* * $Id: colisn.F,v 1.1.1.1 1995/10/24 10:21:56 cernlib Exp $ * * $Log: colisn.F,v $ * Revision 1.1.1.1 1995/10/24 10:21:56 cernlib * Geant * * #include "geant321/pilot.h" *CMZ : 3.21/04 23/02/95 14.46.01 by S.Giani *-- Author : SUBROUTINE COLISN(D,LD,IGAMS,LGAM,INABS,LNAB,ITHRMS,LTHRM, + IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR,Q,NSEI,NAEI,NMT2,NMT4, + NMT16,NMT17,NMT18,NMT22,NMT23,NMT24,NMT28,NMT51,NMT91, + NMT102,NMT103,NMT104,NMT105,NMT106,NMT107,NMT108,NMT109, + NMT111,NMT112,NMT113,NMT114,IGCBS2,LGCB2,KZ,LR,QLR, + IIN,IIM) C THIS ROUTINE IS CALLED AT EACH COLLISION TO C DETERMINE THE POST COLLISION PARAMETERS #include "geant321/minput.inc" #include "geant321/mconst.inc" #include "geant321/mnutrn.inc" #include "geant321/mapoll.inc" #include "geant321/mcross.inc" #include "geant321/mmass.inc" #include "geant321/mupsca.inc" #include "geant321/mpstor.inc" #include "geant321/mmicab.inc" DIMENSION D(*),LD(*),IGAMS(*),LGAM(*),INABS(*),LNAB(*), + ITHRMS(*),LTHRM(*),IDICTS(NNR,NNUC),LDICT(NNR,NNUC),NTX(*), + NTS(*),IGCBS(NGR,NNUC),LGCB(NGR,NNUC),AWR(*),Q(NQ,NNUC), + NSEI(*),NAEI(*),NMT2(*),NMT4(*),NMT16(1),NMT17(*),NMT18(*), + NMT22(*),NMT23(*),NMT24(*),NMT28(*),NMT51(*),NMT91(*), + NMT102(*),NMT103(*),NMT104(*),NMT105(*),NMT106(*),NMT107(*), + NMT108(*),NMT109(*),NMT111(*),NMT112(*),NMT113(*),NMT114(*), + IGCBS2(NGR,NNUC),LGCB2(NGR,NNUC),KZ(*),LR(NQ,NNUC),QLR(NQ,NNUC), + FM(MAXNEU) C CHARACTER*80 COMM C DATA QBE8/-7.3686E+06/ SAVE CALL GTMED(NMED,MED) C INITIALIZE THE COUNTERS AND FLAGS C ITRY ALLOWS FOR MULTIPLE ATTEMPTS IF THE ENDF/B PARTIAL C CROSS SECTIONS DO NOT EXACTLY SUM TO THE TOTAL 10 ISTOP=0 ITRY=0 NCOL=NCOL+1 SIGREC=0.0 SUMREC=0.0 FSUMS = 1.0 FSUMIS = 1.0 FSUMA = 1.0 20 ID=0 MT=0 QI=0.0 LRI=0 QLRI=0.0 DO 30 I=1,MAXNEU FM(I)=1.0 30 CONTINUE DO 40 I=1,MAXNEU ENE(I)=0.0 40 CONTINUE INEU = 0 U1=0.0 V1=0.0 W1=0.0 ERFGM=0.0 IFLG=0 LIFLAG=0 AWRI=AWR(IIN) KZI=KZ(IIM) #if defined(CERNLIB_MDEBUG) PRINT *,' COLISN: A=',AWRI,' K=',KZI #endif C INITIALIZE THE CROSS SECTION VARIABLES SIGT=0.0 SIGTNS=0.0 SIGTNA=0.0 SIGNES=0.0 SIGNIS=0.0 SGNISD=0.0 SGNISC=0.0 SIGN2N=0.0 SIGN3N=0.0 SIGNNA=0.0 SGNN3A=0.0 SGN2NA=0.0 SIGNNP=0.0 SIGNF=0.0 SIGNG=0.0 SIGNP=0.0 SIGND=0.0 SIGNT=0.0 SGN3HE=0.0 SIGNA=0.0 SIGN2A=0.0 SIGN3A=0.0 SIGN2P=0.0 SIGNPA=0.0 SGNT2A=0.0 SGND2A=0.0 SUMIS=0.0 SUMS=0.0 