root/branches/newmole/source/atom_feii.cpp
| Revision 2582, 91.9 kB (checked in by rporter, 2 weeks ago) | |
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| 1 | /* This file is part of Cloudy and is copyright (C)1978-2008 by Gary J. Ferland and |
| 2 | * others. For conditions of distribution and use see copyright notice in license.txt */ |
| 3 | /*FeII_Colden maintain H2 column densities within X */ |
| 4 | /*FeIILevelPops main FeII routine, called by CoolIron to evaluate iron cooling */ |
| 5 | /*FeIICreate read in needed data from file |
| 6 | * convert form of FeII data, as read in from file within routine FeIICreate |
| 7 | * into physical form. called by atmdat_readin */ |
| 8 | /*FeIIPunPop - punch level populations */ |
| 9 | /*AssertFeIIDep called by assert FeII depart coef command */ |
| 10 | /*FeIIPrint print FeII information */ |
| 11 | /*FeIICollRatesBoltzmann evaluate collision strenths, |
| 12 | * both interpolating on r-mat and creating g-bar |
| 13 | * find Boltzmann factors, evaluate collisional rate coefficients */ |
| 14 | /*FeIIPrint print output from large FeII atom, called by prtzone */ |
| 15 | /*FeIISumBand sum up large FeII emission over certain bands, called in lineset4 */ |
| 16 | /*FeII_RT_TauInc called once per zone in RT_tau_inc to increment large FeII atom line optical depths */ |
| 17 | /*FeII_RT_tau_reset reset optical depths for large FeII atom, called by update after each iteration */ |
| 18 | /*FeIIPoint called by ContCreatePointers to create pointers for lines in large FeII atom */ |
| 19 | /*FeIIAccel called by rt_line_driving to compute radiative acceleration due to FeII lines */ |
| 20 | /*FeIIAddLines save accumulated FeII intensities called by lineset4 */ |
| 21 | /*FeIIPunchLines punch FeII lines at end of calculation, if punch verner set, called by punch_do*/ |
| 22 | /*FeIIPunchOpticalDepth punch FeII line optical depth at end of calculation, called by punch_do*/ |
| 23 | /*FeIIPunchLevels punch FeII levels and energies */ |
| 24 | /*FeII_LineZero zero out storage for large FeII atom, called by tauout */ |
| 25 | /*FeIIIntenZero zero out intensity of FeII atom */ |
| 26 | /*FeIIZero initialize some variables, called by zero one time before commands parsed */ |
| 27 | /*FeIIReset reset some variables, called by zero */ |
| 28 | /*FeIIPunData punch line data */ |
| 29 | /*FeIIPunDepart punch some departure coef for large atom, |
| 30 | * set with punch FeII departure command*/ |
| 31 | /*FeIIPun1Depart send the departure coef for physical level nPUN to unit ioPUN */ |
| 32 | /*FeIIContCreate create FeII continuum bins to add lines into ncell cells between wavelengths lambda low and high, |
| 33 | * returns number of cells used */ |
| 34 | /*FeIIBandsCreate returns number of FeII bands */ |
| 35 | /*FeII_RT_Out do outward rates for FeII, called by RT_diffuse */ |
| 36 | /*FeII_OTS do ots rates for FeII, called by RT_OTS */ |
| 37 | /*FeII_RT_Make called by RT_line_all, does large FeII atom radiative transfer */ |
| 38 | /*FeIILyaPump find rate of Lya excitation of the FeII atom */ |
| 39 | /*FeIIOvrLap handle overlapping FeII lines */ |
| 40 | /*ParseAtomFeII parse the atom FeII command */ |
| 41 | /*FeIIPunchLineStuff include FeII lines in punched optical depths, etc, called from PunchLineStuff */ |
| 42 | #include "cddefines.h" |
| 43 | #include "cddrive.h" |
| 44 | #include "thermal.h" |
| 45 | #include "physconst.h" |
| 46 | #include "doppvel.h" |
| 47 | #include "taulines.h" |
| 48 | #include "dense.h" |
| 49 | #include "rfield.h" |
| 50 | #include "radius.h" |
| 51 | #include "lines_service.h" |
| 52 | #include "ipoint.h" |
| 53 | #include "thirdparty.h" |
| 54 | #include "hydrogenic.h" |
| 55 | #include "lines.h" |
| 56 | #include "rt.h" |
| 57 | #include "trace.h" |
| 58 | #include "punch.h" |
| 59 | #include "phycon.h" |
| 60 | #include "atomfeii.h" |
| 61 | #include "iso.h" |
| 62 | #include "pressure.h" |
| 63 | |
| 64 | /* FeIIOvrLap handle overlapping FeII lines */ |
| 65 | STATIC void FeIIOvrLap(void); |
| 66 | |
| 67 | /* add FeII lines into ncell cells between wavelengths lambda low and high */ |
| 68 | STATIC void FeIIContCreate(double xLamLow , double xLamHigh , long int ncell ); |
| 69 | |
| 70 | /* read in the FeII Bands file, and sets nFeIIBands, the number of bands, |
| 71 | * if argument is "" then use default file with bands, |
| 72 | * if filename within "" then use it instead, |
| 73 | * return value is 0 if success, 1 if failed */ |
| 74 | STATIC int FeIIBandsCreate( const char chFile[] ); |
| 75 | |
| 76 | /* this will be the smallest collision strength we will permit with the gbar |
