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updated to share with kirk
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159
notes
159
notes
@ -1,159 +0,0 @@
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immediate things
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─────────────
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trim labels in fort file header, do any other header things
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look at paper from kirk's student and find the value of that parameter
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copy grids from thor
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this shows only the transition between 1s and 2p... where are the rest of the contributions?
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if indeed cloudy is meaning to print these out individually?
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this may not be true for hydrogen-like iron, but for H-alpha the three transitions should be included
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is this just sloppy notation in output file, or is this really accurate and then where is all the rest of it?
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save species line "species_lines" all
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save species labels "species_labels" all
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OR
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save species labels "species_labels"
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H[:]
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end
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For SED
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─────────────
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At low end transition to slope of 2
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at high end cutoff to slope -2.5
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check out Kirk's slope explanation for better approximations
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2017 grids needed
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mehdipour SED, solar, 10²² - 10²⁴
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magdziarz SED, solar, 10²² - 10²⁴
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magdziarz SED, metals 0.5 & element scale factor carbon 2, 10²² - 10²⁴
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By end of March: two grids run, continuum points decided upon, models decided upon
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Run grid with new SED, or at least a point, check values: how to find the appropriate values to change our list accordingly, and what might need to be change?
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✓ faint to equivalent width of 0.001 angstrom
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✓ compare between c13 and c17 -- show diferences in emergent line lists
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✓ new print lines to help reduce number of printed lines -- and to show old lines?
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✓ run models for comparising: 10.5,19.5
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✓ Why so many Fe 2 lines?
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✓ check if blnds are sums of the expected multiplets
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✓ add in more levels to the H atom, unresolved, 20, also add some to paschen, maybe others -- check how much time is lost
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✓ punch the paschen and balmer lines up to 18
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✓ Read Intrinsic Lines
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□ Smoothing algorithm using n-dimensional smoothing
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□ Contour plots
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✓ Run Grids in c17
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✓ Email about order of lines
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✓ Find blend correlated names and update
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check on ratios of inwd lines for blends
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check hazy for RRC H 1 meaning
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c 3 1175->538, seen twice? -- looked again, I don't see that now
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2 TOTL lines -> He 1
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for c13 if thor open:
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magziarz, 10^23, use 2000 korista and goad abundances apj, also default abundance
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use notes from paper to design contour plots
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what is the right way to model the components? check mehdipour and magdziarz paper, and comptonization paper
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other codes
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─────────────
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mappings, ion, X-STAR
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include lines:
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8205A
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hapsed lines
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BAC 3646 ✓
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BAC 0 ✓
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Pac 0 ✓
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lines not found:
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TOTL 1.08299m
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He 1 1.08291m # 1S1 to 3P0 <
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He 1 1.08303m # 1S1 to 3P1 <
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He 1 1.08303m # 1S1 to 3P2
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He 1 3888.63A
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Ca2K 3934.00A
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Ca2H 3969.00A
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Ca2X 8498.00A
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Ca2Y 8542.00A
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Ca2Z 8662.00A
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Fe 2 1500.00A
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Fe 2 1.15000m
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Fe 2 2500.00A
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Fe 2 2300.00A
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Fe 2 8900.00A
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Fe 2 1786.00A
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Fe 3 1125.79A
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Missing blend for Ne 5 ~1142A
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No good matches for these, included closest ones
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Si 2 1813.99A
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Si 2 1531.00A
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Si 2 1307.66A
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Si 2 1263.32A
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Si 3 1207.00A
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@ -1,9 +0,0 @@
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By end of March: two grids run, continuum points decided upon, models decided upon
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Run grid with new SED, or at least a point, check values: how to find the appropriate values to change our list accordingly, and what might need to be change?
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use notes from paper to design contour plots
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what is the right way to model the components? check mehdipour and magdziarz paper, and comptonization paper
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more?
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|
||||
s0 errorbar pattern 1
|
||||
s0 errorbar size 1.000000
|
||||
s0 errorbar linewidth 1.0
|
||||
s0 errorbar linestyle 1
|
||||
s0 errorbar riser linewidth 1.0
|
||||
s0 errorbar riser linestyle 1
|
||||
s0 errorbar riser clip off
|
||||
s0 errorbar riser clip length 0.100000
|
||||
s0 comment "mehdipour_magdziarz_compare.tab"
|
||||
s0 legend "Mehdipour"
|
||||
s1 hidden false
|
||||
s1 type xy
|
||||
s1 symbol 0
|
||||
s1 symbol size 1.000000
|
||||
s1 symbol color 2
|
||||
s1 symbol pattern 1
|
||||
s1 symbol fill color 2
|
||||
s1 symbol fill pattern 0
|
||||
s1 symbol linewidth 1.0
|
||||
s1 symbol linestyle 1
|
||||
s1 symbol char 65
|
||||
s1 symbol char font 0
|
||||
s1 symbol skip 0
|
||||
s1 line type 1
|
||||
s1 line linestyle 1
|
||||
s1 line linewidth 1.0
|
||||
s1 line color 2
|
||||
s1 line pattern 1
|
||||
s1 baseline type 0
|
||||
s1 baseline off
|
||||
s1 dropline off
|
||||
s1 fill type 0
|
||||
s1 fill rule 0
|
||||
s1 fill color 1
|
||||
s1 fill pattern 1
|
||||
s1 avalue off
|
||||
s1 avalue type 2
|
||||
s1 avalue char size 1.000000
|
||||
s1 avalue font 0
|
||||
s1 avalue color 1
|
||||
s1 avalue rot 0
|
||||
s1 avalue format general
|
||||
s1 avalue prec 3
|
||||
s1 avalue prepend ""
|
||||
s1 avalue append ""
|
||||
s1 avalue offset 0.000000 , 0.000000
|
||||
s1 errorbar on
|
||||
s1 errorbar place both
|
||||
s1 errorbar color 2
|
||||
s1 errorbar pattern 1
|
||||
s1 errorbar size 1.000000
|
||||
s1 errorbar linewidth 1.0
|
||||
s1 errorbar linestyle 1
|
||||
s1 errorbar riser linewidth 1.0
|
||||
s1 errorbar riser linestyle 1
|
||||
s1 errorbar riser clip off
|
||||
s1 errorbar riser clip length 0.100000
|
||||
s1 comment "mehdipour_magdziarz_compare.tab"
|
||||
s1 legend "Magdziarz"
|
Binary file not shown.
@ -1 +0,0 @@
|
||||
linelist
|
@ -1,37 +0,0 @@
|
||||
O III] 1661 and 1666 with
|
||||
TOTL 1665.
|
||||
|
||||
NIII] (about 1750)
|
||||
|
||||
S IV]
|
||||
|
||||
O IV] quintuplets (both near 1400A).
|
||||
|
||||
|
||||
S 5,
|
||||
TOTL 2798 (Mg 2)
|
||||
TOTL 1860 (Al 3)
|
||||
TOTL 2798 (Mg 2)
|
||||
TOTL 1860 (Al 3)
|
||||
TOTL 1397 (Si IV)
|
||||
|
||||
|
||||
TOTL 1240 (N 5) adds up properly.
|
||||
TOTL 1035 (O 6) does as well.
|
||||
|
||||
Yes for TOTL 1549
|
||||
No for TOTL 1397 (Si IV)
|
||||
|
||||
|
||||
Si IV
|
||||
|
||||
|
||||
TOTL 1549 = C 4 1548 + C 4 1551?
|
||||
Si IV 1394, 1403 and TOTL 1397
|
||||
|
||||
|
||||
|
||||
|
||||
|
||||
|
||||
|
@ -1,291 +0,0 @@
|
||||
# version of 2003 oct 27, cleaned up some lines whose wl had changed
|
||||
#
|
||||
