| 1 | /////////////////////////////////////////////////////////////////////////
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| 2 | // Starfield Generator
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| 3 | //
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| 4 | // (c) 2000 D. Petry
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| 5 | //
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| 6 | // 15/09/2004, A. Moralejo:
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| 7 | // - Adapted to gcc 3.2 under root 3.05.07
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| 8 | // - Fixed algorithm to calculate director cosines of incident photons.
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| 9 | // Former algorithm resulted in mirrored images on the camera (which we
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| 10 | // must not have after reflection on a parabollic dish).
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| 11 | //
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| 12 | /////////////////////////////////////////////////////////////////////////
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| 13 |
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| 14 |
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| 15 | #include "starfield.h"
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| 16 |
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| 17 | #define PROGRAMID "$Id: starfield.cxx,v 1.4 2004-09-17 17:36:25 moralejo Exp $"
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| 18 |
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| 19 | /////////////////////////////////////////////////////////////////////////
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| 20 |
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| 21 | int main(int argc, char **argv)
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| 22 | {
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| 23 |
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| 24 | parameters pars;
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| 25 | star stars[iMAXSTARS];
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| 26 | photon *photons;
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| 27 |
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| 28 | ifstream in;
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| 29 | FILE *catfile;
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| 30 | char parfilename[160];
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| 31 | char catfilename[160];
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| 32 |
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| 33 |
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| 34 | int i, j, k, numstars, subnumstars, starnumber, totalnumphot, photinside;
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| 35 | int totalphotinside, idum;
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| 36 | int istart_ra_h, iend_ra_h;
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| 37 | int nph[4]; // numbers of photons in the four wavebands
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| 38 | float lmin_nm[4] = {ULMIN_nm, BLMIN_nm, VLMIN_nm, RLMIN_nm}; // wave band definitions
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| 39 | float lmax_nm[4] = {ULMAX_nm, BLMAX_nm, VLMAX_nm, RLMAX_nm};
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| 40 | float theta_rad, costheta, sintheta, phi_rad, randtime, lambda_nm, xdum_m, ydum_m;
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| 41 | float cosa, cosA, sinA;
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| 42 | float angdist;
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| 43 |
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| 44 | //welcome
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| 45 |
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| 46 | cout << "This is STARFIELD. (c) 2000 D. Petry\n";
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| 47 | cout << PROGRAMID << "\n";
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| 48 |
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| 49 | // check command line arguments
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| 50 |
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| 51 | if(argc == 1){
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| 52 | sprintf(parfilename, "starfield.par");
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| 53 | }
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| 54 | else{ // a filename was given
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| 55 | sprintf(parfilename, "%s", argv[1]);
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| 56 | }
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| 57 |
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| 58 | // read parameter file
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| 59 |
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| 60 | in.open(parfilename, ios::in); // open the parameter file
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| 61 |
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| 62 | if(!in){
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| 63 | cout << "Failed to open " << parfilename << "\n"
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| 64 | << "Value of stream \"in\" was " << in << "\n";
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| 65 | cout << "\nThere shoud be a parameter file "<< parfilename
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| 66 | <<" in the working directory with the following format:\n-----\n";
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| 67 | pars.usage(&cout);
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| 68 | cout << "-----\nExiting.\n";
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| 69 | exit(1);
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| 70 | }
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| 71 |
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| 72 | cout << "Opened " << parfilename << " for reading ...\n";
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| 73 |
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| 74 | if( !(pars.readparameters(&in)) ){ // read not OK?
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| 75 | if(!in.eof()){ // was the error not due to EOF?