SUMA=0.0 C DETERMINE THE TOTAL CROSS SECTION (MT-1) L1=LDICT(1,IIN) IF(L1.EQ.0)GO TO 50 LS1=IDICTS(1,IIN) + LMOX2 LEN=L1/2 CALL TBSPLT(D(LS1),E,LEN,SIGT) GO TO 60 50 CONTINUE COMM=' COLISN: TOTAL CROSS SECTION LENGTH IS ZERO' SIGREC = 0.0 SUMREC = 0.0 GOTO 980 60 CONTINUE C DETERMINE THE TOTAL NEUTRON DISAPPEARANCE (MT-102 TO MT-114 C AND MT-18) L1=LNAB(IIN) IF(L1.EQ.0)GO TO 70 LS1=INABS(IIN)+LMOX2 LEN=L1/2 CALL TBSPLT(D(LS1),E,LEN,SIGTNA) GO TO 80 70 SIGTNA=0.0 80 CONTINUE C DETERMINE THE NON-ABSORPTION PROBABILITY PNAB=1.0-SIGTNA/SIGT C DETERMINE THE COLLISION TYPE (ABSORPTION OR SCATTERING) R=FLTRNF(0) IF(R.GT.PNAB)GO TO 570 C THE REACTION TYPE IS A SCATTER NSEI(IIN)=NSEI(IIN)+1 SIGTNS=SIGT-SIGTNA R=FLTRNF(0) C DETERMINE (N,N) CROSS SECTION (MT-2) ID=2 L1=LDICT(ID,IIN) IF(L1.EQ.0)GO TO 110 LS1=IDICTS(ID,IIN)+LMOX2 LEN=L1/2 CALL TBSPLT(D(LS1),E,LEN,SIGNES) SUMS=SIGNES/SIGTNS*FSUMS IF(R.GT.SUMS)GO TO 120 C REACTION TYPE IS (N,N) NMT2(MED)=NMT2(MED)+1 C DETERMINE IF SCATTERING OCCURS IN THE THERMAL ENERGY RANGE ETHERM = 500.*8.617E-5*TEMP/AWRI IF(E.LE.ETHERM) THEN C Reaction is a thermal scatter CALL THRMSC(D,D,ITHRMS,LTHRM,E,U,V,W,TEMP,FM,AWR,IIN, + IFLG,IOUT) QI=Q(ID,IIN) CALL CMLABE(D,D,AWRI,KZI,ID,FM,QI,IFLG) EP = E VP = V UP = U WP = W AGEP = AGE MTP = 2 CALL STOPAR(IDNEU,NNEU) RETURN ENDIF C DETERMINE THE COSINE OF THE NEUTRON SCATTERING ANGLE IN THE C CENTER OF MASS COORDINATE SYSTEM L1=LDICT(67,IIN) IF(L1.EQ.0)GO TO 90 LS1=IDICTS(67,IIN)+LMOX2 LEN=L1 CALL CANGLE(D(LS1),D(LS1),E,FM(1),LEN) GO TO 100 C ASSUME ISOTROPIC IN THE CENTER OF MASS COORDINATE SYSTEM 90 R=FLTRNF(0) FM(1)=2.0*R-1.0 C DETERMINE THE EXIT COLLISION PARAMETERS IN THE LABORATORY C COORDINATE SYSTEM 100 CONTINUE QI=Q(ID,IIN) CALL CMLABE(D,D,AWRI,KZI,ID,FM(1),QI,IFLG) EP = E VP = V UP = U WP = W AGEP = AGE MTP = 2 CALL STOPAR(IDNEU,NNEU) RETURN 110 SIGNES=0.0 120 CONTINUE C DETERMINE (N,N") CROSS SECTION (MT-4) ID=3 L1=LDICT(ID,IIN) IF(L1.EQ.0)GO TO 240 LS1=IDICTS(ID,IIN)+LMOX2 LEN=L1/2 CALL TBSPLT(D(LS1),E,LEN,SIGNIS) SUMS=SUMS+SIGNIS/SIGTNS*FSUMS IF(R.GT.SUMS)GO TO 250 C REACTION TYPE IS (N,N") NMT4(MED)=NMT4(MED)+1 C DETERMINE (N,N"-DISCRETE) CROSS SECTION (MT-51 TO MT-90) R=FLTRNF(0) DO 130 I=14,53 L1=LDICT(I,IIN) IF(L1.EQ.0)GO TO 170 LS1=IDICTS(I,IIN)+LMOX2 LEN=L1/2 CALL XSECNU(D,LEN,E,SGNISD,LS1,L1) SUMIS=SUMIS+SGNISD/SIGNIS*FSUMIS