# for information on the format of this file, see readme_LineList_dat.txt
|
||||
# this is the standard list list, appropriate for dense gas like the BLR,
|
||||
# which will use used if no name appears
|
||||
#
|
||||
# Begin CLOUDY grid output line list...
|
||||
# 2 X-ray lines:
|
||||
FeKa 2 Iron K-alpha line (near 6.4 keV)
|
||||
o 8 18.97 O VIII 19A H-like Lya
|
||||
#
|
||||
# UV lines: lambda > 600 Angstroms
|
||||
mg10 609.8A total Mg X 610
|
||||
#inwd 609.8A inward flux of Mg X 610
|
||||
mg10 624.9A total Mg X 625
|
||||
#inwd 624.9A inward flux of Mg X 625
|
||||
totl 615 total of sum of both Mg X components
|
||||
o 5 629.7A total O V 630
|
||||
s 4 655.1A total S IV 655; level 2 line
|
||||
n 3 678.2A total N III 679; level 2 line
|
||||
o 3 698.2 total O III 703; level 2 line
|
||||
s 4 737.3 total S IV 737; level 2 line
|
||||
n 3 752.1 total N III 764; level 2 line
|
||||
n 4 765.1 total N IV 765
|
||||
ne 8 770.4 total Ne VIII 770
|
||||
ne 8 780.3 total Ne VIII 780
|
||||
totl 774 total of sum of both Ne VIII component
|
||||
#inwd 774 inward flux of sum of both Ne VIII components
|
||||
s 5 786.5 total S V 786
|
||||
o 4 789.4 total O IV 789
|
||||
#inwd 789.4 inward flux of O IV 789
|
||||
s 4 798.8 total S IV 799
|
||||
O 2 833.8 total O II 834A
|
||||
o 3 834.5 total O III 834
|
||||
totl 895 total Ne VII] 895
|
||||
s 6 933.4 total S VI 933
|
||||
s 6 944.5 total S VI 944
|
||||
totl 933 total of sum of both S VI components
|
||||
p 4 950.7 total P IV 951; level 2 line
|
||||
h 1 972.5 total Lyman-gamma 973
|
||||
#inwd 972.5 inward flux of Lyman-gamma 973
|
||||
c 3 977 total C III 977
|
||||
#inwd 977 inward flux of C III 977
|
||||
n 3 991 total N III 990
|
||||
#inwd 991 inward flux of N III 990
|
||||
h 1 1026 total Lyman-beta 1025
|
||||
#inwd 1025 inward flux of Lyman-beta 1025
|
||||
o 6 1032 total O VI 1032
|
||||
o 6 1038 total O VI 1037
|
||||
totl 1035 total of sum of both O VI components
|
||||
#inwd 1035 inward flux of sum of both O VI components
|
||||
he 2 1085 total He II Balmer-gamma 1085
|
||||
n 2 1085 total N II 1085
|
||||
s 4 1086 total S IV 1086; level 2 line
|
||||
p 5 1121 total P V 1121; level 2 line
|
||||
fe 3 1126 total Fe III 1122
|
||||
ne 5 1141 total Ne V 1141
|
||||
c 3 1176 total C III* 1176 (excited state)
|
||||
#inwd 1176 inward flux of C III* 1176
|
||||
s 3 1198 total S III 1198
|
||||
totl 1198 total S V 1198
|
||||
si 3 1207 total Si III 1207
|
||||
inci 1215 incident continuum at 1215 Angstroms in units of nuF(nu)
|
||||
totl 1216 total Hydrogen Lyman-alpha 1215.67
|
||||
inwd 1216 inward flux of Lyman-alpha
|
||||
he 2 1215 total He II Balmer-beta 1216
|
||||
#inwd 1215 inward flux of He II Balmer-beta 1216
|
||||
totl 1218 total of sum of O V] 1218 + [O V] 1218
|
||||
#inwd 1218 inward flux of O V]
|
||||
n 5 1239 total N V 1238.82
|
||||
n 5 1243 total N V 1242.80
|
||||
totl 1240 total of sum of both N V components
|
||||
#inwd 1240 inward flux of sum of both N V components
|
||||
s 2 1256 total S II 1256
|
||||
si 2 1263 total Si II 1260 + 1263
|
||||
6lev 1304 total O I 1302 + 1305
|
||||
si 2 1308 total Si II 1308
|
||||
c 2 1335 total C II 1335 + 1336
|
||||
si 4 1394 total Si IV 1394
|
||||
si 4 1403 total Si IV 1403
|
||||
totl 1397 total of sum of both Si IV components
|
||||
#inwd 1397 inward flux of sum of both Si IV components
|
||||
totl 1402 total O IV] 1402; 5 components to line:
|
||||
#
|
||||
# 1397.2, 1399.77, 1401.16, 1404.81, 1407.39 --- not computed individually
|
||||
#inwd 1402 inward flux of O IV]
|
||||
totl 1406 total S IV 1406
|
||||
totl 1486 total of sum of N IV] 1486 + [N IV]
|
||||
N 4 1485 most forbidden of the pair
|
||||
#N 4 1486 stonger of the pair, at high density this will be the same as total
|
||||
#inwd 1488 inward flux of N IV]
|
||||
si 2 1531 total Si II 1527 + 1533
|
||||
c 4 1548 total C IV 1548.19
|
||||
c 4 1551 total C IV 1550.77
|
||||
totl 1549 total of sum of both C IV components
|
||||
inwd 1549 inward flux of sum of both C IV components
|
||||
he 2 1640 total He II Balmer-alpha 1640
|
||||
inwd 1640 inward flux of He II Balmer-alpha 1640
|
||||
o 3 1661 total O III] 1661
|
||||
#inwd 1661 inward flux of O III] 1661
|
||||
o 3 1666 total O III] 1666
|
||||
#inwd 1666 inward flux of O III] 1666
|
||||
totl 1665 total of sum of both O III] components
|
||||
al 2 1671 total Al II 1670.8; level 2 line
|
||||
s 3 1720 total S III 1720
|
||||
totl 1750 total N III] 1750 (all components; not computed seperately)
|
||||
#inwd 1750 inward flux of N III]
|
||||
fe 2 1786 total Fe II 1787 (probably selectively excited)
|
||||
si 2 1814 total Si II 1814 (1808.0 + 1816.9 + 1817.5)
|
||||
al 3 1855 total Al III 1855
|
||||
al 3 1863 total Al III 1863
|
||||
totl 1860 total sum of both Al III components
|
||||
#inwd 1860 inward flux of sum of both Al III components
|
||||
totl 1888 total of sum of Si III] 1892 + [Si III]
|
||||
Si 3 1883 the most forbidden of the doublet
|
||||
#inwd 1892 inward flux of Si III] 1892
|
||||
totl 1909 total of sum of C III] 1908.73 + [C III]
|
||||
#inwd 1910 inward flux of C III] 1908.73
|
||||
n 2 2141 total sum of N II] 2139.01, 2142.77
|
||||
o 3 2321 single line from 5-level atom
|
||||
totl 2326 total C II] 2324.69 + 2328.12
|
||||
totl 2335 total Si II] 2335
|
||||
totl 2665 total of sum of Al II] 2669 + [Al II] 2660
|
||||
al 2 2660 emission from most forbidden line of multiplet
|
||||
mg 2 2796 total Mg II 2796 of the doublet
|
||||
mg 2 2803 total Mg II 2803 of the doublet
|
||||
totl 2798 total of sum of both Mg II components
|
||||
inwd 2798 inward flux of sum of both Mg II components
|
||||
#
|
||||
# optical emission lines and continua
|
||||
he 2 3203 total He II Paschen-beta line
|
||||
BA C 0 total of integrated H balmer continuum
|
||||
BaC 3646 total nuFnu of Balmer jump at 3646 (the head)
|
||||
#h 1 3835 total H-7 (H-Balmer)
|
||||
He 1 3889 total H-6 (H-Balmer)
|
||||
ca2k 3934 total Ca II 3934 emission
|
||||
ca2h 3969 total Ca II 3969 emission
|
||||
#h 1 3970 total H-epsilon
|
||||
h 1 4102 total H-delta
|
||||
#inwd 4102 inward flux of H-delta
|
||||
h 1 4340 total H-gamma
|
||||
#inwd 4340 inward flux of H-gamma
|
||||
ca b 4471 total He I 4471, case B approximation
|
||||
he 2 4686 total He II 4686 (Paschen-alpha)
|
||||
inwd 4686 inward flux of He II 4686
|
||||
totl 4861 total H-beta 4861
|
||||
inwd 4861 inward flux of H-beta 4861
|
||||
He 1 5876 total He I 5876
|
||||
#inwd 5876 inward flux of He I 5876
|
||||
na 1 5892 total Na ID 5892
|
||||
h 1 6563 total H-alpha 6563
|
||||
#inwd 6563 inward flux of H-alpha 6563
|
||||
#
|
||||
# near IR emission lines and continua
|
||||
k 1 7676 total K I 7745
|
||||
6lev 8446 total O I 8446
|
||||
ca2x 8498 total Ca II 8498
|
||||
ca2y 8542 total Ca II 8542
|
||||
ca2z 8662 total Ca II 8662
|
||||
PA C 0 total of integrated H Paschen continuum
|
||||
totl 10830 total He I 10,830A, all three lines within multiplet
|
||||
h 1 1.875m total H Paschen-alpha
|
||||
#
|
||||
# The following 11 "lines" represent emission by a "6-level" Fe II atom
|
||||
# of Hamann & Ferland, a modification of the Wills, Netzer, and Wills.
|
||||
# See HAZY for some details.
|
||||
fe 2 6200
|
||||
fe 2 4300
|
||||
fe 2 2400
|
||||
fe 2 1080
|
||||
fe 2 1500
|
||||
fe 2 11500
|
||||
fe 2 2500
|
||||
fe 2 2300
|
||||
fe 2 8900
|
||||
fe 2 1216 pumping of the Fe II atom via H Lya 1216
|
||||
fe2c 0 cooling from the Fe II atom
|
||||
#
|
||||
# Some high critical density forbidden lines
|
||||
ne 5 3426 total [Ne V] 3426
|
||||
ne 3 3869 total [Ne III] 3869
|
||||
totl 4363 total [O III] 4363
|
||||
o 3 5007 total [O III] 5007
|
||||
Fe14 5303 total [Fe XIV] 5303
|
||||
o 1 5577 total [O I] 5577
|
||||
Fe 7 6087 total [Fe VII] 6087
|
||||
o 1 6300 total [O I] 6300
|
||||
Fe10 6373 total [Fe X] 6373
|
||||
Fe11 7892 total [Fe XI] 7892
|
||||
#
|
||||
# an optical incident continuum bin in units of nuFnu
|
||||
inci 4860 incident continuum at 4860 Angstroms in units of nuF(nu)
|
||||
#
|
||||
# The following are the total non-line emission from the cloud
|
||||
# (diffuse + reflected continuum) at a given wavelength in Angstroms.
|
||||
# All have units of nuF(nu).
|
||||
nFnu 122.4m microns
|
||||
#
|
||||
nFnu 8330 A
|
||||
nFnu 8079
|
||||
nFnu 6210
|
||||
nFnu 4885
|
||||
nFnu 3704
|
||||
nFnu 3588
|
||||
nFnu 2392
|
||||
nFnu 2071
|
||||
nFnu 2053
|
||||
nFnu 1793
|
||||
nFnu 1585
|
||||
#
|
||||
# In optically thick clouds of significant H I columns, Lya "Rayleigh
|
||||
# scattering" of incident continuum becomes important beginning here and
|
||||
# extending down to the Lyman limit.
|
||||
#
|
||||
nFnu 1458
|
||||
nFnu 1357
|
||||
nFnu 1297
|
||||
nFnu 1263
|
||||
nFnu 1218
|
||||
nFnu 1196
|
||||
nFnu 1175
|
||||
nFnu 1144
|
||||
nFnu 1113
|
||||
nFnu 1103
|
||||
nFnu 1074
|
||||
nFnu 1064
|
||||
nFnu 1036
|
||||
nFnu 1000
|
||||
nFnu 925.1
|
||||
nFnu 897.8
|
||||
nFnu 760
|
||||
nFnu 701.5
|
||||
nFnu 608.2
|
||||
nFnu 575.1
|
||||
nFnu 511.9
|
||||
nFnu 496.9
|
||||
nFnu 399.2
|
||||
#
|
||||
# The following are the inward directed non-line emission from the cloud
|
||||
# (diffuse + reflected continuum) at a given wavelength in Angstroms.
|
||||
# All have units of nuF(nu).
|
||||
#
|
||||
#InwT 1.119m
|
||||
#InwT 8220
|
||||
#InwT 8205
|
||||
#InwT 6209
|
||||
#InwT 4885
|
||||
#InwT 3649
|
||||
#InwT 3644
|
||||
#InwT 2392
|
||||
#InwT 2071
|
||||
#InwT 2052
|
||||
#InwT 1793
|
||||
#InwT 1585
|
||||
#InwT 1458
|
||||
#InwT 1356
|
||||
#InwT 1297
|
||||
#InwT 1262
|
||||
#InwT 1218
|
||||
#InwT 1196
|
||||
#InwT 1175
|
||||
#InwT 1143
|
||||
#InwT 1113
|
||||
#InwT 1103
|
||||
#InwT 1073
|
||||
#InwT 1064
|
||||
#InwT 1035
|
||||
#InwT 1000
|
||||
#InwT 897.8
|
||||
#InwT 925.1
|
||||
#InwT 760
|
||||
#InwT 701.5
|
||||
#InwT 608.2
|
||||
#InwT 575.1
|
||||
#InwT 399.2
|
||||
#
|
||||
# lines from he-like ions
|
||||
#>>chng 06 aug 17, mean wl of multiplet now used
|
||||
TOTL 5484A Li 2
|
||||
TOTL 3722A Be 3
|
||||
TOTL 2824A B 4
|
||||
TOTL 2275A C 5
|
||||
TOTL 1904A N 6
|
||||
TOTL 1634A O 7
|
||||
TOTL 1409A F 8
|
||||
TOTL 1266A Ne 9
|
||||
TOTL 1134A Na 10
|
||||
TOTL 1025A Mg 11
|
||||
# end dense line list
|
||||
# the file ends with the end of file, or a cr in the first col
|
||||
|
@ -1,31 +0,0 @@
|
||||
he 2 3203 total He II Paschen-beta line
|
||||
BA C 0 total of integrated H balmer continuum
|
||||
BaC 3646 total nuFnu of Balmer jump at 3646 (the head)
|
||||
He 1 3889 total H-6 (H-Balmer)
|
||||
ca2k 3934 total Ca II 3934 emission
|
||||
ca2h 3969 total Ca II 3969 emission
|
||||
h 1 4102 total H-delta
|
||||
h 1 4340 total H-gamma
|
||||
ca b 4471 total He I 4471, case B approximation
|
||||
he 2 4686 total He II 4686 (Paschen-alpha)