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| 76 | cout << "Error: rdstate = " << in.rdstate() << "\n";
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| 77 | }
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| 78 | else{
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| 79 | cout << "Error: premature EOF in parameter file.\n";
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| 80 | }
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| 81 | exit(1);
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| 82 | }
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| 83 |
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| 84 | in.close();
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| 85 |
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| 86 | // Allocate memory for photons
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| 87 |
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| 88 | photons=new photon[iMAXPHOT];
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| 89 |
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| 90 |
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| 91 | // prepare loop over star catalog files
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| 92 |
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| 93 | cout << "SKY2000 - Master Star Catalog - Star Catalog Database, Version 2\n";
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| 94 | cout << "Sande C.B., Warren W.H.Jr., Tracewell D.A., Home A.T., Miller A.C.\n";
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| 95 | cout << "<Goddard Space Flight Center, Flight Dynamics Division (1998)>\n";
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| 96 |
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| 97 | angdist = fmod( (float) (pars.catalog_fov_deg/cos( pars.ct_dec_rad )),
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| 98 | (float) 360.);
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| 99 |
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| 100 | if(angdist > 180.){ // too near to the pole, have to loop over all files
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| 101 |
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| 102 | istart_ra_h = 0;
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| 103 | iend_ra_h = 23;
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| 104 |
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| 105 | }
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| 106 | else{ // can loop over selected files only
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| 107 |
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| 108 | istart_ra_h = (int) (pars.ct_ra_h - angdist / 360. * 24.) - 1;
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| 109 | iend_ra_h = (int) (pars.ct_ra_h + angdist / 360. * 24. ) + 1;
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| 110 |
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| 111 | }
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| 112 |
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| 113 | //read catalog
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| 114 |
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| 115 | i = 0;
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| 116 | for (j = istart_ra_h; j <= iend_ra_h; j++){
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| 117 |
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| 118 | subnumstars = 0;
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| 119 |
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| 120 | if ( j < 0){
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| 121 | idum = j + 24;
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| 122 | }
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| 123 | else if ( j > 23 ){
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| 124 | idum = j - 24;
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| 125 | }
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| 126 | else {
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| 127 | idum = j;
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| 128 | }
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| 129 |
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| 130 | sprintf(catfilename, "%s/sky%02d.dat", pars.datapath, idum);
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| 131 |
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| 132 | if((catfile = fopen(catfilename, "r")) == NULL){ // open the star catalog
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| 133 | cout << "Failed to open " << catfilename << "\n";
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| 134 | exit(1);
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| 135 | }
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| 136 | cout << "Opened file " << catfilename << " for reading ...\n";
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| 137 |
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| 138 | while( stars[i].readstar(catfile, pars.verbose) ){ // read next star OK
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| 139 |
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| 140 | angdist = acos( cos( pars.ct_dec_rad ) * cos( stars[i].dec_rad ) *
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| 141 | cos( stars[i].ra_rad - pars.ct_ra_rad ) +
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| 142 | sin( pars.ct_dec_rad ) * sin( stars[i].dec_rad ) );
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| 143 |
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| 144 | if( angdist < pars.catalog_fov_deg / 180. * PI ){ // star in Field Of View?
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| 145 |
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| 146 | stars[i].calcmissingmags(pars.verbose);
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| 147 | if (pars.verbose) stars[i].printstar();
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| 148 |
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| 149 | if( stars[i].umag > -100. ){
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| 150 | i++; // accept star
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| 151 | subnumstars++;
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| 152 | }
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| 153 | else{
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| 154 | cout << "Star rejected.\n";
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| 155 | }
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| 156 |
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| 157 | if( i > iMAXSTARS ){
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| 158 | i--;
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| 159 | cout << "Error: Star memory full. Accepted " << i << " stars.\n";
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| 160 | break;
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| 161 | }
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| 162 | }
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| 163 | }
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| 164 | if( feof(catfile) ){ // was EOF reached?
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| 165 | cout << "EOF reached; accepted "<< subnumstars << " stars from this segment.\n";
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| 166 | }
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| 167 | if( ferror(catfile) ){ // did an error occur?
