1 | #include "sopnamsp.h"
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2 | #include "machdefs.h"
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3 | #include <iostream>
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4 | #include <stdlib.h>
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5 | #include <stdio.h>
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6 | #include <string.h>
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7 | #include <math.h>
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8 | #include <unistd.h>
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9 |
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10 | #include "constcosmo.h"
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11 | #include "cosmocalc.h"
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12 | #include "geneutils.h"
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13 | #include "schechter.h"
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14 | #include "planckspectra.h"
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15 |
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16 | /* --- Check Peterson at al. astro-ph/0606104 v1 (pb facteur sqrt(2) sur S/N !)
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17 | cmvdefsurv -U 0.75,0.3,0.7,-1,1 -V 300 -z 0.0025,0.2,Z -x 1,90,A -O 400000,6000 -N 75 -M 6.156e9 -F 3 -2 1.5
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18 | --- */
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19 |
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20 | inline double rad2deg(double trad) {return trad/M_PI*180.;}
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21 | inline double rad2min(double trad) {return trad/M_PI*180.*60.;}
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22 | inline double rad2sec(double trad) {return trad/M_PI*180.*3600.;}
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23 | inline double deg2rad(double tdeg) {return tdeg*M_PI/180.;}
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24 | inline double min2rad(double tmin) {return tmin*M_PI/(180.*60.);}
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25 | inline double sec2rad(double tsec) {return tsec*M_PI/(180.*3600.);}
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26 |
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27 | void usage(void);
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28 | void usage(void) {
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29 | cout<<"cmvdefsurv [-r] -x adtx,atxlarg[,unit_x] -y adty,atylarg[,unit_y] -z dred,redlarg[,unit_z] redshift"<<endl
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30 | <<"----------------"<<endl
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31 | <<" -x adtx,atxlarg : resolution et largeur dans le plan transverse selon X"<<endl
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32 | <<" -y adty,atylarg : idem selon Y, si <=0 meme que X"<<endl
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33 | <<" -z dred,redlarg : resolution et largeur sur la ligne de visee"<<endl
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34 | <<"-- Unites pour X-Y:"<<endl
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35 | <<" \'A\' : en angles (pour X-Y) : resolution=ArcMin, largeur=Degre (defaut)"<<endl
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36 | <<" \'Z\' : en redshift (pour Z) : resolution et largeur en redshift (defaut)"<<endl
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37 | <<" \'F\' : en frequence (pour Z) : resolution et largeur MHz"<<endl
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38 | <<" \'M\' : en distance (pour X-Y-Z) : resolution et largeur Mpc"<<endl
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39 | <<"----------------"<<endl
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40 | <<" -O surf,tobs : surface effective (m^2) et temps d\'observation (s)"<<endl
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41 | <<" -N Tsys : temperature du system (K)"<<endl
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42 | <<" -L lobewidth,freqlob : taille du lobe d\'observation (FWHM) en arcmin (def= 1\')"<<endl
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43 | <<" pour la frequence freqlob en MHz"<<endl
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44 | <<" Si lobewidth<=0 : l'angle solide du lobe = celui du pixel"<<endl
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45 | <<" Si freqlob<=0 : la frequence de reference est celle du redshift etudie"<<endl
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46 | <<" Si freqlob absent : la frequence de reference 1.4 GHz"<<endl
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47 | <<" -2 : two polarisations measured"<<endl
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48 | <<" -M : masse de HI de reference (MSol), si <=0 mean schechter in pixel"<<endl
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49 | <<" -F : HI flux factor to be applied for our redshift"<<endl
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50 | <<" -V Vrot : largeur en vitesse (km/s) pour l\'elargissement doppler (def=300km/s)"<<endl
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51 | <<"----------------"<<endl
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52 | <<" -S Tsynch,indnu : temperature (K) synch a 408 Mhz, index d\'evolution"<<endl
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53 | <<" (indnu==0 no evolution with freq.)"<<endl
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54 | <<"----------------"<<endl
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55 | <<" -U h100,om0,ol0,w0,or0,flat : cosmology"<<endl
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56 | <<"----------------"<<endl
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57 | <<" -A <log10(S_agn)> : moyenne du flux AGN en Jy dans le pixel"<<endl
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58 | <<" redshift : redshift moyen du survey"<<endl
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59 | <<endl;
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60 | }
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61 |
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62 | int main(int narg,char *arg[])
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63 | {
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64 | // --- Valeurs fixes
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65 | // WMAP
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66 | unsigned short flat = 0;
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67 | double h100=0.71, om0=0.267804, or0=7.9e-05*0., ol0=0.73,w0=-1.;
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68 | // Schechter
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69 | double h75 = h100 / 0.75;
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70 | double nstar = 0.006*pow(h75,3.); //
