prt_lines_hydro.cpp

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/* This file is part of Cloudy and is copyright (C)1978-2013 by Gary J. Ferland and
 * others.  For conditions of distribution and use see copyright notice in license.txt */
/*lines_hydro put H-like iso sequence into line intensity stack */
#include "cddefines.h"
#include "atmdat.h"
#include "dense.h"
#include "prt.h"
#include "hydrogenic.h"
#include "iso.h"
#include "rfield.h"
#include "geometry.h"
#include "lines.h"
#include "lines_service.h"
#include "phycon.h"
#include "radius.h"
#include "secondaries.h"
#include "taulines.h"
#include "trace.h"
 
void lines_hydro(void)
{
        long ipISO = ipH_LIKE;
        long int i, nelem, ipHi, ipLo;
        char chLabel[5]="    ";
 
        double hbetab, 
                em , 
                pump ,
                caseb;
 
        DEBUG_ENTRY( "lines_hydro()" );
 
        if( trace.lgTrace )
                fprintf( ioQQQ, "   lines_hydro called\n" );
 
        // this can be changed with the atom levels command but must be at least 3
        ASSERT( iso_sp[ipH_LIKE][ipHYDROGEN].n_HighestResolved_max >= 3 );
        ASSERT( iso_sp[ipH_LIKE][ipHELIUM].n_HighestResolved_max >= 3 );
 
        i = StuffComment( "H-like iso-sequence" );
        linadd( 0., (realnum)i , "####", 'i',
                " start H -like iso sequence ");
 
        linadd(MAX2(0.,iso_sp[ipH_LIKE][ipHYDROGEN].xLineTotCool),0,"H1 c",'c',
                "  total collisional cooling due to all hydrogen lines ");
 
        linadd(MAX2(0.,-iso_sp[ipH_LIKE][ipHYDROGEN].xLineTotCool),0,"H1 h",'h' ,
                "  total collisional heating due to all hydrogen lines ");
 
        linadd(MAX2(0.,iso_sp[ipH_LIKE][ipHELIUM].xLineTotCool),0,"He2c",'c',
                "  total collisional cooling due to all HeII lines ");
 
        linadd(MAX2(0.,-iso_sp[ipH_LIKE][ipHELIUM].xLineTotCool),0,"He2h",'h'   ,
                "  total collisional heating due to all HeII lines ");
 
        /*fprintf(ioQQQ," debugg\t%.2e\t%.2e\t%.2e\n", 
                radius.drad,
                iso_sp[ipH_LIKE][ipHYDROGEN].xLineTotCool , 
                iso_sp[ipH_LIKE][ipHYDROGEN].cLya_cool);*/
 
        /* >>chng 95 jun 25 changed from info to cooling to pick this up in primal.in   */
        linadd(MAX2(0.,iso_sp[ipH_LIKE][ipHYDROGEN].cLya_cool),1216,"Cool",'i',
                "collisionally excited La cooling ");
 
        linadd(MAX2(0.,-iso_sp[ipH_LIKE][ipHYDROGEN].cLya_cool),1216,"Heat",'i',
                "  collisionally de-excited La heating ");
 
        linadd(MAX2(0.,iso_sp[ipH_LIKE][ipHYDROGEN].cLyrest_cool),960,"Crst",'i',
                "  cooling due to n>2 Lyman lines ");
 
        linadd(MAX2(0.,-iso_sp[ipH_LIKE][ipHYDROGEN].cLyrest_cool),960,"Hrst",'i',
                "  heating due to n>2 Lyman lines ");
 
        linadd(MAX2(0.,iso_sp[ipH_LIKE][ipHYDROGEN].cBal_cool),4861,"Crst",'i',
                "  cooling due to n>3 Balmer lines ");
 
        linadd(MAX2(0.,-iso_sp[ipH_LIKE][ipHYDROGEN].cBal_cool),4861,"Hrst",'i',
                "  heating due to n>3 Balmer lines ");
 
        linadd(MAX2(0.,iso_sp[ipH_LIKE][ipHYDROGEN].cRest_cool),0,"Crst",'i',
                "  cooling due to higher Paschen lines ");
 
        linadd(MAX2(0.,-iso_sp[ipH_LIKE][ipHYDROGEN].cRest_cool),0,"Hrst",'i',
                "  heating due to higher Paschen lines ");
 
