1422 M 0 106 R D 9427 1422 M 0 106 R D +9923 1422 M 0 106 R D 10170 1422 M 0 106 R D 10418 1422 M 0 106 R D +10666 1422 M 0 106 R D 10914 1422 M 0 106 R D 11161 1422 M 0 106 R D +11409 1422 M 0 106 R D 11657 1422 M 0 106 R D 11905 1422 M 0 106 R D +12400 1422 M 0 106 R D 12648 1422 M 0 106 R D 12896 1422 M 0 106 R D +13143 1422 M 0 106 R D 13391 1422 M 0 106 R D 13639 1422 M 0 106 R D +13887 1422 M 0 106 R D 14134 1422 M 0 106 R D 14382 1422 M 0 106 R D +14878 1422 M 0 106 R D 15125 1422 M 0 106 R D 15373 1422 M 0 106 R D +15621 1422 M 0 106 R D 15869 1422 M 0 106 R D 16116 1422 M 0 106 R D +16364 1422 M 0 106 R D 16612 1422 M 0 106 R D 16860 1422 M 0 106 R D +gsave 9675 427 translate 0 0 M 1.01 dup scale -1842.82 0 N +(Log\(L) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(2-10 keV) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(\) [erg/s]) show grestore 2242 11989 M 14865 0 R D 2242 11989 M 0 -211 R D +4720 11989 M 0 -211 R D 7197 11989 M 0 -211 R D 9675 11989 M 0 -211 R D +12152 11989 M 0 -211 R D 14630 11989 M 0 -211 R D 17107 11989 M 0 -211 R D +2490 11989 M 0 -106 R D 2738 11989 M 0 -106 R D 2986 11989 M 0 -106 R D +3233 11989 M 0 -106 R D 3481 11989 M 0 -106 R D 3729 11989 M 0 -106 R D +3977 11989 M 0 -106 R D 4224 11989 M 0 -106 R D 4472 11989 M 0 -106 R D +4968 11989 M 0 -106 R D 5215 11989 M 0 -106 R D 5463 11989 M 0 -106 R D +5711 11989 M 0 -106 R D 5959 11989 M 0 -106 R D 6206 11989 M 0 -106 R D +6454 11989 M 0 -106 R D 6702 11989 M 0 -106 R D 6950 11989 M 0 -106 R D +7445 11989 M 0 -106 R D 7693 11989 M 0 -106 R D 7941 11989 M 0 -106 R D +8188 11989 M 0 -106 R D 8436 11989 M 0 -106 R D 8684 11989 M 0 -106 R D +8932 11989 M 0 -106 R D 9179 11989 M 0 -106 R D 9427 11989 M 0 -106 R D +9923 11989 M 0 -106 R D 10170 11989 M 0 -106 R D 10418 11989 M 0 -106 R D +10666 11989 M 0 -106 R D 10914 11989 M 0 -106 R D 11161 11989 M 0 -106 R D +11409 11989 M 0 -106 R D 11657 11989 M 0 -106 R D 11905 11989 M 0 -106 R D +12400 11989 M 0 -106 R D 12648 11989 M 0 -106 R D 12896 11989 M 0 -106 R D +13143 11989 M 0 -106 R D 13391 11989 M 0 -106 R D 13639 11989 M 0 -106 R D +13887 11989 M 0 -106 R D 14134 11989 M 0 -106 R D 14382 11989 M 0 -106 R D +14878 11989 M 0 -106 R D 15125 11989 M 0 -106 R D 15373 11989 M 0 -106 R D +15621 11989 M 0 -106 R D 15869 11989 M 0 -106 R D 16116 11989 M 0 -106 R D +16364 11989 M 0 -106 R D 16612 11989 M 0 -106 R D 16860 11989 M 0 -106 R D +2242 1422 M 0 10567 R D 2242 1422 M 298 0 R D +gsave 2130 1422 translate 0 0 M 1.01 dup scale -588.433 0 N +(0.2) show grestore 2242 3536 M 298 0 R D gsave 2130 3393 translate 0 0 M +1.01 dup scale -588.433 0 N +(0.3) show grestore 2242 5649 M 298 0 R D gsave 2130 5507 translate 0 0 M +1.01 dup scale -588.433 0 N +(0.4) show grestore 2242 7762 M 298 0 R D gsave 2130 7620 translate 0 0 M +1.01 dup scale -588.433 0 N +(0.5) show grestore 2242 9876 M 298 0 R D gsave 2130 9733 translate 0 0 M +1.01 dup scale -588.433 0 N +(0.6) show grestore 2242 11989 M 298 0 R D gsave 2130 11740 translate 0 0 M +1.01 dup scale -588.433 0 N +(0.7) show grestore 2242 1633 M 149 0 R D 2242 1845 M 149 0 R D 2242 2056 M +149 0 R D 2242 2267 M 149 0 R D 2242 2479 M 149 0 R D 2242 2690 M 149 0 R D +2242 2902 M 149 0 R D 2242 3113 M 149 0 R D 2242 3324 M 149 0 R D +2242 3747 M 149 0 R D 2242 3958 M 149 0 R D 2242 4170 M 149 0 R D +2242 4381 M 149 0 R D 2242 4592 M 149 0 R D 2242 4804 M 149 0 R D +2242 5015 M 149 0 R D 2242 5226 M 149 0 R D 2242 5438 M 149 0 R D +2242 5860 M 149 0 R D 2242 6072 M 149 0 R D 2242 6283 M 149 0 R D +2242 6494 M 149 0 R D 2242 6706 M 149 0 R D 2242 6917 M 149 0 R D +2242 7128 M 149 0 R D 2242 7340 M 149 0 R D 2242 7551 M 149 0 R D +2242 7974 M 149 0 R D 2242 8185 M 149 0 R D 2242 8396 M 149 0 R D +2242 8608 M 149 0 R D 2242 8819 M 149 0 R D 2242 9030 M 149 0 R D +2242 9242 M 149 0 R D 2242 9453 M 149 0 R D 2242 9664 M 149 0 R D +2242 10087 M 149 0 R D 2242 10298 M 149 0 R D 2242 10510 M 149 0 R D +2242 10721 M 149 0 R D 2242 10932 M 149 0 R D 2242 11144 M 149 0 R D +2242 11355 M 149 0 R D 2242 11566 M 149 0 R D 2242 11778 M 149 0 R D +gsave 1200 6706 translate 0 0 M 90 rotate 1.01 dup scale -3268.61 0 N +(Obscured Fraction \(N) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(H) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( > 10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(22) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( cm) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(-2) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(\)) show grestore 17107 1422 M 0 10567 R D 17107 1422 M -297 0 R D +17107 3536 M -297 0 R D 17107 5649 M -297 0 R D 17107 7762 M -297 0 R D +17107 9876 M -297 0 R D 17107 11989 M -297 0 R D 17107 1633 M -148 0 R D +17107 1845 M -148 0 R D 17107 2056 M -148 0 R D 17107 2267 M -148 0 R D +17107 2479 M -148 0 R D 17107 2690 M -148 0 R D 17107 2902 M -148 0 R D +17107 3113 M -148 0 R D 17107 3324 M -148 0 R D 17107 3747 M -148 0 R D +17107 3958 M -148 0 R D 17107 4170 M -148 0 R D 17107 4381 M -148 0 R D +17107 4592 M -148 0 R D 17107 4804 M -148 0 R D 17107 5015 M -148 0 R D +17107 5226 M -148 0 R D 17107 5438 M -148 0 R D 17107 5860 M -148 0 R D +17107 6072 M -148 0 R D 17107 6283 M -148 0 R D 17107 6494 M -148 0 R D +17107 6706 M -148 0 R D 17107 6917 M -148 0 R D 17107 7128 M -148 0 R D +17107 7340 M -148 0 R D 17107 7551 M -148 0 R D 17107 7974 M -148 0 R D +17107 8185 M -148 0 R D 17107 8396 M -148 0 R D 17107 8608 M -148 0 R D +17107 8819 M -148 0 R D 17107 9030 M -148 0 R D 17107 9242 M -148 0 R D +17107 9453 M -148 0 R D 17107 9664 M -148 0 R D 17107 10087 M -148 0 R D +17107 10298 M -148 0 R D 17107 10510 M -148 0 R D 17107 10721 M -148 0 R D +17107 10932 M -148 0 R D 17107 11144 M -148 0 R D 17107 11355 M -148 0 R D +17107 11566 M -148 0 R D 17107 11778 M -148 0 R D 20 setlinewidth +2242 8019 M 253 -235 R 620 289 R 619 810 R 619 699 R 620 278 R 619 -983 R +619 -1026 R 620 -1679 R 619 -1557 R 620 -369 R 619 164 R 619 1885 R +620 2010 R 619 189 R 619 -2838 R 620 1009 R 619 -29 R 620 -662 R 422 -4552 R +D 2421 7717 M 148 0 R -74 0 R 0 134 R -74 0 R 148 0 R D 3040 8004 M 149 0 R +-74 0 R 0 138 R -75 0 R 149 0 R D 3660 8805 M 148 0 R -74 0 R 0 155 R +-74 0 R 148 0 R D 4279 9496 M 149 0 R -75 0 R 0 173 R -74 0 R 149 0 R D +4898 9762 M 149 0 R -74 0 R 0 196 R -75 0 R 149 0 R D 5518 8767 M 148 0 R +-74 0 R 0 219 R -74 0 R 148 0 R D 6137 7731 M 149 0 R -75 0 R 0 241 R +-74 0 R 149 0 R D 6756 6042 M 149 0 R -74 0 R 0 259 R -75 0 R 149 0 R D +7376 4473 M 149 0 R -75 0 R 0 283 R -74 0 R 149 0 R D 7995 4083 M 149 0 R +-74 0 R 0 326 R -75 0 R 149 0 R D 8615 4213 M 148 0 R -74 0 R 0 395 R +-74 0 R 148 0 R D 9234 6033 M 149 0 R -75 0 R 0 524 R -74 0 R 149 0 R D +9853 7965 M 149 0 R -74 0 R 0 679 R -75 0 R 149 0 R D 10473 8049 M 148 0 R +-74 0 R 0 890 R -74 0 R 148 0 R D 11092 5071 M 149 0 R -75 0 R 0 1170 R +-74 0 R 149 0 R D 11712 5822 M 148 0 R -74 0 R 0 1686 R -74 0 R 148 0 R D +12331 5424 M 149 0 R -75 0 R 0 2423 R -74 0 R 149 0 R D 12950 4187 M 149 0 R +-74 0 R 0 3574 R -75 0 R 149 0 R D 5141 9531 M 0 267 R 267 0 R 0 -267 R +-267 0 R F +8907 7629 M 0 266 R 267 0 R 0 -266 R -267 0 R F +13862 4036 M 0 267 R 267 0 R 0 -267 R -267 0 R F +5275 9242 M 0 845 R D 3491 9664 M 3567 0 R D 5186 9242 M 177 0 R D +5186 10087 M 177 0 R D 3491 9575 M 0 178 R D 7058 9575 M 0 178 R D +9040 6917 M 0 1691 R D 7232 7762 M 3617 0 R D 8951 6917 M 178 0 R D +8951 8608 M 178 0 R D 7232 7673 M 0 178 R D 10849 7673 M 0 178 R D +13995 2902 M 0 2536 R D 10973 4170 M 6045 0 R D 13907 2902 M 177 0 R D +13907 5438 M 177 0 R D 10973 4081 M 0 177 R D 17018 4081 M 0 177 R D +%%PageTrailer +end +restore +showpage +%%PageResources: font Helvetica +%%Trailer +restore +%%Pages: 1 +%%DocumentNeededResources: font Helvetica +%%EOF diff --git a/feedback/papers/0506398/f18.ps b/feedback/papers/0506398/f18.ps new file mode 100644 index 0000000..b9f90d2 --- /dev/null +++ b/feedback/papers/0506398/f18.ps @@ -0,0 +1,568 @@ +%!PS-Adobe-3.0 +%%BoundingBox: 54 360 904 785 +%%Title: Graphics produced by IDL +%%For: phopkins@dhcp152-235.cfa.harvard.edu, +%% /Users/phopkins/Documents/lars_galaxies/plots/LF_massive +%%Creator: IDL Student Edition 6.0.3, Mac OS X (darwin ppc m32) +%%CreationDate: Mon Aug 29 04:02:27 2005 +%%DocumentData: Clean7bit +%%Requirements: color +%%LanguageLevel: 1 +%%PageOrder: Ascend +%%Pages: (atend) +%%DocumentNeededResources: (atend) +%%EndComments +%%BeginProlog +save +%+ prolog.ps -- Prolog for IDL generated PostScript files +%+ Copyright (c) 1988-2003 Research Systems, Inc. All Rights Reserved. +%v 4 +/$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C +{currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint +stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} +bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show +grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 +setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 +{[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 +100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 +{[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef +/ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} +ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont +exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica +findfont exch scalefont setfont (\267) show currentpoint grestore moveto} +bdef end 2.5 setmiterlimit +%%EndProlog +%%Page: 0 1 +%%PageRequirements: color +%%PageResources: (atend) +%%PageOrientation: Portrait +%%PageBoundingBox: 54 360 904 785 +%%BeginPageSetup +save +$IDL_DICT begin 54 360 translate 0.0283465 dup scale +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +%%EndPageSetup +15 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 1121 1422 M 14103 0 R D +2170 1422 M 0 265 R D gsave 2170 889 translate 0 0 M 1.01 dup scale +-308.339 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(5) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 4805 1422 M 0 265 R D +gsave 4805 889 translate 0 0 M 1.01 dup scale -308.339 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(6) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 7440 1422 M 0 265 R D +gsave 7440 889 translate 0 0 M 1.01 dup scale -308.339 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(7) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 10075 1422 M 0 265 R D +gsave 10075 889 translate 0 0 M 1.01 dup scale -308.339 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(8) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 12710 1422 M 0 265 R D +gsave 12710 889 translate 0 0 M 1.01 dup scale -308.339 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(9) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 1121 1422 M 0 132 R D 1377 1422 M 0 132 R D +1585 1422 M 0 132 R D 1762 1422 M 0 132 R D 1914 1422 M 0 132 R D +2049 1422 M 0 132 R D 2963 1422 M 0 132 R D 3427 1422 M 0 132 R D +3756 1422 M 0 132 R D 4012 1422 M 0 132 R D 4220 1422 M 0 132 R D +4397 1422 M 0 132 R D 4549 1422 M 0 132 R D 4684 1422 M 0 132 R D +5598 1422 M 0 132 R D 6062 1422 M 0 132 R D 6391 1422 M 0 132 R D +6647 1422 M 0 132 R D 6855 1422 M 0 132 R D 7032 1422 M 0 132 R D +7185 1422 M 0 132 R D 7319 1422 M 0 132 R D 8233 1422 M 0 132 R D +8697 1422 M 0 132 R D 9026 1422 M 0 132 R D 9282 1422 M 0 132 R D +9490 1422 M 0 132 R D 9667 1422 M 0 132 R D 9820 1422 M 0 132 R D +9954 1422 M 0 132 R D 10868 1422 M 0 132 R D 11332 1422 M 0 132 R D +11661 1422 M 0 132 R D 11917 1422 M 0 132 R D 12125 1422 M 0 132 R D +12302 1422 M 0 132 R D 12455 1422 M 0 132 R D 12589 1422 M 0 132 R D +13503 1422 M 0 132 R D 13967 1422 M 0 132 R D 14296 1422 M 0 132 R D +14552 1422 M 0 132 R D 14760 1422 M 0 132 R D 14937 1422 M 0 132 R D +15090 1422 M 0 132 R D 15224 1422 M 0 132 R D gsave 8173 427 translate 0 0 M +1.01 dup scale -2902.94 0 N +(All Active \(Type I & II\) M) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(BH) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( [M) show CP X -101.051 M +%%IncludeResource: font AvantGarde-Book +262.467 /AvantGarde-Book STDFONT +(O) show M X -58.3193 M +%%IncludeResource: font AvantGarde-Book +186.267 /AvantGarde-Book STDFONT +( \267) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(]) show grestore 1121 14645 M 14103 0 R D 2170 14645 M 0 -265 R D +4805 14645 M 0 -265 R D 7440 14645 M 0 -265 R D 10075 14645 M 0 -265 R D +12710 14645 M 0 -265 R D 1121 14645 M 0 -133 R D 1377 14645 M 0 -133 R D +1585 14645 M 0 -133 R D 1762 14645 M 0 -133 R D 1914 14645 M 0 -133 R D +2049 14645 M 0 -133 R D 2963 14645 M 0 -133 R D 3427 14645 M 0 -133 R D +3756 14645 M 0 -133 R D 4012 14645 M 0 -133 R D 4220 14645 M 0 -133 R D +4397 14645 M 0 -133 R D 4549 14645 M 0 -133 R D 4684 14645 M 0 -133 R D +5598 14645 M 0 -133 R D 6062 14645 M 0 -133 R D 6391 14645 M 0 -133 R D +6647 14645 M 0 -133 R D 6855 14645 M 0 -133 R D 7032 14645 M 0 -133 R D +7185 14645 M 0 -133 R D 7319 14645 M 0 -133 R D 8233 14645 M 0 -133 R D +8697 14645 M 0 -133 R D 9026 14645 M 0 -133 R D 9282 14645 M 0 -133 R D +9490 14645 M 0 -133 R D 9667 14645 M 0 -133 R D 9820 14645 M 0 -133 R D +9954 14645 M 0 -133 R D 10868 14645 M 0 -133 R D 11332 14645 M 0 -133 R D +11661 14645 M 0 -133 R D 11917 14645 M 0 -133 R D 12125 14645 M 0 -133 R D +12302 14645 M 0 -133 R D 12455 14645 M 0 -133 R D 12589 14645 M 0 -133 R D +13503 14645 M 0 -133 R D 13967 14645 M 0 -133 R D 14296 14645 M 0 -133 R D +14552 14645 M 0 -133 R D 14760 14645 M 0 -133 R D 14937 14645 M 0 -133 R D +15090 14645 M 0 -133 R D 15224 14645 M 0 -133 R D 1121 1422 M 0 13223 R D +1121 1422 M 282 0 R D gsave 1009 1422 translate 0 0 M 1.01 dup scale +-117.687 0 N +( ) show grestore 1121 3941 M 282 0 R D gsave 1009 3798 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 1121 6459 M 282 0 R D gsave 1009 6317 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 1121 8978 M 282 0 R D gsave 1009 8836 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 1121 11496 M 282 0 R D gsave 1009 11354 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 1121 14015 M 282 0 R D gsave 1009 13873 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 1121 2052 M 141 0 R D 1121 2681 M 141 0 R D 1121 3311 M +141 0 R D 1121 4570 M 141 0 R D 1121 5200 M 141 0 R D 1121 5830 M 141 0 R D +1121 7089 M 141 0 R D 1121 7719 M 141 0 R D 1121 8348 M 141 0 R D +1121 9607 M 141 0 R D 1121 10237 M 141 0 R D 1121 10867 M 141 0 R D +1121 12126 M 141 0 R D 1121 12756 M 141 0 R D 1121 13385 M 141 0 R D +1121 14645 M 141 0 R D gsave 555 8033 translate 0 0 M 90 rotate +1.01 dup scale -2575.77 0 N +(Probability \(Arbitrary Scale\)) show grestore 15224 1422 M 0 13223 R D +15224 1422 M -282 0 R D 15224 3941 M -282 0 R D 15224 6459 M -282 0 R D +15224 8978 M -282 0 R D 15224 11496 M -282 0 R D 15224 14015 M -282 0 R D +15224 2052 M -141 0 R D 15224 2681 M -141 0 R D 15224 3311 M -141 0 R D +15224 4570 M -141 0 R D 15224 5200 M -141 0 R D 15224 5830 M -141 0 R D +15224 7089 M -141 0 R D 15224 7719 M -141 0 R D 15224 8348 M -141 0 R D +15224 9607 M -141 0 R D 15224 10237 M -141 0 R D 15224 10867 M -141 0 R D +15224 12126 M -141 0 R D 15224 12756 M -141 0 R D 15224 13385 M -141 0 R D +15224 14645 M -141 0 R D 40 setlinewidth L2 1121 2347 M 150 190 R 235 366 R +234 446 R 235 528 R 234 612 R 235 696 R 234 771 R 235 838 R 234 888 R +235 918 R 234 925 R 235 905 R 234 858 R 235 782 R 234 678 R 235 551 R +234 403 R 235 242 R 234 71 R 235 -100 R 234 -266 R 235 -420 R 234 -556 R +235 -672 R 234 -762 R 235 -825 R 234 -863 R 235 -875 R 235 -864 R 234 -833 R +235 -786 R 234 -727 R 235 -660 R 234 -588 R 235 -515 R 234 -444 R 235 -375 R +234 -314 R 235 -257 R 234 -209 R 235 -166 R 234 -131 R 235 -101 R 234 -77 R +235 -58 R 234 -43 R 235 -32 R 234 -22 R 235 -17 R 234 -11 R 235 -8 R +234 -5 R 235 -4 R 234 -2 R 235 -2 R 234 -1 R 235 -1 R 235 0 R 234 0 R +235 -1 R 116 0 R D 20 setlinewidth 1.000 0.000 0.000 setrgbcolor +1121 13739 M 212 -1118 R 264 -1194 R 263 -1275 R 264 -1377 R 263 -1153 R +264 -969 R 263 -813 R 264 -685 R 263 -576 R 264 -486 R 263 -410 R 264 -346 R +263 -293 R 264 -248 R 263 -211 R 264 -179 R 263 -152 R 264 -129 R 263 -111 R +264 -95 R 263 -80 R 264 -70 R 263 -59 R 264 -51 R 263 -43 R 264 -37 R +263 -31 R 264 -26 R 263 -22 R 264 -18 R 263 -14 R 264 -12 R 263 -8 R +264 -7 R 263 -5 R 264 -4 R 263 -3 R 264 -2 R 263 -1 R 264 -1 R 263 -1 R +264 -1 R 263 0 R 264 0 R 263 0 R 264 -1 R 263 0 R 264 0 R 263 0 R 264 0 R +263 0 R 264 0 R 263 0 R 189 0 R D L0 1121 3178 M 212 167 R 264 239 R +263 213 R 264 144 R 263 154 R 264 167 R 263 179 R 264 193 R 263 208 R +264 223 R 263 239 R 264 256 R 263 275 R 264 292 R 263 310 R 264 328 R +263 343 R 264 357 R 263 367 R 264 371 R 263 368 R 264 354 R 263 329 R +264 290 R 263 233 R 264 161 R 263 73 R 264 -28 R 263 -136 R 264 -243 R +263 -344 R 264 -429 R 263 -496 R 264 -539 R 263 -562 R 264 -562 R 263 -548 R +264 -520 R 263 -484 R 264 -443 R 263 -402 R 264 -359 R 263 -319 R 264 -282 R +263 -248 R 264 -216 R 263 -189 R 264 -165 R 263 -143 R 264 -124 R 263 -108 R +264 -93 R 263 -81 R 189 -51 R D 0.000 0.000 0.000 setrgbcolor +gsave 10075 10867 translate 0 0 M 1.01 dup scale +(Full Model) show grestore 1.000 0.000 0.000 setrgbcolor +gsave 10075 10237 translate 0 0 M 1.01 dup scale +(Light-bulb/Exponential) show grestore gsave 11917 9607 translate 0 0 M +1.01 dup scale +(Model) show grestore L1 0.000 0.000 0.000 setrgbcolor 1121 1422 M 150 0 R +235 0 R 234 0 R 235 0 R 234 0 R 235 0 R 234 0 R 235 0 R 234 0 R 235 0 R +234 22 R 235 65 R 234 154 R 235 301 R 234 508 R 235 756 R 234 1013 R +235 1244 R 234 1410 R 235 1489 R 234 1467 R 235 1348 R 234 1142 R 235 872 R +234 563 R 235 239 R 234 -76 R 235 -363 R 235 -607 R 234 -799 R 235 -936 R +234 -1019 R 235 -1051 R 234 -1042 R 235 -996 R 234 -926 R 235 -838 R +234 -740 R 235 -639 R 234 -542 R 235 -450 R 234 -367 R 235 -294 R 234 -232 R +235 -179 R 234 -137 R 235 -102 R 234 -76 R 235 -55 R 234 -40 R 235 -28 R +234 -19 R 235 -14 R 234 -9 R 235 -6 R 234 -4 R 235 -2 R 235 -2 R 234 -1 R +235 -1 R 116 0 R D L3 1121 1422 M 150 0 R 235 0 R 234 0 R 235 0 R 234 0 R +235 0 R 234 0 R 235 0 R 234 0 R 235 0 R 234 2 R 235 7 R 234 24 R 235 66 R +234 149 R 235 290 R 234 494 R 235 755 R 234 1044 R 235 1315 R 234 1523 R +235 1623 R 234 1591 R 235 1423 R 234 1139 R 235 774 R 234 374 R 235 -23 R +235 -379 R 234 -673 R 235 -891 R 234 -1034 R 235 -1107 R 234 -1118 R +235 -1083 R 234 -1014 R 235 -921 R 234 -815 R 235 -706 R 234 -599 R +235 -497 R 234 -405 R 235 -325 R 234 -256 R 235 -198 R 234 -151 R 235 -113 R +234 -84 R 235 -61 R 234 -44 R 235 -31 R 234 -21 R 235 -15 R 234 -10 R +235 -7 R 234 -4 R 235 -3 R 235 -2 R 234 -1 R 235 -1 R 116 0 R D +40 setlinewidth L0 1121 1422 M 150 0 R 235 0 R 234 0 R 235 0 R 234 0 R +235 0 R 234 0 R 235 0 R 234 0 R 235 0 R 234 0 R 235 2 R 234 6 R 235 18 R +234 44 R 235 96 R 234 182 R 235 311 R 234 483 R 235 688 R 234 907 R +235 1114 R 234 1281 R 235 1381 R 234 1400 R 235 1329 R 234 1178 R 235 958 R +235 694 R 234 405 R 235 116 R 234 -157 R 235 -401 R 234 -604 R 235 -765 R +234 -880 R 235 -951 R 234 -982 R 235 -977 R 234 -945 R 235 -889 R 234 -816 R +235 -734 R 234 -647 R 235 -558 R 234 -474 R 235 -395 R 234 -323 R 235 -261 R +234 -208 R 235 -161 R 234 -125 R 235 -94 R 234 -71 R 235 -52 R 234 -37 R +235 -27 R 235 -19 R 234 -13 R 235 -9 R 116 -3 R D +1.000 0.000 0.000 setrgbcolor 6525 5200 M -2 18 R -3 18 R -6 17 R -8 16 R +-10 15 R -12 14 R -14 12 R -15 10 R -16 8 R -17 6 R -18 4 R -18 1 R -18 -1 R +-18 -4 R -17 -6 R -17 -8 R -15 -10 R -13 -12 R -12 -14 R -10 -15 R -8 -16 R +-6 -17 R -4 -18 R -1 -18 R 1 -18 R 4 -18 R 6 -17 R 8 -16 R 10 -15 R 12 -14 R +13 -12 R 15 -10 R 17 -8 R 17 -6 R 18 -4 R 18 -1 R 18 1 R 18 4 R 17 6 R +16 8 R 15 10 R 14 12 R 12 14 R 10 15 R 8 16 R 6 17 R 3 18 R 2 18 R F +7842 12126 M -1 18 R -4 18 R -5 17 R -8 16 R -11 15 R -12 14 R -13 12 R +-15 10 R -17 8 R -17 6 R -18 4 R -18 1 R -18 -1 R -18 -4 R -17 -6 R -16 -8 R +-15 -10 R -14 -12 R -12 -14 R -10 -15 R -8 -16 R -6 -17 R -3 -18 R -1 -18 R +1 -18 R 3 -18 R 6 -17 R 8 -16 R 10 -15 R 12 -14 R 14 -12 R 15 -10 R 16 -8 R +17 -6 R 18 -4 R 18 -1 R 18 1 R 18 4 R 17 6 R 17 8 R 15 10 R 13 12 R 12 14 R +11 15 R 8 16 R 5 17 R 4 18 R 1 18 R F +9160 14015 M -2 18 R -3 18 R -6 17 R -8 16 R -10 15 R -12 14 R -14 12 R +-15 10 R -16 8 R -17 6 R -18 3 R -18 2 R -18 -2 R -18 -3 R -17 -6 R -16 -8 R +-16 -10 R -13 -12 R -12 -14 R -10 -15 R -8 -16 R -6 -17 R -4 -18 R -1 -18 R +1 -18 R 4 -18 R 6 -17 R 8 -16 R 10 -16 R 12 -13 R 13 -12 R 16 -10 R 16 -8 R +17 -6 R 18 -4 R 18 -1 R 18 1 R 18 4 R 17 6 R 16 8 R 15 10 R 14 12 R 12 13 R +10 16 R 8 16 R 6 17 R 3 18 R 2 18 R F +9950 8978 M -1 18 R -4 18 R -5 17 R -8 16 R -11 15 R -11 14 R -14 12 R +-15 10 R -17 8 R -17 6 R -17 3 R -19 2 R -18 -2 R -18 -3 R -17 -6 R -16 -8 R +-15 -10 R -14 -12 R -12 -14 R -10 -15 R -8 -16 R -6 -17 R -3 -18 R -1 -18 R +1 -18 R 3 -18 R 6 -17 R 8 -17 R 10 -15 R 12 -13 R 14 -12 R 15 -10 R 16 -8 R +17 -6 R 18 -4 R 18 -1 R 19 1 R 17 4 R 17 6 R 17 8 R 15 10 R 14 12 R 11 13 R +11 15 R 8 17 R 5 17 R 4 18 R 1 18 R F +11268 3311 M -2 18 R -3 18 R -6 17 R -8 16 R -10 16 R -12 13 R -14 12 R +-15 10 R -16 8 R -17 6 R -18 4 R -18 1 R -18 -1 R -18 -4 R -17 -6 R -16 -8 R +-16 -10 R -13 -12 R -12 -13 R -10 -16 R -8 -16 R -6 -17 R -4 -18 R -1 -18 R +1 -18 R 4 -18 R 6 -17 R 8 -16 R 10 -15 R 12 -14 R 13 -12 R 16 -10 R 16 -8 R +17 -6 R 18 -3 R 18 -2 R 18 2 R 18 3 R 17 6 R 16 8 R 15 10 R 14 12 R 12 14 R +10 15 R 8 16 R 6 17 R 3 18 R 2 18 R F +12585 1422 M -1 18 R -4 18 R -5 17 R -8 17 R -11 15 R -11 13 R -14 12 R +-15 10 R -16 8 R -18 6 R -17 4 R -19 1 R -18 -1 R -17 -4 R -18 -6 R -16 -8 R +-15 -10 R -14 -12 R -12 -13 R -10 -15 R -8 -17 R -6 -17 R -3 -18 R -1 -18 R +277 0 R F +6525 5200 M -2 18 R -3 18 R -6 17 R -8 16 R -10 15 R -12 14 R -14 12 R +-15 10 R -16 8 R -17 6 R -18 4 R -18 1 R -18 -1 R -18 -4 R -17 -6 R -17 -8 R +-15 -10 R -13 -12 R -12 -14 R -10 -15 R -8 -16 R -6 -17 R -4 -18 R -1 -18 R +1 -18 R 4 -18 R 6 -17 R 8 -16 R 10 -15 R 12 -14 R 13 -12 R 15 -10 R 17 -8 R +17 -6 R 18 -4 R 18 -1 R 18 1 R 18 4 R 17 6 R 16 8 R 15 10 R 14 12 R 12 14 R +10 15 R 8 16 R 6 17 R 3 18 R 2 18 R F +7842 12126 M -1 18 R -4 18 R -5 17 R -8 16 R -11 15 R -12 14 R -13 12 R +-15 10 R -17 8 R -17 6 R -18 4 R -18 1 R -18 -1 R -18 -4 R -17 -6 R -16 -8 R +-15 -10 R -14 -12 R -12 -14 R -10 -15 R -8 -16 R -6 -17 R -3 -18 R -1 -18 R +1 -18 R 3 -18 R 6 -17 R 8 -16 R 10 -15 R 12 -14 R 14 -12 R 15 -10 R 16 -8 R +17 -6 R 18 -4 R 18 -1 R 18 1 R 18 4 R 17 6 R 17 8 R 15 10 R 13 12 R 12 14 R +11 15 R 8 16 R 5 17 R 4 18 R 1 18 R F +9160 14015 M -2 18 R -3 18 R -6 17 R -8 16 R -10 15 R -12 14 R -14 12 R +-15 10 R -16 8 R -17 6 R -18 3 R -18 2 R -18 -2 R -18 -3 R -17 -6 R -16 -8 R +-16 -10 R -13 -12 R -12 -14 R -10 -15 R -8 -16 R -6 -17 R -4 -18 R -1 -18 R +1 -18 R 4 -18 R 6 -17 R 8 -16 R 10 -16 R 12 -13 R 13 -12 R 16 -10 R 16 -8 R +17 -6 R 18 -4 R 18 -1 R 18 1 R 18 4 R 17 6 R 16 8 R 15 10 R 14 12 R 12 13 R +10 16 R 8 16 R 6 17 R 3 18 R 2 18 R F +9950 8978 M -1 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-13 R -10 -15 R -8 -17 R -6 -17 R -3 -18 R -1 -18 R +277 0 R F +20 setlinewidth 6386 3941 M 0 1259 R -527 0 R D 6236 3941 M 300 0 R D +5859 5050 M 0 300 R D 7703 11811 M 0 315 R -527 0 R D 7553 11811 M 300 0 R D +7176 11976 M 0 300 R D 9021 12756 M 0 1259 R -527 0 R D 8871 12756 M 300 0 R +D 8494 13865 M 0 300 R D 9811 8348 M 0 630 R -527 0 R D 9661 8348 M 300 0 R +D 9284 8828 M 0 300 R D 11129 2681 M 0 630 R -527 0 R D 10979 2681 M 300 0 R +D 10602 3161 M 0 300 R D 12446 1422 M -527 0 R 0 150 R D 6525 5200 M -2 18 R +-3 18 R -6 17 R -8 16 R -10 15 R -12 14 R -14 12 R -15 10 R -16 8 R -17 6 R +-18 4 R -18 1 R -18 -1 R -18 -4 R -17 -6 R -17 -8 R -15 -10 R -13 -12 R +-12 -14 R -10 -15 R -8 -16 R -6 -17 R -4 -18 R -1 -18 R 1 -18 R 4 -18 R +6 -17 R 8 -16 R 10 -15 R 12 -14 R 13 -12 R 15 -10 R 17 -8 R 17 -6 R 18 -4 R +18 -1 R 18 1 R 18 4 R 17 6 R 16 8 R 15 10 R 14 12 R 12 14 R 10 15 R 8 16 R +6 17 R 3 18 R 2 18 R F +7842 12126 M -1 18 R -4 18 R -5 17 R -8 16 R -11 15 R -12 14 R -13 12 R +-15 10 R -17 8 R -17 6 R -18 4 R -18 1 R -18 -1 R -18 -4 R -17 -6 R -16 -8 R +-15 -10 R -14 -12 R -12 -14 R -10 -15 R -8 -16 R -6 -17 R -3 -18 R -1 -18 R +1 -18 R 3 -18 R 6 -17 R 8 -16 R 10 -15 R 12 -14 R 14 -12 R 15 -10 R 16 -8 R +17 -6 R 18 -4 R 18 -1 R 18 1 R 18 4 R 17 6 R 17 8 R 15 10 R 13 12 R 12 14 R +11 15 R 8 16 R 5 17 R 4 18 R 1 18 R F +9160 14015 M -2 18 R -3 18 R -6 17 R -8 16 R -10 15 R -12 14 R -14 12 R +-15 10 R -16 8 R -17 6 R -18 3 R -18 2 R -18 -2 R -18 -3 R -17 -6 R -16 -8 R +-16 -10 R -13 -12 R -12 -14 R -10 -15 R -8 -16 R -6 -17 R -4 -18 R -1 -18 R +1 -18 R 4 -18 R 6 -17 R 8 -16 R 10 -16 R 12 -13 R 13 -12 R 16 -10 R 16 -8 R +17 -6 R 18 -4 R 18 -1 R 18 1 R 18 4 R 17 6 R 16 8 R 15 10 R 14 12 R 12 13 R +10 16 R 8 16 R 6 17 R 3 18 R 2 18 R F +9950 8978 M -1 18 R -4 18 R -5 17 R -8 16 R -11 15 R -11 14 R -14 12 R +-15 10 R -17 8 R -17 6 R -17 3 R -19 2 R -18 -2 R -18 -3 R -17 -6 R -16 -8 R +-15 -10 R -14 -12 R -12 -14 R -10 -15 R -8 -16 R -6 -17 R -3 -18 R -1 -18 R +1 -18 R 3 -18 R 6 -17 R 8 -17 R 10 -15 R 12 -13 R 14 -12 R 15 -10 R 16 -8 R +17 -6 R 18 -4 R 18 -1 R 19 1 R 17 4 R 17 6 R 17 8 R 15 10 R 14 12 R 11 13 R +11 15 R 8 17 R 5 17 R 4 18 R 1 18 R F +11268 3311 M -2 18 R -3 18 R -6 17 R -8 16 R -10 16 R -12 13 R -14 12 R +-15 10 R -16 8 R -17 6 R -18 4 R -18 1 R -18 -1 R -18 -4 R -17 -6 R -16 -8 R +-16 -10 R -13 -12 R -12 -13 R -10 -16 R -8 -16 R -6 -17 R -4 -18 R -1 -18 R +1 -18 R 4 -18 R 6 -17 R 8 -16 R 10 -15 R 12 -14 R 13 -12 R 16 -10 R 16 -8 R +17 -6 R 18 -3 R 18 -2 R 18 2 R 18 3 R 17 6 R 16 8 R 15 10 R 14 12 R 12 14 R +10 15 R 8 16 R 6 17 R 3 18 R 2 18 R F +12585 1422 M -1 18 R -4 18 R -5 17 R -8 17 R -11 15 R -11 13 R -14 12 R +-15 10 R -16 8 R -18 6 R -17 4 R -19 1 R -18 -1 R -17 -4 R -18 -6 R -16 -8 R +-15 -10 R -14 -12 R -12 -13 R -10 -15 R -8 -17 R -6 -17 R -3 -18 R -1 -18 R +277 0 R F +6386 5200 M 0 1259 R D 6386 5200 M 527 0 R D 6236 6459 M 300 0 R D +6913 5050 M 0 300 R D 7703 12126 M 0 315 R D 7703 12126 M 527 0 R D +7553 12441 M 300 0 R D 8230 11976 M 0 300 R D 9021 14015 M 0 629 R D +9021 14015 M 527 0 R D 9548 13865 M 0 300 R D 9811 8978 M 0 629 R D +9811 8978 M 527 0 R D 9661 9607 M 300 0 R D 10338 8828 M 0 300 R D +11129 3311 M 0 315 R D 11129 3311 M 527 0 R D 10979 3626 M 300 0 R D +11656 3161 M 0 300 R D 12446 1422 M 0 315 R D 12446 1422 M 527 0 R D +12296 1737 M 300 0 R D 12973 1422 M 0 150 R D 40 setlinewidth L2 +0.000 0.000 0.000 setrgbcolor 9609 13871 M 1998 0 R D +gsave 11940 13739 translate 0 0 M 1.05 dup scale +(All \(Type I & II\)) show grestore 20 setlinewidth L1 9609 13343 M 1998 0 R +D gsave 11940 13211 translate 0 0 M 1.05 dup scale +(L) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(O III) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( > 10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(6) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( L) show CP X -101.051 M +%%IncludeResource: font AvantGarde-Book +262.467 /AvantGarde-Book STDFONT +(O) show M X -58.3193 M +%%IncludeResource: font AvantGarde-Book +186.267 /AvantGarde-Book STDFONT +( \267) show +%%IncludeResource: font Helvetica +186.267 /Helvetica STDFONT grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT L3 9609 12815 M 1998 0 R D +gsave 11940 12683 translate 0 0 M 1.05 dup scale +( + ) show +%%IncludeResource: font Symbol +423.333 /Symbol STDFONT +(s) show +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( > 70 km s) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(-1) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 40 setlinewidth L0 9609 12287 M 1998 0 R D +gsave 11940 12155 translate 0 0 M 1.05 dup scale +( + L) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(O III) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(-weighted) show grestore gsave 1585 13385 translate 0 0 M 1.2 dup scale +(z < 0.3) show grestore 15 setlinewidth 15449 1422 M 14103 0 R D +17275 1422 M 0 265 R D gsave 17275 889 translate 0 0 M 1.01 dup scale +-308.339 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(5) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 19887 1422 M 0 265 R D +gsave 19887 889 translate 0 0 M 1.01 dup scale -308.339 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(6) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 22500 1422 M 0 265 R D +gsave 22500 889 translate 0 0 M 1.01 dup scale -308.339 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(7) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 25113 1422 M 0 265 R D +gsave 25113 889 translate 0 0 M 1.01 dup scale -308.339 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(8) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 27726 1422 M 0 265 R D +gsave 27726 889 translate 0 0 M 1.01 dup scale -308.339 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(9) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 15449 1422 M 0 132 R D 15909 1422 M 0 132 R D +16235 1422 M 0 132 R D 16488 1422 M 0 132 R D 16695 1422 M 0 132 R D +16870 1422 M 0 132 R D 17022 1422 M 0 132 R D 17155 1422 M 0 132 R D +18061 1422 M 0 132 R D 18521 1422 M 0 132 R D 18848 1422 M 0 132 R D +19101 1422 M 0 132 R D 19308 1422 M 0 132 R D 19483 1422 M 0 132 R D +19634 1422 M 0 132 R D 19768 1422 M 0 132 R D 20674 1422 M 0 132 R D +21134 1422 M 0 132 R D 21460 1422 M 0 132 R D 21714 1422 M 0 132 R D +21921 1422 M 0 132 R D 22095 1422 M 0 132 R D 22247 1422 M 0 132 R D +22381 1422 M 0 132 R D 23287 1422 M 0 132 R D 23747 1422 M 0 132 R D +24073 1422 M 0 132 R D 24326 1422 M 0 132 R D 24533 1422 M 0 132 R D +24708 1422 M 0 132 R D 24860 1422 M 0 132 R D 24993 1422 M 0 132 R D +25899 1422 M 0 132 R D 26359 1422 M 0 132 R D 26686 1422 M 0 132 R D +26939 1422 M 0 132 R D 27146 1422 M 0 132 R D 27321 1422 M 0 132 R D +27472 1422 M 0 132 R D 27606 1422 M 0 132 R D 28512 1422 M 0 132 R D +28972 1422 M 0 132 R D 29299 1422 M 0 132 R D 29552 1422 M 0 132 R D +gsave 22500 427 translate 0 0 M 1.01 dup scale -2538.45 0 N +(Active Broad-Line M) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(BH) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( [M) show CP X -101.051 M +%%IncludeResource: font AvantGarde-Book +262.467 /AvantGarde-Book STDFONT +(O) show M X -58.3193 M +%%IncludeResource: font AvantGarde-Book +186.267 /AvantGarde-Book STDFONT +( \267) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(]) show grestore 15449 14645 M 14103 0 R D 17275 14645 M 0 -265 R D +19887 14645 M 0 -265 R D 22500 14645 M 0 -265 R D 25113 14645 M 0 -265 R D +27726 14645 M 0 -265 R D 15449 14645 M 0 -133 R D 15909 14645 M 0 -133 R D +16235 14645 M 0 -133 R D 16488 14645 M 0 -133 R D 16695 14645 M 0 -133 R D +16870 14645 M 0 -133 R D 17022 14645 M 0 -133 R D 17155 14645 M 0 -133 R D +18061 14645 M 0 -133 R D 18521 14645 M 0 -133 R D 18848 14645 M 0 -133 R D +19101 14645 M 0 -133 R D 19308 14645 M 0 -133 R D 19483 14645 M 0 -133 R D +19634 14645 M 0 -133 R D 19768 14645 M 0 -133 R D 20674 14645 M 0 -133 R D +21134 14645 M 0 -133 R D 21460 14645 M 0 -133 R D 21714 14645 M 0 -133 R D +21921 14645 M 0 -133 R D 22095 14645 M 0 -133 R D 22247 14645 M 0 -133 R D +22381 14645 M 0 -133 R D 23287 14645 M 0 -133 R D 23747 14645 M 0 -133 R D +24073 14645 M 0 -133 R D 24326 14645 M 0 -133 R D 24533 14645 M 0 -133 R D +24708 14645 M 0 -133 R D 24860 14645 M 0 -133 R D 24993 14645 M 0 -133 R D +25899 14645 M 0 -133 R D 26359 14645 M 0 -133 R D 26686 14645 M 0 -133 R D +26939 14645 M 0 -133 R D 27146 14645 M 0 -133 R D 27321 14645 M 0 -133 R D +27472 14645 M 0 -133 R D 27606 14645 M 0 -133 R D 28512 14645 M 0 -133 R D +28972 14645 M 0 -133 R D 29299 14645 M 0 -133 R D 29552 14645 M 0 -133 R D +15449 1422 M 0 13223 R D 15449 1422 M 282 0 R D +gsave 15336 1422 translate 0 0 M 1.01 dup scale -117.687 0 N +( ) show grestore 15449 3941 M 282 0 R D gsave 15336 3798 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 15449 6459 M 282 0 R D gsave 15336 6317 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 15449 8978 M 282 0 R D gsave 15336 8836 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 15449 11496 M 282 0 R D gsave 15336 11354 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 15449 14015 M 282 0 R D gsave 15336 13873 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 15449 2052 M 141 0 R D 15449 2681 M 141 0 R D 15449 3311 M +141 0 R D 15449 4570 M 141 0 R D 15449 5200 M 141 0 R D 15449 5830 M 141 0 R +D 15449 7089 M 141 0 R D 15449 7719 M 141 0 R D 15449 8348 M 141 0 R D +15449 9607 M 141 0 R D 15449 10237 M 141 0 R D 15449 10867 M 141 0 R D +15449 12126 M 141 0 R D 15449 12756 M 141 0 R D 15449 13385 M 141 0 R D +15449 14645 M 141 0 R D 29552 1422 M 0 13223 R D 29552 1422 M -282 0 R D +29552 3941 M -282 0 R D 29552 6459 M -282 0 R D 29552 8978 M -282 0 R D +29552 11496 M -282 0 R D 29552 14015 M -282 0 R D 29552 2052 M -141 0 R D +29552 2681 M -141 0 R D 29552 3311 M -141 0 R D 29552 4570 M -141 0 R D +29552 5200 M -141 0 R D 29552 5830 M -141 0 R D 29552 7089 M -141 0 R D +29552 7719 M -141 0 R D 29552 8348 M -141 0 R D 29552 9607 M -141 0 R D +29552 10237 M -141 0 R D 29552 10867 M -141 0 R D 29552 12126 M -141 0 R D +29552 12756 M -141 0 R D 29552 13385 M -141 0 R D 29552 14645 M -141 0 R D +40 setlinewidth 15448 1450 M 94 4 R 261 14 R 262 19 R 261 28 R 261 37 R +261 50 R 262 66 R 261 86 R 261 112 R 262 143 R 261 180 R 261 223 R 261 274 R +262 330 R 261 394 R 261 463 R 261 537 R 262 611 R 261 687 R 261 759 R +261 826 R 262 883 R 261 926 R 261 954 R 262 960 R 261 945 R 261 906 R +261 837 R 262 311 R 261 -159 R 261 -573 R 261 -932 R 262 -1236 R 261 -1487 R +261 -1682 R 262 -1397 R 261 -1145 R 261 -924 R 261 -737 R 262 -580 R +261 -450 R 261 -344 R 261 -261 R 262 -195 R 261 -143 R 261 -105 R 261 -75 R +262 -53 R 261 -37 R 261 -26 R 262 -18 R 261 -12 R 261 -7 R 261 -6 R 162 -2 R +D 20 setlinewidth L1 15448 1472 M 94 7 R 261 25 R 262 36 R 261 49 R 261 67 R +261 90 R 262 120 R 261 156 R 261 203 R 262 258 R 261 325 R 261 403 R +261 495 R 262 598 R 261 712 R 261 837 R 261 969 R 262 1106 R 261 1241 R +261 1373 R 261 1493 R 262 1085 R 261 663 R 261 232 R 262 -202 R 261 -635 R +261 -1061 R 261 -1476 R 262 -1364 R 261 -1239 R 261 -1107 R 261 -975 R +262 -845 R 261 -722 R 261 -608 R 262 -505 R 261 -414 R 261 -334 R 261 -267 R +262 -209 R 261 -163 R 261 -125 R 261 -94 R 262 -70 R 261 -52 R 261 -38 R +261 -27 R 262 -19 R 261 -14 R 261 -9 R 262 -6 R 261 -5 R 261 -3 R 261 -2 R +162 -1 R D L2 15448 1446 M 94 4 R 261 13 R 262 17 R 261 24 R 261 33 R +261 44 R 262 59 R 261 77 R 261 99 R 262 127 R 261 160 R 261 198 R 261 243 R +262 293 R 261 350 R 261 411 R 261 476 R 262 543 R 261 609 R 261 675 R +261 733 R 262 783 R 261 823 R 261 846 R 262 852 R 261 839 R 261 805 R +261 746 R 262 668 R 261 569 R 261 450 R 261 -73 R 262 -511 R 261 -870 R +261 -1157 R 262 -1376 R 261 -1536 R 261 -1641 R 261 -1309 R 262 -1029 R +261 -799 R 261 -612 R 261 -463 R 262 -345 R 261 -255 R 261 -185 R 261 -133 R +262 -95 R 261 -66 R 261 -46 R 262 -31 R 261 -21 R 261 -14 R 261 -10 R +162 -4 R D 40 setlinewidth L0 16408 13871 M 1998 0 R D +gsave 18739 13739 translate 0 0 M 1.05 dup scale +(All \(Type I\)) show grestore 20 setlinewidth L2 16408 13343 M 1998 0 R D +gsave 18739 13211 translate 0 0 M 1.05 dup scale +(+ 1) show +%%IncludeResource: font Symbol +423.333 /Symbol STDFONT +(s) show +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT grestore L1 16408 12815 M 1998 0 R D +gsave 18739 12683 translate 0 0 M 1.05 dup scale +(-- 1) show +%%IncludeResource: font Symbol +423.333 /Symbol STDFONT +(s) show +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT grestore L0 1.000 0.000 0.000 setrgbcolor +16081 14644 M 103 -636 R 261 -1387 R 262 -1194 R 261 -1275 R 261 -1377 R +261 -1153 R 262 -969 R 261 -813 R 261 -685 R 261 -576 R 262 -486 R +261 -410 R 261 -346 R 262 -293 R 261 -248 R 261 -211 R 261 -179 R 262 -152 R +261 -129 R 261 -111 R 261 -95 R 262 -80 R 261 -70 R 261 -59 R 261 -51 R +262 -43 R 261 -37 R 261 -31 R 262 -26 R 261 -22 R 261 -18 R 261 -14 R +262 -12 R 261 -8 R 261 -7 R 261 -5 R 262 -4 R 261 -3 R 261 -2 R 262 -1 R +261 -1 R 261 -1 R 261 -1 R 262 0 R 261 0 R 261 0 R 261 -1 R 262 0 R 261 0 R +261 0 R 261 0 R 262 0 R 42 0 R D 0.000 0.514 1.000 setrgbcolor 15448 5319 M +213 329 R 262 460 R 261 528 R 261 605 R 262 696 R 261 601 R 261 377 R +261 391 R 262 400 R 261 404 R 261 401 R 261 390 R 262 366 R 261 329 R +261 276 R 262 206 R 261 120 R 261 17 R 261 -97 R 262 -221 R 261 -345 R +261 -464 R 261 -571 R 262 -661 R 261 -729 R 261 -773 R 261 -794 R 262 -791 R +261 -767 R 261 -724 R 262 -667 R 261 -599 R 261 -523 R 261 -447 R 262 -372 R +261 -301 R 261 -239 R 261 -186 R 262 -142 R 261 -106 R 261 -78 R 262 -57 R +261 -41 R 261 -29 R 261 -21 R 262 -14 R 261 -10 R 261 -8 R 261 -5 R 262 -3 R +261 -2 R 261 -2 R 261 -1 R 262 -1 R 42 -1 R D 0.000 0.000 0.000 setrgbcolor +gsave 25113 10867 translate 0 0 M 1.01 dup scale +(Full Model) show grestore 1.000 0.000 0.000 setrgbcolor +gsave 25113 10237 translate 0 0 M 1.01 dup scale +(Light-bulb) show grestore gsave 25320 9607 translate 0 0 M 1.01 dup scale +(+ Standard Torus) show grestore 0.000 0.514 1.000 setrgbcolor +gsave 25113 8978 translate 0 0 M 1.01 dup scale +(Light-bulb) show grestore gsave 25320 8348 translate 0 0 M 1.01 dup scale +(+ Receding Torus) show grestore +%%PageTrailer +end +restore +showpage +%%PageResources: font Helvetica +%%+ font Symbol +%%+ font AvantGarde-Book +%%Trailer +restore +%%Pages: 1 +%%DocumentNeededResources: font Helvetica +%%+ font Symbol +%%+ font AvantGarde-Book +%%EOF diff --git a/feedback/papers/0506398/f19.ps b/feedback/papers/0506398/f19.ps new file mode 100644 index 0000000..b717fbc --- /dev/null +++ b/feedback/papers/0506398/f19.ps @@ -0,0 +1,792 @@ +%!PS-Adobe-3.0 +%%BoundingBox: 54 360 558 720 +%%Title: Graphics produced by IDL +%%For: phopkins@dhcp152-85.cfa.harvard.edu, +%% /Users/phopkins/Documents/lars_galaxies/plots/high_z +%%Creator: IDL Student Edition 6.0, Mac OS X (darwin ppc m32) +%%CreationDate: Mon Apr 11 12:07:33 2005 +%%DocumentData: Clean7bit +%%Requirements: color +%%LanguageLevel: 1 +%%PageOrder: Ascend +%%Pages: (atend) +%%DocumentNeededResources: (atend) +%%EndComments +%%BeginProlog +save +%+ prolog.ps -- Prolog for IDL generated PostScript files +%+ Copyright (c) 1988-2003 Research Systems, Inc. All Rights Reserved. +%v 4 +/$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C +{currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint +stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} +bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show +grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 +setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 +{[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 +100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 +{[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef +/ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} +ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont +exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica +findfont exch scalefont setfont (\267) show currentpoint grestore moveto} +bdef end 2.5 setmiterlimit +%%EndProlog +%%Page: 0 1 +%%PageRequirements: color +%%PageResources: (atend) +%%PageOrientation: Portrait +%%PageBoundingBox: 54 360 558 720 +%%BeginPageSetup +save +$IDL_DICT begin 54 360 translate 0.0283465 dup scale +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +%%EndPageSetup +15 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 1333 9701 M 7557 0 R D +1333 9701 M 0 57 R D gsave 1333 9173 translate 0 0 M 1.0005 dup scale +-58.8433 0 N +( ) show grestore 3090 9701 M 0 57 R D gsave 3090 9173 translate 0 0 M +1.0005 dup scale -58.8433 0 N +( ) show grestore 4847 9701 M 0 57 R D gsave 4847 9173 translate 0 0 M +1.0005 dup scale -58.8433 0 N +( ) show grestore 6604 9701 M 0 57 R D gsave 6604 9173 translate 0 0 M +1.0005 dup scale -58.8433 0 N +( ) show grestore 8361 9701 M 0 57 R D gsave 8361 9173 translate 0 0 M +1.0005 dup scale -58.8433 0 N +( ) show grestore 1862 9701 M 0 28 R D 2171 9701 M 0 28 R D 2391 9701 M +0 28 R D 2561 9701 M 0 28 R D 2700 9701 M 0 28 R D 2818 9701 M 0 28 R D +2920 9701 M 0 28 R D 3009 9701 M 0 28 R D 3619 9701 M 0 28 R D 3928 9701 M +0 28 R D 4148 9701 M 0 28 R D 4318 9701 M 0 28 R D 4457 9701 M 0 28 R D +4575 9701 M 0 28 R D 4677 9701 M 0 28 R D 4767 9701 M 0 28 R D 5376 9701 M +0 28 R D 5685 9701 M 0 28 R D 5905 9701 M 0 28 R D 6075 9701 M 0 28 R D +6214 9701 M 0 28 R D 6332 9701 M 0 28 R D 6434 9701 M 0 28 R D 6524 9701 M +0 28 R D 7133 9701 M 0 28 R D 7442 9701 M 0 28 R D 7662 9701 M 0 28 R D +7832 9701 M 0 28 R D 7971 9701 M 0 28 R D 8089 9701 M 0 28 R D 8191 9701 M +0 28 R D 8281 9701 M 0 28 R D 8890 9701 M 0 28 R D +gsave 5111 8715 translate 0 0 M 1.0005 dup scale -58.8433 0 N +( ) show grestore 1333 12524 M 7557 0 R D 1333 12524 M 0 -56 R D +3090 12524 M 0 -56 R D 4847 12524 M 0 -56 R D 6604 12524 M 0 -56 R D +8361 12524 M 0 -56 R D 1862 12524 M 0 -28 R D 2171 12524 M 0 -28 R D +2391 12524 M 0 -28 R D 2561 12524 M 0 -28 R D 2700 12524 M 0 -28 R D +2818 12524 M 0 -28 R D 2920 12524 M 0 -28 R D 3009 12524 M 0 -28 R D +3619 12524 M 0 -28 R D 3928 12524 M 0 -28 R D 4148 12524 M 0 -28 R D +4318 12524 M 0 -28 R D 4457 12524 M 0 -28 R D 4575 12524 M 0 -28 R D +4677 12524 M 0 -28 R D 4767 12524 M 0 -28 R D 5376 12524 M 0 -28 R D +5685 12524 M 0 -28 R D 5905 12524 M 0 -28 R D 6075 12524 M 0 -28 R D +6214 12524 M 0 -28 R D 6332 12524 M 0 -28 R D 6434 12524 M 0 -28 R D +6524 12524 M 0 -28 R D 7133 12524 M 0 -28 R D 7442 12524 M 0 -28 R D +7662 12524 M 0 -28 R D 7832 12524 M 0 -28 R D 7971 12524 M 0 -28 R D +8089 12524 M 0 -28 R D 8191 12524 M 0 -28 R D 8281 12524 M 0 -28 R D +8890 12524 M 0 -28 R D 1333 9701 M 0 2823 R D 1333 9701 M 151 0 R D +gsave 1222 9701 translate 0 0 M 1.0005 dup scale -117.687 0 N +( ) show grestore 1333 10642 M 151 0 R D gsave 1222 10501 translate 0 0 M +1.0005 dup scale -117.687 0 N +( ) show grestore 1333 11583 M 151 0 R D gsave 1222 11442 translate 0 0 M +1.0005 dup scale -117.687 0 N +( ) show grestore 1333 12524 M 151 0 R D gsave 1222 12277 translate 0 0 M +1.0005 dup scale -117.687 0 N +( ) show grestore 1333 9984 M 75 0 R D 1333 10150 M 75 0 R D 1333 10268 M +75 0 R D 1333 10359 M 75 0 R D 1333 10433 M 75 0 R D 1333 10496 M 75 0 R D +1333 10551 M 75 0 R D 1333 10599 M 75 0 R D 1333 10925 M 75 0 R D +1333 11091 M 75 0 R D 1333 11209 M 75 0 R D 1333 11300 M 75 0 R D +1333 11374 M 75 0 R D 1333 11437 M 75 0 R D 1333 11492 M 75 0 R D +1333 11540 M 75 0 R D 1333 11866 M 75 0 R D 1333 12032 M 75 0 R D +1333 12150 M 75 0 R D 1333 12241 M 75 0 R D 1333 12315 M 75 0 R D +1333 12378 M 75 0 R D 1333 12433 M 75 0 R D 1333 12481 M 75 0 R D +gsave 772 11113 translate 0 0 M 90 rotate 1.0005 dup scale -58.8433 0 N +( ) show grestore 8890 9701 M 0 2823 R D 8890 9701 M -151 0 R D 8890 10642 M +-151 0 R D 8890 11583 M -151 0 R D 8890 12524 M -151 0 R D 8890 9984 M +-75 0 R D 8890 10150 M -75 0 R D 8890 10268 M -75 0 R D 8890 10359 M -75 0 R +D 8890 10433 M -75 0 R D 8890 10496 M -75 0 R D 8890 10551 M -75 0 R D +8890 10599 M -75 0 R D 8890 10925 M -75 0 R D 8890 11091 M -75 0 R D +8890 11209 M -75 0 R D 8890 11300 M -75 0 R D 8890 11374 M -75 0 R D +8890 11437 M -75 0 R D 8890 11492 M -75 0 R D 8890 11540 M -75 0 R D +8890 11866 M -75 0 R D 8890 12032 M -75 0 R D 8890 12150 M -75 0 R D +8890 12241 M -75 0 R D 8890 12315 M -75 0 R D 8890 12378 M -75 0 R D +8890 12433 M -75 0 R D 8890 12481 M -75 0 R D 40 setlinewidth 1333 9701 M +251 0 R 0 698 R 188 0 R 251 0 R 0 22 R 188 0 R 251 0 R 0 768 R 189 0 R +250 0 R 0 340 R 189 0 R 251 0 R 0 18 R 188 0 R 251 0 R 0 -174 R 188 0 R +251 0 R 0 203 R 189 0 R 250 0 R 0 -294 R 189 0 R 251 0 R 0 114 R 188 0 R +251 0 R 0 -7 R 189 0 R 250 0 R 0 -67 R 189 0 R 251 0 R 0 -389 R 188 0 R +251 0 R 0 158 R 188 0 R 251 0 R 0 564 R 189 0 R 250 0 R 0 158 R 189 0 R +251 0 R 0 -589 R 188 0 R 251 0 R 0 -1523 R D 20 setlinewidth L1 1333 9701 M +251 0 R 0 1047 R 188 0 R 251 0 R 0 22 R 188 0 R 251 0 R 0 768 R 189 0 R +250 0 R 0 340 R 189 0 R 251 0 R 0 18 R 188 0 R 251 0 R 0 -174 R 188 0 R +251 0 R 189 0 R 250 0 R 0 -605 R 189 0 R 251 0 R 0 -154 R 188 0 R 251 0 R +0 -188 R 189 0 R 250 0 R 0 138 R 189 0 R 251 0 R 0 -374 R 188 0 R 251 0 R +0 236 R 188 0 R 251 0 R 0 -421 R 189 0 R 250 0 R 0 846 R 189 0 R 251 0 R +0 -129 R 188 0 R 251 0 R 0 -1370 R D L2 1333 11408 M 251 0 R 0 -360 R +188 0 R 251 0 R 0 -74 R 188 0 R 251 0 R 0 485 R 189 0 R 250 0 R 0 -577 R +189 0 R 251 0 R 0 374 R 188 0 R 251 0 R 0 218 R 188 0 R 251 0 R 0 -426 R +189 0 R 250 0 R 0 254 R 189 0 R 251 0 R 0 115 R 188 0 R 251 0 R 0 -8 R +189 0 R 250 0 R 0 -66 R 189 0 R 251 0 R 0 -390 R 188 0 R 251 0 R 0 159 R +188 0 R 251 0 R 0 564 R 189 0 R 250 0 R 0 158 R 189 0 R 251 0 R 0 -590 R +188 0 R 251 0 R 0 -1543 R D gsave 1472 11866 translate 0 0 M 1.1 dup scale +(Entire Simulation) show grestore 15 setlinewidth L0 9779 9701 M 7557 0 R D +9779 9701 M 0 57 R D gsave 9779 9173 translate 0 0 M 1.0005 dup scale +-58.8433 0 N +( ) show grestore 11668 9701 M 0 57 R D gsave 11668 9173 translate 0 0 M +1.0005 dup scale -58.8433 0 N +( ) show grestore 13557 9701 M 0 57 R D gsave 13557 9173 translate 0 0 M +1.0005 dup scale -58.8433 0 N +( ) show grestore 15447 9701 M 0 57 R D gsave 15447 9173 translate 0 0 M +1.0005 dup scale -58.8433 0 N +( ) show grestore 17336 9701 M 0 57 R D gsave 17336 9173 translate 0 0 M +1.0005 dup scale -58.8433 0 N +( ) show grestore 10347 9701 M 0 28 R D 10680 9701 M 0 28 R D 10916 9701 M +0 28 R D 11099 9701 M 0 28 R D 11249 9701 M 0 28 R D 11375 9701 M 0 28 R D +11485 9701 M 0 28 R D 11581 9701 M 0 28 R D 12237 9701 M 0 28 R D +12569 9701 M 0 28 R D 12805 9701 M 0 28 R D 12988 9701 M 0 28 R D +13138 9701 M 0 28 R D 13265 9701 M 0 28 R D 13374 9701 M 0 28 R D +13471 9701 M 0 28 R D 14126 9701 M 0 28 R D 14459 9701 M 0 28 R D +14695 9701 M 0 28 R D 14878 9701 M 0 28 R D 15027 9701 M 0 28 R D +15154 9701 M 0 28 R D 15263 9701 M 0 28 R D 15360 9701 M 0 28 R D +16015 9701 M 0 28 R D 16348 9701 M 0 28 R D 16584 9701 M 0 28 R D +16767 9701 M 0 28 R D 16917 9701 M 0 28 R D 17043 9701 M 0 28 R D +17153 9701 M 0 28 R D 17249 9701 M 0 28 R D gsave 13557 8715 translate 0 0 M +1.0005 dup scale -58.8433 0 N +( ) show grestore 9779 12524 M 7557 0 R D 9779 12524 M 0 -56 R D +11668 12524 M 0 -56 R D 13557 12524 M 0 -56 R D 15447 12524 M 0 -56 R D +17336 12524 M 0 -56 R D 10347 12524 M 0 -28 R D 10680 12524 M 0 -28 R D +10916 12524 M 0 -28 R D 11099 12524 M 0 -28 R D 11249 12524 M 0 -28 R D +11375 12524 M 0 -28 R D 11485 12524 M 0 -28 R D 11581 12524 M 0 -28 R D +12237 12524 M 0 -28 R D 12569 12524 M 0 -28 R D 12805 12524 M 0 -28 R D +12988 12524 M 0 -28 R D 13138 12524 M 0 -28 R D 13265 12524 M 0 -28 R D +13374 12524 M 0 -28 R D 13471 12524 M 0 -28 R D 14126 12524 M 0 -28 R D +14459 12524 M 0 -28 R D 14695 12524 M 0 -28 R D 14878 12524 M 0 -28 R D +15027 12524 M 0 -28 R D 15154 12524 M 0 -28 R D 15263 12524 M 0 -28 R D +15360 12524 M 0 -28 R D 16015 12524 M 0 -28 R D 16348 12524 M 0 -28 R D +16584 12524 M 0 -28 R D 16767 12524 M 0 -28 R D 16917 12524 M 0 -28 R D +17043 12524 M 0 -28 R D 17153 12524 M 0 -28 R D 17249 12524 M 0 -28 R D +9779 9701 M 0 2823 R D 9779 9701 M 151 0 R D gsave 9667 9701 translate 0 0 M +1.0005 dup scale -117.687 0 N +( ) show grestore 9779 10642 M 151 0 R D gsave 9667 10501 translate 0 0 M +1.0005 dup scale -117.687 0 N +( ) show grestore 9779 11583 M 151 0 R D gsave 9667 11442 translate 0 0 M +1.0005 dup scale -117.687 0 N +( ) show grestore 9779 12524 M 151 0 R D gsave 9667 12277 translate 0 0 M +1.0005 dup scale -117.687 0 N +( ) show grestore 9779 9984 M 75 0 R D 9779 10150 M 75 0 R D 9779 10268 M +75 0 R D 9779 10359 M 75 0 R D 9779 10433 M 75 0 R D 9779 10496 M 75 0 R D +9779 10551 M 75 0 R D 9779 10599 M 75 0 R D 9779 10925 M 75 0 R D +9779 11091 M 75 0 R D 9779 11209 M 75 0 R D 9779 11300 M 75 0 R D +9779 11374 M 75 0 R D 9779 11437 M 75 0 R D 9779 11492 M 75 0 R D +9779 11540 M 75 0 R D 9779 11866 M 75 0 R D 9779 12032 M 75 0 R D +9779 12150 M 75 0 R D 9779 12241 M 75 0 R D 9779 12315 M 75 0 R D +9779 12378 M 75 0 R D 9779 12433 M 75 0 R D 9779 12481 M 75 0 R D +gsave 9217 11113 translate 0 0 M 90 rotate 1.0005 dup scale -58.8433 0 N +( ) show grestore 17336 9701 M 0 2823 R D 17336 9701 M -151 0 R D +17336 10642 M -151 0 R D 17336 11583 M -151 0 R D 17336 12524 M -151 0 R D +17336 9984 M -76 0 R D 17336 10150 M -76 0 R D 17336 10268 M -76 0 R D +17336 10359 M -76 0 R D 17336 10433 M -76 0 R D 17336 10496 M -76 0 R D +17336 10551 M -76 0 R D 17336 10599 M -76 0 R D 17336 10925 M -76 0 R D +17336 11091 M -76 0 R D 17336 11209 M -76 0 R D 17336 11300 M -76 0 R D +17336 11374 M -76 0 R D 17336 11437 M -76 0 R D 17336 11492 M -76 0 R D +17336 11540 M -76 0 R D 17336 11866 M -76 0 R D 17336 12032 M -76 0 R D +17336 12150 M -76 0 R D 17336 12241 M -76 0 R D 17336 12315 M -76 0 R D +17336 12378 M -76 0 R D 17336 12433 M -76 0 R D 17336 12481 M -76 0 R D +40 setlinewidth 9779 9701 M 210 0 R 167 0 R 211 0 R 0 1444 R 167 0 R 211 0 R +0 -12 R 167 0 R 211 0 R 0 -377 R 167 0 R 210 0 R 0 -108 R 168 0 R 210 0 R +0 367 R 168 0 R 210 0 R 0 89 R 168 0 R 210 0 R 0 -24 R 167 0 R 211 0 R +0 -1 R 167 0 R 211 0 R 0 -87 R 167 0 R 211 0 R 0 183 R 167 0 R 211 0 R +0 -230 R 167 0 R 210 0 R 0 50 R 168 0 R 210 0 R 0 853 R 168 0 R 210 0 R +0 -97 R 168 0 R 210 0 R 0 -656 R 167 0 R 211 0 R 0 960 R 167 0 R 211 0 R +0 -2354 R 167 0 R 211 0 R 167 0 R D 20 setlinewidth L1 9779 9701 M 210 0 R +167 0 R 211 0 R 167 0 R 211 0 R 167 0 R 211 0 R 167 0 R 210 0 R 168 0 R +210 0 R 168 0 R 210 0 R 168 0 R 210 0 R 167 0 R 211 0 R 167 0 R 211 0 R +167 0 R 211 0 R 167 0 R 211 0 R 167 0 R 210 0 R 168 0 R 210 0 R 168 0 R +210 0 R 0 2130 R 168 0 R 210 0 R 0 -387 R 167 0 R 211 0 R 0 960 R 167 0 R +211 0 R 0 -2703 R 167 0 R 211 0 R 167 0 R D L2 9779 9701 M 210 0 R 167 0 R +211 0 R 0 1444 R 167 0 R 211 0 R 0 -12 R 167 0 R 211 0 R 0 -377 R 167 0 R +210 0 R 0 -108 R 168 0 R 210 0 R 0 367 R 168 0 R 210 0 R 0 89 R 168 0 R +210 0 R 0 -24 R 167 0 R 211 0 R 0 -1 R 167 0 R 211 0 R 0 -87 R 167 0 R +211 0 R 0 183 R 167 0 R 211 0 R 0 -230 R 167 0 R 210 0 R 0 50 R 168 0 R +210 0 R 0 853 R 168 0 R 210 0 R 0 -97 R 168 0 R 210 0 R 0 -656 R 167 0 R +211 0 R 0 960 R 167 0 R 211 0 R 0 -2354 R 167 0 R 211 0 R 167 0 R D +15 setlinewidth L0 1333 6878 M 7557 0 R D 1333 6878 M 0 57 R D +gsave 1333 6350 translate 0 0 M 1.0005 dup scale -58.8433 0 N +( ) show grestore 3090 6878 M 0 57 R D gsave 3090 6350 translate 0 0 M +1.0005 dup scale -58.8433 0 N +( ) show grestore 4847 6878 M 0 57 R D gsave 4847 6350 translate 0 0 M +1.0005 dup scale -58.8433 0 N +( ) show grestore 6604 6878 M 0 57 R D gsave 6604 6350 translate 0 0 M +1.0005 dup scale -58.8433 0 N +( ) show grestore 8361 6878 M 0 57 R D gsave 8361 6350 translate 0 0 M +1.0005 dup scale -58.8433 0 N +( ) show grestore 1862 6878 M 0 29 R D 2171 6878 M 0 29 R D 2391 6878 M +0 29 R D 2561 6878 M 0 29 R D 2700 6878 M 0 29 R D 2818 6878 M 0 29 R D +2920 6878 M 0 29 R D 3009 6878 M 0 29 R D 3619 6878 M 0 29 R D 3928 6878 M +0 29 R D 4148 6878 M 0 29 R D 4318 6878 M 0 29 R D 4457 6878 M 0 29 R D +4575 6878 M 0 29 R D 4677 6878 M 0 29 R D 4767 6878 M 0 29 R D 5376 6878 M +0 29 R D 5685 6878 M 0 29 R D 5905 6878 M 0 29 R D 6075 6878 M 0 29 R D +6214 6878 M 0 29 R D 6332 6878 M 0 29 R D 6434 6878 M 0 29 R D 6524 6878 M +0 29 R D 7133 6878 M 0 29 R D 7442 6878 M 0 29 R D 7662 6878 M 0 29 R D +7832 6878 M 0 29 R D 7971 6878 M 0 29 R D 8089 6878 M 0 29 R D 8191 6878 M +0 29 R D 8281 6878 M 0 29 R D 8890 6878 M 0 29 R D +gsave 5111 5892 translate 0 0 M 1.0005 dup scale -58.8433 0 N +( ) show grestore 1333 9701 M 7557 0 R D 1333 9701 M 0 -56 R D 3090 9701 M +0 -56 R D 4847 9701 M 0 -56 R D 6604 9701 M 0 -56 R D 8361 9701 M 0 -56 R D +1862 9701 M 0 -28 R D 2171 9701 M 0 -28 R D 2391 9701 M 0 -28 R D +2561 9701 M 0 -28 R D 2700 9701 M 0 -28 R D 2818 9701 M 0 -28 R D +2920 9701 M 0 -28 R D 3009 9701 M 0 -28 R D 3619 9701 M 0 -28 R D +3928 9701 M 0 -28 R D 4148 9701 M 0 -28 R D 4318 9701 M 0 -28 R D +4457 9701 M 0 -28 R D 4575 9701 M 0 -28 R D 4677 9701 M 0 -28 R D +4767 9701 M 0 -28 R D 5376 9701 M 0 -28 R D 5685 9701 M 0 -28 R D +5905 9701 M 0 -28 R D 6075 9701 M 0 -28 R D 6214 9701 M 0 -28 R D +6332 9701 M 0 -28 R D 6434 9701 M 0 -28 R D 6524 9701 M 0 -28 R D +7133 9701 M 0 -28 R D 7442 9701 M 0 -28 R D 7662 9701 M 0 -28 R D +7832 9701 M 0 -28 R D 7971 9701 M 0 -28 R D 8089 9701 M 0 -28 R D +8191 9701 M 0 -28 R D 8281 9701 M 0 -28 R D 8890 9701 M 0 -28 R D +1333 6878 M 0 2823 R D 1333 6878 M 151 0 R D gsave 1222 6878 translate 0 0 M +1.0005 dup scale -117.687 0 N +( ) show grestore 1333 7819 M 151 0 R D gsave 1222 7678 translate 0 0 M +1.0005 dup scale -117.687 0 N +( ) show grestore 1333 8760 M 151 0 R D gsave 1222 8619 translate 0 0 M +1.0005 dup scale -117.687 0 N +( ) show grestore 1333 9701 M 151 0 R D gsave 1222 9455 translate 0 0 M +1.0005 dup scale -117.687 0 N +( ) show grestore 1333 7162 M 75 0 R D 1333 7327 M 75 0 R D 1333 7445 M +75 0 R D 1333 7536 M 75 0 R D 1333 7611 M 75 0 R D 1333 7674 M 75 0 R D +1333 7728 M 75 0 R D 1333 7776 M 75 0 R D 1333 8103 M 75 0 R D 1333 8268 M +75 0 R D 1333 8386 M 75 0 R D 1333 8477 M 75 0 R D 1333 8551 M 75 0 R D +1333 8614 M 75 0 R D 1333 8669 M 75 0 R D 1333 8717 M 75 0 R D 1333 9043 M +75 0 R D 1333 9209 M 75 0 R D 1333 9327 M 75 0 R D 1333 9418 M 75 0 R D +1333 9492 M 75 0 R D 1333 9555 M 75 0 R D 1333 9610 M 75 0 R D 1333 9658 M +75 0 R D gsave 772 8290 translate 0 0 M 90 rotate 1.0005 dup scale +-58.8433 0 N +( ) show grestore 8890 6878 M 0 2823 R D 8890 6878 M -151 0 R D 8890 7819 M +-151 0 R D 8890 8760 M -151 0 R D 8890 9701 M -151 0 R D 8890 7162 M -75 0 R +D 8890 7327 M -75 0 R D 8890 7445 M -75 0 R D 8890 7536 M -75 0 R D +8890 7611 M -75 0 R D 8890 7674 M -75 0 R D 8890 7728 M -75 0 R D +8890 7776 M -75 0 R D 8890 8103 M -75 0 R D 8890 8268 M -75 0 R D +8890 8386 M -75 0 R D 8890 8477 M -75 0 R D 8890 8551 M -75 0 R D +8890 8614 M -75 0 R D 8890 8669 M -75 0 R D 8890 8717 M -75 0 R D +8890 9043 M -75 0 R D 8890 9209 M -75 0 R D 8890 9327 M -75 0 R D +8890 9418 M -75 0 R D 8890 9492 M -75 0 R D 8890 9555 M -75 0 R D +8890 9610 M -75 0 R D 8890 9658 M -75 0 R D 40 setlinewidth 1333 6878 M +251 0 R 0 824 R 188 0 R 251 0 R 0 23 R 188 0 R 251 0 R 0 767 R 189 0 R +250 0 R 0 341 R 189 0 R 251 0 R 0 18 R 188 0 R 251 0 R 0 -175 R 188 0 R +251 0 R 0 204 R 189 0 R 250 0 R 0 -295 R 189 0 R 251 0 R 0 77 R 188 0 R +251 0 R 0 -35 R 189 0 R 250 0 R 0 -1749 R 189 0 R 251 0 R 188 0 R 251 0 R +0 851 R 188 0 R 251 0 R 0 999 R 189 0 R 250 0 R 0 95 R 189 0 R 251 0 R +0 -438 R 188 0 R 251 0 R 0 -1507 R 188 0 R 90 0 R D 20 setlinewidth L1 +1333 6878 M 251 0 R 0 1109 R 188 0 R 251 0 R 0 22 R 188 0 R 251 0 R 0 768 R +189 0 R 250 0 R 0 340 R 189 0 R 251 0 R 0 18 R 188 0 R 251 0 R 0 -174 R +188 0 R 251 0 R 0 1 R 189 0 R 250 0 R 0 -605 R 189 0 R 251 0 R 0 -527 R +188 0 R 251 0 R 0 -952 R 189 0 R 250 0 R 189 0 R 251 0 R 188 0 R 251 0 R +188 0 R 251 0 R 189 0 R 250 0 R 189 0 R 251 0 R 188 0 R 251 0 R 188 0 R +90 0 R D L2 1333 6878 M 251 0 R 0 1520 R 188 0 R 251 0 R 0 -74 R 188 0 R +251 0 R 0 485 R 189 0 R 250 0 R 0 -577 R 189 0 R 251 0 R 0 374 R 188 0 R +251 0 R 0 218 R 188 0 R 251 0 R 0 -426 R 189 0 R 250 0 R 0 254 R 189 0 R +251 0 R 0 77 R 188 0 R 251 0 R 0 -34 R 189 0 R 250 0 R 0 -1817 R 189 0 R +251 0 R 188 0 R 251 0 R 0 918 R 188 0 R 251 0 R 0 1000 R 189 0 R 250 0 R +0 94 R 189 0 R 251 0 R 0 -437 R 188 0 R 251 0 R 0 -1575 R 188 0 R 90 0 R D +gsave 1472 9043 translate 0 0 M 1.1 dup scale +( L < 10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(11) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( L) show CP X -101.051 M +%%IncludeResource: font AvantGarde-Book +262.467 /AvantGarde-Book STDFONT +(O) show M X -58.3193 M +%%IncludeResource: font AvantGarde-Book +186.267 /AvantGarde-Book STDFONT +( \267) show +%%IncludeResource: font Helvetica +186.267 /Helvetica STDFONT grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 15 setlinewidth L0 9779 6878 M 7557 0 R D +9779 6878 M 0 57 R D gsave 9779 6350 translate 0 0 M 1.0005 dup scale +-58.8433 0 N +( ) show grestore 11668 6878 M 0 57 R D gsave 11668 6350 translate 0 0 M +1.0005 dup scale -58.8433 0 N +( ) show grestore 13557 6878 M 0 57 R D gsave 13557 6350 translate 0 0 M +1.0005 dup scale -58.8433 0 N +( ) show grestore 15447 6878 M 0 57 R D gsave 15447 6350 translate 0 0 M +1.0005 dup scale -58.8433 0 N +( ) show grestore 17336 6878 M 0 57 R D gsave 17336 6350 translate 0 0 M +1.0005 dup scale -58.8433 0 N +( ) show grestore 10347 6878 M 0 29 R D 10680 6878 M 0 29 R D 10916 6878 M +0 29 R D 11099 6878 M 0 29 R D 11249 6878 M 0 29 R D 11375 6878 M 0 29 R D +11485 6878 M 0 29 R D 11581 6878 M 0 29 R D 12237 6878 M 0 29 R D +12569 6878 M 0 29 R D 12805 6878 M 0 29 R D 12988 6878 M 0 29 R D +13138 6878 M 0 29 R D 13265 6878 M 0 29 R D 13374 6878 M 0 29 R D +13471 6878 M 0 29 R D 14126 6878 M 0 29 R D 14459 6878 M 0 29 R D +14695 6878 M 0 29 R D 14878 6878 M 0 29 R D 15027 6878 M 0 29 R D +15154 6878 M 0 29 R D 15263 6878 M 0 29 R D 15360 6878 M 0 29 R D +16015 6878 M 0 29 R D 16348 6878 M 0 29 R D 16584 6878 M 0 29 R D +16767 6878 M 0 29 R D 16917 6878 M 0 29 R D 17043 6878 M 0 29 R D +17153 6878 M 0 29 R D 17249 6878 M 0 29 R D gsave 13557 5892 translate 0 0 M +1.0005 dup scale -58.8433 0 N +( ) show grestore 9779 9701 M 7557 0 R D 9779 9701 M 0 -56 R D 11668 9701 M +0 -56 R D 13557 9701 M 0 -56 R D 15447 9701 M 0 -56 R D 17336 9701 M 0 -56 R +D 10347 9701 M 0 -28 R D 10680 9701 M 0 -28 R D 10916 9701 M 0 -28 R D +11099 9701 M 0 -28 R D 11249 9701 M 0 -28 R D 11375 9701 M 0 -28 R D +11485 9701 M 0 -28 R D 11581 9701 M 0 -28 R D 12237 9701 M 0 -28 R D +12569 9701 M 0 -28 R D 12805 9701 M 0 -28 R D 12988 9701 M 0 -28 R D +13138 9701 M 0 -28 R D 13265 9701 M 0 -28 R D 13374 9701 M 0 -28 R D +13471 9701 M 0 -28 R D 14126 9701 M 0 -28 R D 14459 9701 M 0 -28 R D +14695 9701 M 0 -28 R D 14878 9701 M 0 -28 R D 15027 9701 M 0 -28 R D +15154 9701 M 0 -28 R D 15263 9701 M 0 -28 R D 15360 9701 M 0 -28 R D +16015 9701 M 0 -28 R D 16348 9701 M 0 -28 R D 16584 9701 M 0 -28 R D +16767 9701 M 0 -28 R D 16917 9701 M 0 -28 R D 17043 9701 M 0 -28 R D +17153 9701 M 0 -28 R D 17249 9701 M 0 -28 R D 9779 6878 M 0 2823 R D +9779 6878 M 151 0 R D gsave 9667 6878 translate 0 0 M 1.0005 dup scale +-117.687 0 N +( ) show grestore 9779 7819 M 151 0 R D gsave 9667 7678 translate 0 0 M +1.0005 dup scale -117.687 0 N +( ) show grestore 9779 8760 M 151 0 R D gsave 9667 8619 translate 0 0 M +1.0005 dup scale -117.687 0 N +( ) show grestore 9779 9701 M 151 0 R D gsave 9667 9455 translate 0 0 M +1.0005 dup scale -117.687 0 N +( ) show grestore 9779 7162 M 75 0 R D 9779 7327 M 75 0 R D 9779 7445 M +75 0 R D 9779 7536 M 75 0 R D 9779 7611 M 75 0 R D 9779 7674 M 75 0 R D +9779 7728 M 75 0 R D 9779 7776 M 75 0 R D 9779 8103 M 75 0 R D 9779 8268 M +75 0 R D 9779 8386 M 75 0 R D 9779 8477 M 75 0 R D 9779 8551 M 75 0 R D +9779 8614 M 75 0 R D 9779 8669 M 75 0 R D 9779 8717 M 75 0 R D 9779 9043 M +75 0 R D 9779 9209 M 75 0 R D 9779 9327 M 75 0 R D 9779 9418 M 75 0 R D +9779 9492 M 75 0 R D 9779 9555 M 75 0 R D 9779 9610 M 75 0 R D 9779 9658 M +75 0 R D gsave 9217 8290 translate 0 0 M 90 rotate 1.0005 dup scale +-58.8433 0 N +( ) show grestore 17336 6878 M 0 2823 R D 17336 6878 M -151 0 R D +17336 7819 M -151 0 R D 17336 8760 M -151 0 R D 17336 9701 M -151 0 R D +17336 7162 M -76 0 R D 17336 7327 M -76 0 R D 17336 7445 M -76 0 R D +17336 7536 M -76 0 R D 17336 7611 M -76 0 R D 17336 7674 M -76 0 R D +17336 7728 M -76 0 R D 17336 7776 M -76 0 R D 17336 8103 M -76 0 R D +17336 8268 M -76 0 R D 17336 8386 M -76 0 R D 17336 8477 M -76 0 R D +17336 8551 M -76 0 R D 17336 8614 M -76 0 R D 17336 8669 M -76 0 R D +17336 8717 M -76 0 R D 17336 9043 M -76 0 R D 17336 9209 M -76 0 R D +17336 9327 M -76 0 R D 17336 9418 M -76 0 R D 17336 9492 M -76 0 R D +17336 9555 M -76 0 R D 17336 9610 M -76 0 R D 17336 9658 M -76 0 R D +40 setlinewidth 9779 6878 M 210 0 R 167 0 R 211 0 R 0 1571 R 167 0 R 211 0 R +0 -13 R 167 0 R 211 0 R 0 -377 R 167 0 R 210 0 R 0 -108 R 168 0 R 210 0 R +0 367 R 168 0 R 210 0 R 0 90 R 168 0 R 210 0 R 0 -25 R 167 0 R 211 0 R +0 -589 R 167 0 R 211 0 R 0 -333 R 167 0 R 211 0 R 0 -31 R 167 0 R 211 0 R +0 -552 R 167 0 R 210 0 R 168 0 R 210 0 R 0 2036 R 168 0 R 210 0 R 0 86 R +168 0 R 210 0 R 0 -1968 R 167 0 R 211 0 R 0 2311 R 167 0 R 211 0 R 0 -2465 R +167 0 R 211 0 R 167 0 R D 20 setlinewidth L1 9779 6878 M 210 0 R 167 0 R +211 0 R 167 0 R 211 0 R 167 0 R 211 0 R 167 0 R 210 0 R 168 0 R 210 0 R +168 0 R 210 0 R 168 0 R 210 0 R 167 0 R 211 0 R 167 0 R 211 0 R 167 0 R +211 0 R 167 0 R 211 0 R 167 0 R 210 0 R 168 0 R 210 0 R 168 0 R 210 0 R +0 2080 R 168 0 R 210 0 R 0 -1641 R 167 0 R 211 0 R 0 2310 R 167 0 R 211 0 R +0 -2749 R 167 0 R 211 0 R 167 0 R D L2 9779 6878 M 210 0 R 167 0 R 211 0 R +0 1638 R 167 0 R 211 0 R 0 -12 R 167 0 R 211 0 R 0 -377 R 167 0 R 210 0 R +0 -108 R 168 0 R 210 0 R 0 367 R 168 0 R 210 0 R 0 89 R 168 0 R 210 0 R +0 -25 R 167 0 R 211 0 R 0 -588 R 167 0 R 211 0 R 0 -334 R 167 0 R 211 0 R +0 -31 R 167 0 R 211 0 R 0 -619 R 167 0 R 210 0 R 168 0 R 210 0 R 0 2103 R +168 0 R 210 0 R 0 87 R 168 0 R 210 0 R 0 -1969 R 167 0 R 211 0 R 0 2125 R +167 0 R 211 0 R 0 -2346 R 167 0 R 211 0 R 167 0 R D 15 setlinewidth L0 +1333 4056 M 7557 0 R D 1333 4056 M 0 56 R D gsave 1333 3527 translate 0 0 M +1.0005 dup scale -58.8433 0 N +( ) show grestore 3090 4056 M 0 56 R D gsave 3090 3527 translate 0 0 M +1.0005 dup scale -58.8433 0 N +( ) show grestore 4847 4056 M 0 56 R D gsave 4847 3527 translate 0 0 M +1.0005 dup scale -58.8433 0 N +( ) show grestore 6604 4056 M 0 56 R D gsave 6604 3527 translate 0 0 M +1.0005 dup scale -58.8433 0 N +( ) show grestore 8361 4056 M 0 56 R D gsave 8361 3527 translate 0 0 M +1.0005 dup scale -58.8433 0 N +( ) show grestore 1862 4056 M 0 28 R D 2171 4056 M 0 28 R D 2391 4056 M +0 28 R D 2561 4056 M 0 28 R D 2700 4056 M 0 28 R D 2818 4056 M 0 28 R D +2920 4056 M 0 28 R D 3009 4056 M 0 28 R D 3619 4056 M 0 28 R D 3928 4056 M +0 28 R D 4148 4056 M 0 28 R D 4318 4056 M 0 28 R D 4457 4056 M 0 28 R D +4575 4056 M 0 28 R D 4677 4056 M 0 28 R D 4767 4056 M 0 28 R D 5376 4056 M +0 28 R D 5685 4056 M 0 28 R D 5905 4056 M 0 28 R D 6075 4056 M 0 28 R D +6214 4056 M 0 28 R D 6332 4056 M 0 28 R D 6434 4056 M 0 28 R D 6524 4056 M +0 28 R D 7133 4056 M 0 28 R D 7442 4056 M 0 28 R D 7662 4056 M 0 28 R D +7832 4056 M 0 28 R D 7971 4056 M 0 28 R D 8089 4056 M 0 28 R D 8191 4056 M +0 28 R D 8281 4056 M 0 28 R D 8890 4056 M 0 28 R D +gsave 5111 3069 translate 0 0 M 1.0005 dup scale -58.8433 0 N +( ) show grestore 1333 6878 M 7557 0 R D 1333 6878 M 0 -56 R D 3090 6878 M +0 -56 R D 4847 6878 M 0 -56 R D 6604 6878 M 0 -56 R D 8361 6878 M 0 -56 R D +1862 6878 M 0 -28 R D 2171 6878 M 0 -28 R D 2391 6878 M 0 -28 R D +2561 6878 M 0 -28 R D 2700 6878 M 0 -28 R D 2818 6878 M 0 -28 R D +2920 6878 M 0 -28 R D 3009 6878 M 0 -28 R D 3619 6878 M 0 -28 R D +3928 6878 M 0 -28 R D 4148 6878 M 0 -28 R D 4318 6878 M 0 -28 R D +4457 6878 M 0 -28 R D 4575 6878 M 0 -28 R D 4677 6878 M 0 -28 R D +4767 6878 M 0 -28 R D 5376 6878 M 0 -28 R D 5685 6878 M 0 -28 R D +5905 6878 M 0 -28 R D 6075 6878 M 0 -28 R D 6214 6878 M 0 -28 R D +6332 6878 M 0 -28 R D 6434 6878 M 0 -28 R D 6524 6878 M 0 -28 R D +7133 6878 M 0 -28 R D 7442 6878 M 0 -28 R D 7662 6878 M 0 -28 R D +7832 6878 M 0 -28 R D 7971 6878 M 0 -28 R D 8089 6878 M 0 -28 R D +8191 6878 M 0 -28 R D 8281 6878 M 0 -28 R D 8890 6878 M 0 -28 R D +1333 4056 M 0 2822 R D 1333 4056 M 151 0 R D gsave 1222 4056 translate 0 0 M +1.0005 dup scale -117.687 0 N +( ) show grestore 1333 4996 M 151 0 R D gsave 1222 4856 translate 0 0 M +1.0005 dup scale -117.687 0 N +( ) show grestore 1333 5937 M 151 0 R D gsave 1222 5797 translate 0 0 M +1.0005 dup scale -117.687 0 N +( ) show grestore 1333 6878 M 151 0 R D gsave 1222 6632 translate 0 0 M +1.0005 dup scale -117.687 0 N +( ) show grestore 1333 4339 M 75 0 R D 1333 4504 M 75 0 R D 1333 4622 M +75 0 R D 1333 4713 M 75 0 R D 1333 4788 M 75 0 R D 1333 4851 M 75 0 R D +1333 4905 M 75 0 R D 1333 4953 M 75 0 R D 1333 5280 M 75 0 R D 1333 5445 M +75 0 R D 1333 5563 M 75 0 R D 1333 5654 M 75 0 R D 1333 5729 M 75 0 R D +1333 5792 M 75 0 R D 1333 5846 M 75 0 R D 1333 5894 M 75 0 R D 1333 6221 M +75 0 R D 1333 6386 M 75 0 R D 1333 6504 M 75 0 R D 1333 6595 M 75 0 R D +1333 6670 M 75 0 R D 1333 6733 M 75 0 R D 1333 6787 M 75 0 R D 1333 6835 M +75 0 R D gsave 772 5467 translate 0 0 M 90 rotate 1.0005 dup scale +-4435.05 0 N +( Logarithmic Probability Distribution) show grestore +8890 4056 M 0 2822 R D 8890 4056 M -151 0 R D 8890 4996 M -151 0 R D +8890 5937 M -151 0 R D 8890 6878 M -151 0 R D 8890 4339 M -75 0 R D +8890 4504 M -75 0 R D 8890 4622 M -75 0 R D 8890 4713 M -75 0 R D +8890 4788 M -75 0 R D 8890 4851 M -75 0 R D 8890 4905 M -75 0 R D +8890 4953 M -75 0 R D 8890 5280 M -75 0 R D 8890 5445 M -75 0 R D +8890 5563 M -75 0 R D 8890 5654 M -75 0 R D 8890 5729 M -75 0 R D +8890 5792 M -75 0 R D 8890 5846 M -75 0 R D 8890 5894 M -75 0 R D +8890 6221 M -75 0 R D 8890 6386 M -75 0 R D 8890 6504 M -75 0 R D +8890 6595 M -75 0 R D 8890 6670 M -75 0 R D 8890 6733 M -75 0 R D +8890 6787 M -75 0 R D 8890 6835 M -75 0 R D 40 setlinewidth 1333 4056 M +251 0 R 188 0 R 251 0 R 188 0 R 251 0 R 189 0 R 250 0 R 189 0 R 251 0 R +188 0 R 251 0 R 188 0 R 251 0 R 189 0 R 250 0 R 189 0 R 251 0 R 0 1303 R +188 0 R 251 0 R 0 200 R 189 0 R 250 0 R 0 717 R 189 0 R 251 0 R 0 -389 R +188 0 R 251 0 R 0 -11 R 188 0 R 251 0 R 0 373 R 189 0 R 250 0 R 0 162 R +189 0 R 251 0 R 0 -2355 R 188 0 R 251 0 R 188 0 R 90 0 R D 20 setlinewidth +L1 1333 4056 M 251 0 R 188 0 R 251 0 R 188 0 R 251 0 R 189 0 R 250 0 R +189 0 R 251 0 R 188 0 R 251 0 R 188 0 R 251 0 R 189 0 R 250 0 R 189 0 R +251 0 R 0 2217 R 188 0 R 251 0 R 0 22 R 189 0 R 250 0 R 0 137 R 189 0 R +251 0 R 0 -374 R 188 0 R 251 0 R 0 -306 R 188 0 R 251 0 R 0 -1696 R 189 0 R +250 0 R 189 0 R 251 0 R 188 0 R 251 0 R 188 0 R 90 0 R D L2 1333 4056 M +251 0 R 188 0 R 251 0 R 188 0 R 251 0 R 189 0 R 250 0 R 189 0 R 251 0 R +188 0 R 251 0 R 188 0 R 251 0 R 189 0 R 250 0 R 189 0 R 251 0 R 0 1303 R +188 0 R 251 0 R 0 200 R 189 0 R 250 0 R 0 717 R 189 0 R 251 0 R 0 -389 R +188 0 R 251 0 R 0 -11 R 188 0 R 251 0 R 0 373 R 189 0 R 250 0 R 0 162 R +189 0 R 251 0 R 0 -2355 R 188 0 R 251 0 R 188 0 R 90 0 R D +gsave 1472 6221 translate 0 0 M 1.1 dup scale +( 10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(11) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( L) show CP X -101.051 M +%%IncludeResource: font AvantGarde-Book +262.467 /AvantGarde-Book STDFONT +(O) show M X -58.3193 M +%%IncludeResource: font AvantGarde-Book +186.267 /AvantGarde-Book STDFONT +( \267) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( < L < 10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(12) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( L) show CP X -101.051 M +%%IncludeResource: font AvantGarde-Book +262.467 /AvantGarde-Book STDFONT +(O) show M X -58.3193 M +%%IncludeResource: font AvantGarde-Book +186.267 /AvantGarde-Book STDFONT +( \267) show +%%IncludeResource: font Helvetica +186.267 /Helvetica STDFONT grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 15 setlinewidth L0 9779 4056 M 7557 0 R D +9779 4056 M 0 56 R D gsave 9779 3527 translate 0 0 M 1.0005 dup scale +-58.8433 0 N +( ) show grestore 11668 4056 M 0 56 R D gsave 11668 3527 translate 0 0 M +1.0005 dup scale -58.8433 0 N +( ) show grestore 13557 4056 M 0 56 R D gsave 13557 3527 translate 0 0 M +1.0005 dup scale -58.8433 0 N +( ) show grestore 15447 4056 M 0 56 R D gsave 15447 3527 translate 0 0 M +1.0005 dup scale -58.8433 0 N +( ) show grestore 17336 4056 M 0 56 R D gsave 17336 3527 translate 0 0 M +1.0005 dup scale -58.8433 0 N +( ) show grestore 10347 4056 M 0 28 R D 10680 4056 M 0 28 R D 10916 4056 M +0 28 R D 11099 4056 M 0 28 R D 11249 4056 M 0 28 R D 11375 4056 M 0 28 R D +11485 4056 M 0 28 R D 11581 4056 M 0 28 R D 12237 4056 M 0 28 R D +12569 4056 M 0 28 R D 12805 4056 M 0 28 R D 12988 4056 M 0 28 R D +13138 4056 M 0 28 R D 13265 4056 M 0 28 R D 13374 4056 M 0 28 R D +13471 4056 M 0 28 R D 14126 4056 M 0 28 R D 14459 4056 M 0 28 R D +14695 4056 M 0 28 R D 14878 4056 M 0 28 R D 15027 4056 M 0 28 R D +15154 4056 M 0 28 R D 15263 4056 M 0 28 R D 15360 4056 M 0 28 R D +16015 4056 M 0 28 R D 16348 4056 M 0 28 R D 16584 4056 M 0 28 R D +16767 4056 M 0 28 R D 16917 4056 M 0 28 R D 17043 4056 M 0 28 R D +17153 4056 M 0 28 R D 17249 4056 M 0 28 R D gsave 13557 3069 translate 0 0 M +1.0005 dup scale -58.8433 0 N +( ) show grestore 9779 6878 M 7557 0 R D 9779 6878 M 0 -56 R D 11668 6878 M +0 -56 R D 13557 6878 M 0 -56 R D 15447 6878 M 0 -56 R D 17336 6878 M 0 -56 R +D 10347 6878 M 0 -28 R D 10680 6878 M 0 -28 R D 10916 6878 M 0 -28 R D +11099 6878 M 0 -28 R D 11249 6878 M 0 -28 R D 11375 6878 M 0 -28 R D +11485 6878 M 0 -28 R D 11581 6878 M 0 -28 R D 12237 6878 M 0 -28 R D +12569 6878 M 0 -28 R D 12805 6878 M 0 -28 R D 12988 6878 M 0 -28 R D +13138 6878 M 0 -28 R D 13265 6878 M 0 -28 R D 13374 6878 M 0 -28 R D +13471 6878 M 0 -28 R D 14126 6878 M 0 -28 R D 14459 6878 M 0 -28 R D +14695 6878 M 0 -28 R D 14878 6878 M 0 -28 R D 15027 6878 M 0 -28 R D +15154 6878 M 0 -28 R D 15263 6878 M 0 -28 R D 15360 6878 M 0 -28 R D +16015 6878 M 0 -28 R D 16348 6878 M 0 -28 R D 16584 6878 M 0 -28 R D +16767 6878 M 0 -28 R D 16917 6878 M 0 -28 R D 17043 6878 M 0 -28 R D +17153 6878 M 0 -28 R D 17249 6878 M 0 -28 R D 9779 4056 M 0 2822 R D +9779 4056 M 151 0 R D gsave 9667 4056 translate 0 0 M 1.0005 dup scale +-117.687 0 N +( ) show grestore 9779 4996 M 151 0 R D gsave 9667 4856 translate 0 0 M +1.0005 dup scale -117.687 0 N +( ) show grestore 9779 5937 M 151 0 R D gsave 9667 5797 translate 0 0 M +1.0005 dup scale -117.687 0 N +( ) show grestore 9779 6878 M 151 0 R D gsave 9667 6632 translate 0 0 M +1.0005 dup scale -117.687 0 N +( ) show grestore 9779 4339 M 75 0 R D 9779 4504 M 75 0 R D 9779 4622 M +75 0 R D 9779 4713 M 75 0 R D 9779 4788 M 75 0 R D 9779 4851 M 75 0 R D +9779 4905 M 75 0 R D 9779 4953 M 75 0 R D 9779 5280 M 75 0 R D 9779 5445 M +75 0 R D 9779 5563 M 75 0 R D 9779 5654 M 75 0 R D 9779 5729 M 75 0 R D +9779 5792 M 75 0 R D 9779 5846 M 75 0 R D 9779 5894 M 75 0 R D 9779 6221 M +75 0 R D 9779 6386 M 75 0 R D 9779 6504 M 75 0 R D 9779 6595 M 75 0 R D +9779 6670 M 75 0 R D 9779 6733 M 75 0 R D 9779 6787 M 75 0 R D 9779 6835 M +75 0 R D gsave 9217 5467 translate 0 0 M 90 rotate 1.0005 dup scale +-58.8433 0 N +( ) show grestore 17336 4056 M 0 2822 R D 17336 4056 M -151 0 R D +17336 4996 M -151 0 R D 17336 5937 M -151 0 R D 17336 6878 M -151 0 R D +17336 4339 M -76 0 R D 17336 4504 M -76 0 R D 17336 4622 M -76 0 R D +17336 4713 M -76 0 R D 17336 4788 M -76 0 R D 17336 4851 M -76 0 R D +17336 4905 M -76 0 R D 17336 4953 M -76 0 R D 17336 5280 M -76 0 R D +17336 5445 M -76 0 R D 17336 5563 M -76 0 R D 17336 5654 M -76 0 R D +17336 5729 M -76 0 R D 17336 5792 M -76 0 R D 17336 5846 M -76 0 R D +17336 5894 M -76 0 R D 17336 6221 M -76 0 R D 17336 6386 M -76 0 R D +17336 6504 M -76 0 R D 17336 6595 M -76 0 R D 17336 6670 M -76 0 R D +17336 6733 M -76 0 R D 17336 6787 M -76 0 R D 17336 6835 M -76 0 R D +40 setlinewidth 9779 4056 M 210 0 R 167 0 R 211 0 R 167 0 R 211 0 R 167 0 R +211 0 R 167 0 R 210 0 R 168 0 R 210 0 R 168 0 R 210 0 R 168 0 R 210 0 R +167 0 R 211 0 R 0 1866 R 167 0 R 211 0 R 0 -33 R 167 0 R 211 0 R 0 208 R +167 0 R 211 0 R 0 -198 R 167 0 R 210 0 R 0 51 R 168 0 R 210 0 R 0 518 R +168 0 R 210 0 R 0 -1234 R 168 0 R 210 0 R 0 417 R 167 0 R 211 0 R 0 -94 R +167 0 R 211 0 R 0 -1501 R 167 0 R 211 0 R 167 0 R D 20 setlinewidth L1 +9779 4056 M 210 0 R 167 0 R 211 0 R 167 0 R 211 0 R 167 0 R 211 0 R 167 0 R +210 0 R 168 0 R 210 0 R 168 0 R 210 0 R 168 0 R 210 0 R 167 0 R 211 0 R +167 0 R 211 0 R 167 0 R 211 0 R 167 0 R 211 0 R 167 0 R 210 0 R 168 0 R +210 0 R 168 0 R 210 0 R 0 2091 R 168 0 R 210 0 R 0 417 R 167 0 R 211 0 R +0 -93 R 167 0 R 211 0 R 0 -2415 R 167 0 R 211 0 R 167 0 R D L2 9779 4056 M +210 0 R 167 0 R 211 0 R 167 0 R 211 0 R 167 0 R 211 0 R 167 0 R 210 0 R +168 0 R 210 0 R 168 0 R 210 0 R 168 0 R 210 0 R 167 0 R 211 0 R 0 1866 R +167 0 R 211 0 R 0 -33 R 167 0 R 211 0 R 0 208 R 167 0 R 211 0 R 0 -198 R +167 0 R 210 0 R 0 51 R 168 0 R 210 0 R 0 518 R 168 0 R 210 0 R 0 -1234 R +168 0 R 210 0 R 0 417 R 167 0 R 211 0 R 0 -94 R 167 0 R 211 0 R 0 -1501 R +167 0 R 211 0 R 167 0 R D 15 setlinewidth L0 1333 1233 M 7557 0 R D +1333 1233 M 0 56 R D gsave 1333 704 translate 0 0 M 1.0005 dup scale +-647.277 0 N +(0.0001) show grestore 3090 1233 M 0 56 R D gsave 3090 704 translate 0 0 M +1.0005 dup scale -529.59 0 N +(0.001) show grestore 4847 1233 M 0 56 R D gsave 4847 704 translate 0 0 M +1.0005 dup scale -411.903 0 N +(0.01) show grestore 6604 1233 M 0 56 R D gsave 6604 704 translate 0 0 M +1.0005 dup scale -294.217 0 N +(0.1) show grestore 8361 1233 M 0 56 R D gsave 8361 704 translate 0 0 M +1.0005 dup scale -294.217 0 N +(1.0) show grestore 1862 1233 M 0 28 R D 2171 1233 M 0 28 R D 2391 1233 M +0 28 R D 2561 1233 M 0 28 R D 2700 1233 M 0 28 R D 2818 1233 M 0 28 R D +2920 1233 M 0 28 R D 3009 1233 M 0 28 R D 3619 1233 M 0 28 R D 3928 1233 M +0 28 R D 4148 1233 M 0 28 R D 4318 1233 M 0 28 R D 4457 1233 M 0 28 R D +4575 1233 M 0 28 R D 4677 1233 M 0 28 R D 4767 1233 M 0 28 R D 5376 1233 M +0 28 R D 5685 1233 M 0 28 R D 5905 1233 M 0 28 R D 6075 1233 M 0 28 R D +6214 1233 M 0 28 R D 6332 1233 M 0 28 R D 6434 1233 M 0 28 R D 6524 1233 M +0 28 R D 7133 1233 M 0 28 R D 7442 1233 M 0 28 R D 7662 1233 M 0 28 R D +7832 1233 M 0 28 R D 7971 1233 M 0 28 R D 8089 1233 M 0 28 R D 8191 1233 M +0 28 R D 8281 1233 M 0 28 R D 8890 1233 M 0 28 R D +gsave 5111 247 translate 0 0 M 1.0005 dup scale -2136.1 0 N +(Eddington Ratio L/L) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(EDD) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 1333 4056 M 7557 0 R D 1333 4056 M 0 -57 R D +3090 4056 M 0 -57 R D 4847 4056 M 0 -57 R D 6604 4056 M 0 -57 R D +8361 4056 M 0 -57 R D 1862 4056 M 0 -29 R D 2171 4056 M 0 -29 R D +2391 4056 M 0 -29 R D 2561 4056 M 0 -29 R D 2700 4056 M 0 -29 R D +2818 4056 M 0 -29 R D 2920 4056 M 0 -29 R D 3009 4056 M 0 -29 R D +3619 4056 M 0 -29 R D 3928 4056 M 0 -29 R D 4148 4056 M 0 -29 R D +4318 4056 M 0 -29 R D 4457 4056 M 0 -29 R D 4575 4056 M 0 -29 R D +4677 4056 M 0 -29 R D 4767 4056 M 0 -29 R D 5376 4056 M 0 -29 R D +5685 4056 M 0 -29 R D 5905 4056 M 0 -29 R D 6075 4056 M 0 -29 R D +6214 4056 M 0 -29 R D 6332 4056 M 0 -29 R D 6434 4056 M 0 -29 R D +6524 4056 M 0 -29 R D 7133 4056 M 0 -29 R D 7442 4056 M 0 -29 R D +7662 4056 M 0 -29 R D 7832 4056 M 0 -29 R D 7971 4056 M 0 -29 R D +8089 4056 M 0 -29 R D 8191 4056 M 0 -29 R D 8281 4056 M 0 -29 R D +8890 4056 M 0 -29 R D 1333 1233 M 0 2823 R D 1333 1233 M 151 0 R D +gsave 1222 1233 translate 0 0 M 1.0005 dup scale -117.687 0 N +( ) show grestore 1333 2174 M 151 0 R D gsave 1222 2033 translate 0 0 M +1.0005 dup scale -117.687 0 N +( ) show grestore 1333 3115 M 151 0 R D gsave 1222 2974 translate 0 0 M +1.0005 dup scale -117.687 0 N +( ) show grestore 1333 4056 M 151 0 R D gsave 1222 3809 translate 0 0 M +1.0005 dup scale -117.687 0 N +( ) show grestore 1333 1516 M 75 0 R D 1333 1682 M 75 0 R D 1333 1799 M +75 0 R D 1333 1890 M 75 0 R D 1333 1965 M 75 0 R D 1333 2028 M 75 0 R D +1333 2082 M 75 0 R D 1333 2131 M 75 0 R D 1333 2457 M 75 0 R D 1333 2623 M +75 0 R D 1333 2740 M 75 0 R D 1333 2831 M 75 0 R D 1333 2906 M 75 0 R D +1333 2969 M 75 0 R D 1333 3023 M 75 0 R D 1333 3072 M 75 0 R D 1333 3398 M +75 0 R D 1333 3564 M 75 0 R D 1333 3681 M 75 0 R D 1333 3772 M 75 0 R D +1333 3847 M 75 0 R D 1333 3910 M 75 0 R D 1333 3964 M 75 0 R D 1333 4012 M +75 0 R D gsave 772 2644 translate 0 0 M 90 rotate 1.0005 dup scale +-58.8433 0 N +( ) show grestore 8890 1233 M 0 2823 R D 8890 1233 M -151 0 R D 8890 2174 M +-151 0 R D 8890 3115 M -151 0 R D 8890 4056 M -151 0 R D 8890 1516 M -75 0 R +D 8890 1682 M -75 0 R D 8890 1799 M -75 0 R D 8890 1890 M -75 0 R D +8890 1965 M -75 0 R D 8890 2028 M -75 0 R D 8890 2082 M -75 0 R D +8890 2131 M -75 0 R D 8890 2457 M -75 0 R D 8890 2623 M -75 0 R D +8890 2740 M -75 0 R D 8890 2831 M -75 0 R D 8890 2906 M -75 0 R D +8890 2969 M -75 0 R D 8890 3023 M -75 0 R D 8890 3072 M -75 0 R D +8890 3398 M -75 0 R D 8890 3564 M -75 0 R D 8890 3681 M -75 0 R D +8890 3772 M -75 0 R D 8890 3847 M -75 0 R D 8890 3910 M -75 0 R D +8890 3964 M -75 0 R D 8890 4012 M -75 0 R D 40 setlinewidth 1333 1233 M +251 0 R 188 0 R 251 0 R 188 0 R 251 0 R 189 0 R 250 0 R 189 0 R 251 0 R +188 0 R 251 0 R 188 0 R 251 0 R 189 0 R 250 0 R 189 0 R 251 0 R 188 0 R +251 0 R 189 0 R 250 0 R 189 0 R 251 0 R 188 0 R 251 0 R 0 1962 R 188 0 R +251 0 R 0 -295 R 189 0 R 250 0 R 0 847 R 189 0 R 251 0 R 0 -130 R 188 0 R +251 0 R 0 -1577 R 188 0 R 90 0 R D 20 setlinewidth L1 1333 1233 M 251 0 R +188 0 R 251 0 R 188 0 R 251 0 R 189 0 R 250 0 R 189 0 R 251 0 R 188 0 R +251 0 R 188 0 R 251 0 R 189 0 R 250 0 R 189 0 R 251 0 R 188 0 R 251 0 R +189 0 R 250 0 R 189 0 R 251 0 R 188 0 R 251 0 R 0 1962 R 188 0 R 251 0 R +0 -295 R 189 0 R 250 0 R 0 847 R 189 0 R 251 0 R 0 -130 R 188 0 R 251 0 R +0 -1577 R 188 0 R 90 0 R D L2 1333 1233 M 251 0 R 188 0 R 251 0 R 188 0 R +251 0 R 189 0 R 250 0 R 189 0 R 251 0 R 188 0 R 251 0 R 188 0 R 251 0 R +189 0 R 250 0 R 189 0 R 251 0 R 188 0 R 251 0 R 189 0 R 250 0 R 189 0 R +251 0 R 188 0 R 251 0 R 0 1962 R 188 0 R 251 0 R 0 -295 R 189 0 R 250 0 R +0 847 R 189 0 R 251 0 R 0 -130 R 188 0 R 251 0 R 0 -1577 R 188 0 R 90 0 R D +gsave 1472 3398 translate 0 0 M 1.1 dup scale +( L > 10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(12) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( L) show CP X -101.051 M +%%IncludeResource: font AvantGarde-Book +262.467 /AvantGarde-Book STDFONT +(O) show M 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+%%BeginProlog +save +%+ prolog.ps -- Prolog for IDL generated PostScript files +%+ Copyright (c) 1988-2003 Research Systems, Inc. All Rights Reserved. +%v 4 +/$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C +{currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint +stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} +bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show +grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 +setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 +{[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 +100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 +{[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef +/ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} +ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont +exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica +findfont exch scalefont setfont (\267) show currentpoint grestore moveto} +bdef end 2.5 setmiterlimit +%%EndProlog +%%Page: 0 1 +%%PageRequirements: color +%%PageResources: (atend) +%%PageOrientation: Portrait +%%PageBoundingBox: 54 360 558 720 +%%BeginPageSetup +save +$IDL_DICT begin 54 360 translate 0.0283465 dup scale +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +%%EndPageSetup +15 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 2242 6706 M 7433 0 R D +2863 6706 M 0 105 R D gsave 2863 6172 translate 0 0 M 1.01 dup scale +-58.8433 0 N +( ) show grestore 4927 6706 M 0 105 R D gsave 4927 6172 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 6990 6706 M 0 105 R D gsave 6990 6172 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 9054 6706 M 0 105 R D gsave 9054 6172 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 2242 6706 M 0 52 R D 2406 6706 M 0 52 R D 2544 6706 M +0 52 R D 2663 6706 M 0 52 R D 2769 6706 M 0 52 R D 3485 6706 M 0 52 R D +3848 6706 M 0 52 R D 4106 6706 M 0 52 R D 4306 6706 M 0 52 R D 4469 6706 M +0 52 R D 4607 6706 M 0 52 R D 4727 6706 M 0 52 R D 4832 6706 M 0 52 R D +5548 6706 M 0 52 R D 5911 6706 M 0 52 R D 6169 6706 M 0 52 R D 6369 6706 M +0 52 R D 6533 6706 M 0 52 R D 6671 6706 M 0 52 R D 6790 6706 M 0 52 R D +6896 6706 M 0 52 R D 7611 6706 M 0 52 R D 7975 6706 M 0 52 R D 8233 6706 M +0 52 R D 8433 6706 M 0 52 R D 8596 6706 M 0 52 R D 8734 6706 M 0 52 R D +8854 6706 M 0 52 R D 8959 6706 M 0 52 R D 9675 6706 M 0 52 R D +gsave 5959 5710 translate 0 0 M 1.01 dup scale -58.8433 0 N +( ) show grestore 2242 11989 M 7433 0 R D 2863 11989 M 0 -106 R D +4927 11989 M 0 -106 R D 6990 11989 M 0 -106 R D 9054 11989 M 0 -106 R D +2242 11989 M 0 -53 R D 2406 11989 M 0 -53 R D 2544 11989 M 0 -53 R D +2663 11989 M 0 -53 R D 2769 11989 M 0 -53 R D 3485 11989 M 0 -53 R D +3848 11989 M 0 -53 R D 4106 11989 M 0 -53 R D 4306 11989 M 0 -53 R D +4469 11989 M 0 -53 R D 4607 11989 M 0 -53 R D 4727 11989 M 0 -53 R D +4832 11989 M 0 -53 R D 5548 11989 M 0 -53 R D 5911 11989 M 0 -53 R D +6169 11989 M 0 -53 R D 6369 11989 M 0 -53 R D 6533 11989 M 0 -53 R D +6671 11989 M 0 -53 R D 6790 11989 M 0 -53 R D 6896 11989 M 0 -53 R D +7611 11989 M 0 -53 R D 7975 11989 M 0 -53 R D 8233 11989 M 0 -53 R D +8433 11989 M 0 -53 R D 8596 11989 M 0 -53 R D 8734 11989 M 0 -53 R D +8854 11989 M 0 -53 R D 8959 11989 M 0 -53 R D 9675 11989 M 0 -53 R D +2242 6706 M 0 5283 R D 2242 6706 M 149 0 R D gsave 2130 6706 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 8026 M 149 0 R D gsave 2130 7884 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 9347 M 149 0 R D gsave 2130 9205 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 10668 M 149 0 R D gsave 2130 10526 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 11989 M 149 0 R D gsave 2130 11740 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 6838 M 75 0 R D 2242 6970 M 75 0 R D 2242 7102 M +75 0 R D 2242 7234 M 75 0 R D 2242 7366 M 75 0 R D 2242 7498 M 75 0 R D +2242 7630 M 75 0 R D 2242 7762 M 75 0 R D 2242 7894 M 75 0 R D 2242 8159 M +75 0 R D 2242 8291 M 75 0 R D 2242 8423 M 75 0 R D 2242 8555 M 75 0 R D +2242 8687 M 75 0 R D 2242 8819 M 75 0 R D 2242 8951 M 75 0 R D 2242 9083 M +75 0 R D 2242 9215 M 75 0 R D 2242 9479 M 75 0 R D 2242 9611 M 75 0 R D +2242 9744 M 75 0 R D 2242 9876 M 75 0 R D 2242 10008 M 75 0 R D 2242 10140 M +75 0 R D 2242 10272 M 75 0 R D 2242 10404 M 75 0 R D 2242 10536 M 75 0 R D +2242 10800 M 75 0 R D 2242 10932 M 75 0 R D 2242 11064 M 75 0 R D +2242 11197 M 75 0 R D 2242 11329 M 75 0 R D 2242 11461 M 75 0 R D +2242 11593 M 75 0 R D 2242 11725 M 75 0 R D 2242 11857 M 75 0 R D +gsave 1676 9347 translate 0 0 M 90 rotate 1.01 dup scale -58.8433 0 N +( ) show grestore 9675 6706 M 0 5283 R D 9675 6706 M -149 0 R D 9675 8026 M +-149 0 R D 9675 9347 M -149 0 R D 9675 10668 M -149 0 R D 9675 11989 M +-149 0 R D 9675 6838 M -74 0 R D 9675 6970 M -74 0 R D 9675 7102 M -74 0 R D +9675 7234 M -74 0 R D 9675 7366 M -74 0 R D 9675 7498 M -74 0 R D +9675 7630 M -74 0 R D 9675 7762 M -74 0 R D 9675 7894 M -74 0 R D +9675 8159 M -74 0 R D 9675 8291 M -74 0 R D 9675 8423 M -74 0 R D +9675 8555 M -74 0 R D 9675 8687 M -74 0 R D 9675 8819 M -74 0 R D +9675 8951 M -74 0 R D 9675 9083 M -74 0 R D 9675 9215 M -74 0 R D +9675 9479 M -74 0 R D 9675 9611 M -74 0 R D 9675 9744 M -74 0 R D +9675 9876 M -74 0 R D 9675 10008 M -74 0 R D 9675 10140 M -74 0 R D +9675 10272 M -74 0 R D 9675 10404 M -74 0 R D 9675 10536 M -74 0 R D +9675 10800 M -74 0 R D 9675 10932 M -74 0 R D 9675 11064 M -74 0 R D +9675 11197 M -74 0 R D 9675 11329 M -74 0 R D 9675 11461 M -74 0 R D +9675 11593 M -74 0 R D 9675 11725 M -74 0 R D 9675 11857 M -74 0 R D +40 setlinewidth 2242 6706 M 106 0 R 294 0 R 221 0 R 295 0 R 221 0 R 295 0 R +221 0 R 295 0 R 221 0 R 295 0 R 221 0 R 294 0 R 0 17 R 222 0 R 294 0 R +0 -17 R 222 0 R 294 0 R 0 394 R 221 0 R 295 0 R 0 1796 R 221 0 R 295 0 R +0 -100 R 221 0 R 295 0 R 0 1141 R 221 0 R 295 0 R 0 -250 R 221 0 R 294 0 R +0 -933 R 222 0 R 294 0 R 0 -2048 R 222 0 R 104 0 R D 20 setlinewidth L2 +0.000 0.514 1.000 setrgbcolor 2242 6706 M 106 0 R 515 0 R 516 3 R 516 11 R +516 38 R 516 107 R 516 248 R 516 469 R 515 708 R 516 823 R 516 666 R +516 226 R 516 -322 R 516 -719 R 516 -818 R 104 -135 R D L0 +1.000 0.000 0.000 setrgbcolor 2242 6935 M 106 0 R 294 0 R 0 236 R 221 0 R +295 0 R 0 302 R 221 0 R 295 0 R 0 33 R 221 0 R 295 0 R 0 -139 R 221 0 R +295 0 R 0 -208 R 221 0 R 294 0 R 0 42 R 222 0 R 294 0 R 0 685 R 222 0 R +294 0 R 0 525 R 221 0 R 295 0 R 0 914 R 221 0 R 295 0 R 0 -666 R 221 0 R +295 0 R 0 -585 R 221 0 R 295 0 R 0 -1110 R 221 0 R 294 0 R 0 -180 R 222 0 R +294 0 R 0 -66 R 222 0 R 104 0 R D L1 2242 7174 M 106 0 R 294 0 R 0 74 R +221 0 R 295 0 R 0 -93 R 221 0 R 295 0 R 0 -100 R 221 0 R 295 0 R 0 -15 R +221 0 R 295 0 R 0 21 R 221 0 R 294 0 R 0 151 R 222 0 R 294 0 R 0 701 R +222 0 R 294 0 R 0 536 R 221 0 R 295 0 R 0 934 R 221 0 R 295 0 R 0 -680 R +221 0 R 295 0 R 0 -599 R 221 0 R 295 0 R 0 -1135 R 221 0 R 294 0 R 0 -184 R +222 0 R 294 0 R 0 -67 R 222 0 R 104 0 R D 0.000 0.000 0.000 setrgbcolor +gsave 2406 11329 translate 0 0 M 1.25 dup scale +(Complete Sample) show grestore gsave 2406 10668 translate 0 0 M +1.25 dup scale +( z < 0.5) show grestore 5035 6842 M 0 278 R 277 0 R 0 -278 R -277 0 R F +5398 7117 M 0 278 R 278 0 R 0 -278 R -278 0 R F +5761 6705 M 0 139 R 278 0 R 0 -139 R F +6125 6842 M 0 278 R 277 0 R 0 -278 R -277 0 R F +6488 8218 M 0 277 R 278 0 R 0 -277 R -278 0 R F +6852 9594 M 0 277 R 277 0 R 0 -277 R -277 0 R F +7215 8218 M 0 277 R 277 0 R 0 -277 R -277 0 R F +7578 8493 M 0 278 R 278 0 R 0 -278 R -278 0 R F +7942 9594 M 0 277 R 277 0 R 0 -277 R -277 0 R F +8305 8493 M 0 278 R 277 0 R 0 -278 R -277 0 R F +8668 9594 M 0 277 R 278 0 R 0 -277 R -278 0 R F +9032 9043 M 0 278 R 277 0 R 0 -278 R -277 0 R F +9395 7668 M 0 277 R 277 0 R 0 -277 R -277 0 R F +L0 5136 6797 M 75 0 R -37 0 R 0 367 R -38 0 R 75 0 R D 5500 6997 M 74 0 R +-37 0 R 0 518 R -37 0 R 74 0 R D 5863 6706 M 74 0 R -37 0 R -37 0 R 74 0 R D +6226 6797 M 75 0 R -37 0 R 0 367 R -38 0 R 75 0 R D 6590 7907 M 74 0 R +-37 0 R 0 899 R -37 0 R 74 0 R D 6953 9124 M 74 0 R -37 0 R 0 1217 R -37 0 R +74 0 R D 7316 7907 M 75 0 R -37 0 R 0 899 R -38 0 R 75 0 R D 7680 8146 M +74 0 R -37 0 R 0 971 R -37 0 R 74 0 R D 8043 9124 M 75 0 R -38 0 R 0 1217 R +-37 0 R 75 0 R D 8407 8146 M 74 0 R -37 0 R 0 971 R -37 0 R 74 0 R D +8770 9124 M 74 0 R -37 0 R 0 1217 R -37 0 R 74 0 R D 9133 8632 M 75 0 R +-38 0 R 0 1101 R -37 0 R 75 0 R D 9497 7439 M 74 0 R -37 0 R 0 734 R -37 0 R +74 0 R D 15 setlinewidth 9675 6706 M 7432 0 R D 10296 6706 