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71 | double mstar = pow(10.,9.8/(h75*h75)); // MSol
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72 | double alpha = -1.37;
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73 | cout<<"nstar= "<<nstar<<" mstar="<<mstar<<" alpha="<<alpha<<endl;
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74 |
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75 | // --- Arguments
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76 | double adtx=0., atxlarg=0., dx=0.,txlarg=0.;
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77 | int nx=0; char unit_x = 'A';
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78 | double adty=-1., atylarg=-1., dy=0.,tylarg=0.;
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79 | int ny=0; char unit_y = 'A';
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80 | double dred=0., redlarg=0., dz=0.,tzlarg=0.;
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81 | int nz=0; char unit_z = 'Z';
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82 | double redshift = 0.;
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83 | double tobs = 6000., surfeff = 400000.;
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84 | // taille du lobe d'observation en arcmin pour la frequence
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85 | double lobewidth0 = -1., lobefreq0 = Fr_HyperFin_Par*1.e3;
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86 | double Tsys=75.;
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87 | // a 408 MHz (Haslam) + evol index a -2.6
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88 | double Tsynch408=60., nuhaslam=0.408, indnu = -2.6;
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89 | double mhiref = -1.; // reference Mass en HI (def integ schechter)
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90 | double hifactor = 1.;
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91 | double vrot = 300.; // largeur en vitesse (km/s) pour elargissement doppler
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92 | bool ya2polar = false;
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93 | double facpolar = 0.5; // si on mesure les 2 polars -> 1.0
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94 | double lflux_agn = -3.;
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95 |
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96 | // --- Decodage arguments
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97 | char c;
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98 | while((c = getopt(narg,arg,"h2x:y:z:N:S:O:M:F:V:U:L:A:")) != -1) {
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99 | switch (c) {
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100 | case 'x' :
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101 | sscanf(optarg,"%lf,%lf,%c",&adtx,&atxlarg,&unit_x);
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102 | break;
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103 | case 'y' :
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104 | sscanf(optarg,"%lf,%lf,%c",&adty,&atylarg,&unit_y);
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105 | break;
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106 | case 'z' :
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107 | sscanf(optarg,"%lf,%lf,%c",&dred,&redlarg,&unit_z);
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108 | break;
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109 | case 'O' :
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110 | sscanf(optarg,"%lf,%lf",&surfeff,&tobs);
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111 | break;
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112 | case 'L' :
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113 | sscanf(optarg,"%lf,%lf",&lobewidth0,&lobefreq0);
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114 | break;
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115 | case 'N' :
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116 | sscanf(optarg,"%lf",&Tsys);
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117 | break;
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118 | case 'S' :
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119 | sscanf(optarg,"%lf,%lf",&Tsynch408,&indnu);
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120 | break;
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121 | case 'M' :
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122 | sscanf(optarg,"%lf",&mhiref);
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123 | break;
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124 | case 'F' :
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125 | sscanf(optarg,"%lf",&hifactor);
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126 | break;
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127 | case 'V' :
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128 | sscanf(optarg,"%lf",&vrot);
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129 | break;
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130 | case 'U' :
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131 | sscanf(optarg,"%lf,%lf,%lf,%lf,%hu",&h100,&om0,&ol0,&w0,&flat);
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132 | break;
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133 | case '2' :
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134 | ya2polar = true;
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135 | facpolar = 1.0;
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136 | break;
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137 | case 'A' :
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138 | sscanf(optarg,"%lf",&lflux_agn);
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139 | break;
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140 | case 'h' :
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141 | default :
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142 | usage(); return -1;
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143 | }
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144 | }
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145 | if(optind>=narg) {usage(); return-1;}
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146 | sscanf(arg[optind],"%lf",&redshift);
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147 | if(redshift<=0.) {cout<<"Redshift "<<redshift<<" should be >0"<<endl; return -2;}
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148 |
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149 | // --- Initialisation de la Cosmologie
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150 | cout<<"\n>>>>\n>>>> Cosmologie generale\n>>>>"<<endl;
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151 | cout<<"h100="<<h100<<" Om0="<<om0<<" Or0="<<or0<<" Or0="