| 77 | * collision strengths, or for the data that have zeroes */ |
| 78 | /* >>chng 99 jul 24, this was 1e-9 in the old fortran version and in baldwin et al. 96, |
| 79 | * and has been changed several times, and affects results. this is the smallest |
| 80 | * non-zero collision strength in the r-matrix calculations */ |
| 81 | realnum CS2SMALL = (realnum)1e-5; |
| 82 | /* routines used only within this file */ |
| 83 | |
| 84 | /*FeIICollRatesBoltzmann evaluate collision strenths, |
| 85 | * both interpolating on r-mat and creating g-bar |
| 86 | * find Boltzmann factors, evaluate collisional rate coefficients */ |
| 87 | STATIC void FeIICollRatesBoltzmann(void); |
| 88 | /* find rate of Lya excitation of the FeII atom */ |
| 89 | STATIC void FeIILyaPump(void); |
| 90 | |
| 91 | /*extern realnum Fe2LevN[NFE2LEVN][NFE2LEVN][NTA];*/ |
| 92 | /*extern realnum Fe2LevN[ipHi][ipLo].t[NTA];*/ |
| 93 | /*realnum ***Fe2LevN;*/ |
| 94 | /* >>chng 06 mar 01, boost to global namespace */ |
| 95 | /*transition **Fe2LevN;*/ |
| 96 | /* flag for the collision strength */ |
| 97 | int **ncs1; |
| 98 | |
| 99 | /* all following variables have file scope |
| 100 | #define NFEIILINES 68635 */ |
| 101 | |
| 102 | /* this is size of nnPradDat array */ |
| 103 | #define NPRADDAT 159 |
| 104 | |
| 105 | /* band wavelength, lower and upper bounds, in vacuum Angstroms */ |
| 106 | /* FeII_Bands[n][3], where n is the number of bands in fe2Bands.dat |
| 107 | * these bands are defined in fe2Bands.dat and read in at startup |
| 108 | * of calculation */ |
| 109 | realnum **FeII_Bands; |
| 110 | |
| 111 | /* continuum wavelengths, lower and upper bounds, in vacuum Angstroms, |
| 112 | * third is integrated intensity */ |
| 113 | /* FeII_Cont[n][3], where n is the number of cells needed |
| 114 | * these bands are defined in FeIIContCreate */ |
| 115 | realnum **FeII_Cont; |
| 116 | |
| 117 | /* this is the number of bands read in from FeII_bands.ini */ |
| 118 | long int nFeIIBands; |
| 119 | |
| 120 | /* number of bands in continuum array */ |
| 121 | long int nFeIIConBins; |
| 122 | |
| 123 | /* the dim of this vector this needs one extra since there are 20 numbers per line, |
| 124 | * highest not ever used for anything */ |
| 125 | /*long int nnPradDat[NPRADDAT+1];*/ |
| 126 | static long int *nnPradDat; |
| 127 | |
| 128 | /* malloced in feiidata */ |
| 129 | /* realnum sPradDat[NPRADDAT][NPRADDAT][8];*/ |
| 130 | /* realnum sPradDat[ipHi][ipLo].t[8];*/ |
| 131 | static realnum ***sPradDat; |
| 132 | |
| 133 | /* array used to integrate FeII line intensities over model, |
| 134 | * Fe2SavN[upper][lower], |
| 135 | *static realnum Fe2SavN[NFE2LEVN][NFE2LEVN];*/ |
| 136 | static double **Fe2SavN; |
| 137 | |
| 138 | /* save effective transition rates */ |
| 139 | static double **Fe2A; |
| 140 | |
| 141 | /* induced transition rates */ |
| 142 | static double **Fe2LPump, **Fe2CPump; |
| 143 | |
| 144 | /* energies read in from fe2energies.dat data file */ |
| 145 | realnum *Fe2Energies; |
| 146 | |
| 147 | /* collision rates */ |
| 148 | static realnum **Fe2Coll; |
| 149 | |
| 150 | /* Fe2DepCoef[NFE2LEVN]; |
| 151 | realnum cli[NFEIILINES], |
| 152 | cfe[NFEIILINES];*/ |
| 153 | static double |
| 154 | /* departure coefficients */ |
| 155 | *Fe2DepCoef , |
| 156 | /* level populations */ |
| 157 | *Fe2LevelPop , |
| 158 | /* column densities */ |
| 159 | *Fe2ColDen , |
| 160 | /* this will become array of Boltzmann factors */ |
| 161 | *FeIIBoltzmann; |
| 162 | /*FeIIBoltzmann[NFE2LEVN] ,*/ |
| 163 | |
| 164 | static double EnerLyaProf1, |
| 165 | EnerLyaProf4, |
| 166 | PhotOccNumLyaCenter; |
| 167 | static double |
| 168 | /* the yVector - will become level populations after matrix inversion */ |
| 169 | *yVector, |
| 170 | /* this is used to call matrix routines */ |
| 171 | /*xMatrix[NFE2LEVN][NFE2LEVN] ,*/ |
| 172 | **xMatrix , |
| 173 | /* this will become the very large 1-D array that |
| 174 | * is passed to the matrix inversion routine*/ |
| 175 | *amat; |
| 176 | |
| 177 | |
| 178 | /*FeII_Colden maintain H2 column densities within X */ |
| 179 | void FeII_Colden( const char *chLabel ) |
| 180 | { |
| 181 | long int n; |
| 182 | |
| 183 | DEBUG_ENTRY( "FeII_Colden()" ); |
| 184 | |
| 185 | /* >>chng 05 nov 29, FeII always on, always want to evaluate this */ |
| 186 | /* nothing to do if no FeII |
| 187 | if( !FeII. lgFeIION ) |
| 188 | return;*/ |
| 189 | |
| 190 | if( strcmp(chLabel,"ZERO") == 0 ) |
| 191 | { |
| 192 | /* zero out column density */ |
| 193 | for( n=0; n < FeII.nFeIILevel; ++n ) |
| 194 | { |
| 195 | /* space for the rotation quantum number */ |
| 196 | Fe2ColDen[n] = 0.; |
| 197 | } |
| 198 | } |