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| 168 | cout << "Error while reading catalog file.\n";
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| 169 | exit(1);
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| 170 | }
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| 171 | fclose(catfile);
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| 172 | if(i == iMAXSTARS){
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| 173 | break;
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| 174 | }
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| 175 | }
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| 176 |
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| 177 | cout << "Accepted "<< i << " stars in total.\n";
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| 178 | numstars = i;
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| 179 |
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| 180 | // loop over all photons from all stars, filling their fields
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| 181 |
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| 182 | totalnumphot=0;
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| 183 |
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| 184 | totalphotinside=0;
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| 185 |
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| 186 | for(i=0; i<numstars;i++){
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| 187 |
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| 188 | starnumber=stars[i].icatnum;
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| 189 |
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| 190 | // calculate director cosines (see Montenbruck & Pfleger, 1989, p. 196)
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| 191 |
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| 192 | costheta = cos( pars.ct_dec_rad ) * cos( stars[i].dec_rad ) *
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| 193 | cos( stars[i].ra_rad - pars.ct_ra_rad ) +
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| 194 | sin( pars.ct_dec_rad ) * sin( stars[i].dec_rad );
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| 195 |
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| 196 | if(costheta == 0.){
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| 197 | cout << "Star number " << i << " (catalog number " << stars[i].icatnum <<
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| 198 | ") seems to be at 90 degrees distance from optical axis.\n ... will ignore it.";
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| 199 | continue;
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| 200 | }
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| 201 |
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| 202 | sintheta = sqrt(1.-costheta*costheta);
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| 203 |
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| 204 | //
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| 205 | // A. Moralejo, 15/09/2004
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| 206 | // We want the director cosines of the down-going versors along the photon
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| 207 | // incident directions. This is what the Reflector program expects (also from the
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| 208 | // normal Corsika output). We have used simple spherical trigonometry to obtain
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| 209 | // the formulae.
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| 210 | //
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| 211 |
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| 212 | // "cosa" is the cosine of the angle "a" between the star direction and the direction
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| 213 | // defined by declination = 0 and right ascension = ct_ra. "a" is one of the sides of
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| 214 | // a spherical triangle. It is a quantity needed for the calculations.
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| 215 |
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| 216 | cosa = cos( stars[i].ra_rad - pars.ct_ra_rad ) * cos( stars[i].dec_rad );
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| 217 |
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| 218 | // cosA is the angle between the great circle of constant right ascension = ct_ra and
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| 219 | // the great circle defined by the star direction and the telescope direction. "A" would
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| 220 | // be the angle opposite to the side "a" of a spherical triangle (see above)
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| 221 |
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| 222 | cosA = (cosa - costheta*cos(pars.ct_dec_rad)) / (sintheta*sin(pars.ct_dec_rad));
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| 223 |
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| 224 | // We now want A to be defined in the 0 - 2pi range, so that it becomes the azimuth angle
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| 225 | // of the star in a system defined by the telescope direction. "A" will be defined between
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| 226 | // 0 and pi if sin (star_ra - ct_ra) > 0, and between pi and 2 pi otherwise.
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| 227 |
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| 228 | sinA = sqrt (1.-cosA*cosA);
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| 229 | if ( sin(stars[i].ra_rad - pars.ct_ra_rad ) < 0. )
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| 230 | sinA *= -1.;
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| 231 |
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| 232 | stars[i].u = -1. * sintheta * cosA;
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| 233 | stars[i].v = -1. * sintheta * sinA;
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| 234 |
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| 235 |
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| 236 | // Old implementation, commented out 15/09/2004:
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| 237 | //
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| 238 | // This produced director cosines which, when fed to reflector, makes on the camera plane
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| 239 | // a mirror-inverted image of the FOV (with respect to what one would see "by eye"). That
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| 240 | // is NOT what we want! After reflection on the parabollic mirror, the image on the camera
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| 241 | // is NOT mirrored, but just rotated by 180 degree. The new implementation above produces
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| 242 | // the correct FOV (tested with Reflector 0.6)
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| 243 | //
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| 244 | // stars[i].u = -1. * cos( stars[i].dec_rad ) * sin( stars[i].ra_rad - pars.ct_ra_rad ) / costheta;
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| 245 | // stars[i].v = -1. * ( sin( pars.ct_dec_rad ) * cos( stars[i].dec_rad ) *
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| 246 | // cos( stars[i].ra_rad - pars.ct_ra_rad ) -
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| 247 | // cos( pars.ct_dec_rad ) * sin( stars[i].dec_rad )
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| 248 | // ) / costheta;
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| 249 |
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| 250 |
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| 251 | // calculate the "zenith angle" theta and "azimuth" phi of the star assuming
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| 252 | // the telecope points at the zenith