M 0 105 R D +gsave 10296 6172 translate 0 0 M 1.01 dup scale -58.8433 0 N +( ) show grestore 12359 6706 M 0 105 R D gsave 12359 6172 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 14423 6706 M 0 105 R D gsave 14423 6172 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 16486 6706 M 0 105 R D gsave 16486 6172 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 9675 6706 M 0 52 R D 9838 6706 M 0 52 R D 9976 6706 M +0 52 R D 10096 6706 M 0 52 R D 10202 6706 M 0 52 R D 10917 6706 M 0 52 R D +11281 6706 M 0 52 R D 11538 6706 M 0 52 R D 11738 6706 M 0 52 R D +11902 6706 M 0 52 R D 12040 6706 M 0 52 R D 12159 6706 M 0 52 R D +12265 6706 M 0 52 R D 12981 6706 M 0 52 R D 13344 6706 M 0 52 R D +13602 6706 M 0 52 R D 13802 6706 M 0 52 R D 13965 6706 M 0 52 R D +14103 6706 M 0 52 R D 14223 6706 M 0 52 R D 14328 6706 M 0 52 R D +15044 6706 M 0 52 R D 15407 6706 M 0 52 R D 15665 6706 M 0 52 R D +15865 6706 M 0 52 R D 16029 6706 M 0 52 R D 16167 6706 M 0 52 R D +16286 6706 M 0 52 R D 16392 6706 M 0 52 R D 17107 6706 M 0 52 R D +gsave 13391 5710 translate 0 0 M 1.01 dup scale -58.8433 0 N +( ) show grestore 9675 11989 M 7432 0 R D 10296 11989 M 0 -106 R D +12359 11989 M 0 -106 R D 14423 11989 M 0 -106 R D 16486 11989 M 0 -106 R D +9675 11989 M 0 -53 R D 9838 11989 M 0 -53 R D 9976 11989 M 0 -53 R D +10096 11989 M 0 -53 R D 10202 11989 M 0 -53 R D 10917 11989 M 0 -53 R D +11281 11989 M 0 -53 R D 11538 11989 M 0 -53 R D 11738 11989 M 0 -53 R D +11902 11989 M 0 -53 R D 12040 11989 M 0 -53 R D 12159 11989 M 0 -53 R D +12265 11989 M 0 -53 R D 12981 11989 M 0 -53 R D 13344 11989 M 0 -53 R D +13602 11989 M 0 -53 R D 13802 11989 M 0 -53 R D 13965 11989 M 0 -53 R D +14103 11989 M 0 -53 R D 14223 11989 M 0 -53 R D 14328 11989 M 0 -53 R D +15044 11989 M 0 -53 R D 15407 11989 M 0 -53 R D 15665 11989 M 0 -53 R D +15865 11989 M 0 -53 R D 16029 11989 M 0 -53 R D 16167 11989 M 0 -53 R D +16286 11989 M 0 -53 R D 16392 11989 M 0 -53 R D 17107 11989 M 0 -53 R D +9675 6706 M 0 5283 R D 9675 6706 M 149 0 R D gsave 9563 6706 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9675 8026 M 149 0 R D gsave 9563 7884 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9675 9347 M 149 0 R D gsave 9563 9205 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9675 10668 M 149 0 R D gsave 9563 10526 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9675 11989 M 149 0 R D gsave 9563 11740 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9675 6838 M 74 0 R D 9675 6970 M 74 0 R D 9675 7102 M +74 0 R D 9675 7234 M 74 0 R D 9675 7366 M 74 0 R D 9675 7498 M 74 0 R D +9675 7630 M 74 0 R D 9675 7762 M 74 0 R D 9675 7894 M 74 0 R D 9675 8159 M +74 0 R D 9675 8291 M 74 0 R D 9675 8423 M 74 0 R D 9675 8555 M 74 0 R D +9675 8687 M 74 0 R D 9675 8819 M 74 0 R D 9675 8951 M 74 0 R D 9675 9083 M +74 0 R D 9675 9215 M 74 0 R D 9675 9479 M 74 0 R D 9675 9611 M 74 0 R D +9675 9744 M 74 0 R D 9675 9876 M 74 0 R D 9675 10008 M 74 0 R D 9675 10140 M +74 0 R D 9675 10272 M 74 0 R D 9675 10404 M 74 0 R D 9675 10536 M 74 0 R D +9675 10800 M 74 0 R D 9675 10932 M 74 0 R D 9675 11064 M 74 0 R D +9675 11197 M 74 0 R D 9675 11329 M 74 0 R D 9675 11461 M 74 0 R D +9675 11593 M 74 0 R D 9675 11725 M 74 0 R D 9675 11857 M 74 0 R D +gsave 9108 9347 translate 0 0 M 90 rotate 1.01 dup scale -58.8433 0 N +( ) show grestore 17107 6706 M 0 5283 R D 17107 6706 M -148 0 R D +17107 8026 M -148 0 R D 17107 9347 M -148 0 R D 17107 10668 M -148 0 R D +17107 11989 M -148 0 R D 17107 6838 M -74 0 R D 17107 6970 M -74 0 R D +17107 7102 M -74 0 R D 17107 7234 M -74 0 R D 17107 7366 M -74 0 R D +17107 7498 M -74 0 R D 17107 7630 M -74 0 R D 17107 7762 M -74 0 R D +17107 7894 M -74 0 R D 17107 8159 M -74 0 R D 17107 8291 M -74 0 R D +17107 8423 M -74 0 R D 17107 8555 M -74 0 R D 17107 8687 M -74 0 R D +17107 8819 M -74 0 R D 17107 8951 M -74 0 R D 17107 9083 M -74 0 R D +17107 9215 M -74 0 R D 17107 9479 M -74 0 R D 17107 9611 M -74 0 R D +17107 9744 M -74 0 R D 17107 9876 M -74 0 R D 17107 10008 M -74 0 R D +17107 10140 M -74 0 R D 17107 10272 M -74 0 R D 17107 10404 M -74 0 R D +17107 10536 M -74 0 R D 17107 10800 M -74 0 R D 17107 10932 M -74 0 R D +17107 11064 M -74 0 R D 17107 11197 M -74 0 R D 17107 11329 M -74 0 R D +17107 11461 M -74 0 R D 17107 11593 M -74 0 R D 17107 11725 M -74 0 R D +17107 11857 M -74 0 R D 20 setlinewidth 1.000 0.000 0.000 setrgbcolor +9674 6947 M 106 0 R 295 0 R 0 356 R 221 0 R 295 0 R 0 67 R 221 0 R 294 0 R +0 197 R 222 0 R 294 0 R 0 -289 R 222 0 R 294 0 R 0 5 R 221 0 R 295 0 R +0 115 R 221 0 R 295 0 R 0 272 R 221 0 R 295 0 R 0 918 R 221 0 R 295 0 R +0 -522 R 221 0 R 294 0 R 0 649 R 222 0 R 294 0 R 0 -741 R 222 0 R 294 0 R +0 -395 R 221 0 R 295 0 R 0 -559 R 221 0 R 295 0 R 0 -314 R 221 0 R 105 0 R D +L1 9674 7175 M 106 0 R 295 0 R 0 2 R 221 0 R 295 0 R 0 -46 R 221 0 R 294 0 R +0 -54 R 222 0 R 294 0 R 0 -146 R 222 0 R 294 0 R 0 376 R 221 0 R 295 0 R +0 120 R 221 0 R 295 0 R 0 284 R 221 0 R 295 0 R 0 957 R 221 0 R 295 0 R +0 -544 R 221 0 R 294 0 R 0 677 R 222 0 R 294 0 R 0 -773 R 222 0 R 294 0 R +0 -412 R 221 0 R 295 0 R 0 -582 R 221 0 R 295 0 R 0 -328 R 221 0 R 105 0 R D +40 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 9674 6706 M 106 0 R 295 0 R +221 0 R 295 0 R 221 0 R 294 0 R 222 0 R 294 0 R 222 0 R 294 0 R 221 0 R +295 0 R 221 0 R 295 0 R 0 89 R 221 0 R 295 0 R 0 488 R 221 0 R 295 0 R +0 238 R 221 0 R 294 0 R 0 833 R 222 0 R 294 0 R 0 2598 R 222 0 R 294 0 R +0 -1302 R 221 0 R 295 0 R 0 -585 R 221 0 R 295 0 R 0 -2359 R 221 0 R 105 0 R +D 20 setlinewidth L2 0.000 0.514 1.000 setrgbcolor 9674 6706 M 106 0 R +516 0 R 516 0 R 516 2 R 516 8 R 515 31 R 516 90 R 516 225 R 516 455 R +516 741 R 516 943 R 516 807 R 515 -323 R 516 -719 R 516 -819 R 105 -137 R D +0.000 0.000 0.000 setrgbcolor gsave 9838 11329 translate 0 0 M +1.25 dup scale +(Complete Sample) show grestore gsave 9838 10668 translate 0 0 M +1.25 dup scale +( z = 1.5 - 3.5) show grestore 13921 6720 M 0 278 R 277 0 R 0 -278 R +-277 0 R F +14284 7028 M 0 277 R 278 0 R 0 -277 R -278 0 R F +14647 7181 M 0 278 R 278 0 R 0 -278 R -278 0 R F +15011 7796 M 0 277 R 277 0 R 0 -277 R -277 0 R F +15374 9639 M 0 277 R 278 0 R 0 -277 R -278 0 R F +15738 11174 M 0 278 R 277 0 R 0 -278 R -277 0 R F +16101 8410 M 0 277 R 277 0 R 0 -277 R -277 0 R F +16464 7796 M 0 277 R 278 0 R 0 -277 R -278 0 R F +16828 8563 M 0 278 R 277 0 R 0 -278 R -277 0 R F +L0 14022 6706 M 75 0 R -37 0 R 0 307 R -38 0 R 75 0 R D 14386 6900 M 74 0 R +-37 0 R 0 532 R -37 0 R 74 0 R D 14749 7013 M 74 0 R -37 0 R 0 614 R -37 0 R +74 0 R D 15112 7500 M 75 0 R -37 0 R 0 869 R -38 0 R 75 0 R D 15476 9090 M +74 0 R -37 0 R 0 1374 R -37 0 R 74 0 R D 15839 10472 M 74 0 R -37 0 R +0 1517 R D 16202 8017 M 75 0 R -37 0 R 0 1064 R -38 0 R 75 0 R D +16566 7500 M 74 0 R -37 0 R 0 869 R -37 0 R 74 0 R D 16929 8148 M 74 0 R +-37 0 R 0 1108 R -37 0 R 74 0 R D 0.000 1.000 0.149 setrgbcolor 14152 6706 M +-1 18 R -3 17 R -6 18 R -8 16 R -10 15 R -12 14 R -14 12 R -15 10 R -16 8 R +-18 6 R -17 3 R -18 1 R -19 -1 R -17 -3 R -18 -6 R -16 -8 R -15 -10 R +-14 -12 R -12 -14 R -10 -15 R -8 -16 R -5 -18 R -4 -17 R -1 -18 R 0 -1 R +276 0 R 1 1 R F +14516 7036 M -2 18 R -3 18 R -6 17 R -8 16 R -10 15 R -12 14 R -14 12 R +-15 10 R -16 8 R -17 6 R -18 3 R -18 2 R -18 -2 R -18 -3 R -17 -6 R -16 -8 R +-16 -10 R -13 -12 R -12 -14 R -10 -15 R -8 -16 R -6 -17 R -4 -18 R -1 -18 R +1 -18 R 4 -18 R 6 -17 R 8 -17 R 10 -15 R 12 -13 R 13 -12 R 16 -10 R 16 -8 R +17 -6 R 18 -4 R 18 -1 R 18 1 R 18 4 R 17 6 R 16 8 R 15 10 R 14 12 R 12 13 R +10 15 R 8 17 R 6 17 R 3 18 R 2 18 R F +14879 8026 M -1 19 R -4 17 R -6 18 R -8 16 R -10 15 R -12 14 R -13 12 R +-15 10 R -17 8 R -17 5 R -18 4 R -18 1 R -18 -1 R -18 -4 R -17 -5 R -16 -8 R +-15 -10 R -14 -12 R -12 -14 R -10 -15 R -8 -16 R -6 -18 R -3 -17 R -2 -19 R +2 -18 R 3 -17 R 6 -18 R 8 -16 R 10 -15 R 12 -14 R 14 -12 R 15 -10 R 16 -8 R +17 -6 R 18 -3 R 18 -1 R 18 1 R 18 3 R 17 6 R 17 8 R 15 10 R 13 12 R 12 14 R +10 15 R 8 16 R 6 18 R 4 17 R 1 18 R F +15242 9017 M -1 18 R -3 18 R -6 17 R -8 16 R -10 16 R -12 13 R -14 12 R +-15 10 R -16 8 R -17 6 R -18 4 R -18 1 R -19 -1 R -17 -4 R -18 -6 R -16 -8 R +-15 -10 R -14 -12 R -11 -13 R -11 -16 R -8 -16 R -5 -17 R -4 -18 R -1 -18 R +1 -18 R 4 -18 R 5 -17 R 8 -16 R 11 -15 R 11 -14 R 14 -12 R 15 -10 R 16 -8 R +18 -6 R 17 -3 R 19 -2 R 18 2 R 18 3 R 17 6 R 16 8 R 15 10 R 14 12 R 12 14 R +10 15 R 8 16 R 6 17 R 3 18 R 1 18 R F +15606 10008 M -1 18 R -4 18 R -6 17 R -8 16 R -10 15 R -12 14 R -14 12 R +-15 10 R -16 8 R -17 6 R -18 3 R -18 1 R -18 -1 R -18 -3 R -17 -6 R -16 -8 R +-16 -10 R -13 -12 R -12 -14 R -10 -15 R -8 -16 R -6 -17 R -4 -18 R -1 -18 R +1 -18 R 4 -18 R 6 -17 R 8 -17 R 10 -15 R 12 -13 R 13 -12 R 16 -10 R 16 -8 R +17 -6 R 18 -4 R 18 -1 R 18 1 R 18 4 R 17 6 R 16 8 R 15 10 R 14 12 R 12 13 R +10 15 R 8 17 R 6 17 R 4 18 R 1 18 R F +15969 10668 M -1 18 R -4 18 R -6 17 R -8 17 R -10 15 R -12 13 R -13 12 R +-15 10 R -17 8 R -17 6 R -18 4 R -18 1 R -18 -1 R -18 -4 R -17 -6 R -16 -8 R +-15 -10 R -14 -12 R -12 -13 R -10 -15 R -8 -17 R -6 -17 R -3 -18 R -1 -18 R +1 -18 R 3 -18 R 6 -17 R 8 -16 R 10 -15 R 12 -14 R 14 -12 R 15 -10 R 16 -8 R +17 -6 R 18 -3 R 18 -2 R 18 2 R 18 3 R 17 6 R 17 8 R 15 10 R 13 12 R 12 14 R +10 15 R 8 16 R 6 17 R 4 18 R 1 18 R F +16332 8357 M -1 18 R -3 18 R -6 17 R -8 16 R -10 15 R -12 14 R -14 12 R +-15 10 R -16 8 R -17 6 R -18 3 R -18 1 R -18 -1 R -18 -3 R -17 -6 R -17 -8 R +-15 -10 R -13 -12 R -12 -14 R -11 -15 R -8 -16 R -5 -17 R -4 -18 R -1 -18 R +1 -18 R 4 -18 R 5 -17 R 8 -17 R 11 -15 R 12 -13 R 13 -12 R 15 -11 R 17 -8 R +17 -5 R 18 -4 R 18 -1 R 18 1 R 18 4 R 17 5 R 16 8 R 15 11 R 14 12 R 12 13 R +10 15 R 8 17 R 6 17 R 3 18 R 1 18 R F +16696 7036 M -1 18 R -4 18 R -6 17 R -8 16 R -10 15 R -12 14 R -14 12 R +-15 10 R -16 8 R -17 6 R -18 3 R -18 2 R -18 -2 R -18 -3 R -17 -6 R -16 -8 R +-15 -10 R -14 -12 R -12 -14 R -10 -15 R -8 -16 R -6 -17 R -4 -18 R -1 -18 R +1 -18 R 4 -18 R 6 -17 R 8 -17 R 10 -15 R 12 -13 R 14 -12 R 15 -10 R 16 -8 R +17 -6 R 18 -4 R 18 -1 R 18 1 R 18 4 R 17 6 R 16 8 R 15 10 R 14 12 R 12 13 R +10 15 R 8 17 R 6 17 R 4 18 R 1 18 R F +17059 8357 M -1 18 R -4 18 R -5 17 R -8 16 R -11 15 R -12 14 R -13 12 R +-15 10 R -17 8 R -17 6 R -18 3 R -18 1 R -18 -1 R -18 -3 R -17 -6 R -16 -8 R +-15 -10 R -14 -12 R -12 -14 R -10 -15 R -8 -16 R -6 -17 R -3 -18 R -1 -18 R +1 -18 R 3 -18 R 6 -17 R 8 -17 R 10 -15 R 12 -13 R 14 -12 R 15 -11 R 16 -8 R +17 -5 R 18 -4 R 18 -1 R 18 1 R 18 4 R 17 5 R 17 8 R 15 11 R 13 12 R 12 13 R +11 15 R 8 17 R 5 17 R 4 18 R 1 18 R F +13976 6706 M 75 0 R -37 0 R -38 0 R 75 0 R D 14340 6706 M 74 0 R -37 0 R +0 660 R -37 0 R 74 0 R D 14703 7366 M 74 0 R -37 0 R 0 1321 R -37 0 R 74 0 R +D 15066 8143 M 75 0 R -37 0 R 0 1748 R -38 0 R 75 0 R D 15430 8964 M 74 0 R +-37 0 R 0 2088 R -37 0 R 74 0 R D 15793 9524 M 74 0 R -37 0 R 0 2288 R +-37 0 R 74 0 R D 16156 7618 M 75 0 R -37 0 R 0 1477 R -38 0 R 75 0 R D +16520 6706 M 74 0 R -37 0 R 0 660 R -37 0 R 74 0 R D 16883 7618 M 75 0 R +-38 0 R 0 1477 R -37 0 R 75 0 R D 15 setlinewidth +0.000 0.000 0.000 setrgbcolor 2242 1422 M 7433 0 R D 2863 1422 M 0 106 R D +gsave 2863 889 translate 0 0 M 1.01 dup scale -529.59 0 N +(0.001) show grestore 4927 1422 M 0 106 R D gsave 4927 889 translate 0 0 M +1.01 dup scale -529.59 0 N +(0.010) show grestore 6990 1422 M 0 106 R D gsave 6990 889 translate 0 0 M +1.01 dup scale -529.59 0 N +(0.100) show grestore 9054 1422 M 0 106 R D gsave 9054 889 translate 0 0 M +1.01 dup scale -529.59 0 N +(1.000) show grestore 2242 1422 M 0 53 R D 2406 1422 M 0 53 R D 2544 1422 M +0 53 R D 2663 1422 M 0 53 R D 2769 1422 M 0 53 R D 3485 1422 M 0 53 R D +3848 1422 M 0 53 R D 4106 1422 M 0 53 R D 4306 1422 M 0 53 R D 4469 1422 M +0 53 R D 4607 1422 M 0 53 R D 4727 1422 M 0 53 R D 4832 1422 M 0 53 R D +5548 1422 M 0 53 R D 5911 1422 M 0 53 R D 6169 1422 M 0 53 R D 6369 1422 M +0 53 R D 6533 1422 M 0 53 R D 6671 1422 M 0 53 R D 6790 1422 M 0 53 R D +6896 1422 M 0 53 R D 7611 1422 M 0 53 R D 7975 1422 M 0 53 R D 8233 1422 M +0 53 R D 8433 1422 M 0 53 R D 8596 1422 M 0 53 R D 8734 1422 M 0 53 R D +8854 1422 M 0 53 R D 8959 1422 M 0 53 R D 9675 1422 M 0 53 R D +gsave 5959 427 translate 0 0 M 1.01 dup scale -58.8433 0 N +( ) show grestore 2242 6706 M 7433 0 R D 2863 6706 M 0 -106 R D 4927 6706 M +0 -106 R D 6990 6706 M 0 -106 R D 9054 6706 M 0 -106 R D 2242 6706 M 0 -53 R +D 2406 6706 M 0 -53 R D 2544 6706 M 0 -53 R D 2663 6706 M 0 -53 R D +2769 6706 M 0 -53 R D 3485 6706 M 0 -53 R D 3848 6706 M 0 -53 R D +4106 6706 M 0 -53 R D 4306 6706 M 0 -53 R D 4469 6706 M 0 -53 R D +4607 6706 M 0 -53 R D 4727 6706 M 0 -53 R D 4832 6706 M 0 -53 R D +5548 6706 M 0 -53 R D 5911 6706 M 0 -53 R D 6169 6706 M 0 -53 R D +6369 6706 M 0 -53 R D 6533 6706 M 0 -53 R D 6671 6706 M 0 -53 R D +6790 6706 M 0 -53 R D 6896 6706 M 0 -53 R D 7611 6706 M 0 -53 R D +7975 6706 M 0 -53 R D 8233 6706 M 0 -53 R D 8433 6706 M 0 -53 R D +8596 6706 M 0 -53 R D 8734 6706 M 0 -53 R D 8854 6706 M 0 -53 R D +8959 6706 M 0 -53 R D 9675 6706 M 0 -53 R D 2242 1422 M 0 5284 R D +2242 1422 M 149 0 R D gsave 2130 1422 translate 0 0 M 1.01 dup scale +-117.687 0 N +( ) show grestore 2242 2743 M 149 0 R D gsave 2130 2601 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 4064 M 149 0 R D gsave 2130 3922 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 5385 M 149 0 R D gsave 2130 5243 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 6706 M 149 0 R D gsave 2130 6457 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 1554 M 75 0 R D 2242 1686 M 75 0 R D 2242 1818 M +75 0 R D 2242 1950 M 75 0 R D 2242 2083 M 75 0 R D 2242 2215 M 75 0 R D +2242 2347 M 75 0 R D 2242 2479 M 75 0 R D 2242 2611 M 75 0 R D 2242 2875 M +75 0 R D 2242 3007 M 75 0 R D 2242 3139 M 75 0 R D 2242 3271 M 75 0 R D +2242 3403 M 75 0 R D 2242 3536 M 75 0 R D 2242 3668 M 75 0 R D 2242 3800 M +75 0 R D 2242 3932 M 75 0 R D 2242 4196 M 75 0 R D 2242 4328 M 75 0 R D +2242 4460 M 75 0 R D 2242 4592 M 75 0 R D 2242 4724 M 75 0 R D 2242 4856 M +75 0 R D 2242 4988 M 75 0 R D 2242 5121 M 75 0 R D 2242 5253 M 75 0 R D +2242 5517 M 75 0 R D 2242 5649 M 75 0 R D 2242 5781 M 75 0 R D 2242 5913 M +75 0 R D 2242 6045 M 75 0 R D 2242 6177 M 75 0 R D 2242 6309 M 75 0 R D +2242 6441 M 75 0 R D 2242 6573 M 75 0 R D gsave 1676 4064 translate 0 0 M +90 rotate 1.01 dup scale -58.8433 0 N +( ) show grestore 9675 1422 M 0 5284 R D 9675 1422 M -149 0 R D 9675 2743 M +-149 0 R D 9675 4064 M -149 0 R D 9675 5385 M -149 0 R D 9675 6706 M +-149 0 R D 9675 1554 M -74 0 R D 9675 1686 M -74 0 R D 9675 1818 M -74 0 R D +9675 1950 M -74 0 R D 9675 2083 M -74 0 R D 9675 2215 M -74 0 R D +9675 2347 M -74 0 R D 9675 2479 M -74 0 R D 9675 2611 M -74 0 R D +9675 2875 M -74 0 R D 9675 3007 M -74 0 R D 9675 3139 M -74 0 R D +9675 3271 M -74 0 R D 9675 3403 M -74 0 R D 9675 3536 M -74 0 R D +9675 3668 M -74 0 R D 9675 3800 M -74 0 R D 9675 3932 M -74 0 R D +9675 4196 M -74 0 R D 9675 4328 M -74 0 R D 9675 4460 M -74 0 R D +9675 4592 M -74 0 R D 9675 4724 M -74 0 R D 9675 4856 M -74 0 R D +9675 4988 M -74 0 R D 9675 5121 M -74 0 R D 9675 5253 M -74 0 R D +9675 5517 M -74 0 R D 9675 5649 M -74 0 R D 9675 5781 M -74 0 R D +9675 5913 M -74 0 R D 9675 6045 M -74 0 R D 9675 6177 M -74 0 R D +9675 6309 M -74 0 R D 9675 6441 M -74 0 R D 9675 6573 M -74 0 R D +20 setlinewidth 2242 1827 M 106 0 R 294 0 R 0 575 R 221 0 R 295 0 R 0 -462 R +221 0 R 295 0 R 0 522 R 221 0 R 295 0 R 0 -217 R 221 0 R 295 0 R 0 -362 R +221 0 R 294 0 R 0 43 R 222 0 R 294 0 R 0 773 R 222 0 R 294 0 R 0 -226 R +221 0 R 295 0 R 0 416 R 221 0 R 295 0 R 0 636 R 221 0 R 295 0 R 0 -924 R +221 0 R 295 0 R 0 -486 R 221 0 R 294 0 R 0 -479 R 222 0 R 294 0 R 0 -214 R +222 0 R 104 0 R D L1 2242 1958 M 106 0 R 294 0 R 0 49 R 221 0 R 295 0 R +0 -87 R 221 0 R 295 0 R 0 68 R 221 0 R 295 0 R 0 -172 R 221 0 R 295 0 R +0 133 R 221 0 R 294 0 R 0 49 R 222 0 R 294 0 R 0 884 R 222 0 R 294 0 R +0 -258 R 221 0 R 295 0 R 0 476 R 221 0 R 295 0 R 0 728 R 221 0 R 295 0 R +0 -1058 R 221 0 R 295 0 R 0 -556 R 221 0 R 294 0 R 0 -548 R 222 0 R 294 0 R +0 -244 R 222 0 R 104 0 R D gsave 2406 6045 translate 0 0 M 1.25 dup scale +(L = 10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(10) show +%%IncludeResource: font Symbol +262.467 /Symbol STDFONT +(\261) show +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(0.5) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( L) show CP X -101.051 M +%%IncludeResource: font AvantGarde-Book +262.467 /AvantGarde-Book STDFONT +(O) show M X -58.3193 M +%%IncludeResource: font AvantGarde-Book +186.267 /AvantGarde-Book STDFONT +( \267) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( << L) show X -101.051 M +%%IncludeResource: font Symbol +262.467 /Symbol STDFONT +(*) show +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 15 setlinewidth L0 9675 1422 M 7432 0 R D +10296 1422 M 0 106 R D gsave 10296 889 translate 0 0 M 1.01 dup scale +-529.59 0 N +(0.001) show grestore 12359 1422 M 0 106 R D gsave 12359 889 translate 0 0 M +1.01 dup scale -529.59 0 N +(0.010) show grestore 14423 1422 M 0 106 R D gsave 14423 889 translate 0 0 M +1.01 dup scale -529.59 0 N +(0.100) show grestore 16486 1422 M 0 106 R D gsave 16486 889 translate 0 0 M +1.01 dup scale -529.59 0 N +(1.000) show grestore 9675 1422 M 0 53 R D 9838 1422 M 0 53 R D 9976 1422 M +0 53 R D 10096 1422 M 0 53 R D 10202 1422 M 0 53 R D 10917 1422 M 0 53 R D +11281 1422 M 0 53 R D 11538 1422 M 0 53 R D 11738 1422 M 0 53 R D +11902 1422 M 0 53 R D 12040 1422 M 0 53 R D 12159 1422 M 0 53 R D +12265 1422 M 0 53 R D 12981 1422 M 0 53 R D 13344 1422 M 0 53 R D +13602 1422 M 0 53 R D 13802 1422 M 0 53 R D 13965 1422 M 0 53 R D +14103 1422 M 0 53 R D 14223 1422 M 0 53 R D 14328 1422 M 0 53 R D +15044 1422 M 0 53 R D 15407 1422 M 0 53 R D 15665 1422 M 0 53 R D +15865 1422 M 0 53 R D 16029 1422 M 0 53 R D 16167 1422 M 0 53 R D +16286 1422 M 0 53 R D 16392 1422 M 0 53 R D 17107 1422 M 0 53 R D +gsave 13391 427 translate 0 0 M 1.01 dup scale -58.8433 0 N +( ) show grestore 9675 6706 M 7432 0 R D 10296 6706 M 0 -106 R D +12359 6706 M 0 -106 R D 14423 6706 M 0 -106 R D 16486 6706 M 0 -106 R D +9675 6706 M 0 -53 R D 9838 6706 M 0 -53 R D 9976 6706 M 0 -53 R D +10096 6706 M 0 -53 R D 10202 6706 M 0 -53 R D 10917 6706 M 0 -53 R D +11281 6706 M 0 -53 R D 11538 6706 M 0 -53 R D 11738 6706 M 0 -53 R D +11902 6706 M 0 -53 R D 12040 6706 M 0 -53 R D 12159 6706 M 0 -53 R D +12265 6706 M 0 -53 R D 12981 6706 M 0 -53 R D 13344 6706 M 0 -53 R D +13602 6706 M 0 -53 R D 13802 6706 M 0 -53 R D 13965 6706 M 0 -53 R D +14103 6706 M 0 -53 R D 14223 6706 M 0 -53 R D 14328 6706 M 0 -53 R D +15044 6706 M 0 -53 R D 15407 6706 M 0 -53 R D 15665 6706 M 0 -53 R D +15865 6706 M 0 -53 R D 16029 6706 M 0 -53 R D 16167 6706 M 0 -53 R D +16286 6706 M 0 -53 R D 16392 6706 M 0 -53 R D 17107 6706 M 0 -53 R D +9675 1422 M 0 5284 R D 9675 1422 M 149 0 R D gsave 9563 1422 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9675 2743 M 149 0 R D gsave 9563 2601 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9675 4064 M 149 0 R D gsave 9563 3922 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9675 5385 M 149 0 R D gsave 9563 5243 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9675 6706 M 149 0 R D gsave 9563 6457 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9675 1554 M 74 0 R D 9675 1686 M 74 0 R D 9675 1818 M +74 0 R D 9675 1950 M 74 0 R D 9675 2083 M 74 0 R D 9675 2215 M 74 0 R D +9675 2347 M 74 0 R D 9675 2479 M 74 0 R D 9675 2611 M 74 0 R D 9675 2875 M +74 0 R D 9675 3007 M 74 0 R D 9675 3139 M 74 0 R D 9675 3271 M 74 0 R D +9675 3403 M 74 0 R D 9675 3536 M 74 0 R D 9675 3668 M 74 0 R D 9675 3800 M +74 0 R D 9675 3932 M 74 0 R D 9675 4196 M 74 0 R D 9675 4328 M 74 0 R D +9675 4460 M 74 0 R D 9675 4592 M 74 0 R D 9675 4724 M 74 0 R D 9675 4856 M +74 0 R D 9675 4988 M 74 0 R D 9675 5121 M 74 0 R D 9675 5253 M 74 0 R D +9675 5517 M 74 0 R D 9675 5649 M 74 0 R D 9675 5781 M 74 0 R D 9675 5913 M +74 0 R D 9675 6045 M 74 0 R D 9675 6177 M 74 0 R D 9675 6309 M 74 0 R D +9675 6441 M 74 0 R D 9675 6573 M 74 0 R D gsave 9108 4064 translate 0 0 M +90 rotate 1.01 dup scale -58.8433 0 N +( ) show grestore 17107 1422 M 0 5284 R D 17107 1422 M -148 0 R D +17107 2743 M -148 0 R D 17107 4064 M -148 0 R D 17107 5385 M -148 0 R D +17107 6706 M -148 0 R D 17107 1554 M -74 0 R D 17107 1686 M -74 0 R D +17107 1818 M -74 0 R D 17107 1950 M -74 0 R D 17107 2083 M -74 0 R D +17107 2215 M -74 0 R D 17107 2347 M -74 0 R D 17107 2479 M -74 0 R D +17107 2611 M -74 0 R D 17107 2875 M -74 0 R D 17107 3007 M -74 0 R D +17107 3139 M -74 0 R D 17107 3271 M -74 0 R D 17107 3403 M -74 0 R D +17107 3536 M -74 0 R D 17107 3668 M -74 0 R D 17107 3800 M -74 0 R D +17107 3932 M -74 0 R D 17107 4196 M -74 0 R D 17107 4328 M -74 0 R D +17107 4460 M -74 0 R D 17107 4592 M -74 0 R D 17107 4724 M -74 0 R D +17107 4856 M -74 0 R D 17107 4988 M -74 0 R D 17107 5121 M -74 0 R D +17107 5253 M -74 0 R D 17107 5517 M -74 0 R D 17107 5649 M -74 0 R D +17107 5781 M -74 0 R D 17107 5913 M -74 0 R D 17107 6045 M -74 0 R D +17107 6177 M -74 0 R D 17107 6309 M -74 0 R D 17107 6441 M -74 0 R D +17107 6573 M -74 0 R D 20 setlinewidth 9674 1422 M 106 0 R 295 0 R 221 0 R +295 0 R 221 0 R 294 0 R 222 0 R 294 0 R 222 0 R 294 0 R 221 0 R 295 0 R +221 0 R 295 0 R 221 0 R 295 0 R 0 60 R 221 0 R 295 0 R 0 405 R 221 0 R +294 0 R 0 203 R 222 0 R 294 0 R 0 252 R 222 0 R 294 0 R 0 3200 R 221 0 R +295 0 R 0 990 R 221 0 R 295 0 R 0 -5110 R 221 0 R 105 0 R D L1 9674 1422 M +106 0 R 295 0 R 221 0 R 295 0 R 221 0 R 294 0 R 222 0 R 294 0 R 222 0 R +294 0 R 221 0 R 295 0 R 221 0 R 295 0 R 221 0 R 295 0 R 0 60 R 221 0 R +295 0 R 0 405 R 221 0 R 294 0 R 0 203 R 222 0 R 294 0 R 0 252 R 222 0 R +294 0 R 0 3200 R 221 0 R 295 0 R 0 990 R 221 0 R 295 0 R 0 -5110 R 221 0 R +105 0 R D 40 setlinewidth L0 1.000 0.000 0.000 setrgbcolor 9674 1422 M +106 0 R 295 0 R 221 0 R 295 0 R 221 0 R 294 0 R 222 0 R 294 0 R 222 0 R +294 0 R 221 0 R 295 0 R 221 0 R 295 0 R 221 0 R 295 0 R 0 323 R 221 0 R +295 0 R 0 746 R 221 0 R 294 0 R 0 267 R 222 0 R 294 0 R 0 3677 R 222 0 R +294 0 R 0 -755 R 221 0 R 295 0 R 0 -3048 R 221 0 R 295 0 R 0 -1210 R 221 0 R +105 0 R D 0.000 0.000 0.000 setrgbcolor gsave 9838 6045 translate 0 0 M +1.25 dup scale +(L = 10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(13) show +%%IncludeResource: font Symbol +262.467 /Symbol STDFONT +(\261) show +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(0.5) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( L) show CP X -101.051 M +%%IncludeResource: font AvantGarde-Book +262.467 /AvantGarde-Book STDFONT +(O) show M X -58.3193 M +%%IncludeResource: font AvantGarde-Book +186.267 /AvantGarde-Book STDFONT +( \267) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( >> L) show X -101.051 M +%%IncludeResource: font Symbol +262.467 /Symbol STDFONT +(*) show +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT gsave 9675 365 translate 0 0 M 1.01 dup scale +-2136.1 0 N +(Eddington Ratio L/L) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(EDD) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT gsave 1499 6706 translate 0 0 M 90 rotate +1.01 dup scale -2575.77 0 N +(Probability \(Arbitrary Scale\)) show grestore +%%PageTrailer +end +restore +showpage +%%PageResources: font Helvetica +%%+ font Symbol +%%+ font AvantGarde-Book +%%Trailer +restore +%%Pages: 1 +%%DocumentNeededResources: font Helvetica +%%+ font Symbol +%%+ font AvantGarde-Book +%%EOF diff --git a/feedback/papers/0506398/f21.ps b/feedback/papers/0506398/f21.ps new file mode 100644 index 0000000..e218cff --- /dev/null +++ b/feedback/papers/0506398/f21.ps @@ -0,0 +1,1025 @@ +%!PS-Adobe-3.0 +%%BoundingBox: 54 360 558 720 +%%Title: Graphics produced by IDL +%%For: phopkins@zeus, /home/phopkins/montecarlo_runs +%%Creator: IDL Version 6.1.1 (linux x86 m32) +%%CreationDate: Mon Aug 29 14:33:44 2005 +%%DocumentData: Clean7bit +%%Requirements: color +%%LanguageLevel: 1 +%%PageOrder: Ascend +%%Pages: (atend) +%%DocumentNeededResources: (atend) +%%EndComments +%%BeginProlog +save +%+ prolog.ps -- Prolog for IDL generated PostScript files +%+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. +%v 5 +/$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C +{currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint +stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} +bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show +grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 +setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 +{[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 +100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 +{[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef +/ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} +ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont +exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica +findfont exch scalefont setfont (\267) show currentpoint grestore moveto} +bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end +%%EndProlog +%%Page: 0 1 +%%PageRequirements: color +%%PageResources: (atend) +%%PageOrientation: Portrait +%%PageBoundingBox: 54 360 558 720 +%%BeginPageSetup +save +$IDL_DICT begin 54 360 translate 0.0283465 dup scale MITERLIMIT +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +%%EndPageSetup +15 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 2242 8467 M 4955 0 R D +2242 8467 M 0 70 R D gsave 2242 7933 translate 0 0 M 1.01 dup scale +-58.8433 0 N +( ) show grestore 3143 8467 M 0 70 R D gsave 3143 7933 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 4044 8467 M 0 70 R D gsave 4044 7933 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 4945 8467 M 0 70 R D gsave 4945 7933 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 5846 8467 M 0 70 R D gsave 5846 7933 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 6747 8467 M 0 70 R D gsave 6747 7933 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 2332 8467 M 0 35 R D 2422 8467 M 0 35 R D 2513 8467 M +0 35 R D 2603 8467 M 0 35 R D 2693 8467 M 0 35 R D 2783 8467 M 0 35 R D +2873 8467 M 0 35 R D 2963 8467 M 0 35 R D 3053 8467 M 0 35 R D 3233 8467 M +0 35 R D 3323 8467 M 0 35 R D 3413 8467 M 0 35 R D 3504 8467 M 0 35 R D +3594 8467 M 0 35 R D 3684 8467 M 0 35 R D 3774 8467 M 0 35 R D 3864 8467 M +0 35 R D 3954 8467 M 0 35 R D 4134 8467 M 0 35 R D 4224 8467 M 0 35 R D +4314 8467 M 0 35 R D 4404 8467 M 0 35 R D 4495 8467 M 0 35 R D 4585 8467 M +0 35 R D 4675 8467 M 0 35 R D 4765 8467 M 0 35 R D 4855 8467 M 0 35 R D +5035 8467 M 0 35 R D 5125 8467 M 0 35 R D 5215 8467 M 0 35 R D 5305 8467 M +0 35 R D 5396 8467 M 0 35 R D 5486 8467 M 0 35 R D 5576 8467 M 0 35 R D +5666 8467 M 0 35 R D 5756 8467 M 0 35 R D 5936 8467 M 0 35 R D 6026 8467 M +0 35 R D 6116 8467 M 0 35 R D 6206 8467 M 0 35 R D 6296 8467 M 0 35 R D +6387 8467 M 0 35 R D 6477 8467 M 0 35 R D 6567 8467 M 0 35 R D 6657 8467 M +0 35 R D 6837 8467 M 0 35 R D 6927 8467 M 0 35 R D 7017 8467 M 0 35 R D +7107 8467 M 0 35 R D 7197 8467 M 0 35 R D 2242 11989 M 4955 0 R D +2242 11989 M 0 -70 R D 3143 11989 M 0 -70 R D 4044 11989 M 0 -70 R D +4945 11989 M 0 -70 R D 5846 11989 M 0 -70 R D 6747 11989 M 0 -70 R D +2332 11989 M 0 -35 R D 2422 11989 M 0 -35 R D 2513 11989 M 0 -35 R D +2603 11989 M 0 -35 R D 2693 11989 M 0 -35 R D 2783 11989 M 0 -35 R D +2873 11989 M 0 -35 R D 2963 11989 M 0 -35 R D 3053 11989 M 0 -35 R D +3233 11989 M 0 -35 R D 3323 11989 M 0 -35 R D 3413 11989 M 0 -35 R D +3504 11989 M 0 -35 R D 3594 11989 M 0 -35 R D 3684 11989 M 0 -35 R D +3774 11989 M 0 -35 R D 3864 11989 M 0 -35 R D 3954 11989 M 0 -35 R D +4134 11989 M 0 -35 R D 4224 11989 M 0 -35 R D 4314 11989 M 0 -35 R D +4404 11989 M 0 -35 R D 4495 11989 M 0 -35 R D 4585 11989 M 0 -35 R D +4675 11989 M 0 -35 R D 4765 11989 M 0 -35 R D 4855 11989 M 0 -35 R D +5035 11989 M 0 -35 R D 5125 11989 M 0 -35 R D 5215 11989 M 0 -35 R D +5305 11989 M 0 -35 R D 5396 11989 M 0 -35 R D 5486 11989 M 0 -35 R D +5576 11989 M 0 -35 R D 5666 11989 M 0 -35 R D 5756 11989 M 0 -35 R D +5936 11989 M 0 -35 R D 6026 11989 M 0 -35 R D 6116 11989 M 0 -35 R D +6206 11989 M 0 -35 R D 6296 11989 M 0 -35 R D 6387 11989 M 0 -35 R D +6477 11989 M 0 -35 R D 6567 11989 M 0 -35 R D 6657 11989 M 0 -35 R D +6837 11989 M 0 -35 R D 6927 11989 M 0 -35 R D 7017 11989 M 0 -35 R D +7107 11989 M 0 -35 R D 7197 11989 M 0 -35 R D 2242 8467 M 0 3522 R D +2242 8467 M 99 0 R D gsave 2130 8467 translate 0 0 M 1.01 dup scale +-117.687 0 N +( ) show grestore 2242 8936 M 99 0 R D gsave 2130 8794 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 9406 M 99 0 R D gsave 2130 9264 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 9876 M 99 0 R D gsave 2130 9733 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 10345 M 99 0 R D gsave 2130 10203 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 10815 M 99 0 R D gsave 2130 10673 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 11285 M 99 0 R D gsave 2130 11142 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 11754 M 99 0 R D gsave 2130 11612 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 8584 M 50 0 R D 2242 8702 M 50 0 R D 2242 8819 M +50 0 R D 2242 9054 M 50 0 R D 2242 9171 M 50 0 R D 2242 9289 M 50 0 R D +2242 9523 M 50 0 R D 2242 9641 M 50 0 R D 2242 9758 M 50 0 R D 2242 9993 M +50 0 R D 2242 10110 M 50 0 R D 2242 10228 M 50 0 R D 2242 10463 M 50 0 R D +2242 10580 M 50 0 R D 2242 10698 M 50 0 R D 2242 10932 M 50 0 R D +2242 11050 M 50 0 R D 2242 11167 M 50 0 R D 2242 11402 M 50 0 R D +2242 11519 M 50 0 R D 2242 11637 M 50 0 R D 2242 11872 M 50 0 R D +2242 11989 M 50 0 R D 7197 8467 M 0 3522 R D 7197 8467 M -99 0 R D +7197 8936 M -99 0 R D 7197 9406 M -99 0 R D 7197 9876 M -99 0 R D +7197 10345 M -99 0 R D 7197 10815 M -99 0 R D 7197 11285 M -99 0 R D +7197 11754 M -99 0 R D 7197 8584 M -49 0 R D 7197 8702 M -49 0 R D +7197 8819 M -49 0 R D 7197 9054 M -49 0 R D 7197 9171 M -49 0 R D +7197 9289 M -49 0 R D 7197 9523 M -49 0 R D 7197 9641 M -49 0 R D +7197 9758 M -49 0 R D 7197 9993 M -49 0 R D 7197 10110 M -49 0 R D +7197 10228 M -49 0 R D 7197 10463 M -49 0 R D 7197 10580 M -49 0 R D +7197 10698 M -49 0 R D 7197 10932 M -49 0 R D 7197 11050 M -49 0 R D +7197 11167 M -49 0 R D 7197 11402 M -49 0 R D 7197 11519 M -49 0 R D +7197 11637 M -49 0 R D 7197 11872 M -49 0 R D 7197 11989 M -49 0 R D +20 setlinewidth 1.000 0.000 0.000 setrgbcolor 2242 8467 M 226 0 R 225 0 R +225 0 R 225 0 R 225 0 R 226 0 R 225 0 R 0 3 R 225 0 R 225 0 R 0 78 R 226 0 R +225 0 R 0 408 R 225 0 R 225 0 R 0 819 R 226 0 R 225 0 R 0 724 R 225 0 R +225 0 R 0 -1253 R 225 0 R 226 0 R 0 -776 R 225 0 R 225 0 R 0 -3 R 225 0 R D +0.000 0.514 1.000 setrgbcolor 2242 8467 M 226 0 R 225 0 R 225 0 R 225 0 R +225 0 R 226 0 R 225 0 R 225 0 R 225 0 R 226 0 R 225 0 R 225 0 R 225 0 R +0 917 R 226 0 R 225 0 R 0 1350 R 225 0 R 225 0 R 0 -756 R 225 0 R 226 0 R +0 -1511 R 225 0 R 225 0 R 225 0 R D 0.000 0.000 0.000 setrgbcolor +2242 8467 M 226 0 R 225 0 R 225 0 R 225 0 R 225 0 R 226 0 R 225 0 R 225 0 R +225 0 R 226 0 R 225 0 R 225 0 R 225 0 R 226 0 R 225 0 R 225 0 R 225 0 R +0 3354 R 225 0 R 226 0 R 0 -3354 R 225 0 R 225 0 R 225 0 R D +gsave 2513 11285 translate 0 0 M 1.2 dup scale +(z = 0.5) show grestore 1.000 0.000 0.000 setrgbcolor +gsave 2693 10580 translate 0 0 M 1.01 dup scale +(M) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(B) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( < -19) show grestore 0.000 0.514 1.000 setrgbcolor +gsave 2693 10110 translate 0 0 M 1.01 dup scale +(M) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(B) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( < -22) show grestore 0.000 0.000 0.000 setrgbcolor +gsave 2693 9641 translate 0 0 M 1.01 dup scale +(M) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(B) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( < -25) show grestore 15 setlinewidth 7197 8467 M 4955 0 R D 7197 8467 M +0 70 R D gsave 7197 7933 translate 0 0 M 1.01 dup scale -58.8433 0 N +( ) show grestore 8098 8467 M 0 70 R D gsave 8098 7933 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 8999 8467 M 0 70 R D gsave 8999 7933 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 9900 8467 M 0 70 R D gsave 9900 7933 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 10801 8467 M 0 70 R D gsave 10801 7933 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 11702 8467 M 0 70 R D gsave 11702 7933 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 7287 8467 M 0 35 R D 7378 8467 M 0 35 R D 7468 8467 M +0 35 R D 7558 8467 M 0 35 R D 7648 8467 M 0 35 R D 7738 8467 M 0 35 R D +7828 8467 M 0 35 R D 7918 8467 M 0 35 R D 8008 8467 M 0 35 R D 8188 8467 M +0 35 R D 8278 8467 M 0 35 R D 8369 8467 M 0 35 R D 8459 8467 M 0 35 R D +8549 8467 M 0 35 R D 8639 8467 M 0 35 R D 8729 8467 M 0 35 R D 8819 8467 M +0 35 R D 8909 8467 M 0 35 R D 9089 8467 M 0 35 R D 9179 8467 M 0 35 R D +9269 8467 M 0 35 R D 9360 8467 M 0 35 R D 9450 8467 M 0 35 R D 9540 8467 M +0 35 R D 9630 8467 M 0 35 R D 9720 8467 M 0 35 R D 9810 8467 M 0 35 R D +9990 8467 M 0 35 R D 10080 8467 M 0 35 R D 10170 8467 M 0 35 R D +10260 8467 M 0 35 R D 10351 8467 M 0 35 R D 10441 8467 M 0 35 R D +10531 8467 M 0 35 R D 10621 8467 M 0 35 R D 10711 8467 M 0 35 R D +10891 8467 M 0 35 R D 10981 8467 M 0 35 R D 11071 8467 M 0 35 R D +11161 8467 M 0 35 R D 11251 8467 M 0 35 R D 11342 8467 M 0 35 R D +11432 8467 M 0 35 R D 11522 8467 M 0 35 R D 11612 8467 M 0 35 R D +11792 8467 M 0 35 R D 11882 8467 M 0 35 R D 11972 8467 M 0 35 R D +12062 8467 M 0 35 R D 12152 8467 M 0 35 R D 7197 11989 M 4955 0 R D +7197 11989 M 0 -70 R D 8098 11989 M 0 -70 R D 8999 11989 M 0 -70 R D +9900 11989 M 0 -70 R D 10801 11989 M 0 -70 R D 11702 11989 M 0 -70 R D +7287 11989 M 0 -35 R D 7378 11989 M 0 -35 R D 7468 11989 M 0 -35 R D +7558 11989 M 0 -35 R D 7648 11989 M 0 -35 R D 7738 11989 M 0 -35 R D +7828 11989 M 0 -35 R D 7918 11989 M 0 -35 R D 8008 11989 M 0 -35 R D +8188 11989 M 0 -35 R D 8278 11989 M 0 -35 R D 8369 11989 M 0 -35 R D +8459 11989 M 0 -35 R D 8549 11989 M 0 -35 R D 8639 11989 M 0 -35 R D +8729 11989 M 0 -35 R D 8819 11989 M 0 -35 R D 8909 11989 M 0 -35 R D +9089 11989 M 0 -35 R D 9179 11989 M 0 -35 R D 9269 11989 M 0 -35 R D +9360 11989 M 0 -35 R D 9450 11989 M 0 -35 R D 9540 11989 M 0 -35 R D +9630 11989 M 0 -35 R D 9720 11989 M 0 -35 R D 9810 11989 M 0 -35 R D +9990 11989 M 0 -35 R D 10080 11989 M 0 -35 R D 10170 11989 M 0 -35 R D +10260 11989 M 0 -35 R D 10351 11989 M 0 -35 R D 10441 11989 M 0 -35 R D +10531 11989 M 0 -35 R D 10621 11989 M 0 -35 R D 10711 11989 M 0 -35 R D +10891 11989 M 0 -35 R D 10981 11989 M 0 -35 R D 11071 11989 M 0 -35 R D +11161 11989 M 0 -35 R D 11251 11989 M 0 -35 R D 11342 11989 M 0 -35 R D +11432 11989 M 0 -35 R D 11522 11989 M 0 -35 R D 11612 11989 M 0 -35 R D +11792 11989 M 0 -35 R D 11882 11989 M 0 -35 R D 11972 11989 M 0 -35 R D +12062 11989 M 0 -35 R D 12152 11989 M 0 -35 R D 7197 8467 M 0 3522 R D +7197 8467 M 99 0 R D gsave 7085 8467 translate 0 0 M 1.01 dup scale +-117.687 0 N +( ) show grestore 7197 8936 M 99 0 R D gsave 7085 8794 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 9406 M 99 0 R D gsave 7085 9264 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 9876 M 99 0 R D gsave 7085 9733 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 10345 M 99 0 R D gsave 7085 10203 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 10815 M 99 0 R D gsave 7085 10673 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 11285 M 99 0 R D gsave 7085 11142 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 11754 M 99 0 R D gsave 7085 11612 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 8584 M 50 0 R D 7197 8702 M 50 0 R D 7197 8819 M +50 0 R D 7197 9054 M 50 0 R D 7197 9171 M 50 0 R D 7197 9289 M 50 0 R D +7197 9523 M 50 0 R D 7197 9641 M 50 0 R D 7197 9758 M 50 0 R D 7197 9993 M +50 0 R D 7197 10110 M 50 0 R D 7197 10228 M 50 0 R D 7197 10463 M 50 0 R D +7197 10580 M 50 0 R D 7197 10698 M 50 0 R D 7197 10932 M 50 0 R D +7197 11050 M 50 0 R D 7197 11167 M 50 0 R D 7197 11402 M 50 0 R D +7197 11519 M 50 0 R D 7197 11637 M 50 0 R D 7197 11872 M 50 0 R D +7197 11989 M 50 0 R D 12152 8467 M 0 3522 R D 12152 8467 M -99 0 R D +12152 8936 M -99 0 R D 12152 9406 M -99 0 R D 12152 9876 M -99 0 R D +12152 10345 M -99 0 R D 12152 10815 M -99 0 R D 12152 11285 M -99 0 R D +12152 11754 M -99 0 R D 12152 8584 M -49 0 R D 12152 8702 M -49 0 R D +12152 8819 M -49 0 R D 12152 9054 M -49 0 R D 12152 9171 M -49 0 R D +12152 9289 M -49 0 R D 12152 9523 M -49 0 R D 12152 9641 M -49 0 R D +12152 9758 M -49 0 R D 12152 9993 M -49 0 R D 12152 10110 M -49 0 R D +12152 10228 M -49 0 R D 12152 10463 M -49 0 R D 12152 10580 M -49 0 R D +12152 10698 M -49 0 R D 12152 10932 M -49 0 R D 12152 11050 M -49 0 R D +12152 11167 M -49 0 R D 12152 11402 M -49 0 R D 12152 11519 M -49 0 R D +12152 11637 M -49 0 R D 12152 11872 M -49 0 R D 12152 11989 M -49 0 R D +20 setlinewidth 1.000 0.000 0.000 setrgbcolor 7197 8471 M 226 0 R 0 12 R +225 0 R 225 0 R 0 38 R 225 0 R 225 0 R 0 193 R 226 0 R 225 0 R 0 193 R +225 0 R 225 0 R 0 329 R 226 0 R 225 0 R 0 416 R 225 0 R 225 0 R 0 -564 R +226 0 R 225 0 R 0 -75 R 225 0 R 225 0 R 0 -19 R 225 0 R 226 0 R 0 -243 R +225 0 R 225 0 R 0 -283 R 225 0 R D 0.000 0.514 1.000 setrgbcolor 7197 8467 M +226 0 R 225 0 R 225 0 R 225 0 R 225 0 R 226 0 R 225 0 R 0 122 R 225 0 R +225 0 R 0 123 R 226 0 R 225 0 R 0 137 R 225 0 R 225 0 R 0 251 R 226 0 R +225 0 R 0 815 R 225 0 R 225 0 R 0 91 R 225 0 R 226 0 R 0 -1219 R 225 0 R +225 0 R 0 -316 R 225 0 R D 0.000 0.000 0.000 setrgbcolor 7197 8467 M 226 0 R +225 0 R 225 0 R 225 0 R 225 0 R 226 0 R 225 0 R 225 0 R 225 0 R 226 0 R +225 0 R 225 0 R 225 0 R 0 94 R 226 0 R 225 0 R 0 2817 R 225 0 R 225 0 R +0 -1221 R 225 0 R 226 0 R 0 -1690 R 225 0 R 225 0 R 225 0 R D +1.000 0.000 0.000 setrgbcolor gsave 7648 11285 translate 0 0 M +1.01 dup scale +(log L) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(SX) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( > 40) show grestore 0.000 0.514 1.000 setrgbcolor +gsave 7648 10815 translate 0 0 M 1.01 dup scale +(log L) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(SX) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( > 42) show grestore 0.000 0.000 0.000 setrgbcolor +gsave 7648 10345 translate 0 0 M 1.01 dup scale +(log L) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(SX) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( > 44) show grestore 15 setlinewidth 12152 8467 M 4955 0 R D 12152 8467 M +0 70 R D gsave 12152 7933 translate 0 0 M 1.01 dup scale -58.8433 0 N +( ) show grestore 13053 8467 M 0 70 R D gsave 13053 7933 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 13954 8467 M 0 70 R D gsave 13954 7933 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 14855 8467 M 0 70 R D gsave 14855 7933 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 15756 8467 M 0 70 R D gsave 15756 7933 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 16657 8467 M 0 70 R D gsave 16657 7933 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 12242 8467 M 0 35 R D 12333 8467 M 0 35 R D 12423 8467 M +0 35 R D 12513 8467 M 0 35 R D 12603 8467 M 0 35 R D 12693 8467 M 0 35 R D +12783 8467 M 0 35 R D 12873 8467 M 0 35 R D 12963 8467 M 0 35 R D +13143 8467 M 0 35 R D 13233 8467 M 0 35 R D 13324 8467 M 0 35 R D +13414 8467 M 0 35 R D 13504 8467 M 0 35 R D 13594 8467 M 0 35 R D +13684 8467 M 0 35 R D 13774 8467 M 0 35 R D 13864 8467 M 0 35 R D +14044 8467 M 0 35 R D 14134 8467 M 0 35 R D 14224 8467 M 0 35 R D +14315 8467 M 0 35 R D 14405 8467 M 0 35 R D 14495 8467 M 0 35 R D +14585 8467 M 0 35 R D 14675 8467 M 0 35 R D 14765 8467 M 0 35 R D +14945 8467 M 0 35 R D 15035 8467 M 0 35 R D 15125 8467 M 0 35 R D +15216 8467 M 0 35 R D 15306 8467 M 0 35 R D 15396 8467 M 0 35 R D +15486 8467 M 0 35 R D 15576 8467 M 0 35 R D 15666 8467 M 0 35 R D +15846 8467 M 0 35 R D 15936 8467 M 0 35 R D 16026 8467 M 0 35 R D +16116 8467 M 0 35 R D 16207 8467 M 0 35 R D 16297 8467 M 0 35 R D +16387 8467 M 0 35 R D 16477 8467 M 0 35 R D 16567 8467 M 0 35 R D +16747 8467 M 0 35 R D 16837 8467 M 0 35 R D 16927 8467 M 0 35 R D +17017 8467 M 0 35 R D 17107 8467 M 0 35 R D 12152 11989 M 4955 0 R D +12152 11989 M 0 -70 R D 13053 11989 M 0 -70 R D 13954 11989 M 0 -70 R D +14855 11989 M 0 -70 R D 15756 11989 M 0 -70 R D 16657 11989 M 0 -70 R D +12242 11989 M 0 -35 R D 12333 11989 M 0 -35 R D 12423 11989 M 0 -35 R D +12513 11989 M 0 -35 R D 12603 11989 M 0 -35 R D 12693 11989 M 0 -35 R D +12783 11989 M 0 -35 R D 12873 11989 M 0 -35 R D 12963 11989 M 0 -35 R D +13143 11989 M 0 -35 R D 13233 11989 M 0 -35 R D 13324 11989 M 0 -35 R D +13414 11989 M 0 -35 R D 13504 11989 M 0 -35 R D 13594 11989 M 0 -35 R D +13684 11989 M 0 -35 R D 13774 11989 M 0 -35 R D 13864 11989 M 0 -35 R D +14044 11989 M 0 -35 R D 14134 11989 M 0 -35 R D 14224 11989 M 0 -35 R D +14315 11989 M 0 -35 R D 14405 11989 M 0 -35 R D 14495 11989 M 0 -35 R D +14585 11989 M 0 -35 R D 14675 11989 M 0 -35 R D 14765 11989 M 0 -35 R D +14945 11989 M 0 -35 R D 15035 11989 M 0 -35 R D 15125 11989 M 0 -35 R D +15216 11989 M 0 -35 R D 15306 11989 M 0 -35 R D 15396 11989 M 0 -35 R D +15486 11989 M 0 -35 R D 15576 11989 M 0 -35 R D 15666 11989 M 0 -35 R D +15846 11989 M 0 -35 R D 15936 11989 M 0 -35 R D 16026 11989 M 0 -35 R D +16116 11989 M 0 -35 R D 16207 11989 M 0 -35 R D 16297 11989 M 0 -35 R D +16387 11989 M 0 -35 R D 16477 11989 M 0 -35 R D 16567 11989 M 0 -35 R D +16747 11989 M 0 -35 R D 16837 11989 M 0 -35 R D 16927 11989 M 0 -35 R D +17017 11989 M 0 -35 R D 17107 11989 M 0 -35 R D 12152 8467 M 0 3522 R D +12152 8467 M 99 0 R D gsave 12040 8467 translate 0 0 M 1.01 dup scale +-117.687 0 N +( ) show grestore 12152 8936 M 99 0 R D gsave 12040 8794 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 9406 M 99 0 R D gsave 12040 9264 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 9876 M 99 0 R D gsave 12040 9733 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 10345 M 99 0 R D gsave 12040 10203 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 10815 M 99 0 R D gsave 12040 10673 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 11285 M 99 0 R D gsave 12040 11142 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 11754 M 99 0 R D gsave 12040 11612 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 8584 M 50 0 R D 12152 8702 M 50 0 R D 12152 8819 M +50 0 R D 12152 9054 M 50 0 R D 12152 9171 M 50 0 R D 12152 9289 M 50 0 R D +12152 9523 M 50 0 R D 12152 9641 M 50 0 R D 12152 9758 M 50 0 R D +12152 9993 M 50 0 R D 12152 10110 M 50 0 R D 12152 10228 M 50 0 R D +12152 10463 M 50 0 R D 12152 10580 M 50 0 R D 12152 10698 M 50 0 R D +12152 10932 M 50 0 R D 12152 11050 M 50 0 R D 12152 11167 M 50 0 R D +12152 11402 M 50 0 R D 12152 11519 M 50 0 R D 12152 11637 M 50 0 R D +12152 11872 M 50 0 R D 12152 11989 M 50 0 R D 17107 8467 M 0 3522 R D +17107 8467 M -99 0 R D 17107 8936 M -99 0 R D 17107 9406 M -99 0 R D +17107 9876 M -99 0 R D 17107 10345 M -99 0 R D 17107 10815 M -99 0 R D +17107 11285 M -99 0 R D 17107 11754 M -99 0 R D 17107 8584 M -49 0 R D +17107 8702 M -49 0 R D 17107 8819 M -49 0 R D 17107 9054 M -49 0 R D +17107 9171 M -49 0 R D 17107 9289 M -49 0 R D 17107 9523 M -49 0 R D +17107 9641 M -49 0 R D 17107 9758 M -49 0 R D 17107 9993 M -49 0 R D +17107 10110 M -49 0 R D 17107 10228 M -49 0 R D 17107 10463 M -49 0 R D +17107 10580 M -49 0 R D 17107 10698 M -49 0 R D 17107 10932 M -49 0 R D +17107 11050 M -49 0 R D 17107 11167 M -49 0 R D 17107 11402 M -49 0 R D +17107 11519 M -49 0 R D 17107 11637 M -49 0 R D 17107 11872 M -49 0 R D +17107 11989 M -49 0 R D 20 setlinewidth 1.000 0.000 0.000 setrgbcolor +12152 8468 M 226 0 R 0 5 R 225 0 R 225 0 R 0 18 R 225 0 R 226 0 R 0 148 R +225 0 R 225 0 R 0 273 R 225 0 R 225 0 R 0 240 R 226 0 R 225 0 R 0 371 R +225 0 R 225 0 R 0 -38 R 226 0 R 225 0 R 0 -378 R 225 0 R 225 0 R 0 -223 R +226 0 R 225 0 R 0 -187 R 225 0 R 225 0 R 0 -229 R 225 0 R D +0.000 0.514 1.000 setrgbcolor 12152 8467 M 226 0 R 225 0 R 225 0 R 225 0 R +226 0 R 0 8 R 225 0 R 225 0 R 0 120 R 225 0 R 225 0 R 0 273 R 226 0 R +225 0 R 0 367 R 225 0 R 225 0 R 0 153 R 226 0 R 225 0 R 0 449 R 225 0 R +225 0 R 0 -464 R 226 0 R 225 0 R 0 -715 R 225 0 R 225 0 R 0 -189 R 225 0 R D +0.000 0.000 0.000 setrgbcolor 12152 8467 M 226 0 R 225 0 R 225 0 R 225 0 R +226 0 R 225 0 R 225 0 R 225 0 R 225 0 R 226 0 R 225 0 R 225 0 R 225 0 R +0 208 R 226 0 R 225 0 R 0 2923 R 225 0 R 225 0 R 0 -1775 R 226 0 R 225 0 R +0 -1356 R 225 0 R 225 0 R 225 0 R D 1.000 0.000 0.000 setrgbcolor +gsave 12603 11285 translate 0 0 M 1.01 dup scale +(log L) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(HX) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( > 41) show grestore 0.000 0.514 1.000 setrgbcolor +gsave 12603 10815 translate 0 0 M 1.01 dup scale +(log L) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(HX) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( > 43) show grestore 0.000 0.000 0.000 setrgbcolor +gsave 12603 10345 translate 0 0 M 1.01 dup scale +(log L) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(HX) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( > 45) show grestore 15 setlinewidth 2242 4944 M 4955 0 R D 2242 4944 M +0 71 R D gsave 2242 4411 translate 0 0 M 1.01 dup scale -58.8433 0 N +( ) show grestore 3143 4944 M 0 71 R D gsave 3143 4411 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 4044 4944 M 0 71 R D gsave 4044 4411 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 4945 4944 M 0 71 R D gsave 4945 4411 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 5846 4944 M 0 71 R D gsave 5846 4411 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 6747 4944 M 0 71 R D gsave 6747 4411 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 2332 4944 M 0 36 R D 2422 4944 M 0 36 R D 2513 4944 M +0 36 R D 2603 4944 M 0 36 R D 2693 4944 M 0 36 R D 2783 4944 M 0 36 R D +2873 4944 M 0 36 R D 2963 4944 M 0 36 R D 3053 4944 M 0 36 R D 3233 4944 M +0 36 R D 3323 4944 M 0 36 R D 3413 4944 M 0 36 R D 3504 4944 M 0 36 R D +3594 4944 M 0 36 R D 3684 4944 M 0 36 R D 3774 4944 M 0 36 R D 3864 4944 M +0 36 R D 3954 4944 M 0 36 R D 4134 4944 M 0 36 R D 4224 4944 M 0 36 R D +4314 4944 M 0 36 R D 4404 4944 M 0 36 R D 4495 4944 M 0 36 R D 4585 4944 M +0 36 R D 4675 4944 M 0 36 R D 4765 4944 M 0 36 R D 4855 4944 M 0 36 R D +5035 4944 M 0 36 R D 5125 4944 M 0 36 R D 5215 4944 M 0 36 R D 5305 4944 M +0 36 R D 5396 4944 M 0 36 R D 5486 4944 M 0 36 R D 5576 4944 M 0 36 R D +5666 4944 M 0 36 R D 5756 4944 M 0 36 R D 5936 4944 M 0 36 R D 6026 4944 M +0 36 R D 6116 4944 M 0 36 R D 6206 4944 M 0 36 R D 6296 4944 M 0 36 R D +6387 4944 M 0 36 R D 6477 4944 M 0 36 R D 6567 4944 M 0 36 R D 6657 4944 M +0 36 R D 6837 4944 M 0 36 R D 6927 4944 M 0 36 R D 7017 4944 M 0 36 R D +7107 4944 M 0 36 R D 7197 4944 M 0 36 R D 2242 8467 M 4955 0 R D 2242 8467 M +0 -71 R D 3143 8467 M 0 -71 R D 4044 8467 M 0 -71 R D 4945 8467 M 0 -71 R D +5846 8467 M 0 -71 R D 6747 8467 M 0 -71 R D 2332 8467 M 0 -35 R D +2422 8467 M 0 -35 R D 2513 8467 M 0 -35 R D 2603 8467 M 0 -35 R D +2693 8467 M 0 -35 R D 2783 8467 M 0 -35 R D 2873 8467 M 0 -35 R D +2963 8467 M 0 -35 R D 3053 8467 M 0 -35 R D 3233 8467 M 0 -35 R D +3323 8467 M 0 -35 R D 3413 8467 M 0 -35 R D 3504 8467 M 0 -35 R D +3594 8467 M 0 -35 R D 3684 8467 M 0 -35 R D 3774 8467 M 0 -35 R D +3864 8467 M 0 -35 R D 3954 8467 M 0 -35 R D 4134 8467 M 0 -35 R D +4224 8467 M 0 -35 R D 4314 8467 M 0 -35 R D 4404 8467 M 0 -35 R D +4495 8467 M 0 -35 R D 4585 8467 M 0 -35 R D 4675 8467 M 0 -35 R D +4765 8467 M 0 -35 R D 4855 8467 M 0 -35 R D 5035 8467 M 0 -35 R D +5125 8467 M 0 -35 R D 5215 8467 M 0 -35 R D 5305 8467 M 0 -35 R D +5396 8467 M 0 -35 R D 5486 8467 M 0 -35 R D 5576 8467 M 0 -35 R D +5666 8467 M 0 -35 R D 5756 8467 M 0 -35 R D 5936 8467 M 0 -35 R D +6026 8467 M 0 -35 R D 6116 8467 M 0 -35 R D 6206 8467 M 0 -35 R D +6296 8467 M 0 -35 R D 6387 8467 M 0 -35 R D 6477 8467 M 0 -35 R D +6567 8467 M 0 -35 R D 6657 8467 M 0 -35 R D 6837 8467 M 0 -35 R D +6927 8467 M 0 -35 R D 7017 8467 M 0 -35 R D 7107 8467 M 0 -35 R D +7197 8467 M 0 -35 R D 2242 4944 M 0 3523 R D 2242 4944 M 99 0 R D +gsave 2130 4944 translate 0 0 M 1.01 dup scale -117.687 0 N +( ) show grestore 2242 5414 M 99 0 R D gsave 2130 5272 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 5884 M 99 0 R D gsave 2130 5742 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 6353 M 99 0 R D gsave 2130 6211 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 6823 M 99 0 R D gsave 2130 6681 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 7293 M 99 0 R D gsave 2130 7150 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 7762 M 99 0 R D gsave 2130 7620 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 8232 M 99 0 R D gsave 2130 8090 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 5062 M 50 0 R D 2242 5179 M 50 0 R D 2242 5297 M +50 0 R D 2242 5531 M 50 0 R D 2242 5649 M 50 0 R D 2242 5766 M 50 0 R D +2242 6001 M 50 0 R D 2242 6119 M 50 0 R D 2242 6236 M 50 0 R D 2242 6471 M +50 0 R D 2242 6588 M 50 0 R D 2242 6706 M 50 0 R D 2242 6940 M 50 0 R D +2242 7058 M 50 0 R D 2242 7175 M 50 0 R D 2242 7410 M 50 0 R D 2242 7527 M +50 0 R D 2242 7645 M 50 0 R D 2242 7880 M 50 0 R D 2242 7997 M 50 0 R D +2242 8115 M 50 0 R D 2242 8349 M 50 0 R D 2242 8467 M 50 0 R D 7197 4944 M +0 3523 R D 7197 4944 M -99 0 R D 7197 5414 M -99 0 R D 7197 5884 M -99 0 R D +7197 6353 M -99 0 R D 7197 6823 M -99 0 R D 7197 7293 M -99 0 R D +7197 7762 M -99 0 R D 7197 8232 M -99 0 R D 7197 5062 M -49 0 R D +7197 5179 M -49 0 R D 7197 5297 M -49 0 R D 7197 5531 M -49 0 R D +7197 5649 M -49 0 R D 7197 5766 M -49 0 R D 7197 6001 M -49 0 R D +7197 6119 M -49 0 R D 7197 6236 M -49 0 R D 7197 6471 M -49 0 R D +7197 6588 M -49 0 R D 7197 6706 M -49 0 R D 7197 6940 M -49 0 R D +7197 7058 M -49 0 R D 7197 7175 M -49 0 R D 7197 7410 M -49 0 R D +7197 7527 M -49 0 R D 7197 7645 M -49 0 R D 7197 7880 M -49 0 R D +7197 7997 M -49 0 R D 7197 8115 M -49 0 R D 7197 8349 M -49 0 R D +7197 8467 M -49 0 R D 20 setlinewidth 1.000 0.000 0.000 setrgbcolor +2242 4944 M 226 0 R 225 0 R 225 0 R 225 0 R 225 0 R 226 0 R 225 0 R 0 12 R +225 0 R 225 0 R 0 91 R 226 0 R 225 0 R 0 464 R 225 0 R 225 0 R 0 940 R +226 0 R 225 0 R 0 334 R 225 0 R 225 0 R 0 -1181 R 225 0 R 226 0 R 0 -651 R +225 0 R 225 0 R 0 -9 R 225 0 R D 0.000 0.514 1.000 setrgbcolor 2242 4944 M +226 0 R 225 0 R 225 0 R 225 0 R 225 0 R 226 0 R 225 0 R 225 0 R 225 0 R +226 0 R 225 0 R 225 0 R 225 0 R 0 1115 R 226 0 R 225 0 R 0 1594 R 225 0 R +225 0 R 0 -1871 R 225 0 R 226 0 R 0 -802 R 225 0 R 225 0 R 0 -36 R 225 0 R D +0.000 0.000 0.000 setrgbcolor 2242 4944 M 226 0 R 225 0 R 225 0 R 225 0 R +225 0 R 226 0 R 225 0 R 225 0 R 225 0 R 226 0 R 225 0 R 225 0 R 225 0 R +226 0 R 225 0 R 225 0 R 225 0 R 0 2684 R 225 0 R 226 0 R 0 -2013 R 225 0 R +225 0 R 0 -671 R 225 0 R D gsave 2513 7762 translate 0 0 M 1.2 dup scale +(z = 1.0) show grestore 15 setlinewidth 7197 4944 M 4955 0 R D 7197 4944 M +0 71 R D gsave 7197 4411 translate 0 0 M 1.01 dup scale -58.8433 0 N +( ) show grestore 8098 4944 M 0 71 R D gsave 8098 4411 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 8999 4944 M 0 71 R D gsave 8999 4411 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 9900 4944 M 0 71 R D gsave 9900 4411 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 10801 4944 M 0 71 R D gsave 10801 4411 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 11702 4944 M 0 71 R D gsave 11702 4411 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 7287 4944 M 0 36 R D 7378 4944 M 0 36 R D 7468 4944 M +0 36 R D 7558 4944 M 0 36 R D 7648 4944 M 0 36 R D 7738 4944 M 0 36 R D +7828 4944 M 0 36 R D 7918 4944 M 0 36 R D 8008 4944 M 0 36 R D 8188 4944 M +0 36 R D 8278 4944 M 0 36 R D 8369 4944 M 0 36 R D 8459 4944 M 0 36 R D +8549 4944 M 0 36 R D 8639 4944 M 0 36 R D 8729 4944 M 0 36 R D 8819 4944 M +0 36 R D 8909 4944 M 0 36 R D 9089 4944 M 0 36 R D 9179 4944 M 0 36 R D +9269 4944 M 0 36 R D 9360 4944 M 0 36 R D 9450 4944 M 0 36 R D 9540 4944 M +0 36 R D 9630 4944 M 0 36 R D 9720 4944 M 0 36 R D 9810 4944 M 0 36 R D +9990 4944 M 0 36 R D 10080 4944 M 0 36 R D 10170 4944 M 0 36 R D +10260 4944 M 0 36 R D 10351 4944 M 0 36 R D 10441 4944 M 0 36 R D +10531 4944 M 0 36 R D 10621 4944 M 0 36 R D 10711 4944 M 0 36 R D +10891 4944 M 0 36 R D 10981 4944 M 0 36 R D 11071 4944 M 0 36 R D +11161 4944 M 0 36 R D 11251 4944 M 0 36 R D 11342 4944 M 0 36 R D +11432 4944 M 0 36 R D 11522 4944 M 0 36 R D 11612 4944 M 0 36 R D +11792 4944 M 0 36 R D 11882 4944 M 0 36 R D 11972 4944 M 0 36 R D +12062 4944 M 0 36 R D 12152 4944 M 0 36 R D 7197 8467 M 4955 0 R D +7197 8467 M 0 -71 R D 8098 8467 M 0 -71 R D 8999 8467 M 0 -71 R D +9900 8467 M 0 -71 R D 10801 8467 M 0 -71 R D 11702 8467 M 0 -71 R D +7287 8467 M 0 -35 R D 7378 8467 M 0 -35 R D 7468 8467 M 0 -35 R D +7558 8467 M 0 -35 R D 7648 8467 M 0 -35 R D 7738 8467 M 0 -35 R D +7828 8467 M 0 -35 R D 7918 8467 M 0 -35 R D 8008 8467 M 0 -35 R D +8188 8467 M 0 -35 R D 8278 8467 M 0 -35 R D 8369 8467 M 0 -35 R D +8459 8467 M 0 -35 R D 8549 8467 M 0 -35 R D 8639 8467 M 0 -35 R D +8729 8467 M 0 -35 R D 8819 8467 M 0 -35 R D 8909 8467 M 0 -35 R D +9089 8467 M 0 -35 R D 9179 8467 M 0 -35 R D 9269 8467 M 0 -35 R D +9360 8467 M 0 -35 R D 9450 8467 M 0 -35 R D 9540 8467 M 0 -35 R D +9630 8467 M 0 -35 R D 9720 8467 M 0 -35 R D 9810 8467 M 0 -35 R D +9990 8467 M 0 -35 R D 10080 8467 M 0 -35 R D 10170 8467 M 0 -35 R D +10260 8467 M 0 -35 R D 10351 8467 M 0 -35 R D 10441 8467 M 0 -35 R D +10531 8467 M 0 -35 R D 10621 8467 M 0 -35 R D 10711 8467 M 0 -35 R D +10891 8467 M 0 -35 R D 10981 8467 M 0 -35 R D 11071 8467 M 0 -35 R D +11161 8467 M 0 -35 R D 11251 8467 M 0 -35 R D 11342 8467 M 0 -35 R D +11432 8467 M 0 -35 R D 11522 8467 M 0 -35 R D 11612 8467 M 0 -35 R D +11792 8467 M 0 -35 R D 11882 8467 M 0 -35 R D 11972 8467 M 0 -35 R D +12062 8467 M 0 -35 R D 12152 8467 M 0 -35 R D 7197 4944 M 0 3523 R D +7197 4944 M 99 0 R D gsave 7085 4944 translate 0 0 M 1.01 dup scale +-117.687 0 N +( ) show grestore 7197 5414 M 99 0 R D gsave 7085 5272 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 5884 M 99 0 R D gsave 7085 5742 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 6353 M 99 0 R D gsave 7085 6211 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 6823 M 99 0 R D gsave 7085 6681 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 7293 M 99 0 R D gsave 7085 7150 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 7762 M 99 0 R D gsave 7085 7620 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 8232 M 99 0 R D gsave 7085 8090 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 5062 M 50 0 R D 7197 5179 M 50 0 R D 7197 5297 M +50 0 R D 7197 5531 M 50 0 R D 7197 5649 M 50 0 R D 7197 5766 M 50 0 R D +7197 6001 M 50 0 R D 7197 6119 M 50 0 R D 7197 6236 M 50 0 R D 7197 6471 M +50 0 R D 7197 6588 M 50 0 R D 7197 6706 M 50 0 R D 7197 6940 M 50 0 R D +7197 7058 M 50 0 R D 7197 7175 M 50 0 R D 7197 7410 M 50 0 R D 7197 7527 M +50 0 R D 7197 7645 M 50 0 R D 7197 7880 M 50 0 R D 7197 7997 M 50 0 R D +7197 8115 M 50 0 R D 7197 8349 M 50 0 R D 7197 8467 M 50 0 R D 12152 4944 M +0 3523 R D 12152 4944 M -99 0 R D 12152 5414 M -99 0 R D 12152 5884 M +-99 0 R D 12152 6353 M -99 0 R D 12152 6823 M -99 0 R D 12152 7293 M -99 0 R +D 12152 7762 M -99 0 R D 12152 8232 M -99 0 R D 12152 5062 M -49 0 R D +12152 5179 M -49 0 R D 12152 5297 M -49 0 R D 12152 5531 M -49 0 R D +12152 5649 M -49 0 R D 12152 5766 M -49 0 R D 12152 6001 M -49 0 R D +12152 6119 M -49 0 R D 12152 6236 M -49 0 R D 12152 6471 M -49 0 R D +12152 6588 M -49 0 R D 12152 6706 M -49 0 R D 12152 6940 M -49 0 R D +12152 7058 M -49 0 R D 12152 7175 M -49 0 R D 12152 7410 M -49 0 R D +12152 7527 M -49 0 R D 12152 7645 M -49 0 R D 12152 7880 M -49 0 R D +12152 7997 M -49 0 R D 12152 8115 M -49 0 R D 12152 8349 M -49 0 R D +12152 8467 M -49 0 R D 20 setlinewidth 1.000 0.000 0.000 setrgbcolor +7197 4951 M 226 0 R 0 18 R 225 0 R 225 0 R 0 51 R 225 0 R 225 0 R 0 298 R +226 0 R 225 0 R 0 213 R 225 0 R 225 0 R 0 278 R 226 0 R 225 0 R 0 238 R +225 0 R 225 0 R 0 -532 R 226 0 R 225 0 R 0 -56 R 225 0 R 225 0 R 0 -106 R +225 0 R 226 0 R 0 -239 R 225 0 R 225 0 R 0 -169 R 225 0 R D +0.000 0.514 1.000 setrgbcolor 7197 4944 M 226 0 R 225 0 R 225 0 R 225 0 R +225 0 R 0 2 R 226 0 R 225 0 R 0 168 R 225 0 R 225 0 R 0 196 R 226 0 R +225 0 R 0 102 R 225 0 R 225 0 R 0 303 R 226 0 R 225 0 R 0 736 R 225 0 R +225 0 R 0 -292 R 225 0 R 226 0 R 0 -1015 R 225 0 R 225 0 R 0 -199 R 225 0 R +D 0.000 0.000 0.000 setrgbcolor 7197 4944 M 226 0 R 225 0 R 225 0 R 225 0 R +225 0 R 226 0 R 225 0 R 225 0 R 225 0 R 226 0 R 225 0 R 225 0 R 225 0 R +0 54 R 226 0 R 225 0 R 0 2926 R 225 0 R 225 0 R 0 -1345 R 225 0 R 226 0 R +0 -1605 R 225 0 R 225 0 R 0 -30 R 225 0 R D 15 setlinewidth 12152 4944 M +4955 0 R D 12152 4944 M 0 71 R D gsave 12152 4411 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 13053 4944 M 0 71 R D gsave 13053 4411 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 13954 4944 M 0 71 R D gsave 13954 4411 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 14855 4944 M 0 71 R D gsave 14855 4411 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 15756 4944 M 0 71 R D gsave 15756 4411 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 16657 4944 M 0 71 R D gsave 16657 4411 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 12242 4944 M 0 36 R D 12333 4944 M 0 36 R D 12423 4944 M +0 36 R D 12513 4944 M 0 36 R D 12603 4944 M 0 36 R D 12693 4944 M 0 36 R D +12783 4944 M 0 36 R D 12873 4944 M 0 36 R D 12963 4944 M 0 36 R D +13143 4944 M 0 36 R D 13233 4944 M 0 36 R D 13324 4944 M 0 36 R D +13414 4944 M 0 36 R D 13504 4944 M 0 36 R D 13594 4944 M 0 36 R D +13684 4944 M 0 36 R D 13774 4944 M 0 36 R D 13864 4944 M 0 36 R D +14044 4944 M 0 36 R D 14134 4944 M 0 36 R D 14224 4944 M 0 36 R D +14315 4944 M 0 36 R D 14405 4944 M 0 36 R D 14495 4944 M 0 36 R D +14585 4944 M 0 36 R D 14675 4944 M 0 36 R D 14765 4944 M 0 36 R D +14945 4944 M 0 36 R D 15035 4944 M 0 36 R D 15125 4944 M 0 36 R D +15216 4944 M 0 36 R D 15306 4944 M 0 36 R D 15396 4944 M 0 36 R D +15486 4944 M 0 36 R D 15576 4944 M 0 36 R D 15666 4944 M 0 36 R D +15846 4944 M 0 36 R D 15936 4944 M 0 36 R D 16026 4944 M 0 36 R D +16116 4944 M 0 36 R D 16207 4944 M 0 36 R D 16297 4944 M 0 36 R D +16387 4944 M 0 36 R D 16477 4944 M 0 36 R D 16567 4944 M 0 36 R D +16747 4944 M 0 36 R D 16837 4944 M 0 36 R D 16927 4944 M 0 36 R D +17017 4944 M 0 36 R D 17107 4944 M 0 36 R D 12152 8467 M 4955 0 R D +12152 8467 M 0 -71 R D 13053 8467 M 0 -71 R D 13954 8467 M 0 -71 R D +14855 8467 M 0 -71 R D 15756 8467 M 0 -71 R D 16657 8467 M 0 -71 R D +12242 8467 M 0 -35 R D 12333 8467 M 0 -35 R D 12423 8467 M 0 -35 R D +12513 8467 M 0 -35 R D 12603 8467 M 0 -35 R D 12693 8467 M 0 -35 R D +12783 8467 M 0 -35 R D 12873 8467 M 0 -35 R D 12963 8467 M 0 -35 R D +13143 8467 M 0 -35 R D 13233 8467 M 0 -35 R D 13324 8467 M 0 -35 R D +13414 8467 M 0 -35 R D 13504 8467 M 0 -35 R D 13594 8467 M 0 -35 R D +13684 8467 M 0 -35 R D 13774 8467 M 0 -35 R D 13864 8467 M 0 -35 R D +14044 8467 M 0 -35 R D 14134 8467 M 0 -35 R D 14224 8467 M 0 -35 R D +14315 8467 M 0 -35 R D 14405 8467 M 0 -35 R D 14495 8467 M 0 -35 R D +14585 8467 M 0 -35 R D 14675 8467 M 0 -35 R D 14765 8467 M 0 -35 R D +14945 8467 M 0 -35 R D 15035 8467 M 0 -35 R D 15125 8467 M 0 -35 R D +15216 8467 M 0 -35 R D 15306 8467 M 0 -35 R D 15396 8467 M 0 -35 R D +15486 8467 M 0 -35 R D 15576 8467 M 0 -35 R D 15666 8467 M 0 -35 R D +15846 8467 M 0 -35 R D 15936 8467 M 0 -35 R D 16026 8467 M 0 -35 R D +16116 8467 M 0 -35 R D 16207 8467 M 0 -35 R D 16297 8467 M 0 -35 R D +16387 8467 M 0 -35 R D 16477 8467 M 0 -35 R D 16567 8467 M 0 -35 R D +16747 8467 M 0 -35 R D 16837 8467 M 0 -35 R D 16927 8467 M 0 -35 R D +17017 8467 M 0 -35 R D 17107 8467 M 0 -35 R D 12152 4944 M 0 3523 R D +12152 4944 M 99 0 R D gsave 12040 4944 translate 0 0 M 1.01 dup scale +-117.687 0 N +( ) show grestore 12152 5414 M 99 0 R D gsave 12040 5272 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 5884 M 99 0 R D gsave 12040 5742 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 6353 M 99 0 R D gsave 12040 6211 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 6823 M 99 0 R D gsave 12040 6681 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 7293 M 99 0 R D gsave 12040 7150 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 7762 M 99 0 R D gsave 12040 7620 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 8232 M 99 0 R D gsave 12040 8090 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 5062 M 50 0 R D 12152 5179 M 50 0 R D 12152 5297 M +50 0 R D 12152 5531 M 50 0 R D 12152 5649 M 50 0 R D 12152 5766 M 50 0 R D +12152 6001 M 50 0 R D 12152 6119 M 50 0 R D 12152 6236 M 50 0 R D +12152 6471 M 50 0 R D 12152 6588 M 50 0 R D 12152 6706 M 50 0 R D +12152 6940 M 50 0 R D 12152 7058 M 50 0 R D 12152 7175 M 50 0 R D +12152 7410 M 50 0 R D 12152 7527 M 50 0 R D 12152 7645 M 50 0 R D +12152 7880 M 50 0 R D 12152 7997 M 50 0 R D 12152 8115 M 50 0 R D +12152 8349 M 50 0 R D 12152 8467 M 50 0 R D 17107 4944 M 0 3523 R D +17107 4944 M -99 0 R D 17107 5414 M -99 0 R D 17107 5884 M -99 0 R D +17107 6353 M -99 0 R D 17107 6823 M -99 0 R D 17107 7293 M -99 0 R D +17107 7762 M -99 0 R D 17107 8232 M -99 0 R D 17107 5062 M -49 0 R D +17107 5179 M -49 0 R D 17107 5297 M -49 0 R D 17107 5531 M -49 0 R D +17107 5649 M -49 0 R D 17107 5766 M -49 0 R D 17107 6001 M -49 0 R D +17107 6119 M -49 0 R D 17107 6236 M -49 0 R D 17107 6471 M -49 0 R D +17107 6588 M -49 0 R D 17107 6706 M -49 0 R D 17107 6940 M -49 0 R D +17107 7058 M -49 0 R D 17107 7175 M -49 0 R D 17107 7410 M -49 0 R D +17107 7527 M -49 0 R D 17107 7645 M -49 0 R D 17107 7880 M -49 0 R D +17107 7997 M -49 0 R D 17107 8115 M -49 0 R D 17107 8349 M -49 0 R D +17107 8467 M -49 0 R D 20 setlinewidth 1.000 0.000 0.000 setrgbcolor +12152 4949 M 226 0 R 0 10 R 225 0 R 225 0 R 0 28 R 225 0 R 226 0 R 0 225 R +225 0 R 225 0 R 0 336 R 225 0 R 225 0 R 0 198 R 226 0 R 225 0 R 0 248 R +225 0 R 225 0 R 0 -148 R 226 0 R 225 0 R 0 -338 R 225 0 R 225 0 R 0 -248 R +226 0 R 225 0 R 0 -184 R 225 0 R 225 0 R 0 -131 R 225 0 R D +0.000 0.514 1.000 setrgbcolor 12152 4944 M 226 0 R 225 0 R 225 0 R 225 0 R +226 0 R 0 19 R 225 0 R 225 0 R 0 183 R 225 0 R 225 0 R 0 380 R 226 0 R +225 0 R 0 330 R 225 0 R 225 0 R 0 47 R 226 0 R 225 0 R 0 260 R 225 0 R +225 0 R 0 -525 R 226 0 R 225 0 R 0 -582 R 225 0 R 225 0 R 0 -111 R 225 0 R D +0.000 0.000 0.000 setrgbcolor 12152 4944 M 226 0 R 225 0 R 225 0 R 225 0 R +226 0 R 225 0 R 225 0 R 225 0 R 225 0 R 226 0 R 225 0 R 225 0 R 225 0 R +0 219 R 226 0 R 225 0 R 0 2754 R 225 0 R 225 0 R 0 -1478 R 226 0 R 225 0 R +0 -1484 R 225 0 R 225 0 R 0 -11 R 225 0 R D 15 setlinewidth 2242 1422 M +4955 0 R D 2242 1422 M 0 71 R D gsave 2242 889 translate 0 0 M +1.01 dup scale -188.172 0 N +(-5) show grestore 3143 1422 M 0 71 R D gsave 3143 889 translate 0 0 M +1.01 dup scale -188.172 0 N +(-4) show grestore 4044 1422 M 0 71 R D gsave 4044 889 translate 0 0 M +1.01 dup scale -188.172 0 N +(-3) show grestore 4945 1422 M 0 71 R D gsave 4945 889 translate 0 0 M +1.01 dup scale -188.172 0 N +(-2) show grestore 5846 1422 M 0 71 R D gsave 5846 889 translate 0 0 M +1.01 dup scale -188.172 0 N +(-1) show grestore 6747 1422 M 0 71 R D gsave 6747 889 translate 0 0 M +1.01 dup scale -117.687 0 N +(0) show grestore 2332 1422 M 0 35 R D 2422 1422 M 0 35 R D 2513 1422 M +0 35 R D 2603 1422 M 0 35 R D 2693 1422 M 0 35 R D 2783 1422 M 0 35 R D +2873 1422 M 0 35 R D 2963 1422 M 0 35 R D 3053 1422 M 0 35 R D 3233 1422 M +0 35 R D 3323 1422 M 0 35 R D 3413 1422 M 0 35 R D 3504 1422 M 0 35 R D +3594 1422 M 0 35 R D 3684 1422 M 0 35 R D 3774 1422 M 0 35 R D 3864 1422 M +0 35 R D 3954 1422 M 0 35 R D 4134 1422 M 0 35 R D 4224 1422 M 0 35 R D +4314 1422 M 0 35 R D 4404 1422 M 0 35 R D 4495 1422 M 0 35 R D 4585 1422 M +0 35 R D 4675 1422 M 0 35 R D 4765 1422 M 0 35 R D 4855 1422 M 0 35 R D +5035 1422 M 0 35 R D 5125 1422 M 0 35 R D 5215 1422 M 0 35 R D 5305 1422 M +0 35 R D 5396 1422 M 0 35 R D 5486 1422 M 0 35 R D 5576 1422 M 0 35 R D +5666 1422 M 0 35 R D 5756 1422 M 0 35 R D 5936 1422 M 0 35 R D 6026 1422 M +0 35 R D 6116 1422 M 0 35 R D 6206 1422 M 0 35 R D 6296 1422 M 0 35 R D +6387 1422 M 0 35 R D 6477 1422 M 0 35 R D 6567 1422 M 0 35 R D 6657 1422 M +0 35 R D 6837 1422 M 0 35 R D 6927 1422 M 0 35 R D 7017 1422 M 0 35 R D +7107 1422 M 0 35 R D 7197 1422 M 0 35 R D 2242 4944 M 4955 0 R D 2242 4944 M +0 -70 R D 3143 4944 M 0 -70 R D 4044 4944 M 0 -70 R D 4945 4944 M 0 -70 R D +5846 4944 M 0 -70 R D 6747 4944 M 0 -70 R D 2332 4944 M 0 -35 R D +2422 4944 M 0 -35 R D 2513 4944 M 0 -35 R D 2603 4944 M 0 -35 R D +2693 4944 M 0 -35 R D 2783 4944 M 0 -35 R D 2873 4944 M 0 -35 R D +2963 4944 M 0 -35 R D 3053 4944 M 0 -35 R D 3233 4944 M 0 -35 R D +3323 4944 M 0 -35 R D 3413 4944 M 0 -35 R D 3504 4944 M 0 -35 R D +3594 4944 M 0 -35 R D 3684 4944 M 0 -35 R D 3774 4944 M 0 -35 R D +3864 4944 M 0 -35 R D 3954 4944 M 0 -35 R D 4134 4944 M 0 -35 R D +4224 4944 M 0 -35 R D 4314 4944 M 0 -35 R D 4404 4944 M 0 -35 R D +4495 4944 M 0 -35 R D 4585 4944 M 0 -35 R D 4675 4944 M 0 -35 R D +4765 4944 M 0 -35 R D 4855 4944 M 0 -35 R D 5035 4944 M 0 -35 R D +5125 4944 M 0 -35 R D 5215 4944 M 0 -35 R D 5305 4944 M 0 -35 R D +5396 4944 M 0 -35 R D 5486 4944 M 0 -35 R D 5576 4944 M 0 -35 R D +5666 4944 M 0 -35 R D 5756 4944 M 0 -35 R D 5936 4944 M 0 -35 R D +6026 4944 M 0 -35 R D 6116 4944 M 0 -35 R D 6206 4944 M 0 -35 R D +6296 4944 M 0 -35 R D 6387 4944 M 0 -35 R D 6477 4944 M 0 -35 R D +6567 4944 M 0 -35 R D 6657 4944 M 0 -35 R D 6837 4944 M 0 -35 R D +6927 4944 M 0 -35 R D 7017 4944 M 0 -35 R D 7107 4944 M 0 -35 R D +7197 4944 M 0 -35 R D 2242 1422 M 0 3522 R D 2242 1422 M 99 0 R D +gsave 2130 1422 translate 0 0 M 1.01 dup scale -117.687 0 N +( ) show grestore 2242 1892 M 99 0 R D gsave 2130 1750 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 2361 M 99 0 R D gsave 2130 2219 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 2831 M 99 0 R D gsave 2130 2689 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 3301 M 99 0 R D gsave 2130 3158 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 3770 M 99 0 R D gsave 2130 3628 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 4240 M 99 0 R D gsave 2130 4098 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 4710 M 99 0 R D gsave 2130 4567 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 2242 1540 M 50 0 R D 2242 1657 M 50 0 R D 2242 1774 M +50 0 R D 2242 2009 M 50 0 R D 2242 2127 M 50 0 R D 2242 2244 M 50 0 R D +2242 2479 M 50 0 R D 2242 2596 M 50 0 R D 2242 2714 M 50 0 R D 2242 2948 M +50 0 R D 2242 3066 M 50 0 R D 2242 3183 M 50 0 R D 2242 3418 M 50 0 R D +2242 3536 M 50 0 R D 2242 3653 M 50 0 R D 2242 3888 M 50 0 R D 2242 4005 M +50 0 R D 2242 4123 M 50 0 R D 2242 4357 M 50 0 R D 2242 4475 M 50 0 R D +2242 4592 M 50 0 R D 2242 4827 M 50 0 R D 2242 4944 M 50 0 R D 7197 1422 M +0 3522 R D 7197 1422 M -99 0 R D 7197 1892 M -99 0 R D 7197 2361 M -99 0 R D +7197 2831 M -99 0 R D 7197 3301 M -99 0 R D 7197 3770 M -99 0 R D +7197 4240 M -99 0 R D 7197 4710 M -99 0 R D 7197 1540 M -49 0 R D +7197 1657 M -49 0 R D 7197 1774 M -49 0 R D 7197 2009 M -49 0 R D +7197 2127 M -49 0 R D 7197 2244 M -49 0 R D 7197 2479 M -49 0 R D +7197 2596 M -49 0 R D 7197 2714 M -49 0 R D 7197 2948 M -49 0 R D +7197 3066 M -49 0 R D 7197 3183 M -49 0 R D 7197 3418 M -49 0 R D +7197 3536 M -49 0 R D 7197 3653 M -49 0 R D 7197 3888 M -49 0 R D +7197 4005 M -49 0 R D 7197 4123 M -49 0 R D 7197 4357 M -49 0 R D +7197 4475 M -49 0 R D 7197 4592 M -49 0 R D 7197 4827 M -49 0 R D +7197 4944 M -49 0 R D 20 setlinewidth 1.000 0.000 0.000 setrgbcolor +2242 1422 M 226 0 R 225 0 R 225 0 R 225 0 R 225 0 R 226 0 R 225 0 R 0 15 R +225 0 R 225 0 R 0 123 R 226 0 R 225 0 R 0 559 R 225 0 R 225 0 R 0 911 R +226 0 R 225 0 R 0 79 R 225 0 R 225 0 R 0 -1142 R 225 0 R 226 0 R 0 -537 R +225 0 R 225 0 R 0 -8 R 225 0 R D 0.000 0.514 1.000 setrgbcolor 2242 1422 M +226 0 R 225 0 R 225 0 R 225 0 R 225 0 R 226 0 R 225 0 R 225 0 R 225 0 R +226 0 R 225 0 R 0 5 R 225 0 R 225 0 R 0 1171 R 226 0 R 225 0 R 0 1545 R +225 0 R 225 0 R 0 -1964 R 225 0 R 226 0 R 0 -719 R 225 0 R 225 0 R 0 -38 R +225 0 R D 0.000 0.000 0.000 setrgbcolor 2242 1422 M 226 0 R 225 0 R 225 0 R +225 0 R 225 0 R 226 0 R 225 0 R 225 0 R 225 0 R 226 0 R 225 0 R 225 0 R +225 0 R 226 0 R 225 0 R 225 0 R 225 0 R 0 2890 R 225 0 R 226 0 R 0 -1084 R +225 0 R 225 0 R 0 -1806 R 225 0 R D gsave 2513 4240 translate 0 0 M +1.2 dup scale +(z = 2.0) show grestore 15 setlinewidth 7197 1422 M 4955 0 R D 7197 1422 M +0 71 R D gsave 7197 889 translate 0 0 M 1.01 dup scale -188.172 0 N +(-5) show grestore 8098 1422 M 0 71 R D gsave 8098 889 translate 0 0 M +1.01 dup scale -188.172 0 N +(-4) show grestore 8999 1422 M 0 71 R D gsave 8999 889 translate 0 0 M +1.01 dup scale -188.172 0 N +(-3) show grestore 9900 1422 M 0 71 R D gsave 9900 889 translate 0 0 M +1.01 dup scale -188.172 0 N +(-2) show grestore 10801 1422 M 0 71 R D gsave 10801 889 translate 0 0 M +1.01 dup scale -188.172 0 N +(-1) show grestore 11702 1422 M 0 71 R D gsave 11702 889 translate 0 0 M +1.01 dup scale -117.687 0 N +(0) show grestore 7287 1422 M 0 35 R D 7378 1422 M 0 35 R D 7468 1422 M +0 35 R D 7558 1422 M 0 35 R D 7648 1422 M 0 35 R D 7738 1422 M 0 35 R D +7828 1422 M 0 35 R D 7918 1422 M 0 35 R D 8008 1422 M 0 35 R D 8188 1422 M +0 35 R D 8278 1422 M 0 35 R D 8369 1422 M 0 35 R D 8459 1422 M 0 35 R D +8549 1422 M 0 35 R D 8639 1422 M 0 35 R D 8729 1422 M 0 35 R D 8819 1422 M +0 35 R D 8909 1422 M 0 35 R D 9089 1422 M 0 35 R D 9179 1422 M 0 35 R D +9269 1422 M 0 35 R D 9360 1422 M 0 35 R D 9450 1422 M 0 35 R D 9540 1422 M +0 35 R D 9630 1422 M 0 35 R D 9720 1422 M 0 35 R D 9810 1422 M 0 35 R D +9990 1422 M 0 35 R D 10080 1422 M 0 35 R D 10170 1422 M 0 35 R D +10260 1422 M 0 35 R D 10351 1422 M 0 35 R D 10441 1422 M 0 35 R D +10531 1422 M 0 35 R D 10621 1422 M 0 35 R D 10711 1422 M 0 35 R D +10891 1422 M 0 35 R D 10981 1422 M 0 35 R D 11071 1422 M 0 35 R D +11161 1422 M 0 35 R D 11251 1422 M 0 35 R D 11342 1422 M 0 35 R D +11432 1422 M 0 35 R D 11522 1422 M 0 35 R D 11612 1422 M 0 35 R D +11792 1422 M 0 35 R D 11882 1422 M 0 35 R D 11972 1422 M 0 35 R D +12062 1422 M 0 35 R D 12152 1422 M 0 35 R D 7197 4944 M 4955 0 R D +7197 4944 M 0 -70 R D 8098 4944 M 0 -70 R D 8999 4944 M 0 -70 R D +9900 4944 M 0 -70 R D 10801 4944 M 0 -70 R D 11702 4944 M 0 -70 R D +7287 4944 M 0 -35 R D 7378 4944 M 0 -35 R D 7468 4944 M 0 -35 R D +7558 4944 M 0 -35 R D 7648 4944 M 0 -35 R D 7738 4944 M 0 -35 R D +7828 4944 M 0 -35 R D 7918 4944 M 0 -35 R D 8008 4944 M 0 -35 R D +8188 4944 M 0 -35 R D 8278 4944 M 0 -35 R D 8369 4944 M 0 -35 R D +8459 4944 M 0 -35 R D 8549 4944 M 0 -35 R D 8639 4944 M 0 -35 R D +8729 4944 M 0 -35 R D 8819 4944 M 0 -35 R D 8909 4944 M 0 -35 R D +9089 4944 M 0 -35 R D 9179 4944 M 0 -35 R D 9269 4944 M 0 -35 R D +9360 4944 M 0 -35 R D 9450 4944 M 0 -35 R D 9540 4944 M 0 -35 R D +9630 4944 M 0 -35 R D 9720 4944 M 0 -35 R D 9810 4944 M 0 -35 R D +9990 4944 M 0 -35 R D 10080 4944 M 0 -35 R D 10170 4944 M 0 -35 R D +10260 4944 M 0 -35 R D 10351 4944 M 0 -35 R D 10441 4944 M 0 -35 R D +10531 4944 M 0 -35 R D 10621 4944 M 0 -35 R D 10711 4944 M 0 -35 R D +10891 4944 M 0 -35 R D 10981 4944 M 0 -35 R D 11071 4944 M 0 -35 R D +11161 4944 M 0 -35 R D 11251 4944 M 0 -35 R D 11342 4944 M 0 -35 R D +11432 4944 M 0 -35 R D 11522 4944 M 0 -35 R D 11612 4944 M 0 -35 R D +11792 4944 M 0 -35 R D 11882 4944 M 0 -35 R D 11972 4944 M 0 -35 R D +12062 4944 M 0 -35 R D 12152 4944 M 0 -35 R D 7197 1422 M 0 3522 R D +7197 1422 M 99 0 R D gsave 7085 1422 translate 0 0 M 1.01 dup scale +-117.687 0 N +( ) show grestore 7197 1892 M 99 0 R D gsave 7085 1750 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 2361 M 99 0 R D gsave 7085 2219 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 2831 M 99 0 R D gsave 7085 2689 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 3301 M 99 0 R D gsave 7085 3158 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 3770 M 99 0 R D gsave 7085 3628 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 4240 M 99 0 R D gsave 7085 4098 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 4710 M 99 0 R D gsave 7085 4567 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 7197 1540 M 50 0 R D 7197 1657 M 50 0 R D 7197 1774 M +50 0 R D 7197 2009 M 50 0 R D 7197 2127 M 50 0 R D 7197 2244 M 50 0 R D +7197 2479 M 50 0 R D 7197 2596 M 50 0 R D 7197 2714 M 50 0 R D 7197 2948 M +50 0 R D 7197 3066 M 50 0 R D 7197 3183 M 50 0 R D 7197 3418 M 50 0 R D +7197 3536 M 50 0 R D 7197 3653 M 50 0 R D 7197 3888 M 50 0 R D 7197 4005 M +50 0 R D 7197 4123 M 50 0 R D 7197 4357 M 50 0 R D 7197 4475 M 50 0 R D +7197 4592 M 50 0 R D 7197 4827 M 50 0 R D 7197 4944 M 50 0 R D 12152 1422 M +0 3522 R D 12152 1422 M -99 0 R D 12152 1892 M -99 0 R D 12152 2361 M +-99 0 R D 12152 2831 M -99 0 R D 12152 3301 M -99 0 R D 12152 3770 M -99 0 R +D 12152 4240 M -99 0 R D 12152 4710 M -99 0 R D 12152 1540 M -49 0 R D +12152 1657 M -49 0 R D 12152 1774 M -49 0 R D 12152 2009 M -49 0 R D +12152 2127 M -49 0 R D 12152 2244 M -49 0 R D 12152 2479 M -49 0 R D +12152 2596 M -49 0 R D 12152 2714 M -49 0 R D 12152 2948 M -49 0 R D +12152 3066 M -49 0 R D 12152 3183 M -49 0 R D 12152 3418 M -49 0 R D +12152 3536 M -49 0 R D 12152 3653 M -49 0 R D 12152 3888 M -49 0 R D +12152 4005 M -49 0 R D 12152 4123 M -49 0 R D 12152 4357 M -49 0 R D +12152 4475 M -49 0 R D 12152 4592 M -49 0 R D 12152 4827 M -49 0 R D +12152 4944 M -49 0 R D 20 setlinewidth 1.000 0.000 0.000 setrgbcolor +7197 1434 M 226 0 R 0 29 R 225 0 R 225 0 R 0 74 R 225 0 R 225 0 R 0 411 R +226 0 R 225 0 R 0 205 R 225 0 R 225 0 R 0 191 R 226 0 R 225 0 R 0 51 R +225 0 R 225 0 R 0 -472 R 226 0 R 225 0 R 0 -30 R 225 0 R 225 0 R 0 -161 R +225 0 R 226 0 R 0 -214 R 225 0 R 225 0 R 0 -95 R 225 0 R D +0.000 0.514 1.000 setrgbcolor 7197 1422 M 226 0 R 225 0 R 225 0 R 225 0 R +225 0 R 0 3 R 226 0 R 225 0 R 0 259 R 225 0 R 225 0 R 0 265 R 226 0 R +225 0 R 0 9 R 225 0 R 225 0 R 0 305 R 226 0 R 225 0 R 0 613 R 225 0 R +225 0 R 0 -506 R 225 0 R 226 0 R 0 -821 R 225 0 R 225 0 R 0 -127 R 225 0 R D +0.000 0.000 0.000 setrgbcolor 7197 1422 M 226 0 R 225 0 R 225 0 R 225 0 R +225 0 R 226 0 R 225 0 R 225 0 R 225 0 R 226 0 R 225 0 R 225 0 R 225 0 R +0 88 R 226 0 R 225 0 R 0 3008 R 225 0 R 225 0 R 0 -1600 R 225 0 R 226 0 R +0 -1479 R 225 0 R 225 0 R 0 -17 R 225 0 R D 15 setlinewidth 12152 1422 M +4955 0 R D 12152 1422 M 0 71 R D gsave 12152 889 translate 0 0 M +1.01 dup scale -188.172 0 N +(-5) show grestore 13053 1422 M 0 71 R D gsave 13053 889 translate 0 0 M +1.01 dup scale -188.172 0 N +(-4) show grestore 13954 1422 M 0 71 R D gsave 13954 889 translate 0 0 M +1.01 dup scale -188.172 0 N +(-3) show grestore 14855 1422 M 0 71 R D gsave 14855 889 translate 0 0 M +1.01 dup scale -188.172 0 N +(-2) show grestore 15756 1422 M 0 71 R D gsave 15756 889 translate 0 0 M +1.01 dup scale -188.172 0 N +(-1) show grestore 16657 1422 M 0 71 R D gsave 16657 889 translate 0 0 M +1.01 dup scale -117.687 0 N +(0) show grestore 12242 1422 M 0 35 R D 12333 1422 M 0 35 R D 12423 1422 M +0 35 R D 12513 1422 M 0 35 R D 12603 1422 M 0 35 R D 12693 1422 M 0 35 R D +12783 1422 M 0 35 R D 12873 1422 M 0 35 R D 12963 1422 M 0 35 R D +13143 1422 M 0 35 R D 13233 1422 M 0 35 R D 13324 1422 M 0 35 R D +13414 1422 M 0 35 R D 13504 1422 M 0 35 R D 13594 1422 M 0 35 R D +13684 1422 M 0 35 R D 13774 1422 M 0 35 R D 13864 1422 M 0 35 R D +14044 1422 M 0 35 R D 14134 1422 M 0 35 R D 14224 1422 M 0 35 R D +14315 1422 M 0 35 R D 14405 1422 M 0 35 R D 14495 1422 M 0 35 R D +14585 1422 M 0 35 R D 14675 1422 M 0 35 R D 14765 1422 M 0 35 R D +14945 1422 M 0 35 R D 15035 1422 M 0 35 R D 15125 1422 M 0 35 R D +15216 1422 M 0 35 R D 15306 1422 M 0 35 R D 15396 1422 M 0 35 R D +15486 1422 M 0 35 R D 15576 1422 M 0 35 R D 15666 1422 M 0 35 R D +15846 1422 M 0 35 R D 15936 1422 M 0 35 R D 16026 1422 M 0 35 R D +16116 1422 M 0 35 R D 16207 1422 M 0 35 R D 16297 1422 M 0 35 R D +16387 1422 M 0 35 R D 16477 1422 M 0 35 R D 16567 1422 M 0 35 R D +16747 1422 M 0 35 R D 16837 1422 M 0 35 R D 16927 1422 M 0 35 R D +17017 1422 M 0 35 R D 17107 1422 M 0 35 R D 12152 4944 M 4955 0 R D +12152 4944 M 0 -70 R D 13053 4944 M 0 -70 R D 13954 4944 M 0 -70 R D +14855 4944 M 0 -70 R D 15756 4944 M 0 -70 R D 16657 4944 M 0 -70 R D +12242 4944 M 0 -35 R D 12333 4944 M 0 -35 R D 12423 4944 M 0 -35 R D +12513 4944 M 0 -35 R D 12603 4944 M 0 -35 R D 12693 4944 M 0 -35 R D +12783 4944 M 0 -35 R D 12873 4944 M 0 -35 R D 12963 4944 M 0 -35 R D +13143 4944 M 0 -35 R D 13233 4944 M 0 -35 R D 13324 4944 M 0 -35 R D +13414 4944 M 0 -35 R D 13504 4944 M 0 -35 R D 13594 4944 M 0 -35 R D +13684 4944 M 0 -35 R D 13774 4944 M 0 -35 R D 13864 4944 M 0 -35 R D +14044 4944 M 0 -35 R D 14134 4944 M 0 -35 R D 14224 4944 M 0 -35 R D +14315 4944 M 0 -35 R D 14405 4944 M 0 -35 R D 14495 4944 M 0 -35 R D +14585 4944 M 0 -35 R D 14675 4944 M 0 -35 R D 14765 4944 M 0 -35 R D +14945 4944 M 0 -35 R D 15035 4944 M 0 -35 R D 15125 4944 M 0 -35 R D +15216 4944 M 0 -35 R D 15306 4944 M 0 -35 R D 15396 4944 M 0 -35 R D +15486 4944 M 0 -35 R D 15576 4944 M 0 -35 R D 15666 4944 M 0 -35 R D +15846 4944 M 0 -35 R D 15936 4944 M 0 -35 R D 16026 4944 M 0 -35 R D +16116 4944 M 0 -35 R D 16207 4944 M 0 -35 R D 16297 4944 M 0 -35 R D +16387 4944 M 0 -35 R D 16477 4944 M 0 -35 R D 16567 4944 M 0 -35 R D +16747 4944 M 0 -35 R D 16837 4944 M 0 -35 R D 16927 4944 M 0 -35 R D +17017 4944 M 0 -35 R D 17107 4944 M 0 -35 R D 12152 1422 M 0 3522 R D +12152 1422 M 99 0 R D gsave 12040 1422 translate 0 0 M 1.01 dup scale +-117.687 0 N +( ) show grestore 12152 1892 M 99 0 R D gsave 12040 1750 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 2361 M 99 0 R D gsave 12040 2219 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 2831 M 99 0 R D gsave 12040 2689 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 3301 M 99 0 R D gsave 12040 3158 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 3770 M 99 0 R D gsave 12040 3628 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 4240 M 99 0 R D gsave 12040 4098 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 4710 M 99 0 R D gsave 12040 4567 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 12152 1540 M 50 0 R D 12152 1657 M 50 0 R D 12152 1774 M +50 0 R D 12152 2009 M 50 0 R D 12152 2127 M 50 0 R D 12152 2244 M 50 0 R D +12152 2479 M 50 0 R D 12152 2596 M 50 0 R D 12152 2714 M 50 0 R D +12152 2948 M 50 0 R D 12152 3066 M 50 0 R D 12152 3183 M 50 0 R D +12152 3418 M 50 0 R D 12152 3536 M 50 0 R D 12152 3653 M 50 0 R D +12152 3888 M 50 0 R D 12152 4005 M 50 0 R D 12152 4123 M 50 0 R D +12152 4357 M 50 0 R D 12152 4475 M 50 0 R D 12152 4592 M 50 0 R D +12152 4827 M 50 0 R D 12152 4944 M 50 0 R D 17107 1422 M 0 3522 R D +17107 1422 M -99 0 R D 17107 1892 M -99 0 R D 17107 2361 M -99 0 R D +17107 2831 M -99 0 R D 17107 3301 M -99 0 R D 17107 3770 M -99 0 R D +17107 4240 M -99 0 R D 17107 4710 M -99 0 R D 17107 1540 M -49 0 R D +17107 1657 M -49 0 R D 17107 1774 M -49 0 R D 17107 2009 M -49 0 R D +17107 2127 M -49 0 R D 17107 2244 M -49 0 R D 17107 2479 M -49 0 R D +17107 2596 M -49 0 R D 17107 2714 M -49 0 R D 17107 2948 M -49 0 R D +17107 3066 M -49 0 R D 17107 3183 M -49 0 R D 17107 3418 M -49 0 R D +17107 3536 M -49 0 R D 17107 3653 M -49 0 R D 17107 3888 M -49 0 R D +17107 4005 M -49 0 R D 17107 4123 M -49 0 R D 17107 4357 M -49 0 R D +17107 4475 M -49 0 R D 17107 4592 M -49 0 R D 17107 4827 M -49 0 R D +17107 4944 M -49 0 R D 20 setlinewidth 1.000 0.000 0.000 setrgbcolor +12152 1430 M 226 0 R 0 17 R 225 0 R 225 0 R 0 39 R 225 0 R 226 0 R 0 315 R +225 0 R 225 0 R 0 393 R 225 0 R 225 0 R 0 127 R 226 0 R 225 0 R 0 107 R +225 0 R 225 0 R 0 -244 R 226 0 R 225 0 R 0 -284 R 225 0 R 225 0 R 0 -244 R +226 0 R 225 0 R 0 -163 R 225 0 R 225 0 R 0 -71 R 225 0 R D +0.000 0.514 1.000 setrgbcolor 12152 1422 M 226 0 R 225 0 R 225 0 R 225 0 R +226 0 R 0 32 R 225 0 R 225 0 R 0 265 R 225 0 R 225 0 R 0 461 R 226 0 R +225 0 R 0 272 R 225 0 R 225 0 R 0 -98 R 226 0 R 225 0 R 0 132 R 225 0 R +225 0 R 0 -547 R 226 0 R 225 0 R 0 -451 R 225 0 R 225 0 R 0 -66 R 225 0 R D +0.000 0.000 0.000 setrgbcolor 12152 1422 M 226 0 R 225 0 R 225 0 R 225 0 R +226 0 R 225 0 R 225 0 R 225 0 R 225 0 R 226 0 R 225 0 R 225 0 R 225 0 R +0 270 R 226 0 R 225 0 R 0 2749 R 225 0 R 225 0 R 0 -1622 R 226 0 R 225 0 R +0 -1386 R 225 0 R 225 0 R 0 -11 R 225 0 R D gsave 4621 365 translate 0 0 M +1.01 dup scale -1596.38 0 N +(log) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(10) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(\(12 L) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(B) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( / L) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(Edd) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(\)) show grestore gsave 9675 365 translate 0 0 M 1.01 dup scale +-1683.91 0 N +(log) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(10) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(\(52 L) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(SX) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( / L) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(Edd) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(\)) show grestore gsave 14878 365 translate 0 0 M 1.01 dup scale +-1691.13 0 N +(log) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(10) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(\(35 L) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(HX) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( / L) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(Edd) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(\)) show grestore gsave 1499 6706 translate 0 0 M 90 rotate 1.01 dup scale +-2575.77 0 N +(Probability \(Arbitrary Scale\)) show grestore +%%PageTrailer +end +restore +showpage +%%PageResources: font Helvetica +%%Trailer +restore +%%Pages: 1 +%%DocumentNeededResources: font Helvetica +%%EOF diff --git a/feedback/papers/0506398/f22.ps b/feedback/papers/0506398/f22.ps new file mode 100644 index 0000000..d79bdea --- /dev/null +++ b/feedback/papers/0506398/f22.ps @@ -0,0 +1,431 @@ +%!PS-Adobe-3.0 +%%BoundingBox: 54 360 620 643 +%%Title: Graphics produced by IDL +%%For: phopkins@net-93286, +%% /Users/phopkins/Documents/lars_galaxies/plots/high_z +%%Creator: IDL Student Edition 6.0, Mac OS X (darwin ppc m32) +%%CreationDate: Sun May 15 17:00:20 2005 +%%DocumentData: Clean7bit +%%Requirements: color +%%LanguageLevel: 1 +%%PageOrder: Ascend +%%Pages: (atend) +%%DocumentNeededResources: (atend) +%%EndComments +%%BeginProlog +save +%+ prolog.ps -- Prolog for IDL generated PostScript files +%+ Copyright (c) 1988-2003 Research Systems, Inc. All Rights Reserved. +%v 4 +/$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C +{currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint +stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} +bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show +grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 +setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 +{[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 +100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 +{[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef +/ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} +ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont +exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica +findfont exch scalefont setfont (\267) show currentpoint grestore moveto} +bdef end 2.5 setmiterlimit +%%EndProlog +%%Page: 0 1 +%%PageRequirements: color +%%PageResources: (atend) +%%PageOrientation: Portrait +%%PageBoundingBox: 54 360 620 643 +%%BeginPageSetup +save +$IDL_DICT begin 54 360 translate 0.0283465 dup scale +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +%%EndPageSetup +15 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 1794 1422 M 8206 0 R D +1794 1422 M 0 165 R D gsave 1794 889 translate 0 0 M 1.01 dup scale +-308.339 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(6) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 3845 1422 M 0 165 R D +gsave 3845 889 translate 0 0 M 1.01 dup scale -308.339 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(7) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 5897 1422 M 0 165 R D +gsave 5897 889 translate 0 0 M 1.01 dup scale -308.339 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(8) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 7949 1422 M 0 165 R D +gsave 7949 889 translate 0 0 M 1.01 dup scale -308.339 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(9) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 10000 1422 M 0 165 R D +gsave 10000 889 translate 0 0 M 1.01 dup scale -381.305 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(10) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 2411 1422 M 0 82 R D 2773 1422 M 0 82 R D +3029 1422 M 0 82 R D 3228 1422 M 0 82 R D 3390 1422 M 0 82 R D 3528 1422 M +0 82 R D 3647 1422 M 0 82 R D 3752 1422 M 0 82 R D 4463 1422 M 0 82 R D +4824 1422 M 0 82 R D 5081 1422 M 0 82 R D 5279 1422 M 0 82 R D 5442 1422 M +0 82 R D 5579 1422 M 0 82 R D 5698 1422 M 0 82 R D 5803 1422 M 0 82 R D +6515 1422 M 0 82 R D 6876 1422 M 0 82 R D 7132 1422 M 0 82 R D 7331 1422 M +0 82 R D 7493 1422 M 0 82 R D 7631 1422 M 0 82 R D 7750 1422 M 0 82 R D +7855 1422 M 0 82 R D 8566 1422 M 0 82 R D 8927 1422 M 0 82 R D 9184 1422 M +0 82 R D 9383 1422 M 0 82 R D 9545 1422 M 0 82 R D 9682 1422 M 0 82 R D +9801 1422 M 0 82 R D 9906 1422 M 0 82 R D gsave 5897 427 translate 0 0 M +1.01 dup scale -2026.61 0 N +(Black Hole Mass [M) show CP X -101.051 M +%%IncludeResource: font AvantGarde-Book +262.467 /AvantGarde-Book STDFONT +(O) show M X -58.3193 M +%%IncludeResource: font AvantGarde-Book +186.267 /AvantGarde-Book STDFONT +( \267) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(]) show grestore 1794 9645 M 8206 0 R D 1794 9645 M 0 -165 R D 3845 9645 M +0 -165 R D 5897 9645 M 0 -165 R D 7949 9645 M 0 -165 R D 10000 9645 M +0 -165 R D 2411 9645 M 0 -83 R D 2773 9645 M 0 -83 R D 3029 9645 M 0 -83 R D +3228 9645 M 0 -83 R D 3390 9645 M 0 -83 R D 3528 9645 M 0 -83 R D +3647 9645 M 0 -83 R D 3752 9645 M 0 -83 R D 4463 9645 M 0 -83 R D +4824 9645 M 0 -83 R D 5081 9645 M 0 -83 R D 5279 9645 M 0 -83 R D +5442 9645 M 0 -83 R D 5579 9645 M 0 -83 R D 5698 9645 M 0 -83 R D +5803 9645 M 0 -83 R D 6515 9645 M 0 -83 R D 6876 9645 M 0 -83 R D +7132 9645 M 0 -83 R D 7331 9645 M 0 -83 R D 7493 9645 M 0 -83 R D +7631 9645 M 0 -83 R D 7750 9645 M 0 -83 R D 7855 9645 M 0 -83 R D +8566 9645 M 0 -83 R D 8927 9645 M 0 -83 R D 9184 9645 M 0 -83 R D +9383 9645 M 0 -83 R D 9545 9645 M 0 -83 R D 9682 9645 M 0 -83 R D +9801 9645 M 0 -83 R D 9906 9645 M 0 -83 R D 1794 1422 M 0 8223 R D +1794 2490 M 164 0 R D gsave 1682 2348 translate 0 0 M 1.01 dup scale +-704.08 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(-8) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 1794 4626 M 164 0 R D +gsave 1682 4484 translate 0 0 M 1.01 dup scale -704.08 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(-6) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 1794 6762 M 164 0 R D +gsave 1682 6620 translate 0 0 M 1.01 dup scale -704.08 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(-4) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 1794 8898 M 164 0 R D +gsave 1682 8756 translate 0 0 M 1.01 dup scale -704.08 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(-2) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 1794 1422 M 82 0 R D 1794 3558 M 82 0 R D +1794 5694 M 82 0 R D 1794 7830 M 82 0 R D gsave 634 5533 translate 0 0 M +90 rotate 1.01 dup scale -2080.72 0 N +(n\(M\) / dlog\(M\) [Mpc) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(-3) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(]) show grestore 10000 1422 M 0 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D gsave 10527 5533 translate 0 0 M 90 rotate +1.01 dup scale -2521.45 0 N +(AGN Relic ) show +%%IncludeResource: font Symbol +423.333 /Symbol STDFONT +(r) show X -95.92 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(BH) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(\(z\) / ) show +%%IncludeResource: font Symbol +423.333 /Symbol STDFONT +(r) show X -95.92 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(BH) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(\(z=0\)) show grestore 19776 1422 M 0 8223 R D 19776 1422 M -164 0 R D +19776 2988 M -164 0 R D 19776 4554 M -164 0 R D 19776 6121 M -164 0 R D +19776 7687 M -164 0 R D 19776 9253 M -164 0 R D 19776 1814 M -82 0 R D +19776 2205 M -82 0 R D 19776 2597 M -82 0 R D 19776 3380 M -82 0 R D +19776 3771 M -82 0 R D 19776 4163 M -82 0 R D 19776 4946 M -82 0 R D +19776 5338 M -82 0 R D 19776 5729 M -82 0 R D 19776 6512 M -82 0 R D +19776 6904 M -82 0 R D 19776 7295 M -82 0 R D 19776 8078 M -82 0 R D +19776 8470 M -82 0 R D 19776 8861 M -82 0 R D 19776 9645 M -82 0 R D +20 setlinewidth 11570 9253 M 164 -91 R 164 -125 R 164 -157 R 164 -191 R +164 -225 R 164 -255 R 165 -284 R 164 -307 R 164 -327 R 164 -342 R 164 -355 R +164 -363 R 164 -368 R 164 -371 R 165 -370 R 164 -368 R 164 -364 R 164 -359 R +164 -353 R 164 -345 R 164 -314 R 164 -263 R 165 -221 R 164 -184 R 164 -155 R +164 -129 R 164 -107 R 164 -90 R 164 -75 R 164 -62 R 165 -52 R 164 -44 R +164 -36 R 164 -29 R 164 -25 R 164 -21 R 164 -17 R 164 -15 R 165 -12 R +164 -10 R 164 -8 R 164 -7 R 164 -6 R 164 -5 R 164 -4 R 164 -3 R 165 -3 R +164 -2 R 164 -2 R 163 -2 R D gsave 12768 8940 translate 0 0 M 1.15 dup scale +%%IncludeResource: font Symbol +423.333 /Symbol STDFONT +(r) show X -95.92 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(BH) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(\(z=0\) = 2.9) show CP X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(+2.3) show M X -101.051 M +(-1.2 ) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( ) show +%%IncludeResource: font Symbol +423.333 /Symbol STDFONT +(\264) show +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(5) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( M) show CP X -101.051 M +%%IncludeResource: font AvantGarde-Book +262.467 /AvantGarde-Book STDFONT +(O) show M X -58.3193 M +%%IncludeResource: font AvantGarde-Book +186.267 /AvantGarde-Book STDFONT +( \267) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( Mpc) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(-3) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT L1 11570 9253 M 164 -105 R 164 -140 R 164 -173 R +164 -207 R 164 -241 R 164 -269 R 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+%%PageTrailer +end +restore +showpage +%%PageResources: font Helvetica +%%+ font Symbol +%%+ font AvantGarde-Book +%%Trailer +restore +%%Pages: 1 +%%DocumentNeededResources: font Helvetica +%%+ font Symbol +%%+ font AvantGarde-Book +%%EOF diff --git a/feedback/papers/0506398/f23.ps b/feedback/papers/0506398/f23.ps new file mode 100644 index 0000000..8728c2c --- /dev/null +++ b/feedback/papers/0506398/f23.ps @@ -0,0 +1,341 @@ +%!PS-Adobe-3.0 +%%BoundingBox: 54 360 620 643 +%%Title: Graphics produced by IDL +%%For: phopkins@net-93286-2, +%% /Users/phopkins/Documents/lars_galaxies/plots/LF_massive +%%Creator: IDL Student Edition 6.0.3, Mac OS X (darwin ppc m32) +%%CreationDate: Sat Aug 20 03:30:45 2005 +%%DocumentData: Clean7bit +%%Requirements: color +%%LanguageLevel: 1 +%%PageOrder: Ascend +%%Pages: (atend) +%%DocumentNeededResources: (atend) +%%EndComments +%%BeginProlog +save +%+ prolog.ps -- Prolog for IDL generated PostScript files +%+ Copyright (c) 1988-2003 Research Systems, Inc. All Rights Reserved. +%v 4 +/$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C +{currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint +stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} +bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show +grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 +setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 +{[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 +100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 +{[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef +/ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} +ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont +exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica +findfont exch scalefont setfont (\267) show currentpoint grestore moveto} +bdef end 2.5 setmiterlimit +%%EndProlog +%%Page: 0 1 +%%PageRequirements: color +%%PageResources: (atend) +%%PageOrientation: Portrait +%%PageBoundingBox: 54 360 620 643 +%%BeginPageSetup +save +$IDL_DICT begin 54 360 translate 0.0283465 dup scale +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +%%EndPageSetup +15 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 1794 1422 M 8991 0 R D +1794 1422 M 0 157 R D gsave 1794 889 translate 0 0 M 1.01 dup scale +-117.687 0 N +(0) show grestore 4099 1422 M 0 157 R D gsave 4099 889 translate 0 0 M +1.01 dup scale -117.687 0 N +(1) show grestore 6405 1422 M 0 157 R D gsave 6405 889 translate 0 0 M +1.01 dup scale -117.687 0 N +(2) show grestore 8710 1422 M 0 157 R D gsave 8710 889 translate 0 0 M +1.01 dup scale -117.687 0 N +(3) show grestore 2024 1422 M 0 79 R D 2255 1422 M 0 79 R D 2485 1422 M +0 79 R D 2716 1422 M 0 79 R D 2947 1422 M 0 79 R D 3177 1422 M 0 79 R D +3408 1422 M 0 79 R D 3638 1422 M 0 79 R D 3869 1422 M 0 79 R D 4330 1422 M +0 79 R D 4560 1422 M 0 79 R D 4791 1422 M 0 79 R D 5021 1422 M 0 79 R D +5252 1422 M 0 79 R D 5482 1422 M 0 79 R D 5713 1422 M 0 79 R D 5944 1422 M +0 79 R D 6174 1422 M 0 79 R D 6635 1422 M 0 79 R D 6866 1422 M 0 79 R D +7096 1422 M 0 79 R D 7327 1422 M 0 79 R D 7557 1422 M 0 79 R D 7788 1422 M +0 79 R D 8018 1422 M 0 79 R D 8249 1422 M 0 79 R D 8479 1422 M 0 79 R D +8941 1422 M 0 79 R D 9171 1422 M 0 79 R D 9402 1422 M 0 79 R D 9632 1422 M +0 79 R D 9863 1422 M 0 79 R D 10093 1422 M 0 79 R D 10324 1422 M 0 79 R D +10554 1422 M 0 79 R D 10785 1422 M 0 79 R D gsave 6289 427 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 1794 9289 M 8991 0 R D 1794 9289 M 0 -157 R D 4099 9289 M +0 -157 R D 6405 9289 M 0 -157 R D 8710 9289 M 0 -157 R D 2024 9289 M 0 -79 R +D 2255 9289 M 0 -79 R D 2485 9289 M 0 -79 R D 2716 9289 M 0 -79 R D +2947 9289 M 0 -79 R D 3177 9289 M 0 -79 R D 3408 9289 M 0 -79 R D +3638 9289 M 0 -79 R D 3869 9289 M 0 -79 R D 4330 9289 M 0 -79 R D +4560 9289 M 0 -79 R D 4791 9289 M 0 -79 R D 5021 9289 M 0 -79 R D +5252 9289 M 0 -79 R D 5482 9289 M 0 -79 R D 5713 9289 M 0 -79 R D +5944 9289 M 0 -79 R D 6174 9289 M 0 -79 R D 6635 9289 M 0 -79 R D +6866 9289 M 0 -79 R D 7096 9289 M 0 -79 R D 7327 9289 M 0 -79 R D +7557 9289 M 0 -79 R D 7788 9289 M 0 -79 R D 8018 9289 M 0 -79 R D +8249 9289 M 0 -79 R D 8479 9289 M 0 -79 R D 8941 9289 M 0 -79 R D +9171 9289 M 0 -79 R D 9402 9289 M 0 -79 R D 9632 9289 M 0 -79 R D +9863 9289 M 0 -79 R D 10093 9289 M 0 -79 R D 10324 9289 M 0 -79 R D +10554 9289 M 0 -79 R D 10785 9289 M 0 -79 R D 1794 1422 M 0 7867 R D +1794 1573 M 180 0 R D gsave 1682 1431 translate 0 0 M 1.01 dup scale +-588.433 0 N +(0.0) show grestore 1794 3086 M 180 0 R D gsave 1682 2944 translate 0 0 M +1.01 dup scale -588.433 0 N +(0.2) show grestore 1794 4599 M 180 0 R D gsave 1682 4457 translate 0 0 M +1.01 dup scale -588.433 0 N +(0.4) show grestore 1794 6112 M 180 0 R D gsave 1682 5970 translate 0 0 M +1.01 dup scale -588.433 0 N +(0.6) show grestore 1794 7625 M 180 0 R D gsave 1682 7483 translate 0 0 M +1.01 dup scale -588.433 0 N +(0.8) show grestore 1794 9138 M 180 0 R D gsave 1682 8996 translate 0 0 M +1.01 dup scale -588.433 0 N +(1.0) show grestore 1794 1952 M 90 0 R D 1794 2330 M 90 0 R D 1794 2708 M +90 0 R D 1794 3464 M 90 0 R D 1794 3843 M 90 0 R D 1794 4221 M 90 0 R D +1794 4977 M 90 0 R D 1794 5356 M 90 0 R D 1794 5734 M 90 0 R D 1794 6490 M +90 0 R D 1794 6868 M 90 0 R D 1794 7247 M 90 0 R D 1794 8003 M 90 0 R D +1794 8381 M 90 0 R D 1794 8760 M 90 0 R D gsave 751 5356 translate 0 0 M +90 rotate 1.01 dup scale -1734.82 0 N +(n\(M, z\) / n\(M, z=0\)) show grestore 10785 1422 M 0 7867 R D 10785 1573 M +-180 0 R D 10785 3086 M -180 0 R D 10785 4599 M -180 0 R D 10785 6112 M +-180 0 R D 10785 7625 M -180 0 R D 10785 9138 M -180 0 R D 10785 1952 M +-90 0 R D 10785 2330 M -90 0 R D 10785 2708 M -90 0 R D 10785 3464 M -90 0 R +D 10785 3843 M -90 0 R D 10785 4221 M -90 0 R D 10785 4977 M 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230 -7 R 231 -6 R 230 -5 R 231 -4 R 230 -3 R +231 -3 R 230 -2 R 230 -1 R D L2 0.000 1.000 0.580 setrgbcolor 1794 9138 M +230 -111 R 231 -166 R 230 -225 R 231 -279 R 231 -325 R 230 -361 R 231 -386 R +230 -401 R 231 -406 R 230 -406 R 231 -399 R 230 -389 R 231 -375 R 230 -360 R +231 -344 R 230 -328 R 231 -311 R 231 -294 R 230 -279 R 231 -263 R 230 -215 R +231 -174 R 230 -142 R 231 -115 R 230 -94 R 231 -76 R 230 -62 R 231 -51 R +230 -41 R 231 -34 R 231 -28 R 230 -22 R 231 -19 R 230 -15 R 231 -12 R +230 -10 R 231 -8 R 230 -7 R 230 -6 R D L3 1.000 0.780 0.000 setrgbcolor +1794 9138 M 230 -17 R 231 -33 R 230 -58 R 231 -90 R 231 -128 R 230 -168 R +231 -211 R 230 -250 R 231 -287 R 230 -319 R 231 -346 R 230 -368 R 231 -384 R +230 -397 R 231 -405 R 230 -409 R 231 -409 R 231 -408 R 230 -405 R 231 -399 R +230 -337 R 231 -285 R 230 -239 R 231 -201 R 230 -168 R 231 -141 R 230 -117 R +231 -99 R 230 -81 R 231 -69 R 231 -56 R 230 -48 R 231 -39 R 230 -33 R +231 -27 R 230 -23 R 231 -18 R 230 -16 R 230 -13 R D L4 +1.000 0.000 0.000 setrgbcolor 1794 9138 M 230 -2 R 231 -6 R 230 -12 R +231 -23 R 231 -40 R 230 -63 R 231 -92 R 230 -125 R 231 -163 R 230 -201 R +231 -240 R 230 -279 R 231 -316 R 230 -350 R 231 -381 R 230 -409 R 231 -433 R +231 -454 R 230 -470 R 231 -484 R 230 -425 R 231 -373 R 230 -324 R 231 -280 R +230 -242 R 231 -208 R 230 -178 R 231 -152 R 230 -130 R 231 -110 R 231 -94 R +230 -79 R 231 -68 R 230 -57 R 231 -48 R 230 -41 R 231 -34 R 230 -29 R +230 -24 R D L0 0.000 0.000 0.000 setrgbcolor 6443 8364 M 1998 0 R D +gsave 8774 8232 translate 0 0 M 1.1 dup scale +( 10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(6) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( M) show CP X -101.051 M +%%IncludeResource: font AvantGarde-Book +262.467 /AvantGarde-Book STDFONT +(O) show M X -58.3193 M +%%IncludeResource: font AvantGarde-Book +186.267 /AvantGarde-Book STDFONT +( \267) show +%%IncludeResource: font Helvetica +186.267 /Helvetica STDFONT grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT L1 0.000 0.082 1.000 setrgbcolor 6443 7836 M +1998 0 R D 0.000 0.000 0.000 setrgbcolor gsave 8774 7704 translate 0 0 M +1.1 dup scale +( 10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(7) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( M) show CP X -101.051 M +%%IncludeResource: font AvantGarde-Book +262.467 /AvantGarde-Book STDFONT +(O) show M X -58.3193 M +%%IncludeResource: font AvantGarde-Book +186.267 /AvantGarde-Book STDFONT +( \267) show +%%IncludeResource: font Helvetica +186.267 /Helvetica STDFONT grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT L2 0.000 1.000 0.580 setrgbcolor 6443 7308 M +1998 0 R D 0.000 0.000 0.000 setrgbcolor gsave 8774 7176 translate 0 0 M +1.1 dup scale +( 10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(8) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( M) show CP X -101.051 M +%%IncludeResource: font AvantGarde-Book +262.467 /AvantGarde-Book STDFONT +(O) show M X -58.3193 M +%%IncludeResource: font AvantGarde-Book +186.267 /AvantGarde-Book STDFONT +( \267) show +%%IncludeResource: font Helvetica +186.267 /Helvetica STDFONT grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT L3 1.000 0.780 0.000 setrgbcolor 6443 6780 M +1998 0 R D 0.000 0.000 0.000 setrgbcolor gsave 8774 6648 translate 0 0 M +1.1 dup scale +( 10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(9) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( M) show CP X -101.051 M +%%IncludeResource: font AvantGarde-Book +262.467 /AvantGarde-Book STDFONT +(O) show M X -58.3193 M +%%IncludeResource: font AvantGarde-Book +186.267 /AvantGarde-Book STDFONT +( \267) show +%%IncludeResource: font Helvetica +186.267 /Helvetica STDFONT grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT L4 1.000 0.000 0.000 setrgbcolor 6443 6252 M +1998 0 R D 0.000 0.000 0.000 setrgbcolor gsave 8774 6120 translate 0 0 M +1.1 dup scale +( 10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(10) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( M) show CP X -101.051 M +%%IncludeResource: font AvantGarde-Book +262.467 /AvantGarde-Book STDFONT +(O) show M X -58.3193 M +%%IncludeResource: font AvantGarde-Book +186.267 /AvantGarde-Book STDFONT +( \267) show +%%IncludeResource: font Helvetica +186.267 /Helvetica STDFONT grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT gsave 6405 9516 translate 0 0 M 1.01 dup scale +-1881.93 0 N +(Full Lifetimes Model) show grestore 15 setlinewidth L0 10785 1422 M +8991 0 R D 10785 1422 M 0 157 R D gsave 10785 889 translate 0 0 M +1.01 dup scale -117.687 0 N +(0) show grestore 13090 1422 M 0 157 R D gsave 13090 889 translate 0 0 M +1.01 dup scale -117.687 0 N +(1) show grestore 15396 1422 M 0 157 R D gsave 15396 889 translate 0 0 M +1.01 dup scale -117.687 0 N +(2) show grestore 17701 1422 M 0 157 R D gsave 17701 889 translate 0 0 M +1.01 dup scale -117.687 0 N +(3) show grestore 11015 1422 M 0 79 R D 11246 1422 M 0 79 R D 11476 1422 M +0 79 R D 11707 1422 M 0 79 R D 11938 1422 M 0 79 R D 12168 1422 M 0 79 R D +12399 1422 M 0 79 R D 12629 1422 M 0 79 R D 12860 1422 M 0 79 R D +13321 1422 M 0 79 R D 13551 1422 M 0 79 R D 13782 1422 M 0 79 R D +14012 1422 M 0 79 R D 14243 1422 M 0 79 R D 14473 1422 M 0 79 R D +14704 1422 M 0 79 R D 14935 1422 M 0 79 R D 15165 1422 M 0 79 R D +15626 1422 M 0 79 R D 15857 1422 M 0 79 R D 16087 1422 M 0 79 R D +16318 1422 M 0 79 R D 16548 1422 M 0 79 R D 16779 1422 M 0 79 R D +17009 1422 M 0 79 R D 17240 1422 M 0 79 R D 17470 1422 M 0 79 R D +17932 1422 M 0 79 R D 18162 1422 M 0 79 R D 18393 1422 M 0 79 R D +18623 1422 M 0 79 R D 18854 1422 M 0 79 R D 19084 1422 M 0 79 R D +19315 1422 M 0 79 R D 19545 1422 M 0 79 R D 19776 1422 M 0 79 R D +gsave 15280 427 translate 0 0 M 1.01 dup scale -58.8433 0 N +( ) show grestore 10785 9289 M 8991 0 R D 10785 9289 M 0 -157 R D +13090 9289 M 0 -157 R D 15396 9289 M 0 -157 R D 17701 9289 M 0 -157 R D +11015 9289 M 0 -79 R D 11246 9289 M 0 -79 R D 11476 9289 M 0 -79 R D +11707 9289 M 0 -79 R D 11938 9289 M 0 -79 R D 12168 9289 M 0 -79 R D +12399 9289 M 0 -79 R D 12629 9289 M 0 -79 R D 12860 9289 M 0 -79 R D +13321 9289 M 0 -79 R D 13551 9289 M 0 -79 R D 13782 9289 M 0 -79 R D +14012 9289 M 0 -79 R D 14243 9289 M 0 -79 R D 14473 9289 M 0 -79 R D +14704 9289 M 0 -79 R D 14935 9289 M 0 -79 R D 15165 9289 M 0 -79 R D +15626 9289 M 0 -79 R D 15857 9289 M 0 -79 R D 16087 9289 M 0 -79 R D +16318 9289 M 0 -79 R D 16548 9289 M 0 -79 R D 16779 9289 M 0 -79 R D +17009 9289 M 0 -79 R D 17240 9289 M 0 -79 R D 17470 9289 M 0 -79 R D +17932 9289 M 0 -79 R D 18162 9289 M 0 -79 R D 18393 9289 M 0 -79 R D +18623 9289 M 0 -79 R D 18854 9289 M 0 -79 R D 19084 9289 M 0 -79 R D +19315 9289 M 0 -79 R D 19545 9289 M 0 -79 R D 19776 9289 M 0 -79 R D +10785 1422 M 0 7867 R D 10785 1573 M 180 0 R D +gsave 10673 1431 translate 0 0 M 1.01 dup scale -117.687 0 N +( ) show grestore 10785 3086 M 180 0 R D gsave 10673 2944 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 10785 4599 M 180 0 R D gsave 10673 4457 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 10785 6112 M 180 0 R D gsave 10673 5970 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 10785 7625 M 180 0 R D gsave 10673 7483 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 10785 9138 M 180 0 R D gsave 10673 8996 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 10785 1952 M 90 0 R D 10785 2330 M 90 0 R D 10785 2708 M +90 0 R D 10785 3464 M 90 0 R D 10785 3843 M 90 0 R D 10785 4221 M 90 0 R D +10785 4977 M 90 0 R D 10785 5356 M 90 0 R D 10785 5734 M 90 0 R D +10785 6490 M 90 0 R D 10785 6868 M 90 0 R D 10785 7247 M 90 0 R D +10785 8003 M 90 0 R D 10785 8381 M 90 0 R D 10785 8760 M 90 0 R D +gsave 10218 5356 translate 0 0 M 90 rotate 1.01 dup scale -58.8433 0 N +( ) show grestore 19776 1422 M 0 7867 R D 19776 1573 M -180 0 R D +19776 3086 M -180 0 R D 19776 4599 M -180 0 R D 19776 6112 M -180 0 R D +19776 7625 M -180 0 R D 19776 9138 M -180 0 R D 19776 1952 M -90 0 R D +19776 2330 M -90 0 R D 19776 2708 M -90 0 R D 19776 3464 M -90 0 R D +19776 3843 M -90 0 R D 19776 4221 M -90 0 R D 19776 4977 M -90 0 R D +19776 5356 M -90 0 R D 19776 5734 M -90 0 R D 19776 6490 M -90 0 R D +19776 6868 M -90 0 R D 19776 7247 M -90 0 R D 19776 8003 M -90 0 R D +19776 8381 M -90 0 R D 19776 8760 M -90 0 R D +gsave 10785 363 translate 0 0 M 1.01 dup scale -105.833 0 N +(z) show grestore gsave 15396 9516 translate 0 0 M 1.01 dup scale +-2729.44 0 N +(Light-bulb/Exponential Model) show grestore 40 setlinewidth 10785 9138 M +230 -387 R 231 -487 R 230 -597 R 231 -716 R 231 -844 R 230 -712 R 231 -576 R +230 -470 R 231 -387 R 230 -321 R 231 -269 R 230 -226 R 231 -191 R 230 -163 R +231 -139 R 230 -120 R 231 -104 R 231 -91 R 230 -78 R 231 -70 R 230 -61 R +231 -53 R 230 -48 R 231 -43 R 230 -38 R 231 -33 R 230 -31 R 231 -27 R +230 -25 R 231 -23 R 231 -20 R 230 -18 R 231 -17 R 230 -16 R 231 -14 R +230 -13 R 231 -11 R 230 -11 R 230 -10 R D L1 0.000 0.082 1.000 setrgbcolor +10785 9138 M 230 -164 R 231 -207 R 230 -253 R 231 -304 R 231 -358 R +230 -416 R 231 -476 R 230 -540 R 231 -606 R 230 -570 R 231 -477 R 230 -401 R +231 -339 R 230 -289 R 231 -248 R 230 -213 R 231 -185 R 231 -160 R 230 -140 R +231 -123 R 230 -108 R 231 -96 R 230 -85 R 231 -75 R 230 -67 R 231 -61 R +230 -54 R 231 -48 R 230 -44 R 231 -40 R 231 -36 R 230 -33 R 231 -30 R +230 -27 R 231 -25 R 230 -23 R 231 -21 R 230 -20 R 230 -17 R D L2 +0.000 1.000 0.580 setrgbcolor 10785 9138 M 230 -60 R 231 -76 R 230 -92 R +231 -111 R 231 -131 R 230 -152 R 231 -174 R 230 -197 R 231 -222 R 230 -246 R +231 -272 R 230 -299 R 231 -327 R 230 -355 R 231 -384 R 230 -414 R 231 -439 R +231 -382 R 230 -333 R 231 -292 R 230 -258 R 231 -227 R 230 -202 R 231 -179 R +230 -160 R 231 -144 R 230 -128 R 231 -116 R 230 -105 R 231 -95 R 231 -86 R +230 -78 R 231 -71 R 230 -65 R 231 -59 R 230 -55 R 231 -50 R 230 -46 R +230 -42 R D L3 1.000 0.780 0.000 setrgbcolor 10785 9138 M 230 -49 R +231 -61 R 230 -74 R 231 -90 R 231 -106 R 230 -123 R 231 -140 R 230 -159 R +231 -179 R 230 -199 R 231 -220 R 230 -242 R 231 -263 R 230 -287 R 231 -310 R +230 -335 R 231 -359 R 231 -385 R 230 -411 R 231 -360 R 230 -317 R 231 -281 R +230 -248 R 231 -221 R 230 -198 R 231 -176 R 230 -159 R 231 -143 R 230 -129 R +231 -117 R 231 -106 R 230 -96 R 231 -88 R 230 -80 R 231 -73 R 230 -67 R +231 -62 R 230 -56 R 230 -53 R D L4 1.000 0.000 0.000 setrgbcolor +10785 9138 M 230 -49 R 231 -61 R 230 -74 R 231 -90 R 231 -106 R 230 -123 R +231 -140 R 230 -159 R 231 -179 R 230 -199 R 231 -220 R 230 -242 R 231 -263 R +230 -287 R 231 -310 R 230 -335 R 231 -359 R 231 -385 R 230 -411 R 231 -360 R +230 -317 R 231 -281 R 230 -248 R 231 -221 R 230 -198 R 231 -176 R 230 -159 R +231 -143 R 230 -129 R 231 -117 R 231 -106 R 230 -96 R 231 -88 R 230 -80 R +231 -73 R 230 -67 R 231 -62 R 230 -56 R 230 -53 R D +%%PageTrailer +end +restore +showpage +%%PageResources: font Helvetica +%%+ font AvantGarde-Book +%%Trailer +restore +%%Pages: 1 +%%DocumentNeededResources: font Helvetica +%%+ font AvantGarde-Book +%%EOF diff --git a/feedback/papers/0506398/f24.ps b/feedback/papers/0506398/f24.ps new file mode 100644 index 0000000..0cfa667 --- /dev/null +++ b/feedback/papers/0506398/f24.ps @@ -0,0 +1,3113 @@ +%!PS-Adobe-3.0 +%%BoundingBox: 54 360 734 700 +%%Title: Graphics produced by IDL +%%For: phopkins@net-93286, +%% /Users/phopkins/Documents/lars_galaxies/plots/high_z +%%Creator: IDL Student Edition 6.0, Mac OS X (darwin ppc m32) +%%CreationDate: Tue Apr 12 00:34:28 2005 +%%DocumentData: Clean7bit +%%Requirements: color +%%LanguageLevel: 1 +%%PageOrder: Ascend +%%Pages: (atend) +%%DocumentNeededResources: (atend) +%%EndComments +%%BeginProlog +save +%+ prolog.ps -- Prolog for IDL generated PostScript files +%+ Copyright (c) 1988-2003 Research Systems, Inc. All Rights Reserved. +%v 4 +/$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C +{currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint +stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} +bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show +grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 +setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 +{[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 +100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 +{[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef +/ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} +ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont +exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica +findfont exch scalefont setfont (\267) show currentpoint grestore moveto} +bdef end 2.5 setmiterlimit +%%EndProlog +%%Page: 0 1 +%%PageRequirements: color +%%PageResources: (atend) +%%PageOrientation: Portrait +%%PageBoundingBox: 54 360 734 700 +%%BeginPageSetup +save +$IDL_DICT begin 54 360 translate 0.0283465 dup scale +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +%%EndPageSetup +15 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 1794 1422 M 9758 0 R D +1794 1422 M 0 205 R D gsave 1794 889 translate 0 0 M 1.01 dup scale +-235.373 0 N +(14) show grestore 3188 1422 M 0 205 R D gsave 3188 889 translate 0 0 M +1.01 dup scale -235.373 0 N +(15) show grestore 4582 1422 M 0 205 R D gsave 4582 889 translate 0 0 M +1.01 dup scale -235.373 0 N +(16) show grestore 5976 1422 M 0 205 R D gsave 5976 889 translate 0 0 M +1.01 dup scale -235.373 0 N +(17) show grestore 7370 1422 M 0 205 R D gsave 7370 889 translate 0 0 M +1.01 dup scale -235.373 0 N +(18) show grestore 8764 1422 M 0 205 R D gsave 8764 889 translate 0 0 M +1.01 dup scale -235.373 0 N +(19) show grestore 10158 1422 M 0 205 R D gsave 10158 889 translate 0 0 M +1.01 dup scale -235.373 0 N +(20) show grestore 11552 1422 M 0 205 R D gsave 11552 889 translate 0 0 M +1.01 dup scale -235.373 0 N +(21) show grestore 1933 1422 M 0 102 R D 2073 1422 M 0 102 R D 2212 1422 M +0 102 R D 2351 1422 M 0 102 R D 2491 1422 M 0 102 R D 2630 1422 M 0 102 R D +2770 1422 M 0 102 R D 2909 1422 M 0 102 R D 3048 1422 M 0 102 R D +3327 1422 M 0 102 R D 3467 1422 M 0 102 R D 3606 1422 M 0 102 R D +3745 1422 M 0 102 R D 3885 1422 M 0 102 R D 4024 1422 M 0 102 R D +4164 1422 M 0 102 R D 4303 1422 M 0 102 R D 4442 1422 M 0 102 R D +4721 1422 M 0 102 R D 4861 1422 M 0 102 R D 5000 1422 M 0 102 R D +5139 1422 M 0 102 R D 5279 1422 M 0 102 R D 5418 1422 M 0 102 R D +5558 1422 M 0 102 R D 5697 1422 M 0 102 R D 5836 1422 M 0 102 R D +6115 1422 M 0 102 R D 6255 1422 M 0 102 R D 6394 1422 M 0 102 R D +6533 1422 M 0 102 R D 6673 1422 M 0 102 R D 6812 1422 M 0 102 R D +6952 1422 M 0 102 R D 7091 1422 M 0 102 R D 7230 1422 M 0 102 R D +7509 1422 M 0 102 R D 7649 1422 M 0 102 R D 7788 1422 M 0 102 R D +7927 1422 M 0 102 R D 8067 1422 M 0 102 R D 8206 1422 M 0 102 R D +8346 1422 M 0 102 R D 8485 1422 M 0 102 R D 8624 1422 M 0 102 R D +8903 1422 M 0 102 R D 9043 1422 M 0 102 R D 9182 1422 M 0 102 R D +9321 1422 M 0 102 R D 9461 1422 M 0 102 R D 9600 1422 M 0 102 R D +9740 1422 M 0 102 R D 9879 1422 M 0 102 R D 10018 1422 M 0 102 R D +10297 1422 M 0 102 R D 10437 1422 M 0 102 R D 10576 1422 M 0 102 R D +10715 1422 M 0 102 R D 10855 1422 M 0 102 R D 10994 1422 M 0 102 R D +11133 1422 M 0 102 R D 11273 1422 M 0 102 R D 11412 1422 M 0 102 R D +gsave 6673 427 translate 0 0 M 1.01 dup scale -1929.13 0 N +(Log\(Frequency\) [Hz]) show grestore 1794 11645 M 9758 0 R D 1794 11645 M +0 -205 R D 3188 11645 M 0 -205 R D 4582 11645 M 0 -205 R D 5976 11645 M +0 -205 R D 7370 11645 M 0 -205 R D 8764 11645 M 0 -205 R D 10158 11645 M +0 -205 R D 11552 11645 M 0 -205 R D 1933 11645 M 0 -103 R D 2073 11645 M +0 -103 R D 2212 11645 M 0 -103 R D 2351 11645 M 0 -103 R D 2491 11645 M +0 -103 R D 2630 11645 M 0 -103 R D 2770 11645 M 0 -103 R D 2909 11645 M +0 -103 R D 3048 11645 M 0 -103 R D 3327 11645 M 0 -103 R D 3467 11645 M +0 -103 R D 3606 11645 M 0 -103 R D 3745 11645 M 0 -103 R D 3885 11645 M +0 -103 R D 4024 11645 M 0 -103 R D 4164 11645 M 0 -103 R D 4303 11645 M +0 -103 R D 4442 11645 M 0 -103 R D 4721 11645 M 0 -103 R D 4861 11645 M +0 -103 R D 5000 11645 M 0 -103 R D 5139 11645 M 0 -103 R D 5279 11645 M +0 -103 R D 5418 11645 M 0 -103 R D 5558 11645 M 0 -103 R D 5697 11645 M +0 -103 R D 5836 11645 M 0 -103 R D 6115 11645 M 0 -103 R D 6255 11645 M +0 -103 R D 6394 11645 M 0 -103 R D 6533 11645 M 0 -103 R D 6673 11645 M +0 -103 R D 6812 11645 M 0 -103 R D 6952 11645 M 0 -103 R D 7091 11645 M +0 -103 R D 7230 11645 M 0 -103 R D 7509 11645 M 0 -103 R D 7649 11645 M +0 -103 R D 7788 11645 M 0 -103 R D 7927 11645 M 0 -103 R D 8067 11645 M +0 -103 R D 8206 11645 M 0 -103 R D 8346 11645 M 0 -103 R D 8485 11645 M +0 -103 R D 8624 11645 M 0 -103 R D 8903 11645 M 0 -103 R D 9043 11645 M +0 -103 R D 9182 11645 M 0 -103 R D 9321 11645 M 0 -103 R D 9461 11645 M +0 -103 R D 9600 11645 M 0 -103 R D 9740 11645 M 0 -103 R D 9879 11645 M +0 -103 R D 10018 11645 M 0 -103 R D 10297 11645 M 0 -103 R D 10437 11645 M +0 -103 R D 10576 11645 M 0 -103 R D 10715 11645 M 0 -103 R D 10855 11645 M +0 -103 R D 10994 11645 M 0 -103 R D 11133 11645 M 0 -103 R D 11273 11645 M +0 -103 R D 11412 11645 M 0 -103 R D 1794 1422 M 0 10223 R D 1794 1422 M +195 0 R D gsave 1682 1422 translate 0 0 M 1.01 dup scale -704.08 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(-4) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 1794 2882 M 195 0 R D +gsave 1682 2740 translate 0 0 M 1.01 dup scale -704.08 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(-3) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 1794 4343 M 195 0 R D +gsave 1682 4201 translate 0 0 M 1.01 dup scale -704.08 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(-2) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 1794 5803 M 195 0 R D +gsave 1682 5661 translate 0 0 M 1.01 dup scale -704.08 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(-1) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 1794 7264 M 195 0 R D +gsave 1682 7121 translate 0 0 M 1.01 dup scale -616.678 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(0) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 1794 8724 M 195 0 R D +gsave 1682 8582 translate 0 0 M 1.01 dup scale -616.678 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(1) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 1794 10184 M 195 0 R D +gsave 1682 10042 translate 0 0 M 1.01 dup scale -616.678 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(2) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 1794 11645 M 195 0 R D +gsave 1682 11396 translate 0 0 M 1.01 dup scale -616.678 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(3) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT gsave 634 6533 translate 0 0 M 90 rotate +1.01 dup scale -2333.42 0 N +(Integrated ) show +%%IncludeResource: font Symbol +423.333 /Symbol STDFONT +(n) show +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(E) show X -101.051 M +%%IncludeResource: font Symbol +262.467 /Symbol STDFONT +(n) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( [10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(60) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( ergs]) show grestore 11552 1422 M 0 10223 R D 11552 1422 M -195 0 R D +11552 2882 M -195 0 R D 11552 4343 M -195 0 R D 11552 5803 M -195 0 R D +11552 7264 M -195 0 R D 11552 8724 M -195 0 R D 11552 10184 M -195 0 R D +11552 11645 M -195 0 R D 40 setlinewidth 1794 3575 M 97 307 R 98 307 R +98 306 R 97 307 R 98 307 R 97 306 R 98 261 R 98 57 R 97 57 R 98 58 R 97 57 R +98 57 R 97 57 R 98 58 R 98 57 R 97 57 R 98 57 R 97 57 R 98 58 R 97 77 R +98 -78 R 98 -77 R 97 -78 R 98 -78 R 97 -77 R 98 -49 R 97 -29 R 98 -30 R +98 -29 R 97 -29 R 98 -29 R 97 -28 R 98 -29 R 98 -28 R 97 -28 R 98 -28 R +97 -28 R 98 -28 R 97 -27 R 98 -28 R 98 -27 R 97 -27 R 98 -26 R 97 -27 R +98 -26 R 97 -26 R 98 -26 R 98 -26 R 97 -2 R 98 10 R 97 11 R 98 11 R 98 11 R +97 12 R 98 13 R 97 15 R 98 17 R 97 21 R 98 26 R 98 32 R 97 -3 R 98 31 R +97 42 R 98 59 R 97 71 R 98 83 R 98 75 R 97 53 R 98 33 R 97 16 R 98 5 R +97 -6 R 98 -13 R 98 -19 R 97 -24 R 98 -29 R 97 -33 R 98 -39 R 98 -47 R +97 -56 R 98 -68 R 97 -82 R 98 -80 R 97 -78 R 98 -83 R 98 -92 R 97 -104 R +98 -118 R 97 -137 R 98 -157 R 97 -183 R 98 -212 R 98 -249 R 97 -292 R +98 -343 R 97 -405 R 98 -475 R 98 -562 R 92 -628 R D 20 setlinewidth +1794 3531 M 97 292 R 98 286 R 98 279 R 97 270 R 98 259 R 97 246 R 98 185 R +98 -33 R 97 -48 R 98 -61 R 97 -68 R 98 -72 R 97 -74 R 98 -76 R 98 -88 R +97 -127 R 98 -99 R 97 -145 R 98 -172 R 97 -136 R 98 -236 R 21 -2491 R D +5520 1422 M 79 320 R 98 483 R 98 339 R 97 463 R 98 406 R 97 429 R 98 -77 R +97 367 R 98 239 R 98 163 R 97 239 R 98 169 R 97 152 R 98 111 R 98 67 R +97 55 R 98 49 R 97 37 R 98 34 R 97 31 R 98 32 R 98 35 R 97 -4 R 98 33 R +97 44 R 98 60 R 97 71 R 98 84 R 98 75 R 97 54 R 98 33 R 97 16 R 98 4 R +97 -5 R 98 -13 R 98 -19 R 97 -24 R 98 -28 R 97 -34 R 98 -39 R 98 -47 R +97 -56 R 98 -68 R 97 -82 R 98 -80 R 97 -78 R 98 -83 R 98 -92 R 97 -104 R +98 -118 R 97 -137 R 98 -157 R 97 -183 R 98 -212 R 98 -249 R 97 -292 R +98 -343 R 97 -405 R 98 -475 R 98 -562 R 92 -628 R D 10 setlinewidth L2 +1794 3708 M 97 307 R 98 307 R 98 306 R 97 307 R 98 307 R 97 306 R 98 261 R +98 57 R 97 57 R 98 58 R 97 57 R 98 57 R 97 57 R 98 58 R 98 57 R 97 57 R +98 57 R 97 58 R 98 57 R 97 77 R 98 -78 R 98 -77 R 97 -78 R 98 -78 R 97 -77 R +98 -64 R 97 -55 R 98 -55 R 98 -55 R 97 -55 R 98 -55 R 97 -55 R 98 -55 R +98 -54 R 97 -55 R 98 -55 R 97 -55 R 98 -55 R 97 -55 R 98 -55 R 98 -55 R +97 -55 R 98 -55 R 97 -54 R 98 -55 R 97 -55 R 98 -55 R 98 -55 R 97 -12 R +98 10 R 97 11 R 98 11 R 98 11 R 97 12 R 98 13 R 97 15 R 98 17 R 97 21 R +98 26 R 98 32 R 97 -3 R 98 31 R 97 42 R 98 59 R 97 71 R 98 83 R 98 75 R +97 53 R 98 33 R 97 16 R 98 4 R 97 -5 R 98 -13 R 98 -20 R 97 -23 R 98 -29 R +97 -33 R 98 -39 R 98 -47 R 97 -56 R 98 -68 R 97 -82 R 98 -81 R 97 -77 R +98 -83 R 98 -92 R 97 -104 R 98 -118 R 97 -137 R 98 -157 R 97 -183 R +98 -212 R 98 -249 R 97 -292 R 98 -343 R 97 -405 R 98 -476 R 98 -561 R +20 -137 R D 20 setlinewidth L3 1793 3812 M 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R +2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R +2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R +2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R +2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R +2 5 R 2 6 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R +2 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R +1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R +1 6 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R +1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R +1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 2 5 R 1 5 R 2 6 R +2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R +2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R +2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R +2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R +2 5 R 1 6 R 2 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R +2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R +2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R +2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R +2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R +1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R +1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R +1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R +1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R +1 5 R 2 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R +2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R +2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R +2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R +2 5 R 1 6 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 2 5 R 1 5 R +2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R +2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R +2 6 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R +2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R +2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 2 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 0 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R D 3047 6250 M 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 0 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R +1 1 R 2 0 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 2 R 1 1 R 2 2 R 2 2 R 1 2 R 2 2 R 2 1 R +1 2 R 2 2 R 2 2 R 1 1 R 2 2 R 2 2 R 1 2 R 2 1 R 2 2 R 1 2 R 2 2 R 2 1 R +1 2 R 2 2 R 2 2 R 2 1 R 1 2 R 2 2 R 2 2 R 1 1 R 2 2 R 2 2 R 1 2 R 2 -2 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R +2 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R +2 0 R 1 -1 R 2 0 R D 4302 6250 M 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R +2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R +2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R +1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R +2 -1 R 1 -1 R 2 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R +1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R +2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R +2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R +1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R +2 -1 R 1 0 R 2 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R +1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R +2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R +2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R +1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R +2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R +1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R +2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R +2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R +1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R +2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R +1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R +2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R +2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R +1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R +2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R +1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R +2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R +2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R +1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R +2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R +1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R +2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R +2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R +1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R +2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R +1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R +2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R +2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R +1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R +2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R +1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R +2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R +2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R +1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R +2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R +1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R +2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R +2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R +1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R +2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R +1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R +2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R +2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R +1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R +2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R +1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R +2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R +2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R +1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 2 -1 R 1 0 R +2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R +1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R +2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R +2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R +1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 2 -1 R 1 0 R +2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R +1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R +2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R +2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R +1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R D 5556 5802 M 2 0 R 2 -1 R +2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R +2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R +1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R +2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R +2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R +2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R +2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R +1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R +2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R +2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R +2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R +2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R +1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R +2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R +2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R +2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R +2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R +1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R +2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R +2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R +2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R +2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R +1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R +2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R +2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R +2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R +2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R +1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R +2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R +2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R +2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R +2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R +1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R +2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R +2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R +2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R +2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R +1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R +2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R +2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R +2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R +2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R +1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R +2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R +2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R +2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R +2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R +1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R +2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R +2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R +2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R +2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R +2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R +2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R +2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R +1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R +1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R +1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R +1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R +2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R +2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R +2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R +2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R +2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R +2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R +2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R +2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R D 6811 5516 M 2 0 R 1 1 R 2 0 R +2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R +2 0 R 1 0 R 2 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R +2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R +2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R +2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R +2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R +1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R +1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R +1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R +1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R +1 0 R 2 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R +2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R +2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R +2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R +2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 2 0 R 1 1 R +2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R +2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R +2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R +2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R +2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R +1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R +1 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R +1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R +1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R +2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R +2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R +2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R +2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R +2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R +2 1 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R +2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R +2 1 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R +2 1 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R +2 1 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 0 R +1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R +1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R +1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R +1 1 R 2 0 R 2 1 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 2 1 R 1 0 R 2 1 R +2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R +2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 0 R +2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R +2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 1 R 2 0 R +2 1 R 1 0 R 2 1 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 0 R 2 0 R 1 1 R 2 0 R +2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R +2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 2 1 R 1 0 R +2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R +2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 0 R +2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R +2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R +2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 1 R 2 0 R +1 1 R 2 0 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 1 R +1 0 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R 2 0 R 2 1 R +1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 0 R 2 1 R +1 1 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 0 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 2 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 2 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R D 8066 5816 M 1 1 R 2 1 R 2 2 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 2 R 1 1 R 2 1 R 2 1 R 1 1 R 2 2 R 2 1 R 1 1 R 2 1 R +2 2 R 1 1 R 2 1 R 2 1 R 1 2 R 2 1 R 2 1 R 1 1 R 2 2 R 2 1 R 1 1 R 2 2 R +2 1 R 1 1 R 2 2 R 2 1 R 2 1 R 1 1 R 2 2 R 2 1 R 1 2 R 2 1 R 2 1 R 1 2 R +2 1 R 2 1 R 1 2 R 2 1 R 2 1 R 1 2 R 2 1 R 2 2 R 1 1 R 2 1 R 2 2 R 1 1 R +2 2 R 2 1 R 1 1 R 2 2 R 2 1 R 1 2 R 2 1 R 2 2 R 1 1 R 2 1 R 2 2 R 1 1 R +2 2 R 2 1 R 1 2 R 2 1 R 2 1 R 1 2 R 2 1 R 2 2 R 1 1 R 2 2 R 2 1 R 1 2 R +2 1 R 2 1 R 1 2 R 2 1 R 2 2 R 1 1 R 2 2 R 2 1 R 1 2 R 2 1 R 2 1 R 2 2 R +1 1 R 2 2 R 2 1 R 1 2 R 2 1 R 2 1 R 1 2 R 2 1 R 2 2 R 1 1 R 2 2 R 2 1 R +1 1 R 2 2 R 2 1 R 1 2 R 2 1 R 2 1 R 1 2 R 2 1 R 2 2 R 1 1 R 2 1 R 2 2 R +1 1 R 2 1 R 2 2 R 1 1 R 2 1 R 2 2 R 1 1 R 2 2 R 2 1 R 1 1 R 2 2 R 2 1 R +1 1 R 2 1 R 2 2 R 1 1 R 2 1 R 2 2 R 1 1 R 2 1 R 2 1 R 1 2 R 2 1 R 2 1 R +1 2 R 2 1 R 2 1 R 1 1 R 2 2 R 2 1 R 2 1 R 1 1 R 2 1 R 2 2 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 2 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 2 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R 2 1 R +2 1 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R +2 1 R 2 0 R 1 1 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R +2 0 R 2 1 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 1 1 R +2 0 R 2 1 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R +2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R +1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R +1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R +1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R +1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R +2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R +2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R +2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R +2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R +2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R +2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R +2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R +2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R +2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 -1 R +2 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 -1 R +1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 -1 R 1 0 R 2 0 R 2 0 R +1 0 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 -1 R 2 0 R +1 0 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R +1 0 R 2 0 R 2 -1 R 1 0 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R 2 0 R 1 0 R 2 -1 R +2 0 R 1 0 R 2 0 R 2 -1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 0 R 2 0 R +2 -1 R 1 0 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 0 R 2 0 R +2 -1 R 1 0 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 0 R 2 -1 R +2 0 R 1 0 R 2 -1 R 2 0 R 1 0 R 2 0 R 2 -1 R 1 0 R 2 0 R 2 -1 R 1 0 R 2 0 R +2 -1 R 1 0 R 2 0 R 2 0 R 2 -1 R 1 0 R 2 0 R 2 -1 R 1 0 R 2 0 R 2 -1 R 1 0 R +2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 -1 R +2 0 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R +2 0 R 2 -1 R 1 0 R 2 0 R 2 -1 R 1 0 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 0 R +2 -1 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R 2 -1 R +1 0 R 2 -1 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 -1 R +1 0 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R +1 0 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 -1 R +1 0 R 2 -1 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R +1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R +2 -1 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R +1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R +2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R +2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R +1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R +2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R +1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R +2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R +2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R +1 -1 R 2 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R D +9320 6006 M 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R +2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R +1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 0 R +2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R +2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R +2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R +2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R +2 -1 R 1 -2 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 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6 R 1 5 R 2 5 R 2 6 R +1 5 R 2 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 2 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 0 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 0 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R D +3047 7249 M 2 1 R 2 0 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 0 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 2 R 1 2 R 2 2 R 2 1 R 1 2 R 2 2 R 2 2 R 1 1 R +2 2 R 2 2 R 1 2 R 2 1 R 2 2 R 1 2 R 2 2 R 2 1 R 1 2 R 2 2 R 2 2 R 1 1 R +2 2 R 2 2 R 2 2 R 1 1 R 2 2 R 2 2 R 1 2 R 2 1 R 2 2 R 1 2 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +1 0 R 2 -1 R D 4302 7244 M 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R +1 -1 R 2 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R +2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R +2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R D 5556 6618 M 2 -1 R 2 0 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R +2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R +2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 2 0 R +1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R +2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R +2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 2 -1 R +1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 2 -1 R +1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R +2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 2 -1 R +1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R +2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R +1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 2 0 R +1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 0 R +1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R +1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 0 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R +2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R +1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 0 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R +1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R +2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 0 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R +2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R +2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R +1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 0 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 0 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R +2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R +2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R +2 0 R 1 1 R 2 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R +2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R +2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R +2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R +2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 2 0 R +1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R +1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R +1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R +1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R +1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R +2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R +2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R +2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R D 6811 6197 M 2 0 R 1 0 R 2 0 R 2 0 R +1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R +1 0 R 2 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R +2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R +2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R +2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R +2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R +2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R +2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R +2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R +2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R +2 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R +1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R +1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R +1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R +1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 2 0 R 1 0 R 2 0 R +2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R +2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R +2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R +2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R +2 0 R 1 0 R 2 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 1 R +2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R +2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R +2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R +2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 2 0 R +1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R +1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R +1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R +1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R +1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R +2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 1 R +2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R +2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R +2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R +2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R +2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R +2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R +2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R +2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R +1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 1 R 2 0 R 2 1 R +1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 1 R 2 0 R +1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R +1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 1 R 2 0 R +1 1 R 2 0 R 2 1 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 0 R +2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R +1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R +1 0 R 2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 2 0 R 1 1 R 2 0 R +2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R +2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R +2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R +2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R +2 1 R 1 0 R 2 1 R 2 0 R 2 1 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 1 R 1 0 R +2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R +2 0 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 1 R 1 0 R +2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R 2 1 R 2 0 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R +1 1 R 2 0 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 2 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 2 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R D 8066 6496 M 1 2 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 2 R 2 1 R 2 1 R 1 1 R 2 1 R 2 2 R 1 1 R 2 1 R 2 1 R 1 1 R 2 2 R 2 1 R +1 1 R 2 1 R 2 2 R 1 1 R 2 1 R 2 2 R 1 1 R 2 1 R 2 1 R 1 2 R 2 1 R 2 1 R +1 2 R 2 1 R 2 1 R 2 2 R 1 1 R 2 1 R 2 2 R 1 1 R 2 1 R 2 2 R 1 1 R 2 1 R +2 2 R 1 1 R 2 1 R 2 2 R 1 1 R 2 2 R 2 1 R 1 1 R 2 2 R 2 1 R 1 2 R 2 1 R +2 1 R 1 2 R 2 1 R 2 2 R 1 1 R 2 1 R 2 2 R 1 1 R 2 2 R 2 1 R 1 2 R 2 1 R +2 1 R 1 2 R 2 1 R 2 2 R 1 1 R 2 2 R 2 1 R 1 2 R 2 1 R 2 1 R 1 2 R 2 1 R +2 2 R 1 1 R 2 2 R 2 1 R 1 2 R 2 1 R 2 1 R 1 2 R 2 1 R 2 2 R 2 1 R 1 2 R +2 1 R 2 1 R 1 2 R 2 1 R 2 2 R 1 1 R 2 2 R 2 1 R 1 1 R 2 2 R 2 1 R 1 2 R +2 1 R 2 2 R 1 1 R 2 1 R 2 2 R 1 1 R 2 2 R 2 1 R 1 1 R 2 2 R 2 1 R 1 1 R +2 2 R 2 1 R 1 1 R 2 2 R 2 1 R 1 2 R 2 1 R 2 1 R 1 2 R 2 1 R 2 1 R 1 1 R +2 2 R 2 1 R 1 1 R 2 2 R 2 1 R 1 1 R 2 2 R 2 1 R 1 1 R 2 1 R 2 2 R 1 1 R +2 1 R 2 1 R 1 2 R 2 1 R 2 1 R 2 1 R 1 1 R 2 2 R 2 1 R 1 1 R 2 1 R 2 1 R +1 2 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 2 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 2 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 0 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R +2 1 R 1 1 R 2 0 R 2 1 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R +2 1 R 1 0 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 0 R 2 1 R +2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R +2 0 R 1 1 R 2 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R +2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R +2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 1 R +2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R +2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 2 0 R +1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R +1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R +1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R +1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R +1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R +2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R +2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 -1 R 2 1 R +2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R +2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R +2 0 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R +2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 -1 R 1 0 R +2 0 R 2 0 R 1 0 R 2 0 R 2 -1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 -1 R +2 0 R 2 0 R 1 0 R 2 0 R 2 -1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 0 R +2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 -1 R 2 0 R 1 0 R 2 0 R 2 0 R +1 -1 R 2 0 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 0 R 2 0 R 2 -1 R 1 0 R 2 0 R 2 0 R +1 -1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 -1 R 1 0 R 2 0 R 2 -1 R 1 0 R 2 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0 R +2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R +1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R +2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R +2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R +2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R +2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R +1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R +2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R +2 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R D +9320 6687 M 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R +2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R +1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R +2 0 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R +2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 2 -1 R 1 -1 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5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R +2 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R +1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R +1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R +1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 6 R +1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R +2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R +2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 6 R 2 5 R +2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R +2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R +2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R +2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R +2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R +2 5 R 2 6 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R +2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R +1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R +1 6 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R +1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R +1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R +1 5 R 2 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 0 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 0 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 0 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R D +3047 8707 M 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 0 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 0 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 2 R 2 2 R 2 2 R 1 1 R 2 2 R 2 2 R 1 2 R +2 1 R 2 2 R 1 2 R 2 2 R 2 1 R 1 2 R 2 2 R 2 2 R 1 1 R 2 2 R 2 2 R 1 2 R +2 1 R 2 2 R 2 2 R 1 2 R 2 1 R 2 2 R 1 2 R 2 2 R 2 1 R 1 2 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R +1 -1 R 2 -1 R D 4302 8696 M 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R D 5556 7821 M 2 -1 R 2 -1 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 0 R 2 1 R 1 0 R +2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R +2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R +2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R +1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R +1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R +1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R +1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R +2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R +2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R +2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R +2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R +2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R +2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R +2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R +2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R D 6811 7210 M 2 0 R 1 0 R 2 0 R +2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R +2 1 R 1 0 R 2 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R +2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R +2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R +2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R +2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R +1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R +1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R +1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R +1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R +1 0 R 2 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R +2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R +2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R +2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R +2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 2 0 R 1 0 R +2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R +2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 1 R +2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 1 R +2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 1 R +2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R +1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R +1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R +1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R +1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R +2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R +2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R +2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R +2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R +2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R +2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 0 R +2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R +2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 1 R +2 0 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 1 R +2 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R +1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R +1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R +1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R +1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 2 1 R 1 0 R 2 1 R +2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 0 R +2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 1 R +2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R +2 1 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 1 R +2 0 R 1 1 R 2 0 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R +2 0 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 0 R 2 1 R 1 0 R 2 1 R +2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R +2 0 R 1 0 R 2 1 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 2 0 R 1 1 R +2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R +2 0 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R +2 0 R 2 1 R 1 0 R 2 1 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R +2 1 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 1 R 2 0 R 2 1 R 1 0 R +2 1 R 2 1 R 1 0 R 2 1 R 2 0 R 2 1 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 1 R +1 0 R 2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R +1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 1 R +1 0 R 2 1 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 1 R +1 0 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 2 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 2 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R D 8066 7509 M 1 2 R 2 1 R 2 1 R 1 1 R 2 1 R +2 2 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 2 R 1 1 R 2 1 R 2 1 R 1 2 R 2 1 R +2 1 R 1 1 R 2 2 R 2 1 R 1 1 R 2 1 R 2 2 R 1 1 R 2 1 R 2 1 R 1 2 R 2 1 R +2 1 R 1 2 R 2 1 R 2 1 R 2 2 R 1 1 R 2 1 R 2 2 R 1 1 R 2 1 R 2 2 R 1 1 R +2 1 R 2 2 R 1 1 R 2 1 R 2 2 R 1 1 R 2 2 R 2 1 R 1 1 R 2 2 R 2 1 R 1 2 R +2 1 R 2 1 R 1 2 R 2 1 R 2 2 R 1 1 R 2 2 R 2 1 R 1 1 R 2 2 R 2 1 R 1 2 R +2 1 R 2 2 R 1 1 R 2 1 R 2 2 R 1 1 R 2 2 R 2 1 R 1 2 R 2 1 R 2 2 R 1 1 R +2 1 R 2 2 R 1 1 R 2 2 R 2 1 R 1 2 R 2 1 R 2 1 R 1 2 R 2 1 R 2 2 R 2 1 R +1 2 R 2 1 R 2 2 R 1 1 R 2 1 R 2 2 R 1 1 R 2 2 R 2 1 R 1 2 R 2 1 R 2 1 R +1 2 R 2 1 R 2 2 R 1 1 R 2 1 R 2 2 R 1 1 R 2 2 R 2 1 R 1 1 R 2 2 R 2 1 R +1 1 R 2 2 R 2 1 R 1 2 R 2 1 R 2 1 R 1 2 R 2 1 R 2 1 R 1 2 R 2 1 R 2 1 R +1 2 R 2 1 R 2 1 R 1 1 R 2 2 R 2 1 R 1 1 R 2 2 R 2 1 R 1 1 R 2 1 R 2 2 R +1 1 R 2 1 R 2 1 R 1 2 R 2 1 R 2 1 R 2 1 R 1 2 R 2 1 R 2 1 R 1 1 R 2 1 R +2 2 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 2 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 2 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 0 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 1 R 2 0 R 1 1 R +2 1 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 1 1 R +2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 0 R +2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 1 R 2 0 R 2 1 R 1 0 R +2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R +1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R +1 1 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R +1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R +1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R +2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R +2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R +2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R +2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R +2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R +2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R +2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R +2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 -1 R 2 0 R 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2 5 R 1 6 R 2 5 R 2 5 R +1 5 R 2 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R +2 5 R 1 6 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R +2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R +2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 6 R +2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 2 5 R 1 6 R +2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R +2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 6 R 1 5 R +2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R +2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R +2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R +1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R +1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R +1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R +1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 2 5 R 1 5 R 2 5 R +2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R +2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R +2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R +2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R +2 5 R 1 5 R 2 5 R 2 6 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R +2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R +2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R +2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R +2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 2 5 R +1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R +1 5 R 2 6 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R +1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R +1 6 R 2 5 R 2 5 R 1 5 R 2 6 R 2 5 R 1 5 R 2 5 R 2 6 R 1 5 R 2 5 R 2 5 R +1 6 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 2 5 R 1 6 R 2 5 R 2 5 R 1 2 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R D 3047 9244 M 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 0 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 0 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 2 R 1 2 R 2 1 R 2 2 R 1 2 R 2 2 R +2 1 R 1 2 R 2 2 R 2 2 R 1 1 R 2 2 R 2 2 R 1 2 R 2 1 R 2 2 R 1 2 R 2 2 R +2 1 R 1 2 R 2 2 R 2 2 R 2 1 R 1 2 R 2 2 R 2 2 R 1 1 R 2 2 R 2 2 R 1 2 R +2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -2 R D 4302 9231 M 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R D 5556 8267 M 2 -2 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R +1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R +1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R +1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 0 R 2 0 R +2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R +2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R +2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R +2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R +2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R +2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R +2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R +2 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R +1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R +1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R +1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R +1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 2 0 R 1 0 R 2 0 R +2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R +2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R +2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R D 6811 7586 M 2 1 R +1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R +1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R +2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R +2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R +2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R +2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 2 0 R 1 0 R +2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R +2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R +2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R +2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R +2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R +1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R +1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R +1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R +1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R +2 1 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R +2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R +2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R +2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R +2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R +2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R +2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R +2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R +2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R +2 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R +1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R +1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R +1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R +1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 2 0 R 1 1 R 2 0 R +2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R +2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R +2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 1 R +2 0 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 1 R +2 0 R 1 0 R 2 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 1 R +2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R +2 1 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R +2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R +2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 2 1 R +1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R +1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 1 R 1 0 R 2 1 R 2 0 R +1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R +1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 1 R 2 0 R +1 1 R 2 0 R 2 1 R 1 1 R 2 0 R 2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R +2 0 R 1 1 R 2 0 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 0 R 2 0 R +1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R +1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R +2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 0 R +2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 1 R +2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 1 R 2 0 R +2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R +2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 1 R 1 0 R +2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R +2 0 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R +2 1 R 2 0 R 1 1 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R +2 1 R 2 0 R 1 1 R 2 1 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 2 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 0 R 2 2 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 2 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R D 8066 7886 M 1 1 R 2 2 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 2 R 2 1 R 1 1 R 2 1 R 2 1 R 1 2 R 2 1 R 2 1 R +1 1 R 2 1 R 2 2 R 1 1 R 2 1 R 2 2 R 1 1 R 2 1 R 2 1 R 1 2 R 2 1 R 2 1 R +1 1 R 2 2 R 2 1 R 1 1 R 2 2 R 2 1 R 2 1 R 1 2 R 2 1 R 2 1 R 1 2 R 2 1 R +2 1 R 1 2 R 2 1 R 2 1 R 1 2 R 2 1 R 2 2 R 1 1 R 2 1 R 2 2 R 1 1 R 2 2 R +2 1 R 1 1 R 2 2 R 2 1 R 1 2 R 2 1 R 2 1 R 1 2 R 2 1 R 2 2 R 1 1 R 2 2 R +2 1 R 1 1 R 2 2 R 2 1 R 1 2 R 2 1 R 2 2 R 1 1 R 2 1 R 2 2 R 1 1 R 2 2 R +2 1 R 1 2 R 2 1 R 2 2 R 1 1 R 2 1 R 2 2 R 1 1 R 2 2 R 2 1 R 1 2 R 2 1 R +2 2 R 2 1 R 1 1 R 2 2 R 2 1 R 1 2 R 2 1 R 2 2 R 1 1 R 2 1 R 2 2 R 1 1 R +2 2 R 2 1 R 1 2 R 2 1 R 2 1 R 1 2 R 2 1 R 2 2 R 1 1 R 2 1 R 2 2 R 1 1 R +2 1 R 2 2 R 1 1 R 2 2 R 2 1 R 1 1 R 2 2 R 2 1 R 1 1 R 2 2 R 2 1 R 1 1 R +2 2 R 2 1 R 1 1 R 2 2 R 2 1 R 1 1 R 2 2 R 2 1 R 1 1 R 2 1 R 2 2 R 1 1 R +2 1 R 2 1 R 1 2 R 2 1 R 2 1 R 1 1 R 2 2 R 2 1 R 2 1 R 1 1 R 2 2 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 2 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 2 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 2 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 0 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 0 R +1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 1 R 1 1 R 2 0 R +2 1 R 1 1 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R 2 1 R +2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R +2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R +2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 1 R +2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R +2 1 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R +2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R +2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R +2 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R +1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R +1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R +1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R +1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 2 0 R 1 0 R 2 0 R +2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R +2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R +2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R +2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R +2 0 R 1 0 R 2 0 R 2 -1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R +2 0 R 2 0 R 1 0 R 2 0 R 2 -1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R +2 -1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R +2 0 R 2 -1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 -1 R +2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 0 R 2 -1 R 2 0 R 2 0 R +1 0 R 2 0 R 2 -1 R 1 0 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 -1 R +1 0 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 0 R 2 0 R 2 -1 R +1 0 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 0 R 2 -1 R 2 0 R +1 0 R 2 0 R 2 -1 R 1 0 R 2 0 R 2 -1 R 1 0 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R +1 -1 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 -1 R 2 0 R +2 0 R 1 -1 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 -1 R 2 0 R +2 0 R 1 -1 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 -1 R 2 0 R +2 0 R 1 -1 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 0 R 2 -1 R 1 0 R 2 0 R +2 -1 R 1 0 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 0 R 2 -1 R +2 0 R 2 -1 R 1 0 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 -1 R +2 0 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R +2 0 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 -1 R +2 0 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 -1 R +2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 0 R +1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R +2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R +2 -1 R 1 -1 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R +2 -1 R 2 0 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R +1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R +2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R +1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R +2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R +2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R +1 0 R 2 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 -1 R D +9320 8076 M 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R +2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R +1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R +2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R +2 0 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R +2 0 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R +2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R +1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R +2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R +2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R +1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R +2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R +2 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R +2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R +2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -1 R +1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R +2 -1 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R +2 -1 R 2 -2 R 2 -2 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R +2 -2 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R 1 -2 R +2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R 1 -2 R 2 -2 R 2 -2 R 1 -2 R 2 -2 R 2 -1 R +1 -2 R 2 -2 R 2 -2 R 1 -2 R 2 -2 R 2 -2 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R +2 -2 R 1 -2 R 2 -2 R 2 -2 R 1 -2 R 2 -2 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R +2 -2 R 2 -2 R 2 -3 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -2 R 2 -2 R 1 -2 R 2 -2 R +2 -3 R 1 -2 R 2 -2 R 2 -2 R 1 -2 R 2 -2 R 2 -2 R 1 -2 R 2 -2 R 2 -2 R 1 -2 R +2 -2 R 2 -2 R 1 -2 R 2 -2 R 2 -2 R 1 -2 R 2 -3 R 2 -2 R 1 -2 R 2 -2 R 2 -2 R +1 -2 R 2 -2 R 2 -2 R 1 -3 R 2 -2 R 2 -2 R 1 -2 R 2 -2 R 2 -2 R 1 -3 R 2 -2 R +2 -2 R 1 -2 R 2 -2 R 2 -3 R 1 -2 R 2 -2 R 2 -2 R 1 -2 R 2 -3 R 2 -2 R 1 -2 R +2 -3 R 2 -2 R 2 -2 R 1 -2 R 2 -2 R 2 -3 R 1 -2 R 2 -2 R 2 -3 R 1 -2 R 2 -2 R +2 -2 R 1 -3 R 2 -2 R 2 -2 R 1 -3 R 2 -2 R 2 -2 R 1 -3 R 2 -2 R 2 -2 R 1 -3 R +2 -2 R 2 -2 R 1 -3 R 2 -2 R 2 -3 R 1 -2 R 2 -3 R 2 -2 R 1 -2 R 2 -3 R 2 -2 R +1 -3 R 2 -2 R 2 -3 R 1 -2 R 2 -3 R 2 -2 R 1 -2 R 2 -3 R 2 -2 R 1 -3 R 2 -2 R +2 -3 R 1 -3 R 2 -2 R 2 -2 R 1 -3 R 2 -2 R 2 -3 R 1 -2 R 2 -3 R 2 -3 R 1 -2 R +2 -3 R 2 -2 R 2 -3 R 1 -2 R 2 -3 R 2 -3 R 1 -2 R 2 -3 R 2 -3 R 1 -2 R 2 -3 R +2 -2 R 1 -3 R 2 -3 R 2 -2 R 1 -3 R 2 -3 R 2 -3 R 1 -2 R 2 -3 R 2 -2 R 1 -3 R 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1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 0 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 0 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 2 R 1 2 R 2 1 R 2 2 R 1 2 R 2 2 R 2 1 R 1 2 R +2 2 R 2 2 R 1 1 R 2 2 R 2 2 R 1 2 R 2 1 R 2 2 R 1 2 R 2 2 R 2 1 R 1 2 R +2 2 R 2 2 R 2 1 R 1 2 R 2 2 R 2 2 R 1 1 R 2 2 R 2 2 R 1 2 R 2 -2 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R +2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R +1 -2 R 2 -2 R D 4302 10464 M 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R +2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R +2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R +1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R +2 -2 R 1 -1 R 2 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R +1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R +2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R +2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R +1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R +2 -1 R 1 -2 R 2 -1 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R +1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R +2 -2 R 1 -1 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R +2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R +1 -1 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -1 R +2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R +1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R +2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R +2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R +1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R +2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R +1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R +2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R +2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R +1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R +2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R +1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -1 R +2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R +2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R +1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R +2 -1 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R +1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R +2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R +2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R +1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R +2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R +1 -1 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -1 R +2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R +2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R +1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R +2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R +1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R +2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R +2 -1 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R +1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -1 R +2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R +1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R +2 -2 R 1 -1 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R +2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R +1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R +2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R +1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R +2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R +2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R +1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R +2 -1 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R +1 -1 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R +2 -1 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R +2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R +1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 2 -1 R 1 -2 R +2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R +1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R +2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R +2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R +1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 2 -1 R 1 -2 R +2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R +1 -1 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R +2 -1 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R +2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R +1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R D 5556 9294 M 2 -1 R 2 -2 R +2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R +2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R +1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R +2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R +2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R +2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R +2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -1 R +1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R +2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R +2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R +2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R +2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R +1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R +2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R +2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R +2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R +2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R +1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R +2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R +2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -1 R +2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R +2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R +1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R +2 -2 R 1 -1 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R +2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R +2 -1 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R +2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R +1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R +2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R +2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R +2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R +2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -1 R +1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R +2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R +2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R +2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R +2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R +1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R +2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R +2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R +2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R +2 -1 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R +1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R +2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R +2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R +2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R +2 -1 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R +1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R +2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R +2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R +2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R +2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 0 R 2 1 R 2 0 R +1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R +1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R +1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R +2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R +2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R +2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R +2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R +2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R +2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R +2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R +2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R +2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R +1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R +1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R +1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R D 6811 8458 M 2 0 R 1 0 R +2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R +2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R +1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R +1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R +1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R +1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 2 0 R 1 1 R 2 0 R +2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R +2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R +2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R +2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R +2 0 R 1 0 R 2 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R +2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R +2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R +2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R +2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 2 0 R +1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R +1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R +1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R +1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R +1 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R +2 1 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R +2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R +2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R +2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R +2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R +2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R +2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 1 R +2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 1 R +2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R +1 0 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R +1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 1 R +1 0 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 0 R +1 1 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R +1 1 R 2 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R +2 0 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R +2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R +2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R +2 0 R 1 0 R 2 1 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 2 0 R 1 1 R +2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R +2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 1 R 2 0 R 2 1 R 1 0 R +2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R +2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 1 R 1 0 R +2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R +1 0 R 2 0 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 0 R 2 1 R 1 0 R +2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R +2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 2 0 R +1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R +1 1 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R +1 0 R 2 0 R 2 1 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R +1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R +1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 1 R 2 0 R +2 1 R 1 0 R 2 1 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R +2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 1 R 1 0 R 2 1 R +2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R +2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 2 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 2 R 2 1 R 1 1 R 2 1 R 2 1 R +1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 2 R D 8066 8758 M 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 2 R 1 1 R 2 1 R 2 1 R 1 1 R 2 2 R 2 1 R 1 1 R 2 1 R 2 1 R 1 2 R +2 1 R 2 1 R 1 1 R 2 2 R 2 1 R 1 1 R 2 1 R 2 2 R 1 1 R 2 1 R 2 2 R 1 1 R +2 1 R 2 1 R 1 2 R 2 1 R 2 1 R 2 2 R 1 1 R 2 1 R 2 2 R 1 1 R 2 1 R 2 2 R +1 1 R 2 1 R 2 2 R 1 1 R 2 2 R 2 1 R 1 1 R 2 2 R 2 1 R 1 2 R 2 1 R 2 1 R +1 2 R 2 1 R 2 2 R 1 1 R 2 1 R 2 2 R 1 1 R 2 2 R 2 1 R 1 1 R 2 2 R 2 1 R +1 2 R 2 1 R 2 2 R 1 1 R 2 2 R 2 1 R 1 1 R 2 2 R 2 1 R 1 2 R 2 1 R 2 2 R +1 1 R 2 2 R 2 1 R 1 1 R 2 2 R 2 1 R 1 2 R 2 1 R 2 2 R 1 1 R 2 2 R 2 1 R +2 1 R 1 2 R 2 1 R 2 2 R 1 1 R 2 2 R 2 1 R 1 1 R 2 2 R 2 1 R 1 2 R 2 1 R +2 1 R 1 2 R 2 1 R 2 2 R 1 1 R 2 2 R 2 1 R 1 1 R 2 2 R 2 1 R 1 1 R 2 2 R +2 1 R 1 2 R 2 1 R 2 1 R 1 2 R 2 1 R 2 1 R 1 2 R 2 1 R 2 1 R 1 2 R 2 1 R +2 1 R 1 2 R 2 1 R 2 1 R 1 2 R 2 1 R 2 1 R 1 1 R 2 2 R 2 1 R 1 1 R 2 2 R +2 1 R 1 1 R 2 1 R 2 2 R 1 1 R 2 1 R 2 1 R 2 1 R 1 2 R 2 1 R 2 1 R 1 1 R +2 1 R 2 2 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 2 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 2 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 1 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R +2 1 R 2 0 R 2 1 R 1 1 R 2 1 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R 2 1 R 2 1 R +1 0 R 2 1 R 2 1 R 1 1 R 2 0 R 2 1 R 1 1 R 2 1 R 2 0 R 1 1 R 2 1 R 2 1 R +1 0 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R 1 0 R 2 1 R 2 1 R +1 0 R 2 1 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R +1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R +2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R +2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 1 R 2 0 R 1 0 R 2 1 R 2 0 R 1 1 R 2 0 R +2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R 2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R +2 1 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 1 R 2 0 R +2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R +2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 1 R 1 0 R 2 0 R 2 0 R 1 0 R +2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R +2 1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 1 R 2 0 R 2 0 R 1 0 R +2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R +1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 1 R 2 0 R +1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R +1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R +1 0 R 2 0 R 2 -1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R +1 0 R 2 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 0 R 2 0 R +2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R 2 -1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 0 R +2 0 R 1 -1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 0 R 2 0 R +2 0 R 1 0 R 2 -1 R 2 0 R 1 0 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 0 R 2 0 R +2 -1 R 1 0 R 2 0 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 0 R 2 0 R 2 0 R 2 -1 R 1 0 R +2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 0 R 2 0 R 2 -1 R 1 0 R 2 0 R 2 0 R 1 -1 R +2 0 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 0 R 2 0 R 2 -1 R 1 0 R 2 0 R 2 0 R 1 -1 R +2 0 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 0 R 2 0 R 2 -1 R 1 0 R 2 0 R 2 -1 R 1 0 R +2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 0 R +2 -1 R 2 0 R 1 0 R 2 -1 R 2 0 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 0 R 2 -1 R 2 0 R +1 0 R 2 -1 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 0 R 2 -1 R 2 0 R +1 0 R 2 -1 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 0 R 2 -1 R 2 0 R +1 0 R 2 -1 R 2 0 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 0 R +1 -1 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 0 R 2 -1 R 1 0 R 2 0 R 2 -1 R +2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 0 R 2 -1 R 1 0 R 2 0 R 2 -1 R 1 0 R 2 -1 R +2 0 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R +2 0 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 0 R 2 -1 R 1 0 R 2 -1 R +2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R +2 -1 R 1 0 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R +1 -1 R 2 0 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R +2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R +2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R +1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R +2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R +1 0 R 2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R +2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R +2 -1 R 2 0 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R +1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R +2 0 R 1 -1 R 2 -1 R 2 0 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 0 R 2 -1 R 2 -1 R +1 0 R D 9320 8948 M 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R +1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R +2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R +2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R +1 0 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R +2 0 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R +1 -1 R 2 0 R 2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R +2 -1 R 1 -1 R 2 -1 R 2 0 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 0 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 0 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 0 R +1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 0 R +2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R +1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R +2 -1 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R +2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R +1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R +2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R +2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R +1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R +1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -1 R +2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -1 R 1 -2 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R +1 -2 R 2 -1 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 2 -1 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R +2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R +1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R +2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R +2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R +1 -2 R 2 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R +2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -1 R +1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -1 R +2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R +2 -1 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -2 R +1 -1 R 2 -2 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R +2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -2 R 2 -2 R 2 -2 R +1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -2 R 1 -1 R 2 -2 R 2 -2 R 1 -2 R 2 -2 R +2 -2 R 1 -2 R 2 -2 R 2 -1 R 1 -2 R 2 -2 R 2 -2 R 1 -2 R 2 -2 R 2 -2 R 1 -2 R +2 -2 R 2 -2 R 1 -2 R 2 -1 R 2 -2 R 1 -3 R 2 -1 R 2 -2 R 1 -2 R 2 -2 R 2 -2 R +1 -2 R 2 -2 R 2 -2 R 2 -2 R 1 -2 R 2 -2 R 2 -2 R 1 -2 R 2 -2 R 2 -2 R 1 -2 R +2 -2 R 2 -2 R 1 -2 R 2 -2 R 2 -2 R 1 -2 R 2 -2 R 2 -2 R 1 -2 R 2 -3 R 2 -2 R +1 -2 R 2 -2 R 2 -2 R 1 -2 R 2 -2 R 2 -2 R 1 -2 R 2 -2 R 2 -3 R 1 -2 R 2 -2 R +2 -2 R 1 -2 R 2 -2 R 2 -2 R 1 -2 R 2 -3 R 2 -2 R 1 -2 R 2 -2 R 2 -2 R 1 -2 R +2 -2 R 2 -3 R 1 -2 R 2 -2 R 2 -2 R 1 -2 R 2 -3 R 2 -2 R 1 -2 R 2 -2 R 2 -3 R +1 -2 R 2 -2 R 2 -2 R 2 -3 R 1 -2 R 2 -2 R 2 -2 R 1 -3 R 2 -2 R 2 -2 R 1 -3 R +2 -2 R 2 -2 R 1 -2 R 2 -3 R 2 -2 R 1 -2 R 2 -3 R 2 -2 R 1 -3 R 2 -2 R 2 -2 R +1 -2 R 2 -3 R 2 -2 R 1 -3 R 2 -2 R 2 -2 R 1 -3 R 2 -2 R 2 -3 R 1 -2 R 2 -2 R +2 -3 R 1 -2 R 2 -3 R 2 -2 R 1 -3 R 2 -2 R 2 -3 R 1 -2 R 2 -2 R 2 -3 R 1 -2 R +2 -3 R 2 -3 R 1 -2 R 2 -3 R 2 -2 R 1 -2 R 2 -3 R 2 -3 R 1 -2 R 2 -3 R 2 -2 R +1 -3 R 2 -2 R 2 -3 R 2 -2 R 1 -3 R 2 -3 R 2 -2 R 1 -3 R 2 -3 R 2 -2 R 1 -3 R +2 -2 R 2 -3 R 1 -3 R 2 -2 R 2 -3 R 1 -3 R 2 -3 R 2 -2 R 1 -3 R 2 -2 R 2 -3 R +1 -3 R 2 -3 R 2 -2 R 1 -3 R 2 -3 R 2 -3 R 1 -2 R 2 -3 R 2 -3 R 1 -2 R 2 -3 R +2 -3 R 1 -3 R 2 -3 R 2 -3 R 1 -2 R 2 -3 R 2 -3 R 1 -3 R 2 -3 R 2 -3 R 1 -3 R +2 -3 R 2 -2 R 1 -3 R 2 -3 R 2 -3 R D 10575 7813 M 1 -3 R 2 -3 R 2 -3 R +1 -3 R 2 -3 R 2 -2 R 1 -3 R 2 -3 R 2 -3 R 2 -3 R 1 -3 R 2 -3 R 2 -3 R 1 -3 R +2 -3 R 2 -3 R 1 -3 R 2 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R +2 -9 R 1 -9 R 2 -9 R 2 -10 R 1 -10 R 2 -10 R 2 -10 R 2 -11 R 1 -10 R 2 -9 R +2 -9 R 1 -10 R 2 -10 R 2 -10 R 1 -10 R 2 -11 R 2 -11 R 1 -10 R 2 -9 R +2 -10 R 1 -10 R 2 -10 R 2 -10 R 1 -11 R 2 -11 R 2 -11 R 1 -10 R 2 -10 R +2 -10 R 1 -10 R 2 -10 R 2 -11 R 1 -11 R 2 -11 R 2 -12 R 1 -10 R 2 -10 R +2 -10 R 1 -10 R 2 -11 R 2 -11 R 1 -12 R 2 -11 R 2 -12 R 1 -10 R 2 -10 R +2 -11 R 1 -10 R 2 -11 R 2 -12 R 1 -11 R 2 -13 R 2 -11 R 1 -10 R 2 -11 R +2 -11 R 1 -11 R 2 -11 R 2 -12 R 1 -12 R 2 -12 R 2 -12 R 2 -10 R 1 -11 R +2 -11 R 2 -12 R 1 -12 R 2 -12 R 2 -12 R 1 -13 R 2 -11 R 2 -11 R 1 -11 R +2 -12 R 2 -11 R 1 -13 R 2 -12 R 2 -13 R 1 -13 R 2 -11 R 2 -12 R 1 -11 R +2 -12 R 2 -12 R 1 -12 R 2 -13 R 2 -13 R 1 -14 R 2 -11 R 2 -12 R 1 -11 R +2 -13 R 2 -12 R 1 -13 R 2 -13 R 2 -14 R 1 -13 R 2 -12 R 2 -12 R 1 -12 R +2 -12 R 2 -13 R 1 -13 R 2 -14 R 2 -14 R 1 -14 R 2 -11 R 2 -12 R 1 -13 R +2 -13 R 2 -13 R 1 -13 R 2 -15 R 2 -14 R 1 -14 R 2 -12 R 2 -12 R 2 -13 R +1 -13 R 2 -14 R 2 -14 R 1 -14 R 2 -15 R 2 -14 R 1 -12 R 2 -13 R 2 -13 R +1 -14 R 2 -14 R 2 -14 R 1 -15 R 2 -15 R 2 -14 R 1 -13 R 2 -13 R 2 -13 R +1 -14 R 2 -15 R 2 -15 R 1 -15 R 2 -16 R 2 -13 R 1 -13 R 2 -14 R 1 -7 R D +15 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 13794 1422 M 9758 0 R D +13794 1422 M 0 205 R D gsave 13794 889 translate 0 0 M 1.01 dup scale +-294.217 0 N +(0.1) show grestore 18673 1422 M 0 205 R D gsave 18673 889 translate 0 0 M +1.01 dup scale -294.217 0 N +(1.0) show grestore 23552 1422 M 0 205 R D gsave 23552 889 translate 0 0 M +1.01 dup scale -411.903 0 N +(10.0) show grestore 15263 1422 M 0 102 R D 16122 1422 M 0 102 R D +16731 1422 M 0 102 R D 17204 1422 M 0 102 R D 17590 1422 M 0 102 R D +17917 1422 M 0 102 R D 18200 1422 M 0 102 R D 18450 1422 M 0 102 R D +20141 1422 M 0 102 R D 21001 1422 M 0 102 R D 21610 1422 M 0 102 R D +22083 1422 M 0 102 R D 22469 1422 M 0 102 R D 22796 1422 M 0 102 R D +23079 1422 M 0 102 R D 23328 1422 M 0 102 R D +gsave 18673 427 translate 0 0 M 1.01 dup scale -1541.15 0 N +(Frequency [keV]) show grestore 13794 11645 M 9758 0 R D 13794 11645 M +0 -205 R D 18673 11645 M 0 -205 R D 23552 11645 M 0 -205 R D 15263 11645 M +0 -103 R D 16122 11645 M 0 -103 R D 16731 11645 M 0 -103 R D 17204 11645 M +0 -103 R D 17590 11645 M 0 -103 R D 17917 11645 M 0 -103 R D 18200 11645 M +0 -103 R D 18450 11645 M 0 -103 R D 20141 11645 M 0 -103 R D 21001 11645 M +0 -103 R D 21610 11645 M 0 -103 R D 22083 11645 M 0 -103 R D 22469 11645 M +0 -103 R D 22796 11645 M 0 -103 R D 23079 11645 M 0 -103 R D 23328 11645 M +0 -103 R D 13794 1422 M 0 10223 R D 13794 1422 M 195 0 R D +gsave 13682 1422 translate 0 0 M 1.01 dup scale -821.766 0 N +( 10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(-4) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 13794 3598 M 195 0 R D +gsave 13682 3455 translate 0 0 M 1.01 dup scale -821.766 0 N +( 10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(-3) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 13794 5773 M 195 0 R D +gsave 13682 5631 translate 0 0 M 1.01 dup scale -821.766 0 N +( 10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(-2) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 13794 7949 M 195 0 R D +gsave 13682 7806 translate 0 0 M 1.01 dup scale -821.766 0 N +( 10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(-1) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 13794 10124 M 195 0 R D +gsave 13682 9982 translate 0 0 M 1.01 dup scale -734.365 0 N +( 10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(0) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 13794 2077 M 97 0 R D 13794 2460 M 97 0 R D +13794 2732 M 97 0 R D 13794 2943 M 97 0 R D 13794 3115 M 97 0 R D +13794 3261 M 97 0 R D 13794 3387 M 97 0 R D 13794 3498 M 97 0 R D +13794 4252 M 97 0 R D 13794 4636 M 97 0 R D 13794 4907 M 97 0 R D +13794 5118 M 97 0 R D 13794 5290 M 97 0 R D 13794 5436 M 97 0 R D +13794 5562 M 97 0 R D 13794 5674 M 97 0 R D 13794 6428 M 97 0 R D +13794 6811 M 97 0 R D 13794 7083 M 97 0 R D 13794 7294 M 97 0 R D +13794 7466 M 97 0 R D 13794 7612 M 97 0 R D 13794 7738 M 97 0 R D +13794 7849 M 97 0 R D 13794 8603 M 97 0 R D 13794 8986 M 97 0 R D +13794 9258 M 97 0 R D 13794 9469 M 97 0 R D 13794 9641 M 97 0 R D +13794 9787 M 97 0 R D 13794 9913 M 97 0 R D 13794 10024 M 97 0 R D +13794 10779 M 97 0 R D 13794 11162 M 97 0 R D 13794 11434 M 97 0 R D +13794 11645 M 97 0 R D gsave 12516 6533 translate 0 0 M 90 rotate +1.01 dup scale -2333.42 0 N +(Integrated ) show +%%IncludeResource: font Symbol +423.333 /Symbol STDFONT +(n) show +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(E) show X -101.051 M +%%IncludeResource: font Symbol +262.467 /Symbol STDFONT +(n) show X 0 M +%%IncludeResource: font 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R +195 18 R 195 15 R 195 16 R 196 16 R 195 15 R 195 17 R 195 17 R 195 18 R +195 20 R 196 22 R 195 25 R 195 27 R 195 28 R 195 -24 R 195 24 R 196 29 R +194 32 R D 16076 1422 M 60 342 R 195 2053 R 195 1547 R 195 1162 R 195 740 R +196 681 R 195 506 R 195 -655 R 195 473 R 195 353 R 195 135 R 195 202 R +196 13 R 195 126 R 195 165 R 195 133 R 195 81 R 195 89 R 196 72 R 195 58 R +195 33 R 195 43 R 195 36 R 195 24 R 195 28 R 196 25 R 195 21 R 195 22 R +195 21 R 195 22 R 195 22 R 196 25 R 195 26 R 195 28 R 195 29 R 195 -26 R +195 25 R 196 29 R 194 33 R D 17011 1422 M 101 1192 R 195 1763 R 195 -1912 R +195 1659 R 195 1278 R 195 587 R 195 800 R 196 205 R 195 560 R 195 505 R +195 401 R 195 238 R 195 262 R 196 207 R 195 165 R 195 85 R 195 114 R +195 91 R 195 55 R 195 64 R 196 53 R 195 41 R 195 39 R 195 34 R 195 33 R +195 31 R 196 30 R 195 31 R 195 31 R 195 32 R 195 -32 R 195 28 R 196 31 R +194 35 R D 18547 1422 M 126 1242 R 195 1584 R 195 1247 R 195 735 R 195 806 R +196 636 R 195 501 R 195 251 R 195 338 R 195 267 R 195 152 R 195 180 R +196 141 R 195 103 R 195 92 R 195 74 R 195 71 R 195 55 R 196 49 R 195 45 R +195 41 R 195 40 R 195 -48 R 195 37 R 196 37 R 194 41 R D 19499 1422 M +150 1522 R 195 1564 R 195 774 R 195 1050 R 195 821 R 195 458 R 195 545 R +196 420 R 195 301 R 195 259 R 195 204 R 195 188 R 195 133 R 196 108 R +195 89 R 195 76 R 195 65 R 195 -101 R 195 65 R 196 57 R 194 58 R D +20 setlinewidth L2 0.000 0.082 1.000 setrgbcolor 15915 1422 M 26 132 R +195 398 R 195 897 R 195 821 R 195 748 R 195 567 R 196 624 R 195 564 R +195 -713 R 195 525 R 195 472 R 195 228 R 195 373 R 196 83 R 195 318 R +195 358 R 195 321 R 195 212 R 195 253 R 196 223 R 195 194 R 195 106 R +195 151 R 195 129 R 195 80 R 195 98 R 196 82 R 195 64 R 195 60 R 195 51 R +195 50 R 195 42 R 196 40 R 195 38 R 195 36 R 195 36 R 195 -40 R 195 33 R +196 34 R 194 37 R D 0.000 1.000 0.149 setrgbcolor 13794 2170 M 195 467 R +195 449 R 195 430 R 196 413 R 195 396 R 195 380 R 195 366 R 195 351 R +195 338 R 195 326 R 196 316 R 195 97 R 195 284 R 195 263 R 195 244 R +195 179 R 196 208 R 195 193 R 195 -342 R 195 176 R 195 161 R 195 59 R +195 129 R 196 -1 R 195 113 R 195 182 R 195 173 R 195 119 R 195 149 R +196 138 R 195 128 R 195 75 R 195 111 R 195 101 R 195 67 R 195 87 R 196 78 R +195 65 R 195 64 R 195 59 R 195 60 R 195 52 R 196 48 R 195 47 R 195 44 R +195 43 R 195 -53 R 195 39 R 196 40 R 194 42 R D +1.000 0.000 0.000 setrgbcolor 13794 5740 M 195 224 R 195 216 R 195 206 R +196 198 R 195 190 R 195 182 R 195 175 R 195 168 R 195 163 R 195 157 R +196 153 R 195 26 R 195 137 R 195 127 R 195 116 R 195 79 R 196 100 R 195 91 R +195 -241 R 195 81 R 195 73 R 195 11 R 195 56 R 196 -27 R 195 48 R 195 124 R +195 120 R 195 85 R 195 108 R 196 101 R 195 97 R 195 58 R 195 88 R 195 82 R +195 56 R 195 74 R 196 70 R 195 60 R 195 61 R 195 57 R 195 62 R 195 55 R +196 53 R 195 51 R 195 50 R 195 48 R 195 -63 R 195 44 R 196 44 R 194 47 R D +40 setlinewidth 0.000 0.000 0.000 setrgbcolor 14853 1422 M 112 282 R +195 480 R 195 482 R 195 472 R 195 461 R 196 457 R 195 199 R 195 438 R +195 416 R 195 402 R 195 321 R 196 374 R 195 353 R 195 -415 R 195 324 R +195 308 R 195 161 R 195 269 R 196 70 R 195 247 R 195 279 R 195 263 R +195 182 R 195 231 R 196 215 R 195 197 R 195 112 R 195 170 R 195 152 R +195 97 R 195 126 R 196 111 R 195 89 R 195 84 R 195 75 R 195 75 R 195 61 R +196 54 R 195 51 R 195 47 R 195 44 R 195 -57 R 195 42 R 196 40 R 194 44 R D +%%PageTrailer +end +restore +showpage +%%PageResources: font Helvetica +%%+ font Symbol +%%Trailer +restore +%%Pages: 1 +%%DocumentNeededResources: font Helvetica +%%+ font Symbol +%%EOF diff --git a/feedback/papers/0506398/f25.ps b/feedback/papers/0506398/f25.ps new file mode 100644 index 0000000..4a7ddcf --- /dev/null +++ b/feedback/papers/0506398/f25.ps @@ -0,0 +1,692 @@ +%!PS-Adobe-3.0 +%%BoundingBox: 54 360 507 1040 +%%Title: Graphics produced by IDL +%%For: phopkins@core-62-42.cruznet.ucsc.edu, +%% /Users/phopkins/Documents/lars_galaxies/plots/LF_massive +%%Creator: IDL Student Edition 6.0.3, Mac OS X (darwin ppc m32) +%%CreationDate: Thu Aug 18 17:04:39 2005 +%%DocumentData: Clean7bit +%%Requirements: color +%%LanguageLevel: 1 +%%PageOrder: Ascend +%%Pages: (atend) +%%DocumentNeededResources: (atend) +%%EndComments +%%BeginProlog +save +%+ prolog.ps -- Prolog for IDL generated PostScript files +%+ Copyright (c) 1988-2003 Research Systems, Inc. All Rights Reserved. +%v 4 +/$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C +{currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint +stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} +bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show +grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 +setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 +{[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 +100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 +{[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef +/ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} +ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont +exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica +findfont exch scalefont setfont (\267) show currentpoint grestore moveto} +bdef end 2.5 setmiterlimit +%%EndProlog +%%Page: 0 1 +%%PageRequirements: color +%%PageResources: (atend) +%%PageOrientation: Portrait +%%PageBoundingBox: 54 360 507 1040 +%%BeginPageSetup +save +$IDL_DICT begin 54 360 translate 0.0283465 dup scale +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +%%EndPageSetup +15 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 1687 16000 M 14102 0 R D +3616 16000 M 0 147 R D gsave 3616 15499 translate 0 0 M 0.95 dup scale +-58.8433 0 N +( ) show grestore 7303 16000 M 0 147 R D gsave 7303 15499 translate 0 0 M +0.95 dup scale -58.8433 0 N +( ) show grestore 10991 16000 M 0 147 R D gsave 10991 15499 translate 0 0 M +0.95 dup scale -58.8433 0 N +( ) show grestore 14679 16000 M 0 147 R D gsave 14679 15499 translate 0 0 M +0.95 dup scale -58.8433 0 N +( ) show grestore 1687 16000 M 0 73 R D 2148 16000 M 0 73 R D 2505 16000 M +0 73 R D 2797 16000 M 0 73 R D 3044 16000 M 0 73 R D 3258 16000 M 0 73 R D +3447 16000 M 0 73 R D 4726 16000 M 0 73 R D 5375 16000 M 0 73 R D +5836 16000 M 0 73 R D 6193 16000 M 0 73 R D 6485 16000 M 0 73 R D +6732 16000 M 0 73 R D 6946 16000 M 0 73 R D 7135 16000 M 0 73 R D +8414 16000 M 0 73 R D 9063 16000 M 0 73 R D 9524 16000 M 0 73 R D +9881 16000 M 0 73 R D 10173 16000 M 0 73 R D 10420 16000 M 0 73 R D +10634 16000 M 0 73 R D 10822 16000 M 0 73 R D 12101 16000 M 0 73 R D +12751 16000 M 0 73 R D 13212 16000 M 0 73 R D 13569 16000 M 0 73 R D +13861 16000 M 0 73 R D 14108 16000 M 0 73 R D 14322 16000 M 0 73 R D +14510 16000 M 0 73 R D 15789 16000 M 0 73 R D +gsave 8738 15064 translate 0 0 M 0.95 dup scale -58.8433 0 N +( ) show grestore 1687 23331 M 14102 0 R D 3616 23331 M 0 -146 R D +7303 23331 M 0 -146 R D 10991 23331 M 0 -146 R D 14679 23331 M 0 -146 R D +1687 23331 M 0 -73 R D 2148 23331 M 0 -73 R D 2505 23331 M 0 -73 R D +2797 23331 M 0 -73 R D 3044 23331 M 0 -73 R D 3258 23331 M 0 -73 R D +3447 23331 M 0 -73 R D 4726 23331 M 0 -73 R D 5375 23331 M 0 -73 R D +5836 23331 M 0 -73 R D 6193 23331 M 0 -73 R D 6485 23331 M 0 -73 R D +6732 23331 M 0 -73 R D 6946 23331 M 0 -73 R D 7135 23331 M 0 -73 R D +8414 23331 M 0 -73 R D 9063 23331 M 0 -73 R D 9524 23331 M 0 -73 R D +9881 23331 M 0 -73 R D 10173 23331 M 0 -73 R D 10420 23331 M 0 -73 R D +10634 23331 M 0 -73 R D 10822 23331 M 0 -73 R D 12101 23331 M 0 -73 R D +12751 23331 M 0 -73 R D 13212 23331 M 0 -73 R D 13569 23331 M 0 -73 R D +13861 23331 M 0 -73 R D 14108 23331 M 0 -73 R D 14322 23331 M 0 -73 R D +14510 23331 M 0 -73 R D 15789 23331 M 0 -73 R D 1687 16000 M 0 7331 R D +1687 17696 M 282 0 R D gsave 1582 17563 translate 0 0 M 0.95 dup scale +-470.747 0 N +(10) show grestore 1687 23331 M 282 0 R D gsave 1582 23097 translate 0 0 M +0.95 dup scale -706.12 0 N +(100) show grestore 1687 16000 M 141 0 R D 1687 16446 M 141 0 R D +1687 16824 M 141 0 R D 1687 17150 M 141 0 R D 1687 17439 M 141 0 R D +1687 19393 M 141 0 R D 1687 20385 M 141 0 R D 1687 21089 M 141 0 R D +1687 21635 M 141 0 R D 1687 22081 M 141 0 R D 1687 22458 M 141 0 R D +1687 22785 M 141 0 R D 1687 23073 M 141 0 R D 15789 16000 M 0 7331 R D +15789 17696 M -282 0 R D 15789 23331 M -282 0 R D 15789 16000 M -141 0 R D +15789 16446 M -141 0 R D 15789 16824 M -141 0 R D 15789 17150 M -141 0 R D +15789 17439 M -141 0 R D 15789 19393 M -141 0 R D 15789 20385 M -141 0 R D +15789 21089 M -141 0 R D 15789 21635 M -141 0 R D 15789 22081 M -141 0 R D +15789 22458 M -141 0 R D 15789 22785 M -141 0 R D 15789 23073 M -141 0 R D +20 setlinewidth 2550 16000 M 33 41 R 74 97 R 73 101 R 74 104 R 74 105 R +74 104 R 74 104 R 73 105 R 74 105 R 74 104 R 74 104 R 73 102 R 74 103 R +74 102 R 74 101 R 73 100 R 74 98 R 74 97 R 74 95 R 73 95 R 74 93 R 74 92 R +74 90 R 73 90 R 74 88 R 74 86 R 74 84 R 73 83 R 74 81 R 74 80 R 74 77 R +73 75 R 74 72 R 74 70 R 74 68 R 73 68 R 74 66 R 74 66 R 74 67 R 73 65 R +74 66 R 74 67 R 74 67 R 74 68 R 73 69 R 74 70 R 74 72 R 74 72 R 73 74 R +74 75 R 74 77 R 74 77 R 73 78 R 74 78 R 74 79 R 74 79 R 73 78 R 74 77 R +74 77 R 74 78 R 73 75 R 74 73 R 74 70 R 74 67 R 73 63 R 74 61 R 74 56 R +74 54 R 73 49 R 74 46 R 74 42 R 74 38 R 73 34 R 74 30 R 74 26 R 74 23 R +73 18 R 74 15 R 74 12 R 74 7 R 73 5 R 74 1 R 74 -2 R 74 -5 R 74 -7 R +73 -10 R 74 -13 R 74 -15 R 74 -17 R 73 -19 R 74 -21 R 74 -24 R 74 -25 R +73 -27 R 74 -30 R 74 -31 R 74 -33 R 73 -35 R 74 -37 R 74 -38 R 74 -41 R +73 -43 R 74 -45 R 74 -47 R 74 -49 R 73 -51 R 74 -54 R 74 -55 R 74 -58 R +73 -60 R 74 -63 R 74 -64 R 74 -66 R 73 -69 R 74 -71 R 74 -73 R 74 -75 R +73 -77 R 74 -79 R 74 -81 R 74 -84 R 74 -85 R 73 -87 R 74 -90 R 74 -91 R +74 -94 R 73 -95 R 74 -98 R 74 -100 R 74 -101 R 73 -105 R 74 -106 R 74 -109 R +74 -111 R 73 -114 R 74 -117 R 74 -121 R 74 -125 R 73 -128 R 74 -133 R +74 -136 R 74 -142 R 73 -147 R 74 -151 R 74 -157 R 74 -162 R 73 -168 R +74 -174 R 74 -180 R 74 -186 R 73 -193 R 74 -200 R 61 -171 R D +0.980 1.000 0.000 setrgbcolor 2509 16136 M 74 68 R 74 67 R 73 68 R 74 68 R +74 67 R 74 68 R 74 67 R 73 68 R 74 68 R 74 67 R 74 68 R 73 67 R 74 68 R +74 68 R 74 67 R 73 68 R 74 68 R 74 67 R 74 68 R 73 67 R 74 68 R 74 68 R +74 67 R 73 68 R 74 68 R 74 67 R 74 68 R 73 67 R 74 68 R 74 68 R 74 67 R +73 68 R 74 67 R 74 68 R 74 68 R 73 67 R 74 68 R 74 68 R 74 67 R 73 68 R +74 67 R 74 68 R 74 68 R 74 67 R 73 68 R 74 68 R 74 67 R 74 68 R 73 67 R +74 68 R 74 68 R 74 67 R 73 68 R 74 67 R 74 68 R 74 68 R 73 67 R 74 68 R +74 68 R 74 67 R 73 68 R 74 67 R 74 68 R 74 68 R 73 67 R 0 993 R -73 -68 R +-74 -68 R -74 -67 R -74 -68 R -73 -68 R -74 -67 R -74 -68 R -74 -67 R +-73 -68 R -74 -68 R -74 -67 R -74 -68 R -73 -68 R -74 -67 R -74 -68 R +-74 -67 R -73 -68 R -74 -68 R -74 -67 R -74 -68 R -73 -67 R -74 -68 R +-74 -68 R -74 -67 R -74 -68 R -73 -68 R -74 -67 R -74 -68 R -74 -67 R +-73 -68 R -74 -68 R -74 -67 R -74 -68 R -73 -68 R -74 -67 R -74 -68 R +-74 -67 R -73 -68 R -74 -68 R -74 -67 R -74 -68 R -73 -67 R -74 -68 R +-74 -68 R -74 -67 R -73 -68 R -74 -68 R -74 -67 R -74 -68 R -73 -67 R +-74 -68 R -74 -68 R -74 -67 R -73 -68 R -74 -68 R -74 -67 R -74 -68 R +-73 -67 R -74 -68 R -74 -68 R -74 -67 R -74 -68 R -73 -67 R -74 -68 R +-74 -68 R 0 -992 R F +5386 18873 M 73 71 R 74 71 R 74 71 R 74 70 R 74 70 R 73 70 R 74 68 R 74 69 R +74 67 R 73 68 R 74 66 R 74 66 R 74 66 R 73 64 R 74 64 R 74 63 R 74 62 R +73 62 R 74 61 R 74 59 R 74 59 R 73 58 R 74 56 R 74 56 R 74 54 R 73 54 R +74 52 R 74 50 R 74 50 R 73 47 R 74 47 R 74 44 R 74 43 R 73 42 R 74 39 R +74 38 R 74 35 R 73 34 R 74 31 R 74 29 R 74 27 R 73 24 R 74 21 R 74 19 R +74 16 R 74 12 R 73 10 R 74 6 R 74 3 R 74 -1 R 73 -4 R 74 -9 R 74 -13 R +74 -17 R 73 -22 R 74 -27 R 74 -31 R 74 -37 R 73 -42 R 74 -49 R 74 -54 R +74 -60 R 73 -67 R 74 -75 R 74 -81 R 74 -80 R 73 -78 R 74 -75 R 74 -73 R +74 -71 R 73 -69 R 74 -68 R 74 -67 R 74 -66 R 73 -65 R 74 -65 R 74 -63 R +74 -64 R 73 -62 R 74 -63 R 74 -62 R 74 -61 R 74 -62 R 73 -61 R 74 -61 R +74 -61 R 74 -60 R 73 -61 R 74 -60 R 74 -60 R 74 -60 R 73 -59 R 74 -60 R +74 -59 R 74 -59 R 73 -59 R 74 -59 R 74 -59 R 74 -58 R 73 -59 R 74 -58 R +74 -58 R 74 -58 R 73 -58 R 74 -57 R 74 -58 R 74 -57 R 73 -57 R 74 -57 R +74 -57 R 74 -56 R 73 -56 R 74 -57 R 74 -56 R 74 -55 R 73 -56 R 74 -55 R +74 -55 R 74 -55 R 73 -55 R 74 -55 R 74 -54 R 74 -54 R 74 -54 R 73 -53 R +74 -54 R 0 992 R -74 54 R -73 53 R -74 54 R -74 54 R -74 55 R -74 54 R +-73 55 R -74 55 R -74 55 R -74 55 R -73 56 R -74 56 R -74 56 R -74 56 R +-73 56 R -74 57 R -74 56 R -74 57 R -73 57 R -74 58 R -74 57 R -74 58 R +-73 57 R -74 58 R -74 58 R -74 59 R -73 58 R -74 58 R -74 59 R -74 59 R +-73 59 R -74 59 R -74 60 R -74 59 R -73 60 R -74 60 R -74 60 R -74 60 R +-73 60 R -74 61 R -74 60 R -74 61 R -73 61 R -74 62 R -74 61 R -74 62 R +-74 63 R -73 63 R -74 63 R -74 64 R -74 64 R -73 65 R -74 66 R -74 67 R +-74 68 R -73 69 R -74 71 R -74 73 R -74 75 R -73 78 R -74 81 R -74 81 R +-74 74 R -73 67 R -74 60 R -74 55 R -74 48 R -73 42 R -74 37 R -74 32 R +-74 26 R -73 22 R -74 17 R -74 13 R -74 9 R -73 4 R -74 1 R -74 -2 R +-74 -7 R -73 -9 R -74 -13 R -74 -16 R -74 -18 R -74 -22 R -73 -24 R +-74 -27 R -74 -29 R -74 -31 R -73 -33 R -74 -36 R -74 -37 R -74 -40 R +-73 -41 R -74 -43 R -74 -45 R -74 -46 R -73 -48 R -74 -49 R -74 -51 R +-74 -52 R -73 -53 R -74 -55 R -74 -55 R -74 -57 R -73 -58 R -74 -58 R +-74 -60 R -74 -61 R -73 -61 R -74 -63 R -74 -63 R -74 -64 R -73 -64 R +-74 -66 R -74 -65 R -74 -67 R -73 -67 R -74 -68 R -74 -68 R -74 -69 R +-73 -70 R -74 -69 R -74 -71 R -74 -70 R -74 -72 R -73 -71 R 0 -992 R F +80 setlinewidth 0.000 0.514 1.000 setrgbcolor 2509 16682 M 74 68 R 74 67 R +73 68 R 74 68 R 74 67 R 74 68 R 74 67 R 73 68 R 74 68 R 74 67 R 74 68 R +73 68 R 74 67 R 74 68 R 74 67 R 73 68 R 74 68 R 74 67 R 74 68 R 73 67 R +74 68 R 74 68 R 74 67 R 73 68 R 74 68 R 74 67 R 74 68 R 73 67 R 74 68 R +74 68 R 74 67 R 73 68 R 74 68 R 74 67 R 74 68 R 73 67 R 74 68 R 74 68 R +74 67 R 73 68 R 74 67 R 74 68 R 74 68 R 74 67 R 73 68 R 74 68 R 74 67 R +74 68 R 73 67 R 74 68 R 74 68 R 74 67 R 73 68 R 74 68 R 74 67 R 74 68 R +73 67 R 74 68 R 74 68 R 74 67 R 73 68 R 74 67 R 74 68 R 74 68 R 73 67 R D +1.000 0.000 0.000 setrgbcolor 5386 19419 M 73 71 R 74 71 R 74 71 R 74 70 R +74 70 R 73 70 R 74 68 R 74 69 R 74 68 R 73 67 R 74 66 R 74 66 R 74 66 R +73 64 R 74 64 R 74 63 R 74 63 R 73 61 R 74 61 R 74 59 R 74 59 R 73 58 R +74 57 R 74 55 R 74 55 R 73 53 R 74 52 R 74 50 R 74 50 R 73 47 R 74 47 R +74 45 R 74 43 R 73 41 R 74 39 R 74 38 R 74 36 R 73 33 R 74 31 R 74 29 R +74 27 R 73 24 R 74 21 R 74 19 R 74 16 R 74 13 R 73 9 R 74 6 R 74 3 R 74 -1 R +73 -4 R 74 -9 R 74 -13 R 74 -17 R 73 -22 R 74 -26 R 74 -32 R 74 -37 R +73 -42 R 74 -49 R 74 -54 R 74 -60 R 73 -67 R 74 -74 R 74 -81 R 74 -81 R +73 -78 R 74 -75 R 74 -73 R 74 -71 R 73 -69 R 74 -68 R 74 -67 R 74 -66 R +73 -65 R 74 -65 R 74 -63 R 74 -64 R 73 -62 R 74 -63 R 74 -62 R 74 -61 R +74 -62 R 73 -61 R 74 -61 R 74 -61 R 74 -60 R 73 -61 R 74 -60 R 74 -60 R +74 -59 R 73 -60 R 74 -60 R 74 -59 R 74 -59 R 73 -59 R 74 -59 R 74 -59 R +74 -58 R 73 -59 R 74 -58 R 74 -58 R 74 -58 R 73 -58 R 74 -57 R 74 -58 R +74 -57 R 73 -57 R 74 -57 R 74 -57 R 74 -56 R 73 -56 R 74 -57 R 74 -55 R +74 -56 R 73 -56 R 74 -55 R 74 -55 R 74 -55 R 73 -55 R 74 -54 R 74 -55 R +74 -54 R 74 -54 R 73 -53 R 74 -54 R D 20 setlinewidth +0.000 0.000 0.000 setrgbcolor 2550 16000 M 33 41 R 74 97 R 73 101 R 74 104 R +74 105 R 74 104 R 74 104 R 73 105 R 74 105 R 74 104 R 74 104 R 73 102 R +74 103 R 74 102 R 74 101 R 73 100 R 74 98 R 74 97 R 74 95 R 73 95 R 74 93 R +74 92 R 74 90 R 73 90 R 74 88 R 74 86 R 74 84 R 73 83 R 74 81 R 74 80 R +74 77 R 73 75 R 74 72 R 74 70 R 74 68 R 73 68 R 74 66 R 74 66 R 74 67 R +73 65 R 74 66 R 74 67 R 74 67 R 74 68 R 73 69 R 74 70 R 74 72 R 74 72 R +73 74 R 74 75 R 74 77 R 74 77 R 73 78 R 74 78 R 74 79 R 74 79 R 73 78 R +74 77 R 74 77 R 74 78 R 73 75 R 74 73 R 74 70 R 74 67 R 73 63 R 74 61 R +74 56 R 74 54 R 73 49 R 74 46 R 74 42 R 74 38 R 73 34 R 74 30 R 74 26 R +74 23 R 73 18 R 74 15 R 74 12 R 74 7 R 73 5 R 74 1 R 74 -2 R 74 -5 R 74 -7 R +73 -10 R 74 -13 R 74 -15 R 74 -17 R 73 -19 R 74 -21 R 74 -24 R 74 -25 R +73 -27 R 74 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78 R +73 75 R 74 73 R 74 70 R 74 68 R 73 64 R 74 61 R 74 57 R 74 55 R 73 50 R +74 47 R 74 43 R 74 39 R 73 35 R 74 32 R 74 27 R 74 24 R 73 19 R 74 16 R +74 13 R 74 8 R 73 6 R 74 2 R 74 -1 R 74 -4 R 74 -7 R 73 -10 R 74 -11 R +74 -15 R 74 -16 R 73 -19 R 74 -21 R 74 -22 R 74 -25 R 73 -27 R 74 -29 R +74 -30 R 74 -33 R 73 -34 R 74 -36 R 74 -39 R 74 -40 R 73 -42 R 74 -44 R +74 -47 R 74 -48 R 73 -51 R 74 -53 R 74 -55 R 74 -57 R 73 -59 R 74 -62 R +74 -63 R 74 -66 R 73 -68 R 74 -70 R 74 -72 R 74 -75 R 73 -76 R 74 -79 R +74 -80 R 74 -83 R 74 -85 R 73 -87 R 74 -89 R 74 -91 R 74 -93 R 73 -95 R +74 -97 R 74 -99 R 74 -101 R 73 -104 R 74 -105 R 74 -108 R 74 -111 R +73 -113 R 74 -116 R 74 -119 R 74 -124 R 73 -127 R 74 -131 R 74 -135 R +74 -141 R 73 -145 R 74 -149 R 74 -156 R 74 -160 R 73 -166 R 74 -172 R +74 -178 R 3 -9 R D 1876 16000 M 43 41 R 74 75 R 74 78 R 73 79 R 74 82 R +74 86 R 74 88 R 73 91 R 74 92 R 74 95 R 74 97 R 73 102 R 74 105 R 74 105 R +74 105 R 74 105 R 73 106 R 74 105 R 74 105 R 74 104 R 73 104 R 74 103 R +74 103 R 74 102 R 73 101 R 74 99 R 74 98 R 74 97 R 73 95 R 74 94 R 74 93 R +74 92 R 73 90 R 74 89 R 74 87 R 74 85 R 73 84 R 74 82 R 74 80 R 74 78 R +73 75 R 74 73 R 74 70 R 74 69 R 73 67 R 74 67 R 74 67 R 74 66 R 73 67 R +74 66 R 74 68 R 74 68 R 74 69 R 73 70 R 74 71 R 74 72 R 74 74 R 73 75 R +74 77 R 74 78 R 74 78 R 73 79 R 74 80 R 74 80 R 74 80 R 73 79 R 74 78 R +74 78 R 74 78 R 73 75 R 74 72 R 74 70 R 74 67 R 73 63 R 74 60 R 74 56 R +74 53 R 73 48 R 74 45 R 74 41 R 74 37 R 73 33 R 74 30 R 74 25 R 74 22 R +73 17 R 74 14 R 74 11 R 74 6 R 73 4 R 74 0 R 74 -2 R 74 -6 R 74 -8 R +73 -11 R 74 -13 R 74 -15 R 74 -18 R 73 -20 R 74 -21 R 74 -24 R 74 -26 R +73 -28 R 74 -30 R 74 -31 R 74 -34 R 73 -35 R 74 -38 R 74 -39 R 74 -41 R +73 -44 R 74 -45 R 74 -48 R 74 -50 R 73 -52 R 74 -54 R 74 -56 R 74 -59 R +73 -60 R 74 -63 R 74 -65 R 74 -68 R 73 -69 R 74 -71 R 74 -74 R 74 -76 R +73 -77 R 74 -80 R 74 -82 R 74 -84 R 74 -85 R 73 -88 R 74 -90 R 74 -92 R +74 -94 R 73 -96 R 74 -99 R 74 -100 R 74 -102 R 73 -105 R 74 -107 R 74 -110 R +74 -112 R 73 -115 R 74 -119 R 74 -122 R 74 -125 R 73 -130 R 74 -134 R +74 -138 R 74 -143 R 73 -148 R 74 -153 R 74 -159 R 74 -164 R 73 -169 R +74 -176 R 74 -182 R 74 -188 R 73 -195 R 74 -202 R 74 -209 R 74 -217 R +73 -224 R 74 -232 R 8 -29 R D L2 3270 16000 M 51 150 R 73 211 R 74 206 R +74 199 R 74 192 R 73 187 R 74 179 R 74 174 R 74 167 R 73 160 R 74 156 R +74 149 R 74 144 R 73 138 R 74 132 R 74 126 R 74 121 R 73 115 R 74 109 R +74 105 R 74 99 R 73 94 R 74 88 R 74 83 R 74 79 R 73 76 R 74 74 R 74 71 R +74 69 R 73 67 R 74 65 R 74 65 R 74 65 R 74 64 R 73 64 R 74 64 R 74 65 R +74 65 R 73 66 R 74 67 R 74 68 R 74 68 R 73 69 R 74 69 R 74 70 R 74 70 R +73 69 R 74 69 R 74 69 R 74 69 R 73 68 R 74 65 R 74 62 R 74 60 R 73 58 R +74 54 R 74 51 R 74 48 R 73 45 R 74 41 R 74 37 R 74 34 R 73 31 R 74 26 R +74 24 R 74 19 R 73 16 R 74 12 R 74 9 R 74 6 R 73 2 R 74 -1 R 74 -3 R 74 -7 R +74 -8 R 73 -12 R 74 -13 R 74 -16 R 74 -18 R 73 -21 R 74 -22 R 74 -24 R +74 -26 R 73 -28 R 74 -29 R 74 -32 R 74 -33 R 73 -36 R 74 -37 R 74 -39 R +74 -41 R 73 -43 R 74 -45 R 74 -47 R 74 -50 R 73 -51 R 74 -54 R 74 -56 R +74 -58 R 73 -60 R 74 -62 R 74 -65 R 74 -66 R 73 -69 R 74 -71 R 74 -73 R +74 -75 R 73 -77 R 74 -79 R 74 -81 R 74 -84 R 74 -85 R 73 -87 R 74 -90 R +74 -91 R 74 -94 R 73 -96 R 74 -97 R 74 -100 R 74 -102 R 73 -104 R 74 -107 R +74 -108 R 74 -112 R 73 -114 R 74 -117 R 74 -121 R 74 -124 R 73 -128 R +74 -133 R 74 -137 R 74 -142 R 73 -146 R 74 -152 R 74 -156 R 74 -163 R +73 -168 R 74 -173 R 74 -180 R 74 -187 R 73 -193 R 74 -200 R 74 -206 R +35 -103 R D L0 6235 17826 M 1599 0 R D gsave 8100 17720 translate 0 0 M +0.9 dup scale +(Full Model) show grestore L1 6235 17403 M 1599 0 R D +gsave 8100 17298 translate 0 0 M 0.9 dup scale +(~1) show +%%IncludeResource: font Symbol +423.333 /Symbol STDFONT +(s) show +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( Uncertainty) show grestore L2 6235 16981 M 1599 0 R D +gsave 8100 16875 translate 0 0 M 0.9 dup scale +(Full model, but) show grestore gsave 6946 16446 translate 0 0 M +0.9 dup scale +(no N) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(H) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( Variance with Population) show grestore 15 setlinewidth L0 1687 8669 M +14102 0 R D 3616 8669 M 0 147 R D gsave 3616 8167 translate 0 0 M +0.95 dup scale -58.8433 0 N +( ) show grestore 7303 8669 M 0 147 R D gsave 7303 8167 translate 0 0 M +0.95 dup scale -58.8433 0 N +( ) show grestore 10991 8669 M 0 147 R D gsave 10991 8167 translate 0 0 M +0.95 dup scale -58.8433 0 N +( ) show grestore 14679 8669 M 0 147 R D gsave 14679 8167 translate 0 0 M +0.95 dup scale -58.8433 0 N +( ) show grestore 1687 8669 M 0 73 R D 2148 8669 M 0 73 R D 2505 8669 M +0 73 R D 2797 8669 M 0 73 R D 3044 8669 M 0 73 R D 3258 8669 M 0 73 R D +3447 8669 M 0 73 R D 4726 8669 M 0 73 R D 5375 8669 M 0 73 R D 5836 8669 M +0 73 R D 6193 8669 M 0 73 R D 6485 8669 M 0 73 R D 6732 8669 M 0 73 R D +6946 8669 M 0 73 R D 7135 8669 M 0 73 R D 8414 8669 M 0 73 R D 9063 8669 M +0 73 R D 9524 8669 M 0 73 R D 9881 8669 M 0 73 R D 10173 8669 M 0 73 R D +10420 8669 M 0 73 R D 10634 8669 M 0 73 R D 10822 8669 M 0 73 R D +12101 8669 M 0 73 R D 12751 8669 M 0 73 R D 13212 8669 M 0 73 R D +13569 8669 M 0 73 R D 13861 8669 M 0 73 R D 14108 8669 M 0 73 R D +14322 8669 M 0 73 R D 14510 8669 M 0 73 R D 15789 8669 M 0 73 R D +gsave 8738 7733 translate 0 0 M 0.95 dup scale -58.8433 0 N +( ) show grestore 1687 16000 M 14102 0 R D 3616 16000 M 0 -147 R D +7303 16000 M 0 -147 R D 10991 16000 M 0 -147 R D 14679 16000 M 0 -147 R D +1687 16000 M 0 -73 R D 2148 16000 M 0 -73 R D 2505 16000 M 0 -73 R D +2797 16000 M 0 -73 R D 3044 16000 M 0 -73 R D 3258 16000 M 0 -73 R D +3447 16000 M 0 -73 R D 4726 16000 M 0 -73 R D 5375 16000 M 0 -73 R D +5836 16000 M 0 -73 R D 6193 16000 M 0 -73 R D 6485 16000 M 0 -73 R D +6732 16000 M 0 -73 R D 6946 16000 M 0 -73 R D 7135 16000 M 0 -73 R D +8414 16000 M 0 -73 R D 9063 16000 M 0 -73 R D 9524 16000 M 0 -73 R D +9881 16000 M 0 -73 R D 10173 16000 M 0 -73 R D 10420 16000 M 0 -73 R D +10634 16000 M 0 -73 R D 10822 16000 M 0 -73 R D 12101 16000 M 0 -73 R D +12751 16000 M 0 -73 R D 13212 16000 M 0 -73 R D 13569 16000 M 0 -73 R D +13861 16000 M 0 -73 R D 14108 16000 M 0 -73 R D 14322 16000 M 0 -73 R D +14510 16000 M 0 -73 R D 15789 16000 M 0 -73 R D 1687 8669 M 0 7331 R D +1687 10365 M 282 0 R D gsave 1582 10231 translate 0 0 M 0.95 dup scale +-470.747 0 N +(10) show grestore 1687 16000 M 282 0 R D gsave 1582 15766 translate 0 0 M +0.95 dup scale -706.12 0 N +(100) show grestore 1687 8669 M 141 0 R D 1687 9115 M 141 0 R D 1687 9492 M +141 0 R D 1687 9819 M 141 0 R D 1687 10107 M 141 0 R D 1687 12061 M 141 0 R +D 1687 13054 M 141 0 R D 1687 13758 M 141 0 R D 1687 14304 M 141 0 R D +1687 14750 M 141 0 R D 1687 15127 M 141 0 R D 1687 15454 M 141 0 R D +1687 15742 M 141 0 R D gsave 595 12335 translate 0 0 M 90 rotate +0.95 dup scale -2962.79 0 N +(E I\(E\) [ keV) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(2) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( cm) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(-2) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( s) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(-1) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( keV) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(-1) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( sr) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(-1) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( ]) show grestore 15789 8669 M 0 7331 R D 15789 10365 M -282 0 R D +15789 16000 M -282 0 R D 15789 8669 M -141 0 R D 15789 9115 M -141 0 R D +15789 9492 M -141 0 R D 15789 9819 M -141 0 R D 15789 10107 M -141 0 R D +15789 12061 M -141 0 R D 15789 13054 M -141 0 R D 15789 13758 M -141 0 R D +15789 14304 M -141 0 R D 15789 14750 M -141 0 R D 15789 15127 M -141 0 R D +15789 15454 M -141 0 R D 15789 15742 M -141 0 R D +0.980 1.000 0.000 setrgbcolor 2509 8805 M 74 67 R 74 68 R 73 68 R 74 67 R +74 68 R 74 68 R 74 67 R 73 68 R 74 67 R 74 68 R 74 68 R 73 67 R 74 68 R +74 68 R 74 67 R 73 68 R 74 67 R 74 68 R 74 68 R 73 67 R 74 68 R 74 67 R +74 68 R 73 68 R 74 67 R 74 68 R 74 68 R 73 67 R 74 68 R 74 67 R 74 68 R +73 68 R 74 67 R 74 68 R 74 68 R 73 67 R 74 68 R 74 67 R 74 68 R 73 68 R +74 67 R 74 68 R 74 67 R 74 68 R 73 68 R 74 67 R 74 68 R 74 68 R 73 67 R +74 68 R 74 67 R 74 68 R 73 68 R 74 67 R 74 68 R 74 68 R 73 67 R 74 68 R +74 67 R 74 68 R 73 68 R 74 67 R 74 68 R 74 67 R 73 68 R 0 992 R -73 -67 R +-74 -68 R -74 -68 R -74 -67 R -73 -68 R -74 -67 R -74 -68 R -74 -68 R +-73 -67 R -74 -68 R -74 -67 R -74 -68 R -73 -68 R 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74 -27 R 74 -31 R 74 -37 R 73 -43 R 74 -48 R 74 -54 R +74 -61 R 73 -67 R 74 -74 R 74 -81 R 74 -80 R 73 -78 R 74 -75 R 74 -73 R +74 -71 R 73 -69 R 74 -68 R 74 -67 R 74 -66 R 73 -65 R 74 -65 R 74 -64 R +74 -63 R 73 -63 R 74 -62 R 74 -62 R 74 -62 R 74 -61 R 73 -61 R 74 -61 R +74 -61 R 74 -60 R 73 -61 R 74 -60 R 74 -60 R 74 -60 R 73 -59 R 74 -60 R +74 -59 R 74 -59 R 73 -59 R 74 -59 R 74 -59 R 74 -59 R 73 -58 R 74 -58 R +74 -58 R 74 -58 R 73 -58 R 74 -57 R 74 -58 R 74 -57 R 73 -57 R 74 -57 R +74 -57 R 74 -56 R 73 -57 R 74 -56 R 74 -56 R 74 -56 R 73 -55 R 74 -55 R +74 -56 R 74 -55 R 73 -54 R 74 -55 R 74 -54 R 74 -54 R 74 -54 R 73 -54 R +74 -53 R 0 992 R -74 54 R -73 53 R -74 54 R -74 54 R -74 54 R -74 55 R +-73 55 R -74 55 R -74 55 R -74 55 R -73 56 R -74 56 R -74 55 R -74 57 R +-73 56 R -74 56 R -74 57 R -74 57 R -73 57 R -74 57 R -74 58 R -74 57 R +-73 58 R -74 58 R -74 58 R -74 58 R -73 59 R -74 58 R -74 59 R -74 59 R +-73 59 R -74 59 R -74 59 R -74 60 R -73 60 R -74 59 R -74 60 R -74 60 R +-73 61 R -74 60 R -74 61 R -74 61 R -73 61 R -74 62 R -74 61 R -74 62 R +-74 63 R -73 62 R -74 64 R -74 63 R -74 65 R -73 65 R -74 66 R -74 67 R +-74 68 R -73 69 R -74 71 R -74 73 R -74 75 R -73 78 R -74 81 R -74 81 R +-74 74 R -73 67 R -74 60 R -74 54 R -74 49 R -73 42 R -74 37 R -74 32 R +-74 26 R -73 22 R -74 17 R -74 13 R -74 9 R -73 4 R -74 1 R -74 -3 R +-74 -6 R -73 -9 R -74 -13 R -74 -16 R -74 -19 R -74 -21 R -73 -24 R +-74 -27 R -74 -29 R -74 -31 R -73 -34 R -74 -35 R -74 -38 R -74 -39 R +-73 -41 R -74 -44 R -74 -44 R -74 -47 R -73 -47 R -74 -50 R -74 -50 R +-74 -52 R -73 -53 R -74 -55 R -74 -56 R -74 -56 R -73 -58 R -74 -59 R +-74 -59 R -74 -61 R -73 -61 R -74 -63 R -74 -63 R -74 -64 R -73 -64 R +-74 -66 R -74 -66 R -74 -66 R -73 -67 R -74 -68 R -74 -69 R -74 -68 R +-73 -70 R -74 -70 R -74 -70 R -74 -71 R -74 -71 R -73 -71 R 0 -993 R F +80 setlinewidth 0.000 0.514 1.000 setrgbcolor 2509 9351 M 74 68 R 74 67 R +73 68 R 74 67 R 74 68 R 74 68 R 74 67 R 73 68 R 74 67 R 74 68 R 74 68 R +73 67 R 74 68 R 74 68 R 74 67 R 73 68 R 74 67 R 74 68 R 74 68 R 73 67 R +74 68 R 74 68 R 74 67 R 73 68 R 74 67 R 74 68 R 74 68 R 73 67 R 74 68 R +74 67 R 74 68 R 73 68 R 74 67 R 74 68 R 74 68 R 73 67 R 74 68 R 74 67 R +74 68 R 73 68 R 74 67 R 74 68 R 74 68 R 74 67 R 73 68 R 74 67 R 74 68 R +74 68 R 73 67 R 74 68 R 74 67 R 74 68 R 73 68 R 74 67 R 74 68 R 74 68 R +73 67 R 74 68 R 74 67 R 74 68 R 73 68 R 74 67 R 74 68 R 74 68 R 73 67 R D +1.000 0.000 0.000 setrgbcolor 5386 12087 M 73 72 R 74 71 R 74 71 R 74 70 R +74 70 R 73 69 R 74 69 R 74 69 R 74 67 R 73 68 R 74 66 R 74 66 R 74 65 R +73 65 R 74 64 R 74 63 R 74 62 R 73 62 R 74 60 R 74 60 R 74 59 R 73 58 R +74 56 R 74 56 R 74 54 R 73 54 R 74 52 R 74 50 R 74 49 R 73 48 R 74 47 R +74 44 R 74 43 R 73 42 R 74 39 R 74 38 R 74 35 R 73 34 R 74 31 R 74 29 R +74 27 R 73 24 R 74 21 R 74 19 R 74 16 R 74 12 R 73 10 R 74 6 R 74 3 R +74 -1 R 73 -5 R 74 -8 R 74 -13 R 74 -17 R 73 -22 R 74 -27 R 74 -31 R +74 -37 R 73 -43 R 74 -48 R 74 -54 R 74 -60 R 73 -68 R 74 -74 R 74 -81 R +74 -80 R 73 -78 R 74 -75 R 74 -73 R 74 -71 R 73 -69 R 74 -68 R 74 -67 R +74 -66 R 73 -65 R 74 -65 R 74 -63 R 74 -64 R 73 -63 R 74 -62 R 74 -62 R +74 -62 R 74 -61 R 73 -61 R 74 -61 R 74 -61 R 74 -60 R 73 -61 R 74 -60 R +74 -60 R 74 -60 R 73 -59 R 74 -60 R 74 -59 R 74 -59 R 73 -59 R 74 -59 R +74 -59 R 74 -58 R 73 -59 R 74 -58 R 74 -58 R 74 -58 R 73 -58 R 74 -57 R +74 -58 R 74 -57 R 73 -57 R 74 -57 R 74 -57 R 74 -56 R 73 -57 R 74 -56 R +74 -56 R 74 -55 R 73 -56 R 74 -55 R 74 -55 R 74 -55 R 73 -55 R 74 -55 R +74 -54 R 74 -54 R 74 -54 R 73 -54 R 74 -53 R D 20 setlinewidth +0.000 0.000 0.000 setrgbcolor 2549 8668 M 34 42 R 74 97 R 73 101 R 74 104 R +74 104 R 74 105 R 74 104 R 73 105 R 74 105 R 74 104 R 74 103 R 73 103 R +74 103 R 74 102 R 74 101 R 73 99 R 74 99 R 74 97 R 74 95 R 73 94 R 74 94 R +74 91 R 74 91 R 73 89 R 74 88 R 74 87 R 74 84 R 73 83 R 74 81 R 74 80 R +74 77 R 73 75 R 74 72 R 74 70 R 74 68 R 73 67 R 74 67 R 74 66 R 74 66 R +73 66 R 74 66 R 74 67 R 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+1687 10821 M 11 -2 R 74 -20 R 73 -18 R 74 -17 R 74 -16 R 74 -12 R 73 -11 R +74 -9 R 74 -4 R 74 -1 R 73 2 R 74 5 R 74 9 R 74 13 R 73 17 R 74 22 R 74 25 R +74 28 R 74 31 R 73 33 R 74 37 R 74 38 R 74 41 R 73 42 R 74 45 R 74 47 R +74 49 R 73 50 R 74 51 R 74 52 R 74 52 R 73 54 R 74 54 R 74 56 R 74 55 R +73 57 R 74 57 R 74 57 R 74 57 R 73 57 R 74 57 R 74 57 R 74 56 R 73 56 R +74 54 R 74 54 R 74 52 R 73 53 R 74 54 R 74 53 R 74 54 R 73 54 R 74 55 R +74 56 R 74 57 R 74 59 R 73 59 R 74 61 R 74 63 R 74 64 R 73 65 R 74 67 R +74 69 R 74 70 R 73 71 R 74 71 R 74 72 R 74 73 R 73 71 R 74 72 R 74 71 R +74 72 R 73 70 R 74 67 R 74 65 R 74 63 R 73 59 R 74 57 R 74 53 R 74 50 R +73 46 R 74 43 R 74 39 R 74 36 R 73 32 R 74 28 R 74 24 R 74 21 R 73 17 R +74 13 R 74 10 R 74 7 R 73 3 R 74 0 R 74 -3 R 74 -6 R 74 -8 R 73 -11 R +74 -13 R 74 -15 R 74 -18 R 73 -20 R 74 -22 R 74 -23 R 74 -26 R 73 -28 R +74 -29 R 74 -31 R 74 -34 R 73 -35 R 74 -37 R 74 -39 R 74 -41 R 73 -43 R +74 -45 R 74 -47 R 74 -49 R 73 -52 R 74 -53 R 74 -56 R 74 -58 R 73 -60 R +74 -62 R 74 -65 R 74 -66 R 73 -69 R 74 -71 R 74 -73 R 74 -75 R 73 -77 R +74 -79 R 74 -81 R 74 -84 R 74 -85 R 73 -87 R 74 -90 R 74 -91 R 74 -94 R +73 -95 R 74 -98 R 74 -100 R 74 -102 R 73 -104 R 74 -106 R 74 -109 R +74 -111 R 73 -115 R 74 -117 R 74 -120 R 74 -125 R 73 -128 R 74 -133 R +74 -137 R 74 -141 R 73 -147 R 74 -151 R 74 -157 R 74 -162 R 73 -168 R +74 -174 R 74 -180 R 74 -187 R 73 -193 R 74 -199 R 74 -207 R 32 -94 R D L1 +2784 8668 M 20 51 R 74 184 R 74 178 R 74 174 R 73 168 R 74 162 R 74 157 R +74 151 R 73 146 R 74 142 R 74 137 R 74 132 R 73 127 R 74 123 R 74 119 R +74 114 R 73 111 R 74 107 R 74 103 R 74 100 R 73 97 R 74 93 R 74 90 R 74 87 R +73 84 R 74 81 R 74 78 R 74 76 R 73 73 R 74 70 R 74 67 R 74 66 R 73 64 R +74 63 R 74 61 R 74 61 R 73 60 R 74 60 R 74 59 R 74 60 R 74 60 R 73 61 R +74 61 R 74 62 R 74 63 R 73 64 R 74 64 R 74 67 R 74 66 R 73 68 R 74 68 R +74 69 R 74 68 R 73 68 R 74 68 R 74 69 R 74 69 R 73 68 R 74 65 R 74 63 R +74 61 R 73 57 R 74 55 R 74 52 R 74 48 R 73 45 R 74 41 R 74 38 R 74 34 R +73 31 R 74 27 R 74 24 R 74 19 R 73 17 R 74 12 R 74 9 R 74 6 R 73 3 R 74 -1 R +74 -3 R 74 -6 R 74 -9 R 73 -11 R 74 -14 R 74 -15 R 74 -18 R 73 -20 R +74 -22 R 74 -24 R 74 -26 R 73 -28 R 74 -29 R 74 -32 R 74 -33 R 73 -36 R +74 -37 R 74 -39 R 74 -41 R 73 -43 R 74 -45 R 74 -47 R 74 -49 R 73 -52 R +74 -53 R 74 -56 R 74 -58 R 73 -60 R 74 -63 R 74 -64 R 74 -67 R 73 -68 R +74 -71 R 74 -73 R 74 -75 R 73 -77 R 74 -79 R 74 -82 R 74 -83 R 74 -85 R +73 -88 R 74 -89 R 74 -92 R 74 -93 R 73 -96 R 74 -98 R 74 -99 R 74 -102 R +73 -104 R 74 -107 R 74 -109 R 74 -111 R 73 -114 R 74 -117 R 74 -121 R +74 -124 R 73 -129 R 74 -132 R 74 -137 R 74 -142 R 73 -146 R 74 -152 R +74 -157 R 74 -162 R 73 -168 R 74 -174 R 74 -180 R 74 -186 R 73 -193 R +74 -200 R 74 -207 R 35 -103 R D gsave 5836 10365 translate 0 0 M +0.9 dup scale +(Full Lifetimes Model) show grestore L2 6235 10024 M 1599 0 R D +gsave 8100 9918 translate 0 0 M 0.9 dup scale +(+ Standard Torus) show grestore L1 6235 9601 M 1599 0 R D +gsave 8100 9496 translate 0 0 M 0.9 dup scale +(+ Receding Torus) show grestore L0 6235 9179 M 1599 0 R D +gsave 8100 9073 translate 0 0 M 0.9 dup scale +(+ Full Obscuration Model) show grestore 15 setlinewidth 1687 1338 M +14102 0 R D 3616 1338 M 0 146 R D gsave 3616 836 translate 0 0 M +0.95 dup scale -117.687 0 N +(1) show grestore 7303 1338 M 0 146 R D gsave 7303 836 translate 0 0 M +0.95 dup scale -235.373 0 N +(10) show grestore 10991 1338 M 0 146 R D gsave 10991 836 translate 0 0 M +0.95 dup scale -353.06 0 N +(100) show grestore 14679 1338 M 0 146 R D gsave 14679 836 translate 0 0 M +0.95 dup scale -470.747 0 N +(1000) show grestore 1687 1338 M 0 73 R D 2148 1338 M 0 73 R D 2505 1338 M +0 73 R D 2797 1338 M 0 73 R D 3044 1338 M 0 73 R D 3258 1338 M 0 73 R D +3447 1338 M 0 73 R D 4726 1338 M 0 73 R D 5375 1338 M 0 73 R D 5836 1338 M +0 73 R D 6193 1338 M 0 73 R D 6485 1338 M 0 73 R D 6732 1338 M 0 73 R D +6946 1338 M 0 73 R D 7135 1338 M 0 73 R D 8414 1338 M 0 73 R D 9063 1338 M +0 73 R D 9524 1338 M 0 73 R D 9881 1338 M 0 73 R D 10173 1338 M 0 73 R D +10420 1338 M 0 73 R D 10634 1338 M 0 73 R D 10822 1338 M 0 73 R D +12101 1338 M 0 73 R D 12751 1338 M 0 73 R D 13212 1338 M 0 73 R D +13569 1338 M 0 73 R D 13861 1338 M 0 73 R D 14108 1338 M 0 73 R D +14322 1338 M 0 73 R D 14510 1338 M 0 73 R D 15789 1338 M 0 73 R D +gsave 8738 401 translate 0 0 M 0.95 dup scale -1235.07 0 N +(Energy \(keV\)) show grestore 1687 8669 M 14102 0 R D 3616 8669 M 0 -147 R +D 7303 8669 M 0 -147 R D 10991 8669 M 0 -147 R D 14679 8669 M 0 -147 R D +1687 8669 M 0 -73 R D 2148 8669 M 0 -73 R D 2505 8669 M 0 -73 R D +2797 8669 M 0 -73 R D 3044 8669 M 0 -73 R D 3258 8669 M 0 -73 R D +3447 8669 M 0 -73 R D 4726 8669 M 0 -73 R D 5375 8669 M 0 -73 R D +5836 8669 M 0 -73 R D 6193 8669 M 0 -73 R D 6485 8669 M 0 -73 R D +6732 8669 M 0 -73 R D 6946 8669 M 0 -73 R D 7135 8669 M 0 -73 R D +8414 8669 M 0 -73 R D 9063 8669 M 0 -73 R D 9524 8669 M 0 -73 R D +9881 8669 M 0 -73 R D 10173 8669 M 0 -73 R D 10420 8669 M 0 -73 R D +10634 8669 M 0 -73 R D 10822 8669 M 0 -73 R D 12101 8669 M 0 -73 R D +12751 8669 M 0 -73 R D 13212 8669 M 0 -73 R D 13569 8669 M 0 -73 R D +13861 8669 M 0 -73 R D 14108 8669 M 0 -73 R D 14322 8669 M 0 -73 R D +14510 8669 M 0 -73 R D 15789 8669 M 0 -73 R D 1687 1338 M 0 7331 R D +1687 3034 M 282 0 R D gsave 1582 2900 translate 0 0 M 0.95 dup scale +-470.747 0 N +(10) show grestore 1687 8669 M 282 0 R D gsave 1582 8435 translate 0 0 M +0.95 dup scale -706.12 0 N +(100) show grestore 1687 1338 M 141 0 R D 1687 1784 M 141 0 R D 1687 2161 M +141 0 R D 1687 2488 M 141 0 R D 1687 2776 M 141 0 R D 1687 4730 M 141 0 R D +1687 5723 M 141 0 R D 1687 6427 M 141 0 R D 1687 6973 M 141 0 R D +1687 7419 M 141 0 R D 1687 7796 M 141 0 R D 1687 8123 M 141 0 R D +1687 8411 M 141 0 R D 15789 1338 M 0 7331 R D 15789 3034 M -282 0 R D +15789 8669 M -282 0 R D 15789 1338 M -141 0 R D 15789 1784 M -141 0 R D +15789 2161 M -141 0 R D 15789 2488 M -141 0 R D 15789 2776 M -141 0 R D +15789 4730 M -141 0 R D 15789 5723 M -141 0 R D 15789 6427 M -141 0 R D +15789 6973 M -141 0 R D 15789 7419 M -141 0 R D 15789 7796 M -141 0 R D +15789 8123 M -141 0 R D 15789 8411 M -141 0 R D +0.980 1.000 0.000 setrgbcolor 2509 1474 M 74 67 R 74 68 R 73 67 R 74 68 R +74 68 R 74 67 R 74 68 R 73 68 R 74 67 R 74 68 R 74 67 R 73 68 R 74 68 R +74 67 R 74 68 R 73 68 R 74 67 R 74 68 R 74 67 R 73 68 R 74 68 R 74 67 R +74 68 R 73 67 R 74 68 R 74 68 R 74 67 R 73 68 R 74 68 R 74 67 R 74 68 R +73 67 R 74 68 R 74 68 R 74 67 R 73 68 R 74 68 R 74 67 R 74 68 R 73 67 R +74 68 R 74 68 R 74 67 R 74 68 R 73 67 R 74 68 R 74 68 R 74 67 R 73 68 R +74 68 R 74 67 R 74 68 R 73 67 R 74 68 R 74 68 R 74 67 R 73 68 R 74 68 R +74 67 R 74 68 R 73 67 R 74 68 R 74 68 R 74 67 R 73 68 R 0 992 R -73 -67 R +-74 -68 R -74 -68 R -74 -67 R -73 -68 R -74 -68 R -74 -67 R -74 -68 R +-73 -67 R -74 -68 R -74 -68 R -74 -67 R -73 -68 R -74 -68 R -74 -67 R +-74 -68 R -73 -67 R -74 -68 R -74 -68 R 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+%%DocumentNeededResources: font Helvetica +%%+ font Symbol +%%EOF diff --git a/feedback/papers/0506398/f3.ps b/feedback/papers/0506398/f3.ps new file mode 100644 index 0000000..d265951 --- /dev/null +++ b/feedback/papers/0506398/f3.ps @@ -0,0 +1,5577 @@ +%!PS-Adobe-3.0 +%%Creator: (ImageMagick) +%%Title: (f3.n.ps) +%%CreationDate: (Wed Oct 26 01:03:42 2005) +%%BoundingBox: 0 0 504 360 +%%DocumentData: Clean7Bit +%%LanguageLevel: 1 +%%Orientation: Portrait +%%PageOrder: Ascend +%%Pages: 1 +%%EndComments + +%%BeginDefaults +%%EndDefaults + +%%BeginProlog +% +% Display a color image. The image is displayed in color on +% Postscript viewers or printers that support color, otherwise +% it is displayed as grayscale. +% +/DirectClassPacket +{ + % + % Get a DirectClass packet. + % + % Parameters: + % red. + % green. + % blue. + % length: number of pixels minus one of this color (optional). + % + currentfile color_packet readhexstring pop pop + compression 0 eq + { + /number_pixels 3 def + } + { + currentfile byte readhexstring pop 0 get + /number_pixels exch 1 add 3 mul def + } ifelse + 0 3 number_pixels 1 sub + { + pixels exch color_packet putinterval + } for + pixels 0 number_pixels getinterval +} bind def + +/DirectClassImage +{ + % + % Display a DirectClass image. + % + systemdict /colorimage known + { + columns rows 8 + [ + columns 0 0 + rows neg 0 rows + ] + { DirectClassPacket } false 3 colorimage + } + { + % + % No colorimage operator; convert to grayscale. + % + columns rows 8 + [ + columns 0 0 + rows neg 0 rows + ] + { GrayDirectClassPacket } image + } ifelse +} bind def + +/GrayDirectClassPacket +{ + % + % Get a DirectClass packet; convert to grayscale. + % + % Parameters: + % red + % green + % blue + % length: number of pixels minus one of this color (optional). + % + currentfile color_packet readhexstring pop pop + color_packet 0 get 0.299 mul + color_packet 1 get 0.587 mul add + color_packet 2 get 0.114 mul add + cvi + /gray_packet exch def + compression 0 eq + { + /number_pixels 1 def + } + { + currentfile byte readhexstring pop 0 get + /number_pixels exch 1 add def + } ifelse + 0 1 number_pixels 1 sub + { + pixels exch gray_packet put + } for + pixels 0 number_pixels getinterval +} bind def + +/GrayPseudoClassPacket +{ + % + % Get a PseudoClass packet; convert to grayscale. + % + % Parameters: + % index: index into the colormap. + % length: number of pixels minus one of this color (optional). + % + currentfile byte readhexstring pop 0 get + /offset exch 3 mul def + /color_packet colormap offset 3 getinterval def + color_packet 0 get 0.299 mul + color_packet 1 get 0.587 mul add + color_packet 2 get 0.114 mul add + cvi + /gray_packet exch def + compression 0 eq + { + /number_pixels 1 def + } + { + currentfile byte readhexstring pop 0 get + /number_pixels exch 1 add def + } ifelse + 0 1 number_pixels 1 sub + { + pixels exch gray_packet put + } for + pixels 0 number_pixels getinterval +} bind def + +/PseudoClassPacket +{ + % + % Get a PseudoClass packet. + % + % Parameters: + % index: index into the colormap. + % length: number of pixels minus one of this color (optional). + % + currentfile byte readhexstring pop 0 get + /offset exch 3 mul def + /color_packet colormap offset 3 getinterval def + compression 0 eq + { + /number_pixels 3 def + } + { + currentfile byte readhexstring pop 0 get + /number_pixels exch 1 add 3 mul def + } ifelse + 0 3 number_pixels 1 sub + { + pixels exch color_packet putinterval + } for + pixels 0 number_pixels getinterval +} bind def + +/PseudoClassImage +{ + % + % Display a PseudoClass image. + % + % Parameters: + % class: 0-PseudoClass or 1-Grayscale. + % + currentfile buffer readline pop + token pop /class exch def pop + class 0 gt + { + currentfile buffer readline pop + token pop /depth exch def pop + /grays columns 8 add depth sub depth mul 8 idiv string def + columns rows depth + [ + columns 0 0 + rows neg 0 rows + ] + { currentfile grays readhexstring pop } image + } + { + % + % Parameters: + % colors: number of colors in the colormap. + % colormap: red, green, blue color packets. + % + currentfile buffer readline pop + token pop /colors exch def pop + /colors colors 3 mul def + /colormap colors string def + currentfile colormap readhexstring pop pop + systemdict /colorimage known + { + columns rows 8 + [ + columns 0 0 + rows neg 0 rows + ] + { PseudoClassPacket } false 3 colorimage + } + { + % + % No colorimage operator; convert to grayscale. + % + columns rows 8 + [ + columns 0 0 + rows neg 0 rows + ] + { GrayPseudoClassPacket } image + } ifelse + } ifelse +} bind def + +/DisplayImage +{ + % + % Display a DirectClass or PseudoClass image. + % + % Parameters: + % x & y translation. + % x & y scale. + % label pointsize. + % image label. + % image columns & rows. + % class: 0-DirectClass or 1-PseudoClass. + % compression: 0-none or 1-RunlengthEncoded. + % hex color packets. + % + gsave + /buffer 512 string def + /byte 1 string def + /color_packet 3 string def + /pixels 768 string def + + currentfile buffer readline pop + token pop /x exch def + token pop /y exch def pop + x y translate + currentfile buffer readline pop + token pop /x exch def + token pop /y exch def pop + currentfile buffer readline pop + token pop /pointsize exch def pop + /Times-Roman findfont pointsize scalefont setfont + x y scale + currentfile buffer readline pop + token pop /columns exch def + token pop /rows exch def pop + currentfile buffer readline pop + token pop /class exch def pop + currentfile buffer readline pop + token pop /compression exch def pop + class 0 gt 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gsave 13529 6172 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 15064 6706 M 0 105 R D gsave 15064 6172 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 16599 6706 M 0 105 R D gsave 16599 6172 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 10922 6706 M 0 52 R D 11192 6706 M 0 52 R D 11384 6706 M +0 52 R D 11532 6706 M 0 52 R D 11654 6706 M 0 52 R D 11757 6706 M 0 52 R D +11846 6706 M 0 52 R D 11924 6706 M 0 52 R D 12457 6706 M 0 52 R D +12727 6706 M 0 52 R D 12919 6706 M 0 52 R D 13067 6706 M 0 52 R D +13189 6706 M 0 52 R D 13292 6706 M 0 52 R D 13381 6706 M 0 52 R D +13459 6706 M 0 52 R D 13992 6706 M 0 52 R D 14262 6706 M 0 52 R D +14454 6706 M 0 52 R D 14602 6706 M 0 52 R D 14724 6706 M 0 52 R D +14827 6706 M 0 52 R D 14916 6706 M 0 52 R D 14994 6706 M 0 52 R D +15526 6706 M 0 52 R D 15797 6706 M 0 52 R D 15989 6706 M 0 52 R D +16137 6706 M 0 52 R D 16259 6706 M 0 52 R D 16362 6706 M 0 52 R D +16451 6706 M 0 52 R D 16529 6706 M 0 52 R D 17061 6706 M 0 52 R D +17332 6706 M 0 52 R D gsave 13896 5710 translate 0 0 M 1.01 dup scale +-58.8433 0 N +( ) show grestore 10460 11989 M 6872 0 R D 10460 11989 M 0 -106 R D +11995 11989 M 0 -106 R D 13529 11989 M 0 -106 R D 15064 11989 M 0 -106 R D +16599 11989 M 0 -106 R D 10922 11989 M 0 -53 R D 11192 11989 M 0 -53 R D +11384 11989 M 0 -53 R D 11532 11989 M 0 -53 R D 11654 11989 M 0 -53 R D +11757 11989 M 0 -53 R D 11846 11989 M 0 -53 R D 11924 11989 M 0 -53 R D +12457 11989 M 0 -53 R D 12727 11989 M 0 -53 R D 12919 11989 M 0 -53 R D +13067 11989 M 0 -53 R D 13189 11989 M 0 -53 R D 13292 11989 M 0 -53 R D +13381 11989 M 0 -53 R D 13459 11989 M 0 -53 R D 13992 11989 M 0 -53 R D +14262 11989 M 0 -53 R D 14454 11989 M 0 -53 R D 14602 11989 M 0 -53 R D +14724 11989 M 0 -53 R D 14827 11989 M 0 -53 R D 14916 11989 M 0 -53 R D +14994 11989 M 0 -53 R D 15526 11989 M 0 -53 R D 15797 11989 M 0 -53 R D +15989 11989 M 0 -53 R D 16137 11989 M 0 -53 R D 16259 11989 M 0 -53 R D +16362 11989 M 0 -53 R D 16451 11989 M 0 -53 R D 16529 11989 M 0 -53 R D +17061 11989 M 0 -53 R D 17332 11989 M 0 -53 R D 10460 6706 M 0 5283 R D +10460 8426 M 137 0 R D gsave 10348 8284 translate 0 0 M 1.01 dup scale +-706.12 0 N +(500) show grestore 10460 10147 M 137 0 R D +gsave 10348 10005 translate 0 0 M 1.01 dup scale -941.493 0 N +(1000) show grestore 10460 11868 M 137 0 R D +gsave 10348 11726 translate 0 0 M 1.01 dup scale -941.493 0 N +(2000) show grestore gsave 9061 9347 translate 0 0 M 90 rotate +1.01 dup scale -897.979 0 N +(t) show CP X 192.937 M +%%IncludeResource: font Symbol +262.467 /Symbol STDFONT +(*) show M X -95.92 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(Q ) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( \(Myr\)) show grestore 17332 6706 M 0 5283 R D 17332 8426 M -138 0 R D +17332 10147 M -138 0 R D 17332 11868 M -138 0 R D 10 setlinewidth +11033 10916 M -1 14 R -3 15 R -5 13 R -6 13 R -8 12 R -10 11 R -11 10 R +-12 8 R -13 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+262.467 /AvantGarde-Book STDFONT +(O) show M X -58.3193 M +%%IncludeResource: font AvantGarde-Book +186.267 /AvantGarde-Book STDFONT +( \267) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(\)) show grestore 10460 6706 M 6872 0 R D 10460 6706 M 0 -106 R D +11995 6706 M 0 -106 R D 13529 6706 M 0 -106 R D 15064 6706 M 0 -106 R D +16599 6706 M 0 -106 R D 10922 6706 M 0 -53 R D 11192 6706 M 0 -53 R D +11384 6706 M 0 -53 R D 11532 6706 M 0 -53 R D 11654 6706 M 0 -53 R D +11757 6706 M 0 -53 R D 11846 6706 M 0 -53 R D 11924 6706 M 0 -53 R D +12457 6706 M 0 -53 R D 12727 6706 M 0 -53 R D 12919 6706 M 0 -53 R D +13067 6706 M 0 -53 R D 13189 6706 M 0 -53 R D 13292 6706 M 0 -53 R D +13381 6706 M 0 -53 R D 13459 6706 M 0 -53 R D 13992 6706 M 0 -53 R D +14262 6706 M 0 -53 R D 14454 6706 M 0 -53 R D 14602 6706 M 0 -53 R D +14724 6706 M 0 -53 R D 14827 6706 M 0 -53 R D 14916 6706 M 0 -53 R D +14994 6706 M 0 -53 R D 15526 6706 M 0 -53 R D 15797 6706 M 0 -53 R D +15989 6706 M 0 -53 R D 16137 6706 M 0 -53 R D 16259 6706 M 0 -53 R D +16362 6706 M 0 -53 R D 16451 6706 M 0 -53 R D 16529 6706 M 0 -53 R D +17061 6706 M 0 -53 R D 17332 6706 M 0 -53 R D 10460 1422 M 0 5284 R D +10460 1422 M 137 0 R D gsave 10348 1422 translate 0 0 M 1.01 dup scale +-616.678 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(9) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 10460 2479 M 137 0 R D +gsave 10348 2337 translate 0 0 M 1.01 dup scale -762.61 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(10) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 10460 3536 M 137 0 R D +gsave 10348 3393 translate 0 0 M 1.01 dup scale -762.61 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(11) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 10460 4592 M 137 0 R D +gsave 10348 4450 translate 0 0 M 1.01 dup scale -762.61 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(12) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 10460 5649 M 137 0 R D +gsave 10348 5507 translate 0 0 M 1.01 dup scale -762.61 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(13) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 10460 6706 M 137 0 R D +gsave 10348 6457 translate 0 0 M 1.01 dup scale -762.61 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(14) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 10460 1740 M 68 0 R D 10460 1926 M 68 0 R D +10460 2058 M 68 0 R D 10460 2161 M 68 0 R D 10460 2244 M 68 0 R D +10460 2315 M 68 0 R D 10460 2376 M 68 0 R D 10460 2430 M 68 0 R D +10460 2797 M 68 0 R D 10460 2983 M 68 0 R D 10460 3115 M 68 0 R D +10460 3217 M 68 0 R D 10460 3301 M 68 0 R D 10460 3372 M 68 0 R D +10460 3433 M 68 0 R D 10460 3487 M 68 0 R D 10460 3854 M 68 0 R D +10460 4040 M 68 0 R D 10460 4172 M 68 0 R D 10460 4274 M 68 0 R D +10460 4358 M 68 0 R D 10460 4429 M 68 0 R D 10460 4490 M 68 0 R D +10460 4544 M 68 0 R D 10460 4910 M 68 0 R D 10460 5096 M 68 0 R D +10460 5228 M 68 0 R D 10460 5331 M 68 0 R D 10460 5414 M 68 0 R D +10460 5485 M 68 0 R D 10460 5546 M 68 0 R D 10460 5601 M 68 0 R D +10460 5967 M 68 0 R D 10460 6153 M 68 0 R D 10460 6285 M 68 0 R D +10460 6387 M 68 0 R D 10460 6471 M 68 0 R D 10460 6542 M 68 0 R D +10460 6603 M 68 0 R D 10460 6657 M 68 0 R D gsave 9241 4064 translate 0 0 M +90 rotate 1.01 dup scale -742.302 0 N +(L) show CP X 192.937 M +%%IncludeResource: font Symbol +262.467 /Symbol STDFONT +(*) show M X -95.92 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(Q ) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( \(L) show CP X -101.051 M +%%IncludeResource: font AvantGarde-Book +262.467 /AvantGarde-Book STDFONT +(O) show M X -58.3193 M +%%IncludeResource: font AvantGarde-Book +186.267 /AvantGarde-Book STDFONT +( \267) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(\)) show grestore 17332 1422 M 0 5284 R D 17332 1422 M -138 0 R D +17332 2479 M -138 0 R D 17332 3536 M -138 0 R D 17332 4592 M -138 0 R D +17332 5649 M -138 0 R D 17332 6706 M -138 0 R D 17332 1740 M -69 0 R D +17332 1926 M -69 0 R D 17332 2058 M -69 0 R D 17332 2161 M -69 0 R D +17332 2244 M -69 0 R D 17332 2315 M -69 0 R D 17332 2376 M -69 0 R D +17332 2430 M -69 0 R D 17332 2797 M -69 0 R D 17332 2983 M -69 0 R D +17332 3115 M -69 0 R D 17332 3217 M -69 0 R D 17332 3301 M -69 0 R D +17332 3372 M -69 0 R D 17332 3433 M -69 0 R D 17332 3487 M -69 0 R D +17332 3854 M -69 0 R D 17332 4040 M -69 0 R D 17332 4172 M -69 0 R D +17332 4274 M -69 0 R D 17332 4358 M -69 0 R D 17332 4429 M -69 0 R D +17332 4490 M -69 0 R D 17332 4544 M -69 0 R D 17332 4910 M -69 0 R D +17332 5096 M -69 0 R D 17332 5228 M -69 0 R D 17332 5331 M -69 0 R D +17332 5414 M -69 0 R D 17332 5485 M -69 0 R D 17332 5546 M -69 0 R D +17332 5601 M -69 0 R D 17332 5967 M -69 0 R D 17332 6153 M -69 0 R D +17332 6285 M -69 0 R D 17332 6387 M -69 0 R D 17332 6471 M -69 0 R D +17332 6542 M -69 0 R D 17332 6603 M -69 0 R D 17332 6657 M -69 0 R D +10 setlinewidth 11033 2041 M -1 15 R -3 14 R -5 14 R -6 13 R -8 12 R +-10 11 R -11 9 R -12 8 R -13 7 R -14 4 R -14 3 R -14 1 R -15 -1 R -14 -3 R +-14 -4 R -13 -7 R -12 -8 R -11 -9 R -9 -11 R -8 -12 R -7 -13 R -5 -14 R +-2 -14 R -1 -15 R 1 -14 R 2 -15 R 5 -13 R 7 -13 R 8 -12 R 9 -11 R 11 -10 R +12 -8 R 13 -6 R 14 -5 R 14 -3 R 15 -1 R 14 1 R 14 3 R 14 5 R 13 6 R 12 8 R +11 10 R 10 11 R 8 12 R 6 13 R 5 13 R 3 15 R 1 14 R D 11367 2198 M -1 15 R +-3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 9 R -12 8 R -13 7 R -14 4 R +-14 3 R -14 1 R -15 -1 R -14 -3 R -14 -4 R -13 -7 R -12 -8 R -11 -9 R +-10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R 0 -15 R 0 -14 R 3 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12368 2938 M -1 14 R -3 14 R -4 14 R -7 13 R -8 12 R +-10 11 R -10 10 R -13 8 R -13 6 R -13 5 R -15 3 R -14 1 R -15 -1 R -14 -3 R +-14 -5 R -13 -6 R -12 -8 R -11 -10 R -9 -11 R -8 -12 R -7 -13 R -4 -14 R +-3 -14 R -1 -14 R 1 -15 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -10 R +12 -8 R 13 -6 R 14 -5 R 14 -2 R 15 -1 R 14 1 R 15 2 R 13 5 R 13 6 R 13 8 R +10 10 R 10 11 R 8 12 R 7 13 R 4 14 R 3 14 R 1 15 R D 12702 3194 M -1 14 R +-3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -13 5 R +-15 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R +-9 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -14 R 1 -15 R 3 -14 R +4 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -9 R 12 -9 R 13 -6 R 14 -5 R 14 -2 R +15 -1 R 14 1 R 15 2 R 13 5 R 13 6 R 12 9 R 11 9 R 10 11 R 8 12 R 6 13 R +5 14 R 3 14 R 1 15 R D 13036 3360 M -1 15 R -3 14 R -5 14 R -6 13 R -8 12 R +-10 11 R -11 9 R -12 8 R -13 7 R -14 4 R -14 3 R -14 1 R -15 -1 R -14 -3 R +-14 -4 R -13 -7 R -12 -8 R -11 -9 R -9 -11 R -9 -12 R -6 -13 R -5 -14 R +-2 -14 R -1 -15 R 1 -14 R 2 -15 R 5 -13 R 6 -13 R 9 -12 R 9 -11 R 11 -10 R +12 -8 R 13 -6 R 14 -5 R 14 -3 R 15 -1 R 14 1 R 14 3 R 14 5 R 13 6 R 12 8 R +11 10 R 10 11 R 8 12 R 6 13 R 5 13 R 3 15 R 1 14 R D 13369 3704 M -1 15 R +-2 14 R -5 14 R -6 13 R -9 12 R -9 11 R -11 10 R -12 8 R -13 6 R -14 5 R +-14 3 R -15 0 R -14 0 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R +-10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -14 R +5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R +14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 9 11 R 9 12 R 6 13 R +5 14 R 2 14 R 1 14 R D 13703 3894 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R +-9 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -15 0 R -14 0 R -14 -3 R +-14 -5 R -13 -6 R -12 -8 R -11 -10 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R +-3 -14 R -1 -15 R 1 -14 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -10 R +12 -8 R 13 -6 R 14 -5 R 14 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R 12 8 R +11 10 R 9 11 R 8 12 R 7 13 R 4 14 R 3 14 R 1 14 R D 14037 4130 M -1 14 R +-3 14 R -4 14 R -7 13 R -8 12 R -9 11 R -11 10 R -12 8 R -13 6 R -14 5 R +-14 3 R -15 1 R -14 -1 R -15 -3 R -13 -5 R -13 -6 R -13 -8 R -10 -10 R +-10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -14 R 1 -15 R 3 -14 R +5 -14 R 6 -13 R 8 -12 R 10 -11 R 10 -9 R 13 -9 R 13 -6 R 13 -5 R 15 -2 R +14 -1 R 15 1 R 14 2 R 14 5 R 13 6 R 12 9 R 11 9 R 9 11 R 8 12 R 7 13 R +4 14 R 3 14 R 1 15 R D 14371 4424 M -1 15 R -3 14 R -5 14 R -6 13 R -8 12 R +-10 11 R -11 9 R -12 8 R -13 7 R -13 5 R -15 2 R -14 1 R -15 -1 R -14 -2 R +-14 -5 R -13 -7 R -12 -8 R -11 -9 R -9 -11 R -8 -12 R -7 -13 R -4 -14 R +-3 -14 R -1 -15 R 1 -14 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -10 R +12 -8 R 13 -6 R 14 -5 R 14 -3 R 15 -1 R 14 1 R 15 3 R 13 5 R 13 6 R 12 8 R +11 10 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 14 R D 14705 4674 M -1 15 R +-3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -14 5 R +-14 3 R -14 0 R -15 0 R -14 -3 R -14 -5 R 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15 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 9 11 R 8 12 R 7 13 R +5 13 R 2 15 R 1 14 R D 15706 5386 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R +-9 11 R -11 9 R -12 8 R -13 7 R -14 4 R -14 3 R -15 1 R -14 -1 R -15 -3 R +-13 -4 R -13 -7 R -12 -8 R -11 -9 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R +-3 -14 R -1 -15 R 1 -14 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -10 R +12 -8 R 13 -6 R 13 -5 R 15 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R 12 8 R +11 10 R 9 11 R 8 12 R 7 13 R 4 14 R 3 14 R 1 14 R D 16040 5540 M -1 15 R +-3 14 R -4 14 R -7 13 R -8 12 R -10 11 R -10 9 R -13 8 R -13 7 R -13 4 R +-15 3 R -14 1 R -14 -1 R -15 -3 R -13 -4 R -14 -7 R -12 -8 R -10 -9 R +-10 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -15 R +4 -13 R 7 -13 R 8 -12 R 10 -11 R 10 -10 R 12 -8 R 14 -6 R 13 -5 R 15 -3 R +14 -1 R 14 1 R 15 3 R 13 5 R 13 6 R 13 8 R 10 10 R 10 11 R 8 12 R 7 13 R +4 13 R 3 15 R 1 14 R D 16374 5860 M -1 14 R -3 14 R -5 14 R -6 13 R -8 12 R +-10 11 R -11 10 R -12 8 R -13 6 R -13 5 R -15 3 R -14 1 R -15 -1 R -14 -3 R +-14 -5 R -13 -6 R -12 -8 R -11 -10 R -9 -11 R -8 -12 R -7 -13 R -4 -14 R +-3 -14 R -1 -14 R 1 -15 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -9 R +12 -8 R 13 -7 R 14 -5 R 14 -2 R 15 -1 R 14 1 R 15 2 R 13 5 R 13 7 R 12 8 R +11 9 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 15 R D 16708 5990 M -1 15 R +-3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 9 R -12 8 R -13 7 R -14 4 R +-14 3 R -14 1 R -15 -1 R -14 -3 R -14 -4 R -13 -7 R -12 -8 R -11 -9 R +-9 -11 R -8 -12 R -7 -13 R -5 -14 R -2 -14 R -1 -15 R 1 -14 R 2 -15 R +5 -13 R 7 -13 R 8 -12 R 9 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R +15 -1 R 14 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 10 11 R 8 12 R 6 13 R +5 13 R 3 15 R 1 14 R D 17041 6457 M 0 14 R -3 14 R -5 14 R -6 13 R -8 12 R +-10 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -15 1 R -14 -1 R -14 -3 R +-14 -5 R -13 -6 R -12 -8 R -11 -10 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R +-3 -14 R -1 -14 R 1 -15 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -9 R +12 -8 R 13 -7 R 14 -5 R 14 -2 R 14 -1 R 15 1 R 14 2 R 14 5 R 13 7 R 12 8 R +11 9 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 0 15 R D 17331 6545 M -11 8 R +-13 6 R -14 5 R -14 3 R -15 1 R -14 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R +-11 -10 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -14 R 1 -15 R +3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -9 R 12 -8 R 13 -7 R 14 -5 R +14 -2 R 14 -1 R 15 1 R 14 2 R 14 5 R 13 7 R 11 7 R D 20 setlinewidth +10887 1866 M 69 0 R -34 0 R 0 302 R -35 0 R 69 0 R D 11221 2037 M 69 0 R +-34 0 R 0 280 R -35 0 R 69 0 R D 11555 2216 M 69 0 R -35 0 R 0 363 R -34 0 R +69 0 R D 11889 2569 M 69 0 R -35 0 R 0 315 R -34 0 R 69 0 R D 12223 2766 M +68 0 R -34 0 R 0 296 R -34 0 R 68 0 R D 12556 3035 M 69 0 R -34 0 R 0 276 R +-35 0 R 69 0 R D 12890 3214 M 69 0 R -34 0 R 0 257 R -35 0 R 69 0 R D +13224 3512 M 69 0 R -35 0 R 0 328 R -34 0 R 69 0 R D 13558 3735 M 69 0 R +-35 0 R 0 277 R -34 0 R 69 0 R D 13892 3977 M 68 0 R -34 0 R 0 267 R -34 0 R +68 0 R D 14226 4194 M 68 0 R -34 0 R 0 383 R -34 0 R 68 0 R D 14559 4521 M +69 0 R -34 0 R 0 268 R -35 0 R 69 0 R D 14893 4736 M 69 0 R -34 0 R 0 248 R +-35 0 R 69 0 R D 15227 4951 M 69 0 R -35 0 R 0 227 R -34 0 R 69 0 R D +15561 5184 M 69 0 R -35 0 R 0 342 R -34 0 R 69 0 R D 15895 5311 M 68 0 R +-34 0 R 0 382 R -34 0 R 68 0 R D 16228 5389 M 69 0 R -34 0 R 0 698 R -35 0 R +69 0 R D 16562 4242 M 69 0 R -34 0 R 0 2061 R -35 0 R 69 0 R D 16896 5581 M +69 0 R -35 0 R 0 1124 R D 17230 5581 M 69 0 R -35 0 R 0 1124 R D +1.000 0.000 0.000 setrgbcolor 10459 1737 M 1 1 R 153 106 R 154 105 R +153 106 R 154 106 R 153 105 R 154 106 R 153 106 R 154 105 R 153 106 R +154 106 R 153 105 R 154 106 R 153 106 R 154 105 R 153 106 R 154 106 R +153 105 R 153 106 R 154 106 R 153 105 R 154 106 R 153 106 R 154 105 R +153 106 R 154 106 R 153 105 R 154 106 R 153 106 R 154 105 R 153 106 R +154 106 R 153 105 R 154 106 R 153 106 R 154 105 R 153 106 R 154 106 R +153 105 R 154 106 R 153 106 R 154 105 R 153 106 R 154 106 R 153 105 R +118 81 R D +%%PageTrailer +end +restore +showpage +%%PageResources: font Helvetica +%%+ font Symbol +%%+ font AvantGarde-Book +%%Trailer +restore +%%Pages: 1 +%%DocumentNeededResources: font Helvetica +%%+ font Symbol +%%+ font AvantGarde-Book +%%EOF diff --git a/feedback/papers/0506398/f6.ps b/feedback/papers/0506398/f6.ps new file mode 100644 index 0000000..bb3a3f1 --- /dev/null +++ b/feedback/papers/0506398/f6.ps @@ -0,0 +1,1160 @@ +%!PS-Adobe-3.0 +%%BoundingBox: 54 360 558 720 +%%Title: Graphics produced by IDL +%%For: phopkins@zeus, /home/phopkins/lars_project/utils +%%Creator: IDL Version 6.1.1 (linux x86 m32) +%%CreationDate: Wed Jun 1 23:53:19 2005 +%%DocumentData: Clean7bit +%%Requirements: color +%%LanguageLevel: 1 +%%PageOrder: Ascend +%%Pages: (atend) +%%DocumentNeededResources: (atend) +%%EndComments +%%BeginProlog +save +%+ prolog.ps -- Prolog for IDL generated PostScript files +%+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. +%v 5 +/$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C +{currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint +stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} +bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show +grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 +setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 +{[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 +100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 +{[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef +/ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} +ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont +exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica +findfont exch scalefont setfont (\267) show currentpoint grestore moveto} +bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end +%%EndProlog +%%Page: 0 1 +%%PageRequirements: color +%%PageResources: (atend) +%%PageOrientation: Portrait +%%PageBoundingBox: 54 360 558 720 +%%BeginPageSetup +save +$IDL_DICT begin 54 360 translate 0.0283465 dup scale MITERLIMIT +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +%%EndPageSetup +15 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 2242 8467 M 7433 0 R D +2242 8467 M 0 70 R D gsave 2242 7933 translate 0 0 M 1.01 dup scale +-58.8433 0 N +( ) show grestore 3758 8467 M 0 70 R D gsave 3758 7933 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 5274 8467 M 0 70 R D gsave 5274 7933 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 6790 8467 M 0 70 R D gsave 6790 7933 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 8306 8467 M 0 70 R D gsave 8306 7933 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 2699 8467 M 0 35 R D 2966 8467 M 0 35 R D 3155 8467 M +0 35 R D 3302 8467 M 0 35 R D 3422 8467 M 0 35 R D 3523 8467 M 0 35 R D +3611 8467 M 0 35 R D 3689 8467 M 0 35 R D 4215 8467 M 0 35 R D 4481 8467 M +0 35 R D 4671 8467 M 0 35 R D 4818 8467 M 0 35 R D 4938 8467 M 0 35 R D +5039 8467 M 0 35 R D 5127 8467 M 0 35 R D 5205 8467 M 0 35 R D 5730 8467 M +0 35 R D 5997 8467 M 0 35 R D 6187 8467 M 0 35 R D 6334 8467 M 0 35 R D +6454 8467 M 0 35 R D 6555 8467 M 0 35 R D 6643 8467 M 0 35 R D 6721 8467 M +0 35 R D 7246 8467 M 0 35 R D 7513 8467 M 0 35 R D 7703 8467 M 0 35 R D +7850 8467 M 0 35 R D 7970 8467 M 0 35 R D 8071 8467 M 0 35 R D 8159 8467 M +0 35 R D 8237 8467 M 0 35 R D 8762 8467 M 0 35 R D 9029 8467 M 0 35 R D +9219 8467 M 0 35 R D 9365 8467 M 0 35 R D 9485 8467 M 0 35 R D 9587 8467 M +0 35 R D 9675 8467 M 0 35 R D 2242 11989 M 7433 0 R D 2242 11989 M 0 -70 R D +3758 11989 M 0 -70 R D 5274 11989 M 0 -70 R D 6790 11989 M 0 -70 R D +8306 11989 M 0 -70 R D 2699 11989 M 0 -35 R D 2966 11989 M 0 -35 R D +3155 11989 M 0 -35 R D 3302 11989 M 0 -35 R D 3422 11989 M 0 -35 R D +3523 11989 M 0 -35 R D 3611 11989 M 0 -35 R D 3689 11989 M 0 -35 R D +4215 11989 M 0 -35 R D 4481 11989 M 0 -35 R D 4671 11989 M 0 -35 R D +4818 11989 M 0 -35 R D 4938 11989 M 0 -35 R D 5039 11989 M 0 -35 R D +5127 11989 M 0 -35 R D 5205 11989 M 0 -35 R D 5730 11989 M 0 -35 R D +5997 11989 M 0 -35 R D 6187 11989 M 0 -35 R D 6334 11989 M 0 -35 R D +6454 11989 M 0 -35 R D 6555 11989 M 0 -35 R D 6643 11989 M 0 -35 R D +6721 11989 M 0 -35 R D 7246 11989 M 0 -35 R D 7513 11989 M 0 -35 R D +7703 11989 M 0 -35 R D 7850 11989 M 0 -35 R D 7970 11989 M 0 -35 R D +8071 11989 M 0 -35 R D 8159 11989 M 0 -35 R D 8237 11989 M 0 -35 R D +8762 11989 M 0 -35 R D 9029 11989 M 0 -35 R D 9219 11989 M 0 -35 R D +9365 11989 M 0 -35 R D 9485 11989 M 0 -35 R D 9587 11989 M 0 -35 R D +9675 11989 M 0 -35 R D 2242 8467 M 0 3522 R D 2242 8665 M 149 0 R D +gsave 2130 8522 translate 0 0 M 1.01 dup scale -470.747 0 N +(10) show grestore 2242 9942 M 149 0 R D gsave 2130 9800 translate 0 0 M +1.01 dup scale -706.12 0 N +(100) show grestore 2242 11220 M 149 0 R D gsave 2130 11078 translate 0 0 M +1.01 dup scale -941.493 0 N +(1000) show grestore 2242 8467 M 75 0 R D 2242 8541 M 75 0 R D 2242 8606 M +75 0 R D 2242 9049 M 75 0 R D 2242 9274 M 75 0 R D 2242 9434 M 75 0 R D +2242 9558 M 75 0 R D 2242 9659 M 75 0 R D 2242 9744 M 75 0 R D 2242 9818 M +75 0 R D 2242 9884 M 75 0 R D 2242 10327 M 75 0 R D 2242 10552 M 75 0 R D +2242 10711 M 75 0 R D 2242 10835 M 75 0 R D 2242 10936 M 75 0 R D +2242 11022 M 75 0 R D 2242 11096 M 75 0 R D 2242 11161 M 75 0 R D +2242 11604 M 75 0 R D 2242 11829 M 75 0 R D 2242 11989 M 75 0 R D +9675 8467 M 0 3522 R D 9675 8665 M -149 0 R D 9675 9942 M -149 0 R D +9675 11220 M -149 0 R D 9675 8467 M -74 0 R D 9675 8541 M -74 0 R D +9675 8606 M -74 0 R D 9675 9049 M -74 0 R D 9675 9274 M -74 0 R D +9675 9434 M -74 0 R D 9675 9558 M -74 0 R D 9675 9659 M -74 0 R D +9675 9744 M -74 0 R D 9675 9818 M -74 0 R D 9675 9884 M -74 0 R D +9675 10327 M -74 0 R D 9675 10552 M -74 0 R D 9675 10711 M -74 0 R D +9675 10835 