| 199 | |
| 200 | else if( strcmp(chLabel,"ADD ") == 0 ) |
| 201 | { |
| 202 | /* add together column densities */ |
| 203 | for( n=0; n < FeII.nFeIILevel; ++n ) |
| 204 | { |
| 205 | /* state-specific FeII column density */ |
| 206 | Fe2ColDen[n] += Fe2LevelPop[n]*radius.drad_x_fillfac; |
| 207 | } |
| 208 | } |
| 209 | |
| 210 | /* check for the print option, which we can't do, else we have a problem */ |
| 211 | else if( strcmp(chLabel,"PRIN") != 0 ) |
| 212 | { |
| 213 | fprintf( ioQQQ, " FeII_Colden does not understand the label %s\n", |
| 214 | chLabel ); |
| 215 | cdEXIT(EXIT_FAILURE); |
| 216 | } |
| 217 | |
| 218 | return; |
| 219 | } |
| 220 | |
| 221 | /* |
| 222 | *===================================================================== |
| 223 | */ |
| 224 | /* FeIICreate read in FeII data from files on disk. called by atmdat_readin |
| 225 | * but only if FeII. lgFeIION is true, set with atom FeII verner command */ |
| 226 | void FeIICreate(void) |
| 227 | { |
| 228 | FILE *ioDATA; |
| 229 | |
| 230 | char chLine[FILENAME_PATH_LENGTH_2]; |
| 231 | |
| 232 | long int i, |
| 233 | ipHi , |
| 234 | ipLo, |
| 235 | lo, |
| 236 | ihi, |
| 237 | k, |
| 238 | m1, |
| 239 | m2, |
| 240 | m3; |
| 241 | |
| 242 | DEBUG_ENTRY( "FeIICreate()" ); |
| 243 | |
| 244 | if( lgFeIIMalloc ) |
| 245 | { |
| 246 | /* we have already been called one time, just bail out */ |
| 247 | |
| 248 | return; |
| 249 | } |
| 250 | |
| 251 | /* now set flag so never done again - this is set false when initi |
| 252 | * when this is true it is no longer possible to change the number of levels |
| 253 | * in the model atom with the atom FeII levels command */ |
| 254 | lgFeIIMalloc = true; |
| 255 | |
| 256 | /* remember how many levels this was, so that in future calculations |
| 257 | * we can reset the atom to full value */ |
| 258 | FeII.nFeIILevelAlloc = FeII.nFeIILevel; |
| 259 | |
| 260 | /* set up array to save FeII transition probabilities */ |
| 261 | Fe2A = (double **)MALLOC(sizeof(double *)*(unsigned long)FeII.nFeIILevelAlloc ); |
| 262 | |
| 263 | /* second dimension, lower level, for line save array */ |
| 264 | for( ipHi=0; ipHi < FeII.nFeIILevelAlloc; ++ipHi ) |
| 265 | { |
| 266 | Fe2A[ipHi]=(double*)MALLOC(sizeof(double )*(unsigned long)FeII.nFeIILevelAlloc); |
| 267 | } |
| 268 | |
| 269 | /* set up array to save FeII pumping rates */ |
| 270 | Fe2CPump = (double **)MALLOC(sizeof(double *)*(unsigned long)FeII.nFeIILevelAlloc ); |
| 271 | |
| 272 | /* set up array to save FeII pumping rates */ |
| 273 | Fe2LPump = (double **)MALLOC(sizeof(double *)*(unsigned long)FeII.nFeIILevelAlloc ); |
| 274 | |
| 275 | /* second dimension, lower level, for line save array */ |
| 276 | for( ipHi=0; ipHi < FeII.nFeIILevelAlloc; ++ipHi ) |
| 277 | { |
| 278 | Fe2CPump[ipHi]=(double*)MALLOC(sizeof(double )*(unsigned long)FeII.nFeIILevelAlloc); |
| 279 | |
| 280 | Fe2LPump[ipHi]=(double*)MALLOC(sizeof(double )*(unsigned long)FeII.nFeIILevelAlloc); |
| 281 | } |
| 282 | |
| 283 | /* set up array to save FeII collision rates */ |
| 284 | Fe2Energies = (realnum *)MALLOC(sizeof(realnum)*(unsigned long)FeII.nFeIILevelAlloc ); |
| 285 | |
| 286 | /* set up array to save FeII collision rates */ |
| 287 | Fe2Coll = (realnum **)MALLOC(sizeof(realnum *)*(unsigned long)FeII.nFeIILevelAlloc ); |
| 288 | |
| 289 | /* second dimension, lower level, for line save array */ |
| 290 | for( ipHi=0; ipHi < FeII.nFeIILevelAlloc; ++ipHi ) |
| 291 | { |
| 292 | Fe2Coll[ipHi]=(realnum*)MALLOC(sizeof(realnum )*(unsigned long)FeII.nFeIILevelAlloc); |
| 293 | } |
| 294 | |
| 295 | /* MALLOC space for the 2D matrix array */ |
| 296 | xMatrix = (double **)MALLOC(sizeof(double *)*(unsigned long)FeII.nFeIILevelAlloc ); |
| 297 | |
| 298 | /* now do the second dimension */ |
| 299 | for( i=0; i<FeII.nFeIILevelAlloc; ++i ) |
| 300 | { |
| 301 | xMatrix[i] = (double *)MALLOC(sizeof(double)*(unsigned long)FeII.nFeIILevelAlloc ); |
| 302 | } |
| 303 | /* MALLOC space for the 1-yVector array */ |
| 304 | amat=(double*)MALLOC( (sizeof(double)*(unsigned long)(FeII.nFeIILevelAlloc*FeII.nFeIILevelAlloc) )); |
| 305 | |
| 306 | /* MALLOC space for the 1-yVector array */ |
| 307 | yVector=(double*)MALLOC( (sizeof(double)*(unsigned long)(FeII.nFeIILevelAlloc) )); |
| 308 | |
| 309 | /* set up array to save FeII line intensities */ |
| 310 | Fe2SavN = (double **)MALLOC(sizeof(double *)*(unsigned long)FeII.nFeIILevelAlloc ); |
| 311 | |
| 312 | /* second dimension, lower level, for line save array */ |
| 313 | for( ipHi=1; ipHi < FeII.nFeIILevelAlloc; ++ipHi ) |
| 314 | { |
| 315 | Fe2SavN[ipHi]=(double*)MALLOC(sizeof(double )*(unsigned long)ipHi); |