|
||||
inwd 4686 inward flux of He II 4686
|
||||
totl 4861 total H-beta 4861
|
||||
inwd 4861 inward flux of H-beta 4861
|
||||
He 1 5876 total He I 5876
|
||||
na 1 5892 total Na ID 5892
|
||||
h 1 6563 total H-alpha 6563
|
||||
# near IR emission lines and continua
|
||||
k 1 7676 total K I 7745
|
||||
6lev 8446 total O I 8446 #17
|
||||
ca2x 8498 total Ca II 8498
|
||||
ca2y 8542 total Ca II 8542
|
||||
ca2z 8662 total Ca II 8662
|
||||
PA C 0 total of integrated H Paschen continuum
|
||||
totl 10830 total He I 10,830A, all three lines within multiplet
|
||||
o 1 1.130m the O I line #added by dre #23
|
||||
h 1 1.875m total H Paschen-alpha
|
||||
#
|
||||
# The following 11 "lines" represent emission by a "6-level" Fe II atom
|
||||
# of Hamann & Ferland, a modification of the Wills, Netzer, and Wills.
|
||||
# See HAZY for some details.
|
||||
|
@ -1,109 +0,0 @@
|
||||
mg10 609.8A total Mg X 610 #0
|
||||
mg10 624.9A total Mg X 625
|
||||
totl 615 total of sum of both Mg X components
|
||||
o 5 629.7A total O V 630
|
||||
s 4 655.1A total S IV 655; level 2 line
|
||||
n 3 678.2A total N III 679; level 2 line #5
|
||||
o 3 698.2 total O III 703; level 2 line
|
||||
s 4 737.3 total S IV 737; level 2 line
|
||||
n 3 752.1 total N III 764; level 2 line
|
||||
n 4 765.1 total N IV 765
|
||||
ne 8 770.4 total Ne VIII 770 #10
|
||||
ne 8 780.3 total Ne VIII 780
|
||||
totl 774 total of sum of both Ne VIII component
|
||||
s 5 786.5 total S V 786
|
||||
o 4 789.4 total O IV 789
|
||||
s 4 798.8 total S IV 799 #15
|
||||
O 2 833.8 total O II 834A
|
||||
o 3 834.5 total O III 834
|
||||
totl 895 total Ne VII] 895
|
||||
s 6 933.4 total S VI 933
|
||||
s 6 944.5 total S VI 944 #20
|
||||
totl 933 total of sum of both S VI components
|
||||
p 4 950.7 total P IV 951; level 2 line
|
||||
h 1 972.5 total Lyman-gamma 973
|
||||
c 3 977 total C III 977
|
||||
n 3 991 total N III 990 #25
|
||||
h 1 1026 total Lyman-beta 1025
|
||||
o 6 1032 total O VI 1032
|
||||
o 6 1038 total O VI 1037
|
||||
totl 1035 total of sum of both O VI components #29
|
||||
he 2 1085 total He II Balmer-gamma 1085
|
||||
n 2 1085 total N II 1085
|
||||
s 4 1086 total S IV 1086; level 2 line
|
||||
p 5 1121 total P V 1121; level 2 line
|
||||
fe 3 1126 total Fe III 1122
|
||||
ne 5 1141 total Ne V 1141
|
||||
c 3 1176 total C III* 1176 (excited state)
|
||||
#inwd 1176 inward flux of C III* 1176
|
||||
s 3 1198 total S III 1198
|
||||
totl 1198 total S V 1198
|
||||
si 3 1207 total Si III 1207
|
||||
inci 1215 incident continuum at 1215 Angstroms in units of nuF(nu)
|
||||
totl 1216 total Hydrogen Lyman-alpha 1215.67
|
||||
inwd 1216 inward flux of Lyman-alpha
|
||||
he 2 1215 total He II Balmer-beta 1216
|
||||
#inwd 1215 inward flux of He II Balmer-beta 1216
|
||||
totl 1218 total of sum of O V] 1218 + [O V] 1218
|
||||
#inwd 1218 inward flux of O V]
|
||||
n 5 1239 total N V 1238.82
|
||||
n 5 1243 total N V 1242.80
|
||||
totl 1240 total of sum of both N V components #50
|
||||
#inwd 1240 inward flux of sum of both N V components
|
||||
s 2 1256 total S II 1256
|
||||
si 2 1263 total Si II 1260 + 1263
|
||||
6lev 1304 total O I 1302 + 1305
|
||||
si 2 1308 total Si II 1308
|
||||
c 2 1335 total C II 1335 + 1336
|
||||
si 4 1394 total Si IV 1394
|
||||
si 4 1403 total Si IV 1403 #58
|
||||
totl 1397 total of sum of both Si IV components
|
||||
#inwd 1397 inward flux of sum of both Si IV components
|
||||
totl 1402 total O IV] 1402; 5 components to line: #61
|
||||
#
|
||||
# 1397.2, 1399.77, 1401.16, 1404.81, 1407.39 --- not computed individually
|
||||
#inwd 1402 inward flux of O IV]
|
||||
totl 1406 total S IV 1406
|
||||
totl 1486 total of sum of N IV] 1486 + [N IV]
|
||||
N 4 1485 most forbidden of the pair
|
||||
#N 4 1486 stonger of the pair, at high density this will be the same as total
|
||||
#inwd 1488 inward flux of N IV]
|
||||
si 2 1531 total Si II 1527 + 1533
|
||||
c 4 1548 total C IV 1548.19
|
||||
c 4 1551 total C IV 1550.77
|
||||
totl 1549 total of sum of both C IV components #73
|
||||
inwd 1549 inward flux of sum of both C IV components
|
||||
he 2 1640 total He II Balmer-alpha 1640 #75
|
||||
inwd 1640 inward flux of He II Balmer-alpha 1640
|
||||
o 3 1661 total O III] 1661
|
||||
#inwd 1661 inward flux of O III] 1661
|
||||
o 3 1666 total O III] 1666
|
||||
#inwd 1666 inward flux of O III] 1666
|
||||
totl 1665 total of sum of both O III] components #81
|
||||
al 2 1671 total Al II 1670.8; level 2 line
|
||||
s 3 1720 total S III 1720
|
||||
totl 1750 total N III] 1750 (all components; not computed seperately)
|
||||
#inwd 1750 inward flux of N III]
|
||||
fe 2 1786 total Fe II 1787 (probably selectively excited)
|
||||
si 2 1814 total Si II 1814 (1808.0 + 1816.9 + 1817.5)
|
||||
al 3 1855 total Al III 1855
|
||||
al 3 1863 total Al III 1863
|
||||
totl 1860 total sum of both Al III components
|
||||
#inwd 1860 inward flux of sum of both Al III components
|
||||
totl 1888 total of sum of Si III] 1892 + [Si III] #92
|
||||
Si 3 1883 the most forbidden of the doublet
|
||||
#inwd 1892 inward flux of Si III] 1892
|
||||
totl 1909 total of sum of C III] 1908.73 + [C III] #95
|
||||
#inwd 1910 inward flux of C III] 1908.73
|
||||
n 2 2141 total sum of N II] 2139.01, 2142.77
|
||||
o 3 2321 single line from 5-level atom
|
||||
totl 2326 total C II] 2324.69 + 2328.12
|
||||
totl 2335 total Si II] 2335
|
||||
totl 2665 total of sum of Al II] 2669 + [Al II] 2660
|
||||
al 2 2660 emission from most forbidden line of multiplet
|
||||
mg 2 2796 total Mg II 2796 of the doublet
|
||||
mg 2 2803 total Mg II 2803 of the doublet
|
||||
totl 2798 total of sum of both Mg II components #105
|
||||
inwd 2798 inward flux of sum of both Mg II components
|
||||
#
|
||||
|
@ -1,101 +0,0 @@
|
||||
#
|
||||
# hydrogen Lyman series
|
||||
h 1 1216 total Lyman-alpha 1216
|
||||
h 1 1026 total Lyman-beta 1025
|
||||
H 1 972.5
|
||||
H 1 949.7
|
||||
H 1 937.8
|
||||
H 1 930.8
|
||||
H 1 926.2
|
||||
H 1 923.2
|
||||
H 1 921.0
|
||||
H 1 921.0
|
||||
H 1 918.1
|
||||
H 1 917.2
|
||||
H 1 916.4
|
||||
H 1 915.8
|
||||
H 1 915.3
|
||||
H 1 914.9
|
||||
H 1 914.6
|
||||
H 1 914.3
|
||||
H 1 914.0
|
||||
H 1 913.8
|
||||
H 1 913.6
|
||||
H 1 913.5
|
||||
H 1 913.3
|
||||
#
|
||||
#
|
||||
# hydrogen Balmer series
|
||||
#
|
||||
h 1 6563 total H-alpha 6563
|
||||
h 1 4861 total H-beta
|
||||
h 1 4340 total H-gamma
|
||||
h 1 4102 total H-delta
|
||||
h 1 3970 total H-epsilon
|
||||
h 1 3889 total H-8 (H-Balmer)
|
||||
h 1 3835 total H-9 (H-Balmer)
|
||||
H 1 3798
|
||||
H 1 3771
|
||||
H 1 3750
|
||||
H 1 3734
|
||||
H 1 3722
|
||||
H 1 3712
|
||||
H 1 3704
|
||||
H 1 3697
|
||||
H 1 3692
|
||||
H 1 3687
|
||||
H 1 3683
|
||||
H 1 3679
|
||||
H 1 3676
|
||||
H 1 3674
|
||||
H 1 3671
|
||||
#
|
||||
#
|
||||
# hydrogen Paschen series
|
||||
#
|
||||
h 1 1.875m total H Paschen-alpha
|
||||
H 1 1.282m total H Paschen-beta
|
||||
H 1 1.094m total H Paschen-gamma
|
||||
H 1 1.005m total H Paschen-delta
|
||||
H 1 0.9546m total H Paschen-8
|
||||
H 1 0.9229m total H Paschen-9
|
||||
H 1 0.9015m total H Paschen-10
|
||||
H 1 0.8863m total H Paschen-11
|
||||
H 1 8750
|
||||
H 1 8665
|
||||
H 1 8598
|
||||
H 1 8545
|
||||
H 1 8502
|
||||
H 1 8467
|
||||
H 1 8438
|
||||
H 1 8413
|
||||
H 1 8392
|
||||
H 1 8374
|
||||
H 1 8359
|
||||
H 1 8346
|
||||
H 1 8334
|
||||
#
|
||||
#
|
||||
# Brackett series
|
||||
#
|
||||
H 1 4.051m Brackett-alpha
|
||||
H 1 2.625m Brackett-beta
|
||||
H 1 2.166m Brackett-gamma
|
||||
H 1 1.945m Brackett-delta
|
||||
H 1 1.817m Brackett-epsilon
|
||||
H 1 1.736m Brackett 10
|
||||
H 1 1.681m Brackett 11
|
||||
H 1 1.641m Brackett 12
|
||||
H 1 1.611m Brackett 13
|
||||
H 1 1.588m
|
||||
H 1 1.570m
|
||||
H 1 1.556m
|
||||
H 1 1.544m
|
||||
H 1 1.534m
|
||||
H 1 1.526m
|
||||
H 1 1.519m
|
||||
H 1 1.513m
|
||||
H 1 1.508m
|
||||
H 1 1.504m
|
||||
H 1 1.500m
|
||||
#
|
@ -1,101 +0,0 @@
|
||||
#
|
||||
# hydrogen Lyman series
|
||||
h 1 1216 total Lyman-alpha 1216
|
||||
h 1 1026 total Lyman-beta 1025
|
||||
H 1 972.5
|
||||
H 1 949.7
|
||||
H 1 937.8
|
||||
H 1 930.8
|
||||
H 1 926.2
|
||||
H 1 923.2
|
||||
H 1 921.0
|
||||
#H 1 919.4
|
||||
#H 1 918.1
|
||||
#H 1 917.2
|
||||
#H 1 916.4
|
||||
#H 1 915.8
|
||||
#H 1 915.3
|
||||
#H 1 914.9
|
||||
#H 1 914.6
|
||||
#H 1 914.3
|
||||
#H 1 914.0
|
||||
#H 1 913.8
|
||||
#H 1 913.6
|
||||
#H 1 913.5
|
||||
#H 1 913.3
|
||||
#
|
||||
#
|
||||
# hydrogen Balmer series
|
||||
#
|
||||
h 1 6563 total H-alpha 6563
|
||||
h 1 4861 total H-beta
|
||||
h 1 4340 total H-gamma
|
||||
h 1 4102 total H-delta
|
||||
h 1 3970 total H-epsilon
|
||||
h 1 3889 total H-8 (H-Balmer)
|
||||
h 1 3835 total H-9 (H-Balmer)
|
||||
H 1 3798
|
||||
##H 1 3771
|
||||
#H 1 3750
|
||||
#H 1 3734
|
||||
#H 1 3722
|
||||
#H 1 3712
|
||||
#H 1 3704
|
||||
#H 1 3697
|
||||
#H 1 3692
|
||||
#H 1 3687
|
||||
#H 1 3683
|
||||
#H 1 3679
|
||||
#H 1 3676
|
||||
#H 1 3674
|
||||
#H 1 3671
|
||||
#
|
||||