IF(R.LE.SUMIS)GO TO 140 130 CONTINUE GO TO 180 140 CONTINUE C REACTION TYPE IS (N,N") DISCRETE NMT51(MED)=NMT51(MED)+1 I=I+68 C DETERMINE THE COSINE OF THE NEUTRON SCATTERING ANGLE IN THE C CENTER OF MASS COORDINATE SYSTEM L1=LDICT(I,IIN) IF(L1.EQ.0)GO TO 150 LS1=IDICTS(I,IIN)+LMOX2 LEN=L1 CALL CANGLE(D(LS1),D(LS1),E,FM(1),LEN) GO TO 160 C ASSUME ISOTROPIC IN THE CENTER OF MASS COORDINATE SYSTEM 150 R=FLTRNF(0) FM(1)=2.0*R-1.0 C DETERMINE THE EXIT COLLISION PARAMETERS IN THE LABORATORY C COORDINATE SYSTEM 160 ID=I-68 QI=Q(ID,IIN) LRI=LR(ID,IIN) QLRI=QLR(ID,IIN) CALL CMLABI(D,D,AWRI,KZI,ID,FM(1),QI,IFLG,LIFLAG,LRI) C Re-sample if no energy determined in CMLABI IF(IFLG.EQ.-1) GOTO 10 EP = E VP = V UP = U WP = W AGEP = AGE MTP = 51 CALL STOPAR(IDNEU,NNEU) IF(LRI.EQ.22)GO TO 520 IF(LRI.EQ.23)GO TO 530 IF(LRI.EQ.28)GO TO 540 CALL PHOTON(D,D,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, +IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SGNISD) RETURN 170 SGNISD=0.0 180 CONTINUE C DISCRETE INELASTIC SCATTERING LEVEL WAS NOT CHOSEN C DETERMINE (N,N"-CONTINUUM) CROSS SECTION (MT-91) ID=54 L1=LDICT(ID,IIN) IF(L1.EQ.0)GO TO 210 LS1=IDICTS(ID,IIN)+LMOX2 LEN=L1/2 CALL TBSPLT(D(LS1),E,LEN,SGNISC) SUMIS=SUMIS+SGNISC/SIGNIS*FSUMIS IF(R.GT.SUMIS)GO TO 220 C REACTION TYPE IS (N,N") CONTINUUM NMT91(MED)=NMT91(MED)+1 C DETERMINE THE COSINE OF THE NEUTRON SCATTERING ANGLE IN THE C LABORATORY COORDINATE SYSTEM L1=LDICT(122,IIN) IF(L1.EQ.0)GO TO 190 LS1=IDICTS(122,IIN)+LMOX2 LEN=L1 CALL CANGLE(D(LS1),D(LS1),E,FM(1),LEN) GO TO 200 C ASSUME ISOTROPIC IN THE LABORATORY COORDINATE SYSTEM 190 CALL GTISO(U1,V1,W1) U=U1 V=V1 W=W1 LIFLAG=1 C DETERMINE THE EXIT NEUTRON ENERGY IN THE LABORATORY C COORDINATE SYSTEM 200 L1=LDICT(133,IIN) IF(L1.EQ.0)GO TO 230 LS1=IDICTS(133,IIN)+LMOX2 CALL SECEGY(EX,D(LS1),E,D(LS1)) E=EX IFLG=1 C DETERMINE THE EXIT COLLISION PARAMETERS IN THE LABORATORY C COORDINATE SYSTEM QI=Q(ID,IIN) LRI=LR(ID,IIN) QLRI=QLR(ID,IIN) CALL CMLABI(D,D,AWRI,KZI,ID,FM(1),QI,IFLG,LIFLAG,LRI) C Re-sample if no energy determined in CMLABI IF(IFLG.EQ.