M -74 0 R D 9675 10936 M -74 0 R D 9675 11022 M -74 0 R D +9675 11096 M -74 0 R D 9675 11161 M -74 0 R D 9675 11604 M -74 0 R D +9675 11829 M -74 0 R D 9675 11989 M -74 0 R D 20 setlinewidth 2242 11371 M +111 0 R -111 0 R 0 111 R 0 -222 R D 2242 11371 M Z 2283 11371 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 2242 11371 M 152 0 R D 2434 11371 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 2394 11371 M 151 0 R D 2586 11361 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 2545 11371 M 152 -10 R D 2738 11268 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 2697 11361 M 152 -93 R D 2889 11239 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 2849 11268 M 151 -29 R D 3041 11178 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 3000 11239 M 152 -61 R D 3192 11178 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 3152 11178 M 151 0 R D 3344 11173 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 3303 11178 M 152 -5 R D 3496 11160 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 3455 11173 M 152 -13 R D 3647 11116 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 3607 11160 M 151 -44 R D 3799 11108 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 3758 11116 M 152 -8 R D 3950 11091 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 3910 11108 M 151 -17 R D 4102 11080 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 4061 11091 M 152 -11 R D 4254 11075 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 4213 11080 M 152 -5 R D 4405 11070 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 4365 11075 M 151 -5 R D 4557 11067 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 4516 11070 M 152 -3 R D 4708 11064 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 4668 11067 M 151 -3 R D 4860 11059 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 4819 11064 M 152 -5 R D 5011 10997 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 4971 11059 M 151 -62 R D 5163 10909 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 5122 10997 M 152 -88 R D 5315 10783 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 5274 10909 M 152 -126 R D 5466 10633 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 5426 10783 M 151 -150 R D 5618 10561 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 5577 10633 M 152 -72 R D 5769 10481 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 5729 10561 M 151 -80 R D 5921 10370 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 5880 10481 M 152 -111 R D 6073 10266 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 6032 10370 M 152 -104 R D 6224 10176 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 6184 10266 M 151 -90 R D 6376 9954 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 6335 10176 M 152 -222 R D 6527 9753 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 6487 9954 M 151 -201 R D 6679 9444 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 6638 9753 M 152 -309 R D 6831 8884 M 222 0 R +-111 0 R 0 111 R 0 -222 R D 6790 9444 M 152 -560 R D 7093 8466 M 0 27 R +0 -27 R D 6942 8884 M 125 -418 R D 1.000 0.000 0.000 setrgbcolor +2242 11720 M 111 -111 R -111 -111 R D 2242 11720 M Z 2242 11609 M Z +2394 11697 M 111 -111 R -111 -111 R -111 111 R 111 111 R D 2242 11609 M +152 -23 R D 2545 11673 M 111 -111 R -111 -111 R -111 111 R 111 111 R D +2394 11586 M 151 -24 R D 2697 11649 M 111 -111 R -111 -111 R -111 111 R +111 111 R D 2545 11562 M 152 -24 R D 2849 11623 M 111 -111 R -111 -111 R +-111 111 R 111 111 R D 2697 11538 M 152 -26 R D 3000 11596 M 111 -111 R +-111 -111 R -111 111 R 111 111 R D 2849 11512 M 151 -27 R D 3152 11567 M +111 -111 R -111 -111 R -111 111 R 111 111 R D 3000 11485 M 152 -29 R D +3303 11537 M 111 -111 R -111 -111 R -111 111 R 111 111 R D 3152 11456 M +151 -30 R D 3455 11505 M 111 -111 R -111 -111 R -111 111 R 111 111 R D +3303 11426 M 152 -32 R D 3607 11472 M 111 -111 R -111 -111 R -111 111 R +111 111 R D 3455 11394 M 152 -33 R D 3758 11436 M 111 -111 R -111 -111 R +-111 111 R 111 111 R D 3607 11361 M 151 -36 R D 3910 11399 M 111 -111 R +-111 -111 R -111 111 R 111 111 R D 3758 11325 M 152 -37 R D 4061 11358 M +111 -111 R -111 -111 R -111 111 R 111 111 R D 3910 11288 M 151 -41 R D +4213 11315 M 111 -111 R -111 -111 R -111 111 R 111 111 R D 4061 11247 M +152 -43 R D 4365 11269 M 111 -111 R -111 -111 R -111 111 R 111 111 R D +4213 11204 M 152 -46 R D 4516 11219 M 111 -111 R -111 -111 R -111 111 R +111 111 R D 4365 11158 M 151 -50 R D 4668 11165 M 111 -111 R -111 -111 R +-111 111 R 111 111 R D 4516 11108 M 152 -54 R D 4819 11106 M 111 -111 R +-111 -111 R -111 111 R 111 111 R D 4668 11054 M 151 -59 R D 4971 11041 M +111 -111 R -111 -111 R -111 111 R 111 111 R D 4819 10995 M 152 -65 R D +5122 10970 M 111 -111 R -111 -111 R -111 111 R 111 111 R D 4971 10930 M +151 -71 R D 5274 10892 M 111 -111 R -111 -111 R -111 111 R 111 111 R D +5122 10859 M 152 -78 R D 5426 10805 M 111 -111 R -111 -111 R -111 111 R +111 111 R D 5274 10781 M 152 -87 R D 5577 10707 M 111 -111 R -111 -111 R +-111 111 R 111 111 R D 5426 10694 M 151 -98 R D 5729 10597 M 111 -111 R +-111 -111 R -111 111 R 111 111 R D 5577 10596 M 152 -110 R D 5880 10472 M +111 -111 R -111 -111 R -111 111 R 111 111 R D 5729 10486 M 151 -125 R D +6032 10330 M 111 -111 R -111 -111 R -111 111 R 111 111 R D 5880 10361 M +152 -142 R D 6184 10166 M 111 -111 R -111 -111 R -111 111 R 111 111 R D +6032 10219 M 152 -164 R D 6335 9976 M 111 -111 R -111 -111 R -111 111 R +111 111 R D 6184 10055 M 151 -190 R D 6487 9755 M 111 -111 R -111 -111 R +-111 111 R 111 111 R D 6335 9865 M 152 -221 R D 6638 9494 M 111 -111 R +-111 -111 R -111 111 R 111 111 R D 6487 9644 M 151 -261 R D 6790 9186 M +111 -111 R -111 -111 R -111 111 R 111 111 R D 6638 9383 M 152 -308 R D +6942 8818 M 111 -111 R -111 -111 R -111 111 R 111 111 R D 6790 9075 M +152 -368 R 82 -241 R D 0.000 0.000 0.000 setrgbcolor +gsave 5997 12113 translate 0 0 M 1.01 dup scale -976.418 0 N +(No Bulges) show grestore gsave 6334 11321 translate 0 0 M 1.01 dup scale +(M) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(BH) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(\(t) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(0) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(\) = 10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(5) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( M) show CP X -101.051 M +%%IncludeResource: font AvantGarde-Book +262.467 /AvantGarde-Book STDFONT +(O) show M X -58.3193 M +%%IncludeResource: font AvantGarde-Book +186.267 /AvantGarde-Book STDFONT +( \267) show +%%IncludeResource: font Helvetica +186.267 /Helvetica STDFONT grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 15 setlinewidth 9675 8467 M 7432 0 R D +9675 8467 M 0 70 R D gsave 9675 7933 translate 0 0 M 1.01 dup scale +-58.8433 0 N +( ) show grestore 11191 8467 M 0 70 R D gsave 11191 7933 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 12707 8467 M 0 70 R D gsave 12707 7933 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 14223 8467 M 0 70 R D gsave 14223 7933 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 15738 8467 M 0 70 R D gsave 15738 7933 translate 0 0 M +1.01 dup scale -58.8433 0 N +( ) show grestore 10131 8467 M 0 35 R D 10398 8467 M 0 35 R D 10588 8467 M +0 35 R D 10734 8467 M 0 35 R D 10854 8467 M 0 35 R D 10956 8467 M 0 35 R D +11044 8467 M 0 35 R D 11121 8467 M 0 35 R D 11647 8467 M 0 35 R D +11914 8467 M 0 35 R D 12103 8467 M 0 35 R D 12250 8467 M 0 35 R D +12370 8467 M 0 35 R D 12472 8467 M 0 35 R D 12560 8467 M 0 35 R D +12637 8467 M 0 35 R D 13163 8467 M 0 35 R D 13430 8467 M 0 35 R D +13619 8467 M 0 35 R D 13766 8467 M 0 35 R D 13886 8467 M 0 35 R D +13988 8467 M 0 35 R D 14076 8467 M 0 35 R D 14153 8467 M 0 35 R D +14679 8467 M 0 35 R D 14946 8467 M 0 35 R D 15135 8467 M 0 35 R D +15282 8467 M 0 35 R D 15402 8467 M 0 35 R D 15504 8467 M 0 35 R D +15592 8467 M 0 35 R D 15669 8467 M 0 35 R D 16195 8467 M 0 35 R D +16462 8467 M 0 35 R D 16651 8467 M 0 35 R D 16798 8467 M 0 35 R D +16918 8467 M 0 35 R D 17020 8467 M 0 35 R D 17107 8467 M 0 35 R D +9675 11989 M 7432 0 R D 9675 11989 M 0 -70 R D 11191 11989 M 0 -70 R D +12707 11989 M 0 -70 R D 14223 11989 M 0 -70 R D 15738 11989 M 0 -70 R D +10131 11989 M 0 -35 R D 10398 11989 M 0 -35 R D 10588 11989 M 0 -35 R D +10734 11989 M 0 -35 R D 10854 11989 M 0 -35 R D 10956 11989 M 0 -35 R D +11044 11989 M 0 -35 R D 11121 11989 M 0 -35 R D 11647 11989 M 0 -35 R D +11914 11989 M 0 -35 R D 12103 11989 M 0 -35 R D 12250 11989 M 0 -35 R D +12370 11989 M 0 -35 R D 12472 11989 M 0 -35 R D 12560 11989 M 0 -35 R D +12637 11989 M 0 -35 R D 13163 11989 M 0 -35 R D 13430 11989 M 0 -35 R D +13619 11989 M 0 -35 R D 13766 11989 M 0 -35 R D 13886 11989 M 0 -35 R D +13988 11989 M 0 -35 R D 14076 11989 M 0 -35 R D 14153 11989 M 0 -35 R D +14679 11989 M 0 -35 R D 14946 11989 M 0 -35 R D 15135 11989 M 0 -35 R D +15282 11989 M 0 -35 R D 15402 11989 M 0 -35 R D 15504 11989 M 0 -35 R D +15592 11989 M 0 -35 R D 15669 11989 M 0 -35 R D 16195 11989 M 0 -35 R D +16462 11989 M 0 -35 R D 16651 11989 M 0 -35 R D 16798 11989 M 0 -35 R D +16918 11989 M 0 -35 R D 17020 11989 M 0 -35 R D 17107 11989 M 0 -35 R D +9675 8467 M 0 3522 R D 9675 8665 M 149 0 R D gsave 9563 8522 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9675 9942 M 149 0 R D gsave 9563 9800 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9675 11220 M 149 0 R D gsave 9563 11078 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 9675 8467 M 74 0 R D 9675 8541 M 74 0 R D 9675 8606 M +74 0 R D 9675 9049 M 74 0 R D 9675 9274 M 74 0 R D 9675 9434 M 74 0 R D +9675 9558 M 74 0 R D 9675 9659 M 74 0 R D 9675 9744 M 74 0 R D 9675 9818 M +74 0 R D 9675 9884 M 74 0 R D 9675 10327 M 74 0 R D 9675 10552 M 74 0 R D +9675 10711 M 74 0 R D 9675 10835 M 74 0 R D 9675 10936 M 74 0 R D +9675 11022 M 74 0 R D 9675 11096 M 74 0 R D 9675 11161 M 74 0 R D +9675 11604 M 74 0 R D 9675 11829 M 74 0 R D 9675 11989 M 74 0 R D +17107 8467 M 0 3522 R D 17107 8665 M -148 0 R D 17107 9942 M -148 0 R D +17107 11220 M -148 0 R D 17107 8467 M -74 0 R D 17107 8541 M -74 0 R D +17107 8606 M -74 0 R D 17107 9049 M -74 0 R D 17107 9274 M -74 0 R D +17107 9434 M -74 0 R D 17107 9558 M -74 0 R D 17107 9659 M -74 0 R D +17107 9744 M -74 0 R D 17107 9818 M -74 0 R D 17107 9884 M -74 0 R D +17107 10327 M -74 0 R D 17107 10552 M -74 0 R D 17107 10711 M -74 0 R D +17107 10835 M -74 0 R D 17107 10936 M -74 0 R D 17107 11022 M -74 0 R D +17107 11096 M -74 0 R D 17107 11161 M -74 0 R D 17107 11604 M -74 0 R D +17107 11829 M -74 0 R D 17107 11989 M -74 0 R D 20 setlinewidth +0.000 0.514 1.000 setrgbcolor 9674 11516 M 112 0 R -111 0 R 0 111 R 0 -222 R +D 9674 11516 M 1 0 R D 9715 11516 M 222 0 R -111 0 R 0 111 R 0 -222 R D +9675 11516 M 151 0 R D 9867 11516 M 222 0 R -111 0 R 0 111 R 0 -222 R D +9826 11516 M 152 0 R D 10019 11516 M 222 0 R -111 0 R 0 111 R 0 -222 R D +9978 11516 M 152 0 R D 10170 11516 M 222 0 R -111 0 R 0 111 R 0 -222 R D +10130 11516 M 151 0 R D 10322 11516 M 222 0 R -111 0 R 0 111 R 0 -222 R D +10281 11516 M 152 0 R D 10473 11510 M 222 0 R -111 0 R 0 111 R 0 -222 R D +10433 11516 M 151 -6 R D 10625 11495 M 222 0 R -111 0 R 0 111 R 0 -222 R D +10584 11510 M 152 -15 R D 10777 11446 M 222 0 R -111 0 R 0 111 R 0 -222 R D +10736 11495 M 152 -49 R D 10928 11388 M 222 0 R -111 0 R 0 111 R 0 -222 R D +10888 11446 M 151 -58 R D 11080 11367 M 222 0 R -111 0 R 0 111 R 0 -222 R D +11039 11388 M 152 -21 R D 11231 11348 M 222 0 R -111 0 R 0 111 R 0 -222 R D +11191 11367 M 151 -19 R D 11383 11343 M 222 0 R -111 0 R 0 111 R 0 -222 R D +11342 11348 M 152 -5 R D 11535 11339 M 222 0 R -111 0 R 0 111 R 0 -222 R D +11494 11343 M 152 -4 R D 11686 11332 M 222 0 R -111 0 R 0 111 R 0 -222 R D +11646 11339 M 151 -7 R D 11838 11322 M 222 0 R -111 0 R 0 111 R 0 -222 R D +11797 11332 M 152 -10 R D 11989 11316 M 222 0 R -111 0 R 0 111 R 0 -222 R D +11949 11322 M 151 -6 R D 12141 11280 M 222 0 R -111 0 R 0 111 R 0 -222 R D +12100 11316 M 152 -36 R D 12292 11217 M 222 0 R -111 0 R 0 111 R 0 -222 R D +12252 11280 M 151 -63 R D 12444 11122 M 222 0 R -111 0 R 0 111 R 0 -222 R D +12403 11217 M 152 -95 R D 12596 10975 M 222 0 R -111 0 R 0 111 R 0 -222 R D +12555 11122 M 152 -147 R D 12747 10766 M 222 0 R -111 0 R 0 111 R 0 -222 R D +12707 10975 M 151 -209 R D 12899 10467 M 222 0 R -111 0 R 0 111 R 0 -222 R D +12858 10766 M 152 -299 R D 13050 10179 M 222 0 R -111 0 R 0 111 R 0 -222 R D +13010 10467 M 151 -288 R D 13202 9896 M 222 0 R -111 0 R 0 111 R 0 -222 R D +13161 10179 M 152 -283 R D 13354 9753 M 222 0 R -111 0 R 0 111 R 0 -222 R D +13313 9896 M 152 -143 R D 13505 9681 M 222 0 R -111 0 R 0 111 R 0 -222 R D +13465 9753 M 151 -72 R D 13657 9637 M 222 0 R -111 0 R 0 111 R 0 -222 R D +13616 9681 M 152 -44 R D 13808 9471 M 222 0 R -111 0 R 0 111 R 0 -222 R D +13768 9637 M 151 -166 R D 13960 9316 M 222 0 R -111 0 R 0 111 R 0 -222 R D +13919 9471 M 152 -155 R D 14112 9087 M 222 0 R -111 0 R 0 111 R 0 -222 R D +14071 9316 M 152 -229 R D 14263 8975 M 222 0 R -111 0 R 0 111 R 0 -222 R D +14223 9087 M 151 -112 R D 14415 8586 M 222 0 R -111 0 R 0 111 R 0 -222 R D +14374 8975 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gsave 9675 889 translate 0 0 M 1.01 dup scale +-308.339 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(8) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 11191 1422 M 0 71 R D +gsave 11191 889 translate 0 0 M 1.01 dup scale -308.339 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(9) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 12707 1422 M 0 71 R D +gsave 12707 889 translate 0 0 M 1.01 dup scale -381.305 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(10) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 14223 1422 M 0 71 R D +gsave 14223 889 translate 0 0 M 1.01 dup scale -381.305 0 N +(10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(11) show grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT 15738 1422 M 0 71 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0 R D 0.000 0.000 0.000 setrgbcolor +gsave 11939 1769 translate 0 0 M 1.01 dup scale +(Simulation) show grestore gsave 13766 4276 translate 0 0 M 1.01 dup scale +(M) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(BH) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(\(t) show X -101.051 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(0) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(\) = 10) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(7) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( M) show CP X -101.051 M +%%IncludeResource: font AvantGarde-Book +262.467 /AvantGarde-Book STDFONT +(O) show M X -58.3193 M +%%IncludeResource: font AvantGarde-Book +186.267 /AvantGarde-Book STDFONT +( \267) show +%%IncludeResource: font Helvetica +186.267 /Helvetica STDFONT grestore +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +%%PageTrailer +end +restore +showpage +%%PageResources: font Helvetica +%%+ font AvantGarde-Book +%%Trailer +restore +%%Pages: 1 +%%DocumentNeededResources: font Helvetica +%%+ font AvantGarde-Book +%%EOF diff --git a/feedback/papers/0506398/f7.ps b/feedback/papers/0506398/f7.ps new file mode 100644 index 0000000..55da5f7 --- /dev/null +++ b/feedback/papers/0506398/f7.ps @@ -0,0 +1,748 @@ +%!PS-Adobe-3.0 +%%BoundingBox: 54 360 558 720 +%%Title: Graphics produced by IDL +%%For: phopkins@net-93286, +%% /Users/phopkins/Documents/lars_galaxies/plots/high_z +%%Creator: IDL Student Edition 6.0, Mac OS X (darwin ppc m32) +%%CreationDate: Mon May 16 05:27:49 2005 +%%DocumentData: Clean7bit +%%Requirements: color +%%LanguageLevel: 1 +%%PageOrder: Ascend +%%Pages: (atend) +%%DocumentNeededResources: (atend) +%%EndComments +%%BeginProlog +save +%+ prolog.ps -- Prolog for IDL generated PostScript files +%+ Copyright (c) 1988-2003 Research Systems, Inc. All Rights Reserved. +%v 4 +/$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C +{currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint +stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} +bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show +grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 +setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 +{[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 +100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 +{[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef +/ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} +ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont +exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica +findfont exch scalefont setfont (\267) show currentpoint 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R D 5006 11989 M 0 -106 R D 5241 11989 M 0 -106 R D +5433 11989 M 0 -106 R D 5595 11989 M 0 -106 R D 5736 11989 M 0 -106 R D +5860 11989 M 0 -106 R D 6701 11989 M 0 -106 R D 7128 11989 M 0 -106 R D +7431 11989 M 0 -106 R D 7666 11989 M 0 -106 R D 7858 11989 M 0 -106 R D +8020 11989 M 0 -106 R D 8161 11989 M 0 -106 R D 8285 11989 M 0 -106 R D +9126 11989 M 0 -106 R D 1121 1422 M 0 10567 R D 1121 1422 M 162 0 R D +gsave 1009 1422 translate 0 0 M 1.01 dup scale -117.687 0 N +( ) show grestore 1121 3183 M 162 0 R D gsave 1009 3041 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 1121 4944 M 162 0 R D gsave 1009 4802 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 1121 6706 M 162 0 R D gsave 1009 6563 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 1121 8467 M 162 0 R D gsave 1009 8325 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 1121 10228 M 162 0 R D gsave 1009 10086 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 1121 11989 M 162 0 R D gsave 1009 11740 translate 0 0 M +1.01 dup scale -117.687 0 N +( ) show grestore 1121 1774 M 81 0 R D 1121 2127 M 81 0 R D 1121 2479 M +81 0 R D 1121 2831 M 81 0 R D 1121 3536 M 81 0 R D 1121 3888 M 81 0 R D +1121 4240 M 81 0 R D 1121 4592 M 81 0 R D 1121 5297 M 81 0 R D 1121 5649 M +81 0 R D 1121 6001 M 81 0 R D 1121 6353 M 81 0 R D 1121 7058 M 81 0 R D +1121 7410 M 81 0 R D 1121 7762 M 81 0 R D 1121 8115 M 81 0 R D 1121 8819 M +81 0 R D 1121 9171 M 81 0 R D 1121 9523 M 81 0 R D 1121 9876 M 81 0 R D +1121 10580 M 81 0 R D 1121 10932 M 81 0 R D 1121 11285 M 81 0 R D +1121 11637 M 81 0 R D gsave 555 6706 translate 0 0 M 90 rotate +1.01 dup scale -2575.77 0 N +(Probability \(Arbitrary Scale\)) show grestore 9226 1422 M 0 10567 R D +9226 1422 M -162 0 R D 9226 3183 M -162 0 R D 9226 4944 M -162 0 R D +9226 6706 M -162 0 R D 9226 8467 M -162 0 R D 9226 10228 M -162 0 R D +9226 11989 M -162 0 R D 9226 1774 M -81 0 R D 9226 2127 M -81 0 R D +9226 2479 M -81 0 R D 9226 2831 M -81 0 R D 9226 3536 M -81 0 R D +9226 3888 M -81 0 R D 9226 4240 M -81 0 R D 9226 4592 M -81 0 R D +9226 5297 M -81 0 R D 9226 5649 M -81 0 R D 9226 6001 M -81 0 R D +9226 6353 M -81 0 R D 9226 7058 M -81 0 R D 9226 7410 M -81 0 R D +9226 7762 M -81 0 R D 9226 8115 M -81 0 R D 9226 8819 M -81 0 R D +9226 9171 M -81 0 R D 9226 9523 M -81 0 R D 9226 9876 M -81 0 R D +9226 10580 M -81 0 R D 9226 10932 M -81 0 R D 9226 11285 M -81 0 R D +9226 11637 M -81 0 R D 20 setlinewidth 1121 1423 M 111 0 R -111 0 R 0 111 R +0 -112 R D 1374 1424 M 222 0 R -111 0 R 0 111 R 0 -113 R D 1121 1423 M +364 1 R D 1738 1425 M 222 0 R -111 0 R 0 111 R 0 -114 R D 1485 1424 M +364 1 R D 2101 1425 M 222 0 R -111 0 R 0 111 R 0 -114 R D 1849 1425 M +363 0 R D 2465 1427 M 222 0 R -111 0 R 0 111 R 0 -116 R D 2212 1425 M +364 2 R D 2829 1431 M 222 0 R -111 0 R 0 111 R 0 -120 R D 2576 1427 M +364 4 R D 3193 1434 M 222 0 R -111 0 R 0 111 R 0 -123 R D 2940 1431 M +364 3 R D 3556 1444 M 222 0 R -111 0 R 0 111 R 0 -133 R D 3304 1434 M +363 10 R D 3920 1447 M 222 0 R -111 0 R 0 111 R 0 -136 R D 3667 1444 M +364 3 R D 4284 1475 M 222 0 R -111 0 R 0 111 R 0 -164 R D 4031 1447 M +364 28 R D 4648 1485 M 222 0 R -111 0 R 0 111 R 0 -174 R D 4395 1475 M +364 10 R D 5011 1545 M 222 0 R -111 0 R 0 111 R 0 -222 R D 4759 1485 M +363 60 R D 5375 1595 M 222 0 R -111 0 R 0 111 R 0 -222 R D 5122 1545 M +364 50 R D 5739 1736 M 222 0 R -111 0 R 0 111 R 0 -222 R D 5486 1595 M +364 141 R D 6103 1913 M 222 0 R -111 0 R 0 111 R 0 -222 R D 5850 1736 M +364 177 R D 6466 2161 M 222 0 R -111 0 R 0 111 R 0 -222 R D 6214 1913 M +363 248 R D 6830 2795 M 222 0 R -111 0 R 0 111 R 0 -222 R D 6577 2161 M +364 634 R D 7194 3626 M 222 0 R -111 0 R 0 111 R 0 -222 R D 6941 2795 M +364 831 R D 7558 5343 M 222 0 R -111 0 R 0 111 R 0 -222 R D 7305 3626 M +364 1717 R D 7921 7860 M 222 0 R -111 0 R 0 111 R 0 -222 R D 7669 5343 M +363 2517 R D 8285 11635 M 222 0 R -111 0 R 0 111 R 0 -222 R D 8032 7860 M +364 3775 R D 8649 10393 M 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setlinewidth +16181 1422 M -1 15 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 9 R +-12 8 R -13 7 R -13 4 R -15 3 R -14 1 R -15 -1 R -14 -3 R -14 -4 R -13 -7 R +-12 -8 R -11 -9 R -9 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -15 R D +16181 1422 M Z 20 setlinewidth 15518 1422 M 552 0 R D 10 setlinewidth +16732 1422 M -1 15 R -2 14 R -5 14 R -6 13 R -9 12 R -9 11 R -11 9 R -12 8 R +-13 7 R -14 4 R -14 3 R -15 1 R -14 -1 R -14 -3 R -14 -4 R -13 -7 R -12 -8 R +-11 -9 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -15 R D +16732 1422 M Z 20 setlinewidth 16070 1422 M 551 0 R D 10 setlinewidth +17284 1422 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -10 11 R -10 9 R +-13 8 R -13 7 R -13 4 R -15 3 R -14 1 R -14 -1 R -15 -3 R -13 -4 R -14 -7 R +-12 -8 R -10 -9 R -10 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -15 R D +17284 1422 M Z 20 setlinewidth 16621 1422 M 552 0 R 382 0 R D +%%PageTrailer +end +restore +showpage +%%PageResources: font Helvetica +%%+ font AvantGarde-Book +%%Trailer +restore +%%Pages: 1 +%%DocumentNeededResources: font Helvetica +%%+ font AvantGarde-Book +%%EOF diff --git a/feedback/papers/0506398/f8.ps b/feedback/papers/0506398/f8.ps new file mode 100644 index 0000000..c7a144c --- /dev/null +++ b/feedback/papers/0506398/f8.ps @@ -0,0 +1,210 @@ +%!PS-Adobe-3.0 +%%BoundingBox: 54 360 558 720 +%%Title: Graphics produced by IDL +%%For: phopkins@net-93286, +%% /Users/phopkins/Documents/lars_galaxies/plots/high_z/from_zeus +%%Creator: IDL Student Edition 6.0, Mac OS X (darwin ppc m32) +%%CreationDate: Mon Apr 11 03:37:15 2005 +%%DocumentData: Clean7bit +%%Requirements: color +%%LanguageLevel: 1 +%%PageOrder: Ascend +%%Pages: (atend) +%%DocumentNeededResources: (atend) +%%EndComments +%%BeginProlog +save +%+ prolog.ps -- Prolog for IDL generated PostScript files +%+ Copyright (c) 1988-2003 Research Systems, Inc. All Rights Reserved. +%v 4 +/$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C +{currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint +stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} +bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show +grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 +setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 +{[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 +100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 +{[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef +/ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} +ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont +exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica +findfont exch scalefont setfont (\267) show currentpoint grestore moveto} +bdef end 2.5 setmiterlimit +%%EndProlog +%%Page: 0 1 +%%PageRequirements: color +%%PageResources: (atend) +%%PageOrientation: Portrait +%%PageBoundingBox: 54 360 558 720 +%%BeginPageSetup +save +$IDL_DICT begin 54 360 translate 0.0283465 dup scale +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +%%EndPageSetup +15 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 1570 1422 M 15762 0 R D +1570 1422 M 0 211 R D gsave 1570 889 translate 0 0 M 1.01 dup scale +-117.687 0 N +(8) show grestore 4435 1422 M 0 211 R D gsave 4435 889 translate 0 0 M +1.01 dup scale -117.687 0 N +(9) show grestore 7301 1422 M 0 211 R D gsave 7301 889 translate 0 0 M +1.01 dup scale -235.373 0 N +(10) show grestore 10167 1422 M 0 211 R D gsave 10167 889 translate 0 0 M +1.01 dup scale -235.373 0 N +(11) show grestore 13033 1422 M 0 211 R D gsave 13033 889 translate 0 0 M +1.01 dup scale -235.373 0 N +(12) show grestore 15899 1422 M 0 211 R D gsave 15899 889 translate 0 0 M +1.01 dup scale -235.373 0 N +(13) show grestore 1856 1422 M 0 106 R D 2143 1422 M 0 106 R D 2429 1422 M +0 106 R D 2716 1422 M 0 106 R D 3003 1422 M 0 106 R D 3289 1422 M 0 106 R D +3576 1422 M 0 106 R D 3862 1422 M 0 106 R D 4149 1422 M 0 106 R D +4722 1422 M 0 106 R D 5009 1422 M 0 106 R D 5295 1422 M 0 106 R D +5582 1422 M 0 106 R D 5868 1422 M 0 106 R D 6155 1422 M 0 106 R D +6442 1422 M 0 106 R D 6728 1422 M 0 106 R D 7015 1422 M 0 106 R D +7588 1422 M 0 106 R D 7874 1422 M 0 106 R D 8161 1422 M 0 106 R D +8448 1422 M 0 106 R D 8734 1422 M 0 106 R D 9021 1422 M 0 106 R D +9307 1422 M 0 106 R D 9594 1422 M 0 106 R D 9881 1422 M 0 106 R D +10454 1422 M 0 106 R D 10740 1422 M 0 106 R D 11027 1422 M 0 106 R D +11313 1422 M 0 106 R D 11600 1422 M 0 106 R D 11887 1422 M 0 106 R D +12173 1422 M 0 106 R D 12460 1422 M 0 106 R D 12746 1422 M 0 106 R D +13319 1422 M 0 106 R D 13606 1422 M 0 106 R D 13893 1422 M 0 106 R D +14179 1422 M 0 106 R D 14466 1422 M 0 106 R D 14752 1422 M 0 106 R D +15039 1422 M 0 106 R D 15326 1422 M 0 106 R D 15612 1422 M 0 106 R D +16185 1422 M 0 106 R D 16472 1422 M 0 106 R D 16758 1422 M 0 106 R D +17045 1422 M 0 106 R D 17332 1422 M 0 106 R D gsave 9451 427 translate 0 0 M +1.01 dup scale -3065.68 0 N +(Log\( Bolometric Luminosity / L) show CP X -101.051 M +%%IncludeResource: font AvantGarde-Book +262.467 /AvantGarde-Book STDFONT +(O) show M X -58.3193 M +%%IncludeResource: font AvantGarde-Book +186.267 /AvantGarde-Book STDFONT +( \267) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( \)) show grestore 1570 11989 M 15762 0 R D 1570 11989 M 0 -211 R D +4435 11989 M 0 -211 R D 7301 11989 M 0 -211 R D 10167 11989 M 0 -211 R D +13033 11989 M 0 -211 R D 15899 11989 M 0 -211 R D 1856 11989 M 0 -106 R D +2143 11989 M 0 -106 R D 2429 11989 M 0 -106 R D 2716 11989 M 0 -106 R D +3003 11989 M 0 -106 R D 3289 11989 M 0 -106 R D 3576 11989 M 0 -106 R D +3862 11989 M 0 -106 R D 4149 11989 M 0 -106 R D 4722 11989 M 0 -106 R D +5009 11989 M 0 -106 R D 5295 11989 M 0 -106 R D 5582 11989 M 0 -106 R D +5868 11989 M 0 -106 R D 6155 11989 M 0 -106 R D 6442 11989 M 0 -106 R D +6728 11989 M 0 -106 R D 7015 11989 M 0 -106 R D 7588 11989 M 0 -106 R D +7874 11989 M 0 -106 R D 8161 11989 M 0 -106 R D 8448 11989 M 0 -106 R D +8734 11989 M 0 -106 R D 9021 11989 M 0 -106 R D 9307 11989 M 0 -106 R D +9594 11989 M 0 -106 R D 9881 11989 M 0 -106 R D 10454 11989 M 0 -106 R D +10740 11989 M 0 -106 R D 11027 11989 M 0 -106 R D 11313 11989 M 0 -106 R D +11600 11989 M 0 -106 R D 11887 11989 M 0 -106 R D 12173 11989 M 0 -106 R D +12460 11989 M 0 -106 R D 12746 11989 M 0 -106 R D 13319 11989 M 0 -106 R D +13606 11989 M 0 -106 R D 13893 11989 M 0 -106 R D 14179 11989 M 0 -106 R D +14466 11989 M 0 -106 R D 14752 11989 M 0 -106 R D 15039 11989 M 0 -106 R D +15326 11989 M 0 -106 R D 15612 11989 M 0 -106 R D 16185 11989 M 0 -106 R D +16472 11989 M 0 -106 R D 16758 11989 M 0 -106 R D 17045 11989 M 0 -106 R D +17332 11989 M 0 -106 R D 1570 1422 M 0 10567 R D 1570 2077 M 315 0 R D +gsave 1458 1935 translate 0 0 M 1.01 dup scale -376.343 0 N +(-8) show grestore 1570 3947 M 315 0 R D gsave 1458 3805 translate 0 0 M +1.01 dup scale -376.343 0 N +(-7) show grestore 1570 5817 M 315 0 R D gsave 1458 5675 translate 0 0 M +1.01 dup scale -376.343 0 N +(-6) show grestore 1570 7687 M 315 0 R D gsave 1458 7545 translate 0 0 M +1.01 dup scale -376.343 0 N +(-5) show grestore 1570 9558 M 315 0 R D gsave 1458 9415 translate 0 0 M +1.01 dup scale -376.343 0 N +(-4) show grestore 1570 11428 M 315 0 R D gsave 1458 11286 translate 0 0 M +1.01 dup scale -376.343 0 N +(-3) show grestore 1570 1516 M 157 0 R D 1570 1703 M 157 0 R D 1570 1890 M +157 0 R D 1570 2264 M 157 0 R D 1570 2451 M 157 0 R D 1570 2638 M 157 0 R D +1570 2825 M 157 0 R D 1570 3012 M 157 0 R D 1570 3199 M 157 0 R D +1570 3386 M 157 0 R D 1570 3573 M 157 0 R D 1570 3760 M 157 0 R D +1570 4134 M 157 0 R D 1570 4321 M 157 0 R D 1570 4508 M 157 0 R D +1570 4695 M 157 0 R D 1570 4882 M 157 0 R D 1570 5069 M 157 0 R D +1570 5256 M 157 0 R D 1570 5443 M 157 0 R D 1570 5630 M 157 0 R D +1570 6004 M 157 0 R D 1570 6191 M 157 0 R D 1570 6378 M 157 0 R D +1570 6565 M 157 0 R D 1570 6752 M 157 0 R D 1570 6939 M 157 0 R D +1570 7126 M 157 0 R D 1570 7313 M 157 0 R D 1570 7500 M 157 0 R D +1570 7874 M 157 0 R D 1570 8062 M 157 0 R D 1570 8249 M 157 0 R D +1570 8436 M 157 0 R D 1570 8623 M 157 0 R D 1570 8810 M 157 0 R D +1570 8997 M 157 0 R D 1570 9184 M 157 0 R D 1570 9371 M 157 0 R D +1570 9745 M 157 0 R D 1570 9932 M 157 0 R D 1570 10119 M 157 0 R D +1570 10306 M 157 0 R D 1570 10493 M 157 0 R D 1570 10680 M 157 0 R D +1570 10867 M 157 0 R D 1570 11054 M 157 0 R D 1570 11241 M 157 0 R D +1570 11615 M 157 0 R D 1570 11802 M 157 0 R D 1570 11989 M 157 0 R D +gsave 741 6706 translate 0 0 M 90 rotate 1.01 dup scale -2423.88 0 N +(Log\( d) show +%%IncludeResource: font Symbol +423.333 /Symbol STDFONT +(F) show +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( / dlogL \) [Mpc) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(-3) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(]) show grestore 17332 1422 M 0 10567 R D 17332 2077 M -316 0 R D +17332 3947 M -316 0 R D 17332 5817 M -316 0 R D 17332 7687 M -316 0 R D +17332 9558 M -316 0 R D 17332 11428 M -316 0 R D 17332 1516 M -158 0 R D +17332 1703 M -158 0 R D 17332 1890 M -158 0 R D 17332 2264 M -158 0 R D +17332 2451 M -158 0 R D 17332 2638 M -158 0 R D 17332 2825 M -158 0 R D +17332 3012 M -158 0 R D 17332 3199 M -158 0 R D 17332 3386 M -158 0 R D +17332 3573 M -158 0 R D 17332 3760 M -158 0 R D 17332 4134 M -158 0 R D +17332 4321 M -158 0 R D 17332 4508 M -158 0 R D 17332 4695 M -158 0 R D +17332 4882 M -158 0 R D 17332 5069 M -158 0 R D 17332 5256 M -158 0 R D +17332 5443 M -158 0 R D 17332 5630 M -158 0 R D 17332 6004 M -158 0 R D +17332 6191 M -158 0 R D 17332 6378 M -158 0 R D 17332 6565 M -158 0 R D +17332 6752 M -158 0 R D 17332 6939 M -158 0 R D 17332 7126 M -158 0 R D +17332 7313 M -158 0 R D 17332 7500 M -158 0 R D 17332 7874 M -158 0 R D +17332 8062 M -158 0 R D 17332 8249 M -158 0 R D 17332 8436 M -158 0 R D +17332 8623 M -158 0 R D 17332 8810 M -158 0 R D 17332 8997 M -158 0 R D +17332 9184 M -158 0 R D 17332 9371 M -158 0 R D 17332 9745 M -158 0 R D +17332 9932 M -158 0 R D 17332 10119 M -158 0 R D 17332 10306 M -158 0 R D +17332 10493 M -158 0 R D 17332 10680 M -158 0 R D 17332 10867 M -158 0 R D +17332 11054 M -158 0 R D 17332 11241 M -158 0 R D 17332 11615 M -158 0 R D +17332 11802 M -158 0 R D 17332 11989 M -158 0 R D 20 setlinewidth +3003 11569 M 286 -109 R 287 -107 R 286 -102 R 287 -100 R 286 -97 R 287 -93 R +287 -89 R 286 -86 R 287 -83 R 286 -78 R 287 -76 R 287 -71 R 286 -68 R +287 -65 R 286 -60 R 287 -58 R 286 -53 R 287 -51 R 287 -47 R 286 -67 R +287 -142 R 286 -142 R 287 -145 R 287 -148 R 286 -151 R 287 -156 R 286 -160 R +287 -168 R 286 -174 R 287 -183 R 287 -193 R 286 -203 R 287 -214 R 286 -224 R +287 -236 R 287 -245 R 286 -256 R 287 -264 R 286 -272 R 287 -279 R 286 -284 R +287 -289 R 287 -293 R 286 -295 R 287 -298 R 286 -300 R 287 -302 R 286 -302 R +287 -303 R D 3003 10946 M 143 0 R 0 -85 R 143 0 R 143 0 R 0 113 R 144 0 R +143 0 R 0 110 R 143 0 R 144 0 R 0 -80 R 143 0 R 143 0 R 0 23 R 143 0 R +144 0 R 0 8 R 143 0 R 143 0 R 0 7 R 144 0 R 143 0 R 0 -127 R 143 0 R 143 0 R +0 -18 R 144 0 R 143 0 R 0 -100 R 143 0 R 144 0 R 0 -186 R 143 0 R 143 0 R +0 -71 R 144 0 R 143 0 R 0 -50 R 143 0 R 143 0 R 0 -142 R 144 0 R 143 0 R +0 -85 R 143 0 R 144 0 R 0 -145 R 143 0 R 143 0 R 0 -100 R 143 0 R 144 0 R +0 -15 R 143 0 R 143 0 R 0 -37 R 144 0 R 143 0 R 0 -86 R 143 0 R 143 0 R +0 22 R 144 0 R 143 0 R 0 -131 R 143 0 R 144 0 R 0 -132 R 143 0 R 143 0 R +0 -201 R 144 0 R 143 0 R 0 -105 R 143 0 R 143 0 R 0 -255 R 144 0 R 143 0 R +0 -109 R 143 0 R 144 0 R 0 -228 R 143 0 R 143 0 R 0 -148 R 143 0 R 144 0 R +0 -187 R 143 0 R 143 0 R 0 -88 R 144 0 R 143 0 R 0 -233 R 143 0 R 143 0 R +0 -256 R 144 0 R 143 0 R 0 -403 R 143 0 R 144 0 R 0 23 R 143 0 R 143 0 R +0 -302 R 144 0 R 143 0 R 0 -371 R 143 0 R 143 0 R 0 -142 R 144 0 R 143 0 R +0 -309 R 143 0 R 144 0 R 0 -258 R 143 0 R 143 0 R 0 -273 R 143 0 R 144 0 R +0 -317 R 143 0 R 143 0 R 0 -365 R 144 0 R 143 0 R 0 -196 R 143 0 R 143 0 R +0 -173 R 144 0 R 143 0 R 0 -276 R 143 0 R 144 0 R 0 -878 R 143 0 R 143 0 R +0 -1075 R 143 0 R 144 0 R 0 -1078 R 143 0 R D 40 setlinewidth 7660 1422 M +0 5071 R 358 0 R 358 0 R 0 -5071 R D 9092 1422 M 0 4828 R 359 0 R 358 0 R +0 -2430 R 358 0 R 358 0 R 0 1711 R 359 0 R 358 0 R 0 -1426 R 358 0 R 358 0 R +0 1952 R 358 0 R 359 0 R 0 -2390 R 358 0 R 358 0 R 0 825 R 358 0 R 359 0 R +0 -2121 R 358 0 R 358 0 R 0 -197 R 358 0 R 359 0 R 0 -654 R 358 0 R 358 0 R +0 885 R 358 0 R D gsave 14466 10867 translate 0 0 M 1.25 dup scale +(z = 0.5) show grestore +%%PageTrailer +end +restore +showpage +%%PageResources: font Helvetica +%%+ font Symbol +%%+ font AvantGarde-Book +%%Trailer +restore +%%Pages: 1 +%%DocumentNeededResources: font Helvetica +%%+ font Symbol +%%+ font AvantGarde-Book +%%EOF diff --git a/feedback/papers/0506398/f9.ps b/feedback/papers/0506398/f9.ps new file mode 100644 index 0000000..4ddd9c9 --- /dev/null +++ b/feedback/papers/0506398/f9.ps @@ -0,0 +1,1110 @@ +%!PS-Adobe-3.0 +%%BoundingBox: 54 360 904 926 +%%Title: Graphics produced by IDL +%%For: phopkins@net-93286, +%% /Users/phopkins/Documents/lars_galaxies/plots/high_z +%%Creator: IDL Student Edition 6.0, Mac OS X (darwin ppc m32) +%%CreationDate: Sun May 15 00:07:55 2005 +%%DocumentData: Clean7bit +%%Requirements: color +%%LanguageLevel: 1 +%%PageOrder: Ascend +%%Pages: (atend) +%%DocumentNeededResources: (atend) +%%EndComments +%%BeginProlog +save +%+ prolog.ps -- Prolog for IDL generated PostScript files +%+ Copyright (c) 1988-2003 Research Systems, Inc. All Rights Reserved. +%v 4 +/$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C +{currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint +stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} +bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show +grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 +setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 +{[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 +100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 +{[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef +/ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} +ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont +exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica +findfont exch scalefont setfont (\267) show currentpoint grestore moveto} +bdef end 2.5 setmiterlimit +%%EndProlog +%%Page: 0 1 +%%PageRequirements: color +%%PageResources: (atend) +%%PageOrientation: Portrait +%%PageBoundingBox: 54 360 904 926 +%%BeginPageSetup +save +$IDL_DICT begin 54 360 translate 0.0283465 dup scale +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +%%EndPageSetup +15 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 1776 11408 M 9334 0 R D +2710 11408 M 0 158 R D gsave 2710 10880 translate 0 0 M -117.687 0 N +(9) show grestore 4043 11408 M 0 158 R D gsave 4043 10880 translate 0 0 M +-235.373 0 N +(10) show grestore 5376 11408 M 0 158 R D gsave 5376 10880 translate 0 0 M +-235.373 0 N +(11) show grestore 6710 11408 M 0 158 R D gsave 6710 10880 translate 0 0 M +-235.373 0 N +(12) show grestore 8043 11408 M 0 158 R D gsave 8043 10880 translate 0 0 M +-235.373 0 N +(13) show grestore 9377 11408 M 0 158 R D gsave 9377 10880 translate 0 0 M +-235.373 0 N +(14) show grestore 10710 11408 M 0 158 R D gsave 10710 10880 translate 0 0 M +-235.373 0 N +(15) show grestore 1776 11408 M 0 79 R D 1909 11408 M 0 79 R D 2043 11408 M +0 79 R D 2176 11408 M 0 79 R D 2310 11408 M 0 79 R D 2443 11408 M 0 79 R D +2576 11408 M 0 79 R D 2843 11408 M 0 79 R D 2976 11408 M 0 79 R D +3110 11408 M 0 79 R D 3243 11408 M 0 79 R D 3376 11408 M 0 79 R D +3510 11408 M 0 79 R D 3643 11408 M 0 79 R D 3776 11408 M 0 79 R D +3910 11408 M 0 79 R D 4176 11408 M 0 79 R D 4310 11408 M 0 79 R D +4443 11408 M 0 79 R D 4576 11408 M 0 79 R D 4710 11408 M 0 79 R D +4843 11408 M 0 79 R D 4976 11408 M 0 79 R D 5110 11408 M 0 79 R D +5243 11408 M 0 79 R D 5510 11408 M 0 79 R D 5643 11408 M 0 79 R D +5776 11408 M 0 79 R D 5910 11408 M 0 79 R D 6043 11408 M 0 79 R D +6176 11408 M 0 79 R D 6310 11408 M 0 79 R D 6443 11408 M 0 79 R D +6576 11408 M 0 79 R D 6843 11408 M 0 79 R D 6977 11408 M 0 79 R D +7110 11408 M 0 79 R D 7243 11408 M 0 79 R D 7377 11408 M 0 79 R D +7510 11408 M 0 79 R D 7643 11408 M 0 79 R D 7777 11408 M 0 79 R D +7910 11408 M 0 79 R D 8177 11408 M 0 79 R D 8310 11408 M 0 79 R D +8443 11408 M 0 79 R D 8577 11408 M 0 79 R D 8710 11408 M 0 79 R D +8843 11408 M 0 79 R D 8977 11408 M 0 79 R D 9110 11408 M 0 79 R D +9243 11408 M 0 79 R D 9510 11408 M 0 79 R D 9643 11408 M 0 79 R D +9777 11408 M 0 79 R D 9910 11408 M 0 79 R D 10043 11408 M 0 79 R D +10177 11408 M 0 79 R D 10310 11408 M 0 79 R D 10443 11408 M 0 79 R D +10577 11408 M 0 79 R D 10843 11408 M 0 79 R D 10977 11408 M 0 79 R D +11110 11408 M 0 79 R D 1776 19296 M 9334 0 R D 2710 19296 M 0 -158 R D +4043 19296 M 0 -158 R D 5376 19296 M 0 -158 R D 6710 19296 M 0 -158 R D +8043 19296 M 0 -158 R D 9377 19296 M 0 -158 R D 10710 19296 M 0 -158 R D +1776 19296 M 0 -79 R D 1909 19296 M 0 -79 R D 2043 19296 M 0 -79 R D +2176 19296 M 0 -79 R D 2310 19296 M 0 -79 R D 2443 19296 M 0 -79 R D +2576 19296 M 0 -79 R D 2843 19296 M 0 -79 R D 2976 19296 M 0 -79 R D +3110 19296 M 0 -79 R D 3243 19296 M 0 -79 R D 3376 19296 M 0 -79 R D +3510 19296 M 0 -79 R D 3643 19296 M 0 -79 R D 3776 19296 M 0 -79 R D +3910 19296 M 0 -79 R D 4176 19296 M 0 -79 R D 4310 19296 M 0 -79 R D +4443 19296 M 0 -79 R D 4576 19296 M 0 -79 R D 4710 19296 M 0 -79 R D +4843 19296 M 0 -79 R D 4976 19296 M 0 -79 R D 5110 19296 M 0 -79 R D +5243 19296 M 0 -79 R D 5510 19296 M 0 -79 R D 5643 19296 M 0 -79 R D +5776 19296 M 0 -79 R D 5910 19296 M 0 -79 R D 6043 19296 M 0 -79 R D +6176 19296 M 0 -79 R D 6310 19296 M 0 -79 R D 6443 19296 M 0 -79 R D +6576 19296 M 0 -79 R D 6843 19296 M 0 -79 R D 6977 19296 M 0 -79 R D +7110 19296 M 0 -79 R D 7243 19296 M 0 -79 R D 7377 19296 M 0 -79 R D +7510 19296 M 0 -79 R D 7643 19296 M 0 -79 R D 7777 19296 M 0 -79 R D +7910 19296 M 0 -79 R D 8177 19296 M 0 -79 R D 8310 19296 M 0 -79 R D +8443 19296 M 0 -79 R D 8577 19296 M 0 -79 R D 8710 19296 M 0 -79 R D +8843 19296 M 0 -79 R D 8977 19296 M 0 -79 R D 9110 19296 M 0 -79 R D +9243 19296 M 0 -79 R D 9510 19296 M 0 -79 R D 9643 19296 M 0 -79 R D +9777 19296 M 0 -79 R D 9910 19296 M 0 -79 R D 10043 19296 M 0 -79 R D +10177 19296 M 0 -79 R D 10310 19296 M 0 -79 R D 10443 19296 M 0 -79 R D +10577 19296 M 0 -79 R D 10843 19296 M 0 -79 R D 10977 19296 M 0 -79 R D +11110 19296 M 0 -79 R D 1776 11408 M 0 7888 R D 1776 11408 M 187 0 R D +gsave 1665 11408 translate 0 0 M -611.717 0 N +(-12) show grestore 1776 13104 M 187 0 R D gsave 1665 12964 translate 0 0 M +-611.717 0 N +(-10) show grestore 1776 14801 M 187 0 R D gsave 1665 14660 translate 0 0 M +-376.343 0 N +(-8) show grestore 1776 16497 M 187 0 R D gsave 1665 16356 translate 0 0 M +-376.343 0 N +(-6) show grestore 1776 18193 M 187 0 R D gsave 1665 18053 translate 0 0 M +-376.343 0 N +(-4) show grestore 1776 11832 M 93 0 R D 1776 12256 M 93 0 R D 1776 12680 M +93 0 R D 1776 13529 M 93 0 R D 1776 13953 M 93 0 R D 1776 14377 M 93 0 R D +1776 15225 M 93 0 R D 1776 15649 M 93 0 R D 1776 16073 M 93 0 R D +1776 16921 M 93 0 R D 1776 17345 M 93 0 R D 1776 17769 M 93 0 R D +1776 18618 M 93 0 R D 1776 19042 M 93 0 R D 11110 11408 M 0 7888 R D +11110 11408 M -187 0 R D 11110 13104 M -187 0 R D 11110 14801 M -187 0 R D +11110 16497 M -187 0 R D 11110 18193 M -187 0 R D 11110 11832 M -93 0 R D +11110 12256 M -93 0 R D 11110 12680 M -93 0 R D 11110 13529 M -93 0 R D +11110 13953 M -93 0 R D 11110 14377 M -93 0 R D 11110 15225 M -93 0 R D +11110 15649 M -93 0 R D 11110 16073 M -93 0 R D 11110 16921 M -93 0 R D +11110 17345 M -93 0 R D 11110 17769 M -93 0 R D 11110 18618 M -93 0 R D +11110 19042 M -93 0 R D 3241 18683 M -2 22 R -4 21 R -7 21 R -10 19 R +-12 18 R -14 17 R -16 14 R -19 12 R -19 10 R -21 7 R -21 4 R -22 1 R +-21 -1 R -22 -4 R -20 -7 R -20 -10 R -18 -12 R -16 -14 R -15 -17 R -12 -18 R +-10 -19 R -7 -21 R -4 -21 R -1 -22 R 1 -22 R 4 -21 R 7 -21 R 10 -19 R +12 -19 R 15 -16 R 16 -14 R 18 -12 R 20 -10 R 20 -7 R 22 -4 R 21 -2 R 22 2 R +21 4 R 21 7 R 19 10 R 19 12 R 16 14 R 14 16 R 12 19 R 10 19 R 7 21 R 4 21 R +2 22 R F +4434 18027 M -2 21 R -4 22 R -7 20 R -10 20 R -12 18 R -14 16 R -16 15 R +-18 12 R -20 9 R -21 7 R -21 5 R -22 1 R -21 -1 R -22 -5 R -20 -7 R -20 -9 R +-18 -12 R -16 -15 R -15 -16 R -12 -18 R -10 -20 R -7 -20 R -4 -22 R -1 -21 R +1 -22 R 4 -21 R 7 -21 R 10 -20 R 12 -18 R 15 -16 R 16 -14 R 18 -13 R 20 -9 R +20 -7 R 22 -4 R 21 -2 R 22 2 R 21 4 R 21 7 R 20 9 R 18 13 R 16 14 R 14 16 R +12 18 R 10 20 R 7 21 R 4 21 R 2 22 R F +5243 17867 M -1 22 R -5 21 R -7 21 R -9 19 R -12 18 R -15 17 R -16 14 R +-18 12 R -20 10 R -20 7 R -22 4 R -21 1 R -22 -1 R -22 -4 R -20 -7 R +-20 -10 R -18 -12 R -16 -14 R -15 -17 R -12 -18 R -9 -19 R -7 -21 R -5 -21 R +-1 -22 R 1 -22 R 5 -21 R 7 -21 R 9 -19 R 12 -18 R 15 -17 R 16 -14 R 18 -12 R +20 -10 R 20 -7 R 22 -4 R 22 -2 R 21 2 R 22 4 R 20 7 R 20 10 R 18 12 R +16 14 R 15 17 R 12 18 R 9 19 R 7 21 R 5 21 R 1 22 R F +5698 17434 M -1 22 R -4 21 R -7 21 R -10 19 R -12 18 R -14 17 R -17 14 R +-18 12 R -19 10 R -21 7 R -21 4 R -22 2 R -22 -2 R -21 -4 R -21 -7 R +-19 -10 R -18 -12 R -17 -14 R -14 -17 R -12 -18 R -10 -19 R -7 -21 R +-4 -21 R -2 -22 R 2 -22 R 4 -21 R 7 -21 R 10 -19 R 12 -18 R 14 -17 R +17 -14 R 18 -12 R 19 -10 R 21 -7 R 21 -4 R 22 -1 R 22 1 R 21 4 R 21 7 R +19 10 R 18 12 R 17 14 R 14 17 R 12 18 R 10 19 R 7 21 R 4 21 R 1 22 R F +6385 16918 M -1 22 R -4 21 R -7 21 R -10 19 R -12 18 R -14 17 R -17 14 R +-18 12 R -20 10 R -20 7 R -21 4 R -22 1 R -22 -1 R -21 -4 R -21 -7 R +-19 -10 R -19 -12 R -16 -14 R -14 -17 R -12 -18 R -10 -19 R -7 -21 R +-4 -21 R -2 -22 R 2 -22 R 4 -21 R 7 -21 R 10 -19 R 12 -18 R 14 -17 R +16 -14 R 19 -12 R 19 -10 R 21 -7 R 21 -4 R 22 -2 R 22 2 R 21 4 R 20 7 R +20 10 R 18 12 R 17 14 R 14 17 R 12 18 R 10 19 R 7 21 R 4 21 R 1 22 R F +6996 16573 M -1 22 R -5 21 R -7 21 R -9 19 R -12 18 R -15 17 R -16 14 R +-18 12 R -20 10 R -20 7 R -22 4 R -21 2 R -22 -2 R -22 -4 R -20 -7 R +-20 -10 R -18 -12 R -16 -14 R -15 -17 R -12 -18 R -9 -19 R -7 -21 R -5 -21 R +-1 -22 R 1 -22 R 5 -21 R 7 -21 R 9 -19 R 12 -18 R 15 -17 R 16 -14 R 18 -12 R +20 -10 R 20 -7 R 22 -4 R 22 -1 R 21 1 R 22 4 R 20 7 R 20 10 R 18 12 R +16 14 R 15 17 R 12 18 R 9 19 R 7 21 R 5 21 R 1 22 R F +7634 16087 M -1 22 R -4 21 R -7 21 R -10 20 R -12 18 R -14 16 R -17 14 R +-18 12 R -19 10 R -21 7 R -21 4 R -22 2 R -22 -2 R -21 -4 R -21 -7 R +-19 -10 R -19 -12 R -16 -14 R -14 -16 R -12 -18 R -10 -20 R -7 -21 R +-4 -21 R -2 -22 R 2 -21 R 4 -22 R 7 -20 R 10 -20 R 12 -18 R 14 -16 R +16 -15 R 19 -12 R 19 -10 R 21 -7 R 21 -4 R 22 -1 R 22 1 R 21 4 R 21 7 R +19 10 R 18 12 R 17 15 R 14 16 R 12 18 R 10 20 R 7 20 R 4 22 R 1 21 R F +8623 14809 M -2 22 R -4 21 R -7 21 R -10 20 R -12 18 R -14 16 R -16 14 R +-19 13 R -19 9 R -21 7 R -21 4 R -22 2 R -22 -2 R -21 -4 R -21 -7 R -19 -9 R +-18 -13 R -17 -14 R -14 -16 R -12 -18 R -10 -20 R -7 -21 R -4 -21 R -1 -22 R +1 -21 R 4 -22 R 7 -20 R 10 -20 R 12 -18 R 14 -16 R 17 -15 R 18 -12 R +19 -10 R 21 -7 R 21 -4 R 22 -1 R 22 1 R 21 4 R 21 7 R 19 10 R 19 12 R +16 15 R 14 16 R 12 18 R 10 20 R 7 20 R 4 22 R 2 21 R F +10137 13745 M -2 22 R -4 21 R -7 21 R -10 19 R -12 18 R -14 17 R -16 14 R +-18 12 R -20 10 R -21 7 R -21 4 R -22 2 R -21 -2 R -22 -4 R -20 -7 R +-20 -10 R -18 -12 R -16 -14 R -15 -17 R -12 -18 R -10 -19 R -7 -21 R +-4 -21 R -1 -22 R 1 -22 R 4 -21 R 7 -21 R 10 -19 R 12 -18 R 15 -17 R +16 -14 R 18 -12 R 20 -10 R 20 -7 R 22 -4 R 21 -1 R 22 1 R 21 4 R 21 7 R +20 10 R 18 12 R 16 14 R 14 17 R 12 18 R 10 19 R 7 21 R 4 21 R 2 22 R F +20 setlinewidth 3028 18440 M 93 0 R -47 0 R 0 485 R -46 0 R 93 0 R D +4221 17815 M 93 0 R -47 0 R 0 424 R -46 0 R 93 0 R D 5030 17740 M 93 0 R +-46 0 R 0 254 R -47 0 R 93 0 R D 5485 17307 M 94 0 R -47 0 R 0 254 R -47 0 R +94 0 R D 6172 16791 M 93 0 R -46 0 R 0 254 R -47 0 R 93 0 R D 6783 16392 M +93 0 R -46 0 R 0 363 R -47 0 R 93 0 R D 7421 15906 M 94 0 R -47 0 R 0 363 R +-47 0 R 94 0 R D 8410 14507 M 93 0 R -47 0 R 0 605 R -46 0 R 93 0 R D +9924 13109 M 93 0 R -47 0 R 0 1272 R -46 0 R 93 0 R D 1776 18920 M 67 -10 R +66 -10 R 67 -10 R 67 -11 R 67 -11 R 66 -12 R 67 -12 R 67 -13 R 66 -13 R +67 -13 R 67 -15 R 66 -14 R 67 -15 R 67 -16 R 66 -16 R 67 -16 R 67 -18 R +66 -17 R 67 -19 R 67 -18 R 66 -20 R 67 -20 R 67 -20 R 66 -21 R 67 -22 R +67 -22 R 66 -23 R 67 -24 R 67 -24 R 66 -24 R 67 -26 R 67 -26 R 66 -26 R +67 -28 R 67 -27 R 66 -29 R 67 -29 R 67 -30 R 66 -31 R 67 -31 R 67 -32 R +66 -32 R 67 -33 R 67 -34 R 66 -35 R 67 -35 R 67 -36 R 66 -37 R 67 -37 R +67 -38 R 66 -39 R 67 -39 R 67 -40 R 66 -41 R 67 -42 R 67 -42 R 66 -43 R +67 -44 R 67 -45 R 66 -45 R 67 -46 R 67 -47 R 66 -47 R 67 -48 R 67 -49 R +66 -50 R 67 -50 R 67 -52 R 66 -52 R 67 -52 R 67 -54 R 66 -54 R 67 -55 R +67 -56 R 67 -56 R 66 -58 R 67 -58 R 67 -59 R 66 -59 R 67 -61 R 67 -61 R +66 -62 R 67 -63 R 67 -63 R 66 -65 R 67 -65 R 67 -66 R 66 -66 R 67 -68 R +67 -68 R 66 -69 R 67 -70 R 67 -71 R 66 -71 R 67 -72 R 67 -73 R 66 -74 R +67 -75 R 67 -75 R 66 -76 R 67 -77 R 67 -78 R 66 -79 R 67 -79 R 67 -81 R +66 -81 R 67 -82 R 67 -82 R 66 -84 R 67 -84 R 67 -86 R 66 -85 R 67 -87 R +67 -88 R 66 -88 R 67 -90 R 67 -90 R 66 -91 R 67 -91 R 67 -93 R 66 -93 R +67 -94 R 67 -95 R 66 -96 R 67 -97 R 67 -97 R 66 -99 R 67 -99 R 67 -100 R +66 -100 R 67 -102 R 67 -103 R 66 -103 R 67 -104 R 67 -105 R 66 -106 R +67 -106 R 67 -108 R 13 -22 R D 1.000 0.000 0.000 setrgbcolor 2209 18711 M +0 250 R 250 0 R 0 -250 R -250 0 R F +3185 17797 M 0 250 R 250 0 R 0 -250 R -250 0 R F +4200 17359 M 0 249 R 250 0 R 0 -249 R -250 0 R F +4926 17137 M 0 250 R 250 0 R 0 -250 R -250 0 R F +5586 16782 M 0 250 R 250 0 R 0 -250 R -250 0 R F +6173 16344 M 0 250 R 250 0 R 0 -250 R -250 0 R F +6856 15770 M 0 249 R 250 0 R 0 -249 R -250 0 R F +7636 15069 M 0 249 R 250 0 R 0 -249 R -250 0 R F +8692 13588 M 0 249 R 249 0 R 0 -249 R -249 0 R F +2287 18454 M 94 0 R -47 0 R 0 730 R -47 0 R 94 0 R D 3263 17625 M 94 0 R +-47 0 R 0 577 R -47 0 R 94 0 R D 4279 17212 M 93 0 R -47 0 R 0 534 R -46 0 R +93 0 R D 5005 17042 M 93 0 R -47 0 R 0 441 R -46 0 R 93 0 R D 5664 16678 M +94 0 R -47 0 R 0 450 R -47 0 R 94 0 R D 6252 16240 M 93 0 R -47 0 R 0 449 R +-46 0 R 93 0 R D 6934 15665 M 93 0 R -46 0 R 0 458 R -47 0 R 93 0 R D +7714 14939 M 94 0 R -47 0 R 0 492 R -47 0 R 94 0 R D 8770 12864 M 93 0 R +-46 0 R 0 1425 R -47 0 R 93 0 R D L2 1909 18229 M 67 219 R 67 63 R 67 30 R +66 15 R 67 7 R 67 1 R 66 -2 R 67 -4 R 67 -7 R 66 -9 R 67 -10 R 67 -11 R +66 -13 R 67 -14 R 67 -15 R 66 -16 R 67 -16 R 67 -18 R 66 -18 R 67 -20 R +67 -20 R 66 -20 R 67 -22 R 67 -22 R 66 -23 R 67 -24 R 67 -25 R 66 -25 R +67 -26 R 67 -27 R 66 -28 R 67 -28 R 67 -29 R 66 -30 R 67 -30 R 67 -32 R +66 -32 R 67 -32 R 67 -34 R 66 -34 R 67 -35 R 67 -36 R 66 -36 R 67 -38 R +67 -38 R 66 -38 R 67 -40 R 67 -40 R 66 -41 R 67 -42 R 67 -43 R 66 -43 R +67 -44 R 67 -45 R 66 -46 R 67 -46 R 67 -47 R 66 -48 R 67 -49 R 67 -50 R +66 -50 R 67 -51 R 67 -52 R 66 -53 R 67 -54 R 67 -54 R 66 -55 R 67 -56 R +67 -57 R 66 -58 R 67 -58 R 67 -59 R 67 -61 R 66 -60 R 67 -62 R 67 -63 R +66 -63 R 67 -64 R 67 -65 R 66 -66 R 67 -67 R 67 -67 R 66 -69 R 67 -69 R +67 -70 R 66 -71 R 67 -71 R 67 -73 R 66 -73 R 67 -74 R 67 -75 R 66 -76 R +67 -77 R 67 -78 R 66 -78 R 67 -79 R 67 -80 R 66 -81 R 67 -82 R 67 -83 R +66 -84 R 67 -84 R 67 -85 R 66 -86 R 67 -88 R 67 -87 R 66 -89 R 67 -90 R +67 -90 R 66 -92 R 67 -92 R 67 -93 R 66 -94 R 67 -95 R 67 -95 R 66 -97 R +67 -97 R 67 -99 R 66 -99 R 67 -100 R 67 -101 R 66 -102 R 67 -102 R 67 -104 R +66 -104 R 67 -106 R 67 -106 R 66 -107 R 67 -108 R 67 -109 R 33 -56 R D +0.000 0.000 0.000 setrgbcolor gsave 2376 14207 translate 0 0 M +1.25 dup scale +( z < 0.2) show grestore L3 0.000 0.965 1.000 setrgbcolor 2442 12147 M +1599 0 R D 0.000 0.000 0.000 setrgbcolor gsave 4307 12042 translate 0 0 M +0.9 dup scale +(Broad-line X-ray \(Barger 2005\)) show grestore L1 +0.000 0.282 1.000 setrgbcolor 2442 12570 M 1599 0 R D +0.000 0.000 0.000 setrgbcolor gsave 4307 12464 translate 0 0 M 0.9 dup scale +(B-Band \(Croom 2004\)) show grestore L2 1.000 0.000 0.000 setrgbcolor +2442 12992 M 1599 0 R D 0.000 0.000 0.000 setrgbcolor +gsave 4307 12887 translate 0 0 M 0.9 dup scale +(Soft X-ray \(Miyaji 2001\)) show grestore L0 2442 13415 M 1599 0 R D +gsave 4307 13309 translate 0 0 M 0.9 dup scale +(Hard X-ray \(Ueda 2003\)) show grestore gsave 709 11408 translate 0 0 M +90 rotate 1.5 dup scale -2423.88 0 N +(Log\( d) show +%%IncludeResource: font Symbol +423.333 /Symbol STDFONT +(F) show +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +( / dlogL \) [Mpc) show X 192.937 M +%%IncludeResource: font Helvetica +262.467 /Helvetica STDFONT +(-3) show X 0 M +%%IncludeResource: font Helvetica +423.333 /Helvetica STDFONT +(]) show grestore 15 setlinewidth 11110 11408 M 9334 0 R D 12044 11408 M +0 158 R D gsave 12044 10880 translate 0 0 M -117.687 0 N +(9) show grestore 13377 11408 M 0 158 R D gsave 13377 10880 translate 0 0 M +-235.373 0 N +(10) show grestore 14710 11408 M 0 158 R D gsave 14710 10880 translate 0 0 M +-235.373 0 N +(11) show grestore 16044 11408 M 0 158 R D gsave 16044 10880 translate 0 0 M +-235.373 0 N +(12) show grestore 17377 11408 M 0 158 R D gsave 17377 10880 translate 0 0 M +-235.373 0 N +(13) show grestore 18711 11408 M 0 158 R D gsave 18711 10880 translate 0 0 M +-235.373 0 N +(14) show grestore 20044 11408 M 0 158 R D gsave 20044 10880 translate 0 0 M +-235.373 0 N +(15) show grestore 11110 11408 M 0 79 R D 11243 11408 M 0 79 R D +11377 11408 M 0 79 R D 11510 11408 M 0 79 R D 11644 11408 M 0 79 R D +11777 11408 M 0 79 R D 11910 11408 M 0 79 R D 12177 11408 M 0 79 R D +12310 11408 M 0 79 R D 12444 11408 M 0 79 R D 12577 11408 M 0 79 R D +12710 11408 M 0 79 R D 12844 11408 M 0 79 R D 12977 11408 M 0 79 R D +13110 11408 M 0 79 R D 13244 11408 M 0 79 R D 13510 11408 M 0 79 R D +13644 11408 M 0 79 R D 13777 11408 M 0 79 R D 13910 11408 M 0 79 R D +14044 11408 M 0 79 R D 14177 11408 M 0 79 R D 14310 11408 M 0 79 R D +14444 11408 M 0 79 R D 14577 11408 M 0 79 R D 14844 11408 M 0 79 R D +14977 11408 M 0 79 R D 15110 11408 M 0 79 R D 15244 11408 M 0 79 R D +15377 11408 M 0 79 R D 15510 11408 M 0 79 R D 15644 11408 M 0 79 R D +15777 11408 M 0 79 R D 15910 11408 M 0 79 R D 16177 11408 M 0 79 R D +16311 11408 M 0 79 R D 16444 11408 M 0 79 R D 16577 11408 M 0 79 R D +16711 11408 M 0 79 R D 16844 11408 M 0 79 R D 16977 11408 M 0 79 R D +17111 11408 M 0 79 R D 17244 11408 M 0 79 R D 17511 11408 M 0 79 R D +17644 11408 M 0 79 R D 17777 11408 M 0 79 R D 17911 11408 M 0 79 R D +18044 11408 M 0 79 R D 18177 11408 M 0 79 R D 18311 11408 M 0 79 R D +18444 11408 M 0 79 R D 18577 11408 M 0 79 R D 18844 11408 M 0 79 R D +18977 11408 M 0 79 R D 19111 11408 M 0 79 R D 19244 11408 M 0 79 R D +19377 11408 M 0 79 R D 19511 11408 M 0 79 R D 19644 11408 M 0 79 R D +19777 11408 M 0 79 R D 19911 11408 M 0 79 R D 20177 11408 M 0 79 R D +20311 11408 M 0 79 R D 20444 11408 M 0 79 R D 11110 19296 M 9334 0 R D +12044 19296 M 0 -158 R D 13377 19296 M 0 -158 R D 14710 19296 M 0 -158 R D +16044 19296 M 0 -158 R D 17377 19296 M 0 -158 R D 18711 19296 M 0 -158 R D +20044 19296 M 0 -158 R D 11110 19296 M 0 -79 R D 11243 19296 M 0 -79 R D +11377 19296 M 0 -79 R D 11510 19296 M 0 -79 R D 11644 19296 M 0 -79 R D +11777 19296 M 0 -79 R D 11910 19296 M 0 -79 R D 12177 19296 M 0 -79 R D +12310 19296 M 0 -79 R D 12444 19296 M 0 -79 R D 12577 19296 M 0 -79 R D +12710 19296 M 0 -79 R D 12844 19296 M 0 -79 R D 12977 19296 M 0 -79 R D +13110 19296 M 0 -79 R D 13244 19296 M 0 -79 R D 13510 19296 M 0 -79 R D +13644 19296 M 0 -79 R D 13777 19296 M 0 -79 R D 13910 19296 M 0 -79 R D +14044 19296 M 0 -79 R D 14177 19296 M 0 -79 R D 14310 19296 M 0 -79 R D +14444 19296 M 0 -79 R D 14577 19296 M 0 -79 R D 14844 19296 M 0 -79 R D +14977 19296 M 0 -79 R D 15110 19296 M 0 -79 R D 15244 19296 M 0 -79 R D +15377 19296 M 0 -79 R D 15510 19296 M 0 -79 R D 15644 19296 M 0 -79 R D +15777 19296 M 0 -79 R D 15910 19296 M 0 -79 R D 16177 19296 M 0 -79 R D +16311 19296 M 0 -79 R D 16444 19296 M 0 -79 R D 16577 19296 M 0 -79 R D +16711 19296 M 0 -79 R D 16844 19296 M 0 -79 R D 16977 19296 M 0 -79 R D +17111 19296 M 0 -79 R D 17244 19296 M 0 -79 R D 17511 19296 M 0 -79 R D +17644 19296 M 0 -79 R D 17777 19296 M 0 -79 R D 17911 19296 M 0 -79 R D +18044 19296 M 0 -79 R D 18177 19296 M 0 -79 R D 18311 19296 M 0 -79 R D +18444 19296 M 0 -79 R D 18577 19296 M 0 -79 R D 18844 19296 M 0 -79 R D +18977 19296 M 0 -79 R D 19111 19296 M 0 -79 R D 19244 19296 M 0 -79 R D +19377 19296 M 0 -79 R D 19511 19296 M 0 -79 R D 19644 19296 M 0 -79 R D +19777 19296 M 0 -79 R D 19911 19296 M 0 -79 R D 20177 19296 M 0 -79 R D +20311 19296 M 0 -79 R D 20444 19296 M 0 -79 R D 11110 11408 M 0 7888 R D +11110 11408 M 187 0 R D gsave 10999 11408 translate 0 0 M -117.687 0 N +( ) show grestore 11110 13104 M 187 0 R D gsave 10999 12964 translate 0 0 M +-117.687 0 N +( ) show grestore 11110 14801 M 187 0 R D gsave 10999 14660 translate 0 0 M +-117.687 0 N +( ) show grestore 11110 16497 M 187 0 R D gsave 10999 16356 translate 0 0 M +-117.687 0 N +( ) show grestore 11110 18193 M 187 0 R D gsave 10999 18053 translate 0 0 M +-117.687 0 N +( ) show grestore 11110 11832 M 93 0 R D 11110 12256 M 93 0 R D +11110 12680 M 93 0 R D 11110 13529 M 93 0 R D 11110 13953 M 93 0 R D +11110 14377 M 93 0 R D 11110 15225 M 93 0 R D 11110 15649 M 93 0 R D +11110 16073 M 93 0 R D 11110 16921 M 93 0 R D 11110 17345 M 93 0 R D +11110 17769 M 93 0 R D 11110 18618 M 93 0 R D 11110 19042 M 93 0 R D +20444 11408 M 0 7888 R D 20444 11408 M -187 0 R D 20444 13104 M -187 0 R D +20444 14801 M -187 0 R D 20444 16497 M -187 0 R D 20444 18193 M -187 0 R D +20444 11832 M -93 0 R D 20444 12256 M -93 0 R D 20444 12680 M -93 0 R D +20444 13529 M -93 0 R D 20444 13953 M -93 0 R D 20444 14377 M -93 0 R D +20444 15225 M -93 0 R D 20444 15649 M -93 0 R D 20444 16073 M -93 0 R D +20444 16921 M -93 0 R D 20444 17345 M -93 0 R D 20444 17769 M -93 0 R D +20444 18618 M -93 0 R D 20444 19042 M -93 0 R D 12497 18805 M -1 22 R +-5 21 R -7 21 R -9 20 R -12 18 R -15 16 R -16 14 R -18 13 R -20 9 R -20 7 R +-22 4 R -21 2 R -22 -2 R -21 -4 R -21 -7 R -20 -9 R -18 -13 R -16 -14 R +-14 -16 R -13 -18 R -9 -20 R -7 -21 R -4 -21 R -2 -22 R 2 -21 R 4 -22 R +7 -20 R 9 -20 R 13 -18 R 14 -16 R 16 -15 R 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0.000 setrgbcolor +12214 18302 M 0 250 R 250 0 R 0 -250 R -250 0 R F +13061 17603 M 0 249 R 250 0 R 0 -249 R -250 0 R F +14016 17615 M 0 250 R 250 0 R 0 -250 R -250 0 R F +14837 17173 M 0 250 R 249 0 R 0 -250 R -249 0 R F +15593 16691 M 0 249 R 250 0 R 0 -249 R -250 0 R F +16363 15896 M 0 249 R 250 0 R 0 -249 R -250 0 R F +17233 15093 M 0 249 R 249 0 R 0 -249 R -249 0 R F +18381 13502 M 0 250 R 249 0 R 0 -250 R -249 0 R F +L0 12293 17596 M 93 0 R -47 0 R 0 1408 R -46 0 R 93 0 R D 13139 17151 M +94 0 R -47 0 R 0 1034 R -47 0 R 94 0 R D 14095 17477 M 93 0 R -47 0 R +0 535 R -46 0 R 93 0 R D 14915 17035 M 93 0 R -47 0 R 0 518 R -46 0 R 93 0 R +D 15671 16570 M 93 0 R -46 0 R 0 475 R -47 0 R 93 0 R D 16441 15757 M 93 0 R +-46 0 R 0 535 R -47 0 R 93 0 R D 17311 14963 M 93 0 R -47 0 R 0 509 R +-46 0 R 93 0 R D 18459 13203 M 93 0 R -47 0 R 0 797 R -46 0 R 93 0 R D L2 +11977 18146 M 67 212 R 66 61 R 67 28 R 67 13 R 66 4 R 67 0 R 67 -4 R 66 -7 R +67 -9 R 67 -11 R 66 -13 R 67 -14 R 67 -15 R 66 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66 -107 R 67 -108 R 67 -108 R 49 -82 R D +0.000 0.000 0.000 setrgbcolor gsave 11710 12256 translate 0 0 M +1.25 dup scale +( 0.2 < z < 0.4) show grestore 15 setlinewidth L0 20444 11408 M 9334 0 R D +21378 11408 M 0 158 R D gsave 21378 10880 translate 0 0 M -117.687 0 N +(9) show grestore 22711 11408 M 0 158 R D gsave 22711 10880 translate 0 0 M +-235.373 0 N +(10) show grestore 24044 11408 M 0 158 R D gsave 24044 10880 translate 0 0 M +-235.373 0 N +(11) show grestore 25378 11408 M 0 158 R D gsave 25378 10880 translate 0 0 M +-235.373 0 N +(12) show grestore 26711 11408 M 0 158 R D gsave 26711 10880 translate 0 0 M +-235.373 0 N +(13) show grestore 28045 11408 M 0 158 R D gsave 28045 10880 translate 0 0 M +-235.373 0 N +(14) show grestore 29378 11408 M 0 158 R D gsave 29378 10880 translate 0 0 M +-235.373 0 N +(15) show grestore 20444 11408 M 0 79 R D 20577 11408 M 0 79 R D +20711 11408 M 0 79 R D 20844 11408 M 0 79 R D 20978 11408 M 0 79 R D +21111 11408 M 0 79 R D 21244 11408 M 0 79 R D 21511 11408 M 0 79 R D +21644 11408 M 0 79 R D 21778 11408 M 0 79 R D 21911 11408 M 0 79 R D +22044 11408 M 0 79 R D 22178 11408 M 0 79 R D 22311 11408 M 0 79 R D +22444 11408 M 0 79 R D 22578 11408 M 0 79 R D 22844 11408 M 0 79 R D +22978 11408 M 0 79 R D 23111 11408 M 0 79 R D 23244 11408 M 0 79 R D +23378 11408 M 0 79 R D 23511 11408 M 0 79 R D 23644 11408 M 0 79 R D +23778 11408 M 0 79 R D 23911 11408 M 0 79 R D 24178 11408 M 0 79 R D +24311 11408 M 0 79 R D 24444 11408 M 0 79 R D 24578 11408 M 0 79 R D +24711 11408 M 0 79 R D 24844 11408 M 0 79 R D 24978 11408 M 0 79 R D +25111 11408 M 0 79 R D 25244 11408 M 0 79 R D 25511 11408 M 0 79 R D +25645 11408 M 0 79 R D 25778 11408 M 0 79 R D 25911 11408 M 0 79 R D +26045 11408 M 0 79 R D 26178 11408 M 0 79 R D 26311 11408 M 0 79 R D +26445 11408 M 0 79 R D 26578 11408 M 0 79 R D 26845 11408 M 0 79 R D +26978 11408 M 0 79 R D 27111 11408 M 0 79 R D 27245 11408 M 0 79 R D +27378 11408 M 0 79 R D 27511 11408 M 0 79 R D 27645 11408 M 0 79 R D +27778 11408 M 0 79 R D 27911 11408 M 0 79 R D 28178 11408 M 0 79 R D +28311 11408 M 0 79 R D 28445 11408 M 0 79 R D 28578 11408 M 0 79 R D +28711 11408 M 0 79 R D 28845 11408 M 0 79 R D 28978 11408 M 0 79 R D +29111 11408 M 0 79 R D 29245 11408 M 0 79 R D 29511 11408 M 0 79 R D +29645 11408 M 0 79 R D 29778 11408 M 0 79 R D 20444 19296 M 9334 0 R D +21378 19296 M 0 -158 R D 22711 19296 M 0 -158 R D 24044 19296 M 0 -158 R D +25378 19296 M 0 -158 R D 26711 19296 M 0 -158 R D 28045 19296 M 0 -158 R D +29378 19296 M 0 -158 R D 20444 19296 M 0 -79 R D 20577 19296 M 0 -79 R D +20711 19296 M 0 -79 R D 20844 19296 M 0 -79 R D 20978 19296 M 0 -79 R D +21111 19296 M 0 -79 R D 21244 19296 M 0 -79 R D 21511 19296 M 0 -79 R D +21644 19296 M 0 -79 R D 21778 19296 M 0 -79 R D 21911 19296 M 0 -79 R D +22044 19296 M 0 -79 R D 22178 19296 M 0 -79 R D 22311 19296 M 0 -79 R D +22444 19296 M 0 -79 R D 22578 19296 M 0 -79 R D 22844 19296 M 0 -79 R D +22978 19296 M 0 -79 R D 23111 19296 M 0 -79 R D 23244 19296 M 0 -79 R D +23378 19296 M 0 -79 R D 23511 19296 M 0 -79 R D 23644 19296 M 0 -79 R D +23778 19296 M 0 -79 R D 23911 19296 M 0 -79 R D 24178 19296 M 0 -79 R D +24311 19296 M 0 -79 R D 24444 19296 M 0 -79 R D 24578 19296 M 0 -79 R D +24711 19296 M 0 -79 R D 24844 19296 M 0 -79 R D 24978 19296 M 0 -79 R D +25111 19296 M 0 -79 R D 25244 19296 M 0 -79 R D 25511 19296 M 0 -79 R D +25645 19296 M 0 -79 R D 25778 19296 M 0 -79 R D 25911 19296 M 0 -79 R D +26045 19296 M 0 -79 R D 26178 19296 M 0 -79 R D 26311 19296 M 0 -79 R D +26445 19296 M 0 -79 R D 26578 19296 M 0 -79 R D 26845 19296 M 0 -79 R D +26978 19296 M 0 -79 R D 27111 19296 M 0 -79 R D 27245 19296 M 0 -79 R D +27378 19296 M 0 -79 R D 27511 19296 M 0 -79 R D 27645 19296 M 0 -79 R D +27778 19296 M 0 -79 R D 27911 19296 M 0 -79 R D 28178 19296 M 0 -79 R D +28311 19296 M 0 -79 R D 28445 19296 M 0 -79 R D 28578 19296 M 0 -79 R D +28711 19296 M 0 -79 R D 28845 19296 M 0 -79 R D 28978 19296 M 0 -79 R D +29111 19296 M 0 -79 R D 29245 19296 M 0 -79 R D 29511 19296 M 0 -79 R D +29645 19296 M 0 -79 R D 29778 19296 M 0 -79 R D 20444 11408 M 0 7888 R D +20444 11408 M 187 0 R D gsave 20333 11408 translate 0 0 M -117.687 0 N +( ) show grestore 20444 13104 M 187 0 R D gsave 20333 12964 translate 0 0 M +-117.687 0 N +( ) show grestore 20444 14801 M 187 0 R D gsave 20333 14660 translate 0 0 M +-117.687 0 N +( ) show grestore 20444 16497 M 187 0 R D gsave 20333 16356 translate 0 0 M +-117.687 0 N +( ) show grestore 20444 18193 M 187 0 R D gsave 20333 18053 translate 0 0 M +-117.687 0 N +( ) show grestore 20444 11832 M 93 0 R D 20444 12256 M 93 0 R D +20444 12680 M 93 0 R D 20444 13529 M 93 0 R D 20444 13953 M 93 0 R D +20444 14377 M 93 0 R D 20444 15225 M 93 0 R D 20444 15649 M 93 0 R D +20444 16073 M 93 0 R D 20444 16921 M 93 0 R D 20444 17345 M 93 0 R D +20444 17769 M 93 0 R D 20444 18618 M 93 0 R D 20444 19042 M 93 0 R D +29778 11408 M 0 7888 R D 29778 11408 M -187 0 R D 29778 13104 M -187 0 R D +29778 14801 M -187 0 R D 29778 16497 M -187 0 R D 29778 18193 M -187 0 R D +29778 11832 M -93 0 R D 29778 12256 M -93 0 R D 29778 12680 M -93 0 R D +29778 13529 M -93 0 R D 29778 13953 M -93 0 R D 29778 14377 M -93 0 R D +29778 15225 M -93 0 R D 29778 15649 M -93 0 R D 29778 16073 M -93 0 R D +29778 16921 M -93 0 R D 29778 17345 M -93 0 R D 29778 17769 M -93 0 R D +29778 18618 M -93 0 R D 29778 19042 M -93 0 R D 22826 18730 M -1 22 R +-4 21 R -7 21 R -10 19 R -12 19 R -14 16 R -17 14 R -18 12 R -19 10 R +-21 7 R -21 4 R -22 2 R -22 -2 R -21 -4 R -21 -7 R -19 -10 R -18 -12 R +-17 -14 R -14 -16 R -12 -19 R -10 -19 R -7 -21 R -4 -21 R -2 -22 R 2 -22 R +4 -21 R 7 -20 R 10 -20 R 12 -18 R 14 -17 R 17 -14 R 18 -12 R 19 -10 R +21 -7 R 21 -4 R 22 -1 R 22 1 R 21 4 R 21 7 R 19 10 R 18 12 R 17 14 R 14 17 R +12 18 R 10 20 R 7 20 R 4 21 R 1 22 R F +23878 18292 M -2 22 R -4 21 R -7 21 R -10 20 R -12 18 R -14 16 R -16 14 R +-18 12 R -20 10 R -21 7 R -21 4 R -22 2 R -21 -2 R -22 -4 R -20 -7 R +-20 -10 R -18 -12 R -16 -14 R 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21 -4 R 22 -1 R 22 1 R 21 4 R 21 7 R +19 10 R 18 12 R 17 15 R 14 16 R 12 18 R 10 20 R 7 20 R 4 22 R 1 21 R F +26212 16755 M -1 22 R -4 22 R -7 20 R -10 20 R -12 18 R -14 16 R -17 15 R +-18 12 R -19 9 R -21 7 R -21 5 R -22 1 R -22 -1 R -21 -5 R -21 -7 R -19 -9 R +-18 -12 R -17 -15 R -14 -16 R -12 -18 R -10 -20 R -7 -20 R -4 -22 R -2 -22 R +2 -21 R 4 -22 R 7 -20 R 10 -20 R 12 -18 R 14 -16 R 17 -15 R 18 -12 R 19 -9 R +21 -7 R 21 -5 R 22 -1 R 22 1 R 21 5 R 21 7 R 19 9 R 18 12 R 17 15 R 14 16 R +12 18 R 10 20 R 7 20 R 4 22 R 1 21 R F +26966 16204 M -1 22 R -5 22 R -7 20 R -9 20 R -12 18 R -15 16 R -16 15 R +-18 12 R -20 9 R -20 7 R -22 5 R -22 1 R -21 -1 R -22 -5 R -20 -7 R -20 -9 R +-18 -12 R -16 -15 R -15 -16 R -12 -18 R -9 -20 R -7 -20 R -5 -22 R -1 -22 R +1 -21 R 5 -22 R 7 -20 R 9 -20 R 12 -18 R 15 -16 R 16 -15 R 18 -12 R 20 -9 R +20 -7 R 22 -5 R 21 -1 R 22 1 R 22 5 R 20 7 R 20 9 R 18 12 R 16 15 R 15 16 R +12 18 R 9 20 R 7 20 R 5 22 R 1 21 R F +27745 14813 M -1 22 R -4 22 R -7 20 R -10 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-93 R 67 -94 R 66 -95 R 67 -95 R 67 -96 R 66 -97 R 67 -98 R D +0.000 0.965 1.000 setrgbcolor 22459 17116 M -222 -222 R 111 111 R -111 111 R +222 -222 R D 23305 17519 M -222 -222 R 111 111 R -111 111 R 222 -222 R D +24100 17451 M -222 -222 R 111 111 R -111 111 R 222 -222 R D 24995 17450 M +-222 -222 R 111 111 R -111 111 R 222 -222 R D 22301 16157 M 94 0 R -47 0 R +0 1696 R -47 0 R 94 0 R D 23147 17196 M 94 0 R -47 0 R 0 424 R -47 0 R +94 0 R D 23942 17170 M 94 0 R -47 0 R 0 340 R -47 0 R 94 0 R D 24837 17211 M +93 0 R -46 0 R 0 255 R -47 0 R 93 0 R D L3 20444 15364 M 67 68 R 66 67 R +67 66 R 67 65 R 67 65 R 66 63 R 67 63 R 67 62 R 66 61 R 67 60 R 67 59 R +66 58 R 67 57 R 67 57 R 66 55 R 67 55 R 67 53 R 66 53 R 67 52 R 67 51 R +66 51 R 67 49 R 67 48 R 66 48 R 67 46 R 67 46 R 66 45 R 67 44 R 67 43 R +66 42 R 67 41 R 67 41 R 66 39 R 67 39 R 67 38 R 66 37 R 67 36 R 67 35 R +66 34 R 67 33 R 67 33 R 66 31 R 67 20 R 67 12 R 66 5 R 67 0 R 67 -5 R +66 -8 R 67 -11 R 67 -14 R 66 -15 R 67 -18 R 67 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0 250 R 250 0 R 0 -250 R -250 0 R F +25611 16286 M 0 250 R 249 0 R 0 -250 R -249 0 R F +26742 15219 M 0 250 R 250 0 R 0 -250 R -250 0 R F +27803 13909 M 0 249 R 250 0 R 0 -249 R -250 0 R F +28880 12466 M 0 249 R 250 0 R 0 -249 R -250 0 R F +L0 22473 18194 M 94 0 R -47 0 R 0 339 R -47 0 R 94 0 R D 23307 17343 M +94 0 R -47 0 R 0 746 R -47 0 R 94 0 R D 23960 17437 M 93 0 R -47 0 R 0 543 R +-46 0 R 93 0 R D 24666 17056 M 94 0 R -47 0 R 0 484 R -47 0 R 94 0 R D +25689 16165 M 93 0 R -46 0 R 0 492 R -47 0 R 93 0 R D 26820 15072 M 94 0 R +-47 0 R 0 543 R -47 0 R 94 0 R D 27881 13660 M 93 0 R -46 0 R 0 721 R +-47 0 R 93 0 R D 28959 11759 M 93 0 R -47 0 R 0 1425 R -46 0 R 93 0 R D L2 +22044 17454 M 67 760 R 67 85 R 66 34 R 67 16 R 67 5 R 66 0 R 67 -5 R 67 -8 R +66 -11 R 67 -12 R 67 -15 R 66 -15 R 67 -17 R 67 -19 R 66 -19 R 67 -21 R +67 -21 R 66 -22 R 67 -24 R 67 -24 R 66 -25 R 67 -26 R 67 -27 R 66 -28 R +67 -28 R 67 -29 R 66 -30 R 67 -31 R 67 -32 R 66 -32 R 67 -33 R 67 -34 R +66 -35 R 67 -36 R 67 -36 R 66 -37 R 67 -38 R 67 -38 R 66 -40 R 67 -40 R +67 -41 R 66 -42 R 67 -42 R 67 -44 R 66 -44 R 67 -45 R 67 -45 R 66 -47 R +67 -47 R 67 -48 R 67 -49 R 66 -50 R 67 -50 R 67 -52 R 66 -52 R 67 -52 R +67 -54 R 66 -55 R 67 -55 R 67 -56 R 66 -57 R 67 -58 R 67 -58 R 66 -60 R +67 -60 R 67 -61 R 66 -62 R 67 -62 R 67 -64 R 66 -64 R 67 -65 R 67 -66 R +66 -67 R 67 -68 R 67 -68 R 66 -70 R 67 -70 R 67 -71 R 66 -71 R 67 -73 R +67 -74 R 66 -74 R 67 -75 R 67 -76 R 66 -77 R 67 -78 R 67 -78 R 66 -80 R +67 -80 R 67 -81 R 66 -82 R 67 -83 R 67 -84 R 66 -85 R 67 -85 R 67 -86 R +66 -87 R 67 -88 R 67 -89 R 66 -90 R 67 -91 R 67 -91 R 66 -93 R 67 -93 R +67 -94 R 66 -95 R 67 -96 R 67 -96 R 66 -98 R 67 -98 R 67 -100 R 66 -100 R +67 -101 R 67 -102 R 66 -103 R 67 -104 R D L0 0.000 0.282 1.000 setrgbcolor +24160 17318 M 125 -125 R -125 -125 R -124 125 R 124 125 R D 24403 17290 M +125 -125 R -125 -125 R -125 125 R 125 125 R D 24647 17270 M 125 -124 R +-125 -125 R -125 125 R 125 124 R D 24893 17217 M 125 -125 R 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0.000 setrgbcolor gsave 21044 12256 translate 0 0 M +1.25 dup scale +( 0.4 < z < 0.8) show grestore 15 setlinewidth L0 5100 2000 M 9900 0 R D +6255 2000 M 0 160 R D gsave 6255 1472 translate 0 0 M -235.373 0 N +(11) show grestore 7905 2000 M 0 160 R D gsave 7905 1472 translate 0 0 M +-235.373 0 N +(12) show grestore 9555 2000 M 0 160 R D gsave 9555 1472 translate 0 0 M +-235.373 0 N +(13) show grestore 11205 2000 M 0 160 R D gsave 11205 1472 translate 0 0 M +-235.373 0 N +(14) show grestore 12855 2000 M 0 160 R D gsave 12855 1472 translate 0 0 M +-235.373 0 N +(15) show grestore 14505 2000 M 0 160 R D gsave 14505 1472 translate 0 0 M +-235.373 0 N +(16) show grestore 5100 2000 M 0 80 R D 5265 2000 M 0 80 R D 5430 2000 M +0 80 R D 5595 2000 M 0 80 R D 5760 2000 M 0 80 R D 5925 2000 M 0 80 R D +6090 2000 M 0 80 R D 6420 2000 M 0 80 R D 6585 2000 M 0 80 R D 6750 2000 M +0 80 R D 6915 2000 M 0 80 R D 7080 2000 M 0 80 R D 7245 2000 M 0 80 R D +7410 2000 M 0 80 R D 7575 2000 M 0 80 R D 7740 2000 M 0 80 R D 8070 2000 M +0 80 R D 8235 2000 M 0 80 R D 8400 2000 M 0 80 R D 8565 2000 M 0 80 R D +8730 2000 M 0 80 R D 8895 2000 M 0 80 R D 9060 2000 M 0 80 R D 9225 2000 M +0 80 R D 9390 2000 M 0 80 R D 9720 2000 M 0 80 R D 9885 2000 M 0 80 R D +10050 2000 M 0 80 R D 10215 2000 M 0 80 R D 10380 2000 M 0 80 R D +10545 2000 M 0 80 R D 10710 2000 M 0 80 R D 10875 2000 M 0 80 R D +11040 2000 M 0 80 R D 11370 2000 M 0 80 R D 11535 2000 M 0 80 R D +11700 2000 M 0 80 R D 11865 2000 M 0 80 R D 12030 2000 M 0 80 R D +12195 2000 M 0 80 R D 12360 2000 M 0 80 R D 12525 2000 M 0 80 R D +12690 2000 M 0 80 R D 13020 2000 M 0 80 R D 13185 2000 M 0 80 R D +13350 2000 M 0 80 R D 13515 2000 M 0 80 R D 13680 2000 M 0 80 R D +13845 2000 M 0 80 R D 14010 2000 M 0 80 R D 14175 2000 M 0 80 R D +14340 2000 M 0 80 R D 14670 2000 M 0 80 R D 14835 2000 M 0 80 R D +15000 2000 M 0 80 R D 5100 10000 M 9900 0 R D 6255 10000 M 0 -160 R D +7905 10000 M 0 -160 R D 9555 10000 M 0 -160 R D 11205 10000 M 0 -160 R D +12855 10000 M 0 -160 R D 14505 10000 M 0 -160 R D 5100 10000 M 0 -80 R D +5265 10000 M 0 -80 R D 5430 10000 M 0 -80 R D 5595 10000 M 0 -80 R D +5760 10000 M 0 -80 R D 5925 10000 M 0 -80 R D 6090 10000 M 0 -80 R D +6420 10000 M 0 -80 R D 6585 10000 M 0 -80 R D 6750 10000 M 0 -80 R D +6915 10000 M 0 -80 R D 7080 10000 M 0 -80 R D 7245 10000 M 0 -80 R D +7410 10000 M 0 -80 R D 7575 10000 M 0 -80 R D 7740 10000 M 0 -80 R D +8070 10000 M 0 -80 R D 8235 10000 M 0 -80 R D 8400 10000 M 0 -80 R D +8565 10000 M 0 -80 R D 8730 10000 M 0 -80 R D 8895 10000 M 0 -80 R D +9060 10000 M 0 -80 R D 9225 10000 M 0 -80 R D 9390 10000 M 0 -80 R D +9720 10000 M 0 -80 R D 9885 10000 M 0 -80 R D 10050 10000 M 0 -80 R D +10215 10000 M 0 -80 R D 10380 10000 M 0 -80 R D 10545 10000 M 0 -80 R D +10710 10000 M 0 -80 R D 10875 10000 M 0 -80 R D 11040 10000 M 0 -80 R D +11370 10000 M 0 -80 R D 11535 10000 M 0 -80 R D 11700 10000 M 0 -80 R D +11865 10000 M 0 -80 R D 12030 10000 M 0 -80 R D 12195 10000 M 0 -80 R D +12360 10000 M 0 -80 R D 12525 10000 M 0 -80 R D 12690 10000 M 0 -80 R D +13020 10000 M 0 -80 R D 13185 10000 M 0 -80 R D 13350 10000 M 0 -80 R D +13515 10000 M 0 -80 R D 13680 10000 M 0 -80 R D 13845 10000 M 0 -80 R D +14010 10000 M 0 -80 R D 14175 10000 M 0 -80 R D 14340 10000 M 0 -80 R D +14670 10000 M 0 -80 R D 14835 10000 M 0 -80 R D 15000 10000 M 0 -80 R D +5100 2000 M 0 8000 R D 5100 2000 M 198 0 R D gsave 4989 2000 translate 0 0 M +-611.717 0 N +(-12) show grestore 5100 3720 M 198 0 R D gsave 4989 3580 translate 0 0 M +-611.717 0 N +(-10) show grestore 5100 5441 M 198 0 R D gsave 4989 5300 translate 0 0 M +-376.343 0 N +(-8) show grestore 5100 7161 M 198 0 R D gsave 4989 7020 translate 0 0 M +-376.343 0 N +(-6) show grestore 5100 8882 M 198 0 R D gsave 4989 8741 translate 0 0 M +-376.343 0 N +(-4) show grestore 5100 2430 M 99 0 R D 5100 2860 M 99 0 R D 5100 3290 M +99 0 R D 5100 4151 M 99 0 R D 5100 4581 M 99 0 R D 5100 5011 M 99 0 R D +5100 5871 M 99 0 R D 5100 6301 M 99 0 R D 5100 6731 M 99 0 R D 5100 7591 M +99 0 R D 5100 8022 M 99 0 R D 5100 8452 M 99 0 R D 5100 9312 M 99 0 R D +5100 9742 M 99 0 R D 15000 2000 M 0 8000 R D 15000 2000 M -198 0 R D +15000 3720 M -198 0 R D 15000 5441 M -198 0 R D 15000 7161 M -198 0 R D +15000 8882 M -198 0 R D 15000 2430 M -99 0 R D 15000 2860 M -99 0 R D +15000 3290 M -99 0 R D 15000 4151 M -99 0 R D 15000 4581 M -99 0 R D +15000 5011 M -99 0 R D 15000 5871 M -99 0 R D 15000 6301 M -99 0 R D +15000 6731 M -99 0 R D 15000 7591 M -99 0 R D 15000 8022 M -99 0 R D +15000 8452 M -99 0 R D 15000 9312 M -99 0 R D 15000 9742 M -99 0 R D +6342 8895 M -1 22 R -5 21 R -7 21 R -9 19 R -12 19 R -15 16 R -16 14 R +-18 12 R -20 10 R -20 7 R -22 4 R -22 2 R -21 -2 R -22 -4 R -20 -7 R +-20 -10 R -18 -12 R -16 -14 R -15 -16 R -12 -19 R -9 -19 R -7 -21 R -5 -21 R +-1 -22 R 1 -22 R 5 -21 R 7 -21 R 9 -19 R 12 -18 R 15 -17 R 16 -14 R 18 -12 R +20 -10 R 20 -7 R 22 -4 R 21 -1 R 22 1 R 22 4 R 20 7 R 20 10 R 18 12 R +16 14 R 15 17 R 12 18 R 9 19 R 7 21 R 5 21 R 1 22 R F +7293 8678 M -2 21 R -4 22 R -7 20 R -10 20 R -12 18 R -14 16 R -17 15 R +-18 12 R -19 10 R -21 7 R -21 4 R -22 1 R -22 -1 R -21 -4 R -21 -7 R +-19 -10 R -18 -12 R -17 -15 R -14 -16 R -12 -18 R -10 -20 R -7 -20 R +-4 -22 R -1 -21 R 1 -22 R 4 -21 R 7 -21 R 10 -20 R 12 -18 R 14 -16 R +17 -14 R 18 -13 R 19 -9 R 21 -7 R 21 -4 R 22 -2 R 22 2 R 21 4 R 21 7 R +19 9 R 18 13 R 17 14 R 14 16 R 12 18 R 10 20 R 7 21 R 4 21 R 2 22 R F +8046 8392 M -1 22 R -5 21 R -7 21 R -9 20 R -12 18 R -15 16 R -16 14 R +-18 12 R -20 10 R -20 7 R -22 4 R -22 2 R -21 -2 R -22 -4 R -20 -7 R +-20 -10 R -18 -12 R -16 -14 R -15 -16 R -12 -18 R -9 -20 R -7 -21 R -5 -21 R +-1 -22 R 1 -21 R 5 -22 R 7 -20 R 9 -20 R 12 -18 R 15 -16 R 16 -15 R 18 -12 R +20 -10 R 20 -7 R 22 -4 R 21 -1 R 22 1 R 22 4 R 20 7 R 20 10 R 18 12 R +16 15 R 15 16 R 12 18 R 9 20 R 7 20 R 5 22 R 1 21 R F +9252 7789 M -1 21 R -4 22 R -7 20 R -10 20 R -12 18 R -15 16 R -16 15 R +-18 12 R -20 9 R -20 7 R -22 5 R -21 1 R -22 -1 R -21 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R 16 -14 R 18 -12 R +20 -10 R 20 -7 R 22 -4 R 21 -2 R 22 2 R 21 4 R 21 7 R 20 10 R 18 12 R +16 14 R 14 16 R 13 19 R 9 19 R 7 21 R 4 21 R 2 22 R F +20 setlinewidth 6126 8723 M 99 0 R -50 0 R 0 344 R -49 0 R 99 0 R D +7077 8506 M 99 0 R -50 0 R 0 344 R -49 0 R 99 0 R D 7830 8220 M 99 0 R +-50 0 R 0 344 R -49 0 R 99 0 R D 9036 7605 M 99 0 R -49 0 R 0 368 R -50 0 R +99 0 R D 10264 6461 M 99 0 R -49 0 R 0 430 R -50 0 R 99 0 R D 11437 5065 M +99 0 R -50 0 R 0 516 R -49 0 R 99 0 R D 5100 9270 M 82 -18 R 83 -20 R +82 -19 R 83 -21 R 82 -20 R 83 -22 R 82 -22 R 83 -23 R 82 -23 R 83 -24 R +83 -24 R 82 -25 R 82 -26 R 83 -27 R 83 -27 R 82 -27 R 83 -29 R 82 -29 R +82 -29 R 83 -31 R 82 -31 R 83 -31 R 83 -33 R 82 -33 R 83 -34 R 82 -34 R +83 -35 R 82 -36 R 82 -37 R 83 -37 R 82 -38 R 83 -38 R 83 -40 R 82 -40 R +83 -41 R 82 -41 R 83 -43 R 82 -43 R 83 -43 R 82 -45 R 82 -45 R 83 -46 R +83 -47 R 82 -47 R 83 -49 R 82 -49 R 83 -49 R 82 -51 R 83 -51 R 82 -52 R +83 -53 R 82 -54 R 83 -54 R 82 -55 R 83 -56 R 82 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R 0 689 R -49 0 R 99 0 R D 8278 7308 M 99 0 R +-50 0 R 0 1032 R -49 0 R 99 0 R D L3 5100 8069 M 82 40 R 83 40 R 82 28 R +83 19 R 82 12 R 83 6 R 82 2 R 83 -1 R 82 -4 R 83 -7 R 83 -8 R 82 -11 R +82 -11 R 83 -13 R 83 -14 R 82 -15 R 83 -16 R 82 -17 R 82 -18 R 83 -19 R +82 -20 R 83 -20 R 83 -21 R 82 -23 R 83 -23 R 82 -24 R 83 -25 R 82 -26 R +82 -27 R 83 -27 R 82 -29 R 83 -29 R 83 -30 R 82 -32 R 83 -32 R 82 -33 R +83 -33 R 82 -35 R 83 -36 R 82 -36 R 82 -38 R 83 -38 R 83 -39 R 82 -40 R +83 -41 R 82 -42 R 83 -43 R 82 -43 R 83 -45 R 82 -45 R 83 -46 R 82 -47 R +83 -48 R 82 -49 R 83 -50 R 82 -51 R 83 -51 R 82 -53 R 83 -53 R 82 -54 R +83 -55 R 82 -56 R 83 -57 R 82 -58 R 83 -59 R 82 -59 R 83 -60 R 82 -62 R +83 -62 R 82 -63 R 83 -64 R 82 -65 R 83 -65 R 82 -67 R 83 -67 R 82 -69 R +83 -69 R 82 -70 R 83 -71 R 82 -72 R 83 -72 R 82 -74 R 83 -74 R 82 -76 R +83 -76 R 82 -77 R 83 -78 R 82 -79 R 83 -80 R 82 -80 R 83 -82 R 82 -82 R +83 -83 R 82 -84 R 83 -85 R 82 -86 R 83 -87 R 82 -88 R 83 -88 R 82 -90 R +83 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-125 -125 R -125 125 R +125 124 R D 7305 7915 M 125 -124 R -125 -125 R -125 125 R 125 124 R D +7612 7836 M 125 -125 R -125 -125 R -125 125 R 125 125 R D 7920 7807 M +125 -124 R -125 -125 R -124 125 R 124 124 R D 8231 7754 M 125 -125 R +-125 -125 R -125 125 R 125 125 R D 8543 7726 M 125 -125 R -125 -125 R +-125 125 R 125 125 R D 8856 7595 M 125 -125 R -125 -125 R -125 125 R +125 125 R D 9171 7361 M 125 -125 R -125 -125 R -125 125 R 125 125 R D +9488 7067 M 125 -125 R -125 -125 R -125 125 R 125 125 R D 9805 6790 M +125 -124 R -125 -125 R -124 125 R 124 124 R D 10124 6411 M 125 -125 R +-125 -125 R -125 125 R 125 125 R D 10444 5644 M 125 -125 R -125 -125 R +-125 125 R 125 125 R D 10764 5609 M 125 -125 R -125 -125 R -125 125 R +125 125 R D 6951 7354 M 99 0 R -49 0 R 0 1213 R -50 0 R 99 0 R D 7256 7507 M +99 0 R -50 0 R 0 567 R -49 0 R 99 0 R D 7562 7435 M 99 0 R -49 0 R 0 551 R +-50 0 R 99 0 R D 7871 7407 M 99 0 R -50 0 R 0 551 R -49 0 R 99 0 R D +8181 7354 M 99 0 R -49 0 R 0 550 R -50 0 R 99 0 R D 8493 7334 M 99 0 R +-49 0 R 0 534 R -50 0 R 99 0 R D 8807 7195 M 99 0 R -50 0 R 0 550 R -49 0 R +99 0 R D 9122 6952 M 99 0 R -50 0 R 0 568 R -49 0 R 99 0 R D 9438 6650 M +99 0 R -49 0 R 0 585 R -50 0 R 99 0 R D 9756 6347 M 99 0 R -50 0 R 0 620 R +-49 0 R 99 0 R D 10075 5907 M 99 0 R -50 0 R 0 740 R -49 0 R 99 0 R D +10394 4874 M 99 0 R -49 0 R 0 1213 R -50 0 R 99 0 R D 10715 4839 M 99 0 R +-50 0 R 0 1213 R -49 0 R 99 0 R D L1 6585 7722 M 82 230 R 83 74 R 82 31 R +83 10 R 83 -2 R 82 -9 R 83 -15 R 82 -19 R 83 -23 R 82 -26 R 82 -28 R +83 -30 R 82 -32 R 83 -34 R 83 -35 R 82 -37 R 83 -38 R 82 -39 R 83 -41 R +82 -41 R 83 -43 R 82 -44 R 82 -45 R 83 -46 R 83 -47 R 82 -49 R 83 -49 R +82 -50 R 83 -51 R 82 -52 R 83 -53 R 82 -54 R 83 -55 R 82 -55 R 83 -57 R +82 -58 R 83 -58 R 82 -59 R 83 -61 R 82 -61 R 83 -62 R 82 -63 R 83 -64 R +82 -65 R 83 -65 R 82 -67 R 83 -67 R 82 -69 R 83 -69 R 82 -70 R 83 -71 R +82 -72 R 83 -73 R 82 -73 R 83 -75 R 82 -75 R 83 -77 R 82 -77 R 83 -78 R +82 -79 R 83 -80 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08/10/05 (referee report) + +\newcommand{\tq}{$t_{Q}$} +\newcommand{\tQ}{t_{Q}} +\newcommand{\etal}{et al.} +\newcommand{\NH}{$N_{\rm H}$} +\newcommand{\NHI}{$N_{\rm H\,I}$} +\newcommand{\nh}{N_{\rm H}} +\newcommand{\nhi}{N_{\rm H\,I}} +\newcommand{\Mdot}{\dot{M}} +\newcommand{\Lbol}{L_{\rm bol}} +\newcommand{\dEdt}{\epsilon_r \Mdot c^{2}} +%\newcommand{\LB}{\nu_{B} L_{\nu_{B}}} +\newcommand{\LB}{L_{B}} +\newcommand{\LX}{L_{X}} +\newcommand{\Lm}{L_{\rm min}} +\newcommand{\LBo}{L_{B,{\rm obs}}} +\newcommand{\LBm}{L_{B,{\rm min}}} +\newcommand{\LXo}{L_{X,{\rm obs}}} +\newcommand{\LXm}{L_{X,{\rm min}}} +\newcommand{\Lcut}[1]{10^{#1}\,L_{\sun}} +\newcommand{\EV}[1]{\langle #1 \rangle} +\newcommand{\dlgL}{{\rm d}\log(L)} +\newcommand{\eEdd}{l} +%\newcommand{\nLP}{n(L_{peak})} +\newcommand{\Lp}{L_{\rm peak}} +\newcommand{\mdot}{\dot{m}} +\newcommand{\meanNH}{\bar{N}_{H}} +\newcommand{\sigNH}{\sigma_{N_{H}}} +\newcommand{\dtdL}{{\rm d}t/{\rm d}\log{L}} +\newcommand{\fdtdL}{\frac{{\rm d}t}{{\rm d}\log{L}}} +\newcommand{\ndot}{\dot{n_{\ast}(\Lp)}} +\newcommand{\vvir}{V_{\rm vir}} +\newcommand{\mvir}{M_{\rm vir}} +\newcommand{\qeos}{q_{\rm EOS}} +\newcommand{\fgas}{f_{\rm gas}} +\newcommand{\zgal}{z_{\rm gal}} +\newcommand{\mbh}{M_{\rm BH}} +\newcommand{\mbhf}{M^{f}_{\rm BH}} +\newcommand{\dphi}{{\rm d}\Phi/{\rm d}\log L} +\newcommand{\fdphi}{\frac{{\rm d}\Phi}{{\rm d}\log L}} +\newcommand{\nLP}{\dot{n}(\Lp)} +\newcommand{\nLp}{\nLP} +\newcommand{\nstar}{\dot{n}_{\ast}} +\newcommand{\lstar}{L_{\ast}} +\newcommand{\sstar}{\sigma_{\ast}} +\newcommand{\rhobh}{\rho_{\rm BH}} +\newcommand{\lessim}{\lesssim} +\newcommand{\reducechi}{\chi^{2}/\nu} + +%\renewcommand{\plotone}{ } + +\shorttitle{Quasar Origins \&\ Evolution} +\shortauthors{Hopkins \etal} +\slugcomment{Submitted to ApJ, June 14, 2005} +\begin{document} + +\title{A Unified, Merger-Driven Model for the Origin of Starbursts, Quasars, +the Cosmic X-Ray Background, Supermassive Black Holes and Galaxy Spheroids} +% Relation Between Supermassive Black Holes and Spheroids in Galaxies} +\author{Philip F. Hopkins\altaffilmark{1}, +Lars Hernquist\altaffilmark{1}, +Thomas J. Cox\altaffilmark{1}, +Tiziana Di Matteo\altaffilmark{2}, +Brant Robertson\altaffilmark{1}, +Volker Springel\altaffilmark{3}} +\altaffiltext{1}{Harvard-Smithsonian Center for Astrophysics, +60 Garden Street, Cambridge, MA 02138, USA} +\altaffiltext{2}{Carnegie Mellon University, +Department of Physics, 5000 Forbes Ave., Pittsburgh, PA 15213} +\altaffiltext{3}{Max-Planck-Institut f\"{u}r Astrophysik, +Karl-Schwarzchild-Stra\ss e 1, 85740 Garching bei M\"{u}nchen, Germany} + +\begin{abstract} + +We develop an evolutionary model for starbursts, quasars, and +spheroidal galaxies in which supermassive black holes play a dominant +role. In this picture, mergers between gas-rich galaxies drive +nuclear inflows of gas, producing intense starbursts and feeding the +growth of supermassive black holes. During this phase, the black hole +is heavily obscured (a ``buried'' quasar), but feedback energy from +its growth expels the gas, rendering the black hole briefly visible as +a bright, optical source (a ``visible'' quasar), and eventually +halting accretion (a ``dead'' quasar). The self-regulated growth of +the black hole accounts for the observed correlation between black +hole mass and stellar velocity dispersion in spheroidal galaxies. We +show that the quasar lifetime and obscuring column density depend on +both the instantaneous and peak luminosities of the quasar, and +determine this dependence using a large set of simulations of galaxy +mergers varying the host galaxy properties, orbital geometry, and gas +physics. + +We use our fits to the lifetime and column density to deconvolve +observed quasar luminosity functions and obtain the evolution of the +formation rate of quasars with a certain peak luminosity, $\dot +n(L_{\rm peak}, z)$. In our model, quasars spend extended periods of +time at luminosities well below their peaks, and so $\dot n(L_{\rm +peak}, z)$ has a maximum, falling off at both brighter and fainter +luminosities, corresponding to the ``break'' in the observed quasar +luminosity function. We obtain self-consistent fits to hard and soft +X-ray and optical quasar luminosity functions for a model in which +$\dot n(L_{\rm peak}, z)$ varies with redshift according to pure peak +luminosity evolution. From this form for $\dot n(L_{\rm peak}, z)$, +and our simulation results for the luminosity dependence of the quasar +lifetime and obscuring column, we are able to reproduce many +observable quantities, including: the column density distribution of +both optical and X-ray selected quasar samples, the luminosity +function of broad-line quasars in X-ray samples and the broad-line +(Type I, Type II) fraction as a function of luminosity, the mass +function of active black holes, the observed distribution of Eddington +ratios at both low and high redshift, the present-day mass function of +relic, inactive supermassive black holes and total black hole mass +density, and the spectrum of the cosmic X-ray background. In each +case, our predictions agree well with observations, matching them to +higher precision than previous tunable models for quasar lifetimes and +obscuration similarly fit to the luminosity function. We provide a +library of Monte Carlo realizations of our modeling for comparison +with a wide range of observations, using various selection criteria. + +\end{abstract} + +\keywords{quasars: general --- galaxies: nuclei --- galaxies: active --- +galaxies: evolution --- cosmology: theory} + +\section{Introduction} +\label{sec:intro} + +The measurement of anisotropies in the cosmic microwave background +(e.g.\ Spergel et al.\ 2003) combined with observations of high +redshift supernovae (e.g.\ Riess et al.\ 1998, 2000; Perlmutter et +al.\ 1999) have established a ``standard model'' for the Universe, in +which the energy density is dominated by an unknown form driving +accelerated cosmic expansion, and most of the mass is non-baryonic, in +a ratio of roughly 5:1 to ordinary matter. On small scales, it is +believed that structure formed through gravitational instability. In +the currently favored cold dark matter (CDM) paradigm, objects grow +hierarchically, with smaller ones forming first and then merging into +successively larger bodies. As baryons fall into dark matter +potential wells, the gas is shocked and then cools radiatively to form +stars and galaxies, in a ``bottom-up'' progression (White \& Rees +1978). + +Even with the many successes of this picture, the processes underlying +galaxy formation and evolution are poorly understood. For example, +there has yet to be an ab initio calculation, starting from an initial +state prescribed by the standard model, resulting in a population of +objects that reproduces observed galaxies. However, from the +same initial conditions, computer simulations have yielded a new, +successful interpretation of the Lyman-alpha forest in which +absorption in caused by density fluctuations in the intergalactic +medium (e.g.\ Cen et al.\ 1994; Zhang et al.\ 1995; Hernquist et +al.\ 1996), over many orders of magnitude in column density (e.g.\ Katz +et al.\ 1996a), explicitly related to growth of structure in a CDM +universe (e.g.\ Croft et al.\ 1998, 1999, 2002; McDonald et al.\ 2000, +2004; Hui et al.\ 2001; Viel et al.\ 2003, 2004). This suggests that +the difficulties with understanding galaxy formation and evolution lie +not in the initial conditions or with the description of dark matter, +but rather with the physics that has been used to model the baryons. + +Observations have revealed regularities in the structure of galaxies +that point to some of this ``missing'' physics. Supermassive black +holes appear to reside at the centers of most galaxies (e.g.\ Kormendy +\& Richstone 1995; Richstone et al.\ 1998; Kormendy \& Gebhardt 2001) +and the masses of these black holes are correlated with either the +mass (Magorrian et al.\ 1998; McLure \& Dunlop 2002; Marconi \& Hunt +2003) or the velocity dispersion (i.e.\ the $M_{\rm BH}$-$\sigma$ +relation: Ferrarese \& Merritt 2000; Gebhardt et al.\ 2000; Tremaine et +al.\ 2002) of spheroids, demonstrating a direct link between the origin +of galaxies and supermassive black holes. Simulations which follow +the self-regulated growth of black holes in galaxy mergers (Di Matteo +et al.\ 2005; Springel et al.\ 2005a) have shown that the energy +released through this process has a global impact on the structure of +the merger remnant. If this conclusion applies to spheroid formation +in general, the simulations demonstrate that models for the origin and +evolution of galaxies must account for black hole growth and feedback +in a fully {\it self-consistent} manner. + +Analytical and semi-analytical +modeling \citep{SR98,Fabian99,WL02,WL03,BN05} suggests +that, beyond a certain threshold, feedback energy from black holes can +expel gas from the centers of galaxies, shutting down accretion onto +them and limiting their masses. However, these calculations usually +ignore the impact of this process on star formation and therefore do +not explain the link between black hole growth and spheroid formation, +and furthermore make simplifying assumptions about the dynamics of such accretion. For +example, the duration of black hole growth is a free parameter, which +is fixed either using observational estimates or assumed to be similar +to e.g.