#
|
||||
# hydrogen Paschen series
|
||||
#
|
||||
h 1 1.875m total H Paschen-alpha
|
||||
H 1 1.282m total H Paschen-beta
|
||||
H 1 1.094m total H Paschen-gamma
|
||||
H 1 1.005m total H Paschen-delta
|
||||
H 1 0.9546m total H Paschen-8
|
||||
H 1 0.9229m total H Paschen-9
|
||||
H 1 0.9015m total H Paschen-10
|
||||
#H 1 0.8863m total H Paschen-11
|
||||
#H 1 8750
|
||||
#H 1 8665
|
||||
#H 1 8598
|
||||
#H 1 8545
|
||||
#H 1 8502
|
||||
#H 1 8467
|
||||
#H 1 8438
|
||||
#H 1 8413
|
||||
#H 1 8392
|
||||
#H 1 8374
|
||||
#H 1 8359
|
||||
#H 1 8346
|
||||
#H 1 8334
|
||||
#
|
||||
#
|
||||
# Brackett series
|
||||
#
|
||||
H 1 4.051m Brackett-alpha
|
||||
H 1 2.625m Brackett-beta
|
||||
H 1 2.166m Brackett-gamma
|
||||
H 1 1.945m Brackett-delta
|
||||
H 1 1.817m Brackett-epsilon
|
||||
H 1 1.736m Brackett 10
|
||||
#H 1 1.681m Brackett 11
|
||||
#H 1 1.641m Brackett 12
|
||||
#H 1 1.611m Brackett 13
|
||||
#H 1 1.588m
|
||||
#H 1 1.570m
|
||||
#H 1 1.556m
|
||||
#H 1 1.544m
|
||||
#H 1 1.534m
|
||||
#H 1 1.526m
|
||||
#H 1 1.519m
|
||||
#H 1 1.513m
|
||||
#H 1 1.508m
|
||||
#H 1 1.504m
|
||||
#H 1 1.500m
|
||||
#
|
@ -1,21 +0,0 @@
|
||||
# Singlets
|
||||
#
|
||||
He 1 2.058m #2s-2p
|
||||
He 1 5016 #2s-3p
|
||||
#
|
||||
He 1 7281 #2p-3s
|
||||
He 1 5048 #2p-4s
|
||||
#
|
||||
He 1 6678 #2p-3d
|
||||
He 1 4922 #2p-4d
|
||||
He 1 4388 #2p-5d
|
||||
#Triplets
|
||||
#
|
||||
He 1 1.083m #2s-2p
|
||||
He 1 3889 #2s-3p
|
||||
#
|
||||
He 1 7065 #2p-3s
|
||||
He 1 4713 #2p-4s
|
||||
#
|
||||
He 1 5876 #2p-3d
|
||||
He 1 4471 #2p-4d
|
@ -1,12 +0,0 @@
|
||||
he 2 1215 total He II Balmer-beta 1216
|
||||
he 2 1640 total He II Balmer-alpha 1640
|
||||
he 2 4686 total He II 4686 (Paschen-alpha)
|
||||
he 2 1.012m total He II 10120A
|
||||
#
|
||||
he 2 4339 (near H Balmer gamma)
|
||||
he 2 4542
|
||||
he 2 4860 (near H Balmer beta)
|
||||
he 2 5412
|
||||
he 2 6560 (near H Balmer alpha)
|
||||
he 2 1.163m
|
||||
he 2 1.864m (near H Pa-alpha)
|
@ -1,842 +0,0 @@
|
||||
#Abort? Warnings? phi(h) %f HDEN=%f
|
||||
F F 17.000000 7.000000
|
||||
F F 17.000000 7.250000
|
||||
F F 17.000000 7.500000
|
||||
F F 17.000000 7.750000
|
||||
F F 17.000000 8.000000
|
||||
F F 17.000000 8.250000
|
||||
F F 17.000000 8.500000
|
||||
F F 17.000000 8.750000
|
||||
F F 17.000000 9.000000
|
||||
F F 17.000000 9.250000
|
||||
F F 17.000000 9.500000
|
||||
F F 17.000000 9.750000
|
||||
F F 17.000000 10.000000
|
||||
F F 17.000000 10.250000
|
||||
F F 17.000000 10.500000
|
||||
F F 17.000000 10.750000
|
||||
F F 17.000000 11.000000
|
||||
F F 17.000000 11.250000
|
||||
F F 17.000000 11.500000
|
||||
F F 17.000000 11.750000
|
||||
F F 17.000000 12.000000
|
||||
F F 17.000000 12.250000
|
||||
F F 17.000000 12.500000
|
||||
F F 17.000000 12.750000
|
||||
F F 17.000000 13.000000
|
||||
F F 17.000000 13.250000
|
||||
F F 17.000000 13.500000
|
||||
F F 17.000000 13.750000
|
||||
F F 17.000000 14.000000
|
||||
F F 17.250000 7.000000
|
||||
F F 17.250000 7.250000
|
||||
F F 17.250000 7.500000
|
||||
F F 17.250000 7.750000
|
||||
F F 17.250000 8.000000
|
||||
F F 17.250000 8.250000
|
||||
F F 17.250000 8.500000
|
||||
F F 17.250000 8.750000
|
||||
F F 17.250000 9.000000
|
||||
F F 17.250000 9.250000
|
||||
F F 17.250000 9.500000
|
||||
F F 17.250000 9.750000
|
||||
F F 17.250000 10.000000
|
||||
F F 17.250000 10.250000
|
||||
F F 17.250000 10.500000
|
||||
F F 17.250000 10.750000
|
||||
F F 17.250000 11.000000
|
||||
F F 17.250000 11.250000
|
||||
F F 17.250000 11.500000
|
||||
F F 17.250000 11.750000
|
||||
F F 17.250000 12.000000
|
||||
F F 17.250000 12.250000
|
||||
F F 17.250000 12.500000
|
||||
F F 17.250000 12.750000
|
||||
F F 17.250000 13.000000
|
||||
F F 17.250000 13.250000
|
||||
F F 17.250000 13.500000
|
||||
F F 17.250000 13.750000
|
||||
F F 17.250000 14.000000
|
||||
F F 17.500000 7.000000
|
||||
F F 17.500000 7.250000
|
||||
F F 17.500000 7.500000
|
||||
F F 17.500000 7.750000
|
||||
F F 17.500000 8.000000
|
||||
F F 17.500000 8.250000
|
||||
F F 17.500000 8.500000
|
||||
F F 17.500000 8.750000
|
||||
F F 17.500000 9.000000
|
||||
F F 17.500000 9.250000
|
||||
F F 17.500000 9.500000
|
||||
F F 17.500000 9.750000
|
||||
F F 17.500000 10.000000
|
||||
F F 17.500000 10.250000
|
||||
F F 17.500000 10.500000
|
||||
F F 17.500000 10.750000
|
||||
F F 17.500000 11.000000
|
||||
F F 17.500000 11.250000
|
||||
F F 17.500000 11.500000
|
||||
F F 17.500000 11.750000
|
||||
F F 17.500000 12.000000
|
||||
F F 17.500000 12.250000
|
||||
F F 17.500000 12.500000
|
||||
F F 17.500000 12.750000
|
||||
F F 17.500000 13.000000
|
||||
F F 17.500000 13.250000
|
||||
F F 17.500000 13.500000
|
||||
F F 17.500000 13.750000
|
||||
F F 17.500000 14.000000
|
||||
F F 17.750000 7.000000
|
||||
F F 17.750000 7.250000
|
||||
F F 17.750000 7.500000
|
||||
F F 17.750000 7.750000
|
||||
F F 17.750000 8.000000
|
||||
F F 17.750000 8.250000
|
||||
F F 17.750000 8.500000
|
||||
F F 17.750000 8.750000
|
||||
F F 17.750000 9.000000
|
||||
F F 17.750000 9.250000
|
||||
F F 17.750000 9.500000
|
||||
F F 17.750000 9.750000
|
||||
F F 17.750000 10.000000
|
||||
F F 17.750000 10.250000
|
||||
F F 17.750000 10.500000
|
||||
F F 17.750000 10.750000
|
||||
F F 17.750000 11.000000
|
||||
F F 17.750000 11.250000
|
||||
F F 17.750000 11.500000
|
||||
F F 17.750000 11.750000
|
||||
F F 17.750000 12.000000
|
||||
F F 17.750000 12.250000
|
||||
F F 17.750000 12.500000
|
||||
F F 17.750000 12.750000
|
||||
F F 17.750000 13.000000
|
||||
F F 17.750000 13.250000
|
||||
F F 17.750000 13.500000
|
||||
F F 17.750000 13.750000
|
||||
F F 17.750000 14.000000
|
||||
F F 18.000000 7.000000
|
||||
F F 18.000000 7.250000
|
||||
F F 18.000000 7.500000
|
||||
F F 18.000000 7.750000
|
||||
F F 18.000000 8.000000
|
||||
F F 18.000000 8.250000
|
||||
F F 18.000000 8.500000
|
||||
F F 18.000000 8.750000
|
||||
F F 18.000000 9.000000
|
||||
F F 18.000000 9.250000
|
||||
F F 18.000000 9.500000
|
||||
F F 18.000000 9.750000
|
||||
F F 18.000000 10.000000
|
||||
F F 18.000000 10.250000
|
||||
F F 18.000000 10.500000
|
||||
F F 18.000000 10.750000
|
||||
F F 18.000000 11.000000
|
||||
F F 18.000000 11.250000
|
||||
F F 18.000000 11.500000
|
||||
F F 18.000000 11.750000
|
||||
F F 18.000000 12.000000
|
||||
F F 18.000000 12.250000
|
||||
F F 18.000000 12.500000
|
||||
F F 18.000000 12.750000
|
||||
F F 18.000000 13.000000
|
||||
F F 18.000000 13.250000
|
||||
F F 18.000000 13.500000
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F F 22.000000 8.000000
|
||||
F F 22.000000 8.250000
|
||||
F F 22.000000 8.500000
|
||||
F F 22.000000 8.750000
|
||||
F F 22.000000 9.000000
|
||||
F F 22.000000 9.250000
|
||||
F F 22.000000 9.500000
|
||||
F F 22.000000 9.750000
|
||||
F F 22.000000 10.000000
|
||||
F F 22.000000 10.250000
|
||||
F F 22.000000 10.500000
|
||||
F F 22.000000 10.750000
|
||||
F F 22.000000 11.000000
|
||||
F F 22.000000 11.250000
|
||||
F F 22.000000 11.500000
|
||||
F F 22.000000 11.750000
|
||||
F F 22.000000 12.000000
|
||||
F F 22.000000 12.250000
|
||||
F F 22.000000 12.500000
|
||||
F F 22.000000 12.750000
|
||||
F F 22.000000 13.000000
|
||||
F F 22.000000 13.250000
|
||||
F F 22.000000 13.500000
|
||||
F F 22.000000 13.750000
|
||||
F F 22.000000 14.000000
|
||||
F F 22.250000 7.000000
|
||||
F F 22.250000 7.250000
|
||||
F F 22.250000 7.500000
|
||||
F F 22.250000 7.750000
|
||||
F F 22.250000 8.000000
|
||||
F F 22.250000 8.250000
|
||||
F F 22.250000 8.500000
|
||||
F F 22.250000 8.750000
|
||||
F F 22.250000 9.000000
|
||||
F F 22.250000 9.250000
|
||||
F F 22.250000 9.500000
|
||||
F F 22.250000 9.750000
|
||||
F F 22.250000 10.000000
|
||||
F F 22.250000 10.250000
|
||||
F F 22.250000 10.500000
|
||||
F F 22.250000 10.750000
|
||||
F F 22.250000 11.000000
|
||||
F F 22.250000 11.250000
|
||||
F F 22.250000 11.500000
|
||||
F F 22.250000 11.750000
|
||||
F F 22.250000 12.000000
|
||||
F F 22.250000 12.250000
|
||||
F F 22.250000 12.500000
|
||||
F F 22.250000 12.750000
|
||||
F F 22.250000 13.000000
|
||||
F F 22.250000 13.250000
|
||||
F F 22.250000 13.500000
|
||||
F F 22.250000 13.750000
|
||||
F F 22.250000 14.000000
|
||||
F F 22.500000 7.000000
|
||||
F F 22.500000 7.250000
|
||||
F F 22.500000 7.500000
|
||||
F F 22.500000 7.750000
|
||||
F F 22.500000 8.000000
|
||||
F F 22.500000 8.250000
|
||||
F F 22.500000 8.500000
|
||||
F F 22.500000 8.750000
|
||||
F F 22.500000 9.000000
|
||||
F F 22.500000 9.250000
|
||||
F F 22.500000 9.500000
|
||||
F F 22.500000 9.750000
|
||||
F F 22.500000 10.000000
|
||||
F F 22.500000 10.250000
|
||||
F F 22.500000 10.500000
|
||||
F F 22.500000 10.750000
|
||||
F F 22.500000 11.000000
|
||||
F F 22.500000 11.250000
|
||||
F F 22.500000 11.500000
|
||||
F F 22.500000 11.750000
|
||||
F F 22.500000 12.000000
|
||||
F F 22.500000 12.250000
|
||||
F F 22.500000 12.500000
|
||||
F F 22.500000 12.750000
|
||||
F F 22.500000 13.000000
|
||||
F F 22.500000 13.250000
|
||||
F F 22.500000 13.500000
|
||||
F F 22.500000 13.750000