-1) GOTO 10 EP = E VP = V UP = U WP = W AGEP = AGE MTP = 91 CALL STOPAR(IDNEU,NNEU) IF(LRI.EQ.22)GO TO 520 IF(LRI.EQ.23)GO TO 530 IF(LRI.EQ.28)GO TO 540 CALL PHOTON(D,D,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, +IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SGNISC) RETURN 210 SGNISC=0.0 220 CONTINUE COMM= ' COLISN: INELASTIC SCATTERING CROSS SECTION WAS NOT CHOSEN' NMT4(MED)=NMT4(MED)-1 FSUMIS = 1./SUMIS GO TO 550 230 CONTINUE COMM=' COLISN: NO SECONDARY ENERGY DISTRIBUTION WAS FOUND MT-91' ISTOP=1 GO TO 560 240 SIGNIS=0.0 250 CONTINUE C DETERMINE (N,2N) CROSS SECTION (MT-16) ID=8 L1=LDICT(ID,IIN) IF(L1.EQ.0)GO TO 290 LS1=IDICTS(ID,IIN)+LMOX2 LEN=L1/2 CALL TBSPLT(D(LS1),E,LEN,SIGN2N) SUMS=SUMS+SIGN2N/SIGTNS*FSUMS IF(R.GT.SUMS)GO TO 300 C REACTION TYPE IS (N,2N) NMT16(MED)=NMT16(MED)+1 C USE THE ONE NEUTRON EMISSION MODEL AND MULTIPLY THE C WEIGHT BY TWO C changed to 2 neutron production CZ July 30, 1992 CZ WATE=2.0*WATE C DETERMINE THE COSINE OF THE NEUTRON SCATTERING ANGLE IN THE C LABORATORY COORDINATE SYSTEM L1=LDICT(72,IIN) IF(L1.EQ.0)GO TO 260 LS1=IDICTS(72,IIN)+LMOX2 LEN=L1 C get scattering angle for 1. neutron CALL CANGLE(D(LS1),D(LS1),E,FM(1),LEN) C get scattering angle for 2. neutron CALL CANGLE(D(LS1),D(LS1),E,FM(2),LEN) GO TO 270 C ASSUME ISOTROPIC IN THE LABORATORY COORDINATE SYSTEM 260 CONTINUE IFLG=1 C DETERMINE THE EXIT NEUTRON ENERGY IN THE LABORATORY C COORDINATE SYSTEM 270 INEU = 2 L1=LDICT(123,IIN) IF(L1.EQ.0)GO TO 280 LS1=IDICTS(123,IIN)+LMOX2 CALL GETENE(E,D(LS1),D(LS1),INEU) C DETERMINE THE EXIT COLLISION PARAMETERS IN THE LABORATORY C COORDINATE SYSTEM QI=Q(ID,IIN) CALL N2NN3N(D,D,AWRI,KZI,ID,FM,QI,IFLG) CALL PHOTON(D,D,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, +IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGN2N) RETURN 280 CONTINUE COMM=' COLISN: NO SECONDARY ENERGY DISTRIBUTION WAS FOUND MT-16' ISTOP=1 GO TO 560 290 SIGN2N=0.0 300 CONTINUE C DETERMINE (N,3N) CROSS SECTION (MT-17) ID=9 L1=LDICT(ID,IIN) IF(L1.EQ.0)GO TO 350 LS1=IDICTS(ID,IIN)+LMOX2 LEN=L1/2 CALL TBSPLT(D(LS1),E,LEN,SIGN3N) SUMS=SUMS+SIGN3N/SIGTNS*FSUMS IF(R.GT.SUMS)GO TO 360 C REACTION TYPE IS (N,3N) NMT17(MED)=NMT17(MED)+1 C USE THE ONE NEUTRON EMISSION MODEL AND MULTIPLY THE C WEIGHT BY THREE C changed to 3 neutron production CZ July 30,1992 CZ WATE=3.0*WATE C DETERMINE THE COSINE OF THE NEUTRON SCATTERING ANGLE IN THE C LABORATORY COORDINATE SYSTEM L1=LDICT(73,IIN) IF(L1.EQ.0)GO TO 320 LS1=IDICTS(73,IIN)+LMOX2 LEN=L1 DO 310 KN=1,3 CALL CANGLE(D(LS1),D(LS1),E,FM(KN),LEN) 