| 316 | } |
| 317 | |
| 318 | /* now MALLOC space for energy level table*/ |
| 319 | nnPradDat = (long*)MALLOC( (NPRADDAT+1)*sizeof(long) ); |
| 320 | |
| 321 | /*Fe2DepCoef[NFE2LEVN];*/ |
| 322 | Fe2DepCoef = (double*)MALLOC( (unsigned long)FeII.nFeIILevelAlloc*sizeof(double) ); |
| 323 | |
| 324 | /*Fe2LevelPop[NFE2LEVN];*/ |
| 325 | Fe2LevelPop = (double*)MALLOC( (unsigned long)FeII.nFeIILevelAlloc*sizeof(double) ); |
| 326 | |
| 327 | /*Fe2ColDen[NFE2LEVN];*/ |
| 328 | Fe2ColDen = (double*)MALLOC( (unsigned long)FeII.nFeIILevelAlloc*sizeof(double) ); |
| 329 | |
| 330 | /*FeIIBoltzmann[NFE2LEVN];*/ |
| 331 | FeIIBoltzmann = (double*)MALLOC( (unsigned long)FeII.nFeIILevelAlloc*sizeof(double) ); |
| 332 | |
| 333 | |
| 334 | /* MALLOC the realnum sPradDat[NPRADDAT][NPRADDAT][8] array */ |
| 335 | /* MALLOC the realnum sPradDat[ipHi][ipLo].t[8] array */ |
| 336 | sPradDat = ((realnum ***)MALLOC(NPRADDAT*sizeof(realnum **))); |
| 337 | |
| 338 | /* >>chng 00 dec 06, changed lower limit of loop to 1, Tru64 alpha's will not allocate 0 bytes!, PvH */ |
| 339 | sPradDat[0] = NULL; |
| 340 | for(ipHi=1; ipHi < NPRADDAT; ipHi++) |
| 341 | { |
| 342 | /* >>chng 00 dec 06, changed sizeof(realnum) to sizeof(realnum*), PvH */ |
| 343 | sPradDat[ipHi] = (realnum **)MALLOC((unsigned long)ipHi*sizeof(realnum *)); |
| 344 | |
| 345 | /* now make space for the second dimension */ |
| 346 | for( ipLo=0; ipLo< ipHi; ipLo++ ) |
| 347 | { |
| 348 | sPradDat[ipHi][ipLo] = (realnum *)MALLOC(8*sizeof(realnum )); |
| 349 | } |
| 350 | } |
| 351 | |
| 352 | /* now set junk to make sure reset before used */ |
| 353 | for(ipHi=0; ipHi < NPRADDAT; ipHi++) |
| 354 | { |
| 355 | for( ipLo=0; ipLo< ipHi; ipLo++ ) |
| 356 | { |
| 357 | for( k=0; k<8; ++k ) |
| 358 | { |
| 359 | sPradDat[ipHi][ipLo][k] = -FLT_MAX; |
| 360 | } |
| 361 | } |
| 362 | } |
| 363 | |
| 364 | /* now create the main emission line array and a helper array for the cs flag */ |
| 365 | Fe2LevN=(transition**)MALLOC(sizeof(transition *)*(unsigned long)FeII.nFeIILevelAlloc); |
| 366 | ncs1=(int**)MALLOC(sizeof(int *)*(unsigned long)FeII.nFeIILevelAlloc); |
| 367 | |
| 368 | for( ipHi=1; ipHi < FeII.nFeIILevelAlloc; ++ipHi ) |
| 369 | { |
| 370 | Fe2LevN[ipHi]=(transition*)MALLOC(sizeof(transition)*(unsigned long)ipHi); |
| 371 | |
| 372 | ncs1[ipHi]=(int*)MALLOC(sizeof(int)*(unsigned long)ipHi); |
| 373 | } |
| 374 | |
| 375 | #if 0 |
| 376 | /* now that its created, set to junk */ |
| 377 | for( ipLo=0; ipLo < (FeII.nFeIILevelAlloc - 1); ipLo++ ) |
| 378 | { |
| 379 | for( ipHi=ipLo + 1; ipHi < FeII.nFeIILevelAlloc; ipHi++ ) |
| 380 | { |
| 381 | TransitionJunk( &Fe2LevN[ipHi][ipLo] ); |
| 382 | } |
| 383 | } |
| 384 | #endif |
| 385 | |
| 386 | /* now assign state and Emis pointers */ |
| 387 | Fe2LevN[1][0].Lo = AddState2Stack(); |
| 388 | /* now that its created, set to junk */ |
| 389 | for( ipHi=1; ipHi < FeII.nFeIILevelAlloc; ipHi++ ) |
| 390 | { |
| 391 | /* add this upper level */ |
| 392 | Fe2LevN[ipHi][0].Hi = AddState2Stack(); |
| 393 | for( ipLo=0; ipLo < ipHi; ipLo++ ) |
| 394 | { |
| 395 | if( ipLo == 0 ) |
| 396 | { |
| 397 | Fe2LevN[ipHi][ipLo].Lo = Fe2LevN[1][0].Lo; |
| 398 | } |
| 399 | else |
| 400 | { |
| 401 | /* lower state is same as a previous upper state. */ |
| 402 | Fe2LevN[ipHi][ipLo].Lo = Fe2LevN[ipLo][0].Hi; |
| 403 | } |
| 404 | |
| 405 | Fe2LevN[ipHi][ipLo].Hi = Fe2LevN[ipHi][0].Hi; |
| 406 | Fe2LevN[ipHi][ipLo].Emis = AddLine2Stack( true ); |
| 407 | } |
| 408 | } |
| 409 | |
| 410 | if( trace.lgTrace ) |
| 411 | { |
| 412 | fprintf( ioQQQ," FeIICreate opening fe2nn.dat:"); |
| 413 | } |
| 414 | |
| 415 | ioDATA = open_data( "fe2nn.dat", "r" ); |
| 416 | |
| 417 | ASSERT( ioDATA !=NULL ); |
| 418 | /* read in the fe2nn.dat file - this gives the Zheng and Pradhan number of level |
| 419 | * for every cloudy level. So nnPradDat[1] is the index in the cloudy level |
| 420 | * counting for level 1 of Zheng & Pradan |
| 421 | * note that the order of some levels is different, the nnPradDat file goes |
| 422 | * 21 23 22 - also that many levels are missing, the file goes 95 99 94 93 116 |
| 423 | */ |
| 424 | for( i=0; i < 8; i++ ) |
| 425 | { |
| 426 | if( read_whole_line( chLine , (int)sizeof(chLine) , ioDATA ) == NULL ) |
| 427 | { |
| 428 | fprintf( ioQQQ, " fe2nn.dat error reading data\n" ); |
| 429 | cdEXIT(EXIT_FAILURE); |
| 430 | } |
| 431 | |
| 432 | /* get these integers from fe2nn.dat */ |
| 433 | k = 20*i; |
| 434 | /* NPRADDAT is size of nnPradDat array, 159+1, make sure we do not exceed it */ |
| 435 | ASSERT( k+19 < NPRADDAT+1 ); |
| 436 | sscanf( chLine , |