|
||||
F F 22.500000 14.000000
|
||||
F F 22.750000 7.000000
|
||||
F F 22.750000 7.250000
|
||||
F F 22.750000 7.500000
|
||||
F F 22.750000 7.750000
|
||||
F F 22.750000 8.000000
|
||||
F F 22.750000 8.250000
|
||||
F F 22.750000 8.500000
|
||||
F F 22.750000 8.750000
|
||||
F F 22.750000 9.000000
|
||||
F F 22.750000 9.250000
|
||||
F F 22.750000 9.500000
|
||||
F F 22.750000 9.750000
|
||||
F F 22.750000 10.000000
|
||||
F F 22.750000 10.250000
|
||||
F F 22.750000 10.500000
|
||||
F F 22.750000 10.750000
|
||||
F F 22.750000 11.000000
|
||||
F F 22.750000 11.250000
|
||||
F F 22.750000 11.500000
|
||||
F F 22.750000 11.750000
|
||||
F F 22.750000 12.000000
|
||||
F F 22.750000 12.250000
|
||||
F F 22.750000 12.500000
|
||||
F F 22.750000 12.750000
|
||||
F F 22.750000 13.000000
|
||||
F F 22.750000 13.250000
|
||||
F F 22.750000 13.500000
|
||||
F F 22.750000 13.750000
|
||||
F F 22.750000 14.000000
|
||||
F F 23.000000 7.000000
|
||||
F F 23.000000 7.250000
|
||||
F F 23.000000 7.500000
|
||||
F F 23.000000 7.750000
|
||||
F F 23.000000 8.000000
|
||||
F F 23.000000 8.250000
|
||||
F F 23.000000 8.500000
|
||||
F F 23.000000 8.750000
|
||||
F F 23.000000 9.000000
|
||||
F F 23.000000 9.250000
|
||||
F F 23.000000 9.500000
|
||||
F F 23.000000 9.750000
|
||||
F F 23.000000 10.000000
|
||||
F F 23.000000 10.250000
|
||||
F F 23.000000 10.500000
|
||||
F F 23.000000 10.750000
|
||||
F F 23.000000 11.000000
|
||||
F F 23.000000 11.250000
|
||||
F F 23.000000 11.500000
|
||||
F F 23.000000 11.750000
|
||||
F F 23.000000 12.000000
|
||||
F F 23.000000 12.250000
|
||||
F F 23.000000 12.500000
|
||||
F F 23.000000 12.750000
|
||||
F F 23.000000 13.000000
|
||||
F F 23.000000 13.250000
|
||||
F F 23.000000 13.500000
|
||||
F F 23.000000 13.750000
|
||||
F F 23.000000 14.000000
|
||||
F F 23.250000 7.000000
|
||||
F F 23.250000 7.250000
|
||||
F F 23.250000 7.500000
|
||||
F F 23.250000 7.750000
|
||||
F F 23.250000 8.000000
|
||||
F F 23.250000 8.250000
|
||||
F F 23.250000 8.500000
|
||||
F F 23.250000 8.750000
|
||||
F F 23.250000 9.000000
|
||||
F F 23.250000 9.250000
|
||||
F F 23.250000 9.500000
|
||||
F F 23.250000 9.750000
|
||||
F F 23.250000 10.000000
|
||||
F F 23.250000 10.250000
|
||||
F F 23.250000 10.500000
|
||||
F F 23.250000 10.750000
|
||||
F F 23.250000 11.000000
|
||||
F F 23.250000 11.250000
|
||||
F F 23.250000 11.500000
|
||||
F F 23.250000 11.750000
|
||||
F F 23.250000 12.000000
|
||||
F F 23.250000 12.250000
|
||||
F F 23.250000 12.500000
|
||||
F F 23.250000 12.750000
|
||||
F F 23.250000 13.000000
|
||||
F F 23.250000 13.250000
|
||||
F F 23.250000 13.500000
|
||||
F F 23.250000 13.750000
|
||||
F F 23.250000 14.000000
|
||||
F F 23.500000 7.000000
|
||||
F F 23.500000 7.250000
|
||||
F F 23.500000 7.500000
|
||||
F F 23.500000 7.750000
|
||||
F F 23.500000 8.000000
|
||||
F F 23.500000 8.250000
|
||||
F F 23.500000 8.500000
|
||||
F F 23.500000 8.750000
|
||||
F F 23.500000 9.000000
|
||||
F F 23.500000 9.250000
|
||||
F F 23.500000 9.500000
|
||||
F F 23.500000 9.750000
|
||||
F F 23.500000 10.000000
|
||||
F F 23.500000 10.250000
|
||||
F F 23.500000 10.500000
|
||||
F F 23.500000 10.750000
|
||||
F F 23.500000 11.000000
|
||||
F F 23.500000 11.250000
|
||||
F F 23.500000 11.500000
|
||||
F F 23.500000 11.750000
|
||||
F F 23.500000 12.000000
|
||||
F F 23.500000 12.250000
|
||||
F F 23.500000 12.500000
|
||||
F F 23.500000 12.750000
|
||||
F F 23.500000 13.000000
|
||||
F F 23.500000 13.250000
|
||||
F F 23.500000 13.500000
|
||||
F F 23.500000 13.750000
|
||||
F F 23.500000 14.000000
|
||||
F F 23.750000 7.000000
|
||||
F F 23.750000 7.250000
|
||||
F F 23.750000 7.500000
|
||||
F F 23.750000 7.750000
|
||||
F F 23.750000 8.000000
|
||||
F F 23.750000 8.250000
|
||||
F F 23.750000 8.500000
|
||||
F F 23.750000 8.750000
|
||||
F F 23.750000 9.000000
|
||||
F F 23.750000 9.250000
|
||||
F F 23.750000 9.500000
|
||||
F F 23.750000 9.750000
|
||||
F F 23.750000 10.000000
|
||||
F F 23.750000 10.250000
|
||||
F F 23.750000 10.500000
|
||||
F F 23.750000 10.750000
|
||||
F F 23.750000 11.000000
|
||||
F F 23.750000 11.250000
|
||||
F F 23.750000 11.500000
|
||||
F F 23.750000 11.750000
|
||||
F F 23.750000 12.000000
|
||||
F F 23.750000 12.250000
|
||||
F F 23.750000 12.500000
|
||||
F F 23.750000 12.750000
|
||||
F F 23.750000 13.000000
|
||||
F F 23.750000 13.250000
|
||||
F F 23.750000 13.500000
|
||||
F F 23.750000 13.750000
|
||||
F F 23.750000 14.000000
|
||||
F F 24.000000 7.000000
|
||||
F F 24.000000 7.250000
|
||||
F F 24.000000 7.500000
|
||||
F F 24.000000 7.750000
|
||||
F F 24.000000 8.000000
|
||||
F F 24.000000 8.250000
|
||||
F F 24.000000 8.500000
|
||||
F F 24.000000 8.750000
|
||||
F F 24.000000 9.000000
|
||||
F F 24.000000 9.250000
|
||||
F F 24.000000 9.500000
|
||||
F F 24.000000 9.750000
|
||||
F F 24.000000 10.000000
|
||||
F F 24.000000 10.250000
|
||||
F F 24.000000 10.500000
|
||||
F F 24.000000 10.750000
|
||||
F F 24.000000 11.000000
|
||||
F F 24.000000 11.250000
|
||||
F F 24.000000 11.500000
|
||||
F F 24.000000 11.750000
|
||||
F F 24.000000 12.000000
|
||||
F F 24.000000 12.250000
|
||||
F F 24.000000 12.500000
|
||||
F F 24.000000 12.750000
|
||||
F F 24.000000 13.000000
|
||||
F F 24.000000 13.250000
|
||||
F F 24.000000 13.500000
|
||||
F F 24.000000 13.750000
|
||||
F F 24.000000 14.000000
|
File diff suppressed because it is too large
Load Diff
File diff suppressed because it is too large
Load Diff
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Load Diff
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Load Diff
Binary file not shown.
@ -1,26 +0,0 @@
|
||||
table agn
|
||||
phi(h) 17.000 vary
|
||||
grid from 17.0 to 24.0 in 1.00 dex steps
|
||||
hden 7.000 vary
|
||||
grid from 7.0 to 14.0 in 1.00 dex steps
|
||||
normalize to "inci" 1215 scale factor = 1215
|
||||
C
|
||||
atom H-like element hydrogen levels resolved 18
|
||||
atom He-like element helium levels resolved 15
|
||||
atom H-like element helium levels resolved 15
|
||||
set nend 5000
|
||||
stop column density 23
|
||||
iterate to convergence
|
||||
C
|
||||
print short
|
||||
print line faint 1
|
||||
punch overview "blr_grid_p17-24_n07-14_H18_HeI15_HeII15.ovr" last
|
||||
punch grid "blr_grid_p17-24_n07-14_H18_HeI15_HeII15.gri" last
|
||||
C punch continuum "blr_grid_p17-24_n07-14_H18_HeI15_HeII15.con" units angstroms last
|
||||
C
|
||||
punch linelist "blr_grid_p17-24_n07-14_H18_HeI15_HeII15.llh" "LineList_H_short.dat" last
|
||||
punch linelist "blr_grid_p17-24_n07-14_H18_HeI15_HeII15.llbuv" "LineList_BLR_uv.dat" last
|
||||
punch linelist "blr_grid_p17-24_n07-14_H18_HeI15_HeII15.llbonir" "LineList_BLR_onir.dat" last
|
||||
punch linelist "blr_grid_p17-24_n07-14_H18_HeI15_HeII15.llbhe2" "LineList_HeII.dat" last
|
||||
punch linelist "blr_grid_p17-24_n07-14_H18_HeI15_HeII15.llhe1" "LineList_HeI.dat" last
|
||||
|
@ -1,214 +0,0 @@
|
||||
710044: C-This is the last iteration and H 1 Ly(a) optical depth changed by 84% (was 1.19e+07). Try another iteration.
|
||||
710045- !Charge transfer ionization of H reached 99.4% of the local H ionization rate.
|
||||
710046- !Photoionization of upper level of Mg II 2798 reached 100.0% of the total Mg+ photo rate.
|
||||
710047- !Photoionization of upper levels of [O I] reached 15.1% of the total O destruction rate.
|
||||
710048- !Photoionization of upper levels of [O III] reached 12.8% of the total O++ photo rate.
|
||||
710049- !The largest plasma frequency was 2.46e-07 Ryd = 3.70e+05 micron The continuum is set to 0 below this.
|
||||
710050- !The largest continuum brightness temperature was 5.165e+03K at 9.109e-03 Ryd.
|
||||
710051- !AGE: Cloud age was not set. Longest timescale was 2.00e+03 s.
|
||||
710052- !The excitation temp of Lya exceeded the electron temp, largest value was 1.81e+04K (gas temp there was 1.38e+04K, zone 141)
|
||||
710053- !Some iso-structure lines mased: He-like HELI, line 12-11 had optical depth -1.60e+00
|
||||
710054- !Some iso-structure lines mased: He-like HELI, line 20-17 had optical depth -8.03e-01
|
||||
710055- !Some iso-structure lines mased: He-like HELI, line 29-27 had optical depth -1.29e+00
|
||||
710056- !Some iso-structure lines mased: He-like HELI, line 30-25 had optical depth -7.92e-01
|
||||
710057- !Some iso-structure lines mased: He-like HELI, line 39-37 had optical depth -4.13e-01
|
||||
710058- !Some iso-structure lines mased: He-like HELI, line 41-39 had optical depth -2.04e-01
|
||||
710059- !Some iso-structure lines mased: He-like HELI, line 42-35 had optical depth -4.19e-01
|
||||
710060- !Some iso-structure lines mased: He-like HELI, line 51-49 had optical depth -1.32e-01
|
||||
710061- !Some iso-structure lines mased: He-like HELI, line 56-47 had optical depth -2.21e-01
|
||||
710062- !Some iso-structure lines mased: He-like HELI, line 72-61 had optical depth -1.27e-01
|
||||
710063- !The CMB was not included. This is added with the CMB command.