310 CONTINUE GO TO 330 C ASSUME ISOTROPIC IN THE LABORATORY COORDINATE SYSTEM 320 CONTINUE IFLG=1 C DETERMINE THE EXIT NEUTRON ENERGY IN THE LABORATORY C COORDINATE SYSTEM 330 L1=LDICT(124,IIN) IF(L1.EQ.0)GO TO 340 LS1=IDICTS(124,IIN)+LMOX2 INEU = 3 CALL GETENE(E,D(LS1),D(LS1),INEU) C DETERMINE THE EXIT COLLISION PARAMETERS IN THE LABORATORY C COORDINATE SYSTEM QI=Q(ID,IIN) CALL N2NN3N(D,D,AWRI,KZI,ID,FM,QI,IFLG) CALL PHOTON(D,D,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, +IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGN3N) RETURN 340 CONTINUE COMM= ' COLISN; NO SECONDARY ENERGY DISTRIBUTION WAS FOUND MT-17' ISTOP=1 GO TO 560 350 SIGN3N=0.0 360 CONTINUE C DETERMINE (N,N"A) CROSS SECTION (MT-22) ID=11 L1=LDICT(ID,IIN) IF(L1.EQ.0)GO TO 400 LS1=IDICTS(ID,IIN)+LMOX2 LEN=L1/2 CALL TBSPLT(D(LS1),E,LEN,SIGNNA) SUMS=SUMS+SIGNNA/SIGTNS*FSUMS IF(R.GT.SUMS)GO TO 410 C REACTION TYPE IS (N,N"A) NMT22(MED)=NMT22(MED)+1 C DETERMINE THE COSINE OF THE NEUTRON SCATTERING ANGLE IN THE C LABORATORY COORDINATE SYSTEM L1=LDICT(75,IIN) IF(L1.EQ.0)GO TO 370 LS1=IDICTS(75,IIN)+LMOX2 LEN=L1 CALL CANGLE(D(LS1),D(LS1),E,FM(1),LEN) GO TO 380 C ASSUME ISOTROPIC IN THE LABORATORY COORDINATE SYSTEM 370 CALL GTISO(U1,V1,W1) U=U1 V=V1 W=W1 LIFLAG=1 C DETERMINE THE EXIT NEUTRON ENERGY IN THE LABORATORY C COORDINATE SYSTEM 380 L1=LDICT(126,IIN) IF(L1.EQ.0)GO TO 390 LS1=IDICTS(126,IIN)+LMOX2 CALL SECEGY(EX,D(LS1),E,D(LS1)) E=EX IFLG=1 C DETERMINE THE EXIT COLLISION PARAMETERS IN THE LABORATORY C COORDINATE SYSTEM QI=Q(ID,IIN) LRI=22 CALL CMLABI(D,D,AWRI,KZI,ID,FM(1),QI,IFLG,LIFLAG,LRI) C Re-sample if no energy determined in CMLABI IF(IFLG.EQ.-1) GOTO 10 UP = U VP = V WP = W EP = E AGEP = AGE MTP = 22 CALL STOPAR(IDNEU,NNEU) KZ1=2 KZ2=KZI-KZ1 ATAR=AWRI*AN A1=AA A2=ATAR-AA Z1=ZA Z2=A2*9.31075E+08 MT=22 CALL NN2BOD(D,D,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) CALL PHOTON(D,D,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, +IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGNNA) RETURN 390 CONTINUE COMM=' COLISN; NO SECONDARY ENERGY DISTRIBUTION WAS FOUND MT-22' ISTOP=1 GO TO 560 400 SIGNNA=0.0 410 CONTINUE C DETERMINE (N,2NA) CROSS SECTION (MT-24) ID=12 L1=LDICT(ID,IIN) IF(L1.EQ.0)GO TO 450 LS1=IDICTS(ID,IIN)+LMOX2 LEN=L1/2 CALL TBSPLT(D(LS1),E,LEN,SGN2NA) SUMS=SUMS+SGN2NA/SIGTNS*FSUMS