\ the dynamical time of the host galaxy or the $e$-folding time +for Eddington-limited black hole growth $t_{S}=M_{\rm +BH}/\Mdot=4.5\times10^{7}\,l^{-1}\,(\epsilon_r/0.1)\,$yr for accretion +with radiative efficiency $\epsilon_r=L/\Mdot c^{2}\sim0.1$ and +$l=L/L_{\rm Edd}\lesssim1$ \citep{Salpeter64}. Moreover, these +studies have adopted idealized models for quasar light curves, usually +corresponding to growth at a constant Eddington ratio or +on-off, ``light bulb,'' scenarios. As we discuss below, less +restrictive modeling suggests that this phase is actually more +complex. + +Efforts to model quasar accretion and feedback more self-consistently +\citep[e.g.,][]{CO97,CO01,Granato04} by treating the hydrodynamical +response of gas to black hole growth have generally been restricted to +idealized geometries, such as spherical symmetry, employing simple +models for star formation and galaxy-scale quasar fueling. However, +these works have made it possible to estimate duty cycles of quasars +and shown that the objects left behind have characteristics similar to +those observed, with quasar feedback being a critical element in +reproducing these features (e.g.\ Sazonov et al.\ 2005; Kawata \& +Gibson 2005; Cirasuolo et al.\ 2005; for a review, see Ostriker \& +Ciotti 2005). + +\citet{SDH05b} have incorporated black hole growth and feedback into +simulations of galaxy mergers and included a multiphase model for star +formation and pressurization of the interstellar gas by supernovae +\citep{SH03} to examine implications of these processes for galaxy +formation and evolution. Di Matteo et al.\ (2005) and Springel et +al.\ (2005a,b) have shown that gas inflows excited by gravitational +torques during a merger both trigger starbursts and fuel rapid black +hole growth. The growth of the black hole is determined by the gas +supply and terminates as gas is expelled by feedback, halting +accretion, leaving a dead quasar in an ordinary galaxy. The +self-regulated nature of black hole growth in mergers explains +observed correlations between black hole mass and properties of normal +galaxies \citep{DSH05}, as well as the color distribution of +ellipticals \citep{SDH05a}. These results lend support to the view +that mergers have played an important role in structuring galaxies, as +advocated especially by Toomre \& Toomre (1972) and Toomre (1977). +(For reviews, see, e.g., Barnes \& Hernquist 1992; Barnes 1998; +Schweizer 1998.) + +Subsequent analysis by Hopkins et al.\ (2005a,b,c,d) has shown that the +merger simulations can account for quasar phenomena as a phase of +black hole growth. Unlike what has been assumed in e.g.\ +semi-analytical studies of quasars, the simulations predict +complicated evolution for quasar lifetimes, fueling rates for black +hole accretion, obscuration, and quasar light curves. The light +curves were studied by \citet{H05a,H05b}, who showed that the +self-termination process gives observable lifetimes $\sim10^{7}\,$yr +for bright optical quasars and predicts a large population of obscured +sources as a natural stage of quasar evolution, as implied by +observations (for a review, see Brandt \& Hasinger 2005). +\citet{H05b} analyzed simulations over a range of galaxy masses and +found that the quasar light curves and lifetimes are always +qualitatively similar, with both the intrinsic and observed quasar +lifetimes being decreasing functions of luminosity, with longer +lifetimes at all luminosities for higher-mass (higher peak luminosity) +systems. The dependence of the lifetime on luminosity led +\citet{H05c} to suggest a new interpretation of the quasar luminosity +function, in which the steep bright-end consists of quasars radiating +near the Eddington limit and is directly related to the distribution +of intrinsic peak luminosities (or final black hole masses) as has +been assumed previously +\citep[e.g.,][]{SB92,HL98,HM00,KH00,Somerville01, +Tully02,WL03,V03,HQB04,Croton05}, but where the +shallow, faint-end of the luminosity function describes black holes +growing towards or declining from peak phases of quasar activity, with +Eddington ratios generally between $l \sim0.01$ and 1. The ``break'' +in the luminosity function corresponds directly to the {\em peak} in +the distribution of intrinsic quasar properties. As argued by +\citet{H05c,H05d} this new interpretation of the luminosity function +can self-consistently explain various properties of both the quasar +and galaxy populations, connecting the origin of galaxy spheroids, +supermassive black holes, and quasars. + +%\clearpage +\begin{figure} + \centering + \plotone{f1.ps} + %\includegraphics[width=3.7in]{f1.ps} + \caption{Schematic representation of a ``cosmic cycle'' for + galaxy formation and evolution regulated by black hole growth in + mergers. + \label{fig:cosmiccycle}} +\end{figure} +%\clearpage + +Motivated by these results, and earlier work by many others which we +summarize below, in this paper we consider a picture for galaxy +formation and evolution, illustrated schematically as a ``cosmic +cycle'' in Figure~\ref{fig:cosmiccycle}, in which starbursts, quasars, +and the simultaneous formation of spheroids and supermassive black +holes represent connected phases in the lives of galaxies. Mergers +are expected to occur regularly in a hierarchical universe, +particularly at high redshifts. Those between gas-rich galaxies drive +nuclear inflows of gas, triggering starbursts and fueling the growth +of supermassive black holes. During most of this phase, quasar +activity is obscured, but once a black hole dominates the energetics +of the central region, feedback expels gas and dust, making the black +hole visible briefly as a bright quasar. Eventually, as the gas is +further heated and expelled, quasar activity can no longer be +maintained and the merger remnant relaxes to a normal galaxy with a +spheroid and a supermassive black hole. In some cases, depending on +the gas content of the progenitors, the remnant may also have a disk +(Springel \& Hernquist 2005; Robertson et al.\ 2005a). The remnant +will then evolve passively and would be available as a seed to repeat +the above cycle. As the Universe evolves and more gas is consumed, +the mergers involving gas-rich galaxies will shift towards lower +masses, explaining the decline in the population of the brightest +quasars from $z\sim 2$ to the present, and the remnants that are +gas-poor will redden quickly owing to the termination of star +formation by black hole feedback (Springel et al.\ 2005a), so that they +resemble elliptical galaxies, surrounded by hot X-ray emitting halos +(e.g.\ Cox et al.\ 2005). + +There is considerable observational support for this scenario, which +has led the development of this picture for the co-evolution of +galaxies and quasars over recent decades. Infrared (IR) luminous +galaxies are thought to be powered in part by starbursts (e.g.\ Soifer +et al.\ 1984a,b; Sanders et al.\ 1986, 1988a,b; for a review, see e.g.\ +Soifer et al.\ 1987), and the most intense examples locally, +ultraluminous infrared galaxies (ULIRGs), are invariably associated +with mergers (e.g.\ Allen et al.\ 1985; Joseph \& Wright 1985; Armus et +al.\ 1987; Kleinmann et al.\ 1988; Melnick \& Mirabel 1990; for reviews, +see Sanders \& Mirabel 1996 and Jogee 2004). Radio observations show +that ULIRGs have large, central concentrations of dense gas (e.g.\ +Scoville et al.\ 1986; Sargent et al.\ 1987, 1989), providing a fuel +supply to feed black hole growth. Indeed, some ULIRGs have ``warm'' +IR spectral energy distributions (SEDs), suggesting that they harbor +buried quasars (e.g.\ Sanders et al.\ 1988c), an interpretation +strengthened by X-ray observations demonstrating the presence of two +non-thermal point sources in NGC6240 \citep{Komossa03}, which are +thought to be supermassive black holes that are heavily obscured at +visual wavelengths (e.g.\ Gerssen et al.\ 2004; Max et al.\ 2005, +Alexander et al.\ 2005a,b). These lines of evidence, together with the +overlap between bolometric luminosities of ULIRGs and quasars, +indicate that quasars are the descendents of an infrared luminous +phase of galaxy evolution caused by mergers (Sanders et al.\ 1988a), an +interpretation supported by observations of quasar hosts (e.g.\ +Stockton 1978; Heckman et al.\ 1984; Stockton \& MacKenty 1987; +Stockton \& Ridgway 1991; Hutchings \& Neff 1992; Bahcall et al.\ 1994, +1995, 1997; Canalizo \& Stockton 2001). + +However, many of the physical processes that connect the phases of +evolution in Figure~\ref{fig:cosmiccycle} are not well understood. +Early simulations showed that mergers produce objects resembling +galaxy spheroids (e.g.\ Barnes 1988, 1992; Hernquist 1992, 1993a) and +that if the progenitors are gas-rich, gravitational torques funnel gas +to the center of the remnant (e.g.\ Barnes \& Hernquist 1991, 1996), +producing a starburst (e.g.\ Mihos \& Hernquist 1996), but these works +did not explore the relationship of these events to black hole growth +and quasar activity. While a combination of arguments based on time +variability and energetics suggests that quasars are produced by the +accretion of gas onto supermassive black holes in the centers of +galaxies (e.g.\ Salpeter 1964; Zel'dovich \& Novikov 1964; Lynden-Bell +1969), the mechanism that provides the trigger to fuel quasars +therefore remains uncertain. Furthermore, there have been no +comprehensive models that describe the transition between ULIRGs and +quasars that can simultaneously account for observed correlations like +the $M_{\rm BH}$-$\sigma$ relation. + +Here, we study these relationships using numerical simulations of +galaxy mergers that account for the consequences of black hole growth. +In our simulations, black holes accrete and grow throughout a merger +event, producing complex, time-varying quasar activity. Quasars reach +a peak luminosity, $\Lp$, during the ``blowout'' phase of evolution +where feedback energy from black hole growth begins to drive away the +gas, eventually slowing accretion. Prior to and following this brief +period of peak activity, quasars radiate at instantaneous +luminosities, $L$, with $L < \Lp$. However, we show that even with +this complex behavior, the global characteristics that determine the +observed properties of quasars, i.e.\ lifetimes, light curves, and +obscuration, can be expressed as functions of $L$ and $\Lp$, +allowing us to make predictions for quasar populations that agree well +with observations, supporting the scenario sketched in +Figure~\ref{fig:cosmiccycle}. + +In \S~\ref{sec:methods}, we discuss our methodology and show how the +quasar lifetimes and obscuration from our simulations can be expressed +as functions of the instantaneous and peak luminosities of quasars. +We also define a set of commonly adopted models for the +quasar lifetime and obscuration against which we compare our +predictions throughout. In \S~\ref{sec:LF}, we apply our models to the +quasar luminosity function, using the observed luminosity function to +determine the distribution of quasar peak luminosities, and show that +this allows us to simultaneously reproduce the hard X-ray, soft X-ray, +and optical quasar luminosity functions at all redshifts $z\lesssim3$, +and the distribution of column densities in both optical and X-ray +samples. In \S~\ref{sec:BLqso}, we determine the time in our +simulations when quasars will be observable as broad-line objects, and +use this to predict the broad-line luminosity function and fraction of +broad-line objects in quasar samples, as a function of luminosity, as +well as the mass function of low-redshift, active broad-line +quasars. In \S~\ref{sec:eddington}, we estimate the distribution of +Eddington ratios in our simulations as a function of luminosity, and +infer Eddington ratios in observed samples at different redshifts. In +\S~\ref{sec:smbh}, we use our modeling to predict both the mass +distribution and total density of present-day relic supermassive black +holes, and describe their evolution with redshift. In \S~\ref{sec:xrb}, +we similarly apply this model to predict the integrated cosmic X-ray +background spectrum, accounting for the observed spectrum from +$\sim1-100$\,keV. In \S~\ref{sec:discussion}, we discuss the +primary qualitative implications of our results and propose +falsifiable tests of our picture. Finally, in \S~\ref{sec:finis}, +we conclude and suggest directions for future work. + +Throughout, we adopt a $\Omega_{\rm M}=0.3$, $\Omega_{\Lambda}=0.7$, +$H_{0}=70\,{\rm km\,s^{-1}\,Mpc^{-1}}$ ($h=0.7$) cosmology. + +\section{The Model: Methodology} +\label{sec:methods} + +Our model of quasar evolution has several elements, which we summarize +here and describe in greater detail below. + +\begin{itemize} + +\item In what follows, a ``quasar'' is taken to mean the course of +black hole activity in a {\em single} merger event. We use the term +``quasar lifetime'' to refer to the time spent by such a quasar at a +given luminosity or fraction of the quasar peak luminosity, integrated +over all black hole activity in a single merger event. This is not +meant to suggest that this would constitute the entire accretion +history of a black hole -- a given black hole may have multiple +``lifetimes'' triggered by different mergers, with each merger in +principle fueling a distinct ``quasar'' with its own lifetime. There +is no a priori luminosity threshold for quasar activity -- the time +history can include various epochs at low luminosities and accretion +rates. + +\item We model the galaxy mergers using hydrodynamical simulations, +varying the orbital parameters of the encounter, the internal +properties of the merging galaxies, prescriptions for the gas physics, +initial ``seed'' black hole masses of the merging systems, and +numerical resolution of the simulations. The black hole accretion +rate is determined from the surrounding gas (smoothed over the scale +of our spatial resolution, reaching $20\,$pc in the best cases), i.e.\ +the density and sound speed of the gas, and its motion relative to the +black hole, using Eddington-limited, Bondi-Hoyle-Lyttleton accretion +theory. The black hole radiates with a canonical efficiency +$\epsilon_{r}=0.1$ corresponding to a standard \citet{SS73} thin disk, +and we assume that $\sim5\%$ of this radiated luminosity is deposited +as thermal energy into the surrounding gas, weighted by the SPH +smoothing kernel (which has a $\sim r^{-2}$ profile) over the scale of +the spatial resolution. This scale is such that we cannot resolve the +complex accretion flow immediately around the black hole, but we adopt +this prescription because: (1) it reproduces the observed slope and +normalization in the $M_{\rm BH}-\sigma$ relation (Di Matteo et al.\ +2005), (2) it follows from observations, based on estimates of the +energy contained in highly-absorbed UV portion of the quasar SED +\citep[e.g.,][]{Elvis94,Telfer02}, (3) it follows from theoretical +considerations of momentum coupling to dust grains in the dense gas +very near the quasar \citep{Murray05} and hydrodynamical simulations +of small-scale radiative heating from quasar accretion \citep{CO01}, +and (4) even if the feedback is initially highly collimated, a driven +wind or shock in a dense region such as the center of the merging +galaxies will rapidly isotropize, so long as it is decelerated by +gravity and the surrounding medium, allowing the high sound speed +within the shock to equalize angle-dependent pressure variations +\citep[e.g.,][]{KM90}, and furthermore initial local distortions will +be washed away in favor of triaxial structure determined by the +large-scale density gradients \citep{BKS91}, as occurs in our +simulations. + +\item For each of our merger simulations, we compute the bolometric +black hole luminosity and column density along $\sim1000$ lines of +sight to the black hole(s) (evenly spaced in solid angle), as a +function of time from the beginning of the simulation until the system +has relaxed for $\sim1\,$Gyr after the merger. + +\item We bin different merger simulations by $\Lp$, the peak +bolometric luminosity of the black hole in the simulation, and the +conditional distributions of luminosity, $P(L|\Lp)$, and column +density, $P(\nh | L,\,\Lp)$, are computed using all simulations that +fall into a given bin in $\Lp$. The final black hole mass (black hole +mass at the end of the individual merger -- subsequent mergers and +quasar episodes could further increase the black hole mass) is +approximately $M_{\rm BH}^{f}\approx M_{\rm Edd}(\Lp)$ (but not +exactly, see \S~\ref{sec:detailsCompare}), so we obtain similar +results if we bin instead by $M_{BH}^{f}$. Our calculation of +$M_{BH}^{f}(\Lp)$ allows us to express our conditional distributions +of luminosity and column density in terms of either peak luminosity or +final black hole mass. Critically, we find that expressed in terms of +$\Lp$ or $M_{\rm BH}^{f}$, there is no systematic dependence in the +quasar evolution on the varied merger simulation properties -- this +allows us to calculate a large number of observables in terms of $\Lp$ +or $M_{\rm BH}^{f}$ without the large systematic uncertainties +inherent in attempting to directly estimate e.g.\ quasar light curves +in terms of host galaxy mass, gas fraction, multiphase pressurization +of the interstellar medium, orbital parameters and merger stage, and +other variables. + +\item The observed quasar luminosity function is the convolution of +the time a given quasar spends at some observed luminosity with the +rate at which such quasars are created. Knowing the distributions +$P(L|\Lp)$ and $P(\nh | L,\, \Lp)$, we can calculate the time spent by +a quasar with some $\Lp$ at an observed luminosity in a given +waveband. We use this to fit to observational estimates of the +bolometric quasar luminosity function $\phi(L)$, de-convolving these +quantities to determine the function $\nLp$; i.e.\ the rate at which +quasars of a given peak luminosity must be created or activated +(triggered in mergers) in order to reproduce the observed bolometric +luminosity function. + +\item Given these inputs, we determine the joint distribution in +instantaneous luminosity and black hole mass, column density +distribution, peak luminosity and final black hole mass, as a function +of redshift, i.e.\ $n(L,\,L_{\nu},\,M_{\rm BH},\,\nh ,\,\Lp,\,M_{\rm +BH}^{f}\ |\ z)$, at all redshifts where the observed quasar luminosity +function can provide the necessary constraint. From this joint +distribution, we can compute, for example, luminosity functions in +other wavebands, conditional column density distributions, active +black hole mass functions and Eddington ratio distributions, and relic +black hole mass functions and cosmic backgrounds. We can compare each +of these results to those determined using simpler models for either +the quasar lifetime or column density distributions; in +\S~\ref{sec:altmodels} we describe a canonical set of such +models, to which we compare throughout this paper. + +\end{itemize} + + +\subsection{The Simulations} +\label{sec:sims} + +The simulations were performed with {\small GADGET-2} +\citep{Springel2005}, a new version of the parallel TreeSPH code +{\small GADGET} \citep{SYW01}. {\small GADGET-2} is based on a fully +conservative formulation \citep{SH02} of smoothed particle +hydrodynamics (SPH), which maintains simultaneous energy and entropy +conservation when smoothing lengths evolve adaptively (for a +discussion, see e.g., Hernquist 1993b, O'Shea et al.\ 2005). Our +simulations account for radiative cooling, heating by a UV background +(as in Katz et al.\ 1996b, Dav\'e et al.\ 1999), and incorporate a +sub-resolution model of a multiphase interstellar medium (ISM) to +describe star formation and supernova feedback \citep{SH03}. Feedback +from supernovae is captured in this sub-resolution model through an +effective equation of state for star-forming gas, enabling us to +stably evolve disks with arbitrary gas fractions (see, e.g.\ Springel +et al.\ 2005b; Robertson et al.\ 2004). In order to investigate the +consequences of supernova feedback over a range of conditions, we +employ the scheme of \citet{SDH05b}, introducing a parameter $\qeos$ +to interpolate between an isothermal equation of state ($\qeos=0$) and +the full multiphase equation of state ($\qeos=1$) described above. + +Supermassive black holes (BHs) are represented by ``sink'' particles +that accrete gas at a rate $\Mdot$ estimated using an +Eddington-limited version of Bondi-Hoyle-Lyttleton accretion theory +(Bondi 1952; Bondi \& Hoyle 1944; Hoyle \& Lyttleton 1939). The +bolometric luminosity of the black hole is $\Lbol=\dEdt$, where +$\epsilon_r=0.1$ is the radiative efficiency. We assume that a small +fraction (typically $\approx 5\%$) of $\Lbol$ couples dynamically to +the surrounding gas, and that this feedback is injected into the gas +as thermal energy, as described above. + +We have performed several hundred simulations of colliding galaxies, +varying the numerical resolution, the orbit of the encounter, the +masses and structural properties of the merging galaxies, initial gas +fractions, halo concentrations, and the parameters describing star +formation and feedback from supernovae and black hole growth. This +large set of simulations allows us to investigate merger evolution for +a wide range of galaxy properties and to identify any systematic +dependence of our modeling. The galaxy models are described in +\citet{SDH05b}, and we briefly review their properties here. + +The progenitor galaxies in our simulations have virial +velocities $\vvir=80,$ $113,$ $160,$ $226,$ $320,$ ${\rm and}\ 500\,{\rm +km\,s^{-1}}$. We consider cases with gas equation of state parameters +$\qeos=0.25$ (moderately pressurized, with a mass-weighted temperature +of star-forming gas $\sim10^{4.5} {\rm K}$) and $\qeos=1.0$ (the full, +``stiff'' Springel-Hernquist equation of state, with a mass-weighted +temperature of star-forming gas $\sim10^{5} {\rm K}$), and initial +disk gas fractions (by mass) of $\fgas=0.2,$ $0.4,$ $0.8,$ ${\rm and}\ 1.0$. +Finally, we scale these models with redshift, altering the physical +sizes of the galaxy components and the dark matter halo concentration +in accord with cosmological evolution \citep{Mo1998}. Details are +provided in \citet{Robertson05b}, and here we consider galaxy models +scaled appropriately to resemble galaxies of the same $\vvir, \fgas, +{\rm and}\ \qeos$ at redshifts $\zgal=0,$ $2,$ $3,$ ${\rm and}\ 6$. + +For each simulation, we generate two stable, isolated disk galaxies, +each with an extended dark matter halo with a \citet{Hernquist90} +profile, motivated by cosmological simulations (e.g.\ Navarro et +al.\ 1996; Busha et al.\ 2004) and observations of halo properties +(e.g.\ Rines et al.\ 2002, 2002, 2003, 2004), an exponential disk of +gas and stars, and (optionally) a bulge. The galaxies have masses +$M_{\rm vir}=V_{\rm vir}^{3}/(10GH_{0})$ for $\zgal=0$, with the +baryonic disk having a mass fraction $m_{\rm d}=0.041$, the bulge +(when present) has a mass fraction $m_{\rm b}=0.0136$, and the rest of +the mass is in dark matter typically with a concentration parameter +$c=9.0$. The disk scale-length is computed based on an assumed spin +parameter $\lambda=0.033$, chosen to be near the mode in the observed +$\lambda$ distribution \citep{Vitvitska02}, and the scale-length of +the bulge is set to $0.2$ times the resulting value. In \citet{H05a}, +we describe our analysis of simulation A3, one of our set with +$\vvir=160\, {\rm km\,s^{-1}},\ \fgas=1.0,\ \qeos=1.0,\ {\rm and}\ +\zgal=0$, a fiducial choice with a rotation curve and mass similar to +the Milky Way, and \citet{H05b,H05c,H05d} used a set of simulations +with the same parameters but varying $\vvir=80,$ $113,$ $160,$ $226,$ ${\rm +and}\ 320\,{\rm km\,s^{-1}}$, which we refer to below as runs +A1, A2, A3, A4, and A5, respectively. + +Typically, each galaxy is initially composed of 168000 dark matter +halo particles, 8000 bulge particles (when present), 24000 gas and +24000 stellar disk particles, and one BH particle. We vary the +numerical resolution, with many of our simulations using instead twice +as many particles in each galaxy, and a subset of simulations with up +to 128 times as many particles. We vary the initial seed mass of the +black hole to identify any systematic dependence of our results on +this choice. In most cases, we choose the seed mass either in accord +with the observed $M_{\rm BH}$-$\sigma$ relation or to be sufficiently +small that its presence will not have an immediate +dynamical effect. Given the +particle numbers employed, the dark matter, gas, and star particles +are all of roughly equal mass, and central cusps in the dark matter +and bulge profiles are reasonably well resolved (see Fig 2. in +Springel et al.\ 2005b). The galaxies are then set to collide from a +zero energy orbit, and we vary the inclinations of the disks and the +pericenter separation. + +%\clearpage +\epsscale{0.9} +\begin{figure*} + \centering + \plotone{f2.ps} + %\includegraphics[width=3.7in]{f2.ps} + \caption{ + Time sequence from one of our merger simulations + ($V_{\rm vir}=160\,{\rm km\,s^{-1}}$, + initial gas fraction 20\%). Each panel is $80\,h^{-1}{\rm kpc}$ + on a side and shows the simulation time in the + upper left corner. Brightness of individual pixels gives the + logarithm of the projected stellar mass density, while color hue indicates + the baryonic gas fraction, from 20\% (blue) to less than 5\% (red). + At $T=1.03$, $1.39$ and $1.48\,{\rm Gyr}$, when + the black hole could be seen as an optical quasar, + nuclear point sources are shown, providing a representation of the + relative luminosities of stars and the quasar at these times. + \label{fig:sim.example}} +\end{figure*} +\epsscale{1} +%\clearpage + +A representative example of the behavior of the simulations is +provided in Figure~\ref{fig:sim.example}, which shows the time +sequence of a merger involving two bulge-less progenitor galaxies with +virial velocities of $160\, {\rm km\,s^{-1}}$ and initial gas +fractions of 20\%. During the merger, gas is driven to the galaxy +centers by gravitational tides, fueling nuclear starbursts and black +hole growth. The quasar activity is short-lived and peaks twice in +this merger, both during the first encounter and the final coalescence +of the galaxies. To illustrate the bright, optically observable +phase(s) of quasar activity which we identify below, we have added +nuclear point sources in +the center at the position(s) of the black hole(s) at +times $T=1.03$, $1.39$ and $1.48\,{\rm Gyr}$, generating a +surface density in correspondence to the relative luminosities of +stars and quasar at these times. At other times, the accretion +activity is either obscured or the black hole accretion rate is +negligible. To make the appearance of the quasar visually more +apparent, we have put a small part of its luminosity in ``rays'' +around the quasar. These rays are artificial and are only a visual +guide. + + +\subsection{Column Densities \&\ Quasar Attenuation} +\label{sec:NH} + +From the simulation outputs, we determine the obscuration of the black +hole as a function of time during a merger by calculating the column +density to a distant observer along many lines of sight. Typically, +we generate $\sim1000$ radial lines-of-sight (rays), each with its +origin at the black hole location and with directions uniformly spaced +in solid angle ${\rm d}\cos{\theta}\,{\rm d}\phi$. For each ray, we +begin at the origin and calculate and record the local gas properties +using the SPH formalism and move a distance along the ray $\Delta +r=\eta h_{\rm sml}$, where $\eta \leq 1$ and $h_{\rm sml}$ is the +local SPH smoothing length. The process is repeated until a ray is +sufficiently far from the origin ($\gtrsim 100$ kpc) that the column +has converged. We then integrate the gas properties along a +particular ray to give the line-of-sight column density and mean +metallicity. We have varied $\eta$ and find empirically that gas +properties along a ray converge rapidly and change smoothly for +$\eta=0.5$ and smaller. We similarly vary the number of rays and find +that the distribution of line-of-sight properties converges for +$\gtrsim 100$ rays. + +{}From the local gas properties, we use the multiphase model of the +ISM described in \citet{SH03} to determine the mass fraction in +``hot'' (diffuse) and ``cold'' (molecular and HI cloud core) phases of +dense gas and, assuming pressure equilibrium, we obtain the local +density of the hot and cold phases and their corresponding volume +filling factors. The resulting values are in rough agreement with +those of \citet{MO77}. Given a temperature for the warm, partially +ionized component of the hot-phase $\sim8000\,{\rm K}$, determined by +pressure equilibrium, we further calculate the neutral fraction of +this gas, typically $\sim0.3-0.5$. We denote the neutral and total +column densities as \NHI\ and \NH, respectively. Using only the +hot-phase density allows us to place an effective lower limit on the +column density along a particular line of sight, as it assumes a given +ray passes only through the diffuse ISM, with $\gtrsim 90\%$ of the +mass of the dense ISM concentrated in cold-phase ``clumps.'' Given the +small volume filling factor ($<0.01$) and cross section of cold +clouds, we expect that the majority of sightlines will pass only +through the ``hot-phase'' component. + +Using $\Lbol=\dEdt$, we model the intrinsic quasar continuum SED +following \citet{Marconi04}, based on optical through hard X-ray +observations +\citep[e.g.,][]{Elvis94,George98,VB01,Perola02,Telfer02,Ueda03,VBS03}, +with a reflection component generated by the PEXRAV model +\citep{MZ95}. This yields, for example, a B-band luminosity +$\log{(\LB/L_{\sun})}=0.80-0.067\mathcal{L}+0.017\mathcal{L}^{2}-0.0023\mathcal{L}^{3}$, +where $\mathcal{L} = \log{(\Lbol/L_{\sun})} - 12$, and we take +$\lambda_{B}=4400\,$\AA, but as we model the entire intrinsic SED we +can determine the bolometric correction in any frequency interval. + +We then use a gas-to-dust ratio to determine the extinction along a +given line of sight at optical frequencies. Observations suggest that +the majority of reddened quasars have reddening curves similar to that +of the Small Magellanic Cloud (SMC; Hopkins et al.\ 2004, Ellison et +al.\ 2005), which has a gas-to-dust ratio lower than the Milky Way by +approximately the same factor as its metallicity \citep{Bouchet85}. +Hence, we consider both a gas-to-dust ratio equal to that of the Milky +Way, $(A_{B}/\nhi)_{\rm MW}=8.47\times10^{-22}\,{\rm cm^{2}}$, and a +gas-to-dust ratio scaled by metallicity, $A_{B}/\nhi = +(Z/0.02)(A_{B}/\nhi)_{\rm MW}$. In both cases we use the SMC-like +reddening curve of \citet{Pei92}. The form of the correction for hard +X-ray (2-10 keV) and soft X-ray (0.5-2 keV) luminosities is similar to +that of the B-band luminosity. We calculate extinction at X-ray +frequencies (0.03-10 keV) using the photoelectric absorption cross +sections of \citet{MM83} and non-relativistic Compton scattering cross +sections, similarly scaled by metallicity. In determining the column +density for photoelectric X-ray absorption, we ignore the inferred +ionized fraction of the gas, as it is expected that the inner-shell +electrons which dominate the photoelectric absorption edges will be +unaffected in the temperature ranges of interest. We do not perform a +full radiative transfer calculation, and therefore do not model +scattering or re-processing of radiation by dust in the infrared. + +For a full comparison of quasar lifetimes and column densities +obtained varying our calculation of \NH, we refer to \citet{H05b} (see +their Figures 1, 5, \& 6), and note their conclusion that, after +accounting for clumping of most mass in the dense ISM in cold-phase +structures, the column density does not depend sensitively on our +assumptions for the small-scale physics of the ISM and obscuration -- +typically, the uncertainties in the resulting quasar lifetime as a +function of luminosity are a factor $\sim2$ at low luminosities in the +B-band, and smaller in e.g.\ the hard X-ray. Because our +determination of the quasar luminosity functions is similar using the +hard X-ray data alone or the hard X-ray, soft X-ray, and optical data +simultaneously, the added uncertainties in our calculation of $\nLp$ +in \S~\ref{sec:fullLF} below owing to the uncertainty in our $\nh$ +calculation are small compared to the uncertainties owing to +degeneracies in the fitting procedure and uncertain bolometric +corrections. + +\subsection{The \NH\ Distribution as a Function of Luminosity} +\label{sec:NHfunction} + +Next, we consider the distribution of column densities as a function +of both the instantaneous and peak quasar luminosities. For each +simulation, we consider \NH\ values at all times with a given +bolometric luminosity $L$ (in some logarithmic interval in $L$), and +determine the distribution of column densities at that $L$ weighted by +the total time along all sightlines with a given \NH. At each $L$, we +approximate the simulated distribution and fit it to a lognormal form, +\begin{equation} +P(N_{H}) = \frac{1}{\sigNH \sqrt{2 \pi}}\, \exp\left[ +\frac{-\log^2(N_{H}/\meanNH )}{2 \sigNH^{2}}\right]. +\end{equation} +This provides a good fit for all but the brightest luminosities, where +quasar feedback becomes important driving the ``blowout'' phase, and +the quasar sweeps away surrounding gas and dust to become optically +observable. + +%\clearpage +\begin{figure*} + \centering + \plotone{f3.ps} + %\includegraphics[width=3.7in]{f3.ps} + \caption{The median fitted total (neutral and ionized) column + density $\meanNH$ at each luminosity $L$ in the snapshots from our + series of simulations described in \S~\ref{sec:methods}. We compare changing + concentrations and halo properties with redshift $\zgal$ (upper + left), gas fractions $\fgas$ (upper right), the equation of state + parameter $\qeos$ (lower left), and virial velocity $\vvir$ (lower + right). At lower right, simulations with $\vvir=80, 113, 160, + 226, 320, {\rm and}\ 500\,{\rm km\,s^{-1}}$ are shown as black + asterisks, purple dots, red diamonds, green triangles, yellow + squares, and red crosses, respectively. Other than a possible + weak sensitivity to $\qeos$, the column density distribution as a + function of luminosity shows no systematic dependence on any of + the varied simulation parameters. + \label{fig:NH.systematics}} +\end{figure*} +%\clearpage + +We show the resulting median column density $\meanNH$ at each +luminosity $L$ in Figure~\ref{fig:NH.systematics}. In the upper left +panel, simulations with $\zgal=0$ are shown in black, those with +$\zgal=2$ in blue, and those with $\zgal=3$ in yellow. In the upper +right, simulations with $\fgas=0.4$ are shown in black, those with +$\fgas=0.8$ in red. In the lower left, simulations with $\qeos=0.25$ +are shown in black, those with $\qeos=1.0$ in green. And in the lower +right, simulations with $\vvir=80, 113, 160, 226, 320, {\rm and}\ +500\,{\rm km\,s^{-1}}$ are shown as black asterisks, purple dots, red +diamonds, green triangles, yellow squares, and red crosses, +respectively. Simulations with other values for these parameters (not +shown for clarity, but see e.g. Hopkins et al.\ [2005d]) show similar +trends. + +While the increase in typical $\nh$ values with luminosity +appears to contradict observations suggesting that the obscured +fraction decreases with luminosity, this is because the relationship +shown above is dominated by quasars in growing, heavily obscured +phases. In these stages, the relationship between column density and +luminosity is a natural consequence of the fact that both are fueled +by strong gas flows into the central regions of the galaxy -- more gas +inflow means higher luminosities, but also higher column densities. +During these phases, the lognormal fits to column density as a +function of instantaneous and peak luminosity presented in this +section are reasonable approximations, but they break down in the +brightest, short-lived stages of merger activity when the quasar +rapidly heats the surrounding gas and drives a powerful wind, lowering +the column density, resulting in a bright, optically observable +quasar. Including in greater detail the effects of quasar blowout +during the final stages of its growth in \S~\ref{sec:BLqso}, we find +that this modeling actually predicts the observed decrease in obscured +fraction with luminosity. + +The relationship between \NH\ and $L$ shows no strong systematic +dependence on any of the simulation parameters considered. At most, +there is weak sensitivity to $\qeos$, in the sense that the +simulations with $\qeos=1.0$ have slightly larger column densities at +a given luminosity than those with $\qeos=0.25$. We derive an +analytical model relating both the observed column density and quasar +luminosity to the inflowing mass of gas in \citet{H05d}, by +assuming that while it is growing, the black hole mass is proportional +to the inflowing gas mass in the galaxy core (which ultimately +produces the Magorrian et al.\ [1998] relation between black hole and +bulge mass), and assuming Bondi accretion, with obscuration along a +sightline through this (spherically symmetric) gas inflow. Such a +model gives the observed correlation between $N_{\rm H}$ and $L$, and +explains the weak dependence of the column density-luminosity relation +on the ISM gas equation of state. The assumptions above give a +relationship of the form +\begin{equation} +\nh\sim f_{0}\,\frac{1}{m_{H} R_{c}}\,\Bigl( \frac{c_{s}}{c}\Bigr)\,\Bigl( \frac{c L}{G^{2}}\Bigr)^{1/3}, +\end{equation} +where $f_{0}\sim50$ is a dimensionless factor depending on the +radiative efficiency, mean molecular weight, density profile, and +assumed $M_{\rm BH}-\sigma$ relation; $m_{H}$ is the mass of hydrogen; +$R_{c}$ the radius of the galaxy core ($\sim100\,{\rm pc}$); and +$c_{s}$ the effective sound speed in the central regions of the galaxy. A +$\qeos=1.0$ equation of state, with a higher effective temperature, +results in a factor of $\approx2$ larger sound speed in the densest +regions of the galaxy than a $\qeos=0.25$ equation of state +\citep{SDH05b}, explaining the weak trend seen. In any event, +the dependence is small compared to the intrinsic scatter for either +equation of state in the value of $\meanNH$ at a given luminosity, and +further weakens at high luminosity, so it can be neglected. +What may appear to be a systematic offset in $\meanNH$ with +$\vvir$ is actually just a tendency for larger $\vvir$ systems to be +at higher luminosities; there is no significant change in the +dependence of \NH\ on $L$. + +We use our large set of simulations to improve our fits (relative to +those of Hopkins et al.\ 2005d) to the \NH\ distribution as a function +of instantaneous and peak luminosities. Looking at individual +simulations, there appears to be a ``break'' in the power-law +scaling of $\meanNH$ with $L$ at $L\sim\Lcut{11}$. We find that the +best fit to the median column density $\meanNH$ is then +\begin{equation} + \meanNH = \left\{ \begin{array}{ll} + 10^{22.8}\, {\rm cm^{-2}} \Bigl( \frac{L}{\Lp}\Bigr)^{0.54} & \mathrm{ if\ } L < \Lcut{11} \\ + 10^{21.9}\, {\rm cm^{-2}} \Bigl( \frac{L}{\Lcut{11}}\Bigr)^{0.43} & \mathrm{ if\ } L > \Lcut{11}. +\end{array} + \right. +\end{equation} +Either of these two relations provides an acceptable fit to the +plotted $\meanNH$ distribution if applied to the entire luminosity +range ($\reducechi\approx2.8,\,3.2$ for the first and second +relations, respectively), but their combination provides a +significantly better fit ($\reducechi\approx1.5$), although it is +clear from the large scatter in $\meanNH$ values that any such fit is +a rough approximation. Despite the complicated form of this equation, +it is, in practice, similar to our $\meanNH\propto L^{0.35}$ +fit from previous work and $\meanNH\propto L^{1/3}$ analytical scaling +over the range of relevant luminosities, but is more accurate by a +factor $\sim2-3$ at low ($\lesssim\Lcut{9}$) luminosities. For +comparison, however, we do consider this simpler form for $\nh(L)$ as +well as our more accurate fit above in our subsequent analysis, and +find that it makes little difference to most observable quasar +properties. At the highest luminosities, near the peak luminosities +of the brightest quasars, the scatter about these fitted median +$\meanNH$ values increases, and as noted above the impact of the +quasar in expelling surrounding gas becomes important and column +densities vary rapidly. We consider this ``blowout'' phase in more +detail in \S~\ref{sec:BLqso}. + +We find that any dependence of $\sigNH$ (the fitted lognormal +dispersion) on $L$ or $L_{\rm peak}$ is not statistically significant, +with approximately constant $\sigNH\approx 0.4$ for individual +simulations. We similarly find no systematic dependence of $\sigNH$ on +any of our varied simulation parameters. However, it is important to +note that while the dispersion in \NH\ for an individual simulation is +$\sigNH\approx 0.4$, the dispersion in $\meanNH$ across all simulations at a +given luminosity is large, $\sim1$ dex. Thus, we fit the effective +$\sigNH$ at a given luminosity for the {\em distribution} of quasars +and find it is $\sigNH\approx 1.2$. Although we have slightly revised our +fits for greater accuracy at low luminosities, we note that this +relation is shallower than the relation $\nh\propto L$ roughly +expected if $M_{\rm BH}$ is constant ($L\propto\rho\propto\nh$) or +$L\propto M_{\rm BH}$ always, and strongly contrasts with unification +models which predict static obscuration, or evolutionary +models in which \NH\ is independent of $L$ up to some threshold +\citep[e.g.,][]{Fabian99}. + +\subsection{Quasar Lifetimes \&\ Sensitivity to Simulation Parameters} +\label{sec:detailsCompare} + +We define the luminosity-dependent quasar lifetime $\tQ=\tQ(\Lm)$ as +the time a quasar has a luminosity above a certain reference +luminosity $\Lm$; i.e.\ the total time the quasar shines at +$L\geq\Lm$. For ease of comparison across frequencies, we measure the +lifetime in terms of the bolometric luminosity, $L$, rather than e.g.\ +the B-band luminosity. Knowing the distribution of column densities +\NH\ as a function of luminosity and system properties (see +\S~\ref{sec:NHfunction}), we can then analytically or numerically +calculate the distribution of observed lifetimes at any frequency if +we know this intrinsic lifetime. Below $\sim1$ Myr, our estimates of +\tq\ become uncertain owing to the effects of quasar variability and +our inability to resolve the local small-scale physics of the ISM, but +this is significantly shorter than even the most rapid timescales +$\sim10$\,Myr of substantial quasar evolution. + +%\clearpage +\begin{figure} + \centering + \plotone{f4.ps} + %\includegraphics[width=3.7in]{f4.ps} + \caption{Integrated intrinsic quasar lifetime above a given + reference bolometric luminosity, $t_{Q}(L)$, as a function of + luminosity for simulations with host galaxies with total mass + (top panel) $M_{\rm gal}=0.5-2.0\times10^{12}\,M_{\sun}$, and + simulations with final black hole masses (bottom panel) + $\mbhf=0.5-2.0\times10^{8}\,M_{\sun}$ (i.e.\ similar peak + luminosity $\Lp\sim\Lcut{12}$). The simulations cover a range in + equation of state parameter $\qeos$, initial disk gas fraction + $\fgas$, galaxy redshift (for scaling of halo properties) $\zgal$, + and virial velocities $\vvir=113-160\,{\rm km\,s^{-1}}$. The black + line in both cases is for a merger involving Milky Way-like galaxy + models, which we refer to as A3, with $\fgas=1,\,\qeos=1,\,\zgal=0,\ + {\rm and}\ \vvir=160\,{\rm km\,s^{-1}}$. + \label{fig:tQ.systematics}} +\end{figure} +%\clearpage + +As before, we use our diverse sample of simulations to test for +systematic effects in our parameterization of the quasar lifetime. +Figure~\ref{fig:tQ.systematics} shows the quasar lifetime as a +function of reference luminosity $\Lm$ for both a set of simulations +with similar total galaxy mass, $M_{\rm gal}\approx10^{12}\,M_{\sun}$, +and similar final black hole mass (i.e.\ similar peak quasar +luminosity), $\mbhf\approx10^{8}\,M_{\sun}$. In each case, the +simulations cover a range in $\qeos,$ $\fgas,$ $\zgal,$ ${\rm and}\ \vvir$. + +As Figure~\ref{fig:tQ.systematics} demonstrates, at a given $M_{\rm +gal}$, there is a wide range of lifetimes, with a systematic +dependence on several quantities. For example, for fixed $M_{\rm +gal}$, a lower $\qeos$ means that the gas is less pressurized and more +easily collapses to high density, resulting in larger $\mbhf$ and +longer lifetimes at higher luminosities. Similarly, higher $\fgas$ +provides more fuel for black hole growth at fixed $M_{\rm gal}$. +However, for a given $\mbhf$, the lifetime \tq\ as a function of $\Lm$ +is similar across simulations and shows no systematic dependence on +any of the varied parameters. We find this for all final black hole +masses in our simulations, in the range +$\mbhf\sim10^{6}-10^{10}\,M_{\sun}$. We have further tested this as a +function of resolution, comparing with alternate realizations of our +fiducial A3 simulation with up to 128 times as many particles, and +find similar results as a function of $\mbhf$. + +From Figure~\ref{fig:tQ.systematics}, it is clear that the final black +hole mass or peak luminosity is a better variable to use in describing +the lifetime than the host galaxy mass. The lack of any systematic +dependence of either the quasar lifetime or \NH($L,\Lp$) on host +galaxy properties implies that our earlier results (Hopkins et al.\ +2005a-d) are reliable and can be applied to a wide range of host +galaxy properties, redshifts, and luminosities, although we refine and +expand the various fits of these works and their applications herein. +Furthermore, the large scatter in \tq\ at a given galaxy mass has +important implications for the quasar correlation function as a +function of luminosity, as one cannot associate a single quasar +luminosity with hosts of a given mass (see Lidz et al.\ 2005). + +%\clearpage +\begin{figure} + \centering + \plotone{f5.ps} + %\includegraphics[width=3.7in]{f5.ps} + \caption{Fits to the quasar lifetime as a + function of luminosity from our simulations. Upper left + shows the intrinsic, bolometric quasar lifetime $t_{Q}$ of a set + of simulations with $\Lp$ within a factor of 2 of + $\Lcut{10}$, in the manner of + Figure~\ref{fig:tQ.systematics}. The black histogram shows the + geometric mean of these lifetimes, and the black histogram in the + lower left shows the differential lifetime $\dtdL$ from this + geometric mean. The black thick line in the upper left and red + line in the lower left show the best-fit to our analytical + form, $\dtdL=t^{\ast}_{Q}\,\exp(-L/L^{\ast}_{Q})$. Upper right + shows the fitted $t^{\ast}_{Q}$ and resulting errors in each peak + luminosity (final black hole mass) interval, and the best-fit + power-law to $t^{\ast}_{Q}(\Lp)$ (red line). Lower right shows the fitted + $L^{\ast}_{Q}$ and resulting errors in each peak luminosity (final + black hole mass) interval, and the best-fit proportionality + $L^{\ast}_{Q}\propto\Lp$ (red line). + \label{fig:show.fits}} +\end{figure} +%\clearpage + +Although the truncated power-laws we have previously fitted to \tq\ +using only the A-series simulations \citep{H05b} provide +acceptable fits to all our runs, we use our new, larger set of simulations +to improve the accuracy of the fits and average over peculiarities of +individual simulations, giving a more robust prediction of the +lifetime as a function of instantaneous and peak luminosity. For a +given peak luminosity $\Lp$, we consider simulations with an $\Lp$ +within a factor of 2, and take the geometric mean of their lifetimes +\tq($L$) (we ignore any points where $\tQ<1$\,Myr, as our calculated +lifetimes are uncertain below this limit). We can then differentiate +this numerically to obtain $\dtdL$ (the time spent in a given +logarithmic luminosity interval), and fit some functions to both +curves simultaneously. Figure~\ref{fig:show.fits} illustrates this and +shows the results of our fitting. We find that both the integrated +lifetime \tq($L$) and the differential lifetime $\dtdL$ are well +fitted by an exponential, +\begin{equation} +\dtdL=t^{\ast}_{Q}\, \exp [-L/L^{\ast}_{Q}], +\end{equation} +where both $t^{\ast}_{Q}$ and $L^{\ast}_{Q}$ are functions of $\mbhf$ +or $\Lp$. The best-fit such $\dtdL$ is shown in the figure as a solid +line for simulations with $\Lp\sim\Lcut{10}$, and agrees well +with both the numerical derivative $\dtdL$ (lower left, black +histogram) and the geometric mean $\tQ(L)$ (upper left, black +histogram). This of course implies +\begin{equation} +\tQ(L)=t^{\ast}_{Q}\,\int^{\Lp}_{L}e^{-L/L^{\ast}_{Q}}\,d\log{L}, +\end{equation} +but we are primarily interested in $\dtdL$ in our subsequent +analysis. + +Although our fitted lifetime involves an exponential, it is in no way +similar to the exponential light curve of constant Eddington-ratio +black hole growth or the model in, e.g., \citet{HL98}, which give +$\dtdL=$\,{\em constant}\,$\sim t_{S}\ll t^{\ast}_{Q}$. + +Our +functional form also has the advantage that, although it should formally be +truncated with $\dtdL=0$ for $L>\Lp$, the values in this regime fall +off so quickly that we can safely use the above fit for all large +$L$. Similarly, at $L\lesssim10^{-4}\,\Lp$, $\dtdL$ falls below the +constant $t^{\ast}_{Q}$ to which this equation +asymptotes. Furthermore, in this regime, the fits above begin to +differ significantly from those obtained by fitting e.g.\ truncated +power-laws or Schechter functions. However, these luminosities are +well below those we generally consider and well below the luminosities +where the contribution of a quasar with some $\Lp$ is significant to +the observed quantities we predict. Moreover, this turndown (i.e.\ the +lower value predicted by an exponential as opposed to a power-law or +Schechter function at low luminosities) is at least in part an +artifact of the finite simulation duration. The values here are also +significantly more uncertain, as by these low relative accretion +rates, the system is likely to be accreting in some low-efficiency, +ADAF state (e.g.\ Narayan \& Yi 1995), which we do not implement +directly in our simulations. Rather than introduce additional +uncertainties into our modeling when they do not affect our +predictions, we adopt these exponential fits which are +accurate at $L\gtrsim10^{-4}-10^{-3}\,\Lp$. However, for purposes +where the faint-end behavior of the quasar lifetime is important, +such as predicting the value and evolution of the faint-end quasar +luminosity function slope with redshift, a more detailed examination +of the lifetime at low luminosities and relaxation of quasars after +the ``blowout'' phase is necessary, and we consider these issues +separately in \citet{H05f}. + +We also note that in \citet{H05c} we considered several extreme limits +to our modeling, neglecting all times before the final merger and +applying an ADAF correction at low accretion rates (taken +into account a posteriori by rescaling the radiative efficiency +$\epsilon_{r}$ with accretion rate, given the assumption that such low +accretion rates do not have a large dynamical effect on the system +regardless of radiative efficiency), and found that this does not +change our results -- the lifetime at low luminosities +may be slightly altered but the key qualitative point, that the quasar +lifetime increases with decreasing luminosity, is robust against a +wide range of limits designed to decrease the lifetime at low +luminosities. + +Figure~\ref{fig:show.fits} further shows the fitted $t^{\ast}_{Q}$ +(upper right) and $L^{\ast}_{Q}$ (lower right) as a function of peak +quasar luminosity for each $\Lp$. We find that +$L^{\ast}_{Q}$, the luminosity above which the lifetime rapidly +decreases, is proportional to $\Lp$, +\begin{equation} +L^{\ast}_{Q}=\alpha_{L}\Lp , +\end{equation} +with a best fit coefficient $\alpha_{L}=0.20$ (solid line). The weak +dependence of $t^{\ast}_{Q}$ on $\Lp$ is well-described by a power-law, +\begin{equation} +t^{\ast}_{Q}=t^{(10)}_{\ast}\,\Bigl( \frac{\Lp}{\Lcut{10}}\Bigr)^{\alpha_{T}}, +\end{equation} +with $t^{(10)}_{\ast}=1.37\times10^{9}\,{\rm yr}$ and +$\alpha_{T}=-0.11$ +%, and a double power-law fit (solid line), +%\begin{equation} +%t^{\ast}_{Q}=t^{(10)}_{\ast}\,\left[\Bigl( +%\frac{\Lp}{\Lcut{10}}\Bigr)^{\alpha_{T}}+\Bigl( +%\frac{\Lp}{\Lcut{10}}\Bigr)^{\beta_{T}}\right], +%\end{equation} +%with $t^{(10)}_{\ast}=8.8\times10^{8}\,{\rm yr}$, $\alpha_{T}=-0.71$, +%and $\beta_{T}=-0.07$. We have carried out our analysis with both +%functions and find no significant differences except for slight +%corrections to the high-mass end of the relic black hole mass +%function (see \S~\ref{sec:smbh}). Unless otherwise specified, we adopt the double +%power-law form for our calculations, as it gives a marginally better +%fit to the simulation lifetimes. + +%\clearpage +\begin{figure} + \centering + \plotone{f6.ps} + %\includegraphics[width=3.7in]{f6.ps} + \caption{Predicted quasar lifetime as a function of luminosity + compared to that obtained in simulations with and without bulges + and with different initial seed black hole masses. All simulations shown + in this plot + are initially identical to our fiducial A3 (Milky Way-like) case, + but with or without an initial stellar bulge and with an initial + seed black hole mass as labeled. Diamonds show the predicted + quasar lifetime $t_{Q}$, a function of the peak luminosity of each + simulated quasar, determined from the fits shown in + Figure~\ref{fig:show.fits}. Crosses show the lifetime determined + directly in the simulations. + \label{fig:check.MBHbulge}} +\end{figure} +%\clearpage + +The presence or absence of a stellar bulge in the progenitors can have +a significant impact on the quasar light curve (Springel et al. +2005b), primarily affecting the strength of the strong accretion phase +associated with initial passage of the merging galaxies (e.g.\ Mihos +\& Hernquist 1994). Likewise, the seed mass of the simulation black +holes could have an effect, as black holes with smaller initial masses +will spend more time growing to large sizes, and more massive black +holes may be able to shut down early phases of accretion in mergers in +minor ``blowout'' events. In Figure~\ref{fig:check.MBHbulge}, we show +various tests to examine the robustness of our fitted quasar lifetimes +to these variations. We have re-run our fiducial Milky Way-like A3 +simulation both with (right panels) and without (left panels) initial +stellar bulges in the merging galaxies and varying the initial black +hole seed masses from $10^{4}-10^{7}\,M_{\sun}$. In each case we +compare the lifetime $t_{Q}$ determined directly from the simulations +(crosses) to that predicted from our fits above (diamonds), based only +on the peak luminosity (final black hole mass) of the simulated +quasar. Again, we find that varying these simulation parameters can +have a significant effect on the final black hole mass, but that the +quasar lifetime as a function of peak luminosity is a robust quantity, +independent of initial black hole mass or the presence or absence of a +bulge in the quasar host. + +We can integrate the total radiative output of our model quasars, +\begin{equation} +E_{\rm rad}=\int^{\Lp}_{L_{\rm min}} L\,\fdtdL {\rm d}\log L, +\end{equation} +and using our fitted formulae and $L_{\rm min}\ll L^{\ast}_{Q}$ +we find +\begin{equation} +E_{\rm rad}=L^{\ast}_{Q}\, t^{\ast}_{Q}\,\log{e}\,(1-e^{-\Lp/L^{\ast}_{Q}}). +\label{eq:Erad} +\end{equation} +Knowing $E_{\rm rad}=\epsilon_{r}\mbhf c^{2}$, we can compare the +final black hole mass as a function of peak luminosity to what we +would expect if the peak luminosity were the Eddington +luminosity of a black hole with mass $M_{\rm Edd}$, $L_{\rm +Edd}=\epsilon_{r}M_{\rm Edd} c^{2}/t_{S}$, where $t_{S}$ is the +Salpeter time for $\epsilon_{r}=0.1$. Equating $E_{\rm +rad}=\epsilon_{r}\mbhf c^{2}$ with the value calculated in +Equation~\ref{eq:Erad}, and using the definition of the Eddington mass +at $L=\Lp$ and our fitted $L^{\ast}_{Q}=\alpha_{L}\Lp$, we obtain +\begin{equation} +\frac{\mbhf(\Lp)}{M_{\rm Edd}(\Lp)}=\alpha_{L} \Bigl( \frac{t^{\ast}_{Q}}{t_{S}}\Bigr) \log e +\approx1.24\, f_{T}, +\label{eq:Mbhf} +\end{equation} +where $f_{T}=(\Lp/\Lcut{13})^{-0.11}$ for the power-law fit to +$t^{\ast}_{Q}$. For our calculations explicitly involving black hole +mass, we adopt this conversion unless otherwise noted, as we have +performed our primary calculation (i.e.\ calculated $\nLp$) in terms +of peak luminosity. Moreover, although this agrees well with +the black hole masses in our simulations as a function of peak +luminosity (as it must if the fitted quasar lifetimes are accurate), +this allows us to smoothly interpolate to the highest black hole +masses ($\sim {\rm a\ few}\, \times10^{9}-10^{10}\,M_{\sun}$), which +are of particular interest in examining the black hole population but +for which the number of simulations we have with a given final black +hole mass drops rapidly. + +This gives explicitly the modifications to the black hole mass +compared to that inferred from the ``light bulb'' and +``constant Eddington ratio'' models which we outline below in +\S~\ref{sec:altmodels}, in which quasars shine at constant luminosity +or follow exponential light curves, and for which $M_{\rm +BH}^{f}=M_{\rm Edd}(\Lp) / l$, where $l$, the (constant) Eddington +ratio, is generally adopted. The corrections are small, and therefore +most of the black hole mass is accumulated in the bright, near-peak +quasar phase, in good agreement with observational estimates +\citep[e.g.,][]{Soltan82,YT02}; we discuss this in greater detail in +\S~\ref{sec:BLqso} and \S~\ref{sec:smbh}. Furthermore, the increase of +$f_{T}$ with decreasing $\Lp$ implies that lower-mass quasars +accumulate a larger fraction of their mass in slower, sub-peak +accretion after the final merger, while high-mass objects acquire +essentially all their mass in the peak quasar phase. This is seen +directly in our simulations, and is qualitatively in good agreement +with expectations from simulations and semi-analytical models in which +the $M_{\rm BH}-\sigma$ relation is set by black hole feedback in a +strong quasar phase. Compared to the assumption that +$M_{BH}^{f}=M_{\rm Edd}(\Lp)$, this formula introduces a small but +non-trivial correction in the relic supermassive black hole mass +function implied by the quasar luminosity function and $\nLp$ (see +\S~\ref{sec:smbh}). + +The predictions of our model for the quasar lifetime and evolution can +be applied to observations which attempt to constrain the quasar +lifetime from individual quasars, for example using the proximity +effect in the Ly$\alpha$ forest \citep{BDO88,HC02,Jakobsen03,YL05} and +multi-epoch observations \citep{MartiniSchneider03}. However, many +observations designed to constrain the quasar lifetime do so not for +individual quasars, but using demographic or integral arguments based +on the population of quasars in some luminosity interval +\citep[e.g.,][]{Soltan82,HNR98,YT02,YL04,PMN04,Grazian04}. Our +prediction for these observations is similar but slightly more +complex, as an observed luminosity function at a given luminosity will +consist of sources with different peak luminosities $\Lp$, but the +same instantaneous luminosity, $L$. Furthermore, the lifetime being +probed may be either the integrated quasar lifetime above some +luminosity threshold or the differential lifetime at a particular +luminosity. + +%\clearpage +\begin{figure*} + \centering + \plotone{f7.ps} + %\includegraphics[width=3.7in]{f7.ps} + \caption{Predicted distribution (fractional number density + per logarithmic interval in lifetime) of quasar lifetimes at + different bolometric luminosities, for the luminosity function + determined in \S~\ref{sec:LF} at $z=0.5$. Left panel plots the distribution of + integrated lifetimes $t_{Q}$ (time spent over the course of each + quasar lifetime above the given luminosity). Right panel plots + the distribution of differential lifetimes $\dtdL$ (time spent + by each quasar in a logarithmic interval about the given luminosity). + \label{fig:LF.lifetimes}} +\end{figure*} +%\clearpage + +For a given determination of the quasar luminosity function using our +model for quasar lifetimes and some distribution of peak luminosities, +we can predict the distribution of quasar lifetimes as a function of +the observed luminosity interval. Figure~\ref{fig:LF.lifetimes} shows +an example of such a result, using the determination of the luminosity +function below in \S~\ref{sec:fullLF}, at redshift $z=0.5$. We +consider several bolometric luminosities spanning the luminosity +function from $10^{9}-10^{14}\,L_{\sun}$, and for each, the +distribution of sources (peak luminosities), and the corresponding +distribution of quasar lifetimes. We show both the distribution of +integrated quasar lifetimes $t_{Q}$ (left panel) and the distribution +of differential quasar lifetimes $\dtdL$ (right panel). The evolution +with redshift is weak, with the lifetime increasing by $\sim1.5-2$ at +a given luminosity at $z=2$. There is furthermore an ambiguity of a +factor $\sim2$, as some of the quasars observed at a given luminosity +will only be entering a peak quasar phase, whereas the lifetimes shown +are integrated over the whole quasar evolution. This prediction is +quite different from that of the optical quasar phase which we +describe below in \S~\ref{sec:BLqso} and in \citet{H05a}, as it +considers only the intrinsic bolometric luminosity, but our modeling +and the fits provided above for the bolometric lifetime and column +density distributions should enable the prediction of these +quantities, considering attenuation, in any waveband. In either case, +it is clear that the lifetime distribution for lower-luminosity +quasars is increasingly more strongly peaked and centered around +longer lifetimes, in good agreement with the limited observational +evidence from e.g.\ Adelberger \& Steidel (2005). This is a +consequence of the fact that in our model quasar lifetimes +decrease with increasing luminosity. The range spanned in the figure +corresponds well to the range of quasar lifetimes implied by the +observations above and others \citep[e.g.][and references +therein]{Martini04}. + +\subsection{Alternative Models of Quasar Evolution} +\label{sec:altmodels} + +Our modeling reproduces at least the observed hard X-ray quasar +luminosity function by construction, since we use the observed quasar +luminosity functions to determine the birthrate of quasars of a given +$\Lp$, $\nLp$, in \S~\ref{sec:fullLF}. It is therefore useful to +consider in detail the differences in our subsequent predictions +between various models for the quasar lifetime and obscuration, in +order to determine to what extent these predictions are implied by any +model that successfully reproduces the observed quasar luminosity +function, and to what extent they are independent of the observed +luminosity functions and instead depend on the model of quasar +evolution adopted. To this end, we define two models for the +quasar lifetime, and two models for the distribution of quasar column +densities, combinations of which have been commonly used in most +previous analyses of quasars. + +For the quasar lifetime, we consider the following two cases: + +\bigskip + +{\em ``Light-Bulb Model''} \citep[e.g.,][]{SB92,KH00,WL03,HQB04}. The +simplest possible model for the quasar light curve, the ``feast or +famine'' or ``light-bulb'' model assumes that quasars have only two +states, ``on'' and ``off.'' Quasars turn ``on'', shine at a fixed +bolometric luminosity $L=\Lp$, defined by a ``constant'' Eddington +ratio (i.e.\ $\Lp=l\, M_{\rm BH}^{f}$) and constant quasar lifetime +$t_{Q,\,\rm LB}$. Models where quasars live arbitrarily long with +slowly evolving mean volume emissivity or mean light curve +\citep[e.g.][]{SB92,HM00,KH00} are equivalent to the ``light bulb'' +scenario, as they still assume that quasars observed at a luminosity +$L$ radiate at that approximately constant luminosity over some +universal lifetime $t_{Q,\,\rm LB}$ at a particular redshift. We +adopt $l=0.3$ and $t_{Q,\, \rm LB}=10^{7}\,$yr, as is commonly assumed +in theoretical work and suggested by observations (given this +prior) \citep[e.g.][]{YT02,Martini04, Soltan82,YL04,PMN04,Grazian04}, +and similar to the $e$-folding time of a black hole with canonical +radiative efficiency $\epsilon_{r}=0.1$ \citep{Salpeter64} or the +dynamical time in a typical galactic disk or central regions of the +merger. These choices control only the normalization of $\nLp$, and +therefore do not affect most of our predictions. Where the +normalization (i.e.\ value of the constant $t_{Q}$ or $l$) is +important, we allow it to vary in order to produce the best possible +fit to the observations. + +\bigskip + +{\em ``Exponential (Fixed Eddington Ratio) Model.''} A somewhat more +physical model of the quasar light curve is obtained by assuming +growth at a constant Eddington ratio, as is commonly adopted in e.g.\ +semi-analytical models which attempt to reproduce quasar luminosity +functions \citep[e.g.][]{KH00,WL03,V03}. In this model, a black hole +accretes at a fixed Eddington ratio $\eEdd$ from an initial mass +$M_{i}$ to a final mass $M_{f}$ (or equivalently, a final luminosity +$L_{f}=\eEdd\,L_{Edd}(M_{f})$), and then shuts off. This gives +exponential mass and luminosity growth, and the time spent in any +logarithmic luminosity bin is constant, +\begin{equation} +dt/\dlgL = t_{S}\,(\ln(10)/\eEdd) +\end{equation} +for $L_{i}0$ and +$\lstar=\lstar(z)$ always, the density of sources, especially as a +function of observed luminosity at some frequency, evolves in a +non-trivial manner. + +We do not find significant improvement in the fits +if we additionally allow $\nstar$ or $\sstar$ to evolve with redshift +($\Delta\chi^{2}\sim1-2$, depending on the adopted form for the evolution), +and therefore consider only the simplest parameterization above (Equation~\ref{eqn:param.evol}). +We also find acceptable fits for a pure density evolution model, with +$\lstar=$\,constant and $\nstar=\nstar^{0}\,\exp{(k_{N}\,\tau)}$ (both +keeping $\sstar$ fixed and allowing it to evolve as well). +%The best-fit values in this case are +%$(\log\nstar,k_{S},\,\log\lstar,\,\sstar)= +%(-6.11,\,5.17,\,8.80,\,1.25)$ with +%errors $(0.39,0.45,0.68,0.10)$. +However, the fits are somewhat poorer ($\reducechi\approx1$), and the resulting +parameters over-produce the present-day density of low-mass supermassive +black holes and the intensity of the X-ray background by an order of +magnitude, so we do not consider them further. In either case, there is a +considerable degeneracy between the parameters $\sstar$ and $\lstar$, +where a decrease in $\lstar$ can be compensated by a corresponding +increase in $\sstar$. This degeneracy is present +because, as indicated above, the observed luminosity function only +weakly constrains the faint-end slope of $\nLP$. + +The observations shown are insufficient at high redshift to strongly +resolve the ``turnover'' in the total comoving quasar density at +$z\sim2-3$, and thus we acknowledge that there must be corrections to +this fitted evolution at higher redshift, which we address +below. However, as we primarily consider low redshifts, $z +\lesssim 3$, +and show that +the supermassive black hole population and X-ray background are +dominated by quasars at redshifts for which our $\nLp$ distribution is +well determined, this is not a significant source of error in most of +our calculations even if we extrapolate our evolution to $z\gg3$. + +%\clearpage +\begin{figure*} + \centering + \plotone{f9.ps} + %\includegraphics[width=3.7in]{f9.ps} + \caption{Best-fit luminosity function from the pure + peak-luminosity evolution $\nLp$ distribution, for redshifts + $z=0-3$. From our fitted lognormal $\nLP$ distribution, we + simultaneously reproduce the luminosity function in the hard X-ray + (2-10 keV; solid black line), soft X-ray (0.5-2 keV; dashed red + line), and optical B-band (4400 \AA; dotted blue line) at all + redshifts. Moreover, we reproduce the distribution of broad-line + quasars in hard X-ray selected samples (cyan dot-dashed line), as + described in \S~\ref{sec:BLqso}. All quantities have been rescaled to + bolometric luminosities for ease of comparison, using the + corrections of \citet{Marconi04}, with the plotted error bars + representing both quoted measurement errors and the estimated + errors in the bolometric corrections. The observations are from + \citet{Miyaji01} (soft X-ray; red squares), \citet{Ueda03} (hard + X-ray; black circles), \citet{Croom04} (B-band, blue diamonds), + and \citet{Barger05} (X-ray selected broad-line quasars; cyan + crosses). + \label{fig:LF.all}} +\end{figure*} +%\clearpage + +Figure~\ref{fig:LF.all} shows the resulting best-fit PPLE luminosity +functions from the best-fit $\nLP$ distribution, for redshifts +$z=0-3$. This has the best-fit ($\reducechi=0.67$) values +$(\log\lstar,k_{L},\,\log\nstar,\,\sstar)= +(9.94,\,5.61,\,-6.29,\,0.91)$ +% (10.19,\,4.91,\,-6.43,\,0.91)$ +with corresponding errors $(0.29,0.28,0.13,0.09)$. +%$(0.48,0.36,0.28,0.09)$. +Here, $\lstar$ is in solar luminosities and +$\nstar$ in comoving ${\rm Mpc^{-3}\,Myr^{-1}}$. Fitting to the hard +X-ray data alone gives a similar fit, with the slightly different +values $(\log\lstar,k_{L},\,\log\nstar,\,\sstar)= +(9.54,\,4.90,\,-5.86,\,1.03) \pm (0.66,0.43,0.37,0.13)$, +$\reducechi=0.7$ (note the degeneracy between $\lstar$ and $\sstar$ in +the two fits). Our best-fit value of $k_{L}=5.6$ compares favorably to +the value $\sim6$ found by e.g.\ Boyle et al.\ (2000) and Croom et +al. (2004) for the evolution of the break luminosity in the observed +luminosity function, demonstrating that the break luminosity traces +the {\em peak} in the $\nLp$ distribution at all redshifts. These fits +and the errors were obtained by least-squares minimization over all +data points (comparing each to the predicted curve at its redshift and +luminosity), assuming the functional form we have adopted for $\nLP$. + +The agreement we obtain at all redshifts, in each of +the hard X-ray (black solid line), soft X-ray (red dashed line), and +B-band (dark blue dotted line) is good. This is not at all guaranteed +by our procedure, as the fit is highly over-constrained, because we +fit three luminosity functions each at five redshifts to only four +free parameters. Of course, the choice of the functional form for $\nLp$ +ensures that we should be able to reproduce at least one luminosity +function and its evolution (e.g.\ the hard X-ray luminosity function, +which is least affected by attenuation), but our modeling of the +column density distributions in mergers allows us to simultaneously +reproduce the luminosity functions in different wavebands without +imposing assumptions about obscured fractions or sources of +attenuation. Expressed as bolometric luminosity functions, $\phi_{B}$, +$\phi_{SX}$, and $\phi_{HX}$ would be identical in the absence of +obscuration, similar to the predicted $\phi_{HX}$ as obscuration is +minimal in the hard X-ray. + +%\clearpage +\begin{figure} + \centering + \plotone{f10.ps} + %\includegraphics[width=3.7in]{f10.ps} + \caption{Hard X-ray (thick), soft X-ray (thin), and B-band + (dot-dash) LFs determined from our model of quasar lifetimes and + column densities, based on a distribution of intrinsic source + properties fitted to the observed hard X-ray LF + and the limiting magnitudes of observed samples, at the different + redshifts shown. All quantities are rescaled to bolometric + luminosities with the bolometric corrections of \citet{Marconi04}. + Symbols show the observed LFs for hard X-rays + \citep[][diamonds]{Ueda03}, soft X-rays + \citep[][triangles]{Miyaji00}, and B-band + \citep[][crosses]{Boyle00}. Reproduced from \citet{H05d}. + \label{fig:LF.lowz}} +\end{figure} +%\clearpage + +For redshifts $z\leq1$, we reproduce in our Figure~\ref{fig:LF.lowz}, +Fig.~2 of \citet{H05d}, which shows in detail the agreement between +hard X-ray \citep{Ueda03}, soft X-ray \citep{Miyaji00}, and optical +\citep{Boyle00} luminosity functions resulting from the time and +luminosity dependent column density distributions derived from the +simulations. The differential extinction predicted for different +frequencies (and magnitude limits) of observed samples based on the +column density distributions in our simulations accounts for the +different shape of the luminosity function in each band, and the +evolution of the luminosity function with redshift is driven by a +changing $\lstar$, the peak of the $\nLp$ distribution +(Equation~\ref{eqn:param.evol}). We emphasize that in our analysis, +the key quantity constrained by observations is the fitted $\nLP$ +distribution with redshift. All other quantities and distributions are +derived from the basic input physics of our simulations, with no +further assumptions or adjustable factors in our modeling beyond the +prescription for Bondi (Eddington-limited) accretion and +$\sim5\%$ energy deposition in the ISM, which are themselves +constrained by observations and theory as discussed in +\S~\ref{sec:methods} and in Di Matteo et al.\ (2005). + +We can, of course, fit the previously defined simpler model of quasar +lifetimes, either a ``light-bulb'' or exponential light curve/fixed +Eddington ratio model, and obtain an identical hard X-ray luminosity +function. We determine these fits (see also Equation~\ref{eqn:nLp.LB} +\& \ref{eqn:nLp.Edd}) and use them throughout when we compare the +predictions of such models (described in \S~\ref{sec:altmodels}) to +those of our simulated quasar lifetimes in our subsequent +analysis. Applying a standard torus model to any model of the +luminosity function reproduces, by design, the mean offset between the +B-band and hard X-ray luminosity functions, as the parameters of this +model are {\it tuned} to reproduce this offset. As many observations +show, the fraction of broad-line quasars increases with luminosity +\citep{Steffen03,Ueda03,Hasinger04,sazrev04,Barger05,Simpson05}, and +so reproducing the relationship between B-band and hard X-ray +luminosity functions requires adding parameters to the standard torus +model which allow luminosity-dependent scalings, i.e.\ the class of +``receding torus'' models. These, again by construction, reproduce the +distinction between hard X-ray and B-band quasar luminosity functions, +including the dependence of this difference on luminosity. These are, +however, phenomenological models designed to fit these +observations. Our simulations, on the other hand, provide a +self-consistent description of the column density, which predicts the +{\em differences} between hard X-ray, soft X-ray, and optical +luminosity functions without the addition of tunable parameters or +model features designed to reproduce these observations. + +Our fits are accurate down to low luminosities, as is clear from our +prediction for the X-ray luminosity function at bolometric +luminosities $L\sim\Lcut{9}$. Furthermore, we have calculated the +predicted $z\lessim0.1$ luminosity function in the B-band as well as +in H$\alpha$ emission, using the conversion between the two from +\citet{Hao05} and comparing directly to their luminosity functions for +Seyfert galaxies and low-luminosity active galactic nuclei (AGN) (both +type I and II), and find that our distribution $\nLp$ and model for +quasar lifetimes and obscuration reproduces the complete observed +luminosity function down to a B-band luminosity $M_{B}\sim-16$. +Although our prediction falls below the observed Seyfert luminosity +function at fainter magnitudes, there is no reason to believe that +mergers should be responsible for all nuclear activity at these +luminosities (and indeed alternative fueling mechanisms for such faint +objects likely exist) - it is surprising, in fact, that this picture +reproduces the observed AGN activity to such faint luminosities. + +Using the bolometric corrections of \citet{Elvis94} instead of +\citet{Marconi04} results in a significantly steeper cutoff in the +luminosity function at high bolometric luminosities, as the bolometric +luminosity inferred for the brightest observed X-ray quasars is almost +an order of magnitude smaller using the \citet{Elvis94} +corrections. However, this is because the \citet{Elvis94} bolometric +corrections do not account for any dependence on luminosity, and +further the quasars in the sample of Elvis et al.\ (1994) are X-ray +bright \citep{ERZ02}, whereas it has been well-established that the +ratio of bolometric luminosity to hard or soft X-ray luminosity +increases with increasing luminosity +\citep[e.g.,][]{Wilkes94,Green95,VBS03,Strateva05}. Recent comparisons +between large samples of quasars selected by both optical and X-ray +surveys \citep{RisalitiElvis05} further suggests that this is an +intrinsic correlation, not driven by e.g.\ the dependence of +obscuration on luminosity. For a direct comparison of the bolometric +luminosity functions resulting from the two corrections, we refer to +\citet{H05d}. Our analysis uses the form for the UV to X-ray flux +ratio, $\alpha_{\rm OX}$, from \citet{VBS03}, but our results are +relatively insensitive to the different values found in the +literature. It is important to account for this dependence, as it +creates a significant difference in the high-luminosity end of the +bolometric quasar luminosity function and implies that a +non-negligible fraction of the brightest quasars are not seen in +optical surveys \citep[see the discussion in][]{Marconi04,Richards05}. + +%\clearpage +\begin{figure*} + \centering + \plotone{f11.ps} + %\includegraphics[width=3.7in]{f11.ps} + \caption{Running our predicted broad-line luminosity function + (determined in \S~\ref{sec:LF}, \ref{sec:BLqso}) to high redshifts, with either total + density (dashed lines) or break luminosity ($\lstar$; solid lines) + decreasing exponentially with redshift above $z=2$. In each panel, + our prediction is shown for the minimum and maximum redshift of + the corresponding interval from the COMBO-17 luminosity function + of \citet{Wolf03} (W03; black squares). Other references for the + observations shown are: R05 - \citet{Richards05}, WHO - + \citet{WHO94}, F01 - \citet{Fan01}, SSG - \citet{SSG}, KDC - + \citet{KDC}. + \label{fig:LF.highz}} +\end{figure*} +%\clearpage + +Finally, our fitted form for the evolution of the break luminosity, +with $\lstar\propto\exp{(k_{L}\tau)}$, cannot continue to arbitrarily +high redshift. At redshifts $z\gtrsim2-3$, this asymptotes +because $\tau\rightarrow 1$, whereas the observed quasar population +declines above $z\sim2$. This difference is not important for most of +our calculated observables, as they are either independent of +high-redshift evolution or evolve with cosmic time in some fashion as +$\propto\int{\nLp\,{\rm d}t}$, with little time and thus negligible +contributions to integrated totals at high redshifts. However, some +quantities, in particular the high-mass end of the black hole mass +function (see \S~\ref{sec:smbh}), which is dominated by the small +number of the brightest quasars at high redshifts, can receive large +relative contributions from these terms. Therefore, it is important in +estimating these quantities to be aware of the turnover in the quasar +density at high redshifts. + +We quantify this in Figure~\ref{fig:LF.highz}, where we show the +predicted broad-line luminosity function (where the broad-line phase +is determined below in \S~\ref{sec:smbh}) in six luminosity intervals +from $z\sim1.2-4.8$. The intervals are those of the COMBO-17 +luminosity function from \citet{Wolf03}, but we further compare to the +observed luminosity functions of \citet{WHO94}, \citet{SSG}, +\citet{KDC}, \citet{Fan01}, and \citet{Richards05} at the appropriate +(labeled) redshifts. At each redshift $z>2$, we take the +fitted $\nLp$ distribution above (Equations~\ref{eqn:nLp.lognorm},\ +\ref{eqn:param.evol}) and rescale it according to an exponential +cutoff: either pure density evolution (PDE), +$\nLp\rightarrow\nLp\times10^{-\alpha_{\rm PDE}\,(z-2)}$, or pure peak +luminosity evolution (PPLE), +$\lstar\rightarrow\lstar\times10^{-\alpha_{\rm PPLE}\,(z-2)}$. +Fitting to the data gives $\alpha_{\rm PDE}\sim0.65$ and $\alpha_{\rm +PPLE}\sim0.55$, ($\reducechi\approx1.3$ for both) in reasonable +agreement with the density evolution of e.g.\ Fan et al.\ (2001). We +note that this evolution, extrapolated as far as $z\sim6$, is +consistent also with the constraints on $z\sim6$ quasars from +\citet{Fan03}, especially in the PPLE case. + +In each panel, we plot the resulting broad-line luminosity function +(see \S~\ref{sec:BLqso}), for both the minimum and maximum redshift of +the redshift bin, and both the PPLE (solid lines) and PDE (dashed +lines) cases. The degeneracy between these +possibilities is well-known, as +current observations do not resolve the break in the luminosity +function. Furthermore, the predicted luminosity function should be +considered uncertain especially at low luminosities, as the quasar +lifetime at these luminosities and redshifts can become comparable to +the age of the Universe, at which point our formalism for the +luminosity function as a function of $\nLp$ becomes inaccurate. +However, we are able to make testable predictions, based on +differences between the two models in integrated {\em galaxy} +properties (for example, color-magnitude diagrams of red sequence +galaxies at low masses or the fraction of recently formed spheroids as +a function of mass and redshift), which distinguish the PPLE and PDE +models for the evolution of the quasar luminosity function at +$z\gtrsim2-3$ \citep{H05e}. Owing to these degeneracies and the poor +constraints on the observed high-redshift luminosity functions, we +have not considered them (those at $z>3$) in our fits to $\nLp$, but +use them here to roughly constrain the turnover in the quasar +density above $z\sim2$ (i.e.\ fitting to $\alpha_{\rm PDE}$ and +$\alpha_{\rm PPLE}$). Which form of the turnover we use makes little +difference in our subsequent analysis, but, as discussed above, +including {\em some} turnover is important in calculating select +quantities such as the extreme high-mass end of the black hole mass +function. + +\subsection{The Observed \NH\ Distribution} +\label{sec:NHdistrib} + +%\clearpage +\begin{figure*} + \centering + \plotone{f12.ps} + %\includegraphics[width=3.7in]{f12.ps} + \caption{Left panel: Distribution of column densities expected + from the characteristic quasars $\Lp\sim\lstar$ of the luminosity + function observed in optical samples, for a standard torus model + of quasar obscuration (dashed), + a receding torus model (dotted), and the distributions of column densities + as a function of instantaneous and peak luminosity in our simulations (solid). + The distribution of neutral + \NHI\ values is obtained requiring an observed B-band luminosity + $>\Lcut{11}$. The smooth red curve is the best-fit to the + $E_{B-V}$ distribution of bright SDSS quasars with $z<2.2$, from + \citet{Hopkins04}, rescaled to column densities and plotted about + a peak (mode) \NHI\ (undetermined in Hopkins et al.\ 2004) of + $\nhi\approx0.5\times10^{21}\,{\rm cm^{-2}}$. The $i$-band + absolute magnitude limit imposed in the observed sample, + $M_{i}<-22$, corresponds approximately to our plotted B-band limit + $\LBo>\Lcut{11}$. Reproduced from \citet{H05b}. Right panel: + Integrated distribution of total (neutral and ionized) column + densities expected for a complete hard X-ray sample, from the + column densities of our simulations and the $\nLp$ + distribution. The distribution below $10^{21}\ {\rm cm^{-2}}$ is + shown (dot-dashed line) and re-plotted as a single bin at + $\nh=10^{20}\ {\rm cm^{-2}}$ for our modeled columns. Data shown are the results of + \citet{Treister04} (blue squares) and \citet{Mainieri05} (red + circles), with assumed Poisson errors. Solid squares assume an + intrinsic photon index $\Gamma=1.9$, for the soft X-ray quasar + spectrum, open squares $\Gamma=1.7$. + \label{fig:NH.distrib}} +\end{figure*} +%\clearpage + +Given the column density distributions and quasar lifetimes calculated +from our simulations in \S~\ref{sec:methods}, and the quantity $\nLP$ +determined above (\S~\ref{sec:fullLF}), we can predict the +distribution of column densities observed in a given sample. This will +depend not only on the range of observed luminosities and the redshift +of the sample, but also on the minimum observed magnitude and +frequency (i.e.\ the selection function) of the sample. For a nearly +complete sample or estimate of the luminosity function, for example +the hard X-ray luminosity function, at least to $\nh\sim10^{25}\ {\rm +cm^{-2}}$, we can integrate the $\nh(L,\Lp)$ distribution over +the $\nLP$ distribution (weighted by the lifetime at $L$). + +Figure \ref{fig:NH.distrib} plots the resulting distribution of column +densities for this analysis. The left panel reproduces and expands +upon a portion of Fig.~3 of \citet{H05b}, showing the distribution of +column densities (scaled linearly) expected from the characteristic +quasars $\Lp\sim\lstar$ of the luminosity function observed in optical +samples, based on the simulated column density distributions as a +function of luminosity and peak luminosity (solid black line). +Specifically, we plot the distribution of neutral \NHI\ values +requiring that the observed B-band luminosity be above some reference +value $\LBm$. The smooth curve shown is the best-fit to the $E_{B-V}$ +distribution of bright SDSS quasars with $z<2.2$, from +\citet{Hopkins04}. The curve has been rescaled in terms of the column +density (inverting our gas-to-dust prescription) and plotted about a +peak (mode) \NHI\ (undetermined in Hopkins et al.