|
||||
710064- !The ratio of radiation to gas pressure reached 7.95e-01 at zone 135. Caused by Lyman alpha.
|
||||
710065- !The radiation pressure jumped by 224% at zone 140, from 8.67e-02 to 2.47e-02 to 2.37e-02
|
||||
710066- Charge transfer heating reached 2.98% of the local heating.
|
||||
710067- The largest continuum occupation number was 7.075e+02 at 2.341e-07 Ryd.
|
||||
710068- Photoionization of Ca+ 2D level by Ly-alpha reached 87.3% of the total rate out.
|
||||
710069- G-bar cooling lines reached 1.18% of the local cooling. Line=Mn 2 2589A
|
||||
710070- Line absorption heating reached 1.65% of the local heating.
|
||||
710071- Bound Compton heating reached 2.80% of the local heating.
|
||||
710072- Rate of induced H 2-photon emission reached 1.02e-01 s^-1
|
||||
710073- Induced recombination was 85.5% of the total for H level170
|
||||
710074- Stimulated emission was 99.5% of the total for H transition171 -170
|
||||
710075- Timescale-photoerosion of Fe=4.94e+06 yr
|
||||
710076- The Balmer continuum optical depth was 1.26e-01.
|
||||
710077- The Balmer continuum stimulated emission correction to optical depths reached 1.41e-01.
|
||||
710078- The continuum optical depth at the lowest energy considered (1.055e-08 Ryd) was 4.569e+10.
|
||||
710079- The optical depth to electron scattering is 0.074
|
||||
710080-
|
||||
710081- *********************************> Cloudy 08.00 <**********************************
|
||||
710082- * table agn *
|
||||
710083- * phi(h) 19.750000 range 0.999466 7354000.000000 *
|
||||
710084- * grid from 19.0 to 19.75 in 0.25 dex steps *
|
||||
710085- * HDEN=9.750000 *
|
||||
--
|
||||
919519: C-This is the last iteration and H 1 Ly(a) optical depth changed by 98% (was 5.72e+06). Try another iteration.
|
||||
919520- !Photoionization of upper level of Mg II 2798 reached 10.6% of the total Mg+ photo rate.
|
||||
919521- !Photoionization of upper levels of [O III] reached 12.4% of the total O++ photo rate.
|
||||
919522- !The largest plasma frequency was 7.78e-07 Ryd = 1.17e+05 micron The continuum is set to 0 below this.
|
||||
919523- !The largest continuum brightness temperature was 2.904e+04K at 9.109e-03 Ryd.
|
||||
919524- !AGE: Cloud age was not set. Longest timescale was 1.61e+02 s.
|
||||
919525- !The excitation temp of Lya exceeded the electron temp, largest value was 2.38e+04K (gas temp there was 1.32e+04K, zone 154)
|
||||
919526- !Some iso-structure lines mased: He-like HELI, line 20-17 had optical depth -3.44e-01
|
||||
919527- !Some iso-structure lines mased: He-like HELI, line 30-25 had optical depth -8.74e-01
|
||||
919528- !Some iso-structure lines mased: He-like HELI, line 42-35 had optical depth -5.27e-01
|
||||
919529- !Some iso-structure lines mased: He-like HELI, line 56-47 had optical depth -3.03e-01
|
||||
919530- !Some iso-structure lines mased: He-like HELI, line 72-61 had optical depth -1.57e-01
|
||||
919531- !The CMB was not included. This is added with the CMB command.
|
||||
919532- !The ratio of radiation to gas pressure reached 6.42e-01 at zone 157. Caused by Lyman alpha.
|
||||
919533- !The radiation pressure jumped by 290% at zone 162, from 3.20e-01 to 6.58e-02 to 6.17e-02
|
||||
919534- Continuum fluorescent production of H-beta was significant.
|
||||
919535- Photoionization of upper levels of [O I] reached 4.3% of the total O destruction rate.
|
||||
919536- The largest continuum occupation number was 2.295e+03 at 7.032e-07 Ryd.
|
||||
919537- The continuum brightness temperature fell below 10,000K at 6.985e+00 microns.
|
||||
919538- Photoionization of Ca+ 2D level by Ly-alpha reached 70.3% of the total rate out.
|
||||
919539- Line absorption heating reached 1.99% of the local heating.
|
||||
919540- Rate of induced H 2-photon emission reached 5.45e-01 s^-1
|
||||
919541- Induced recombination was 97.1% of the total for H level170
|
||||
919542- Stimulated emission was 99.9% of the total for H transition171 -170
|
||||
919543- Timescale-photoerosion of Fe=8.78e+05 yr
|
||||
919544- Induced recombination cooling was 1.5% of the total.
|
||||
919545- Free-free heating was 6.1% of the total.
|
||||
919546- The Balmer continuum optical depth was 3.39e-01.
|
||||
919547- The Balmer continuum stimulated emission correction to optical depths reached 1.52e-01.
|
||||
919548- The continuum optical depth at the lowest energy considered (1.055e-08 Ryd) was 5.897e+11.
|
||||
919549- The optical depth to electron scattering is 0.073
|
||||
919550- Line radiation pressure capped by thermalization length.
|
||||
919551-
|
||||
919552- *********************************> Cloudy 08.00 <**********************************
|
||||
919553- * table agn *
|
||||
919554- * phi(h) 20.500000 range 0.999466 7354000.000000 *
|
||||
919555- * grid from 20.0 to 20.75 in 0.25 dex steps *
|
||||
919556- * HDEN=10.750000 *
|
||||
919557- * grid from 7.0 to 14.0 in 0.25 dex steps *
|
||||
919558- * normalize to "inci" 1215 scale factor = 1215 *
|
||||
919559- * C *
|
||||
919560- * atom H-like element hydrogen levels resolved 18 *
|
||||
--
|
||||
981567: C-This is the last iteration and C 6 Bal(a) optical depth changed by 20.6% (was 1.32e+00). Try another iteration.
|
||||
981568- !Photoionization of upper levels of [O III] reached 12.9% of the total O++ photo rate.
|
||||
981569- !The largest plasma frequency was 7.78e-07 Ryd = 1.17e+05 micron The continuum is set to 0 below this.
|
||||
981570- !The largest continuum brightness temperature was 5.165e+04K at 9.109e-03 Ryd.
|
||||
981571- !AGE: Cloud age was not set. Longest timescale was 1.49e+02 s.
|
||||
981572- !The excitation temp of Lya exceeded the electron temp, largest value was 2.36e+04K (gas temp there was 1.49e+04K, zone 162)
|
||||
981573- !Some iso-structure lines mased: He-like HELI, line 12-11 had optical depth -7.88e-01
|
||||
981574- !Some iso-structure lines mased: He-like HELI, line 19-17 had optical depth -1.92e-01
|
||||
981575- !Some iso-structure lines mased: He-like HELI, line 20-17 had optical depth -4.74e-01
|
||||
981576- !Some iso-structure lines mased: He-like HELI, line 29-27 had optical depth -2.18e-01
|
||||
981577- !Some iso-structure lines mased: He-like HELI, line 30-25 had optical depth -6.46e-01
|
||||
981578- !Some iso-structure lines mased: He-like HELI, line 42-35 had optical depth -3.18e-01
|
||||
981579- !Some iso-structure lines mased: He-like HELI, line 56-47 had optical depth -1.76e-01
|
||||
981580- !The CMB was not included. This is added with the CMB command.
|
||||
981581- !The ratio of radiation to gas pressure reached 6.48e-01 at zone 165. Caused by Lyman alpha.
|
||||
981582- !The radiation pressure jumped by 174% at zone 3, from 6.81e-06 to 2.95e-05 to 9.61e-05
|
||||
981583- Continuum fluorescent production of H-beta was significant.
|
||||
981584- Photoionization of upper level of Mg II 2798 reached 2.5% of the total Mg+ photo rate.
|
||||
981585- Photoionization of upper levels of [O I] reached 2.7% of the total O destruction rate.
|
||||
981586- The largest continuum occupation number was 4.081e+03 at 7.032e-07 Ryd.
|
||||
981587- The continuum brightness temperature fell below 10,000K at 5.777e+00 microns.
|
||||
981588- Photoionization of Ca+ 2D level by Ly-alpha reached 76.5% of the total rate out.
|
||||
981589- Line absorption heating reached 2.37% of the local heating.
|
||||
981590- Rate of induced H 2-photon emission reached 9.68e-01 s^-1
|
||||
981591- Induced recombination was 98.3% of the total for H level170
|
||||
981592- Stimulated emission was 99.9% of the total for H transition171 -170
|
||||
981593- Timescale-photoerosion of Fe=4.94e+05 yr
|
||||
981594- Induced recombination cooling was 1.4% of the total.
|
||||
981595- Free-free heating was 6.3% of the total.
|
||||
981596- The Balmer continuum optical depth was 1.36e-01.
|
||||
981597- The Balmer continuum stimulated emission correction to optical depths reached 1.48e-01.
|
||||
981598- The continuum optical depth at the lowest energy considered (1.055e-08 Ryd) was 4.269e+11.
|
||||
981599- The optical depth to electron scattering is 0.074
|
||||
981600- Line radiation pressure capped by thermalization length.
|
||||
981601-
|
||||
981602- *********************************> Cloudy 08.00 <**********************************
|
||||
981603- * table agn *
|
||||
981604- * phi(h) 20.750000 range 0.999466 7354000.000000 *
|
||||
981605- * grid from 20.0 to 20.75 in 0.25 dex steps *
|
||||
981606- * HDEN=10.750000 *
|
||||
981607- * grid from 7.0 to 14.0 in 0.25 dex steps *
|
||||
981608- * normalize to "inci" 1215 scale factor = 1215 *
|
||||
--
|
||||
1329800: C-This is the last iteration and He 2 Ly(a) optical depth changed by 28% (was 6.94e+04). Try another iteration.
|
||||
1329801- !Continuum fluorescent production of H-beta was very important.
|
||||
1329802- !Photoionization of upper levels of [O III] reached 14.6% of the total O++ photo rate.
|
||||
1329803- !The largest plasma frequency was 1.85e-06 Ryd = 4.94e+04 micron The continuum is set to 0 below this.
|
||||
1329804- !The largest continuum brightness temperature was 1.633e+06K at 9.109e-03 Ryd.
|
||||
1329805- !AGE: Cloud age was not set. Longest timescale was 3.59e+01 s.
|
||||
1329806- !The excitation temp of Lya exceeded the electron temp, largest value was 2.42e+04K (gas temp there was 2.22e+04K, zone 232)
|
||||
1329807- !Rate of induced H 2-photon emission reached 3.05e+01 s^-1
|
||||
1329808- !Free-free heating was 33.3% of the total.
|
||||
1329809- !The CMB was not included. This is added with the CMB command.
|
||||
1329810- !The ratio of radiation to gas pressure reached 8.20e-01 at zone 163. Caused by Lyman alpha.
|
||||
1329811- !The radiation pressure jumped by 249% at zone 3, from 1.63e-05 to 1.05e-04 to 5.05e-04
|
||||
1329812- Te-ne bounds of Case B lookup table exceeded, H I Case B line intensities set to zero.
|
||||
1329813- The largest continuum occupation number was 8.228e+04 at 1.730e-06 Ryd.
|
||||
1329814- The continuum occupation number fell below 1 at 1.714e+00 microns.
|
||||
1329815- The continuum brightness temperature fell below 10,000K at 1.820e+00 microns.
|
||||
1329816- Photoionization of Ca+ 2D level by Ly-alpha reached 43.8% of the total rate out.
|
||||
1329817- Line absorption heating reached 2.15% of the global heating.
|
||||
1329818- G-bar cooling lines reached 7.37% of the local cooling. Line=P 5 1121A
|
||||
1329819- Line absorption heating reached 6.53% of the local heating.
|
||||
1329820- Induced recombination was 99.9% of the total for H level170
|
||||
1329821- Stimulated emission was 100.0% of the total for H transition171 -170
|
||||
1329822- Timescale-photoerosion of Fe=1.56e+04 yr
|
||||
1329823- Compton heating was 1.2% of the total.
|
||||
1329824- Induced recombination cooling was 6.3% of the total.