        /* remember largest fractional ionization of H due to secondaries */
        secondaries.SecHIonMax = MAX2( secondaries.SecHIonMax , secondaries.sec2total );
 
        /* remember fraction of H ionizations due to ct */
        atmdat.HIonFracMax = MAX2( atmdat.HIonFracMax, atmdat.HIonFrac);
 
        /* remember largest fraction of thermal collisional ionization of H ground state */
        hydro.HCollIonMax = 
                (realnum)MAX2( hydro.HCollIonMax , hydro.H_ion_frac_collis );
 
        linadd(secondaries.x12tot*iso_sp[ipH_LIKE][ipHYDROGEN].st[ipH1s].Pop()*1.634e-11,1216,"LA X" ,'i',
                "Lyaa contribution from suprathermal secondaries from ground ");
 
        /* factor of 0.4836 is ratio of A(4-2)/(A(4-3)+A(4-2))
         * the IPLNPUMP is the actual pumping rate per atom */
        /* H-beta produced by continuum pumping in optically thin ld limit */
        pump = (double)(iso_sp[ipH_LIKE][ipHYDROGEN].trans(ipH4p,ipH1s).Emis().pump()*iso_sp[ipH_LIKE][ipHYDROGEN].st[ipH1s].Pop()*4.09e-12*0.4836);
        linadd(pump,4861,"Pump",'r',
                   "part of Hbeta formed by continuum pumping");
 
        linadd(MAX2(0.,iso_sp[ipH_LIKE][ipHYDROGEN].coll_ion),0,"CION",'c',
                "collision ionization cooling of hydrogen ");
 
        linadd(MAX2(-iso_sp[ipH_LIKE][ipHYDROGEN].coll_ion,0.),0,"3bHt",'h',
                "  this is the heating due to 3-body recombination ");
 
        linadd(MAX2(0.,iso_sp[ipH_LIKE][ipHELIUM].coll_ion),0,"He2C",'c',
                "collision ionization cooling of He+ ");
 
        linadd(MAX2(-iso_sp[ipH_LIKE][ipHELIUM].coll_ion,0.),0,"He2H",'h',
                "  this is the heating due to 3-body recombination onto He+");
 
        fixit();  //why is there a zero here?
        linadd(iso_sp[ipH_LIKE][ipHYDROGEN].st[ipH2p].Pop()*0.*iso_sp[ipH_LIKE][ipHYDROGEN].ex[ipH2p][ipH1s].pestrk*1.634e-11,1216,"Strk",'i',
          "  Stark broadening contribution to line ");
 
        linadd(iso_sp[ipH_LIKE][ipHYDROGEN].st[ipH3s].Pop()*iso_sp[ipH_LIKE][ipHYDROGEN].ex[ipH3s][ipH2p].pestrk*3.025e-12,
          6563,"Strk",'i',
          "  Stark broadening contribution to line ");
 
        linadd(iso_sp[ipH_LIKE][ipHYDROGEN].st[ipH4s].Pop()*iso_sp[ipH_LIKE][ipHYDROGEN].ex[ipH4s][ipH2p].pestrk*4.084e-12,
          4861,"Strk",'i',
          "Stark broadening contribution to line ");
 
        linadd(iso_sp[ipH_LIKE][ipHYDROGEN].st[ipH4p].Pop()*iso_sp[ipH_LIKE][ipHYDROGEN].ex[ipH4p][ipH3s].pestrk*1.059e-12,
          18751,"Strk",'i',
                   " Stark broadening contribution to line ");
 