\ 2004) of +$\nhi\approx0.5\times10^{21}\,{\rm cm^{-2}}$. The observationally +implied $E_{B-V}$ distribution is determined from fitting to the +distribution of photometric reddening in all SDSS bands (i.e.\ using +the five-band photometry as a proxy for spectral fitting) in Sloan +quasars, relative to the modal quasar colors at each redshift, for +quasars with an absolute magnitude limit $M_{i}<-22$. The $i$-band +absolute magnitude limit imposed in the observed sample, $M_{i}<-22$, +corresponds approximately to our plotted B-band limit +$\LBo>\Lcut{11}$. This estimate does not account for bright but +strongly reddened quasars having their colors altered to the point +where color selection criteria of quasar surveys will not include +them. However, this effect would only serve to bring our distribution +into better agreement with observations, as it would slightly lower +the high-\NHI\ tail. We also consider the predictions of a standard +torus model and receding (luminosity-dependent) torus model in the +figure (dashed and dotted lines, respectively). These should not be +taken literally in this case -- they reflect that these +phenomenological models do not predict the distribution of +low/moderate column densities, but rather assume that all lines +of sight not intersecting the torus are ``unobscured,'' and encounter +some constant, small column density (usually chosen to be +$\nh\sim10^{20}\,{\rm cm^{-2}}$). + +The right panel of \ref{fig:NH.distrib} shows the integrated +distribution (in $\log\nh$) for a complete hard X-ray +sample, both as predicted from our simulations based on the joint +distribution of column density, luminosity, and peak luminosity +(solid), and for both the standard torus model (dashed) and receding +torus model (dotted) described in \S~\ref{sec:altmodels}. The data +shown are the results of \citet{Treister04} (blue squares) and +\citet{Mainieri05} (red circles), with assumed Poisson errors, from +multiband {\it Chandra} and {\it HST} observations of GOODS +fields. The solid squares are obtained by assuming an intrinsic photon +index for the soft X-ray quasar spectrum of $\Gamma=1.9$, the open +squares assuming $\Gamma=1.7$. For the sake of direct comparison with +observed distributions, objects with $\nh<10^{21}\ {\rm cm^{-2}}$, for +which only an upper limit to the column density would be determined in +X-ray observations, are grouped together and plotted as a single bin +at $\nh=10^{20}\ {\rm cm^{-2}}$. The actual distribution below +$10^{21}\ {\rm cm^{-2}}$ is shown as a dot-dashed line. We note that +our model of the quasar spectrum assumes a photon index $\Gamma=1.9$ +in the soft X-ray, but this has no effect on the column densities +calculated from the surrounding gas in our simulations. + +The agreement between the observed column density distribution and the +result of our simulations once the same selection effect is applied +supports our model for quasar evolution, and the good agreement +extends to both optical and X-ray samples. Probing to fainter +luminosities or frequencies less affected by attenuation broadens the +column density distribution, as is seen from the inferred column +density distributions in the X-ray. This broadening occurs because, +at lower luminosities, observers will see both intrinsically bright +periods extinguished by larger column densities (broadening the +distribution to larger \NH\ values) and intrinsically faint periods +with small column densities (broadening the distribution to smaller +\NH\ values). The distribution as a function of reference luminosity +is a natural consequence of the dynamics of the quasar +activity. Throughout much of the duration of bright quasar activity, +column densities rise to high levels as a result of the same process +that feeds accretion, producing the well-known reddened population of +quasars \citep[e.g.][]{Webster95,Brotherton01,Francis01, +Richards01,Gregg02,White03,Richards03}, extending to bright quasars +strongly reddened by large \NHI. Furthermore, a significant number of +quasars are extinguished from optical samples or attenuated to lower +luminosities, giving rise to the distinction between luminosity +functions in the hard X-ray, soft X-ray, and optical. + +The standard torus model described in \S~\ref{sec:altmodels}, although +unable to predict the distribution of column densities seen in +optically, relatively unobscured quasars, does a fair job of reproducing +the observed distribution of X-ray column densities. The parameters of +the model are, of course, chosen to reproduce the data shown +\citep[the model parameters are taken +from][]{Treister04}. Nevertheless, our prediction is still a +better fit to the observed distribution, with +$\reducechi\approx2$ as opposed to $\reducechi\approx7$ (although the +absolute values depend on the estimated systematic +errors in the column density estimations). The receding torus model +fares even more poorly in reproducing the observed column density +distributions, and is ruled out at high significance +($\reducechi\approx10$), although this can be alleviated if the +observed samples are assumed to be incomplete above +$\nh\sim10^{23}\,{\rm cm^{-2}}$. This disagreement results because, in +order to match the observed scaling of broad-line fraction with +luminosity (see \S~\ref{sec:BLqso} below), this model assumes a +larger covering fraction for the torus at lower luminosities, +normalized to a similar obscured fraction as the standard torus model +near the break in the observed quasar luminosity function. However, +since quasars with luminosities below the break dominate the total +number counts, this predicts that the cumulative column density +distribution must be significantly more dominated by objects with +large covering angles, giving a larger Compton-thick population, +inconsistent with the actual observed column density distribution. + +Although we do not see a significant fraction of extremely +Compton-thick column densities $\nh\gtrsim10^{26}\,{\rm cm^{-2}}$ in +the distributions from our simulations, our model does not rule out +such values. It is possible that bright quasars in unusually massive +galaxies or quasars in higher-redshift, compact galaxies which we have +not simulated may, during peak accretion periods, reach such values in +their typical column densities. Moreover, as our model assumes +$\sim90\%$ of the mass of the densest gas is clumped into cold-phase +molecular clouds, a small fraction of sightlines will pass through +such clouds and measure column densities similar to those shown for +the ``cold phase gas'' in, e.g.\ Figure 2 of \citet{H05a}, +$\nh\gtrsim10^{25-26}{\rm cm^{-2}}$. + +Furthermore, we have not determined the ``shape'' at any instant of +the obscuration (e.g.\ the dependence of obscuration on radial +direction), as in practice, for most of the most strongly obscured +phases in peak merger activity, the central regions of the merging +galaxies are highly chaotic. Generally, the scale of the obscuration +in the peak merger phases is $\sim100\,$pc, quite different than that +implied by most traditional molecular torus models, but we note that +our resolution limits, $\sim 20\,$pc in the dense central regions of +the merger, prevent our ruling out collapse of gas in the central +regions into a smaller but more dense torus. However, several efforts +to model traditional tori through radiative transfer simulations +\citep[e.g.,][]{GD94,Schartmann05} suggest significant column +densities produced on scales of $\sim100-200\,$pc, comparable to our +predictions, and we note that only the solid angle covered by a torus, +not the absolute torus scale, is constrained in the typical +phenomenological torus model \citep[e.g.][]{Antonucci93}. + +Whether the obscuration of bright quasars originates on larger scales +than is generally assumed is observationally testable, either through +direct probes of polarized scattered light tracing the +obscuring/reflecting structure \citep[e.g.,][]{Zakamska05}, or through +correlations between obscuration and e.g.\ host galaxy morphologies +and inclinations \citep[e.g.,][]{Donley05}. These larger scales +typical of the central regions of a galaxy are widely accepted as the +scales of obscuration in starbursting systems (e.g.\ Soifer et +al. 1984a,b; Sanders et al.\ 1986, 1988a,b; for a review, see e.g.\ +Soifer et al.\ 1987), which in our modeling is associated with rapid +obscured quasar growth and precedes the quasar phase. Thus, it is +natural to associate obscuration with these large scales in any +picture which associates starbursts and rapid black hole growth or +quasar activity, as opposed to the smaller scales $\sim$\,pc +implied by torus models primarily developed to reproduce observations of +quiescent, low-luminosity Type II AGN, which are usually not directly +associated with merger activity. These low-luminosity AGN are in a +relaxed state, suggesting the possibility that the remaining cold gas +in the central regions of our merger remnants will collapse once the +violent effects of the merger and bright quasar phase have passed, +producing a more traditional small torus in a quiescent nucleus. The +central point is that regardless of the form of obscuration, the +typical magnitude of the obscuration is a strongly evolving function +of time, luminosity, and host system properties, and the observed +column density distributions reflect this evolution. + +\section{Broad-Line Quasars} +\label{sec:BLqso} +\subsection{Determining the Broad-Line Phase} +\label{sec:whenBL} + +Optical samples typically identify quasars through their colors, +relying on the characteristic non-stellar power-law continua of such +objects. However, observations of X-ray selected AGN show a large +population of so-called Type 2 AGN, most of which have Seyfert-like +luminosities and typical spectra in X-rays and wavelengths longward of +$1\,\mu$m \citep[e.g.,][]{Elvis94}, but are optically obscured to the +point where no broad lines are visible. Their optical continua, in +other words, resemble those of typical galaxies and thus they are not +identified by conventional color selection techniques in optical +quasar surveys. Traditional unification models \citep{Antonucci93} +have postulated a static torus as the explanation for the existence of +the Type 2 population, with such objects viewed through the dusty +torus and thus optically obscured. Moreover, both synthesis models +of the X-ray background +\citep{SW89,Madau94,Comastri95,Gilli99,Gilli01} and recent direct +observations in large surveys \citep[e.g.,][]{Zakamska04,Zakamska05} +indicate the existence of a population of Type 2 quasars, with similar +obscuration but intrinsic (unobscured) quasar-like luminosities. + +Observations of both radio-loud +\citep{HGD96,SRL99,Willott00,SR00,GRW04} and radio-quiet +\citep{Steffen03,Ueda03,Hasinger04,sazrev04,Barger05,Simpson05} +quasars, however, have shown that the broad-line fraction increases +with luminosity, with broad-line objects representing a large fraction +of all AGN at luminosities above the ``break'' in the luminosity +function and rapidly falling off at luminosities below the break. +Modifications to the standard torus unification model explain this via +a luminosity-dependent inner torus radius \citep{Lawrence91}, but this +represents a tunable modification to a purely phenomenological +model. Furthermore, as the observations have improved, it has become +clear that even these luminosity-dependent torus models cannot produce +acceptable fits to the broad line fraction as a function of luminosity +\citep[e.g.,][]{Simpson05}. However, we have shown above that the +obscuring column, even at a given luminosity, is an evolutionary +effect, dominated by different stages of gas inflow in different +merging systems giving rise to varying typical column densities, +rather than a single static structure. It is of interest, then, to +calculate when quasars will be observed as broad-line objects, and to +compare this with observations of broad line quasars and their +population as a function of luminosity. + +%\clearpage +\begin{figure*} + \centering + \plotone{f13.ps} + %\includegraphics[width=3.7in]{f13.ps} + \caption{Intrinsic (right panels) and median attenuated (left + panels) B-band luminosity of the quasar (thick line) and host + galaxy (integrated over all stars, thin line; ignoring bulge + stars, dotted line) as a function of time. Results are shown from + three representative simulations: A2, A3, and A5 (see \S~\ref{sec:sims}) + with $\qeos=1.0,\, \zgal=0$, and virial velocities + $\vvir=113,\, 160,\ {\rm and}\ 320\, {\rm km\,s^{-1}}$. Each + quasar should be observable as a broad-line AGN when $L_{\rm + B,\,QSO}\gtrsim L_{\rm B,\,host}$. Colors show the stellar light curve + with different gas fractions $\fgas=1.0$ (black), $\fgas=0.4$ (blue), + and $\fgas=0.2$ (red); quasar light curves are similar for each gas fraction. + \label{fig:BL.in.sims}} +\end{figure*} +%\clearpage + +Figure~\ref{fig:BL.in.sims} shows the B-band luminosity as a function +of time for both the quasars and host galaxies in three representative +simulations: the A2, A3, and A5 cases described in detail in +\S~\ref{sec:sims}. These simulations each have $\fgas=1.0,\, +\qeos=1.0,\, \zgal=0$, with virial velocities $\vvir=113,\, 160\, {\rm +and}\ 320\, {\rm km\,s^{-1}}$, with resulting final black hole masses +$\mbhf=3\times10^{7},\ 3\times10^{8},\ {\rm and}\ 2\times10^{9}\, +M_{\sun}$, respectively. The thick line in each case shows the quasar +B-band luminosity, and the thin line shows the integrated B-band +luminosity of all stars in the galaxy. New stars are formed +self-consistently in the simulations according to the ISM gas +properties, equation of state and star formation model described in +\citet{SH03}, with the age and metallicity taken from the local +star-forming ISM gas, which is enriched by supernova feedback from +previous star formation. We then use the stellar population synthesis +model of \citet{Bruzual03} to determine the B-band luminosity (the +B-band mass-to-light ratio) of new stars based on the stellar age and +metallicity. The dotted line shows the result neglecting bulge +particles, which must be initialized at the beginning of the +simulation with random or uniform ages and metallicities instead of +those quantities being determined self-consistently from the +simulation physics. The right panels plot the intrinsic values of +these quantities, and the left panels plot the median observed values +of these quantities, where we have used our method for determining +column densities and dust attenuation (\S~\ref{sec:NH}) to every star +and bulge particle for each line of sight. + +Unfortunately, the host galaxy luminosity does {\em not} scale +with instantaneous and peak quasar luminosity as do, for example, the +quasar lifetime and obscuration. Rather, there are important +systematic dependencies, the largest of which is the dependence on host galaxy gas +fraction. If the host galaxies are more massive, more concentrated, +or have a weaker ISM equation of state pressurization, then they will +more effectively drive gas into the central regions and maintain high +gas densities for longer periods of time, as the deeper potential well +or lack of gas pressure requires more heat input from the quasar +before the gas can be expelled. These conditions will generally +produce a quasar with a larger peak luminosity (final black hole +mass), but also form more new stars, meaning that the B-band relation +between host and quasar luminosity is roughly preserved. + +However, the the black hole consumes only a small fraction of the +available gas (comparison of e.g.\ the stellar mass and black +hole mass suggests the black hole consumes $\sim0.1\%$ of the gas +mass), and so, at least above some threshold $\fgas\lesssim0.1$, the +quasar peak luminosity does not significantly depend on the galaxy gas +fraction (see, e.g.\ Figure 2 of Robertson et al.\ 2005b). But, the +mass of new stars formed {\it during} the merger does strongly depend on the +available gas. For example, simulations which are otherwise identical +but have initial $\fgas=0.2,\ 0.4,\ 0.8,\ 1.0$ (i.e.\ an increasing +fraction of the initial disk mass in gas instead of stars) produce +similar peak quasar luminosity and final total stellar mass (within +$\sim30\%$ of one another), reflecting the conversion of most +gas into stars and the fact that the peak quasar luminosity is +determined more by the depth of the potential well than the total +available gas supply. But, the mass of {\it new} +stars formed in a merger scales +roughly as $M_{\ast,\, \rm new}\propto \fgas$ (as it must if the +initial gas fraction does not change the final total stellar mass), +and since young stellar populations dominate the observed B-band +luminosity (especially during the peak merger and starburst phases +associated with the bright quasar phase of interest), this implies +roughly that $L_{B}\propto\fgas$. + +We demonstrate this explicitly in Figure~\ref{fig:BL.in.sims}, where +we show in each panel the host galaxy and stellar B-band light curves +for otherwise identical simulations with different gas fractions, +$\fgas=0.2\ {\rm (red)},\ 0.4\ {\rm (blue)},\ {\rm and}\ 1.0\ {\rm +(black)}$. In each of these cases, the quasar light curve is nearly +identical (we show only the $\fgas=1.0$ quasar lightcurve, for +clarity, but the others are within $\sim30\%$ of the curve shown at +most times, with no systematic offset). + +In order for a quasar to be classified as a ``broad-line'' object, the +optical spectrum must be visible and identified as such in the +observed sample. This is clearly related to the ratio of quasar to +host galaxy luminosity, but the threshold for classification is not +obvious. In an X-ray or IR-selected sample, optical follow-up should +be able to disentangle host galaxy light and identify quasar +broad-line spectra with fluxes a factor of several fainter than the +host. However, automated optical selection based on color or +morphological criteria might well exclude objects unless the quasar +luminosity is a factor of several greater than that of the host +galaxy. Therefore, there is significant systematic uncertainty in the +theoretical definition of a broad-line quasar. To first order, based +on the above arguments, we can classify ``broad-line quasars'' as +objects in which the quasar optical luminosity is larger than some +multiple $f_{\rm BL}$ of the host galaxy optical luminosity. Because +the relevant ratio is different depending on the survey and selection +techniques, we consider the range $f_{\rm BL} = 0.3-3$, with a rough +median $f_{\rm BL}=1$. Furthermore, because our simulations do not +allow us to model the broad-line regions of the quasar or spectral +line structures as influenced by e.g.\ reddening and dust absorption, +we adopt the B-band luminosity of the quasar and host galaxy as +a proxy for optical luminosity and more complex (but often quite +sample-specific) color and morphological selection criteria. + +%\clearpage +\begin{figure} + \centering + \plotone{f14.ps} + %\includegraphics[width=3.7in]{f13.ps} + \caption{Ratio of observed (attenuated) B-band quasar luminosity to host galaxy luminosity + as a function of the ratio of instantaneous to peak quasar bolometric luminosity. Results are + from simulations A2 (black diamonds), A3 (blue circles), and A5 (red $\times$'s) + (the same simulations shown in Figure~\ref{fig:BL.in.sims}) + with $\qeos=1.0,\, \zgal=0$, and virial velocities + $\vvir=113,\, 160,\ {\rm and}\ 320\, {\rm km\,s^{-1}}$. + Each panel shows the same simulations except for a + different initial gas fraction $\fgas = 0.2,\ 0.4,\ 0.8,\ 1.0$ as labeled. Solid lines are the + predictions of Equation~\ref{eqn:BL.scaling}. + \label{fig:test.BL}} +\end{figure} +%\clearpage + +In Figure~\ref{fig:BL.in.sims}, the B-band host galaxy luminosity is +quite flat as a function of time, relative to the quasar B-band +luminosity, and is roughly given by $L_{B}^{\rm gal}/L_{\sun}\sim +M_{\ast,\, \rm new}/M_{\sun}$, where $M_{\ast,\, \rm new}$ is the mass +of new stars formed in the merger. As noted above, this scales +approximately linearly with initial gas fraction at fixed final total +stellar mass $M_{\ast}$, giving $L_{B}^{\rm gal}/L_{\sun}\approx +c_{\rm gal} (M_{\ast}/M_{\sun})\fgas$, where $c_{\rm gal}$ is a +correction of order unity which we can fit from the simulations +(essentially a mean mass-to-light ratio for the newly formed stars). +The bolometric correction of the quasar is usually defined by $L_{\rm +bol}^{\rm qso}=c_{B}L_{B}^{\rm qso}$, and the quasar peak luminosity +is $\Lp=c_{L}\, L_{\rm Edd}(M_{\rm BH}^{f})$, where again $c_{L}$ is a +correction factor of order unity which we can calculate from our form +for the quasar lifetime (see Equation~\ref{eq:Mbhf}) or measure in the +simulations. + +If we require that the quasar B-band luminosity be +larger than a factor $f_{\rm BL}$ of the host galaxy B-band +luminosity, we obtain +\begin{equation} +L_{\rm bol}^{\rm qso}/L_{\sun}>f_{\rm BL} c_{B}\, c_{\rm gal} (M_{\ast}/M_{\sun}) \fgas. +\end{equation} +Dividing this through by $\Lp$, we have +\begin{equation} +\frac{L_{\rm bol}^{\rm qso}}{\Lp}\gtrsim0.4\,\fgas\,f_{\rm BL}\ +{\Bigl(}\frac{c_{\rm gal}}{1.0}{\Bigr)} +{\Bigl(}\frac{c_{B}}{12.0}{\Bigr)} +{\Bigl(}\frac{M_{\rm BH}^{f}/M_{\ast}}{0.001}{\Bigr)}^{-1} +{\Bigl(}\frac{c_{L}}{1.24}{\Bigr)}^{-1}. +\end{equation} +We can test this scaling relation against the results of our simulations, +and do so in Figure~\ref{fig:test.BL}. Rearranging the equations above +gives +%\begin{equation} +%\begin{split} +%\frac{L_{B}^{\rm qso}}{L_{B}^{\rm gal}} \approx +%&\ 3.4\,\fgas^{-1}\,\frac{L_{\rm bol}^{\rm qso}}{\Lp}\\ +%&\times{\Bigl(}\frac{c_{\rm gal}}{1.0}{\Bigr)}^{-1} +%{\Bigl(}\frac{c_{B}}{12.0}{\Bigr)}^{-1} +%{\Bigl(}\frac{M_{\rm BH}^{f}/M_{\ast}}{0.001}{\Bigr)} +%{\Bigl(}\frac{c_{L}}{1.24}{\Bigr)}, +%\end{split} +%\label{eqn:BL.predict} +%\end{equation} +\begin{eqnarray} +\frac{L_{B}^{\rm qso}}{L_{B}^{\rm gal}} &\approx +&\ 3.4\,\fgas^{-1}\,\frac{L_{\rm bol}^{\rm qso}}{\Lp}\nonumber\\ +&&\times{\Bigl(}\frac{c_{\rm gal}}{1.0}{\Bigr)}^{-1} +{\Bigl(}\frac{c_{B}}{12.0}{\Bigr)}^{-1} +{\Bigl(}\frac{M_{\rm BH}^{f}/M_{\ast}}{0.001}{\Bigr)} +{\Bigl(}\frac{c_{L}}{1.24}{\Bigr)}, +\label{eqn:BL.predict} +\end{eqnarray} +which we can compare to our direct calculation of +$L_{B}^{\rm qso}/{L_{B}^{\rm gal}}$ and $L_{\rm bol}^{\rm qso}/\Lp$ +for each simulation snapshot. + +Ultimately, we are not interested so much in the intrinsic B-band +luminosity of the quasar and host galaxy, but rather the observed +luminosities; i.e.\ we are interested in the ratio ${L_{B, \rm\ +obs}^{\rm qso}}/{L_{B, \rm\ obs}^{\rm gal}} = ({L_{B}^{\rm +qso}}/{L_{B}^{\rm gal}})\,(\exp\{-(\tau_{Q}-\tau_{G})\})$, where +$\tau_{Q}$ and $\tau_{G}$ are ``effective'' optical depths which we +use to denote the mean attenuation of quasar and host galaxy B-band +luminosities, respectively. We have considered the distribution of +column densities attenuating the quasar as a function of instantaneous +and peak quasar luminosity in detail in \S~\ref{sec:NHfunction} above; +the attenuation of the host galaxy as a function of luminosity, +observed band, halo mass, and star formation rate are discussed in +detail in \citet{Jonsson05}. Combining these fits gives, roughly, +$(\exp\{-(\tau_{Q}-\tau_{G})\})\sim (M_{\rm +BH}^{f}/10^{8}\,M_{\sun})^{0.16}$, but a better approximation can be +determined directly from the simulations. + +This scaling can be understood roughly using toy models of uniformly +mixed luminous sources within the galaxy described by +\citet{Jonsson05}, after accounting for the fact that the luminosity +(star formation rate) dependent portion of the attenuation scales with +luminosity in a similar manner to our quasar attenuation (compare our +$\tau_{Q}\propto\nh\propto L_{\rm qso}^{0.43-0.54}$ to their +$\tau_{G}\propto L_{\rm B,\ gal}^{0.55}$). The key consequence of this +is that more massive systems (higher bulge and black hole masses) have +their host galaxy light proportionally more attenuated in mergers, +meaning that (as suggested by the comparison of light curves in +Figure~\ref{fig:BL.in.sims}) the quasar is more likely to be observed +with an optical luminosity larger than that of its host. + +Figure~\ref{fig:test.BL} plots the ratio of the observed (attenuated) +B-band quasar luminosity to the observed host galaxy B-band luminosity +as a function of the ratio of instantaneous to peak quasar bolometric +luminosity. We show the results for four different gas fractions +$\fgas = 0.2,\ 0.4,\ 0.8,\ 1.0$ as labeled. For each gas fraction, we +consider our simulations A2 (black diamonds), A3 (blue circles), and +A5 (red $\times$'s) (the same simulations shown in +Figure~\ref{fig:BL.in.sims}) with $\qeos=1.0,\, \zgal=0$, and virial +velocities $\vvir=113,\, 160\, {\rm and}\ 320\, {\rm km\,s^{-1}}$, +using the labeled initial gas fraction. The colored lines in each +panel show the predictions of combining the scalings expected for the +intrinsic luminosities (Equation~\ref{eqn:BL.predict}) and +attenuations as above, giving +\begin{equation} +\frac{L_{\rm B,\ obs}^{\rm qso}}{L_{\rm B,\ obs}^{\rm gal}}=7.9\,\frac{1}{\fgas}\, +{\Bigl(}\frac{M_{\rm BH}^{f}}{10^{8}\,M_{\sun}}{\Bigr)}^{0.2}\ \frac{L}{\Lp}, +\label{eqn:BL.scaling} +\end{equation} +where the colored lines each use the $M_{\rm BH}^{f}$ and $\fgas$ of +the simulation of the corresponding color and panel. This scaling +provides a good estimate of the observed optical quasar-to-galaxy +luminosity ratio, including the complicated effects of attenuation, +evolving mass-to-light ratios, metallicities, and host galaxy +properties, as a function of gas fraction, final black hole mass, and +the ratio of the current to peak quasar luminosity. Although, for +clarity, we have not shown a range of simulations varying other +parameters, we find that this scaling is robust to the large number of +quantities we have considered in our simulations -- there +are systematic offsets in e.g.\ $\Lp$ and $M_{\rm BH}^{f}$ with +changes such as e.g.\ different ISM equations of state, but the +scaling in terms of $\Lp$ and $M_{\rm BH}^{f}$ is unchanged. + +Because the ratio of observed quasar and host galaxy B-band +luminosities in our simulations obeys the scaling of +Equation~\ref{eqn:BL.scaling}, we can use it to predict the +properties of ``broad-line'' quasars, defined by $L_{\rm B,\ obs}^{\rm +qso}>f_{\rm BL} L_{\rm B,\ obs}^{\rm gal}$. To do so, +however, we must assume a typical host galaxy gas +fraction. Unfortunately, because our empirical modeling in terms of +the quasar lifetime as a function of $L$ and $\Lp$ does not have a +systematic dependence on host galaxy gas fraction (see +\S~\ref{sec:detailsCompare}), we have no constraint on this parameter. +It is, however, convenient for several reasons to consider +$\fgas=0.3$ as a typical value for bright quasars. + +First, such a gas +fraction is capable of yielding the brightest observed +quasars; second, scaling a Milky-Way like disk with the observed $z=0$ +gas fraction $\sim0.1$ to the redshifts of peak quasar activity gives +a similar gas fraction \citep[e.g.,][]{SDH05a}; third, gas fractions +$\gtrsim30\%$ in major mergers are needed to explain the observed +fundamental plane (Robertson et al.\ 2005c, in preparation), kinematic +properties (Cox et al.\ 2005c, in preparation), and central phase +space densities (Hernquist, Spergel \& Heyl 1993) of elliptical +galaxies; fourth, this choice implies that the brightest quasars with +$M_{\rm BH}^{f}\sim10^{10}\,M_{\sun}$ attain observed B-band +luminosities $\sim1000$ times that of their hosts at their peaks, as +is observed \citep[e.g.,][]{MD04}. Finally, and most important, the +assumed $\fgas$ and $f_{\rm BL}$ are degenerate in our predictions for +the broad-line population, as they both enter linearly in the ratio of +host galaxy to quasar B-band luminosity. Therefore, the range of +$f_{\rm BL}=0.3-3$ which we consider (for a fixed median $\fgas=0.3$) +can be equivalently considered, for a fixed median $f_{\rm BL}=1$, to +represent a theoretical uncertainty in the host galaxy gas fraction, +$\fgas=0.1-0.9$; i.e.\ spanning the range from present, relatively +gas-poor Milky-Way like disks to almost completely gaseous +disks. This, then, gives for our ``broad-line'' criterion, +\begin{equation} +\frac{L}{\Lp}\gtrsim 0.2\,{\Bigl(}\frac{f_{\rm BL}}{1.0}{\Bigr)}\, +{\Bigl(}\frac{\fgas}{0.3}{\Bigr)}\, +{\Bigl(}\frac{M_{\rm BH}^{f}}{10^{7}\,M_{\sun}}{\Bigr)}^{-0.2}. +\label{eqn:BL.min} +\end{equation} + +The ``broad-line'' phase is thus, as is clear from +Figure~\ref{fig:BL.in.sims} and implicit in our definition of the +broad-line phase, closely associated with the final ``blowout'' stages +of quasar evolution, when the mass of the quasar reaches that +corresponding to its location on the $M_{\rm BH}-\sigma$ relation and +gas is expelled from the central regions of the galaxy, shutting down +accretion \citep{DSH05}. We note that combining the equation above +with our fitted quasar lifetimes gives an integrated time when the +quasar would be observable as a broad line object of $t_{\rm +BL}\sim10-20$\,Myr, in good agreement with the optically observable +bright quasar lifetimes we calculate directly from our quasar light +curves, including the effects of attenuation, and with empirical +estimates of the quasar lifetime which are based directly on +optically-selected, broad-line quasar samples. + +The $({M_{\rm BH}^{f}}/{10^{7}\,M_{\sun}})^{0.2}$ term in the above +equation reflects the fact that, below a certain peak luminosity, +quasars are less likely to reach luminosities above that of the host +galaxy, as can be seen in the uppermost panels of +Figure~\ref{fig:BL.in.sims} for a final black hole mass of +$\mbhf=3\times10^{7}$ -- i.e.\ the smallest AGN are +proportionally less optically luminous than their hosts. This does +not imply that such systems are not inherently broad-line objects, but +only that the host galaxy light will increasingly dominate at lower +luminosities. We also caution against extrapolating this to large or +small $M_{\rm BH}^{f}$, as the attenuation becomes more difficult +to predict at these peak luminosities, and the linear formula above is +not always accurate (see Figure~\ref{fig:test.BL}). + +We can use this estimate of the broad-line phase and our model of the +quasar lifetime to calculate the total energy radiated in this bright, +optically observable stage following the calculation of +\S~\ref{sec:detailsCompare}, but with a minimum luminosity determined +by Equation~\ref{eqn:BL.min}. This gives an integrated fraction +$\sim0.3-0.4$ ($\sim\exp\{-0.2\,f_{\rm BL}\,(\fgas/0.3)/\alpha_{L}\}$) +of the total radiant energy emitted during the broad-line phase. Thus, +despite the short duration of this optical quasar stage, a large +fraction of the total radiated energy is emitted (as it represents the +final $e$-folding in the growth of the black hole) when most of the +final black hole mass (\S~\ref{sec:detailsCompare}) is accumulated. +Accounting for the luminosity dependence of our bolometric corrections +(with the optical fraction of the quasar energy increasing with +bolometric luminosity) as well as the small fraction of objects +observable at lower luminosities (with larger typical obscuring column +densities) increases this fraction to as much as $\sim0.6-0.7$ for +bright quasars. Therefore, despite the fact that the {\em duration} +of the optically observable broad-line quasar phase may be $\sim1/10$ +that of the obscured quasar growth phase, the changing quasar +luminosity over this period and non-trivial quasar lifetime as a +function of luminosity implies only small corrections to counting +arguments such as that of \citet{Soltan82}, which rely on the total +observed optical quasar flux density to estimate the relic +supermassive black hole density. + +\subsection{The Broad-Line Fraction as a Function of Luminosity} +\label{sec:BLfraction} + +By estimating the time that a quasar with some $\Lp$ will be +observable as a broad-line quasar at a given luminosity, we can then +calculate the broad-line quasar luminosity function in the same +fashion as the complete quasar luminosity function in +\S~\ref{sec:fullLF}. Instead of the full quasar lifetime $\dtdL$, we +consider only the time during which broad-lines would be observed +(i.e.\ that the quasar spectrum would be recognized as opposed to the +host galaxy spectrum), as identified in our simulations +(\S~\ref{sec:whenBL}). + +For a sample selected in hard X-rays (i.e.\ the selection function +only being relevant at column densities $\gtrsim10^{24}\ {\rm +cm^{-2}}$), we show the resulting ``broad-line'' luminosity function +in Figure~\ref{fig:LF.all} (cyan dot-dashed lines), and compare it to +the broad-line quasar luminosity function identified in the hard X-ray +luminosity function of \citet{Barger05}. The agreement is good at all +luminosities, and our model explains both the fact that broad-line +quasars dominate the luminosity function at luminosities well above +the ``break'' in the luminosity function, and the downturn in the +broad-line quasar population at luminosities below the +peak. Essentially, the broad-line quasar population more closely +traces the shape of the $\nLP$ distribution, giving rise to the +observed behavior as a dual consequence of luminosity-dependent quasar +lifetimes and the evolutionary nature of quasar obscuration in our +simulations. + +%\clearpage +\begin{figure*} + \centering + \plotone{f15.ps} + %\includegraphics[width=3.7in]{f14.ps} + \caption{Broad-line quasar luminosity function of + \citet{Richards05} from the 2dF-SDSS (2SLAQ) survey (black squares) and that + of \citet{Croom04} (green circles) from the 2dF survey, compared + to our predicted ``broad-line'' luminosity function from our + determination of the relative quasar and host galaxy luminosities in our simulations + (solid line), where we estimate that quasars are observable as ``broad-line'' objects + when their observed B-band luminosity is greater than a factor $f_{\rm BL}$ of that of the host galaxy, + Solid lines are + shown for the minimum and maximum observed redshift in each bin + (as labeled), assuming $f_{\rm BL}=1$. Dotted lines show the result for + $f_{\rm BL}=0.3$ and $f_{\rm BL}=3$, at the mean redshift + of the bin, i.e.\ corresponding to ``broad-line'' luminosity functions in surveys + which are complete to quasars with observed optical luminosity $\sim0.3$ + and $3$ times that of the host galaxy, respectively, or alternatively reflecting + nearly complete theoretical uncertainty regarding merging galaxy gas fractions ($\fgas=0.1-0.9$). + Open squares are observations with uncertain incompleteness corrections + in \citet{Richards05}. + \label{fig:LF.sdss}} +\end{figure*} +%\clearpage + +Figure~\ref{fig:LF.sdss} compares our theoretical predictions to the +2dF-SDSS (2SLAQ) g-band luminosity function of broad-line quasars from +\citet{Richards05} (black squares), as well as the B-band luminosity +function from \citet{Croom04} (green circles), at several redshifts +from $z\sim0.3-2$, over which range the surveys are expected to be +relatively complete (for broad-line quasars). The 2dF-SDSS result is +the most recent determination of the broad-line luminosity function, +but compares well with previous determinations by, e.g., +\citet{Boyle88}, \citet{KK88}, \citet{MZZ88}, \citet{Boyle90}, +\citet{BJS91}, \citet{Zitelli92}, \citet{Boyle00}, and +\citet{Croom04}. Open squares correspond to bins in luminosity which +have been corrected for incompleteness following +\citet{PageCarrera00}, but this correction is uncertain as the bins +are not uniformly sampled. We compare this at each redshift to the +prediction of our determination of the quasar ``broad-line'' phase, +where we estimate that the quasar is observable as a broad line object +when its observed B-band luminosity is greater than a factor $f_{\rm +BL}=1$ of that of the host galaxy. We calculate this for both the +minimum and maximum observed redshift of each bin to show the range +owing to evolution of the luminosity function over each interval in +redshift. The systematic uncertainty in our prediction can be +estimated from the dotted lines, which show the prediction (at the +mean redshift of the bin) if we instead require the observed quasar +B-band luminosity to be above a factor of 0.3 (upper lines) or 3 +(lower lines) of the observed host galaxy B-band luminosity, which as +discussed in \S~\ref{sec:whenBL} can alternatively be considered an +uncertainty in host galaxy gas fraction, with $\fgas=0.1$ and +$\fgas=0.9$, respectively. + +The agreement at all luminosities and redshifts shown is encouraging, +given the simplicity of our determination of the broad-line phase from +the simulations, but the systematic uncertainties are large, +emphasizing the importance of calculating detailed selection effects +in contrasting e.g.\ ``broad-line'' samples from optical and X-ray +surveys, as opposed to assuming a constant obscured fraction at a +given luminosity based on the ratio of luminosity functions as has +been adopted in previous phenomenological models. The difference +between different choices of $\fgas$ is suppressed at the high +luminosity (and correspondingly high redshift) end of the luminosity +function, because the quasar-to-galaxy B-band luminosity ratio scales +as $\propto (M_{\rm BH}^{f})^{0.2}$; i.e.\ regardless of the choice of +$f_{\rm BL}$, quasars increasingly overwhelm their host galaxy in +large systems near their peak luminosity. However, at low luminosity, +the predictions rapidly diverge, implying that a measurement of the +faint end of the broad-line quasar luminosity function, with a +reliable calibration of $f_{\rm BL}$, can constrain the typical gas +fractions of quasar host galaxies and the evolution of these gas +fractions with redshift. + +%\clearpage +\begin{figure} + \centering + \plotone{f16.ps} + %\includegraphics[width=3.7in]{f15.ps} + \caption{Predicted ``broad-line'' fraction of a complete X-ray + sample at low $z\lesssim0.3$ redshift, from our simulations (where + the object is observable as a broad-line quasar when it has an observed B-band + luminosity greater than a factor $f_{\rm BL}=1.0$ of that of its host galaxy), is shown (thick black + line). The results, changing our $f_{\rm BL}$ to 0.3 and + 3.0 are shown, or equivalently of assuming a host galaxy gas fraction $\fgas=0.1$ + or 0.9 instead of $\sim0.3$ (dashed), as are the results assuming a + ``light bulb'' model where quasars spend a fixed time + $t_{Q}=20$\,Myr as broad line objects with a luminosity of $\Lp$ + (dotted). For comparison, the (scaled to 2-10 keV luminosity) + observations of \citet{Ueda03} (squares), \citet{Hasinger04} + (circles), \citet{GRW04} (triangles), and \citet{Simpson05} + (diamonds) are shown. The predicted result at higher redshift + ($z\gtrsim1$) is shown (red dot-dashed line), offset owing to the + shift in break luminosity of the luminosity function with + redshift. The best-fit luminosity-dependent torus model, {\em + fitted} to the data, is shown as the solid cyan line. The best-fit + static torus model is a constant broad-line fraction $\sim0.3$ (not shown for clarity). + \label{fig:BL.fraction}} +\end{figure} +%\clearpage + +By dividing out the predicted luminosity function $\phi_{HX}$, we +can estimate the fraction of ``broad line'' objects observed in reasonably +complete X-ray samples as a function of luminosity. This is shown in +Figure~\ref{fig:BL.fraction}, where for ease of comparison we have +shown the broad-line fraction as a function of hard X-ray (2-10 keV) +luminosity. Our prediction, based on determining the time +a quasar with a given luminosity $L$ and peak luminosity $\Lp$ +in our simulations will be observable with a B-band luminosity greater +than a fraction $f_{\rm BL}=1.0$ of the host galaxy observed B-band +luminosity, is shown as the thick black line. This is compared to +the observations of \citet{Ueda03} (squares), \citet{Hasinger04} +(circles), \citet{GRW04} (triangles), and \citet{Simpson05} +(diamonds). The data from \citet{Hasinger04} has been scaled from +soft X-ray (0.5-2 keV) using our bolometric corrections, and the data +from \citet{GRW04} and \citet{Simpson05} have been converted from +[O{\sc~iii}] luminosity as in \citet{Simpson05} using the mean +correction for Seyfert galaxies \citep{Mulchaey94}, $L_{\rm +[O\,III]}=0.015\times L_{\rm 2-10\,keV}$. + +We also plot as upper and lower dashed lines the results of changing +$f_{\rm BL}$, the fraction of the host galaxy B-band luminosity above +which the quasar B-band luminosity must be observed for identification +as a ``broad-line'' object, considering $f_{\rm BL}=0.3,\ {\rm and}\ +3$, respectively. We determine this for the low-redshift +$z\lesssim0.3$ quasar distribution, from which most of the data are +drawn. The red dot-dashed line shows the difference at high redshift, +if just $z\gtrsim1$ quasars are considered (for $f_{\rm BL}=1$). The +broad-line fraction is systematically lower, primarily because the +break luminosity in the luminosity function moves to higher luminosity +with redshift, meaning that at a fixed luminosity below the break, a +smaller fraction of observed objects are at $L\sim\Lp$ in the +``blowout'' phase of peak optical quasar luminosity. Finally, the +dotted line shows the results assuming a ``light bulb'' model for the +broad-line phase (but still using our $\nLp$ distribution, otherwise +this translates to a constant obscured fraction with luminosity) +lifetimes, with a fixed broad-line lifetime of $t_{Q}=20\,$Myr. + +The prediction of the most basic torus model, with constant broad-line +fraction $\sim0.36$, is ruled out to high significance +($\reducechi=18.5,\ 17.2$ if we consider all data points, or if we +consider only the most well-constrained data, from Simpson [2005], +respectively). Furthermore, the solid cyan line shows the best-fit +luminosity-dependent torus model, in which the broad line fraction is +given by \citep[e.g.,][]{Simpson98,GRW04} +\begin{equation} +f = 1 - 1/\sqrt{1 + 3L/L_{0}}, +\end{equation} +where $L_{0}$ is the luminosity where the number of broad line objects +is equal to the number of non-broad line objects. This fit is at best +marginally acceptable over a narrow range in luminosities +($\reducechi=14.0,\ 7.3$). Modified luminosity-dependent, receding +torus models have been proposed which give a better fit to the data +by, for example, allowing the torus height to vary with luminosity +\citep[e.g.,][]{Simpson05}, but there is no physical +motivation for these changes, and they introduce such variation +through additional free parameters that allow a curve of +essentially arbitrary slope to be fitted to the data. + +However, the prediction of our model agrees reasonably well +($\reducechi=4.0,\ 1.2$) with the observations over the entire range +covered, a span of six orders of magnitude in luminosity. We emphasize +that our prediction, which matches the data better than standard torus +models that are actually {\em fitted} to the data, is not a fit to the +observations. Instead, it is derived from the physics of our +simulations, including black hole accretion and feedback which are +critical in driving the ``blowout'' phase which constitutes most of +the time a quasar is visible as a ``broad-line'' object by our +estimation, and from the $\dot n(L_{\rm peak})$ distribution implied +by our model of quasar lifetimes and the {\em bolometric} quasar +luminosity function. The agreement suggests that our choice of the +parameter combination $f_{\rm BL}\fgas=0.3$ is a good approximation. +As noted above, this implies that calibrating $f_{\rm BL}$ for an +observed sample, combined with the mean broad-line fraction and our +modeling, can provide a constraint (albeit model-dependent) on the +host galaxy gas fraction of quasars at a given redshift, which cannot +necessarily be directly measured even with difficult, detailed host +galaxy probes, as gas is rapidly converted into stars throughout the +merger. The uncertainty plotted, while large, actually represents a +larger theoretical uncertainty -- as discussed above, if an +observational sample were well-defined such that it were complete to +broad-line objects with observed optical luminosity above a +fraction $f_{\rm BL}$ of the host galaxy luminosity, the +range we consider would correspond to a range $\fgas=0.1-0.9$ in the +quasar host galaxy gas fraction, which the observations could then +constrain. + +In our modeling, the broad line fraction as a function of luminosity +does not depend sensitively on the observed luminosity function, as +evidenced by the relatively similar prediction at high redshift. The +evolution we do predict with redshift, in fact, agrees well with that +found by \citet{Barger05} over the redshift range $z=0.1-1.2$ (see +also La Franca et al.\ 2005), an aspect of the observations which is +not reproduced in any static or luminosity-dependent torus model but +follows from the evolution of the quasar luminosity function in our +picture for quasar growth. However, we do caution that gas fractions +may systematically evolve with redshift, and as discussed above, a +higher gas fraction will give generally shorter ``broad-line'' +lifetimes using our criteria of quasar optical luminosity being higher +than some fraction of the host galaxy luminosity, which will also +contribute to the evolution in the mean ``broad-line'' fraction with +redshift. Finally, neglecting the role of luminosity-dependent quasar +lifetimes gives unacceptable fits to the data ($\reducechi=66.0,\ +77.5$), as the broad-line fraction as a function of luminosity is a +consequence of both the evolution of obscuration and the dependence of +lifetime on luminosity. + +Our model for quasar evolution provides a direct physical motivation +for the change in broad line fraction with luminosity and suggests +that it is not a complicated selection effect. As an observational +sample considers higher luminosities (i.e.\ approaches and passes the +``break'' in the observed luminosity function), a comparison of the +luminosity function and the underlying $\nLp$ shows that it is +increasingly dominated by sources near their peak luminosity in the +final stages of Eddington limited growth. The final stages of this +growth expel the large gas densities obscuring the quasar, rendering +it a bright, optically observable broad-line object for a short +time. Therefore, we expect that the fraction of broad-line objects +should increase with luminosity in quasar samples, as +indicated by the observations. + +%\clearpage +\begin{figure} + \centering + \plotone{f17.ps} + %\includegraphics[width=3.7in]{f15b.ps} + \caption{Predicted ``obscured'' fraction (solid line) in an X-ray sample with identical + redshift and luminosity range to that of \citet{Ueda03}, as a function of hard X-ray + (2-10 keV) luminosity. Vertical error bars show + Poisson errors estimated from the total time at a given luminosity across all our simulations + (absolute values of the error bars should not be taken literally). The ``obscured'' fraction is defined + as the fraction of quasars with X-ray column densities $\nh>10^{22}\,{\rm cm^{-2}}$ in + bins of $\Delta\log{L_{2-10\,{\rm keV}}}$. The observations from \citet{Ueda03} are shown + as black squares. + \label{fig:Ueda.BL}} +\end{figure} +%\clearpage + +Many observational measures do not consider a direct optical analysis +of the quasar spectrum in estimating the fraction of broad-line +objects as a function of luminosity. For example, \citet{Ueda03} adopt +a proxy, classifying as ``obscured'' any quasars with an X-ray +identified column density $\nh>10^{22}\,{\rm cm^{-2}}$, and as +``unobscured'' quasars below this column density. We can compare to +their observations, using the column density distributions as a +function of luminosity from our simulations, which cover the entire +range in luminosity of the observed sample. Specifically, we use a +Monte Carlo realization of these distributions, employing our fitted +$\nLp$ distribution at each redshift to produce a list of quasar peak +luminosities and then generating all other properties based on the +probability distribution of a given property in simulations with a +similar peak luminosity. We describe this methodology in detail in +\S~\ref{sec:discussion}, and provide several such mock quasar +distributions at different redshifts. + +In Figure~\ref{fig:Ueda.BL}, we compare our estimated ``obscured'' and +``unobscured'' fractions as a function of hard X-ray luminosity, using +the same definitions as well as redshift and luminosity limits as the +observed sample. The solid line shows our prediction, with vertical +error bars representing Poisson errors, where the number of ``counts'' +is proportional to the total time spent by simulations at the plotted +luminosity (the absolute value of these errors should not be taken +seriously). The ``obscured'' fraction is determined in bins of +luminosity $\Delta\log L_{2-10\ {\rm keV}}=0.5$. Despite our large +number of simulations, there is still some artificial ``noise'' owing +to incomplete coverage of the merger parameter space, namely the +apparent oscillations in the obscured fraction. However, the mean +trend agrees well with that observed (black squares), suggesting that +the success of our modeling in reproducing the fraction of ``broad +line'' objects as a function of luminosity is not a consequence of the +definitions chosen above. We do not show the predictions of the +standard and luminosity-dependent torus models, as (because +essentially any line of sight through the torus encounters a column +density $\nh>10^{22}\,{\rm cm^{-2}}$) the predictions of these models +are identical to those shown and compared to the same observations in +Figure~\ref{fig:BL.fraction}. + +Our prediction that the fraction of broad-line objects should rise +with increasing luminosity is counterintuitive, given our fitted +column density distributions in which typical (median) column +densities increase with increasing luminosity. This primarily owes to +the simplicity of our \NH\ fits; we assume the distribution is +lognormal at all times, but a detailed inspection of the cumulative +(time-integrated) column density distribution shows that at bright +(near-peak) luminosities, the distribution is in fact bimodal (see +e.g.\ Figure 3 of Hopkins et al.\ 2005b and Figure 2 of Hopkins et +al.\ 2005d), representing both the heavily obscured growth phase and +the ``blowout'' phase we have identified here as the ``broad line'' +phase. Over most of a simulation, we find the general trend shown in +Figure~\ref{fig:NH.systematics} and discussed above, namely that +typical column densities increase with intrinsic (unobscured) +luminosity. This is because the total time at moderate to large +luminosities is dominated by black holes growing in the +obscured/starburst stages; here, the same gas inflows fueling black +hole growth also give rise to large column densities and starbursts +which obscure the black hole activity. However, when the quasar nears +its final, peak luminosity, there is a rapid ``blowout'' phase as +feedback from the growing accretion heats the surrounding gas, driving +a strong wind and eventually terminating rapid accretion, leaving a +remnant with a black hole satisfying the $M_{\rm BH}-\sigma$ +relation. This can be identified with the traditional bright optical +quasar phase, as the final stage of black hole growth with a rapidly +declining density (allowing the quasar to be observed in optical +samples), giving typical luminosities, column densities, and lifetimes +of optical quasars. In these stages, larger luminosities imply more +violent ``blowout'' events, i.e.\ a brighter peak luminosity quasar +more effectively expels the nearby gas and dust, rendering a dramatic +decrease in column density at these bright stages (see Hopkins et al. +2005f). + +We are essentially modeling this bimodality in more detail by directly +determining the ``broad-line'' phase from our simulations. However, +the broad line fraction-luminosity relation we predict is also a +consequence of the more complicated relationship between column +density, peak luminosity, and bolometric and observed luminosity, as +opposed to the predictions from a model with correlation between $\nh$ +and only observed luminosity. The key point is that we find, near the +{\em peak} luminosity of the quasar, as feedback drives away gas and +slows down accretion, the typical column densities fall rapidly with +luminosity in a manner similar to that observed. In our model for the +luminosity function, quasars below the observed ``break'' are either +accreting efficiently in early stages of growth or are in +sub-Eddington phases coming into or out of their peak quasar +activity. Around and above the break, the luminosity function becomes +dominated by sources at high Eddington ratio at or near their peak +luminosities. Based on the above calculation, we then {\em expect} +what is observed, that in this range of luminosities, the fraction of +objects observed with large column densities will rapidly decrease +with luminosity as the observed sample is increasingly dominated by +sources at their peak luminosities in this blowout phase. This also +further emphasizes that the evolution of quasars dominates over static +geometrical effects in determining the observed column density +distribution at any given luminosity. + +Finally, if host galaxy contamination were not a factor, we would +expect from our column density model that, at low luminosities +($L\lesssim\Lcut{10}$, well below the range of most observations +shown), the broad-line fraction would again increase (i.e.\ the +obscured fraction would decrease), as the lack of gas to power +significant accretion would also imply a lack of gas to produce +obscuring columns. However, at these luminosities, typical of faint +Seyfert galaxies or LINERs, our modeling becomes uncertain; it is +quite possible, as discussed previously, that cold gas remaining in +relaxed systems could collapse to form a traditional dense molecular +torus on scales $\sim\,$pc, well below our resolution +limits. Furthermore, host galaxy light is likely to overwhelm any AGN +broad-line contribution, and selection effects will also become +significant at these luminosities. + + +\subsection{The Distribution of Active Broad-Line Quasar Masses} +\label{sec:BLmasses} + +Our determination of the ``broad-line'' or optical phase in quasar +evolution allows us to make a further prediction, namely the mass +distribution of currently active broad-line quasars. At some +redshift, the total number density of observed, currently active +broad-line quasars with a given $\Lp$ will be (in the absence of +selection effects) +\begin{equation} +n_{\rm BL}(\Lp)\approx\nLP\, t_{\rm BL}(\Lp), +\end{equation} +where $t_{\rm BL}(\Lp)$ is the total integrated time that a quasar +with peak luminosity $\Lp$ spends as a ``broad-line'' object (using +our criterion for the ratio of the observed quasar B-band luminosity to +that of the host galaxy), given by integrating our formulae in +\S~\ref{sec:whenBL} or directly calculated from the simulations. +Since we have determined roughly that a quasar should be observable as +a ``broad-line'' object at times with $L\gtrsim 0.2\,\Lp$ primarily +just after it reaches its peak luminosity, in the ``blowout'' phase of +its evolution, we expect the instantaneous black hole mass at the time +of observation as a broad-line quasar to be, on average, $M^{\rm +BL}_{\rm BH}\approx\mbhf(\Lp)$, where $\mbhf\sim M_{\rm Edd}(\Lp)$ +modulo the order unity corrections described in +\S~\ref{sec:detailsCompare}. Using our fitted $\nLP$ distribution from +the luminosity function, extrapolated to low redshift ($z\sim0$), and +combining it with the integrated ``broad-line'' lifetimes from our +simulations as above, we obtain the differential number density of +sources in a logarithmic interval in $\Lp$. Finally, we use our +Equation~\ref{eq:Mbhf} for $\mbhf(\Lp)$ determined from our fitted +quasar lifetimes (demanding that $E_{\rm rad}=\epsilon_{r}M_{\rm +BH}^{f}c^{2}$) to convert this to a distribution in black hole mass. + +%\clearpage +\begin{figure*} + \centering + \plotone{f18.ps} + %\includegraphics[width=3.7in]{f16.ps} + \caption{Predicted distribution of currently active black hole masses, + both considering all types (Type I \&\ II; left) and only those visible as broad-line quasars (Type I; right), + at low $z\lesssim0.3$ redshift, from our $\nLP$ distribution and the estimation of the ``broad-line'' + phase directly from the simulations. + In the left panel (all quasar types), we consider the result with + arbitrarily faint luminosity limits (dashed line), + and with the luminosity completeness limit (dotted) and both luminosity limit and velocity dispersion limit (dash-dot) + of the SDSS sample of \citet{Heckman04}. We then consider the mass distribution with these limits, + weighted by OIII luminosity, for direct comparison to the mass function of \citet{Heckman04}, shown as + red circles (vertical errors represent the range in different parameterizations of the luminosity-weighted mass function + from \citet{Heckman04}, their Fig.~1, horizontal errors a $\sim0.2$\,dex uncertainty in the black hole mass). + Black lines show this for our full model, red lines show the full distribution (dashed) and + distribution with the same weighting and selection effects as \citet{Heckman04} (solid) for a + light-bulb or exponential light curve model of quasar evolution. + At right, the distribution of active ``broad-line'' quasar masses (solid, where + an object is a ``broad-line'' quasar if the observed quasar B-band luminosity is above + a factor $f_{\rm BL}=1$ of that of the host galaxy -- dotted and dashed lines + show the result if $f_{\rm BL}=0.3$ or 3, respectively). Black lines show the prediction of the full + model, red and blue lines the predictions of a light-bulb/exponential light curve model with + a standard torus model (red) and receding torus model (blue) used to determine the broad-line fraction. + %agrees well with the active broad-line + %mass function from the SDSS, with some expected incompleteness in the SDSS sample at low $M_{\rm BH}$ + %(Greene et al., in preparation). + \label{fig:BL.massfunct}} +\end{figure*} +%\clearpage + +Our predicted $n(M_{\rm BH})$, i.e.\ the number of observed {\em +active} quasars at low redshift in a logarithmic interval of black +hole mass, is shown in Figure~\ref{fig:BL.massfunct}. We consider the +complete distribution of active quasar masses, for both broad-line and +non broad-line objects, in the left panel of the figure, and the +distribution of broad-line objects only, $n(M^{\rm BL}_{\rm BH})$, in +the right panel. On the left, we show the complete distribution which +would be observed without any observational limits (dashed line). We +calculate this from the distributions of Eddington ratios in our +simulations, as a function of current and peak luminosity, and our fit +to $\nLp$ (as, e.g.\ for our Monte Carlo realizations). We also +consider the observed distribution if we apply the luminosity limit +for completeness from the SDSS sample of \citet{Heckman04} (dotted), +$L_{\rm [O\,III]}>\Lcut{6}$, which using their bolometric corrections +yields $L>3.5\times\Lcut{9}$, and then additionally applying their +minimum velocity dispersion $\sigma>70\,{\rm km\,s^{-1}}$ +(dot-dashed). Finally, we can weight this distribution by luminosity +(solid line) to compare directly to that determined in their +Fig.~1. The red points are taken from the luminosity-weighted black +hole mass function of \citet{Heckman04}, which serves as a rough +estimate of the {\em active} black hole mass distribution given their +selection effects. Vertical error bars represent the range in +parameterizations of the mass function from \citet{Heckman04}, +including whether or not star formation is corrected for and limiting +the sample to luminosities $L\gtrsim\Lcut{10}$ or Eddington ratios +$>0.01$. Horizontal errors represent an uncertainty of $0.2\,$dex in the +black hole mass estimation (representative of uncertainties in the +$M_{\rm BH}-\sigma$ relation used). The agreement is good, especially +given the significant effects of the selection criteria and +luminosity-weighting. + +We also consider the predictions of a ``light-bulb'' or ``exponential +/ fixed Eddington ratio'' model of the quasar lifetime for the active +black hole mass distribution (red lines). For purposes of the active +black hole mass function, the two predictions are identical and +independent of the assumed quasar lifetime (modulo the arbitrary +normalization), as both assume that all observed quasars are accreting +at a fixed Eddington ratio, giving the distribution of active black hole +masses. The dashed line shows the prediction for the complete active +black hole mass function, which rises sharply to lower luminosities, +as it must given a luminosity function which increases monotonically +to lower luminosities. The solid line shows the prediction of such a +model with the complete set of selection effects from +\citet{Heckman04} described above applied, as with the solid black +line showing the prediction of our modeling. Here, we chose the +characteristic Eddington ratio $\approx1.0$ by fitting the predicted +curve to the \citet{Heckman04} observations. Note that both the +characteristic Eddington ratio and lifetime (normalization) of the +curve are fitted, so the relative normalization of this curve and our +full model prediction are not the same; for example, the predicted +total absolute number of active $M_{\rm BH}>10^{9}$ quasars is higher +in the full model than in the light-bulb or exponential models. Still, +it is clear that these models produce too broad a distribution of +active black hole masses, in disagreement with the observations. We +could, of course, obtain an arbitrarily close agreement with the +observations if we fit to the {\em distribution} of accretion rates, +but such a model would recover a quasar lifetime and accretion rate +distribution quite similar to ours, as is evident from the agreement +between the predictions of our simulations and the observations. A +purely empirical model of this type is considered by e.g.\ +\citet{Merloni04}, who finds that similar qualitative evolution in the +quasar lifetime and anti-hierarchical black hole assembly to that +predicted by our modeling is implied by the combination of quasar +luminosity functions and the black hole mass function. + +On the right of the figure, we show our predicted mass distribution +for low-redshift, active ``broad-line'' quasars (solid black lines), +where we estimate that an object is a ``broad-line'' quasar if the +observed quasar B-band luminosity is above a factor $f_{\rm BL}=1$ of +that of the host galaxy -- dotted and dashed lines show the result if +$f_{\rm BL}=0.3$ or 3, respectively, parameterizing the range of +different observed samples. As discussed above, the range of $f_{\rm +BL}$ shown can be, alternatively, thought of as a parameterization of +uncertainty in the host galaxy gas fraction, if (in an observed +sample), the sensitivity to seeing quasar broad lines against host +galaxy contamination is known. Therefore, the location of the peak in +the active broad-line black hole mass function can be used, just as +the mean broad line fraction vs.\ luminosity, as a test of the typical +gas fractions of bright quasar host galaxies, and can constrain +potential evolution in these gas fractions with redshift. + +The prediction shown is testable, but appears to be in good +agreement with preliminary results for the distribution of active +broad-line black hole masses from the SDSS \citep[e.g.,][]{MD04}. The +observations may show fewer low-mass black holes than we predict, but +this is expected, as observed samples are likely incomplete at the low +luminosities of these objects (even at the Eddington limit, a +$10^{5}\,M_{\sun}$ black hole has magnitude $M_{g}\sim-16$). If, in +our model, we were to consider instead a standard torus scenario for +the definition of the broad-line phase, we would predict the same +curve as that shown in the left half of the figure (black dashed; our +prediction for the cumulative active black hole mass function). This +is because the standard torus model predicts that a constant fraction of +objects are broad-line quasars, regardless of mass or luminosity, thus +giving identical distributions of Type I and Type II quasar masses. If +we consider a luminosity-dependent or receding torus model, the +prediction is nearly identical to the black line shown. This is +because, as shown in Figure~\ref{fig:BL.fraction}, our prediction for +the broad line fraction as a function of luminosity is similar to that +of the receding torus model. The differences in the model predictions +for the broad-line fraction as a function of luminosity do manifest in +the prediction for the active broad-line black hole mass function, but +the difference in these models is smaller than the $\sim1\sigma$ range +from different values of $f_{\rm BL}$ shown. However, if we consider +different models for the quasar light curve or lifetime, the predicted +active broad-line mass function is quite different (as is the +cumulative active black hole mass function). + +We show the predictions of a light-bulb or exponential light curve +model for quasar evolution in the figure, adopting either a standard +torus model (red) or receding torus model (blue) to determine the +broad-line fraction as a function of luminosity. For the standard +torus model, this predicts that the broad line mass function should +trace the observed luminosity function, rising monotonically to lower +black hole masses in power-law fashion (just as seen in the red dashed +line in the left half of the figure for the cumulative black hole mass +function). For the receding torus model, the active black hole mass +function shows a peak (because, at lower luminosities, there are more +observed quasars, but a larger fraction of them are +obscured). However, the location of this peak is at roughly an order +of magnitude smaller black hole mass than for our prediction. This +assumes a typical Eddington ratio $\sim1$, which we have fitted to the +cumulative black hole mass function -- the peak in the broad-line +active black hole mass function in these models could be shifted to +larger black hole masses by assuming a smaller typical Eddington +ratio, but this would only worsen the agreement with the cumulative +black hole mass function of \citet{Heckman04}. Furthermore, a robust +difference between the models is that the light bulb or +Eddington-limited/exponential models predict, for the standard torus +case, no turnover in the active broad-line black hole mass function, +and for the receding torus case, a broader distribution in active +broad-line quasar black hole masses than is predicted in our +modeling. Roughly, the lognormal width of this distribution in our +model is $\sim0.6$\,dex, whereas the light-bulb or exponential light +curve models have a distribution with width $\sim1.0$\,dex. As noted +above, we obtain a similar prediction if we adopt our full obscuration +model instead of the receding torus model here. A determination of +the range of active, broad-line quasar masses can, therefore, +constrain quasar lifetimes and light curves. + +Our model makes an accurate prediction for the distribution of {\em +active} black hole masses, even at $z\sim0$ where our extrapolation of +the luminosity function is uncertain. It is important to distinguish +this from the predicted relic black hole mass distribution, derived in +\S~\ref{sec:smbh}, which must account for all quasars, i.e.\ $\nLP$ +integrated over redshift. We additionally find for broad-line +quasars, as we expect from our prediction of the broad-line phase, +that these objects are primarily radiating at large Eddington ratios, +$l\sim0.2-1$, but we address this in more detail in +\S~\ref{sec:eddington}. The success of this prediction serves not only +to support our model, but also implies that we can extrapolate to +fairly low luminosities, even bright Seyfert systems at $z\sim0$. +This suggests that many of these systems, at least at the bright end, +may be related to our assumed quasar evolution model, +fueled by similar mechanisms and either exhibiting weak interactions +among galaxies or relaxing from an earlier, brighter stage in their +evolution. As we speculate in \S~\ref{sec:discussion}, our +description of self-regulated black hole growth may also be +relevant to fainter Seyferts, even those that reside in +apparently undisturbed galaxies. + +\section{The Distribution of Eddington Ratios} +\label{sec:eddington} + +In traditional models of quasar lifetimes and light curves, the +Eddington ratio, $l\equiv L/L_{\rm Edd}$ is generally assumed to be +constant. Even complex models of the quasar population which allow +for a wide range of Eddington ratios according to some probability +distribution $P(l)$ implicitly associate a fixed Eddington ratio with +each individual quasar, and do not allow for $P(l)$ to depend on +instantaneous luminosity or host system properties. However, this is a +misleading assumption in the context of our model, as the Eddington +ratio varies in a complicated manner over most of the quasar light +curve. Furthermore, the integrated time at a given Eddington ratio is +different in different systems, with more massive, higher peak +luminosity systems spending more time at large ($l \sim1$) Eddington +ratios. + +The probability of being at a given Eddington ratio should properly be +thought of as a conditional joint distribution $P(l\,|\,L,\,\Lp)$ in +both instantaneous and peak luminosity, just as the quasar +``lifetime'' is more properly a conditional distribution +$t_{Q}(L\,|\,\Lp)$. Rather than adopting a uniform Eddington ratio or +Eddington ratio distribution, empirical estimates must consider more +detailed formulations such as the framework presented in \citet{SW03}, +which allows for a conditional bivariate Eddington ratio distribution +and can therefore incorporate these physically motivated dependencies +and complications in de-convolving observations of the quasar +luminosity function to determine e.g.\ Eddington ratio distributions, +active black hole mass functions, and other physical quantities. + +%\clearpage +\begin{figure} + \centering + \plotone{f19.ps} + %\includegraphics[width=3.7in]{f17.ps} + \caption{Distribution of Eddington ratios (left panels) and + instantaneous black hole mass (right panels) as a function of quasar + bolometric luminosity for our fiducial Milky Way-like A3 simulation, + with $\vvir=160\,{\rm km\,s^{-1}}$ and + $\Lp\sim5\times\Lcut{13}$. The trend of an increasingly narrow + Eddington ratio and mass distribution (concentrated at higher values) + with increasing luminosity is clear. The result of applying an + ADAF-type radiative efficiency correction at low accretion rates is + shown (dashed) as well as the result of considering only times after + the final merger, with $M_{\rm BH}\sim\mbhf$ (dotted). + \label{fig:Pofl.A3}} +\end{figure} +%\clearpage + +Figure~\ref{fig:Pofl.A3} shows the distribution of Eddington ratios as +a function of luminosity for the fiducial, Milky Way-like A3 +simulation ($\vvir=160\,{\rm km\,s^{-1}}$). Over the course of the +simulation, the system spends a roughly comparable amount of time at a +wide range of Eddington ratios from $l\sim0.001-1$. At high +luminosities, $L>\Lcut{12}$ for a system with $\Lp\approx\Lcut{13}$, +the range of Eddington ratios, is concentrated at high values +$l\sim0.5-1$ with some time spent at ratios as low as +$l\sim0.1$. Note, however, that the y-axis of the plot is scaled +logarithmically, so the time spent at $l\sim0.1$ in this luminosity +interval is a factor $\sim5$ smaller than the time spent at +$l\gtrsim0.5$. Considering lower luminosities $\Lcut{11} 0.01 \\ + 100\,\eEdd & \mathrm{ if\ } \eEdd \leq 0.01. +\end{array} + \right. +\end{equation} +This choice for the efficiency factor follows from ADAF models +\citep{NY95} and ensures that the radiative efficiency is continuous +at the critical Eddington ratio $\eEdd_{\rm crit}=0.01$. Applying this +correction and then examining the distribution of Eddington ratios as +a function of luminosity (dashed histograms in +Figure~\ref{fig:Pofl.A3}), we see that the distribution of Eddington +ratios is essentially identical, with only a slightly higher +probability of observing extremely low Eddington ratios +$l\lesssim0.001$. Of course, our modeling of accretion processes does +not allow us to accurately describe ADAF-like accretion at these low +Eddington ratios, but such low values are not relevant for the +observed luminosity functions and quantities with which we make our +comparisons. This implies that such a transition in the radiative +efficiency with accretion rate should not alter our conclusions +regarding the luminosity function and the $\nLp$ distribution +(essentially, the corrections are important only at luminosities well +below those relevant in constructing the observed luminosity +functions; see also Hopkins et al.\ 2005c for a calculation +of the effects of such a correction on the fitted quasar lifetime and +$\nLp$ distributions, which leads to the same conclusion). + +Despite the broad range of Eddington ratios in the simulations, this +entire distribution is unlikely to be observable in many samples. The +effect of this can be predicted based on the behavior seen in +Figure~\ref{fig:Pofl.A3}. For example, we consider the distribution +of Eddington ratios that would be observed if the B-band luminosity +$\LBo\geq\Lcut{11}$, comparable to the selection limits at high +redshift of many optical quasar samples. As expected from the change +in $l$ with luminosity, this restricts the observed range of Eddington +ratios to large values $l\sim0.1-1$, in good agreement with the range +of Eddington ratios actually observed in such samples. Essentially, it +has reduced the observed range to a bolometric luminosity +$L\gtrsim\Lcut{12}$ in the case shown, giving a similar distribution +to that seen in the lower panel of the figure. + +%\clearpage +\begin{figure} + \centering + \plotone{f20.ps} + %\includegraphics[width=3.7in]{f18.ps} + \caption{Predicted distribution of Eddington ratios based on + the luminosity function and the quasar evolution in our + simulations, in two redshift intervals $z<0.5$ (upper left) and + $1.5\Lcut{11}$). + \label{fig:Pofl.all}} +\end{figure} +%\clearpage + +We compare our predicted distribution of Eddington ratios to +observations in Figure~\ref{fig:Pofl.all}. Using the distribution of +peak luminosities $\nLp$ determined from the luminosity function, we +can integrate over all luminosities to infer the observed Eddington +ratio distribution, +%\begin{equation} +% \begin{split} +% P(l)\propto & \int{{\rm d}\log L}\int{{\rm d}\log\Lp} \\ +% & \times P(l | L, \Lp)\,\frac{{\rm d}t(L,\Lp)}{{\rm d}\log L} \nLP . +% \end{split} +%\end{equation} + \begin{eqnarray} + P(l)&\propto& \int{{\rm d}\log L}\int{{\rm d}\log\Lp} \nonumber\\ + && \times P(l | L, \Lp)\,\frac{{\rm d}t(L,\Lp)}{{\rm d}\log L} \nLP . + \end{eqnarray} +As our estimate of $P(l | L, \Lp)$ above is rough, we do this by +binning in $\Lp$ and averaging the binned $P(l | L, \Lp)\,\dtdL$ for +each simulation in the range of $\Lp$, then weighting by $\nLp$ and +integrating. We consider both the entire distribution that would be +observed in the absence of selection effects (red histograms), and +the distribution observed demanding a B-band luminosity above some +reference value, $\LBo>L_{\rm min}$ (black histograms). The results are shown +for redshifts $z<0.5$ and $z=1.5 - 3.5$, along with the observed +distribution from \citet{Vestergaard04}, with assumed Poisson +errors. The observations should be compared to the black histograms, +which have luminosity thresholds $L_{\rm}=\Lcut{10}\ {\rm and}\ +\Lcut{11}$ for $z<0.5$ and $z=1.5 - 3.5$, respectively, corresponding +approximately to the minimum observable luminosities in the observed +samples in each redshift interval. + +The agreement is good, given the observational uncertainties, and it +suggests that the observed Eddington ratio distribution can be related +to the non-trivial nature of quasar lifetimes and light curves we +model, rather than some arbitrary distribution of fixed $l$ across +sources. However, the selection effects in the observed samples are +quite significant -- the complete distribution of Eddington ratios is +similar in both samples, implying that the difference in the observed +Eddington ratio distribution is primarily a consequence of the higher +luminosity limit in the observed samples -- and a more detailed test +of this prediction requires fainter samples. + +Still, there is a systematic offset in the observed samples at $z<0.5$ +and $z=1.5-3.5$ which does not owe to selection effects. At +progressively lower redshifts, more quasars with luminosities further +below the ``break'' in the luminosity function are observed, and +therefore the observed Eddington ratio is broadened to lower Eddington +ratios $l\sim0.1$, whereas at high redshift the distribution is more +peaked at slightly higher Eddington ratios. This difference, although +not dramatic, is a prediction of our model not captured in ``light +bulb'' or ``fixed Eddington ratio'' models, even when allowing for a +distribution of Eddington ratios, if such a distribution is static. We +demonstrate this by fitting the low-redshift Eddington ratio +distribution to a Gaussian (blue dashed lines in upper left), and then +assuming that this distribution of accretion rates is unchanged with +redshift, giving (after applying the same selection effects which +yield the black histograms plotted) the blue dashed line in the upper +right panel. Although the agreement may appear reasonable, the +difference is significant -- such a fit overpredicts the fraction of +high redshift objects at Eddington ratios $\lessim0.1$ and +underpredicts the fraction at $\sim0.3$, giving a somewhat poor fit +overall ($\reducechi=2.7$, but with typical $\gtrsim3\sigma$ +overpredictions for Eddington ratios $\lesssim0.1$). + +Furthermore, without being modified to allow for a distribution of +Eddington ratios, such models are clearly inconsistent with the +observations, as they would predict a single, constant Eddington +ratio. However, models which fit the observed evolution in the quasar +luminosity function with a non-static distribution of accretion rates +do recover the broadening of the Eddington ratio distribution at low +redshift, so long as strong evolution in the distribution of accretion +rates for systems of a given black hole mass is not allowed +\citep{SW03}, giving a qualitatively similar picture of the evolution +we model. Regardless of the evolution in accretion rates, an +advantage of our modeling is that it provides a physically motivated +predicted distribution of accretion rates, as opposed to being forced +to adopt the distribution of accretion rates from observational input +(which can be, as demonstrated in the figure, significantly biased by +observational selection effects). The dotted histograms show the +distribution if we apply our ADAF correction to the intrinsic +distribution, and demonstrate that this does not +significantly change the result. We note that our model for black +hole accretion employs the Eddington limit as a maximum accretion +rate; if we remove this restriction, we find that the simulations +spend some small but non-negligible time with $l\sim1-2$, which is +also consistent with the observations. + +Furthermore, we can make a prediction of this model which can be +falsified, namely that the Eddington ratio distribution at +luminosities well below the break in the luminosity function should be +broader and extend to lower values than the distribution at +luminosities above the break luminosity. We quantify this in the lower +panels of Figure~\ref{fig:Pofl.all}, for the distribution at low +redshifts $z\lesssim1$. Here we consider two bins in luminosity, +$L=10^{9.5}-10^{10.5}\,L_{\sun}$ and +$L=10^{12.5}-10^{13.5}\,L_{\sun}$, for redshifts where the break in +the luminosity function is at approximately +$L\sim10^{11}-10^{12}\,L_{\sun}$. Clearly, the distribution is +broader and extends to lower Eddington ratios in the former +luminosity interval, whereas in the latter it is strongly peaked about +$l\sim0.2-1$, for both the complete distribution (black) and that with +$\LBo\geq\Lcut{11}$ (red). The distribution obtained applying the ADAF +correction described above is shown as dotted histograms. Despite the +fact that the Eddington ratio distribution at low luminosities will be +strongly biased by selection effects, a reasonably complete sample +should be able to test this prediction, at least qualitatively. + +%\clearpage +\begin{figure} + \centering + \plotone{f21.ps} + %\includegraphics[width=3.7in]{f18.ps} + \caption{Predicted distribution of Eddington ratios based on + the luminosity function and the quasar evolution in our + simulations, at three redshifts $z=0.5$ (top panels), $z=1.0$ (middle), and $z=2.0$ (bottom). + The inferred distribution of Eddington ratios, adopting a constant bolometric + correction from the observed (attenuated) luminosity in each of three bands is shown, + i.e.\ assuming $L=12\,L_{B}^{\rm obs}$ ($4400\,$\AA; left), + $L=52\,L_{SX}^{\rm obs}$ (0.5-2 keV; middle), and + $L=35\,L_{HX}^{\rm obs}$ (2-10 keV; right). For each waveband, results are shown + for three reference luminosities. In B-band, $M_{B}<-19$ (red), $M_{B}<-22$ (blue), + and $M_{B}<-25$ (black). In soft X-rays, $\log(L_{SX} [{\rm erg\,s^{-1}}])>40\ (\rm red),\ + 42\ (\rm blue),\ 44\ (\rm black)$. In hard X-rays, $\log(L_{HX} [{\rm erg\,s^{-1}}])>41\ (\rm red),\ + 43\ (\rm blue),\ 45\ (\rm black)$. + \label{fig:Pofl.grid}} +\end{figure} +%\clearpage + +We illustrate the effects of changing observed waveband, redshift, and +luminosity thresholds on the observed Eddington ratio distribution in +Figure~\ref{fig:Pofl.grid}. Here, we plot the predicted distribution +of Eddington ratios determined as in Figure~\ref{fig:Pofl.all}, from +our fitted $\nLp$ distribution at each redshift and the distribution +of Eddington ratios as a function of instantaneous and peak luminosity +in each of our simulations (specifically, these are drawn from the +Monte Carlo realizations of the quasar population described in +\S~\ref{sec:discussion}). We show the predictions at three redshifts +$z=0.5$ (top panels), $z=1.0$ (middle), and $z=2.0$ (bottom). For +each redshift, results are shown in three wavebands, and with three +reference luminosities. In B-band, we require $M_{B}<-19$ (red), +$M_{B}<-22$ (blue), and $M_{B}<-25$ (black). In soft X-rays, +$\log(L_{SX} [{\rm erg\,s^{-1}}])>40\ (\rm red),\ 42\ (\rm blue),\ 44\ +(\rm black)$. In hard X-rays, $\log(L_{HX} [{\rm erg\,s^{-1}}])>41\ +(\rm red),\ 43\ (\rm blue),\ 45\ (\rm black)$. The observationally +inferred distribution of Eddington ratios at each redshift is loosely +estimated by adopting a constant bolometric correction from the +observed (attenuated) luminosity in each of three bands shown, i.e.\ +assuming $L=12\,L_{B}^{\rm obs}$ ($4400\,$\AA; left), +$L=52\,L_{SX}^{\rm obs}$ (0.5-2 keV; middle), and $L=35\,L_{HX}^{\rm +obs}$ (2-10 keV; right). This follows common practice in many +observational estimates of the Eddington ratio distribution and allows +for the effects of attenuation, but we caution that it +can be misleading. + +If we instead use the luminosity-dependent bolometric corrections of +\citet{Marconi04} which we adopt throughout, even given that we are +calculating from the observed (attenuated) luminosities, we do not see +the large population of highly sub-Eddington (Eddington ratios +$\lesssim10^{-3}$) quasars in soft and hard X-ray samples with low +luminosity thresholds. This is because these are actually reasonably +high-Eddington ratio quasars, %, albeit dim ($L\lessim10^{11}\,L_{\sun}$), quasars, +but our bolometric corrections imply that a larger fraction +of the bolometric luminosity is radiated in the X-ray at low +bolometric luminosity, meaning that assuming a constant bolometric +correction will underestimate the Eddington ratios of high-bolometric +luminosity sources. Regardless, the figure illustrates both the importance +of different wavelengths (i.e.\ the ability to observe more +low-Eddington ratio sources in X-ray as compared to optical samples) +and luminosity/magnitude limits on the inferred distribution of +Eddington ratios. For example, even for relatively deep B-band quasar +samples complete to $M_{B}<-23$ (i.e.