|
||||
1329825- The continuum optical depth at the lowest energy considered (1.055e-08 Ryd) was 1.168e+12.
|
||||
1329826- The optical depth to electron scattering is 0.080
|
||||
1329827- Line radiation pressure capped by thermalization length.
|
||||
1329828-
|
||||
1329829- *********************************> Cloudy 08.00 <**********************************
|
||||
1329830- * table agn *
|
||||
1329831- * phi(h) 22.250000 range 0.999466 7354000.000000 *
|
||||
1329832- * grid from 22.0 to 22.75 in 0.25 dex steps *
|
||||
1329833- * HDEN=11.500000 *
|
||||
1329834- * grid from 7.0 to 14.0 in 0.25 dex steps *
|
||||
1329835- * normalize to "inci" 1215 scale factor = 1215 *
|
||||
1329836- * C *
|
||||
1329837- * atom H-like element hydrogen levels resolved 18 *
|
||||
1329838- * atom He-like element helium levels resolved 15 *
|
||||
1329839- * atom H-like element helium levels resolved 15 *
|
||||
1329840- * set nend 5000 *
|
||||
1329841- * stop column density 23 *
|
||||
--
|
||||
1494646: C-This is the last iteration and He 2 Ly(a) optical depth changed by 32% (was 8.28e+04). Try another iteration.
|
||||
1494647- !Continuum fluorescent production of H-beta was very important.
|
||||
1494648- !Photoionization of upper levels of [O III] reached 16.5% of the total O++ photo rate.
|
||||
1494649- !The largest plasma frequency was 5.84e-06 Ryd = 1.56e+04 micron The continuum is set to 0 below this.
|
||||
1494650- !The largest continuum brightness temperature was 9.184e+06K at 9.109e-03 Ryd.
|
||||
1494651- !AGE: Cloud age was not set. Longest timescale was 4.36e+00 s.
|
||||
1494652- !G-bar cooling lines reached 23.72% of the local cooling. Line=O 3 698A
|
||||
1494653- !Rate of induced H 2-photon emission reached 1.72e+02 s^-1
|
||||
1494654- !Free-free heating was 64.8% of the total.
|
||||
1494655- !The CMB was not included. This is added with the CMB command.
|
||||
1494656- !The ratio of radiation to gas pressure reached 5.71e-01 at zone 176. Caused by Lyman alpha.
|
||||
1494657- !The radiation pressure jumped by 334% at zone 3, from 0.00e+00 to 4.65e-05 to 3.10e-04
|
||||
1494658- Thermal collisional ionization of H reached 1.80% of the local ionization rate.
|
||||
1494659- Te-ne bounds of Case B lookup table exceeded, H I Case B line intensities set to zero.
|
||||
1494660- Photoionization of upper levels of [O I] reached 1.3% of the total O destruction rate.
|
||||
1494661- The largest continuum occupation number was 2.669e+05 at 5.196e-06 Ryd.
|
||||
1494662- The continuum occupation number fell below 1 at 1.115e+00 microns.
|
||||
1494663- The continuum brightness temperature fell below 10,000K at 1.024e+00 microns.
|
||||
1494664- Photoionization of Ca+ 2D level by Ly-alpha reached 14.4% of the total rate out.
|
||||
1494665- Line absorption heating reached 3.26% of the global heating.
|
||||
1494666- Line absorption heating reached 7.52% of the local heating.
|
||||
1494667- Induced recombination was 100.0% of the total for H level170
|
||||
1494668- Stimulated emission was 100.0% of the total for H transition171 -170
|
||||
1494669- Timescale-photoerosion of Fe=2.78e+03 yr
|
||||
1494670- Induced recombination cooling was 14.9% of the total.
|
||||
1494671- The Balmer continuum optical depth was 5.26e-02.
|
||||
1494672- The continuum optical depth at the lowest energy considered (1.055e-08 Ryd) was 8.345e+12.
|
||||
1494673- The continuum of the computed structure may be optically thick in the near infrared.
|
||||
1494674- The optical depth to electron scattering is 0.080
|
||||
1494675- Line radiation pressure capped by thermalization length.
|
||||
1494676-
|
||||
1494677- *********************************> Cloudy 08.00 <**********************************
|
||||
1494678- * table agn *
|
||||
1494679- * phi(h) 23.000000 range 0.999466 7354000.000000 *
|
||||
1494680- * grid from 23.0 to 23.25 in 0.25 dex steps *
|
||||
1494681- * HDEN=12.500000 *
|
||||
1494682- * grid from 7.0 to 14.0 in 0.25 dex steps *
|
||||
1494683- * normalize to "inci" 1215 scale factor = 1215 *
|
||||
1494684- * C *
|
||||
1494685- * atom H-like element hydrogen levels resolved 18 *
|
||||
1494686- * atom He-like element helium levels resolved 15 *
|
||||
1494687- * atom H-like element helium levels resolved 15 *
|
@ -1,305 +0,0 @@
|
||||
#Proposed 'emission line list' for dumping -emergent- fluxes to fort.xxx files.
|
||||
# Lines appear in approximate order they appear in Cloudy standard output file.
|
||||
|
||||
#two incident continuum points
|
||||
inci 1215.00A
|
||||
inci 4860.00A
|
||||
|
||||
#Lyman Lines:
|
||||
TOTL 1215.68A
|
||||
H 1 1215.68A
|
||||
H 1 1215.68A
|
||||
H 1 1025.73A
|
||||
H 1 972.543A
|
||||
H 1 949.749A
|
||||
|
||||
#Balmer Lines:
|
||||
H 1 6562.85A
|
||||
H 1 4861.36A
|
||||
H 1 4340.49A
|
||||
H 1 4101.76A
|
||||
H 1 3970.09A
|
||||
H 1 3889.07A
|
||||
#Ba C 0
|
||||
|
||||
#Paschen Lines:
|
||||
H 1 1.87511m
|
||||
H 1 1.28181m
|
||||
H 1 1.09381m
|
||||
H 1 1.00494m
|
||||
H 1 9545.99A
|
||||
H 1 9229.03A
|
||||
#PA C 0
|
||||
|
||||
#Brackett gamma:
|
||||
H 1 2.16553m
|
||||
|
||||
#He II lines:
|
||||
He 2 1640.00A
|
||||
He 2 1215.23A
|
||||
He 2 1085.03A
|
||||
He 2 1025.35A
|
||||
He 2 992.439A
|
||||
He 2 972.186A
|
||||
He 2 4686.01A
|
||||
He 2 3203.30A
|
||||
He 2 2733.46A
|
||||
He 2 1.01242m
|
||||
He 2 6560.44A
|
||||
He 2 5411.80A
|
||||
He 2 4859.57A
|
||||
He 2 4541.82A
|
||||
He 2 4338.89A
|
||||
He 2 4200.05A
|
||||
He 2 4100.25A
|
||||
He 2 4025.81A
|
||||
He 2 3968.64A
|
||||
|
||||
#He I Lines:
|
||||
TOTL 1.08299m
|
||||
He 1 1.08291m # 1S1 to 3P0
|
||||
He 1 1.08303m # 1S1 to 3P1
|
||||
He 1 1.08303m # 1S1 to 3P2
|
||||
He 1 3888.63A
|
||||
He 1 2.05813m
|
||||
He 1 5015.68A
|
||||
He 1 7065.18A
|
||||
He 1 5875.61A
|
||||
He 1 4713.02A
|
||||
He 1 4471.47A
|
||||
He 1 4120.81A
|
||||
He 1 7281.35A
|
||||
He 1 6678.15A
|
||||
He 1 5047.64A
|
||||
He 1 4921.93A
|
||||
He 1 4437.55A
|
||||
He 1 4387.93A
|
||||
|
||||
#Heavy Element Lines:
|
||||
C 1 1656.00A
|
||||
TOTL 2326.00A
|
||||
C 2 2325.00A
|
||||
C 2 2324.00A
|
||||
C 2 2329.00A
|
||||
C 2 2328.00A
|
||||
C 2 2327.00A
|
||||
C 2 1335.00A
|
||||
C 3 977.000A
|
||||
TOTL 1909.00A
|
||||
C 3 1910.00A
|
||||
C 3 1176.00A
|
||||
TOTL 1549.00A
|
||||
C 4 1551.00A
|
||||
C 4 1548.00A
|
||||
N 1 1200.00A
|
||||
N 2 2141.00A
|
||||
N 2 1085.00A
|
||||
TOTL 1750.00A
|
||||
N 3 1749.00A
|
||||
N 3 1747.00A
|
||||
N 3 1754.00A
|
||||
N 3 1752.00A
|
||||
N 3 1751.00A
|
||||
N 3 991.000A
|
||||
TOTL 1486.00A
|
||||
N 4 1486.00A
|
||||
N 4 765.000A
|
||||
TOTL 1240.00A
|
||||
N 5 1243.00A
|
||||
N 5 1239.00A
|
||||
6lev 8446.00A
|
||||
6lev 1304.00A
|
||||
TOTL 1665.00A
|
||||
O 3 1661.00A
|
||||
O 3 1666.00A
|
||||
O 3 835.000A
|
||||
TOTL 1402.00A
|
||||
O 4 1400.00A
|
||||
O 4 1397.00A
|
||||
O 4 1407.00A
|
||||
O 4 1405.00A
|
||||
O 4 1401.00A
|
||||
O 4 789.000A
|
||||
O 5 630.000A
|
||||
TOTL 1218.00A
|
||||
O 5 1218.00A
|
||||
TOTL 1035.00A
|
||||
O 6 1031.93A
|
||||
O 6 1037.62A
|
||||
Ne 5 1141.00A
|
||||
TOTL 774.000A
|
||||
Ne 8 770.404A
|
||||
Ne 8 780.324A
|
||||
Na 1 5891.94A
|
||||
Mg 1 2853.00A
|
||||
TOTL 2798.00A
|
||||
Mg 2 2795.53A
|
||||
Mg 2 2802.71A
|
||||
TOTL 615.000A
|
||||
Mg10 609.793A
|
||||
Mg10 624.941A
|
||||
totl 2665.00A
|
||||
Al 2 2670.00A
|
||||
TOTL 1860.00A
|
||||
Al 3 1855.00A
|
||||
Al 3 1863.00A
|
||||
TOTL 2335.00A
|
||||
Si 2 2334.00A
|
||||
Si 2 2329.00A
|
||||
Si 2 2350.00A
|
||||
Si 2 2344.00A
|
||||
Si 2 2336.00A
|
||||
Si 2 1813.99A
|
||||
Si 2 1531.00A
|
||||
Si 2 1307.66A
|
||||
Si 2 1263.32A
|
||||
Si 3 1207.00A
|
||||
TOTL 1888.00A
|
||||
Si 3 1892.00A
|
||||
TOTL 1397.00A
|
||||
Si 4 1403.00A
|
||||
Si 4 1394.00A
|
||||
S 2 1256.00A
|
||||
S 3 1720.00A
|
||||
S 3 1197.56A
|
||||
TOTL 1406.00A
|
||||
S 4 1405.00A
|
||||
S 4 1398.00A
|
||||
S 4 1424.00A
|
||||
S 4 1417.00A
|
||||
S 4 1406.00A
|
||||
TOTL 1198.00A
|
||||
S 5 1198.00A
|
||||
S 5 786.473A
|
||||
S 6 944.524A
|
||||
S 6 933.380A
|
||||
Ca2K 3934.00A
|
||||
Ca2H 3969.00A
|
||||
Ca2X 8498.00A
|
||||
Ca2Y 8542.00A
|
||||
Ca2Z 8662.00A
|
||||
Fe 2 1500.00A
|
||||
Fe 2 1.15000m
|
||||
Fe 2 2500.00A
|
||||
Fe 2 2300.00A
|
||||
Fe 2 8900.00A
|
||||
Fe 2 1786.00A
|
||||
Fe 3 1125.79A
|
||||
FeKa 1.78000A
|
||||
|
||||
#Diffuse continua:
|
||||
nFnu 4.11370m
|
||||
nInu 4.11370m
|
||||
inwT 4.11370m
|
||||
inwC 4.11370m
|
||||
# need to add in remaining inwT and inwC
|
||||
nFnu 2.32440m
|
||||
nInu 2.32440m
|
||||
nFnu 1.64313m
|
||||
nInu 1.64313m
|
||||
nFnu 1.48022m
|
||||
nInu 1.48022m
|
||||
nFnu 1.43649m
|
||||
nInu 1.43649m
|
||||
nFnu 1.11867m
|
||||
nInu 1.11867m
|
||||
nFnu 8329.68A
|