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152 | <<or0<<" Ol0="<<ol0<<" w0="<<w0<<" flat="<<flat<<endl;
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153 | cout<<"--- Cosmology for z = "<<redshift<<endl;
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154 | CosmoCalc univ(flat,true,2.*redshift);
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155 | double perc=0.01,dzinc=redshift/100.,dzmax=dzinc*10.; unsigned short glorder=4;
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156 | univ.SetInteg(perc,dzinc,dzmax,glorder);
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157 | univ.SetDynParam(h100,om0,or0,ol0,w0);
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158 | univ.Print(0.);
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159 | univ.Print(redshift);
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160 |
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161 | double dang = univ.Dang(redshift);
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162 | double dtrcom = univ.Dtrcom(redshift);
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163 | double dlum = univ.Dlum(redshift);
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164 | double dloscom = univ.Dloscom(redshift);
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165 | double dlosdz = univ.Dhubble()/univ.E(redshift);
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166 | cout<<"dang="<<dang<<" dlum="<<dlum<<" dtrcom="<<dtrcom
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167 | <<" dloscom="<<dloscom<<" dlosdz="<<dlosdz<<" Mpc"<<endl;
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168 |
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169 | cout<<"\n1\" -> "<<dang*sec2rad(1.)<<" Mpc = "<<dtrcom*sec2rad(1.)<<" Mpc com"<<endl;
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170 | cout<<"1\' -> "<<dang*min2rad(1.)<<" Mpc = "<<dtrcom*min2rad(1.)<<" Mpc com"<<endl;
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171 | cout<<"1d -> "<<dang*deg2rad(1.)<<" Mpc = "<<dtrcom*deg2rad(1.)<<" Mpc com"<<endl;
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172 |
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173 | cout<<"dz=1 -> "<<dlosdz<<" Mpc com"<<endl;
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174 |
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175 | cout<<"1 Mpc los com -> dz = "<<1./dlosdz<<endl;
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176 | cout<<"1 Mpc transv com -> "<<rad2sec(1./dtrcom)<<"\" = "
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177 | <<rad2min(1./dtrcom)<<" \' = "<<rad2deg(1./dtrcom)<<" d"<<endl;
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178 |
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179 | // --- Mise en forme dans les unites appropriees
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180 | cout<<"\n>>>>\n>>>> Geometrie\n>>>>"<<endl;
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181 | if(adty<=0. || atylarg<=0.) {adty=adtx; atylarg=atxlarg; unit_y=unit_x;}
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182 | cout<<"X values: resolution="<<adtx<<" largeur="<<atxlarg<<" unite="<<unit_x<<endl;
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183 | if(unit_x == 'A') {
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184 | nx = int(atxlarg*60./adtx+0.5);
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185 | adtx = min2rad(adtx); atxlarg = deg2rad(atxlarg);
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186 | dx = adtx*dtrcom; txlarg = dx*nx;
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187 | } else if(unit_x == 'M') {
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188 | nx = int(atxlarg/adtx+0.5);
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189 | dx = adtx; txlarg = atxlarg;
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190 | adtx = dx/dtrcom; atxlarg = adtx*nx;
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191 | } else {
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192 | cout<<"Unknown unit_x = "<<unit_x<<endl;
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193 | }
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194 | cout<<"Y values: resolution="<<adty<<" largeur="<<atylarg<<" unite="<<unit_y<<endl;
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195 | if(unit_y == 'A') {
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196 | ny = int(atylarg*60./adty+0.5);
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197 | adty = min2rad(adty); atylarg = deg2rad(atylarg);
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198 | dy = adty*dtrcom; tylarg = dy*ny;
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199 | } else if(unit_y == 'M') {
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200 | ny = int(atylarg/adty+0.5);
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201 | dy = adty; tylarg = atylarg;
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202 | adty = dy/dtrcom; atylarg = adty*ny;
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203 | } else {
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204 | cout<<"Unknown unit_y = "<<unit_y<<endl;
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205 | }
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206 | cout<<"Z values: resolution="<<dred<<" largeur="<<redlarg<<" unite="<<unit_z<<endl;
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207 | if(unit_z == 'Z') {
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208 | nz = int(redlarg/dred+0.5);
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209 | dz = dred*dlosdz; tzlarg = dz*nz;
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210 | } else if(unit_z == 'M') {
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211 | nz = int(redlarg/dred+0.5);
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212 | dz = dred; tzlarg = redlarg;
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213 | dred = dz/dlosdz; redlarg = dred*nz;
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214 | } else if(unit_z == 'F') {
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215 | nz = int(redlarg/dred+0.5);
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216 | dred = dred/(Fr_HyperFin_Par*1.e3)*pow(1.+redshift,2.); redlarg = dred*nz;
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217 | dz = dred*dlosdz; tzlarg = dz*nz;
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218 | } else {
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219 | cout<<"Unknown unit_z = "<<unit_z<<endl;
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220 | }
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221 |
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222 | double Npix = (double)nx*(double)ny*(double)nz;
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223 | double redlim[2] = {redshift-redlarg/2.,redshift+redlarg/2.};
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224 | if(redlim[0]<=0.)