| 437 | "%4ld%4ld%4ld%4ld%4ld%4ld%4ld%4ld%4ld%4ld%4ld%4ld%4ld%4ld%4ld%4ld%4ld%4ld%4ld%4ld", |
| 438 | &nnPradDat[k+0], &nnPradDat[k+1], &nnPradDat[k+2], &nnPradDat[k+3], &nnPradDat[k+4], |
| 439 | &nnPradDat[k+5], &nnPradDat[k+6], &nnPradDat[k+7], &nnPradDat[k+8], &nnPradDat[k+9], |
| 440 | &nnPradDat[k+10],&nnPradDat[k+11], &nnPradDat[k+12],&nnPradDat[k+13],&nnPradDat[k+14], |
| 441 | &nnPradDat[k+15],&nnPradDat[k+16], &nnPradDat[k+17],&nnPradDat[k+18],&nnPradDat[k+19] |
| 442 | ); |
| 443 | # if !defined(NDEBUG) |
| 444 | for( m1=0; m1<20; ++m1 ) |
| 445 | { |
| 446 | ASSERT( nnPradDat[k+m1] >= 0 && nnPradDat[k+m1] <= NFE2LEVN ); |
| 447 | } |
| 448 | # endif |
| 449 | } |
| 450 | fclose(ioDATA); |
| 451 | |
| 452 | /* now get energies */ |
| 453 | if( trace.lgTrace ) |
| 454 | { |
| 455 | fprintf( ioQQQ," FeIICreate opening fe2energies.dat:"); |
| 456 | } |
| 457 | |
| 458 | ioDATA = open_data( "fe2energies.dat", "r" ); |
| 459 | |
| 460 | /* file now open, read the data */ |
| 461 | for( ipHi=0; ipHi < FeII.nFeIILevelAlloc; ipHi++ ) |
| 462 | { |
| 463 | /* keep reading until have non-comment line, one that does not |
| 464 | * start with # */ |
| 465 | chLine[0] = '#'; |
| 466 | while( chLine[0] == '#' ) |
| 467 | { |
| 468 | if( read_whole_line( chLine , (int)sizeof(chLine) , ioDATA ) == NULL ) |
| 469 | { |
| 470 | fprintf( ioQQQ, " fe2energies.dat error reading data\n" ); |
| 471 | cdEXIT(EXIT_FAILURE); |
| 472 | } |
| 473 | } |
| 474 | |
| 475 | /* first and last number on this line */ |
| 476 | double help; |
| 477 | sscanf( chLine, "%lf", &help ); |
| 478 | Fe2Energies[ipHi] = (realnum)help; |
| 479 | } |
| 480 | fclose(ioDATA); |
| 481 | |
| 482 | /* transition probabilities */ |
| 483 | |
| 484 | if( trace.lgTrace ) |
| 485 | fprintf( ioQQQ," FeIICreate opening fe2rad.dat:"); |
| 486 | |
| 487 | ioDATA = open_data( "fe2rad.dat", "r" ); |
| 488 | |
| 489 | /* get the first line, this is a version number */ |
| 490 | if( read_whole_line( chLine , (int)sizeof(chLine) , ioDATA ) == NULL ) |
| 491 | { |
| 492 | fprintf( ioQQQ, " fe2rad.dat error reading data\n" ); |
| 493 | cdEXIT(EXIT_FAILURE); |
| 494 | } |
| 495 | /* scan off three integers */ |
| 496 | sscanf( chLine ,"%ld%ld%ld",&lo, &ihi, &m1); |
| 497 | const int nYrFe2Rad=8, nMoFe2Rad=8, nDyFe2Rad=24; |
| 498 | if( lo!=nYrFe2Rad || ihi!=nMoFe2Rad || m1!=nDyFe2Rad ) |
| 499 | { |
| 500 | fprintf( ioQQQ, "DISASTER fe2rad.dat has the wrong magic numbers, expected " |
| 501 | "%2i %2i %2i and got %2li %2li %2li\n" , |
| 502 | nYrFe2Rad, nMoFe2Rad, nDyFe2Rad, |
| 503 | lo, ihi, m1); |
| 504 | cdEXIT(EXIT_FAILURE); |
| 505 | } |
| 506 | |
| 507 | /* file now open, read the data */ |
| 508 | for( ipHi=1; ipHi < FeII.nFeIILevelAlloc; ipHi++ ) |
| 509 | { |
| 510 | for( ipLo=0; ipLo < ipHi; ipLo++ ) |
| 511 | { |
| 512 | /* following double since used in sscanf */ |
| 513 | double save[2]; |
| 514 | /* keep reading until have non-comment line, one that does not |
| 515 | * start with # */ |
| 516 | chLine[0] = '#'; |
| 517 | while( chLine[0] == '#' ) |
| 518 | { |
| 519 | if( read_whole_line( chLine , (int)sizeof(chLine) , ioDATA ) == NULL ) |
| 520 | { |
| 521 | fprintf( ioQQQ, " fe2nn.dat error reading data\n" ); |
| 522 | cdEXIT(EXIT_FAILURE); |
| 523 | } |
| 524 | } |
| 525 | |
| 526 | /* first and last number on this line */ |
| 527 | sscanf( chLine , |
| 528 | "%ld%ld%ld%ld%lf%lf%ld", |
| 529 | &lo, &ihi, &m1, &m2 , |
| 530 | &save[0], &save[1] , &m3); |
| 531 | /* the indices ihi and lo within this array were |
| 532 | * read in from the line above */ |
| 533 | Fe2LevN[ihi-1][lo-1].Lo->g = (realnum)m1; |
| 534 | Fe2LevN[ihi-1][lo-1].Hi->g = (realnum)m2; |
| 535 | Fe2LevN[ihi-1][lo-1].Emis->Aul = (realnum)save[0]; |
| 536 | /*>>chng 06 apr 10, option to use table of energies */ |
| 537 | # define USE_OLD true |
| 538 | if( USE_OLD ) |
| 539 | Fe2LevN[ihi-1][lo-1].EnergyWN = (realnum)save[1]; |
| 540 | else |
| 541 | Fe2LevN[ihi-1][lo-1].EnergyWN = Fe2Energies[ihi-1]-Fe2Energies[lo-1]; |
| 542 | |
| 543 | /* Aul == -1 indicates intercombination line with no real Aul */ |
| 544 | if( fp_equal( Fe2LevN[ihi-1][lo-1].Emis->Aul , (realnum)-1.0f ) ) |
| 545 | { |
| 546 | /* these are made-up intercombination lines, set gf to 1e-5 */ |
| 547 | Fe2LevN[ihi-1][lo-1].Emis->gf = 1e-5f; |
| 548 | |
| 549 | /* get corresponding A */ |
| 550 | Fe2LevN[ihi-1][lo-1].Emis->Aul = Fe2LevN[ihi-1][lo-1].Emis->gf*(realnum)TRANS_PROB_CONST* |
| 551 | POW2(Fe2LevN[ihi-1][lo-1].EnergyWN)*Fe2LevN[ihi-1][lo-1].Lo->g/Fe2LevN[ihi-1][lo-1].Hi->g; |
| 552 | } |
| 553 | |
| 554 | /* the last column of fe2rad.dat, and is 1, 2, or 3. |
| 555 | * 1 signifies that transition is permitted, |