        /* pestrk[5,4] is A[4,5]*pest[4,5] 
         * Stark broadening contribution to line */
        if( iso_sp[ipH_LIKE][ipHYDROGEN].n_HighestResolved_max >= 5 )
        {
                long ip5p = iso_sp[ipH_LIKE][ipHYDROGEN].QuantumNumbers2Index[5][1][2];
                linadd(iso_sp[ipH_LIKE][ipHYDROGEN].st[ip5p].Pop()*iso_sp[ipH_LIKE][ipHYDROGEN].ex[ip5p][ipH4s].pestrk*4.900e-13,40512,"Strk",'i',
                        "Stark broadening part of line");
        }
        /* this can fail if RT_line_all never updates the ots rates, a logic error,
         * but only assert this during actual calculation (ipass>0), */
        ASSERT( LineSave.ipass  <1 ||
                iso_sp[ipH_LIKE][ipHYDROGEN].trans(ipH2p,ipH1s).Emis().ots()>= 0.);
 
        linadd(iso_sp[ipH_LIKE][ipHYDROGEN].trans(ipH2p,ipH1s).Emis().ots()*iso_sp[ipH_LIKE][ipHYDROGEN].trans(ipH2p,ipH1s).EnergyErg(), 1216,"Dest",'i',
                "  portion of line lost due to absorp by background opacity ");
 
        /* portion of line lost due to absorb by background opacity */
        linadd(iso_sp[ipH_LIKE][ipHYDROGEN].trans(ipH3p,ipH2s).Emis().ots()*iso_sp[ipH_LIKE][ipHYDROGEN].trans(ipH3p,ipH2s).EnergyErg(), 6563,"Dest",'i',
                "Ha destroyed by background opacity");
 
        /* portion of line lost due to absorp by background opacity */
        if( iso_sp[ipH_LIKE][ipHYDROGEN].n_HighestResolved_max >= 5 )
        {
                long ip5p = iso_sp[ipH_LIKE][ipHYDROGEN].QuantumNumbers2Index[5][1][2];
                linadd(iso_sp[ipH_LIKE][ipHYDROGEN].trans(ip5p,ipH4s).Emis().ots()*iso_sp[ipH_LIKE][ipHYDROGEN].trans(ip5p,ipH4s).EnergyErg(),40516, "Dest",'i',
                        "portion of line lost due to absorb by background opacity");
        }
 
        /* portion of line lost due to absorb by background opacity */
        if( iso_sp[ipH_LIKE][ipHYDROGEN].numLevels_max > ipH4p )
                linadd(iso_sp[ipH_LIKE][ipHYDROGEN].trans(ipH4p,ipH2s).Emis().ots()*iso_sp[ipH_LIKE][ipHYDROGEN].trans(ipH4p,ipH2s).EnergyErg(), 4861,"Dest",'i',
                        "portion of line lost due to absorb by background opacity");
 
        /* portion of line lost due to absorb by background opacity */
        if( iso_sp[ipH_LIKE][ipHYDROGEN].numLevels_max > ipH4p )
                linadd(iso_sp[ipH_LIKE][ipHYDROGEN].trans(ipH4p,ipH3s).Emis().ots()*iso_sp[ipH_LIKE][ipHYDROGEN].trans(ipH4p,ipH3s).EnergyErg() ,18751, "Dest",'i',
                        "portion of line lost due to absorb by background opacity");
 
        linadd(iso_sp[ipH_LIKE][ipHYDROGEN].st[ipH2p].Pop()*iso_sp[ipH_LIKE][ipHYDROGEN].trans(ipH2p,ipH1s).Emis().Aul()*
                hydro.dstfe2lya*iso_sp[ipH_LIKE][ipHYDROGEN].trans(ipH2p,ipH1s).EnergyErg() , 1216 , "Fe 2" , 'i',
                "Ly-alpha destroyed by overlap with FeII " );
 
        linadd(iso_sp[ipH_LIKE][ipHYDROGEN].RadRec_caseB*dense.xIonDense[ipHYDROGEN][1]*dense.eden * 1.64e-11,1216,"Ca B",'i',
                " simple high-density case b intensity of Ly-alpha, no two photon ");
 