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225 | {cout<<"Lower redshift limit "<<redlim[0]<<" should be >0"<<endl; return -3;}
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226 | double dtrlim[2] = {univ.Dtrcom(redlim[0]),univ.Dtrcom(redlim[1])};
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227 | double loslim[2] = {univ.Dloscom(redlim[0]), univ.Dloscom(redlim[1])};
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228 | double dlumlim[2] = {univ.Dlum(redlim[0]),univ.Dlum(redlim[1])};
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229 |
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230 | cout<<"---- Line of Sight: Redshift = "<<redshift<<endl
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231 | <<"dred = "<<dred<<" redlarg = "<<redlarg<<endl
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232 | <<" dz = "<<dz<<" Mpc redlarg = "<<tzlarg<<" Mpc com, nz = "<<nz<<" pix"<<endl;
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233 | cout<<"---- Transverse X:"<<endl
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234 | <<"adtx = "<<rad2min(adtx)<<"\', atxlarg = "<<rad2deg(atxlarg)<<" d"<<endl
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235 | <<" dx = "<<dx<<" Mpc, txlarg = "<<txlarg<<" Mpc com, nx = "<<nx<<" pix"<<endl;
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236 | cout<<"---- Transverse Y:"<<endl
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237 | <<"adty = "<<rad2min(adty)<<"\', atylarg = "<<rad2deg(atylarg)<<" d"<<endl
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238 | <<" dy = "<<dy<<" Mpc, tylarg = "<<tylarg<<" Mpc com, ny = "<<ny<<" pix"<<endl;
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239 | cout<<"---- Npix total = "<<Npix<<" -> "<<Npix*sizeof(double)/1.e6<<" Mo"<<endl;
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240 |
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241 | // --- Cosmolographie Transverse
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242 | cout<<"\n>>>>\n>>>> Cosmologie & Geometrie transverse\n>>>>"<<endl;
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243 | cout<<"dang comoving = "<<dtrcom<<" Mpc (com) var_in_z ["
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244 | <<dtrlim[0]<<","<<dtrlim[1]<<"]"<<endl;
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245 |
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246 | cout<<"... dx = "<<dx<<" Mpc (com), with angle "<<adtx*dtrcom<<endl
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247 | <<" with angle var_in_z ["<<adtx*dtrlim[0]<<","<<adtx*dtrlim[1]<<"]"<<endl;
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248 | cout<<"... largx = "<<txlarg<<" Mpc (com), with angle "<<atxlarg*dtrcom<<endl
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249 | <<" with angle var_in_z ["<<atxlarg*dtrlim[0]<<","<<atxlarg*dtrlim[1]<<"]"<<endl;
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250 |
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251 | cout<<"... dy = "<<dy<<" Mpc (com), with angle "<<adty*dtrcom<<endl
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252 | <<" with angle var_in_z ["<<adty*dtrlim[0]<<","<<adty*dtrlim[1]<<"]"<<endl;
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253 | cout<<"... largy = "<<tylarg<<" Mpc (com), with angle "<<atylarg*dtrcom<<endl
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254 | <<" with angle var_in_z ["<<atylarg*dtrlim[0]<<","<<atylarg*dtrlim[1]<<"]"<<endl;
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255 |
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256 | // --- Cosmolographie Line of sight
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257 | cout<<"\n>>>>\n>>>> Cosmologie & Geometrie ligne de visee\n>>>>"<<endl;
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258 | cout<<"los comoving distance = "<<dloscom<<" Mpc (com) in ["
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259 | <<loslim[0]<<","<<loslim[1]<<"]"<<endl
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260 | <<" diff = "
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261 | <<loslim[1]-loslim[0]<<" Mpc"<<endl;
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262 |
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263 | cout<<"...dz = "<<dz<<" Mpc (com), with redshift approx "<<dred*dlosdz<<endl;
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264 | cout<<"...tzlarg = "<<tzlarg<<" Mpc (com), with redshift approx "<<redlarg*dlosdz<<endl;
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265 |
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266 | // --- Solid Angle & Volume
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267 | cout<<"\n>>>>\n>>>> Angles solides et Volumes\n>>>>"<<endl;
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268 | cout<<"--- Solid angle"<<endl;
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269 | double angsol = AngSol(adtx/2.,adty/2.,M_PI/2.);
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270 | cout<<"Elementary solid angle = "<<angsol<<" sr = "<<angsol/(4.*M_PI)<<" *4Pi sr"<<endl;
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271 | double angsoltot = AngSol(atxlarg/2.,atylarg/2.,M_PI/2.);
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272 | cout<<"Total solid angle = "<<angsoltot<<" sr = "<<angsoltot/(4.*M_PI)<<" *4Pi sr"<<endl;
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273 |
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274 | cout<<"\n--- Volume"<<endl;
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275 | double dvol = dx*dy*dz;
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276 | cout<<"Pixel volume comoving = "<<dvol<<" Mpc^3"<<endl;
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277 | double vol = univ.Vol4Pi(redlim[0],redlim[1])/(4.*M_PI)*angsoltot;
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278 | cout<<"Volume comoving = "<<vol<<" Mpc^3 = "<<vol/1.e9<<" Gpc^3"<<endl
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279 | <<"Pixel volume comoving = vol/Npix = "<<vol/Npix<<" Mpc^3"<<endl;
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280 |
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281 | // --- Fourier space: k = omega = 2*Pi*Nu
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282 | cout<<"\n>>>>\n>>>> Geometrie dans l'espace de Fourier\n>>>>"<<endl;
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283 | cout<<"Array size: nx = "<<nx<<", ny = "<<ny<<", nz = "<<nz<<endl;
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284 | double dk_x = 2.*M_PI/(nx*dx), knyq_x = M_PI/dx;
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285 | double dk_y = 2.*M_PI/(nx*dy), knyq_y = M_PI/dy;
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286 | double dk_z = 2.*M_PI/(nz*dz), knyq_z = M_PI/dz;
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287 | cout<<"Resolution: dk_x = "<<dk_x<<" Mpc^-1 (2Pi/dk_x="<<2.*M_PI/dk_x<<" Mpc)"<<endl
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288 | <<" dk_y = "<<dk_y<<" Mpc^-1 (2Pi/dk_y="<<2.*M_PI/dk_y<<" Mpc)"<<endl;
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289 | cout<<"Nyquist: kx = "<<knyq_x<<" Mpc^-1 (2Pi/knyq_x="<<2.*M_PI/knyq_x<<" Mpc)"<<endl