| 556 | * 2 is semi-forbidden |
| 557 | * 3 forbidden, within lowest 63 levels are forbidden, first permitted |
| 558 | * transition is from 64 */ |
| 559 | ncs1[ihi-1][lo-1] = (int)m3; |
| 560 | } |
| 561 | } |
| 562 | fclose(ioDATA); |
| 563 | |
| 564 | /* now read collision data in fe2col.dat |
| 565 | * These are from the following sources |
| 566 | >>refer fe2 cs Zhang, H.L., & Pradhan, A.K., 1995, A&A 293, 953 |
| 567 | >>refer fe2 cs Bautista, M., (private communication), |
| 568 | >>refer fe2 cs Mewe, R., 1972, A&AS 20, 215 (the g-bar approximation) |
| 569 | */ |
| 570 | |
| 571 | if( trace.lgTrace ) |
| 572 | { |
| 573 | fprintf( ioQQQ," FeIICreate opening fe2col.dat:"); |
| 574 | } |
| 575 | |
| 576 | ioDATA = open_data( "fe2col.dat", "r" ); |
| 577 | |
| 578 | ASSERT( ioDATA !=NULL); |
| 579 | for( ipHi=1; ipHi<NPRADDAT; ++ipHi ) |
| 580 | { |
| 581 | for( ipLo=0; ipLo<ipHi; ++ipLo ) |
| 582 | { |
| 583 | /* double since used in sscanf */ |
| 584 | double save[8]; |
| 585 | if( read_whole_line( chLine , (int)sizeof(chLine) , ioDATA ) == NULL ) |
| 586 | { |
| 587 | fprintf( ioQQQ, " fe2col.dat error reading data\n" ); |
| 588 | cdEXIT(EXIT_FAILURE); |
| 589 | } |
| 590 | sscanf( chLine , |
| 591 | "%ld%ld%lf%lf%lf%lf%lf%lf%lf%lf", |
| 592 | &m1, &m2, |
| 593 | &save[0], &save[1] , &save[2],&save[3], &save[4] , &save[5], |
| 594 | &save[6], &save[7] |
| 595 | ); |
| 596 | for( k=0; k<8; ++k ) |
| 597 | { |
| 598 | /* the max is here because there are some zeroes in the data file. |
| 599 | * this is unphysical but is part of their distribution. As a result |
| 600 | * don't let the cs fall below 0.01 */ |
| 601 | sPradDat[m2-1][m1-1][k] = max(CS2SMALL , (realnum)save[k] ); |
| 602 | } |
| 603 | } |
| 604 | } |
| 605 | |
| 606 | fclose( ioDATA ); |
| 607 | |
| 608 | /*generate needed opacity data for the large FeII atom */ |
| 609 | |
| 610 | /* this routine is called only one time when cloudy is init |
| 611 | * for the very first time. It converts the FeII data stored |
| 612 | * in the large FeII arrays into the array storage needed by cloudy |
| 613 | * for its line optical depth arrays |
| 614 | */ |
| 615 | |
| 616 | /* convert large FeII line arrays into standard heavy el ar */ |
| 617 | for( ipLo=0; ipLo < (FeII.nFeIILevelAlloc - 1); ipLo++ ) |
| 618 | { |
| 619 | for( ipHi=ipLo + 1; ipHi < FeII.nFeIILevelAlloc; ipHi++ ) |
| 620 | { |
| 621 | /* pull information out of existing data arrays */ |
| 622 | |
| 623 | ASSERT( Fe2LevN[ipHi][ipLo].EnergyWN > 0. ); |
| 624 | ASSERT( Fe2LevN[ipHi][ipLo].Emis->Aul> 0. ); |
| 625 | |
| 626 | /* now put into standard internal line format |
| 627 | Fe2LevN[ipHi][ipLo].WLAng = (realnum)(1.e8/Fe2LevN[ipHi][ipLo].EnergyWN); */ |
| 628 | /* >>chng 03 oct 28, above neglected index of refraction of air - |
| 629 | * convert to below */ |
| 630 | Fe2LevN[ipHi][ipLo].WLAng = |
| 631 | (realnum)(1.0e8/ |
| 632 | Fe2LevN[ipHi][ipLo].EnergyWN/ |
| 633 | RefIndex( Fe2LevN[ipHi][ipLo].EnergyWN )); |
| 634 | |
| 635 | /* generate gf from A */ |
| 636 | Fe2LevN[ipHi][ipLo].Emis->gf = |
| 637 | (realnum)(Fe2LevN[ipHi][ipLo].Emis->Aul*Fe2LevN[ipHi][ipLo].Hi->g/ |
| 638 | TRANS_PROB_CONST/POW2(Fe2LevN[ipHi][ipLo].EnergyWN)); |
| 639 | |
| 640 | Fe2LevN[ipHi][ipLo].Hi->IonStg = 2; |
| 641 | Fe2LevN[ipHi][ipLo].Hi->nelem = 26; |
| 642 | /* which redistribution function?? |
| 643 | * For resonance line use K2 (-1), |
| 644 | * for subordinate lines use CRD with wings */ |
| 645 | /* >>chng 01 mar 09, all had been 1, inc redis with wings */ |
| 646 | /* to reset this, so that the code works as it did pre 01 mar 29, |
| 647 | * use command |
| 648 | * atom FeII redistribution resonance pdr |
| 649 | * atom FeII redistribution subordinate pdr */ |
| 650 | if( ipLo == 0 ) |
| 651 | { |
| 652 | Fe2LevN[ipHi][ipLo].Emis->iRedisFun = FeII.ipRedisFcnResonance; |
| 653 | } |
| 654 | else |
| 655 | { |
| 656 | /* >>chng 01 feb 27, had been -1, crd with core only, |
| 657 | * change to crd with wings as per discussion with Ivan Hubeny */ |
| 658 | Fe2LevN[ipHi][ipLo].Emis->iRedisFun = FeII.ipRedisFcnSubordinate; |
| 659 | } |
| 660 | Fe2LevN[ipHi][ipLo].Emis->phots = 0.; |
| 661 | Fe2LevN[ipHi][ipLo].Emis->ots = 0.; |
| 662 | Fe2LevN[ipHi][ipLo].Emis->FracInwd = 1.; |
| 663 | } |
| 664 | } |
| 665 | |
| 666 | /* finally get FeII bands, this sets */ |
| 667 | if( FeIIBandsCreate("") ) |
| 668 | { |
| 669 | fprintf( ioQQQ," failed to open FeII bands file \n"); |
| 670 | cdEXIT(EXIT_FAILURE); |
| 671 | } |
| 672 | |
| 673 | /* now establish the FeII continuum, these are set to |
| 674 | * 1000, 7000, and 1000 in FeIIZero in this file, and |