||||
nInu 8329.68A
|
||||
nFnu 8078.61A
|
||||
nInu 8078.61A
|
||||
nFnu 6209.66A
|
||||
nInu 6209.66A
|
||||
nFnu 4885.36A
|
||||
nInu 4885.36A
|
||||
nFnu 3704.34A
|
||||
nInu 3704.34A
|
||||
nFnu 3587.67A
|
||||
nInu 3587.67A
|
||||
nFnu 2430.05A
|
||||
nInu 2430.05A
|
||||
nFnu 2392.03A
|
||||
nInu 2392.03A
|
||||
nFnu 2071.34A
|
||||
nInu 2071.34A
|
||||
nFnu 2052.68A
|
||||
nInu 2052.68A
|
||||
nFnu 1793.44A
|
||||
nInu 1793.44A
|
||||
nFnu 1585.12A
|
||||
nInu 1585.12A
|
||||
nFnu 1458.33A
|
||||
nInu 1458.33A
|
||||
nFnu 1356.96A
|
||||
nInu 1356.96A
|
||||
nFnu 1297.29A
|
||||
nInu 1297.29A
|
||||
nFnu 1262.79A
|
||||
nInu 1262.79A
|
||||
nInu 1218.08A
|
||||
nFnu 1196.33A
|
||||
nInu 1196.33A
|
||||
nFnu 1175.06A
|
||||
nInu 1175.06A
|
||||
nFnu 1143.64A
|
||||
nInu 1143.64A
|
||||
nFnu 1113.22A
|
||||
nInu 1113.22A
|
||||
nFnu 1103.23A
|
||||
nInu 1103.23A
|
||||
nFnu 1073.86A
|
||||
nInu 1073.86A
|
||||
nFnu 1064.34A
|
||||
nInu 1064.34A
|
||||
nFnu 1035.92A
|
||||
nInu 1035.92A
|
||||
nFnu 1000.00A
|
||||
nInu 1000.00A
|
||||
nFnu 925.144A
|
||||
nInu 925.144A
|
||||
nFnu 897.800A
|
||||
nInu 897.800A
|
||||
nInu 760.023A
|
||||
nInu 701.514A
|
||||
nInu 608.160A
|
||||
nInu 575.146A
|
||||
nInu 511.948A
|
||||
nInu 496.874A
|
||||
nInu 399.153A
|
||||
nFnu 910.000A
|
||||
nInu 910.000A
|
||||
nFnu 913.000A
|
||||
nInu 913.000A
|
||||
nFnu 1650.00A
|
||||
nInu 1650.00A
|
||||
nFnu 1900.00A
|
||||
nInu 1900.00A
|
||||
nFnu 3644.00A # changed this wavelength bin
|
||||
nInu 3644.00A
|
||||
nFnu 3648.00A
|
||||
nInu 3648.00A
|
||||
nFnu 5100.00A
|
||||
nInu 5100.00A
|
||||
nFnu 6500.00A
|
||||
nInu 6500.00A
|
||||
nFnu 7000.00A
|
||||
nInu 7000.00A
|
||||
nFnu 7500.00A
|
||||
nInu 7500.00A
|
||||
nFnu 8000.00A
|
||||
nInu 8000.00A
|
||||
nFnu 8204.00A
|
||||
nInu 8204.00A
|
||||
nFnu 8207.00A
|
||||
nInu 8207.00A
|
||||
nFnu 8500.00A
|
||||
nInu 8500.00A
|
||||
nFnu 9000.00A
|
||||
nInu 9000.00A
|
||||
nFnu 9500.00A
|
||||
nInu 9500.00A
|
||||
nFnu 10000.0A
|
||||
nInu 10000.0A
|
||||
nFnu 1.05000m
|
||||
nInu 1.05000m
|
||||
nFnu 1.10000m
|
||||
nInu 1.10000m
|
@ -1,47 +0,0 @@
|
||||
how many did we have that don't converge
|
||||
|
||||
optical depth
|
||||
thermal structure
|
||||
|
||||
|
||||
dr. korista to talk about new version of cloudy availability
|
||||
|
||||
|
||||
AGN - other spectrum
|
||||
|
||||
want 10^22 10^23 10^24 with 18 15 15 models
|
||||
|
||||
get these results together ^
|
||||
|
||||
half decades would be good
|
||||
|
||||
numerical recipes
|
||||
|
||||
|
||||
try 45-degree interpolation
|
||||
|
||||
|
||||
|
||||
abundances?
|
||||
|
||||
envelope trend?
|
||||
|
||||
quasars are episode
|
||||
|
||||
|
||||
|
||||
seyfert --
|
||||
|
||||
|
||||
inward fraction of lines
|
||||
|
||||
|
||||
|
||||
|
||||
|
||||
define nfnu, ninu, inwC, inwT
|
||||
|
||||
|
||||
|
||||
|
||||
SED go out to 200KeV
|
@ -1,66 +0,0 @@
|
||||
This regards the multiplets about which we currently obtain information from Cloudy, indexed by TOTL. Specifically, the new way these are treated in Cloudy 15.
|
||||
|
||||
It appears C15 adds a new category of emission lines after "molecules" called "blends". It seems this has largely replaced the TOTL lines we are used to seeing, but there are some exceptions. For example, there is no longer any TOTL line around N III 1750. Here is the readout:
|
||||
|
||||
Inwd 860.205A 4.359 0.0033
|
||||
N 3 1748.65A 6.367 0.3378
|
||||
Inwd 1748.65A 6.150 0.2047
|
||||
N 3 1753.99A 6.381 0.3489
|
||||
Inwd 1753.99A 6.165 0.2118
|
||||
N 3 1746.82A 5.099 0.0182
|
||||
Inwd 1746.82A 4.866 0.0107
|
||||
N 3 1752.16A 5.935 0.1250
|
||||
Inwd 1752.16A 5.709 0.0742
|
||||
N 3 1749.67A 6.719 0.7598
|
||||
Inwd 1749.67A 6.519 0.4794
|
||||
N 3 989.799A 6.761 0.8374
|
||||
|
||||
Instead, presumably, there is a blend line near the relevant wavelength. listed in the blends section. Blended regions can also be accompanied by an inward component. For the N III example I found
|
||||
|
||||
Blnd 1750.00A 7.040 1.5897
|
||||
|
||||
In the blends section, Cloudy also outputs lines with more specific labels, often alongside similarly-located blends. For example:
|
||||
|
||||
Blnd 1657.00A 6.418 0.3794
|
||||
C 1R 1656.00A 6.361 0.3329
|
||||
Blnd 2326.00A 5.748 0.0811
|
||||
Blnd 1335.00A 7.737 7.9093
|
||||
C 2R 1335.00A 7.690 7.1108
|
||||
C 2P 3920.00A 4.311 0.0030
|
||||
Blnd 6580.00A 5.257 0.0262
|
||||
|
||||
My guess is these are physically-modelled multiplets displayed alongside some sort of continuum blending. I read in the "A Multiplet Table of Astrophysical Interest" about a certain type of blending, but the document is huge and I didn't delve far into it; besides, this could be another type of blend altogether, given what I know.
|
||||
|
||||
So, I'm not sure how we might make sense of a blend line alongside the thought of the TOTL in C13 (which is that the TOTL should represent the sum of the multiplet values). In the N III example, the sum of the quintuplet's values does match the blend value. For C I, however, it does not.
|
||||
|
||||
C 1 1656.27A 5.388 0.0354
|
||||
Inwd 1656.27A 5.380 0.0348
|
||||
C 1 1656.93A 5.390 0.0356
|
||||
Inwd 1656.93A 5.374 0.0343
|
||||
C 1 1657.01A 5.506 0.0465
|
||||
Inwd 1657.01A 5.520 0.0480
|
||||
C 1 1657.38A 5.354 0.0327
|
||||
Inwd 1657.38A 5.329 0.0310
|
||||
C 1 1657.91A 5.390 0.0356
|
||||
Inwd 1657.91A 5.374 0.0343
|
||||
C 1 1658.12A 5.417 0.0379
|
||||
Inwd 1658.12A 5.406 0.0369
|
||||
|
||||
(Sum = .2237)
|
||||
|
||||
Blnd 1657.00A 6.418 0.3794
|
||||
C 1R 1656.00A 6.361 0.3329
|
||||
|
||||
|
||||
The only places I found where TOTL lines still exist are in the general properties (i.e. TOTL 4861) and the He-like iso-sequence. For example,
|
||||
|
||||
TOTL 29.0840A 6.811 0.9375
|
||||
N 6 29.0840A 6.309 0.2957
|
||||
Inwd 29.0840A 6.528 0.4886
|
||||
N 6 29.0815A 3.848 0.0010
|
||||
Inwd 29.0815A 4.062 0.0017
|
||||
N 6 28.7870A 5.941 0.1266
|
||||
Inwd 28.7870A 6.062 0.1672
|
||||
|
||||
|
||||
This example does not sum properly, either. So, I really have no idea what's going on, here. But, as we mostly decided before, it shouldn't matter much for our current purposes.
|
@ -17,7 +17,7 @@ module load <module> (load a module)
|
||||
|
||||
For use in this guide, one need load the gcc module with the following command. If version 4.7.3 is no longer available, use module avail to find a compatible version of gcc. An MPI library must also be loaded.
|
||||
|
||||
module load gcc/4.7.3
|
||||
module load gcc/6.3.0
|
||||
module load openmpi/gnu/1.7.3
|
||||
|
||||
To utilize MPI functionality, Cloudy must be compiled with MPI support. Cloudy attempts to provide a simple interface through which to accomplish this. Cloudy provides a system of makefiles for compiling the software with many compatibilities. These makefiles are available under the subdirectories of the c13.03/source directory. In this case, sys_mpi_gcc should be used. Provided the gcc and MPI modules are loaded in a Thor environment, the following sequence should compile Cloudy with MPI support.
|
||||
@ -61,3 +61,8 @@ qstat
|
||||
The directory itself should fill up with input and output files for each point in the grid. Cloudy will clean and compile these into a single output file at the end.
|
||||
|
||||
Voila!
|
||||
|
||||
Some useful commands:
|
||||
|
||||
qnodes | grep -B2 research| less
|
||||
qstat
|
||||
|
@ -5,11 +5,10 @@
|
||||
int main(int argc, char const *argv[])
|
||||
{
|
||||
|
||||
if (agn::verbose)
|
||||
std::cout
|
||||
<< "Setting up environment.\n";
|
||||
|
||||
bool debug=true;
|
||||
|
||||
// Create 2d table using n bins, linear values of SED. The
|
||||
// agn em source class has a function for this. A
|
||||
// std::map<double,double> represents the table.
|
||||
@ -30,7 +29,7 @@ int main(int argc, char const *argv[])
|
||||
std::ofstream::out
|
||||
);
|
||||
|
||||
if(debug) std::cout
|
||||
if(agn::debug) std::cout
|
||||
<< "Debug mode.\n";
|
||||
|
||||
|
||||
@ -56,7 +55,7 @@ int main(int argc, char const *argv[])
|
||||
log_radius_in_cm
|
||||
);
|
||||
|
||||
if(debug) debug_file
|
||||
if(agn::debug) debug_file
|
||||
<< "cutoff_uv_eV: "
|
||||
<< agnsource._cutoff_uv_eV
|
||||
<< "\n"
|
||||
|
@ -8,7 +8,7 @@
|
||||
namespace agn {
|
||||
|
||||
// Continuum domain, step size constant in log space
|
||||
``const double CONT_MIN_ENERGY=1e-2; // eV
|
||||
const double CONT_MIN_ENERGY=1e-2; // eV
|
||||
const double CONT_MAX_ENERGY=1e5; // eV
|
||||
const double CONT_MIN_X=log10(CONT_MIN_ENERGY);
|
||||
const double CONT_MAX_X=log10(CONT_MAX_ENERGY);
|
||||
|
Loading…
Reference in New Issue
Block a user