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working on magdziarz sed program
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@ -84,7 +84,7 @@ timestamp color 1
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timestamp rot 0
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timestamp font 0
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timestamp char size 1.000000
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timestamp def "Wed Jun 1 02:40:17 2016"
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timestamp def "Wed Jun 1 12:59:43 2016"
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r0 off
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link r0 to g0
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r0 type above
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@ -131,7 +131,7 @@ g0 fixedpoint xy 0.000000, 0.000000
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g0 fixedpoint format general general
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g0 fixedpoint prec 6, 6
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with g0
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world 0.001, 1e-40, 1000, 10000
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world 0.001, 0.01, 100, 4
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stack world 0, 0, 0, 0
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znorm 1
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view 0.150000, 0.150000, 1.150000, 0.850000
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@ -205,7 +205,7 @@ with g0
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yaxis bar color 1
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yaxis bar linestyle 1
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yaxis bar linewidth 1.0
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yaxis label "nuFnu (erg / cm^2 / s )"
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yaxis label "Relative Value"
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yaxis label layout para
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yaxis label place auto
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yaxis label char size 1.000000
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@ -1,10 +1,7 @@
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#parents, babies = (1, 1)
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#while babies < 100:
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# #print 'This generation has {0} babies'.format(babies)
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# print('This generation has',babies,'babies.')
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# parents, babies = (babies, parents + babies)
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""" A program to recreate the average spectrum fit for ngc 5548 in Magdziarz et al 1998 """
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import math
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import scipy
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import numpy
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PI=3.14159265358979323846;
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PLANCK_CONST=4.135668e-15; # in eV * s
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@ -13,8 +10,8 @@ RYDBERG_CONST=1.0973731568539e7; # in 1 / m
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RYDBERG_UNIT_EV=13.60569252; # in eV
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RYDBERG_UNIT_ANGSTROM=1e10/RYDBERG_CONST; # in A
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CONT_MIN_ENERGY_keV = 1e-5; # eV
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CONT_MAX_ENERGY_keV = 1e2; # eV
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CONT_MIN_ENERGY_keV = 1e-3;
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CONT_MAX_ENERGY_keV = 1e2;
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CONT_MIN_X = math.log10(CONT_MIN_ENERGY_keV);
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CONT_MAX_X = math.log10(CONT_MAX_ENERGY_keV);
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CONT_WIDTH_X = CONT_MAX_X - CONT_MIN_X;
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@ -41,8 +38,8 @@ IN_EV_2500A = 12398.41929/2500;
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# Soft Excess
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α_SE = 1.1 # Quoted consistent with Korista 1995 and Marshall 1997
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kT_SE = .56
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α_SE_sec2_1 = 1.1 # Quoted consistent with Korista 1995 and Marshall 1997
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kT_SE_sec2_1 = .56
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# Comtonization fitted to ROSAT data
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@ -51,12 +48,17 @@ kT_SE = .56
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# OSSE data fit
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α_HC = 0.86
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R = 0.96
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E_cutoff_HC = 120 # keV, phase 1
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E_cutoff_HC = .120 # keV, phase 1
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F_HC = .38 # keV cm⁻² s⁻¹
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# E_cutoff_HC = 118 # keV, phase 3
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# F_HC = .61 # keV cm⁻² s⁻¹
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# Section 3.3 values
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kT_SE_sec3_2 = .270 # keV
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α_SE_sec3_2 = 1.13
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kT_HC_sec3_2 = 55 # keV
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α_HC_sec3_2 = .76
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@ -78,7 +80,7 @@ def histogram_table(n):
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output.append(value)
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# Add a final point at 100 KeV
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hν = 1e5;
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hν = 1e2;
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value = sed(hν);
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output.append((hν,value))
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return output;
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@ -86,6 +88,9 @@ def histogram_table(n):
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def sed(hν):
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magnitude=0.0;
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magnitude += powlaw_cutoff(hν,α_HC,E_cutoff_HC,1) # OSSE data fit
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# magnitude += powlaw_cutoff(hν,α_SE_sec2_1,kT_SE_sec2_1,1)
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# magnitude += powlaw_cutoff(hν,α_SE_sec3_2,kT_SE_sec3_2,1)
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#magnitude += compt_approx(hν,-1.3,.345,.0034,1)
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if magnitude < CONT_MIN_VAL: return CONT_MIN_VAL
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# magnitude = CONT_MIN_VAL;
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return magnitude;
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@ -94,13 +99,16 @@ def powlaw_cutoff(hν,α,E_cutoff,norm):
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low_cutoff = .1
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resultant = norm
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resultant *= math.exp(-hν/E_cutoff)
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resultant *= math.exp(-low_cutoff/hν)
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#resultant *= math.exp(-low_cutoff/hν)
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resultant *= math.pow(hν,1+α)
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return resultant
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# for t in (22.6, 25.8, 27.3, 29.8):+P B
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# print(t, ": ", fahrenheit(t))
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def compt_approx(hν,α,kT_keV,cutoff_keV,norm):
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magnitude = math.pow(hν,(1+α))
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magnitude *= math.exp(-(hν/kT_keV))
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magnitude *= math.exp(-(cutoff_keV/hν))
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magnitude *= norm
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return magnitude
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test_table = histogram_table(500)
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