| 675 | * are reset with the atom FeII continuum command */ |
| 676 | FeIIContCreate( FeII.fe2con_wl1 , FeII.fe2con_wl2 , FeII.nfe2con ); |
| 677 | |
| 678 | /* this must be true */ |
| 679 | ASSERT( FeII.nFeIILevelAlloc == FeII.nFeIILevel ); |
| 680 | |
| 681 | return; |
| 682 | } |
| 683 | |
| 684 | /* |
| 685 | *===================================================================== |
| 686 | */ |
| 687 | /*********************************************************************** |
| 688 | *** version of FeIILevelPops.f with overlap in procces 05.28.97 ooooooo |
| 689 | ******change in common block *te* sqrte 05.28.97 |
| 690 | *******texc is fixed 03.28.97 |
| 691 | *********this version has work on overlap |
| 692 | *********this version has # of zones (ZoneCnt) 07.03.97 |
| 693 | *********taux - optical depth depends on iter correction 03.03.97 |
| 694 | *********calculate cooling (Fe2_large_cool) and output fecool from Cloudy 01.29.97god |
| 695 | *********and cooling derivative (ddT_Fe2_large_cool) |
| 696 | ************ this program for 371 level iron model 12/14/1995 |
| 697 | ************ this program for 371 level iron model 1/11/1996 |
| 698 | ************ this program for 371 level iron model 3/21/1996 |
| 699 | ************ this program without La 3/27/1996 |
| 700 | ************ this program for 371 level iron model 4/9/1996 |
| 701 | ************ includes:FeIICollRatesBoltzmann;cooling;overlapping in lines */ |
| 702 | void FeIILevelPops( void ) |
| 703 | { |
| 704 | long int i, |
| 705 | ipHi , |
| 706 | ipLo , |
| 707 | n; |
| 708 | /* used in test for non-positive level populations */ |
| 709 | bool lgPopNeg; |
| 710 | |
| 711 | double |
| 712 | EnergyWN, |
| 713 | pop , |
| 714 | sum; |
| 715 | |
| 716 | int32 info; |
| 717 | int32 ipiv[NFE2LEVN]; |
| 718 | |
| 719 | DEBUG_ENTRY( "FeIILevelPops()" ); |
| 720 | |
| 721 | if( trace.lgTrace ) |
| 722 | { |
| 723 | fprintf( ioQQQ," FeIILevelPops fe2 pops called\n"); |
| 724 | } |
| 725 | |
| 726 | /* FeII.lgSimulate was set true with simulate flag on atom FeII command, |
| 727 | * for bebugging without actually calling the routine */ |
| 728 | if( FeII.lgSimulate ) |
| 729 | { |
| 730 | |
| 731 | return; |
| 732 | } |
| 733 | |
| 734 | /* zero out some arrays */ |
| 735 | for( n=0; n<FeII.nFeIILevel; ++n) |
| 736 | { |
| 737 | for( ipLo=0; ipLo<FeII.nFeIILevel; ++ipLo ) |
| 738 | { |
| 739 | Fe2CPump[ipLo][n] = 0.; |
| 740 | Fe2LPump[ipLo][n] = 0.; |
| 741 | Fe2A[ipLo][n] = 0.; |
| 742 | xMatrix[ipLo][n] = 0.; |
| 743 | } |
| 744 | } |
| 745 | |
| 746 | /* make the g-bar collision strengths and do linear interpolation on r-matrix data. |
| 747 | * this also sets Boltzmann factors for all levels, |
| 748 | * sets values of FeColl used below, but only if temp has changed */ |
| 749 | FeIICollRatesBoltzmann(); |
| 750 | |
| 751 | /* pumping and spontantous decays */ |
| 752 | for( n=0; n<FeII.nFeIILevel; ++n) |
| 753 | { |
| 754 | for( ipHi=n+1; ipHi<FeII.nFeIILevel; ++ipHi ) |
| 755 | { |
| 756 | /* continuum pumping rate from n to upper ipHi */ |
| 757 | Fe2CPump[n][ipHi] = Fe2LevN[ipHi][n].Emis->pump; |
| 758 | |
| 759 | /* continuum pumping rate from ipHi to lower n */ |
| 760 | Fe2CPump[ipHi][n] = Fe2LevN[ipHi][n].Emis->pump* |
| 761 | Fe2LevN[ipHi][n].Hi->g/Fe2LevN[ipHi][n].Lo->g; |
| 762 | |
| 763 | /* spontaneous decays */ |
| 764 | Fe2A[ipHi][n] = Fe2LevN[ipHi][n].Emis->Aul*(Fe2LevN[ipHi][n].Emis->Pesc + Fe2LevN[ipHi][n].Emis->Pelec_esc + |
| 765 | Fe2LevN[ipHi][n].Emis->Pdest); |
| 766 | } |
| 767 | } |
| 768 | |
| 769 | /* now do pumping of atom by Lya */ |
| 770 | FeIILyaPump(); |
| 771 | |
| 772 | /* ************************************************************************** |
| 773 | * |
| 774 | * final rates into matrix |
| 775 | * |
| 776 | ***************************************************************************/ |
| 777 | |
| 778 | /* fill in xMatrix with matrix elements */ |
| 779 | for( n=0; n<FeII.nFeIILevel; ++n) |
| 780 | { |
| 781 | /* all processes leaving level n going down*/ |
| 782 | for( ipLo=0; ipLo<n; ++ipLo ) |
| 783 | { |
| 784 | xMatrix[n][n] = xMatrix[n][n] + Fe2CPump[n][ipLo] + Fe2LPump[n][ipLo]+ Fe2A[n][ipLo] + |
| 785 | Fe2Coll[n][ipLo]*dense.eden; |
| 786 | } |
| 787 | /* all processes leaving level n going up*/ |
| 788 | for( ipHi=n+1; ipHi<FeII.nFeIILevel; ++ipHi ) |
| 789 | { |
| 790 | xMatrix[n][n] = xMatrix[n][n] + Fe2CPump[n][ipHi] + Fe2LPump[n][ipHi] + Fe2Coll[n][ipHi]*dense.eden; |
| 791 | } |
| 792 | /* all processes entering level n from below*/ |
| 793 | for( ipLo=0; ipLo<n; ++ipLo ) |
| 794 | { |
| 795 | xMatrix[ipLo][n] = xMatrix[ipLo][n] - Fe2CPump[ipLo][n] - Fe2LPump[ipLo][n] - Fe2Coll[ipLo][n]*dense.eden; |