\ complete to essentially all +objects traditionally classified as having ``quasar-like'' +luminosities), the expected observed Eddington ratio distribution at +$z\sim0.5-2$ is quite sharply peaked about $\sim0.1-0.3$, in good +agreement with recent observational results \citep{Kollmeier05}. + +We do not compare to the $z=0$ distribution of black hole accretion +rates, as this is dominated by objects at extremely low Eddington +ratios $l\sim10^{-5}-10^{-4}$ +\citep[e.g.,][]{Ho02,Marchesini04,Jester05}, which are well below the +range we model, and are not likely to be driven by merger activity +(many of these objects are quiescent, low-luminosity Seyferts in +normal spiral galaxy hosts); furthermore, many of these objects are +not accreting at the Bondi rate +\citep{FC88,BB99,DiMatteo00,NIA00,QG00,DCF01,Loewenstein01,Bower03}, +clearly showing that our simulations must incorporate more +sophisticated models for accretion in quiescent, low-luminosity states +(when gravitational torques cannot provide a mechanism to drive large +amounts of gas to the central regions of the galaxy) in order to +describe such phases. + +However, it has been suggested that the rapid ``blowout'' phase and +subsequent decay in accretion rates seen in our simulations, coupled +with spectral modeling of radiatively inefficient accretion modes, can +explain the apparently bimodal distribution of low-redshift accretion +rates \citep{CX05}. Moreover, present-day, relaxed ellipticals are +observed to have mass accretion rates $\sim10^{-4}$ implying a long +relaxation time at moderate and low accretion rates, qualitatively +similar to that seen after the ``blowout'' in our modeling (Hopkins et +al. 2005f). A pure exponential decay in accretion rate after the peak +quasar phase would give $\dot{m}=\dot{M}/\dot{M}_{\rm +Edd}\sim\exp{(-t_{H}/t_{Q})}$ at present, where $t_{H}$ is the Hubble +time and $t_{Q}$ is the quasar lifetime of order e.g.\ the Salpeter +time $t_{S}=4\times10^{7}$\,yr, yielding an unreasonably low expected +accretion rate $\dot{m}\sim10^{-145}$. Even assuming an order of +magnitude larger quasar lifetime, this gives $\dot{m}\sim10^{-15}$, +far below observed values, implying that regardless of the fueling +mechanisms at low luminosities, the basic key point of our modeling +must be true to some extent, namely that quasars spend long times +relaxing at moderate to low Eddington ratios. + + +\section{The Mass Function of Relic Supermassive Black Holes from Quasars} +\label{sec:smbh} + +From the $M_{\rm BH}$-$\sigma$ relation and other host galaxy-black +hole scalings, +estimates of bulge and spheroid velocity dispersions have been used to +determine the total mass density ($\rhobh$) and mass distribution of +local, primarily inactive supermassive black holes +\citep[e.g.,][]{Salucci99,MS02,YT02,Ferrarese02,AR02,Marconi04,Shankar04}. +These estimates, along with others based on X-ray background synthesis +\citep[e.g.,][]{FI99,ERZ02}, have compared these quantities to those +expected based on the mass distribution of `relic' black holes grown +in quasars. It appears that most, and perhaps nearly all of the +present-day black hole mass density was accumulated in bright quasar +phases, and the $M_{\rm BH}-\sigma$ and $M_{\rm BH}-L_{\rm bulge}$ +correlations yield estimates of the local mass function in good +agreement with those from hard X-ray AGN luminosity functions +\citep{Marconi04}. + +However, this modeling is dependent on several assumptions. Namely, +the average radiative efficiency $\epsilon_{r}$, Eddington ratio $l$, +and average quasar lifetime $t_{Q}$ are generally taken to be +constants and either input into the model or constrained by demanding +agreement with the local mass function. In our simulations, we find +the quasar lifetime and Eddington ratio to be complex functions of +both luminosity and host system properties (as opposed to being +constants). We also find that quasars spend a large fraction of their +lives in obscured growth phases, suggesting some mass gain outside of +the bright quasar phase. It is thus of interest to determine the relic +black hole mass function expected from our model for quasar evolution. + +Using our estimate for the birthrate of quasars with a given peak +luminosity at a particular redshift, $\nLp$, obtained from the +luminosity function in \S~\ref{sec:fullLF}, we can estimate the total +number density of relic quasars accumulated by a particular redshift +that were born with a given $\Lp$ (per logarithmic interval in $\Lp$) +from +\begin{equation} +n(\Lp)=\int{\,\nLp\,{\rm d}t}=\int{\frac{\dot{n}(\Lp,z)\,{\rm d}z}{(1+z)H(z)}}. +\end{equation} +By redshift $z=0$, most of these quasars will be ``dead,'' with only +a small residual fraction having been activated in the recent past. + +Using our log-normal form for $\nLp$, with normalization $\nstar$ and +dispersion $\sstar$ held constant and only the median +$\lstar=\lstar^{0}\,\exp{(k_{L}\tau)}$ evolving with redshift, this +integral can be evaluated numerically to give the space density of +relic quasars $n(\Lp)$. Finally, we use $\mbhf(\Lp)$, roughly the +Eddington mass of the given peak luminosity (but determined more +precisely in \S~\ref{sec:detailsCompare}) to convert from ${\rm +d}n(\Lp)/{\rm d}\log\Lp$ to ${\rm d}n(M_{\rm BH})/{\rm d}\log M_{\rm +BH}$. This formulation implicitly assumes that black holes do not +undergo subsequent mergers after the initial quasar-producing event. +However, this effect should be small (a factor $\lesssim2$) as +subsequent mergers would be dry (gas poor). +We explicitly calculate the effects of dry mergers on the +spheroid mass function (essentially a rescaling of the black hole mass +function calculated here) in \citet{H05e}, and show that this is a +small effect (significantly less than the uncertainties owing to our +fit to the quasar luminosity function) even assuming the maximum dry +merger rates of e.g.\ \citet{vanDokkum05}. + +This mass function can then be integrated over $d M_{\rm BH}$ to give +the total present-day black hole mass density, $\rhobh$. Neglecting +temporarily the small corrections to $\mbhf(\Lp)$ from +\S~\ref{sec:detailsCompare}, we expect +\begin{equation} +\mbhf\approx M_{\rm Edd}(\Lp)=\frac{\Lp\,t_{S}}{\epsilon_{r}c^{2}} +%2.95\times 10^{-5} M_{\sun} \, \Bigl( \frac{\Lp}{L_{\sun}}\Bigr), +\end{equation} +where $t_{S}/\epsilon_{r}c^{2}\approx2.95\times10^{-5}\,M_{\sun}/L_{\sun}$, +so therefore, +\begin{equation} +\rhobh=\frac{t_{S}}{\epsilon_{r}c^{2}}\int{\Lp\,n(\Lp)\,{\rm d}\log \Lp}. +\end{equation} +This can be combined with the integral over redshift for $n(\Lp)$, +giving, at each $z$, a pure Gaussian integral over $\log{(\Lp)}$, +in the form +%\begin{equation} +%\begin{split} +%\rhobh &=\frac{\lstar^{0}\,t_{S}}{\epsilon_{r}c^{2}}\frac{\nstar}{H_{0}}\, +%e^{\frac{1}{2}(\sstar \ln{10})^{2}}\,\int{\frac{e^{k_{L}\tau}\,dz}{(1+z)\,\hat{H}(z)}}\\ +%&= \frac{\lstar^{0}\,t_{S}}{k_{L}\epsilon_{r}c^{2}}\frac{\nstar}{H_{0}}\, +%e^{\frac{1}{2}(\sstar \ln{10})^{2}}\,\Bigl(e^{k_{L}\tau_{f}}-e^{k_{L}\tau}\Bigr), +%\end{split} +%\end{equation} +\begin{eqnarray} +\rhobh &=&\frac{\lstar^{0}\,t_{S}}{\epsilon_{r}c^{2}}\frac{\nstar}{H_{0}}\, +e^{\frac{1}{2}(\sstar \ln{10})^{2}}\,\int{\frac{e^{k_{L}\tau}\,dz}{(1+z)\,\hat{H}(z)}}\nonumber\\ +&=& \frac{\lstar^{0}\,t_{S}}{k_{L}\epsilon_{r}c^{2}}\frac{\nstar}{H_{0}}\, +e^{\frac{1}{2}(\sstar \ln{10})^{2}}\,\Bigl(e^{k_{L}\tau_{f}}-e^{k_{L}\tau}\Bigr), +\end{eqnarray} +where $\hat{H}(z)\equiv H(z)/H_{0}$ and $\tau_{f}$ is the fractional +lookback time at some upper limit. We must modify this integral above +$z\sim2$ to account for the decreasing space density of bright +quasars, applying either our density or peak-luminosity evolution +turnover from \S~\ref{sec:fullLF}, but quasars at these high redshifts +contribute only a small fraction to the present-day density. Thus, in +this formulation, the evolution of the total supermassive black hole +mass density, i.e.\ $\rhobh(z)/\rhobh(z=0)$, is given approximately by +the dimensionless integral above, and depends only on how +$\lstar$ evolves, essentially the rate at which the break +in the quasar luminosity function shifts. Although this is not strictly +true if we include corrections to $\mbhf(\Lp)$ based on $\Lp$, the +difference is small and this behavior is essentially preserved. Note +that the total supermassive black hole mass density is independent of +corrections from subsequent dry mergers, which (being gas poor) conserve +total black hole mass. + +%\clearpage +\begin{figure*} + \centering + \plotone{f22.ps} + %\includegraphics[width=3.7in]{f19.ps} + \caption{Right: Total predicted quasar relic black hole mass + density and evolution of the fractional black hole mass + density with redshift. Dotted lines show the difference resulting + from $1\sigma$ deviation in fitted $\nLp$ from the luminosity + function. Left: Predicted present $z=0$ relic mass function + (thick black line), for comparison with the $1\sigma$ range + (yellow) of the inferred supermassive black hole mass function + from \citet{Marconi04}. Also shown are the results given $1\sigma$ + errors in the fitted $\nLp$ distribution (dotted lines), or ignoring + the small corrections to $\mbhf(\Lp)$ from \S~\ref{sec:detailsCompare} + (thin black line). Dot-dashed lines show the predicted mass + function at $z=1.5,\,3.0,\,5.0$ (blue, green, and red, + respectively). The extensions to $z>2$ includes the turnover (pure + peak luminosity evolution form) in the quasar space density above + $z=2$ from high-redshift luminosity functions described in + \S~\ref{sec:fullLF}, except for the dashed green and red lines + which use the pure density evolution form. + \label{fig:SMBH.distrib}} +\end{figure*} +%\clearpage + +Figure~\ref{fig:SMBH.distrib} shows our prediction for the mass +distribution of supermassive black holes, as well as the total density +$\rhobh$ and its evolution with redshift. We find a total relic black +hole mass density of +$\rhobh=2.9^{+2.3}_{-1.2}\times10^{5}\,M_{\sun}\,{\rm Mpc^{-3}}$, in +agreement with the observational estimate of +$\rhobh=2.9\pm0.5\,h^{2}_{0.7}\times10^{5}\,M_{\sun}\,{\rm Mpc^{-3}}$, +by \citet{YT02} ($h_{0.7}\equiv H_{0}/70\,{\rm km\,s^{-1}\,Mpc^{-1}}$; +their result is converted from $h=0.65$), and within $1\sigma$ of the +value $\rhobh=4.6^{+1.9}_{-1.4}h^{2}_{0.7}\times10^{5}\,M_{\sun}\,{\rm +Mpc^{-3}}$, of \citet{Marconi04}, based on the observations of +\citet{Marzke94}, \citet{Kochanek01}, \citet{Nakamura03}, +\citet{Bernardi03}, and \citet{Sheth03}. The fractional evolution of +$\rhobh$ with redshift is quite well constrained, and we find, as with +previous estimates, that most of the present-day black hole mass +density accumulates at moderate to low redshifts +$z\approx 0.5 - 2.5$. The $1\sigma$ +errors are shown as dotted lines in the figure, and are close to our +best-fit estimate, as we have demonstrated that this quantity depends +only on $k_{L}$, the rate of evolution of the break in +the luminosity function +with redshift, which is fairly well-constrained by +observations (from our fitting to the luminosity functions, +$k_{L}=5.61\pm0.28$). The difference in $\rhobh$ if we include or +neglect the small corrections to $\mbhf$ is negligible compared to our +errors ($\sim5\%$). + +Our estimate for the relic black hole mass distribution (thick black +line) also agrees well with observational estimates, with all +observations within the range allowed by the $1\sigma$ errors of our +fitting to the luminosity function (dotted lines). The observations +shown are again from \citet{Marconi04}, based on the combination of +observations by \citet{Marzke94}, \citet{Kochanek01}, +\citet{Nakamura03}, \citet{Bernardi03}, and \citet{Sheth03}. The high +mass end of the black hole mass function $M_{\rm BH}>10^{9}\,M_{\sun}$ +is relatively sensitive to whether or not we apply the $\mbhf(\Lp)$ +corrections of \S~\ref{sec:detailsCompare}, instead of taking +$\mbhf=M_{\rm Edd}(\Lp)$ (thin line), as well as to our fitting +procedure. However, the agreement is still good, and this is also +where the observational estimates of the mass distribution are most +uncertain, as they are generally extrapolated to these masses, and are +sensitive to the assumed intrinsic dispersions in the $M_{\rm +BH}-\sigma$ and $M_{\rm BH}-L_{\rm bulge}$ relations \citep{YT02}. + +If, instead, we adopt a light-bulb, constant Eddington ratio, or +exponential light curve model for quasar evolution, we would have +$M_{\rm BH}^{f}\propto \Lp$, and thus the prediction would be similar +to the thin black line shown, a somewhat worse fit at high black hole +masses. However, in these models this can be remedied by adjusting the +typical Eddington ratios, quasar lifetimes, or radiative +efficiencies. We do not show the range of predictions of these models +for the relic supermassive black hole mass function, as they have been +examined in detail previously +\citep[e.g.,][]{Salucci99,MS02,YT02,Ferrarese02,AR02,Marconi04,Shankar04}. +These works demonstrate that the observed quasar luminosity functions +are consistent with the relic supermassive black hole mass function, +given typical radiative efficiencies $\epsilon_{r}\sim0.1$ and +Eddington ratios $\sim0.5-1.0$, and that most of the mass of black +holes is accumulated in bright, observed phases, or else the required +radiative efficiency would violate theoretical limits. + +That our model of quasar lifetimes and obscuration reproduces the +observed $z=0$ supermassive black hole mass function explicitly +demonstrates that we are consistent with these constraints. By +choice, the radiative efficiency in our simulations is +$\epsilon_{r}=0.1$, and accretion rates are not allowed to exceed +Eddington. As noted in \S~\ref{sec:BLqso}, most of the black hole mass +is accumulated and radiant energy released in the final, ``blowout'' +phase of quasar evolution, and here our black hole mass function and +cumulative black hole mass density demonstrate that our modeling is +consistent with integrated energy and mass arguments such as that of +\citet{Soltan82}, despite the fact that quasars spend more {\em time} +in obscured phases than they do in bright optical quasar phases. In +fact, comparison of our predicted total black hole mass density with +estimates from the $z=0$ black hole mass distribution allows some +latitude for significant mass gain in radiatively inefficient growth +or black holes in small, disky spheroids, although we emphasize that +this is mainly because the uncertainty in our prediction is large, it +is not inherent or necessary in our modeling. + +%\clearpage +\begin{figure*} + \centering + %\epsscale{1.1} + \plotone{f23.ps} + %\includegraphics[width=3.7in]{f20.ps} + \caption{Fractional number + density $n(M,\,z)/n(M,\,z=0)$ of black holes of a given mass as a function of + redshift, for several different black hole masses as shown. For + $z>2$ this includes the turnover (pure density evolution + form) in the quasar space density above $z=2$ from high-redshift + luminosity functions described in \S~\ref{sec:fullLF}. + Left panel shows the results using our full model of quasar lifetimes, + right panel assuming a ``light-bulb'' or exponential (constant + Eddington ratio) light curve model. + The yellow dot-dash ($10^{9}\,M_{\sun}$) and red triple-dot-dash + ($10^{10}\,M_{\sun}$) curves are nearly identical in the right panel. + \label{fig:SMBH.evol}} +\end{figure*} +%\clearpage + +The anti-hierarchical nature of black hole formation, where less +massive black holes are formed at lower redshift, is reflected in our +modeling by the shift of the break in the quasar luminosity function +to lower values with decreasing redshift. This can be seen in +Figure~\ref{fig:SMBH.distrib}, where the black hole mass distributions +are shown at redshifts $z=1.5,\,3.0\ {\rm and}\ 5.0$, assuming either +pure peak luminosity evolution or pure density evolution for $z>2$ +(dot-dashed and dashed, respectively). While the choice for the +turnover in the $z>2$ quasar density matters little for the $z<2$ +black hole mass functions, the low-$M_{\rm BH}$ distribution at high +redshift (where observations do not constrain $\nLp$ well) is quite +different between the two models. Figure~\ref{fig:SMBH.evol} plots +the fractional number density of black holes of a given mass as a +function of redshift, i.e.\ $n(M,\,z)/n(M,\,z=0)$, where $n(M)={\rm +d}n/{\rm d}\log{(M)}$ is just the number density at mass $M$. This +figure demonstrates that higher-mass black holes originated over a +larger range of redshifts, and that they mostly formed +at higher redshift, compared to lower-mass black holes. + +The right panel of Figure~\ref{fig:SMBH.evol} compares our prediction +to that of a light-bulb or exponential light curve model for quasar +lifetimes. In these models, the anti-hierarchical nature of black +hole assembly is dramatically suppressed. At the high-mass end, there +is no measurable difference in the distribution of formation redshifts +(i.e.\ the $M_{\rm BH}=10^{9}\,M_{\sun}$ and $M_{\rm +BH}=10^{10}\,M_{\sun}$ curves are indistinguishable), and there is +little change in the formation times at $M_{\rm BH}=10^{8}\,M_{\sun}$. +The shift in formation redshift at lower masses, although significant, +is smaller than that predicted in our model. If spheroids and black +holes are produced together, as in our picture, these models of the +quasar lifetime would imply that spheroids of masses $M_{\rm +vir}\sim10^{11}-10^{13}\,M_{\sun}$ all formed over nearly identical +ranges of redshifts, which is inconsistent with many observations +indicating anti-hierarchical growth of the red, elliptical galaxy +population \citep[e.g.,][]{Treu01,vanDokkum01,Treu02, +vDS03,Gebhardt03,Rusin03,vandeVen03,Wuyts04,Treu05,Holden05, +vdW05,SA05,Nelan05}. Implications of our model for the red galaxy +sequence are considered in \citet{H05e}, where we show that this +weaker anti-hierarchical black hole (and correspondingly, spheroid) +evolution is inconsistent with observed luminosity functions, +color-magnitude relations, and mass-to-light ratios of elliptical +galaxies. + +Our modeling reproduces the observed total density and mass +distribution of supermassive black holes at $z=0$ with black holes +accreting at the canonical efficiency $\epsilon_{r}=0.1$ expected for +efficient accretion through a \citet{SS73} disk. Presumably, a large +change in $\epsilon_{r}$ would give a significantly different relation +between peak luminosity and black hole mass (for the same $\Lp$, +$M_{\rm BH}^{f}\propto 1/\epsilon_{r}$), and thus if the quasar +lifetime remained similar as a function of peak luminosity, this would +translate to a shift in the black hole mass function. The long +obscured stage in black hole evolution does not generate problems in +reproducing the black hole mass density, and the final phases of +growth are still in bright optical quasar stages. However, a large +Compton-thick population of black holes at all luminosities (or even +at some range of luminosities at or above the break in the luminosity +function) \citep[e.g.,][]{Gilli01,Ueda03}, or a large population +accreting in a radiatively inefficient ADAF-type solution, +as invoked to explain discrepancies in the X-ray +background produced by synthesis models \citep{DEFN99}, would result in a significant +over-prediction of the present-day supermassive black hole density. +As we demonstrate in \S~\ref{sec:xrb.tot}, invoking such populations +is unnecessary, as our picture for quasar lifetimes and evolutionary +obscuration self-consistently reproduces the observed X-ray +background. + +Finally, we note that we reproduce the $z=0$ distribution of black +hole masses {\em inferred} from the distribution of spheroid velocity +dispersions \citep{Sheth03} and luminosity functions +\citep{Marzke94,Kochanek01,Nakamura03}, based on the observed $M_{\rm +BH}-\sigma$ relation and fundamental plane for galaxy properties +\citep[e.g.,][]{Bernardi03,Gebhardt03}. Therefore, since our modeling +also reproduces the observed $M_{\rm BH}-\sigma$ +\citep{DSH05,Robertson05b} and fundamental plane (Robertson et al., in +preparation) relations, we implicitly reproduce the $z=0$ distribution +of spheroid velocity dispersions and spheroid luminosity functions, +given our basic assumption that the mergers that produce these +spheroids also give rise to luminous quasar activity. + +\section{The Cosmic X-Ray Background} +\label{sec:xrb} +\subsection{The Integrated Spectra of Individual Quasars} +\label{sec:xrb.indiv} + +Unresolved extragalactic sources, specifically obscured AGN, have been +invoked to explain the cosmic X-ray background \citep[e.g,][]{SW89}. +This picture has been confirmed as deep surveys with {\it Chandra} and +{\it XMM-Newton} have resolved most or all of the X-ray background +into discrete sources, primarily obscured and unobscured AGN +\citep{Brandt01,Hasinger01,Rosati02,Giacconi02,Baldi02}. The X-ray +background, however, has a harder X-ray spectrum than typical quasars, +with a photon index $\Gamma\sim1.4$ in the $1-10$\,keV range +\citep{Marshall80}. Therefore, obscured AGN are important in +producing this shape, as absorption in the ultraviolent and soft +X-rays hardens the observed spectrum. Indeed, population synthesis +models based on observed quasar luminosity functions and involving +large numbers of obscured AGN have been successful at matching both +the X-ray background intensity and spectral shape +\citep{Madau94,Comastri95,Gilli99,Gilli01}. However, these models make +arbitrary assumptions about the ratio of obscured to unobscured +sources and its evolution with redshift, choosing these quantities to +reproduce the X-ray background. Furthermore, as X-ray surveys have +been extended to higher redshifts, it has become clear that both the +observed redshift distribution of X-ray sources and the ratio of +obscured to unobscured sources is inconsistent with that required by +these models \citep{Hasinger02,Barger03}. Even synthesis models based +on higher-redshift X-ray surveys and using observationally derived +ratios of obscured to unobscured sources \citep[e.g.,][]{Ueda03} have +invoked ad hoc assumptions about additional populations of obscured +sources to reproduce the X-ray background shape and intensity. + +%\clearpage +\begin{figure*} + \centering + \plotone{f24.ps} + %\includegraphics[width=3.7in]{f21.ps} + \caption{Left: Integrated intrinsic spectra (thick solid lines) + from simulations A1, A2, A3, A4, and A5 (black, blue, green, + yellow, red, respectively), with virial velocities $\vvir=80,\, 113,\, + 160,\, 226,\, {\rm and}\ 320\,{\rm km\,s^{-1}}$. The predicted + integrated spectra from our model for quasar lifetimes are shown + as dot-dashed lines, and the prediction of a ``light bulb'' + model, where the same total energy is radiated at $L=\Lp$, as + dashed lines. Integrated observed spectra are shown as thin solid + lines. Right: Integrated observed X-ray spectrum from the A3 + simulation (thick black line), compared with the integrated + intrinsic spectrum, reddened by various column density + distributions: our fitted \NH\ distributions from \S~\ref{sec:NHfunction} + (thick black dashed line), constant (luminosity-independent) lognormal + \NH\ distribution with $\meanNH=10^{22}\ {\rm cm^{-2}}$ and + $\sigNH=0.4,\,0.7,\,1.0$ (blue, green, and red dashed lines, + respectively), and constant + $\nh=10^{21},\,10^{21.5},\,10^{22},\,10^{22.5},\ {\rm and}\ 10^{23}\ + {\rm cm^{-2}}$ (thin dot-dashed lines). + \label{fig:integ.spectra}} +\end{figure*} +%\clearpage + +We can test our model by examining whether the quasar luminosity +function, relic AGN mass distribution, and X-ray background can be +simultaneously reproduced in a self-consistent manner. Because our +formulation describes the birthrate of quasars with a peak luminosity +$\Lp$, it is most useful to consider the integrated energy spectrum of +such a quasar over its lifetime, +\begin{equation} +\nu E_{\nu} = \int{{\rm d}t\,\nu L_{\nu}(t)} = \int{\nu f_{\nu}(L) + L\,\frac{{\rm d}t(L,\Lp)}{{\rm d}\log L}\,{\rm d}\log L}, +\end{equation} +where $f_{\nu}(L)$ is the bolometric correction ($L_{\nu}\equiv +f_{\nu}\,L$). As an example, +Figure~\ref{fig:integ.spectra} shows the integrated +intrinsic spectra (thick solid lines) from the simulations +A1, A2, A3, A4, and A5, +described in \S~\ref{sec:sims}. The final black hole masses for these +simulations are +$\mbhf=7\times10^{6},\,3\times10^{7},\,3\times10^{8},\,7\times10^{8},\,{\rm +and}\ 2\times10^{9}\, M_{\sun}$, +respectively. The integrated spectral shape in the +X-ray, in particular, is ultimately determined by the observationally +motivated bolometric corrections of \citet{Marconi04}, with a +reflection component in the X-ray determined following \citet{MZ95}, +and, in the case of the observed spectrum, the distribution of column +densities calculated from the simulations. Using our fits +to the lifetime $\dtdL$ as a function of instantaneous and peak +luminosities, we can calculate the expected $\nu E_{\nu}$ from the +integral above. These integrated spectra are shown as the dot-dashed +lines in the figure, and agree well with the actual integrated spectra +of the simulations, demonstrating the self-consistency of our model +and applicability of our fitted lifetimes. + +This can be compared to idealized models for the quasar lifetime, +where we allow the quasar to radiate just at its peak luminosity +$\Lp\approx L_{\rm Edd}(\mbhf)$ for some fixed lifetime +$t_{Q}^{0}$. We determine $t_{Q}^{0}$ by demanding that the total +energetics be correct, $\Lp t_{Q}^{0} = \epsilon_{r}\mbhf c^{2}$. The +predicted integrated energy spectra are shown as the dashed lines, and +under-predict the soft and hard X-ray energy output by a factor +$\sim1.5-2$. This is because higher-luminosity quasars tend to have a +larger fraction of their energy radiated in the UV-optical rather than +the X-ray \citep[e.g.,][]{Wilkes94,Green95,VBS03,Strateva05}, +reflected in our bolometric corrections. Thus, assuming that the +quasar spends all its time at $\Lp$ does not account for extended +times at lower luminosity, where the ratio of X-ray to total +luminosity is higher, which would generate an integrated spectrum with +a larger fraction of its energy in the X-ray. Assuming that the quasar +undergoes pure Eddington-limited growth to its peak luminosity +produces an almost identical integrated spectrum to this light-bulb +model, as it is similarly dominated by $L\sim\Lp$. + +Of course, the intrinsic integrated energy spectrum of the simulations +is not what determines the X-ray background, but rather the integrated +{\em observed} spectrum is the critical quantity. This is shown as the +thin lines in the left panel of Figure~\ref{fig:integ.spectra}, and in +detail for our fiducial A3 simulation in the right panel of the figure +(thick solid line). Along a given sightline, the observed integrated +spectrum will be +\begin{equation} +\nu \frac{{\rm d} E_{\nu}}{{\rm d}\Omega}=\int{{\rm d}t\,\nu \frac{L_{\nu}(t)}{4\pi}\,e^{-\tau_{\nu}(\Omega,\,t)}}, +\end{equation} +where $\tau_{\nu}$ is the optical depth at a given frequency. +We can integrate over solid angle and obtain +\begin{equation} +\nu E_{\nu,\,{\rm obs}} = \int{\nu f_{\nu}\EV{e^{-\tau_{\nu}}}\, + L\,\frac{{\rm d}t(L,\Lp)}{{\rm d}\log L}\,{\rm d}\log L}, +\end{equation} +where $\EV{e^{-\tau_{\nu}}}$ is the averaged $e^{-\tau_{\nu}}$ over +the column density distribution $P(\nh | L,\Lp)$. Using our fits to +the column density distribution and quasar lifetimes and calculating +$\nu E_{\nu,\,{\rm obs}}$ as above, we reproduce the integrated +observed spectrum quite well (black dashed line). For +comparison, we show that it is not a good approximation to redden the +spectrum with a constant \NH, giving the results for +$\nh=10^{21},10^{21.5},10^{22},10^{22.5},\ {\rm and}\ 10^{23}\ {\rm +cm^{-2}}$ (thin dot-dashed lines). Even allowing for a distribution +of \NH\ values, the resulting spectrum is a poor match to the observed +one if that distribution is taken to be static (i.e.\ +luminosity-independent, as in traditional torus models, for +example). We show the results of reddening the intrinsic spectrum by +such a (Gaussian) distribution, varying the dispersion $\sigNH=0.4,\,0.7,\,1.0$ +(blue, green, and red dashed lines, respectively), for a median column +density $\meanNH=10^{22}\ {\rm cm^{-2}}$, the median column density +expected around $\Lp$ in this simulation. Therefore, the luminosity and host system +property dependence of both quasar lifetimes and the column density +distribution must be accounted for in attempting to properly predict +the X-ray background spectrum from observations of the quasar +luminosity function. Finally, note that the hard cutoff in the +observed UV spectra at 912\AA\ owes to our calculated cross-sections +being incomplete in the extreme UV. Properly modeling the escape +fraction and observed emission at these frequencies, while not +important for the X-ray background, is critical to calculating the +contribution of quasars to reionization, and requires a more +detailed modeling of scattering and absorption, especially in the +bright optical quasar phase. + +\subsection{The Integrated X-Ray Background} +\label{sec:xrb.tot} + +Given the volume emissivity $j_{\nu}(z)$ (per unit {\em +comoving} volume) of some isotropic process at a given frequency at +redshift $z$, the resulting background specific intensity at frequency +$\nu_{0}$ at $z=0$ is \citep{Peacock99} +\begin{equation} +I_{\nu_{0}} = \frac{c}{4\pi} +\int{\frac{j_{\nu}[(1+z)\nu_{0},z]}{(1+z)H(z)}} {\rm d}z. +\end{equation} +If we were to consider the emissivity $j_{\nu}$ per unit +physical volume, there would be an extra factor of $(1+z)^{-3}$ in the +integral above. In \S~\ref{sec:xrb.indiv}, we determined the +integrated observed energy $E_{\nu,\, \rm obs}(\Lp)$ produced by a +quasar with peak luminosity $\Lp$. We have also inferred $\nLp(z)$ +in \S~\ref{sec:fullLF}, the rate at which quasars of peak luminosity +$\Lp$ are created per unit comoving volume per unit cosmological +time. Therefore, the comoving volume emissivity is just +\begin{equation} +j_{\nu}(z) = \int{E_{\nu,\, \rm obs}(\Lp)\,\nLp\,d\log \Lp}, +\end{equation} +or, expanding $E_{\nu,\, \rm obs}$, +%\begin{equation} +%\begin{split} +%j_{\nu}(z) = & \int{d\log \Lp\int{d\log L}} \\ +% & \times f_{\nu}\EV{e^{-\tau_{\nu}}}\, L\,\frac{dt(L,\Lp)}{{\rm d}\log L}\,\nLp. +%\end{split} +%\end{equation} +\begin{eqnarray} +j_{\nu}(z)& = & \int{d\log \Lp\int{d\log L}} \nonumber\\ + && \times f_{\nu}\EV{e^{-\tau_{\nu}}}\, L\,\frac{dt(L,\Lp)}{{\rm d}\log L}\,\nLp. +\end{eqnarray} +If the column density distribution were independent of +$\Lp$, as is assumed in even luminosity-dependent torus models or +observationally determined \NH\ functions used for X-ray background +synthesis \citep[e.g.,][]{Ueda03}, then we could combine terms in +$\Lp$ and integrate over them. This simplification, along with the +definition of the luminosity function in terms of $\Lp$, gives the +more traditional formula for the X-ray background in terms of only the +observed column density distribution and luminosity function, +\begin{equation} +j_{\nu}(z) = \int{d\log L\,\frac{d\Phi}{d\log L} L_{\nu}\EV{e^{-\tau_{\nu}}}}. +\label{eq:simple.XRB} +\end{equation} +However, as we showed in \S~\ref{sec:NHdistrib} and +\S~\ref{sec:xrb.indiv}, neglecting the dependence on $\Lp$ is not a +good approximation at all luminosities and gives an inaccurate +estimate of the integrated quasar spectrum; therefore, ``purely +observation-based'' synthesis models of the X-ray background will be +inaccurate in a similar manner to synthesis models with an +inappropriate model for the quasar lifetime. Essentially, this +``averages out'' the varying distribution of column densities with +$\Lp$, which changes the shape of the spectrum in a non-linear manner, +especially when integrated over varying bolometric corrections as +shown above. + +%\clearpage +\begin{figure} + \centering + %\epsscale{.7} + \plotone{f25.ps} + %\includegraphics[width=3.7in]{f22.ps} + \caption{Predicted integrated X-ray background spectrum (solid + black line) from our model of quasar lifetimes and attenuation, + with the peak luminosity distribution $\nLp$ determined from the + luminosity function. Blue and red thick lines show the observed spectrum + from \citet{Barcons00} and \citet{Gruber99}, respectively. The + shaded yellow area illustrates the uncertainty in normalization + between both samples (alternatively, $2\sigma$ errors in the + Barcons et al.\ 2000 normalization). The predictions given + $1\sigma$ deviations in the fitted $\nLp$ distribution (dotted + lines) and given the $\nLp$ distribution determined from hard + X-ray data only (dashed line) are shown in the upper panel. Middle + panel shows the prediction using our modeling of quasar lifetimes + but different models of obscuration, lower panel the prediction with a + ``light-bulb'' or exponential (constant Eddington ratio) model + and different obscuration models. + \label{fig:XRB.spectrum}} +\end{figure} +%\clearpage + +Figure~\ref{fig:XRB.spectrum} (upper panel) shows the predicted X-ray +background spectrum from our full modeling of quasar lifetimes and +obscuration (solid lines). We use our analytical fits to the quasar +lifetime and column density distributions as in \S~\ref{sec:xrb.indiv} +above, as Figure~\ref{fig:integ.spectra} demonstrates that they +accurately reproduce the actual integrated quasar X-ray spectra of the +simulations, and the analytical forms are integrated over all +luminosities and redshifts. The dotted lines show the deviation +resulting from shifting the parameters describing our fitted $\nLp$ +distribution by $1\sigma$ in either direction, although degeneracies +in the parameters suggest that the actual uncertainty in the +background prediction is smaller. The dashed line shows the predicted +X-ray background if we ignore the broadening of the \NH\ distribution +across simulations ($\sigNH=1.2$) and instead consider only the +dispersion of an individual simulation at a given luminosity +($\sigNH=0.4$). + +These can be compared to the observations of \citet{Gruber99} (red +curve, for $E\geq3\,{\rm keV}$) and \citet{Barcons00} (cyan curve, for +$E\leq10\,{\rm keV}$). We increase the normalization of the +\citet{Gruber99} spectrum to match that of the best estimate from +\citet{Barcons00} over the range of overlap, determined from combined +{\it ASCA, BeppoSAX,} and {\it ROSAT} data to be +$10.0^{+0.6}_{-0.9}\,{\rm keV\,cm^{-2}\,s^{-1}\,sr^{-1}\,keV^{-1}}$ at +1\,keV. The uncertainty in the normalization between the two samples, +$\sim20\%$, is shown as the shaded yellow range (alternatively, this +represents the $\sim2\sigma$ errors in the {\it ROSAT} normalization). + +In the middle panel of the figure, we calculate the predicted X-ray +background using our full model of the quasar lifetime, but with +different models for quasar obscuration. The solid black line shows +the prediction using our full model of quasar obscuration, and is +identical to the solid black line in the upper panel. The observations +are likewise shown in an identical manner to the upper panel. The +dashed black line is the prediction adopting the standard torus model +for quasar obscuration, and the dotted line adopts the receding +(luminosity-dependent) torus model. These models produce the same +overall $\sim30\,$keV normalization, as this is relatively unaffected +by obscuration, but they predict a slightly ($\sim20\%$) higher +background at low energies, giving a slightly softer spectrum. This +may appear counterintuitive, given that in Figure~\ref{fig:NH.distrib} +these models tend to overpredict the number of high-column density +sources, but this is because these models predict a strongly {\em +bimodal} column density distribution, with unobscured sightlines +encountering negligible column densities. These unobscured sightlines +dominate the soft X-ray integrated spectrum, where the large column +densities through the torus attenuate the quasar spectrum heavily. +However, this net offset in the predicted background spectrum is +generally within the range of the systematic theoretical and +observational uncertainties, and can further be alleviated by tuning +the parameters of the torus model to fit the X-ray background spectrum +(e.g.\ Treister \& Urry 2005, although their fits require a larger +fraction of Compton-thick $\nh\sim10^{25}\,{\rm cm^{-2}}$ sources than +shown for even the receding torus model in +Figure~\ref{fig:NH.distrib}). The feature at +$\lesssim5\,$keV in the standard torus model prediction is a +consequence of assuming that ``unobscured'' lines of sight encounter +negligible column density, and does not appear if such sightlines +encounter moderate ($\sim10^{21}\,{\rm cm^{-2}}$) columns. + +The lower panel of the figure shows the predicted X-ray background +spectrum if we instead consider a light-bulb or exponential light +curve (fixed Eddington ratio) model for the quasar lifetime, again +with various descriptions of quasar obscuration. In such models, the +predicted X-ray background spectrum is independent of the quasar +lifetime or characteristic Eddington ratio assumed (see +Equation~\ref{eq:simple.XRB}). However, as shown in +Figure~\ref{fig:integ.spectra}, these models do imply a different +integrated spectrum for quasars; i.e.\ different effective bolometric +corrections for predicting the X-ray background. In particular, in +this model, the observed quasar spectrum at a given luminosity +(averaged over the quasar population at that luminosity) is the same +as the ``effective'' quasar spectrum one would use to calculate the +{\em total} contribution to the X-ray background from quasars of the +corresponding observed or peak luminosity, whereas this is not true in +our model of quasar lifetimes. The observations are shown in the same +manner as the preceding panels. The black solid line shows the +prediction with this simplified model for the quasar lifetime, but +still adopting our full model for obscuration as a function of +instantaneous and peak luminosity, the dashed line assumes instead a +standard torus model for obscuration, and the dotted line assumes a +receding torus for the obscuration. The variations among different +obscuration models are relatively small at most energies, and similar +to those discussed above adopting our full model of quasar +lifetimes. + +In all three cases, however, this model for the quasar lifetime +significantly under-predicts the X-ray background, particularly at the +$\sim30\,$keV peak. This shortfall is well-known, and earlier attempts +\citep[e.g.,][]{Madau94,Comastri95,Gilli99,Gilli01,Pompilio00,Ueda03} +have generally had to invoke additional assumptions about large +obscured populations or a strong increase in the obscured fraction +with redshift, neither of which is consistent with observations +\citep[e.g.,][]{Hasinger02,Barger03,Ueda03,Szokoly04,Barger05}. The +difference between the predictions of various quasar lifetime models +is, as explained above, attributable to the difference between the +integrated quasar spectrum produced in our full model of the quasar +lifetime (in which quasars spend long periods of time at low +luminosities, with harder X-ray spectra), and the integrated spectrum +in these simplified quasar lifetime models, which is proportional to +the {\em instantaneous} quasar spectrum, and therefore underpredicts +the hard X-ray portion of the spectrum by as much as $\sim50\%$. + +Our prediction of the X-ray background agrees well with the observed +spectrum over the range $\sim1-100\,{\rm keV}$. (At energies above +$100\,{\rm keV}$ it is likely that processes we have not included, +such as those involving magnetic fields, contribute significantly to +the background.) Unlike previous synthesis models for the X-ray +background, we are able to do so without invoking assumptions about +large Compton thick populations or larger obscured populations at +different redshifts. In part, this is because our modeling allows us +to predict, based on $\nLp$ and our column density formulation, the +population of Compton thick sources (see +Figure~\ref{fig:NH.distrib}). However, as we have demonstrated, it is +primarily because the deficit in previous synthesis models can be +attributed to their inability to properly account for the dependence +of quasar lifetimes and attenuation on both the instantaneous quasar +luminosity and the host system properties (peak luminosity). Our +picture, on the other hand, yields an estimate for the X-ray +background spectrum that is simultaneously consistent with the +observed supermassive black hole mass distribution and total density, +as well as the ``luminosity-dependent density evolution'' observed in +X-ray samples \citep{H05f}. The background is primarily built up from +$z\sim2.5$ to $z\sim0.5$, as is evident from the evolution of the black +hole mass density in Figure~\ref{fig:SMBH.distrib}, although a harder +spectrum at low luminosities will weight this slightly towards lower +redshifts (where more low-luminosity quasars are forming). Compton +thick and relaxing, low-luminosity sources are accounted for, not as +large, independent populations, but as evolutionary phenomena +continuously connected to the ``normal'' quasar population. + +\section{Discussion} +\label{sec:discussion} + +\subsection{General Implications of our Model} +\label{sec:genimpl} + +Our modeling suggests two important paradigm shifts in interpreting +quasar populations and evolution: + +{\bf (1)} First, as proposed in \citet{H05c}, a proper accounting of +the luminosity dependence of quasar lifetimes (as opposed to models in +which quasars grow in a pure exponential fashion or turn on and off as +``light bulbs'') implies a novel interpretation of the luminosity +function. The steep bright end (luminosities above the ``break'' in +the luminosity function) consists of quasars radiating near their +Eddington limits and is directly related to the distribution of +intrinsic peak luminosities (or final black hole masses) as has been +assumed previously. However, the shallow, faint end of the luminosity +function describes black holes either growing in early stages of +activity or in extended, quiescent states going into or coming out of +a peak bright quasar phase, with Eddington ratios generally between $l +\sim0.01$ and 1. The ``break'' luminosity in the luminosity function +corresponds directly to the {\em peak} in the birthrate of quasars +as a function of peak luminosity $\nLP$. + +This interpretation resolves inconsistencies in a number of previous +theoretical studies. For example, semi-analytical models of the quasar +luminosity functions \citep[e.g.,][]{KH00,HM00,WL03} assume, based on +simplified models for the quasar lifetime, that quasars at the faint +end of the luminosity function correspond to low final-mass black +holes (low $\Lp\sim L$), presumably in small halos. Consequently, +these models overpredict the number of active low-mass black holes (as +estimated from radio source counts), especially at high redshift, by +orders of magnitude \citep{HQB04}, and overpredict the number of +low-mass spheroids and red galaxies observed \citep{H05e}. + +Moreover, both observations \citep{MD04} and comparison of the +present-day black hole mass function with radio and X-ray luminosity +functions \citep[e.g.][]{Merloni04} suggest anti-hierarchical +evolution for the growth of supermassive black holes, where the most +massive black holes were produced mainly at high ($z\gtrsim2$) +redshift, and low-mass black holes mostly formed later, which does +not follow from idealized descriptions of quasar lifetimes and the +luminosity function (for a review, see e.g.\ Combes 2005). + +A one-to-one correspondence between observed luminosity and black hole +mass does produce anti-hierarchical behavior in some sense at the +high-mass end, because the most massive black holes are formed at +$z\sim2-3$ during the peak of bright quasar activity and the quasar +luminosity function evolves to lower luminosities at lower redshifts +(as is also the case for our model because the bright end of the +luminosity function is dominated by sources near their peak +luminosities). However, at black hole masses equal to or below +$\sim10^{8}\,M_{\sun}$ (i.e.\ galaxies of stellar mass +$\lesssim10^{11}\,M_{\sun}$), the evolution in the quasar luminosity +function implies a roughly constant production of black holes with +these masses at all redshifts, which is inconsistent with observations +of galaxy spheroids indicating that typical ages increase with mass, +ruling out a large population of low-mass spheroids with ages equal to +or older than those of high-mass spheroids +\citep[e.g.,][]{Treu01,vanDokkum01,Treu02, +vDS03,Gebhardt03,Rusin03,vandeVen03,Wuyts04,Treu05,Holden05,vdW05,SA05, +Nelan05}. As demonstrated in Figure~\ref{fig:SMBH.evol}, such a model +does not produce anti-hierarchical growth or any age gradients within +the high-mass spheroid population, also inconsistent with +observations. Even given observed ``luminosity-dependent density +evolution'' +\citep[e.g.][]{Page97,Miyaji00,Miyaji01,LaFranca02,Cowie03, +Ueda03,Fiore03,Hunt04,Cirasuolo05,HMS05}, implying that the densities +of lower redshift quasars peak at lower redshift, the inferred +anti-hierarchical evolution if observed luminosity directly +corresponds to black hole mass (i.e.\ as in ``light-bulb'' or ``fixed +Eddington ratio'' models) is not strong enough to account for observed +anti-hierarchical growth of the corresponding galaxy spheroids +\citep{H05e}. + +Furthermore, in these earlier models, a ``break'' in the luminosity +function is not necessarily reproduced \citep{WL03}, and the faint-end +slope has no direct physical motivation. The break may be caused by +feedback mechanisms which set a characteristic turnover in both the +galaxy mass function and quasar luminosity function (e.g., Scannapieco +\& Oh 2004; Dekel \& Birnboim 2004), as in our modeling. The $\nLp$ +distributions in our model and ``light bulb'' or ``fixed Eddington +ratio'' models are comparable at and above the break in the quasar +luminosity function, and therefore make similar predictions for some +observations at these luminosities. However, the {\em faint-end} +slope has a different physical motivation in our model. Unlike the +bright-end slope, which is determined directly by the active final +black hole mass function or peak luminosity distribution (in +essentially all models of the quasar lifetime), the faint-end slope in +our modeling is a consequence of the quasar lifetime as a function of +luminosity, and is a prediction of our simulations and modeling almost +independent of the underlying faint-end slope of the active black hole +mass function or peak luminosity distribution. In \citet{H05f} we +examine this in more detail, and demonstrate that it predicts well the +evolution in the faint-end quasar luminosity function slope with +redshift and the observed ``luminosity-dependent density evolution'' +in many samples \citep{Page97,Miyaji00,Miyaji01,LaFranca02,Cowie03, +Ueda03,Fiore03,Hunt04,Cirasuolo05,HMS05}. + +Other observational evidence for our picture exists; for example in +the observed distribution of Eddington ratios (see +\S~\ref{sec:eddington}), the distribution of low-redshift, active +black hole masses (see \S~\ref{sec:BLmasses}), and the turnover in the +expected distribution of black hole masses in early-type galaxies at +$\sim10^{8}\,M_{\sun}$ \citep[e.g.,][]{Sheth03}. Total (integrated) +quasar lifetimes estimated from observations are inferred to increase +with increasing black hole mass as we predict \citep{YT02}, and +furthermore, the Eddington ratios of observed quasar samples are seen +to increase systematically with redshift, as the sample becomes +increasingly dominated by luminosities above the break in the +luminosity function \citep{MD04}. + +Moreover, observations show that the evolution of the luminosity +function with decreasing redshift is driven by a decrease in the +characteristic mass scale of actively accreting black holes +\citep[e.g.,][]{Heckman04}, which can be explained in our model by the +relation of the observed luminosity function to the {\em peak} in the +distribution of active black hole masses $\nLp$. This observation, +however, has caused considerable confusion, as observations of both +radio-quiet \citep{WooUrry02} and radio-loud \citep{ODowd02} local +(low redshift) AGN indicate that nuclear and host luminosities are +uncorrelated, implying that nuclear luminosity does not depend on +black hole mass \citep{Heckman04}, and therefore that the primary +variable determining the nuclear luminosity is the Eddington ratio, +with the luminosity function spanning a broad range in Eddington +ratios \citep{Hao05}. Furthermore, observations show that this is +{\em not} true of high redshift quasars, as both direct estimates of +accretion rates \citep[e.g.,][]{Vestergaard04,MD04} and the fact that +their high luminosities would yield unreasonably large black hole +masses rule out substantially sub-Eddington accretion rates for most +objects. Many previous empirical and semi-analytical models could not +simultaneously account for these observations. To explain just the +low-redshift observations, such models adopt tunable distributions of +Eddington ratios fitted to the data. However, both these observations +are consequences of our interpretation of the luminosity function, as +observations of local AGN and the low-redshift luminosity function are +dominated by quasars below the break in the luminosity function, which +are undergoing sub-Eddington growth and span a wide range of Eddington +ratios, while observations at high redshift are dominated by bright +objects at or above the break in the luminosity function, which are +undergoing Eddington-limited (or near Eddington-limited) growth near +their peak luminosity (see \S~\ref{sec:eddington}). + +{\bf (2)} The second paradigm shift indicated by our modeling is that +quasar obscuration is not a static or quasi-static geometric effect, +but is primarily an {\em evolutionary} effect. The physical reasoning +for this is simple: the massive gas inflows required to fuel quasar +activity produce large obscuring columns, and so column densities are +correlated with quasar luminosity. The basic picture of buried quasar +activity associated with the early growth of supermassive black holes +and starburst activity has been proposed previously and studied for +some time \citep[e.g.,][]{SM96,Fabian99}, but our modeling allows us +to describe the evolution of obscuration in a self-consistent manner, +defining obscured and unobscured phases appropriately and identifying +dynamical correlations between the column density distribution and +instantaneous and peak luminosities. + +There is substantial observational support for this picture. Point-like X-ray +sources have been observed in many bright sub-millimeter or infrared +and starburst sources, with essentially all very luminous infrared +galaxies showing evidence of buried quasar activity +\citep[e.g.,][]{SM96,Komossa03,Ptak03}, indicating simultaneous buried +black hole growth and star formation at redshifts corresponding to +peak quasar activity ($z\gtrsim1$) \citep{Alexander05a,Alexander05b}. +The buried black holes in high-z starbursting galaxies appear to be +active but undermassive compared to the quiescent galaxy black +hole-stellar mass relation \citep{Borys05}, implying that they are +rapidly growing in the starburst but have not yet reached their final +masses, presumably set in the subsequent ``blowout'' phase. +Similarly, observations suggest that obscured AGN are significantly +more likely to exhibit strong sub-millimeter emission characteristic +of star formation, implying both that obscured black hole growth and +star formation are correlated and that obscuration mechanisms +(responsible for re-radiation in the submm and IR) may be primarily +isotropic in at least some cases \citep[e.g.,][]{Page04,Stevens05}. +Evidence from quasar emission line structure +\citep[e.g.,][]{Kuraszkiewicz00,Tran03}, directly related to the inner +broad-line region, suggests that isotropic obscuration of quasars can +be important, in contradiction to angle-dependent models. Finally, +many observations +\citep[e.g.,][]{Steffen03,Ueda03,Hasinger04,GRW04,sazrev04,Barger05,Simpson05} +indicate that the fraction of broad-line or obscured quasars is a +function of luminosity, which cannot be accounted for in traditional +static ``torus'' models \citep[e.g.,][]{Antonucci93} or reproduced +even by modified luminosity-dependent torus models \citep{Lawrence91}, +an observation that is explained by our model (see +\S~\ref{sec:BLqso} for a detailed discussion). + +Much of the obscuration in our modeling comes from large scales, +arising from the inner regions of the host galaxy on scales +$\sim50\,$pc or larger. While our resolution limits prevent our +ruling out the possibility of gas collapse to a dense, $\sim\,$pc +scale torus surrounding the black hole, during the peak obscured +phases of the final merger, our simulations indicate that these large +scales dominate the contribution to the column density, with quite +large columns, which should be observationally testable. Indeed, this +is suggested by the typical scales of obscuration in starbursting +systems (e.g.\ Soifer et al.\ 1984a,b; Sanders et al.\ 1986, 1988a,b; +for a review, see e.g.\ Soifer et al.\ 1987), given that, as discussed +above, the dominant obscured phase of growth is closely associated +with a starburst as implied observationally +\citep{Alexander05a,Alexander05b,Borys05}. + +Observations of polarized light in intrinsically bright Type II AGN +with unobscured luminosities typical of quasars (as opposed to local, +dim Seyfert II objects in relaxed hosts) show scattering on large +scales $\sim$kpc, and in some cases obscuration clearly generated over +scales extending beyond the host galaxy in the form of distortions, +tidal tails, and streams from interactions and major mergers +\citep{Zakamska04,Zakamska05}. The angular structure seen in these +observations is consistent with our modeling. Moreover, in optically +faint X-ray quasars \citep[e.g.][]{Donley05} it appears that +obscuration is generated by the host galaxies, and is directly related +to host galaxy morphologies and line-of-sight distance through the +host. The critical point is that, regardless of the angular structure +of obscuration, typical column densities are strongly evolving +functions of time, luminosity, and host system properties, and the +observed distribution of column densities is dominated by these +effects, not by differences in viewing angle across a uniform +population. This is the case in our modeling as the lognormal +dispersion (across different lines of sight) in column densities is +$\sigNH\sim0.4$ for a given simulation at some instant, whereas +typical column densities across simulations, as a function of +instantaneous and peak luminosities, span several orders of magnitude +from $\nh\sim10^{18}-10^{26}\ {\rm cm^{-2}}$. + +\subsection{Specific Predictions of our Model} +\label{sec:specpred} + +Our predictions include: + +\begin{itemize} + +\item Quasar Lifetimes: We find that for a particular source, the +quasar lifetime depends sensitively on luminosity, with the observed +lifetime in addition depending on the observed waveband. Intrinsic +quasar lifetimes vary from $t_{Q}\sim10^{6}-10^{8}$\,yrs, with +observable lifetimes $\sim10^{7}$\,yrs in optical B-band +\citep{H05a,H05b}, in good agreement with observational estimates +\citep[for a review, see][]{Martini04}. + +\item Luminosity Functions: Using a parameterization of the intrinsic +distribution of peak luminosities (final quasar black hole masses) at +a given redshift, our model of quasar lifetimes allows us to reproduce +the observed luminosity function at all luminosities and redshifts +$z=0-6$. Although this is an empirical determination of the peak +luminosity distribution, it implies a new interpretation of the +luminosity function \citep{H05c}, which provides a physical basis for +the observed ``break'' corresponding to the peak in the peak +luminosity distribution. Moreover, the faint end slope is not +determined by our empirical fitting procedure, but instead by the +dependence of the quasar lifetime on luminosity, with its value and +redshift evolution predicted by our modeling \citep{H05f}. The +evolution of typical column densities in different stages of merger +activity produces a significant population of obscured quasars, +accounting for the difference between hard X-ray \citep[e.g.,][]{Ueda03}, +soft X-ray \citep[e.g.,][]{Miyaji01}, and optical B-band +\citep[e.g.,][]{Croom04} luminosity functions (\S~\ref{sec:fullLF}). + +\item Column Density Distributions: The evolution of the column +densities in our simulations reproduces the observed distribution of +columns in optically-selected quasar samples, when the appropriate +selection criteria are applied \citep{H05b}, as well as complete +column distributions in hard X-ray selected samples +(\S~\ref{sec:NHdistrib}). Column density evolution over the course of +a merger yields a wider observed distribution of columns than that +produced across different viewing angles at a given point in a +merger. + +\item Broad Line Luminosity Function and Fraction: Using our +simulations to estimate when quasars will be observable as broad-line +objects (either based on the ratio of quasar to host galaxy optical +B-band luminosity or the obscuring column density), we reproduce the +luminosity function of broad-line quasars in hard X-ray selected +samples as well as optical broad-line quasar surveys, and the fraction +of broad-line quasars in a given sample as a function of luminosity, +to better precision than traditional or luminosity-dependent (but +non-dynamical) torus models which are fitted to the data +(\S~\ref{sec:BLfraction}). By providing an a priori prediction of the +broad-line fraction as a function of luminosity and redshift which +depends systematically on the typical quasar host galaxy gas fraction, +we propose that observations of the broad line fraction at different +redshifts can be used to constrain the gas fraction of quasar hosts +and its evolution with redshift. + +\item Active Black Hole Mass Functions: Using our prescription for +deciding when objects will be visible as ``broad-line'' quasars, we +predict the distribution of low-redshift, broad-line and non-broad +line active quasar masses, in good agreement with observations from +the SDSS, with expected incompleteness in the observed sample at low +$M_{\rm BH}\lesssim10^{6}\,M_{\sun}$ black hole masses +(\S~\ref{sec:BLmasses}). This is a new prediction which can be tested +in greater detail by future observations, and our calculations allow +us to model the differences in active black hole mass functions of the +Type I and Type II populations. The width of the expected broad-line +black hole mass function depends significantly on the model of quasar +lifetimes, enabling such measurements to probe the statistics of +quasar evolution. + +\item Eddington Ratios: We determine Eddington ratio distributions +from our simulations, given the peak luminosity distribution implied +by the observed quasar luminosity function. The predicted +distribution, once the appropriate observed magnitude limit is +imposed, agrees well with observations at both low ($z<0.5$) and high +($1.5\Lcut{11})\sim1-3\times10^{5}\ +{\rm Mpc^{-3}}$, in agreement with the $\sim5\times10^{5}\ {\rm +Mpc^{-3}}$ density of such sources expected to reproduce the observed +cumulative source density $4\times10^{4}\,{\rm deg^{-2}}$ of 1\,mJy +$850\,\mu{\rm m}$ SCUBA sources \citep{Barger99}. Furthermore, our +prediction of the fraction of buried AGN and its evolution with +redshift agrees well with determinations from X-ray samples +\citep{Barger05} and recent Spitzer results in the mid and +near-infrared at $z\sim2$ \citep{Martinez05}. + +\subsection{AGN not Triggered by Mergers} +\label{sec:nonmerger} + +Some low redshift quasars (e.g.\ Bahcall et al.\ 1996) and many +nearby, low-luminosity Seyferts appear to reside in ordinary, +relatively undisturbed galaxies. Our picture for quasar evolution +does not immediately account for these objects because we suppose that +nuclear activity is mainly triggered by tidal torques during a merger. + +This work is primarily concerned with the origin of the +majority of the mass in spheroids and supermassive black holes, and as +a consequence, the relation of this to the abundance and +evolution of quasars and the cosmic X-ray background. Based on our +present analysis, we believe that a merger-driven picture can account +for the main part of each of these, and, as described earlier, that the +most relevant phase in the history of the Universe to these phenomena +appears to have been at moderate redshifts, $z\sim2.5$ to $z\sim0.5$. + +Our model does not exclude other mechanisms for triggering AGN and it +is likely that a variety of stochastic or continuous processes are +relevant to nuclear activity in undisturbed disks and residual +low-level accretion in relaxed systems. This is not contrary to our +picture because most of the total black hole mass density in the +Universe is in spheroid-dominated systems. The principal requirement +of our model is that AGN activity in undisturbed galaxies should not +contribute a large fraction of the black hole mass density in the +Universe, to avoid spoiling tight correlations between the black hole +and host galaxy properties and producing too large a present-day black +hole mass density in violation of the Soltan (1982) constraint. + +For example, if a molecular cloud passed through the center of our Galaxy near Sgr +A$^{\ast}$, it is possible that the Milky Way would resemble a Seyfert +for some period of time. Alternatively, it has long been recognized +that mass loss from normal stellar evolution of bulge stars or stellar +clusters near the centers of galaxies can provide a continuous supply +of fuel for low-level accretion \citep[e.g.,][]{MLC81,MB81,Shull83}. +Typical galactic stellar mass loss rates +($\dot{M}\sim1\,M_{\sun}\,{\rm yr^{-1}}\,(10^{11}\,M_{\sun})^{-1}$) +yield Bondi-Hoyle accretion rates $\sim10^{-5}-10^{-4}$ of Eddington +in relaxed, dynamically hot systems; and mass loss rates from O and +W-R stars ($\dot{M}\sim10^{-6}\,M_{\sun}\,{\rm +yr^{-1}}\,(10\,M_{\sun})^{-1}$) in young, dense star clusters near the +centers of galaxies with sufficient cold gas for continued star +formation can yield rates as high as $\sim10^{-2}$ of Eddington. + +Even though these fueling mechanisms do not involve mergers, the scenario +we have discussed might still be relevant to the origin of these black holes. Of +course, the black holes and spheroids in disk-dominated systems may +have produced in a manner that did not involve mergers. +Alternatively, most of the black hole mass in these objects (which is +small compared to that in spheroid-dominated galaxies) could have been +assembled long ago in mergers with bright quasar phases and then these +``dead'' quasars are resurrected sporadically by other fueling +mechanisms. + +Independent of how these black holes were formed, elements of our +modeling may still account for certain observed properties of Seyferts. The +observed Seyfert luminosity function appears to join smoothly onto the +quasar luminosity function \citep{Hao05}. It is not obvious that this +would be the case if the two types of objects are produced by entirely +distinct mechanisms. In addressing this, it is useful to +separate the process by which gas is delivered to the black hole from +the subsequent evolution that determines the observed activity. In +our picture, gas is delivered to the black hole by gravitational +torques during a merger, but other mechanisms, like bar-induced +fueling may be important for objects such as Seyferts. Regardless, +the induced activity may be generic, if black hole growth is +self-regulated in the way we describe it in our simulations. + +In Hopkins et al. (2005f) we show that the faint end slope of the +quasar luminosity function in our model is partly determined by the +time dependence of the ``blowout'' phase of black hole growth. We +derive an analytical model for this using a Sedov-Taylor type analysis +and show that the impact of this feedback depends on the mass of the +host. This analysis does not depend on the fueling mechanism, only on +the subsequent evolution. If this self-regulated growth applies to +Seyferts as well (for example if Seyfert growth is regulated by a +balance between accretion feedback and the spheroid potential, as +expected if these objects obey a similar $M_{\rm BH}-\sigma$ +relation), we would expect the Seyfert luminosity function to smoothly +join onto the quasar one, even if the fuel is delivered in a different +manner. + +\section{Conclusions} +\label{sec:finis} + +We have studied the evolution of quasars in simulations of galaxy +mergers spanning a wide region of parameter space. In agreement with +earlier work \citep{H05a}, we find that the lifetime of a particular +source depends on luminosity and increases at lower luminosities, and +that quasar obscuration is time-dependent. Our new, large set of +simulations shows that the lifetime and obscuration can be expressed +in terms of the instantaneous and peak luminosities of a quasar and +that these descriptions are robust, with no systematic dependence on +simulation parameters. We have combined these results with a +semi-empirical method to describe the cosmological distribution of +quasar properties, allowing us to predict a large number of +observables as a function of e.g.\ luminosity and redshift. This +approach also makes it possible to compare our picture to simpler +models for quasar lifetimes and obscuration. + +In the model we examine, quasars are triggered by mergers of gas-rich +galaxies, which produce inflows of gas through gravitational torquing, +fueling starbursts and rapid black hole growth. The large gas +densities obscure the central black hole at optical wavelengths until +feedback energy from the growth of the black hole ejects gas and +rapidly slows further accretion (``blowout''). Quasar lifetimes and +light curves are non-trivial, with strong accretion activity during +first passage of the merging galaxies and extended quiescent +(sub-Eddington) phases leading into and out of the phase of peak +quasar activity associated with the final merger. The ``blowout'' +phase in which the quasar is visible as a bright, near-Eddington +optical source has a lifetime related to the dynamical time in the +inner regions of the merging galaxies, which characterizes the +timescale over which obscuring gas and dust are expelled, but the +quasar spends a longer time at lower luminosities before and after +this stage. These evolutionary processes have important consequences +which cannot be captured in models of pure exponential or ``on/off'' +quasar growth. + +Our work emphasizes several goals for quasar and galaxy observations +and theory. Observationally, it is important to constrain the faint +end of the {\em peak} luminosity distribution; i.e.\ the low-mass +active black hole distribution. Unfortunately, our modeling of quasar +lifetimes implies that the faint-end quasar luminosity function is +dominated by quasars with peak luminosities around the break in the +luminosity function, and can provide only weak constraints on the +faint-end $\Lp$ distribution. However, there is still hope, as for +example broad-line quasar activity is more closely associated with +near-peak luminosities, and thus probing the faint-end of broad-line +luminosity functions may in particular improve the estimates. +Moreover, studies of the black hole mass distribution (or the +distribution of galaxy spheroids) as a function of redshift, extending +to small spheroid masses/velocity dispersions probes the faint end of +$\nLp$. Other techniques, such as studies of faint radio sources at +high redshift \citep{HQB04} can similarly constrain these populations. +Furthermore, the calculations in this paper can be combined to better +determine $\nLp$, as, given a model for the quasar lifetime and +obscuration, they all derive from this fundamental quantity. +Additional observational tests of the modeling we have presented will +provide an important means of constraining models for AGN accretion +and feedback; for example, the faint-end slope of the quasar lifetime +depends on how the ``blowout'' phase occurs and could provide a +sensitive probe of feedback models, enabling the adoption of more +realistic and sophisticated feedback prescriptions than we have thus +far employed. Of course, improved constraints on the luminosity +function at all luminosities at high redshift remains a valuable means +of testing theories of quasar evolution. + +Our simulations are based on isolated galaxy mergers, and thus do not +provide a cosmological prediction for the distribution of peak +luminosities $\nLp$, merger rates, or mass functions - we instead have +adopted a semi-empirical model, in which we use our modeling of quasar +evolution to determine these distributions from the observed +luminosity function. While this allows us to predict a large number +of observables and to demonstrate that a wide range of quasar and +galaxy properties are self-consistent in a model of merger-driven +quasar activity with realistic quasar lifetimes, future theoretical +work in these areas should predict the distribution of peak +luminosities $\nLp$ and its evolution with redshift. These quantities +are to be distinguished from the distribution of observed +luminosities, as the two are not trivially related in our model or any +other with a non-trivial quasar lifetime. + +Although the quasar birthrate as a function of peak luminosity will +be, in general, a complicated function of galaxy merger rates, gas +fractions, morphologies, and other factors, we have parameterized it +for comparison with the results of future cosmological simulations and +semi-analytical models. This distribution is particularly valuable as +a theoretical quantity because it is more directly related to physical +galaxy properties than even the complete (intrinsic) luminosity +function, and additionally because theoretical modeling which +successfully reproduces this $\nLp$ distribution is guaranteed to +reproduce the large number of observable quantities we have discussed +in detail in this work. We cannot determine the cosmological context +in our detailed simulations of the relatively small-scale physics of +galaxy mergers, and conversely, cosmological simulations and +semi-analytical models cannot resolve the detailed physics driving +quasar activity in mergers. However, our determination of quasar +evolution as a function of peak luminosity or final black hole mass +can be grafted onto these cosmological models to greatly increase the +effective dynamic range of such calculations. Combined with our +modeling, this would remove the one significant empirical element we +have adopted, and allow for a complete prediction of the above +quantities from a single theoretical framework. + +In these efforts, we emphasize that the mergers relevant to our +picture are of a specific type. First, the merging galaxies must +contain a supply of cold gas in a rotationally supported disk. Hot, +diffuse gas, as in the halos of elliptical galaxies, will not be +subject to the gravitational torques which drive gas into galaxy +centers and fuel black hole growth. Clearly, gas-poor mergers are also +not important for this process. Second, the mergers will likely +involve galaxies of comparable, although not necessarily equal, mass, +so that the gravitational torques excited are strong enough and +penetrate deep enough into galaxy centers to drive substantial inflows +of gas. The precise requirement for the mass ratio is somewhat +ill-defined because it also depends on the orbit geometry, but mergers +with a mass ratio larger than $10 : 1$ are probably not generally +important to our model. Simulations of minor mergers involving +galaxies with mass ratios $\lesssim 10:1$ (e.g.\ Hernquist 1989; Hernquist +\& Mihos 1995) have shown that for particular orbital geometries, +these events can produce starbursts similar to those in major mergers, +leaving behind disturbed remnants with dynamically heated disks (e.g.\ +Quinn et al.\ 1993; Mihos et al.\ 1995; Walker et al.\ 1996). It is +of interest to establish whether black hole growth can also be +triggered in minor mergers, as these events may be relevant to weak +AGN activity like that in some Seyfert galaxies or LINERs. + +In summary, the work presented here supports the conjecture that many +aspects of galaxy formation and evolution can be understood in terms +of the ``cosmic cycle'' in Figure~\ref{fig:cosmiccycle}. To be sure, +much of what is summarized in Figure~\ref{fig:cosmiccycle} has been +proposed elsewhere, either in the context of observations or +theoretical models. Our modeling of galaxy formation and evolution +emphasizes the possibility that supermassive black holes could be {\it +responsible} for much of what goes on in shaping galaxies, rather than +being bystanders, closing the loop in Figure~\ref{fig:cosmiccycle}. +In this sense, black holes may be the ``prime movers'' driving galaxy +evolution, as has been proposed earlier for extragalactic radio +sources (e.g.\ Begelman, Blandford \& Rees 1984; Rees 1984). It may +seem counterintuitive that compact objects with masses much smaller +than those of galaxies could have such an impact, but it is precisely +the concentrated nature of matter in black holes that makes this idea +plausible. + +Consider a black hole of mass $M_{\rm BH}$ at the center of a +spherical galaxy of mass $M_{\rm sph}$ with a characteristic velocity +dispersion $\sigma$. The energy available to affect the galaxy +through the growth of the black hole will be some small fraction of +its rest-mass, $E_{\rm feed} \sim \epsilon_f M_{\rm BH} c^2$. This +can be compared with the binding energy of the galaxy, $E_{\rm bind} +\sim M_{\rm sph} \sigma^2$. Observations indicate that $M_{\rm BH}$ +and $M_{\rm sph}$ are correlated and that, roughly $M_{\rm BH} \sim +(0.002 - 0.005) M_{\rm sph}$ (Magorrian et al.\ 1998; Marconi \& Hunt +2003). Therefore, the ratio of the feedback energy to the binding +energy of the galaxy is $E_{\rm feed} / E_{\rm sph} > 10 +\epsilon_{f,-2} \, \sigma_{300}^{-2}$, for an assumed efficiency of +1\%, $\epsilon_{f,-2} \equiv \epsilon /0.01$ and scaling the velocity +dispersion to $\sigma_{300} \equiv \sigma / 300$ km/sec, as for +relatively massive galaxies. This result demonstrates that the +supermassive black holes in the centers of spheroidal galaxies are by +far the largest supply of potential energy in these objects, exceeding +even the galaxy binding energy. When viewed in this way, if even a +small fraction of the black hole radiant energy can couple to the +surrounding ISM, then black hole growth is not an implausible +mechanism for regulating galaxy formation and evolution; in fact, it +appears almost inevitable that it should play this role. + +\acknowledgments We thank our referee, David Weinberg, for many +comments and suggestions that greatly improved this paper. We +thank Paul Martini, for +helpful discussion, and Gordon Richards and Alessandro Marconi, for +generously providing data for observational comparisons. This work +was supported in part by NSF grants ACI 96-19019, AST 00-71019, AST +02-06299, and AST 03-07690, and NASA ATP grants NAG5-12140, +NAG5-13292, and NAG5-13381. 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L. 1995, \apj, 453, L57 +\bibitem[Zitelli \etal(1992)]{Zitelli92} +Zitelli, V., Mignoli, M., Zamorani, G., Marano, B., \&\ Boyle, B.~J.\ 1992, \mnras, 256, 349 +\end{thebibliography} + +\clearpage +%\begin{deluxetable}{llllllllllll} +\begin{deluxetable}{cccccccccccc} +\tabletypesize{\scriptsize} +\tablecaption{Mock Quasar Distribution Examples \label{tbl:montecarlo}} +\tablewidth{0pt} +\tablehead{ +\colhead{\tablenotemark{1}$\Lp$} & +\colhead{\tablenotemark{2}$M_{\rm BH}^{f}$} & +\colhead{\tablenotemark{3}$L$} & +\colhead{\tablenotemark{4}$M_{\rm BH}$} & +\colhead{\tablenotemark{5}$\nh$} & +\colhead{\tablenotemark{6}$\nhi$} & +\colhead{\tablenotemark{7}$L_{B}^{\rm i}$} & +\colhead{\tablenotemark{8}$L_{SX}^{\rm i}$} & +\colhead{\tablenotemark{9}$L_{HX}^{\rm i}$} & +\colhead{\tablenotemark{10}$L_{B}^{\rm obs}$} & +\colhead{\tablenotemark{11}$L_{SX}^{\rm obs}$} & +\colhead{\tablenotemark{12}$L_{HX}^{\rm obs}$} +} +\startdata +10.6 & 6.1 & 8.5 & 6.1 & 20.5 & 20.1 & 7.2\ \ 7.5 & 7.4\ \ 6.8 & 7.6\ \ 7.0 & 7.2\ \ 7.4 & 7.4\ \ 6.8 & 7.6\ \ 7.0 \\ +10.4 & 6.4 & 8.7 & 6.0 & 22.2 & 22.0 & 7.4\ \ 7.6 & 7.6\ \ 7.0 & 7.8\ \ 7.2 & 5.8\ \ 6.0 & 7.5\ \ 6.9 & 7.8\ \ 7.2 \\ +... & & & & & & & & & & & +\enddata +\tablenotetext{1}{Peak quasar bolometric luminosity, $\log_{10}(\Lp/L_{\sun})$} +\tablenotetext{2}{Final (post-merger) black hole mass, $\log_{10}(M_{\rm BH}^{f}/M_{\sun})$} +\tablenotetext{3}{Current (at time of ``observation'') intrinsic (no attenuation) +bolometric luminosity, $\log_{10}(L/L_{\sun})$} +\tablenotetext{4}{Current black hole mass, $\log_{10}(M_{\rm BH}/M_{\sun})$} +\tablenotetext{5}{Total (neutral+ionized) hydrogen +column density along the ``observed'' sightline, $\log_{10}(N_{\rm H}/{\rm cm}^{-2})$} +\tablenotetext{6}{Neutral hydrogen +column density along the ``observed'' sightline, $\log_{10}(N_{\rm H\, I}/{\rm cm}^{-2})$} +\tablenotetext{7}{Intrinsic (no attenuation) B-band luminosity, $\log_{10}(L_{B}^{\rm i}/L_{\sun})$, +where $L_{B}=\nu_{B}L_{\nu_{B}}$ at $\nu_{B}=4400$\AA.} +\tablenotetext{ \ }{Calculated with the luminosity-dependent +bolometric corrections from (Marconi et al.\ 2004; left), } +\tablenotetext{ \ }{and constant (luminosity-independent) $L=11.8\,L_{B}$ (Elvis et al.\ 1994; right).} +\tablenotetext{8}{Intrinsic soft X-ray (0.5-2 keV) luminosity, $\log_{10}(L_{SX}^{\rm i}/L_{\sun})$.} +\tablenotetext{ \ }{Calculated with the luminosity-dependent +bolometric corrections from (Marconi et al.\ 2004; left), } +\tablenotetext{ \ }{and constant (luminosity-independent) $L=52.5\,L_{SX}$ (Elvis et al.\ 1994; right).} +\tablenotetext{9}{Intrinsic hard X-ray (2-10 keV) luminosity, $\log_{10}(L_{HX}^{\rm i}/L_{\sun})$.} +\tablenotetext{ \ }{Calculated with the luminosity-dependent +bolometric corrections from (Marconi et al.\ 2004; left), } +\tablenotetext{ \ }{and constant (luminosity-independent) $L=35.0\,L_{HX}$ (Elvis et al.\ 1994; right).} +\tablenotetext{10}{``Observed'' (with attenuation) B-band luminosity, $\log_{10}(L_{B}^{\rm obs}/L_{\sun})$.} +\tablenotetext{ \ }{Left and right use luminosity-dependent and luminosity-independent bolometric corrections, respectively, as $L_{B}^{\rm i}$.} +\tablenotetext{11}{``Observed'' soft X-ray luminosity, $\log_{10}(L_{SX}^{\rm obs}/L_{\sun})$.} +\tablenotetext{ \ }{Left and right use luminosity-dependent and luminosity-independent bolometric corrections, respectively, as $L_{SX}^{\rm i}$.} +\tablenotetext{12}{``Observed'' hard X-ray luminosity, $\log_{10}(L_{HX}^{\rm obs}/L_{\sun})$.} +\tablenotetext{ \ }{Left and right use luminosity-dependent and luminosity-independent bolometric corrections, respectively, as $L_{HX}^{\rm i}$.} +\tablenotetext{ \ }{ \ } +\tablenotetext{ \ }{The complete tables +can be downloaded at \url{ftp://cfa-ftp.harvard.edu/pub/phopkins/qso\_catalogs/}} +\end{deluxetable} + +\end{document} + + diff --git a/feedback/papers/1701.07030.pdf b/feedback/papers/1701.07030.pdf new file mode 100644 index 0000000..50414f6 Binary files /dev/null and b/feedback/papers/1701.07030.pdf differ diff --git a/feedback/papers/1703.06889.pdf b/feedback/papers/1703.06889.pdf new file mode 100644 index 0000000..b8fce73 Binary files /dev/null and b/feedback/papers/1703.06889.pdf differ diff --git a/feedback/report/report.tex b/feedback/report/report.tex index 37e8459..29c3fc3 100644 --- a/feedback/report/report.tex +++ b/feedback/report/report.tex @@ -1,9 +1,5 @@ - - - \documentclass[11pt,letterpaper]{article} -%\usepackage{aas_macros} \usepackage{biblatex} \usepackage{graphicx} \usepackage[margin=1.in,centering]{geometry} @@ -22,38 +18,88 @@ \newcommand{\LCDM}{$\Lambda$CDM} +\newcommand{\apj}{ApJ} +\newcommand{\apjs}{ApJS} +\newcommand{\nat}{Nature} + +\newcommand{\Mo}{M$_\odot$} +\newcommand{\Lo}{L$_\odot$} - - -\title{Active Galactic Nuclei in Cosmology} +\title{Modeling Active Galactic Nuclei Feedback} \author{Otho Ulrich} \maketitle \begin{abstract} - Active Galactic Nuclei (AGN) play a role in cosmology as both component and probe. - They are used to contrain cosmological parameters, to characterize the intergalactic medium, and as a . - AGN interact with their host galaxies, influencing its evolution through a process called AGN feedback. - Modeling AGN feedback presents significant challenges, but has improved upon the \LCDM model as tested by the Millenium Simulation. \cite{2005Natur.435..629S} + Active Galactic Nuclei (AGN) are believed to be intricately involved with the evolution of their host galaxies through a process called AGN feedback. + The mechanisms by which this occurs are not well-understood. + It has been known for some time that the population of high-luminosity AGN, associated with large supermassive black holes, peaked during the early universe, and are extinct in the modern universe. + AGN activity in the universe peaked around the same time as galactic star formation, and while this correlation is not completely understood, astronomers consider it a strong possibility that AGN play an important role in the regulation of star formation rates. + AGN feedback may be responsible for quenching cold stellar winds, reducing star formation rates. + Chaotic cold accretion is shown to be a likely mechanism by which AGN feedback occurs, allowing the AGN to ``cycle'' through a process of heating and cooling that is ultimately able to find equilibrium with the host galaxy, until available cold gasses are consumed. + Modeling AGN feedback presents significant challenges, but has improved upon observational predictions derived from the \LCDM\ cosmology-based Millenium Simulation. + Only a few subclasses of AGN have been studied regarding their feedback mechanisms, and with only the most rudimentary first-principle approaches, but the necessity of including AGN feedback to correctly predict colors and luminosities of galaxy mergers and quasars seems increasingly likely. + Refining modeling methods will be useful once observational resolution is increased by future telescope missions. + + + \cite{2005Natur.435..629S} + + \cite{springelfeedback} \end{abstract} %───────────── -\section{Introduction} - \label{sec:intro} +\section{Active Galactic Nuclei} + \label{sec:AGN} + Quasars are the most luminous objects in the cosmos ($10^{12}-10^{15}$ \Lo. + In 1964, Zel’dovich and Novikov described for the first time the luminosity of a quasar emerging from the accretion of matter by a supermassive black hole (SMBH). + \cite{koristafeedback} + We now know that SMBHs on the order of $10^6$ - $10^9$ \Mo\ are common at the center of galaxies, and when their accretion process results in strong luminosities across the electromagnetic spectrum, we call these Active Galactic Nuclei (AGN). + Gas is readily available in the central region, shed by stars during their evolution, and from tidal disruptions caused by the SMBH. + The Eddington luminosity $L_E$ describes the luminosity necessary to induce radiation-driven outward matter flows, and for pure ionized hydrogen, + \begin{equation} + \centering + L_E=\frac{4\pi cGMm_p}{\sigma_T}\approx1.3\times10^{38}\textrm{ergs s}^{-1}\frac{M}{M_\odot}. + \end{equation} + Quasars are AGN radiating near or above their Eddington luminosities, making this an important measure of their brightness, and at $>10^{45}\textrm{ergs s}^{-1}$ they can outshine their entire host galaxy! + For a $10^9$ \Mo black hole to maintain its Eddington luminosity, it must accrete $40$~\Mo per year. + Central black holes in present-day galaxies apparently accrete at medium-to-low rates compared to rates needed to produce $L_E$, and observational studies show that quasars were much more common in the past, with their activity having peaked about 10 Gyr ago. + \cite{maoz2007astrophysics} + %───────────── -\section{Cosmology} - \label{sec:cosmology} +\section{Galactic Evolution} + \label{sec:galevol} + + \subsection{Millenium Simulation} - The Millenium Run and its following iterations are N-body simulations that predict the evolution of the matter in the universe. It is considered a (successful) test of the \LCDM cosmology. + \label{subsec:millsim} + The Millenium Run and its following iterations are N-body simulations that predict the evolution of the matter in the universe. It is considered a (successful) test of the \LCDM cosmology. + + The Millenium Simulation is used as a basis for simulations of other + + \subsection{Rise of Quasars} + %───────────── \section{Quasar Feedback Simulations} \label{sec:feedbacksims} + \begin{figure} + \centering + \includegraphics[width=.7\textwidth]{feedbackcycle.pdf} + \caption{ + Schematic of the ``cosmic cycle'' that plays out between galaxy formation and evolution regulated by black hole growth in galaxy mergers. + Galaxies in the modern universe typically contain dead quasars. + Mergers and other sources of inward gas flows are believed to trigger black hole growth and strong luminosities, which lead to AGN feedback and the possible continuation of the cycle at each iteration. + \cite{2006ApJS..163....1H} + } + \label{fig:feedbackcycle} + \end{figure} + + One of the It is strongly believed by cosmologists that %─────────────