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290 | <<" ky = "<<knyq_y<<" Mpc^-1 (2Pi/knyq_y="<<2.*M_PI/knyq_y<<" Mpc)"<<endl;
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291 | cout<<"Resolution: dk_z = "<<dk_z<<" Mpc^-1 (2Pi/dk_z="<<2.*M_PI/dk_z<<" Mpc)"<<endl;
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292 | cout<<"Nyquist: kz = "<<knyq_z<<" Mpc^-1 (2Pi/knyq_z="<<2.*M_PI/knyq_z<<" Mpc)"<<endl;
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293 |
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294 | // --- Masse de HI
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295 | cout<<"\n>>>>\n>>>> Mass HI\n>>>>"<<endl;
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296 | Schechter sch(nstar,mstar,alpha);
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297 | sch.SetOutValue(1);
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298 | cout<<"nstar= "<<nstar<<" mstar="<<mstar<<" alpha="<<alpha<<endl;
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299 | cout<<"mstar*sch(mstar) = "<<sch(mstar)<<" Msol/Mpc^3/Msol"<<endl;
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300 | int npt = 10000;
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301 | double lnx1=log10(1e-6), lnx2=log10(1e+14), dlnx=(lnx2-lnx1)/npt;
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302 | double masshimpc3 = IntegrateFuncLog(sch,lnx1,lnx2,0.001,dlnx,10.*dlnx,6);
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303 | cout<<"Mass density: "<<masshimpc3<<" Msol/Mpc^3"<<endl;
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304 |
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305 | double masshipix = masshimpc3*dvol;
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306 | double masshitot = masshimpc3*vol;
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307 | cout<<"Pixel mass = "<<masshipix<<" Msol"<<endl
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308 | <<"Total mass in survey = "<<masshitot<<" Msol"<<endl;
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309 | if(mhiref<=0.) mhiref = masshipix;
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310 |
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311 | // --- Survey values
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312 | cout<<"\n>>>>\n>>>> Observations\n>>>>"<<endl;
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313 | double unplusz = 1.+redshift;
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314 | double nuhiz = Fr_HyperFin_Par / unplusz; // GHz
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315 | // dnu = NuHi/(1.+z0-dz/2) - NuHi/(1.+z0+dz/2)
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316 | // = NuHi*dz/(1.+z0)^2 * 1/[1-(dz/(2*(1+z0)))^2]
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317 | // ~= NuHi*dz/(1.+z0)^2
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318 | double dnuhiz = Fr_HyperFin_Par *dred/(unplusz*unplusz)
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319 | / (1.- pow(dred/.2/unplusz,2.));
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320 | cout<<" surf_eff="<<surfeff<<" m^2, tobs="<<tobs<<" s"<<endl
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321 | <<" nu="<<nuhiz<<" GHz, dnu="<<dnuhiz*1.e3<<" Mhz"<<endl;
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322 | cout<<"dang lumi = "<<dlum<<" in ["<<dlumlim[0]<<","<<dlumlim[1]<<"] Mpc"<<endl;
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323 |
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324 | double nlobes = 1.;
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325 | if(lobewidth0>0.) {
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326 | double lobewidth = lobewidth0; // ArcMin
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327 | if(lobefreq0<=0.) lobefreq0 = nuhiz*1.e3; // MHz
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328 | // La taille angulaire du lobe change avec la frequence donc avec le redshift
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329 | lobewidth *= lobefreq0/(nuhiz*1.e3);
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330 | cout<<"\n--- Lobe: width="<<lobewidth0<<" pour "<<lobefreq0<<" MHz"<<endl
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331 | <<" changed to "<<lobewidth<<" pour "<<nuhiz*1.e3<<" MHz"<<endl;
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332 | double slobe = lobewidth/2.35482; // sigma du lobe en arcmin
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333 | double lobecyl = sqrt(8.)*slobe; // diametre du lobe cylindrique equiv en arcmin
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334 | double lobearea = M_PI*lobecyl*lobecyl/4.; // en arcmin^2 (hypothese lobe gaussien)
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335 | nlobes = rad2min(adtx)*rad2min(adty)/lobearea;
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336 | cout<<"Beam FWHM = "<<lobewidth<<"\' -> sigma = "<<slobe<<"\' -> "
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337 | <<" Dcyl = "<<lobecyl<<"\' -> area = "<<lobearea<<" arcmin^2"<<endl;
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338 | cout<<"Number of beams in one transversal pixel = "<<nlobes<<endl;
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339 | }
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340 |
|
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341 | // --- Power emitted by HI
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342 | cout<<"\n--- Power from HI for M = "<<mhiref<<" Msol at "<<nuhiz<<" GHz"<<endl;
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343 | cout<<"flux factor = "<<hifactor<<" at redshift = "<<redshift<<endl;
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344 |
|
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345 | double fhi = hifactor*Msol2FluxHI(mhiref,dlum);
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346 | cout<<"FluxHI("<<dlum<<" Mpc) all polar:"<<endl
|
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347 | <<" Flux= "<<fhi<<" W/m^2 = "<<fhi/Jansky2Watt_cst<<" Jy.Hz"<<endl
|
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348 | <<" in ["<<hifactor*Msol2FluxHI(mhiref,dlumlim[0])
|
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349 | <<","<<hifactor*Msol2FluxHI(mhiref,dlumlim[1])<<"] W/m^2"<<endl;
|
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350 | double sfhi = fhi / (dnuhiz*1e9) / Jansky2Watt_cst;
|
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351 | cout<<"If spread over pixel depth ("<<dnuhiz<<" GHz), flux density = "<<sfhi<<" Jy"<<endl;
|
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352 |
|
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353 | // --- Signal analysis
|
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354 | cout<<"\n--- Signal analysis"<<endl;
|
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355 | cout<<"Facteur polar = "<<facpolar<<endl;
|
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356 |
|
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357 | PlanckSpectra planck(T_CMB_Par);
|
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358 | planck.SetApprox(1); // Rayleigh spectra
|
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359 | planck.SetVar(0); // frequency
|
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360 | planck.SetUnitOut(0); // output en W/....