        /* these entries only work correctly if the APERTURE command is not in effect */
        if( geometry.iEmissPower == 2 )
        {
                /* H-beta computed from Q(H) and specified covering factor */
                if( nzone == 1 )
                {
                        /* evaluate the case b emissivity by interpolating on the hummer & storey tables */
                        caseb = rfield.qhtot*
                                atmdat_HS_caseB( 4 , 2 , 1 , phycon.te , dense.eden, 'b' ) / iso_sp[ipH_LIKE][ipHYDROGEN].RadRec_caseB;
                        /* the atmdat_HS_caseB returned -1 if the physical conditions were outside range of validity.  
                         * In this case use simple approximation with no temperature or density dependence */
                        if( caseb < 0 )
                        {
                                caseb = rfield.qhtot*4.75e-13;
                        }
                        LineSv[LineSave.nsum].SumLine[0] = 0.;
                        LineSv[LineSave.nsum].SumLine[1] = 0.;
                }
                else
                {
                        caseb = 0.;
                }
                /* H-beta computed from Q(H) and specified covering factor */
                linadd( caseb/radius.dVeffAper*geometry.covgeo , 4861 , "Q(H)" , 'i' ,
                        "Case B H-beta computed from Q(H) and specified covering factor");
 
                if( nzone == 1 )
                {
                        // the cast to double prevents an FPE with Solaris Studio 12.4 (limit_compton_hi_t.in)
                        caseb = rfield.qhtot*double(iso_sp[ipH_LIKE][ipHYDROGEN].trans(ipH2p,ipH1s).EnergyErg());
                        LineSv[LineSave.nsum].SumLine[0] = 0.;
                        LineSv[LineSave.nsum].SumLine[1] = 0.;
                }
                else
                {
                        caseb = 0.;
                }
                /* >>chng 02 nov 05, better approximation for Lya for temperature of first zone */
                linadd( caseb/radius.dVeffAper*geometry.covgeo , 1216 , "Q(H)" , 'i',
                        "Ly-alpha from Q(H), high-dens lim, specified covering factor" );
        }
 
        /* this is the main printout, where line intensities are entered into the stack */
        for( nelem=ipISO; nelem < LIMELM; nelem++ )
        {
                if( dense.lgElmtOn[nelem] )
                {
                        ASSERT( iso_sp[ipH_LIKE][nelem].n_HighestResolved_max >= 3 );
 
                        for( ipHi=1; ipHi < iso_sp[ipISO][nelem].numLevels_max; ipHi++ )
                        {
                                for( ipLo=0; ipLo < ipHi; ipLo++ )
                                {
                                        if( iso_sp[ipISO][nelem].trans(ipHi,ipLo).Emis().Aul() <= iso_ctrl.SmallA )
                                                continue;
 
                                        /* this is in real units not emissivity*/
                                        iso_sp[ipISO][nelem].trans(ipHi,ipLo).Emis().phots() = 
                                                iso_sp[ipISO][nelem].trans(ipHi,ipLo).Emis().Aul()*
                                                iso_sp[ipISO][nelem].st[ipHi].Pop()*
                                                (iso_sp[ipISO][nelem].trans(ipHi,ipLo).Emis().Pesc() +
                                                iso_sp[ipISO][nelem].trans(ipHi,ipLo).Emis().Pelec_esc() );
 
                                        /* now find line intensity  */
                                        iso_sp[ipISO][nelem].trans(ipHi,ipLo).Emis().xIntensity() = 
                                                iso_sp[ipISO][nelem].trans(ipHi,ipLo).Emis().phots()*
                                                iso_sp[ipISO][nelem].trans(ipHi,ipLo).EnergyErg();
                                }
                        }
                }
        }
 
        /* create emissivity or intensity for hydrogenic species,
         * first combine/bring balmer series together */
        for( nelem=0; nelem < LIMELM; nelem++ )
        {
                if( dense.IonHigh[nelem] == nelem + 1 )
                {
                        /* bring nL - n'L' emission together as n-n' emission. */
                        for( ipHi=1; ipHi < iso_sp[ipH_LIKE][nelem].numLevels_max; ipHi++ )
                        {
                                long index_of_nHi_P;
 
                                /* is ipHi is collapsed level, index_of_nHi_P is ipHi */
                                if( N_(ipHi) > iso_sp[ipH_LIKE][nelem].n_HighestResolved_max )
                                        index_of_nHi_P = ipHi;
                                else
                                        index_of_nHi_P = iso_sp[ipH_LIKE][nelem].QuantumNumbers2Index[ N_(ipHi) ][1][2];
 