| 796 | } |
| 797 | /* all processes entering level n from above*/ |
| 798 | for( ipHi=n+1; ipHi<FeII.nFeIILevel; ++ipHi ) |
| 799 | { |
| 800 | xMatrix[ipHi][n] = xMatrix[ipHi][n] - Fe2CPump[ipHi][n] - Fe2LPump[ipHi][n] - Fe2Coll[ipHi][n]*dense.eden - |
| 801 | Fe2A[ipHi][n]; |
| 802 | } |
| 803 | |
| 804 | /* the top row of the matrix is the sum of level populations */ |
| 805 | xMatrix[n][0] = 1.0; |
| 806 | } |
| 807 | |
| 808 | { |
| 809 | /* option to print out entire matrix */ |
| 810 | enum {DEBUG_LOC=false}; |
| 811 | if( DEBUG_LOC ) |
| 812 | { |
| 813 | /* print the matrices */ |
| 814 | for( n=0; n<FeII.nFeIILevel; ++n) |
| 815 | { |
| 816 | /*fprintf(ioQQQ,"\n");*/ |
| 817 | /* now print the matrix*/ |
| 818 | for( ipLo=0; ipLo<FeII.nFeIILevel; ++ipLo ) |
| 819 | { |
| 820 | fprintf(ioQQQ," %.1e", xMatrix[n][ipLo]); |
| 821 | } |
| 822 | fprintf(ioQQQ,"\n"); |
| 823 | } |
| 824 | } |
| 825 | } |
| 826 | |
| 827 | /* define the Y Vector. The oth element is the sum of all level populations |
| 828 | * adding up to the total population. The remaining elements are the level |
| 829 | * balance equations adding up to zero */ |
| 830 | yVector[0] = 1.0; |
| 831 | for( n=1; n < FeII.nFeIILevel; n++ ) |
| 832 | { |
| 833 | yVector[n] = 0.0; |
| 834 | } |
| 835 | |
| 836 | /* create the 1-yVector array that will save vector, |
| 837 | * this is the macro trick */ |
| 838 | # ifdef AMAT |
| 839 | # undef AMAT |
| 840 | # endif |
| 841 | # define AMAT(I_,J_) (*(amat+(I_)*FeII.nFeIILevel+(J_))) |
| 842 | |
| 843 | /* copy current contents of xMatrix array over to special amat array*/ |
| 844 | for( ipHi=0; ipHi < FeII.nFeIILevel; ipHi++ ) |
| 845 | { |
| 846 | for( i=0; i < FeII.nFeIILevel; i++ ) |
| 847 | { |
| 848 | AMAT(i,ipHi) = xMatrix[i][ipHi]; |
| 849 | } |
| 850 | } |
| 851 | |
| 852 | info = 0; |
| 853 | |
| 854 | /* do the linear algebra to find the level populations */ |
| 855 | getrf_wrapper(FeII.nFeIILevel, FeII.nFeIILevel, amat, FeII.nFeIILevel, ipiv, &info); |
| 856 | getrs_wrapper('N', FeII.nFeIILevel, 1, amat, FeII.nFeIILevel, ipiv, yVector, FeII.nFeIILevel, &info); |
| 857 | |
| 858 | if( info != 0 ) |
| 859 | { |
| 860 | fprintf( ioQQQ, "DISASTER FeIILevelPops: dgetrs finds singular or ill-conditioned matrix\n" ); |
| 861 | cdEXIT(EXIT_FAILURE); |
| 862 | } |
| 863 | |
| 864 | /* yVector now contains the level populations */ |
| 865 | |
| 866 | /* this better be false after this loop - if not then non-positive level pops */ |
| 867 | lgPopNeg = false; |
| 868 | /* copy all level pops over to Fe2LevelPop */ |
| 869 | for( ipLo=0; ipLo < FeII.nFeIILevel; ipLo++ ) |
| 870 | { |
| 871 | if(yVector[ipLo] < 0. ) |
| 872 | { |
| 873 | lgPopNeg = true; |
| 874 | fprintf(ioQQQ,"PROBLEM FeIILevelPops finds non-positive level population, level is %ld pop is %g\n", |
| 875 | ipLo , yVector[ipLo] ); |
| 876 | } |
| 877 | /* this is now correct level population, cm^-3 */ |
| 878 | Fe2LevelPop[ipLo] = yVector[ipLo] * dense.xIonDense[ipIRON][1]; |
| 879 | } |
| 880 | if( lgPopNeg ) |
| 881 | { |
| 882 | /* this is here to use the lgPopNeg value for something, if not here then |
| 883 | * lint and some compilers will note that var is never used */ |
| 884 | fprintf(ioQQQ , "PROBLEM FeIILevelPops exits with negative level populations.\n"); |
| 885 | } |
| 886 | |
| 887 | /* >>chng 06 jun 24, make sure remainder of populations up through max |
| 888 | * limit are zero - this makes safe the case where the number |
| 889 | * of levels actually computed has been trimmed down from largest |
| 890 | * possible number of levels, for instance, in cool gas */ |
| 891 | for( ipLo=FeII.nFeIILevel; ipLo < FeII.nFeIILevelAlloc; ++ipLo ) |
| 892 | { |
| 893 | Fe2LevelPop[ipLo] = 0.; |
| 894 | } |
| 895 | |
| 896 | /* now set line opacities, intensities, and level populations |
| 897 | * >>chng 06 jun ipLo should go up to FeII.nFeIILevel-1 since this |
| 898 | * is the largest lower level with non-zero population */ |
| 899 | for( ipLo=0; ipLo < (FeII.nFeIILevel - 1); ipLo++ ) |
| 900 | { |
| 901 | /* >>chng 06 jun 24, upper level should go to limit |
| 902 | * of all that were allocated */ |
| 903 | /*for( ipHi=ipLo+1; ipHi < FeII.nFeIILevel; ipHi++ )*/ |
| 904 | for( ipHi=ipLo+1; ipHi < FeII.nFeIILevelAlloc; ipHi++ ) |
| 905 | { |
| 906 | /* >>chng 06 jun 24, in all of these the product |
| 907 | * yVector[ipHi]*dense.xIonDense[ipIRON][1] has been replaced |
| 908 | * with Fe2LevelPop[ipLo] - should always have been this way, |
| 909 | * and saves a mult */ |
| 910 | Fe2LevN[ipHi][ipLo].Emis->PopOpc = (Fe2LevelPop[ipLo] - |
| 911 | Fe2LevelPop[ipHi]*Fe2LevN[ipHi][ipLo].Lo->g/F |