|
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361 | planck.SetTypSpectra(0); // radiance W/m^2/Sr/Hz
|
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362 |
|
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363 | // Signal
|
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364 | double psig_2polar = fhi * surfeff;
|
---|
365 | double tsig_2polar = psig_2polar / k_Boltzman_Cst / (dnuhiz*1e9);
|
---|
366 | double ssig_2polar = psig_2polar / surfeff / (dnuhiz*1e9) / Jansky2Watt_cst;
|
---|
367 | double psig = facpolar * psig_2polar;
|
---|
368 | double tsig = facpolar * tsig_2polar;
|
---|
369 | double ssig = facpolar * ssig_2polar;
|
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370 | cout<<"\nSignal("<<mhiref<<" Msol): P="<<psig<<" W"<<endl;
|
---|
371 | cout<<" flux density = "<<ssig<<" Jy (for Dnu="<<dnuhiz<<" GHz)"<<endl;
|
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372 | cout<<" Antenna temperature: tsig="<<tsig<<" K"<<endl;
|
---|
373 |
|
---|
374 | // Elargissement doppler de la raie a 21cm: dNu = vrot/C * Nu(21cm) / (1+z)
|
---|
375 | double doplarge = vrot / SpeedOfLight_Cst * nuhiz;
|
---|
376 | double dzvrot = vrot / SpeedOfLight_Cst * unplusz;
|
---|
377 | cout<<" Doppler width="<<doplarge*1.e3<<" MHz for rotation width of "<<vrot<<" km/s"<<endl
|
---|
378 | <<" dx= "<<dzvrot<<" a z="<<redshift<<endl;
|
---|
379 | if(doplarge>dnuhiz)
|
---|
380 | cout<<"Warning: doppler width "<<doplarge<<" GHz > "<<dnuhiz<<" GHz redshift bin width"<<endl;
|
---|
381 |
|
---|
382 | // Synchrotron (T en -2.7 -> Flux en -0.7 dans l'approximation Rayleigh)
|
---|
383 | double tsynch = Tsynch408;
|
---|
384 | if(fabs(indnu)>1.e-50) tsynch *= pow(nuhiz/nuhaslam,indnu);
|
---|
385 | planck.SetTemperature(tsynch);
|
---|
386 | double psynch_2polar = planck(nuhiz*1.e+9) * surfeff * angsol * (dnuhiz*1e9);
|
---|
387 | double ssynch_2polar = psynch_2polar / surfeff / (dnuhiz*1e9) / Jansky2Watt_cst;
|
---|
388 | double psynch = facpolar * psynch_2polar;
|
---|
389 | double ssynch = facpolar * ssynch_2polar;
|
---|
390 | cout<<"\nSynchrotron: T="<<Tsynch408<<" K ("<<nuhaslam<<" GHz), "
|
---|
391 | <<tsynch<<" K ("<<nuhiz<<" GHz)"<<endl
|
---|
392 | <<" P="<<psynch<<" W for pixel"<<endl;
|
---|
393 | cout<<" flux density = "<<ssynch<<" Jy for pixel solid angle"<<endl;
|
---|
394 |
|
---|
395 | // CMB
|
---|
396 | double tcmb = T_CMB_Par;
|
---|
397 | planck.SetTemperature(tcmb);
|
---|
398 | double pcmb_2polar = planck(nuhiz*1.e+9) * surfeff * angsol * (dnuhiz*1e9);
|
---|
399 | double scmb_2polar = pcmb_2polar / surfeff / (dnuhiz*1.e+9) / Jansky2Watt_cst;
|
---|
400 | double pcmb = facpolar * pcmb_2polar;
|
---|
401 | double scmb = facpolar * scmb_2polar;
|
---|
402 | cout<<"\nCMB: T="<<tcmb<<" K -> P="<<pcmb<<" W for pixel"<<endl;
|
---|
403 | cout<<" flux density = "<<scmb<<" Jy for pixel solid angle"<<endl;
|
---|
404 |
|
---|
405 | // AGN
|
---|
406 | double flux_agn = pow(10.,lflux_agn);
|
---|
407 | double mass_agn = FluxHI2Msol(flux_agn*Jansky2Watt_cst,dlum);
|
---|
408 | cout<<"\nAGN: log10(S_agn)="<<lflux_agn<<" -> S_agn="
|
---|
409 | <<flux_agn<<" Jy -> "<<mass_agn<<" equiv. Msol/Hz"<<endl;
|
---|
410 | double flux_agn_pix = flux_agn*(dnuhiz*1e9);
|
---|
411 | double mass_agn_pix = FluxHI2Msol(flux_agn_pix*Jansky2Watt_cst,dlum);
|
---|
412 | double lmass_agn_pix = log10(mass_agn_pix);