                                /* only need to consider resolved lower level here */
                                for( ipLo=0; ipLo < ipHi; ipLo++ )
                                {       
                                        long index_of_nLo_S = iso_sp[ipH_LIKE][nelem].QuantumNumbers2Index[ N_(ipLo) ][0][2];
 
                                        /* jump out if ipLo is collapsed 
                                         * NB this must be up to n_HighestResolved_local and not n_HighestResolved_max */
                                        if( N_(ipLo) > iso_sp[ipH_LIKE][nelem].n_HighestResolved_local || N_(ipLo) == N_(ipHi) )
                                                break;
 
                                        if( iso_sp[ipH_LIKE][nelem].trans(ipHi,ipLo).Emis().Aul() <= iso_ctrl.SmallA )
                                                continue;
 
                                        /* add everything into nP - n'S, skip if current indices are those levels. */
                                        if( ipHi == index_of_nHi_P && ipLo == index_of_nLo_S )
                                                continue;
                                        else
                                        {
                                                /* add resolved line to nP - n'S */
                                                iso_sp[ipH_LIKE][nelem].trans(index_of_nHi_P,index_of_nLo_S).Emis().xIntensity() +=
                                                        iso_sp[ipH_LIKE][nelem].trans(ipHi,ipLo).Emis().xIntensity();
                                                /* zero out the resolved line */
                                                iso_sp[ipH_LIKE][nelem].trans(ipHi,ipLo).Emis().xIntensity() = 0;
                                                //ASSERT( iso_sp[ipH_LIKE][nelem].trans(index_of_nHi_P,index_of_nLo_S).Emis().xIntensity() > 0. );
                                        }
                                }
                        }
                }
        }
 
        /* H beta recombination, assuming old case B */
        hbetab = (double)((pow(10.,-20.89 - 0.10612*POW2(phycon.alogte - 4.4)))/
          phycon.te);
        /* need to pass this assert if CaBo is to have valid array indices for ipCont */
        /* 06 aug 28, from numLevels_max to _local. */
        /* 06 dec 21, change from numLevels_max to _local was mistake for this entire file.  Undo. */
        ASSERT( iso_sp[ipH_LIKE][ipHYDROGEN].numLevels_max > 4 );
        hbetab *= dense.xIonDense[ipHYDROGEN][1]*dense.eden;
 
        lindst(hbetab, -4861 ,"CaBo",
                1 ,'i',false,
                " this is old case b based on Ferland (1980) PASP ");
 
        if( dense.lgElmtOn[ipHELIUM] )
        {
                /* need to pass this assert if CaBo is to have valid array indices for ipCont */
                /* 06 aug 28, from numLevels_max to _local. */
                /* 06 dec 21, change from numLevels_max to _local was mistake for this entire file.  Undo. */
                ASSERT( iso_sp[ipH_LIKE][ipHELIUM].numLevels_max > 4 );
                /* 1640 1640 1640 */
                em = 2.03e-20/(phycon.te70*phycon.te10*phycon.te03);
                em *= dense.xIonDense[ipHELIUM][2]*dense.eden;
 
                lindst(em,-1640,"CaBo",
                        1,'i',false,
                        " old prediction of He II 1640, Case B at low densities");
 
                /* hydrogenic helium */
                /* old prediction of He II 4686, case B */
                em = 2.52e-20/(pow(phycon.te,1.05881));
                em *= dense.xIonDense[ipHELIUM][2]*dense.eden;
 
                lindst(em,-4686,"CaBo", 1,'i',false,
                           " old prediction of He II 4686, Case B at low densities");
        }
 