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| 253 | // take into account the ambiguity of acos()
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| 254 |
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| 255 | theta_rad = acos(costheta);
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| 256 |
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| 257 | if( stars[i].v >= 0. ){
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| 258 | phi_rad = acos(stars[i].u);
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| 259 | }
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| 260 | else{
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| 261 | phi_rad = 2.*PI - acos(stars[i].u);
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| 262 | }
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| 263 |
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| 264 | // calculate number of photons
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| 265 |
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| 266 | // mag_nphot() translates the star magnitude into number of photons,
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| 267 | // using the expression log(flux)=-0.4*m-22.42 for each waveband
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| 268 | // the resulting numbers ar stored in the array nph
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| 269 |
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| 270 | stars[i].mag_nphot(nph, pars.integtime_s, pars.mirr_radius_m, pars.verbose);
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| 271 |
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| 272 | // loop over all photons
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| 273 |
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| 274 | photinside=0;
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| 275 |
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| 276 | for(k=0; k < 4; k++){ // loop over wavebands
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| 277 |
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| 278 | for(j=0; j<nph[k]; j++){ // loop over photons of this waveband
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| 279 |
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| 280 | // Check if we have overflowed the alllowed ph number
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| 281 |
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| 282 | if(totalphotinside >= iMAXPHOT){
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| 283 | cout << "Warning: photon memory full. Can only store " << iMAXPHOT << " photons.\n";
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| 284 | break;
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| 285 | //exit(1);
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| 286 | }
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| 287 |
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| 288 | // for every photon, a pair of uniform random x,y coordinates ( x*x+y*y<300 ) is generated
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| 289 | // and a uniform random arrival time inside a time window given by the integration time.
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| 290 |
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| 291 | xdum_m=rand_coord(pars.mirr_radius_m);
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| 292 | ydum_m=rand_coord(pars.mirr_radius_m);
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| 293 |
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| 294 | if((xdum_m*xdum_m+ydum_m*ydum_m)<pars.mirr_radius_m*pars.mirr_radius_m){
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| 295 |
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| 296 | randtime = rand_time(pars.integtime_s);
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| 297 | lambda_nm = rand_lambda(lmin_nm[k], lmax_nm[k]);
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| 298 |
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| 299 | //fill the photon fields by using the member functions defined in photon.hxx
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| 300 |
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| 301 | photons[totalphotinside].starnum = starnumber;
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| 302 | photons[totalphotinside].arrtime_sec = randtime;
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| 303 | photons[totalphotinside].x_m = xdum_m;
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| 304 | photons[totalphotinside].y_m = ydum_m;
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| 305 | photons[totalphotinside].u = stars[i].u;
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| 306 | photons[totalphotinside].v = stars[i].v;
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| 307 | photons[totalphotinside].lambda_nm = lambda_nm;
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| 308 |
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| 309 | if(pars.verbose > 2)
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| 310 | cout << "PH " << starnumber << " " << randtime << " " << xdum_m << " "
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| 311 | << ydum_m << " " << stars[i].u << " " << stars[i].v << " " << lambda_nm
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| 312 | << "\n";
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| 313 |
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| 314 | photinside++;
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| 315 |
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| 316 | totalphotinside++;
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| 317 |
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| 318 | totalnumphot++;
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| 319 |
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| 320 | }
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| 321 | else{
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| 322 |
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| 323 | totalnumphot++;
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| 324 | continue;
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| 325 |
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| 326 | } // end if
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| 327 |
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| 328 | } // end photon loop
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| 329 | } // end waveband loop
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| 330 |
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| 331 | stars[i].numphot = photinside;
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| 332 | //if (i>81) break;
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| 333 | if (pars.verbose) cout<<"Star number= "<<i<< " (catalog number " <<
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| 334 | starnumber << ") Number of photons accepted = "<< photinside<<endl;
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| 335 |
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| 336 | } // end star loop
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| 337 |
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| 338 | cout << "Total number of photons accepted = " << totalphotinside << "\n";
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| 339 |
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| 340 | convertcorsika(
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| 341 | ((int)pars.ct_ra_h*10)*1000 + (int)(fabs(pars.ct_dec_deg)*10), // the file id
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| 342 | totalphotinside, photons, pars.integtime_s, pars.verbose, pars.output_file);
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| 343 |
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| 344 | return 0;
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| 345 |
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| 346 | } // end main
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