|
---|
413 | cout<<"...pixel: f="<<flux_agn_pix<<" 10^-26 W/m^2"
|
---|
414 | <<" -> "<<mass_agn_pix<<" Msol -> log10 = "<<lmass_agn_pix<<endl;
|
---|
415 |
|
---|
416 | // =====================================================================
|
---|
417 | // ---
|
---|
418 | // --- Noise analysis
|
---|
419 | // ---
|
---|
420 | // --- Puissance du bruit pour un telescope de surface Ae et de BW dNu
|
---|
421 | // Par definition la puissance du bruit est:
|
---|
422 | // Pb = k * Tsys * dNu (W)
|
---|
423 | // Pour une source (non-polarisee) de densite de flux (totale 2 polars)
|
---|
424 | // St (exprimee en Jy=W/m^2/Hz)
|
---|
425 | // Pt = St * Ae * dNu (puissance totale emise en W pour 2 polars)
|
---|
426 | // P1 = 1/2 * St * Ae * dNu (puissance emise en W pour une polar)
|
---|
427 | // la SEFD (system equivalent flux density en Jy) est definie comme
|
---|
428 | // la densite de flux total (2 polars) "St" d'une source (non-polarisee)
|
---|
429 | // dont la puissance P1 mesuree pour une seule polarisation
|
---|
430 | // serait egale a la puissance du bruit. De P1 = Pb on deduit:
|
---|
431 | // SEFD = 2 * k * Tsys / Ae (en Jy)
|
---|
432 | // la puissance du bruit est: Pb = 1/2 * SEFD * Ae * dNu (en W)
|
---|
433 | // la sensibilite Slim tient compte du temps d'integration et de la BW:
|
---|
434 | // le nombre de mesures independantes est "2*dNu*Tobs" donc
|
---|
435 | // Slim = SEFD / sqrt(2*dNu*Tobs) = 2*k*Tsys/[Ae*sqrt(2*dNu*Tobs) (en Jy)
|
---|
436 | // --- Puissance du bruit pour un interferometre
|
---|
437 | // Ae = surface d'un telescope elementaire
|
---|
438 | // N = nombre de telescopes dans l'interferometre (Atot = N*Ae)
|
---|
439 | // La sensibilite Slim en Jy est:
|
---|
440 | // Slim = 2 * k * Tsys / [ Ae * Sqrt(2*N(N-1)/2 *dnu*Tobs) ]
|
---|
441 | // = 2 * k * Tsys / [ Atot/N * Sqrt(2*N(N-1)/2*dnu*Tobs) ]
|
---|
442 | // = 2 * k * Tsys / [ Atot * Sqrt((N-1)/N *dnu*Tobs) ]
|
---|
443 | // - Interferometre a deux antennes:
|
---|
444 | // Slim = 2 * k * Tsys / [ Atot * Sqrt(1/2 *dnu*Tobs) ]
|
---|
445 | // - Interferometre a N antennes (N grand):
|
---|
446 | // Slim -> 2 * k * Tsys / [ Atot * Sqrt(dnu*Tobs) ]
|
---|
447 | // C'est aussi la formule pour un telescope unique de surface Atot
|
---|
448 | // --- On ne mesure qu'une seule polarisation
|
---|
449 | // Ces formules sont valables si on mesure 1 polarisation:
|
---|
450 | // Slim est la densite de flux total "St" (2 polars) d'une source (non-polarisee)
|
---|
451 | // qui donne la meme puissance que le bruit dans un detecteur qui ne
|
---|
452 | // mesure qu'une seule polarisation:
|
---|
453 | // Le rapport S/N pour une source de densite de flux St (totale 2 polars):
|
---|
454 | // S/N = St / Slim
|
---|
455 | // La puissance de bruit est, par definition:
|
---|
456 | // Pb = 1/2 *Slim*Atot*dNu
|
---|
457 | // = k*Tsys*sqrt(2*dNu/Tobs) pour N=2
|
---|
458 | // = k*Tsys*sqrt(dNu/Tobs) pour N>>grand
|
---|
459 | // La densite de flux d'une source a S/N=1 est:
|
---|
460 | // St = Slim
|
---|
461 | // La puissance d'une source a S/N=1 mesuree par un detecteur
|
---|
462 | // qui ne mesure qu'une polar est:
|
---|
463 | // P1_lim = 1/2 *Slim*Atot*dNu
|
---|
464 | // --- On mesure les 2 polarisations avec deux voies d'electronique distinctes
|
---|
465 | // la puissance du signal mesure est multipliee par 2