        /* predict case b intensities of hydrogen lines */
        if( LineSave.ipass <= 0 )
        {
                for(nelem=0; nelem<HS_NZ; ++nelem )
                {
                        atmdat.lgHCaseBOK[0][nelem] = true;
                        atmdat.lgHCaseBOK[1][nelem] = true;
                }
        }
        /* this is the main printout, where line intensities are entered into the stack */
        for( nelem=0; nelem < LIMELM; nelem++ )
        {
                if( dense.lgElmtOn[nelem] )
                {
                        /* HS_NZ is limit to charge of elements in HS predictions, now 8 == oxygen */
                        /* but don't do the minor elements - these were not read in and so should not be
                         * printed - remove equivalent if statement in createdata to read them in */
                        if( nelem < HS_NZ && (nelem<2 || nelem>4) )
                        {
                                int iCase;
                                for( iCase=0; iCase<2; ++iCase )
                                {
                                        char chAB[2]={'A','B'};
                                        char chLab[5]="Ca  ";
 
                                        /* adding iCase means start from n=1 for case A, n=2 for Case B,
                                         * note that principal quantum number is on physics scale, not C */
                                        /* 06 aug 28, both of these from numLevels_max to _local. */
                                        /* 06 dec 21, change from numLevels_max to _local was mistake for this entire file.  Undo. */
                                        for( ipLo=1+iCase; ipLo<MIN2(10,iso_sp[ipH_LIKE][nelem].n_HighestResolved_max + iso_sp[ipH_LIKE][nelem].nCollapsed_max); ++ipLo )
                                        {
                                                for( ipHi=ipLo+1; ipHi< MIN2(25,iso_sp[ipH_LIKE][nelem].n_HighestResolved_max + iso_sp[ipH_LIKE][nelem].nCollapsed_max+1); ++ipHi )
                                                {
                                                        realnum wl;
                                                        double case_b_Intensity;
                                                        long int ipCHi , ipCLo;
                                                        /* Put case b predictions into line stack
                                                         * NB NB NB each Hummer & Storey case b line must be 
                                                         * explicitly clobbered by hand in routine final if 
                                                         * atmdat.lgHCaseBOK[iCase][nelem] flag is set false
                                                         * since this indicates that we exceeded bounds of table,
                                                         * DO NOT want to print lines in that case */
 
                                                        /* first do case b emissivity of balmer lines */
 
                                                        /* get HS predictions */
                                                        case_b_Intensity = atmdat_HS_caseB( ipHi,ipLo , nelem+1, phycon.te , dense.eden, chAB[iCase] );
                                                        if( case_b_Intensity<=0. )
                                                        {
                                                                atmdat.lgHCaseBOK[iCase][nelem] = false;
                                                                case_b_Intensity = 0.;
                                                        }
 
                                                        case_b_Intensity *= dense.xIonDense[nelem][nelem+1-ipISO]*dense.eden;
 
                                                        if( iCase==0 && ipLo==1 )
                                                        {
                                                                /* get physical scal prin quant numbers onto cloudy c scale */
                                                                ipCHi = ipHi;
                                                                ipCLo = 0;
                                                        }
                                                        else
                                                        {
                                                                /* get physical scal prin quant numbers onto cloudy c scale */
                                                                ipCHi = ipHi;
                                                                ipCLo = ipLo;
                                                        }
 
                                                        /* make label either Ca A or Ca B */
                                                        chLab[3] = chAB[iCase];
 
                                                        /* new treatment is different from old for indices greater than 2. */
                                                        if( ipCHi > 2 )
                                                        {
                                                                if( ipCLo >  2 )
                                                                {
                                                                        /* if both indices above two, just treat as nP to n'S transition. */
                                                                        ipCHi = iso_sp[ipH_LIKE][nelem].QuantumNumbers2Index[ipCHi][1][2];
                                                                        ipCLo = iso_sp[ipH_LIKE][nelem].QuantumNumbers2Index[ipCLo][0][2];
                                                                }
                                                                else if(  ipCLo ==  2 )
                                                                {
                                                                        /* treat as nS to 2P transition. */
                                                                        ipCHi = iso_sp[ipH_LIKE][nelem].QuantumNumbers2Index[ipCHi][0][2];
                                                                }
                                                                else if( ipCLo ==  1 || ipCLo == 0 )
                                                                {
                                                                        /* treat as nP to n'S transition. */
                                                                        ipCHi = iso_sp[ipH_LIKE][nelem].QuantumNumbers2Index[ipCHi][1][2];
                                                                }
                                                        }
 