|
---|
466 | // la puissance du bruit est multipliee par sqrt(2)
|
---|
467 | // on a donc un gain d'un facteur sqrt(2) sur le rapport S/N
|
---|
468 | // (cela revient d'ailleur a doubler le temps de pose: Tobs -> 2*Tobs)
|
---|
469 | // En notant arbitrairement: Slim' = Slim / sqrt(2)
|
---|
470 | // ou Slim est defini par les formules ci-dessus
|
---|
471 | // Le rapport S/N pour une source de densite de flux St (totale 2 polars):
|
---|
472 | // (S/N)_2 = (S/N)_1 * sqrt(2) = (St / Slim) * sqrt(2) = St / Slim'
|
---|
473 | // La densite de flux d'une source a S/N=1 est:
|
---|
474 | // St = Slim' = Slim / sqrt(2)
|
---|
475 | // La puissance d'une source a S/N=1 cumulee par les 2 detecteurs est:
|
---|
476 | // P_lim = St*Atot*dNu = Slim'*Atot*dNu = 1/sqrt(2) *Slim*Atot*dNu
|
---|
477 | // = P1_lim * sqrt(2)
|
---|
478 | // La puissance de bruit cumulee par les 2 detecteurs est, par definition:
|
---|
479 | // Pb = P_lim = Slim'*Atot*dNu = P1_lim * sqrt(2)
|
---|
480 | // = 2*k*Tsys*sqrt(dNu/Tobs) pour N=2
|
---|
481 | // = k*Tsys*sqrt(2*dNu/Tobs) pour N>>grand
|
---|
482 | // =====================================================================
|
---|
483 |
|
---|
484 | cout<<"\n---\n--- Noise analysis \n---"<<endl;
|
---|
485 | double psys = k_Boltzman_Cst * Tsys * (dnuhiz*1.e+9);
|
---|
486 | cout<<"Noise: T="<<Tsys<<" K, P="<<psys<<" W (for Dnu="<<dnuhiz<<" GHz)"<<endl;
|
---|
487 |
|
---|
488 | cout<<"...Computation assume that noise dominate the signal."<<endl;
|
---|
489 | if(ya2polar)
|
---|
490 | cout<<"...Assuming 2 polarisations measurements with 2 different electronics."<<endl;
|
---|
491 |
|
---|
492 | double slim,slim_nl,SsN,SsN_nl,smass,smass_nl;
|
---|
493 |
|
---|
494 | //---
|
---|
495 | for(unsigned short it=0;it<2;it++) {
|
---|
496 |
|
---|
497 | double fac = 1.;
|
---|
498 | if(it==0) { // Interferometre a 2 telescopes
|
---|
499 | fac = 0.5;
|
---|
500 | cout<<"\n...Observation limits for a 2 telescope interferometer (with complex correlator)"<<endl
|
---|
501 | <<" (sensitivity is given for real or complex correlator output)"<<endl;
|
---|
502 | } else if (it==1) { // Interferometre a N>> telescopes
|
---|
503 | fac = 1.;
|
---|
504 | cout<<"\n...Observation limits for a N (large) telescope interferometer (with complex correlator)"<<endl
|
---|
505 | <<" (weak source limit sensitivity in a synthetised image)"<<endl
|
---|
506 | <<" Also valid for a single dish telescope."<<endl;
|
---|
507 | } else continue;
|
---|
508 |
|
---|
509 | slim = 2. * k_Boltzman_Cst * Tsys / surfeff
|
---|
510 | / sqrt(fac*(dnuhiz*1.e+9)*tobs) /Jansky2Watt_cst;
|
---|
511 | if(ya2polar) slim /= sqrt(2.);
|
---|
512 | SsN = ssig_2polar / slim;
|
---|
513 | smass = mhiref / ssig_2polar * slim;
|
---|
514 | cout<<"for 1 lobe:"<<endl
|
---|
515 | <<" Slim = "<<slim<<" Jy"<<endl
|
---|
516 | <<" S/N = "<<SsN<<endl
|
---|
517 | <<" Mass HI = "<<smass<<" Msol"<<endl;
|
---|
518 |
|
---|
519 | slim_nl = slim * sqrt(nlobes);
|
---|
520 | SsN_nl = ssig_2polar / slim_nl;
|
---|
521 | smass_nl = mhiref / ssig_2polar * slim_nl;
|
---|
522 | cout<<"for "<<nlobes<<" lobes:"<<endl
|
---|
523 | <<" Flux = "<<slim_nl<<" Jy"<<endl
|
---|
524 | <<" S/N = "<<SsN_nl<<endl
|
---|
525 | <<" Mass HI = "<<smass_nl<<" Msol"<<endl;
|
---|
526 |
|
---|
527 | }
|
---|
528 |
|
---|
529 | return 0;
|
---|
530 | }
|
---|