                                                        /* this is wavelength of interpolated case b from HS tables */
                                                        wl = iso_sp[ipH_LIKE][nelem].trans(ipCHi,ipCLo).WLAng();
                                                        atmdat.WaveLengthCaseB[nelem][ipHi][ipLo] = wl;
 
                                                        lindst(case_b_Intensity,wl,chLab,iso_sp[ipH_LIKE][nelem].trans(ipCHi,ipCLo).ipCont(),'i',false,
                                                                " case a or case b from Hummer & Storey tables" );
                                                }
                                        }
                                }
                        }
 
                        // add two-photon details here
                        if( LineSave.ipass == 0 )
                        {
                                /* chIonLbl is function that generates a null terminated 4 char string, of form "C  2" 
                                 * the result, chLable, is only used when ipass == 0, can be undefined otherwise */
                                chIonLbl(chLabel, nelem+1, nelem+1-ipISO);
                        }
                        for( vector<two_photon>::iterator tnu = iso_sp[ipH_LIKE][nelem].TwoNu.begin(); tnu != iso_sp[ipH_LIKE][nelem].TwoNu.end(); ++tnu )
                        {
                                fixit(); // This was multiplied by Pesc when treated as a line, now what?  Only used for printout?
                                fixit(); // below should be 'i' instead of 'r' ?
                                linadd( tnu->AulTotal * tnu->E2nu * EN1RYD * (*tnu->Pop), 
                                         0, chLabel, 'r',
                                        " two photon continuum ");
 
                                linadd( tnu->induc_dn * tnu->E2nu * EN1RYD * (*tnu->Pop), 
                                        22, chLabel ,'i',
                                        " induced two photon emission ");
                        }
 
                        /* NB NB - low and high must be in this order so that all balmer, paschen,
                         * etc series line up correctly in final printout */
                        for( ipLo=ipH1s; ipLo < iso_sp[ipH_LIKE][nelem].numLevels_max-1; ipLo++ )
                        {
                                /* don't bother with decays to 2p since we set them to zero above */
                                if( ipLo==ipH2p )
                                        continue;
 
                                /* set number of levels we want to print, first is default,
                                 * only print real levels, second is set with "print line
                                 * iso collapsed" command */
                                long int nLoop  = iso_sp[ipH_LIKE][nelem].numLevels_max - iso_sp[ipH_LIKE][nelem].nCollapsed_max;
                                if( prt.lgPrnIsoCollapsed )
                                        nLoop  = iso_sp[ipH_LIKE][nelem].numLevels_max;
 
                                for( ipHi=ipLo+1; ipHi < nLoop; ipHi++ )
                                {
                                        // skip non-radiative transitions
                                        if( iso_sp[ipH_LIKE][nelem].trans(ipHi,ipLo).ipCont() < 1 )
                                                continue;
 
                                        // skip 2s-1s, so that 2p-1s comes first and cdLine finds LyA instead of the M2 transition.     
                                        if( ipHi==1 && ipLo==0 )
                                                continue;
 
                                        char chComment[23];
                                        GenerateTransitionConfiguration( iso_sp[ipH_LIKE][nelem].trans(ipHi,ipLo), chComment);
                                        fixit(); // put chComment instead of the below, cant just punt chComment there.
                                        PutLine(iso_sp[ipH_LIKE][nelem].trans(ipHi,ipLo),
                                                "predicted line, all processes included");
                                }
 
                                // now add 2s-1s M2 transition
                                if( ipLo==0 )
                                {
                                        ipHi=1;
                                        char chComment[23];
                                        GenerateTransitionConfiguration( iso_sp[ipH_LIKE][nelem].trans(ipHi,ipLo), chComment);
                                        fixit(); // put chComment instead of the below, cant just punt chComment there.
                                        PutLine(iso_sp[ipH_LIKE][nelem].trans(ipHi,ipLo),
                                                "predicted line, all processes included");
                                }
                        }
                }
        }
        
        if( trace.lgTrace )
        {
                fprintf( ioQQQ, "   lines_hydro returns\n" );
        }
        return;
}