IF(R.GT.SUMS)GO TO 460 C REACTION TYPE IS (N,2NA) NMT24(MED)=NMT24(MED)+1 C USE THE ONE NEUTRON EMISSION MODEL AND MULTIPLY THE C WEIGHT BY TWO C changed to 2 neutron production CZ July 30,1992 CZ WATE=2.0*WATE C DETERMINE THE COSINE OF THE NEUTRON SCATTERING ANGLE IN THE C LABORATORY COORDINATE SYSTEM L1=LDICT(76,IIN) IF(L1.EQ.0)GO TO 420 LS1=IDICTS(76,IIN)+LMOX2 LEN=L1 CALL CANGLE(D(LS1),D(LS1),E,FM(1),LEN) CALL CANGLE(D(LS1),D(LS1),E,FM(2),LEN) GO TO 430 C ASSUME ISOTROPIC IN THE LABORATORY COORDINATE SYSTEM 420 CONTINUE IFLG=1 C DETERMINE THE EXIT NEUTRON ENERGY IN THE LABORATORY C COORDINATE SYSTEM 430 L1=LDICT(127,IIN) IF(L1.EQ.0)GO TO 440 LS1=IDICTS(127,IIN)+LMOX2 INEU=2 CALL GETENE(E,D(LS1),D(LS1),INEU) C DETERMINE THE EXIT COLLISION PARAMETERS IN THE LABORATORY C COORDINATE SYSTEM QI=Q(ID,IIN) CALL N2NN3N(D,D,AWRI,KZI,ID,FM,QI,IFLG) KZ1=2 KZ2=KZI-KZ1 ATAR=AWRI*AN A1=AA A2=ATAR-AN-AA Z1=ZA Z2=A2*9.31075E+08 MT=24 CALL NN2BOD(D,D,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) CALL PHOTON(D,D,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, +IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SGN2NA) RETURN 440 CONTINUE COMM=' COLISN; NO SECONDARY ENERGY DISTRIBUTION WAS FOUND MT-24' ISTOP=1 GO TO 560 450 SGN2NA=0.0 460 CONTINUE C DETERMINE (N,N"P) CROSS SECTION (MT-28) ID=13 L1=LDICT(ID,IIN) IF(L1.EQ.0)GO TO 500 LS1=IDICTS(ID,IIN)+LMOX2 LEN=L1/2 CALL TBSPLT(D(LS1),E,LEN,SIGNNP) SUMS=SUMS+SIGNNP/SIGTNS*FSUMS IF(R.GT.SUMS)GO TO 510 C REACTION TYPE IS (N,N"P) NMT28(MED)=NMT28(MED)+1 C DETERMINE THE COSINE OF THE NEUTRON SCATTERING ANGLE IN THE C LABORATORY COORDINATE SYSTEM L1=LDICT(77,IIN) IF(L1.EQ.0)GO TO 470 LS1=IDICTS(77,IIN)+LMOX2 LEN=L1 CALL CANGLE(D(LS1),D(LS1),E,FM(1),LEN) GO TO 480 C ASSUME ISOTROPIC IN THE LABORATORY COORDINATE SYSTEM 470 CALL GTISO(U1,V1,W1) U=U1 V=V1 W=W1 LIFLAG=1 C DETERMINE THE EXIT NEUTRON ENERGY IN THE LABORATORY C COORDINATE SYSTEM 480 L1=LDICT(128,IIN) IF(L1.EQ.0)GO TO 490 LS1=IDICTS(128,IIN)+LMOX2 CALL SECEGY(EX,D(LS1),E,D(LS1)) E=EX IFLG=1 C DETERMINE THE EXIT COLLISION PARAMETERS IN THE LABORATORY C COORDINATE SYSTEM QI=Q(ID,IIN) LRI=28 CALL CMLABI(D,D,AWRI,KZI,ID,FM(1),QI,IFLG,LIFLAG,LRI) C Re-sample if no energy determined in CMLABI IF(IFLG.EQ.-1) GOTO 10 EP = E UP = U VP = V WP = W AGEP = AGE MTP = 28 CALL STOPAR(IDNEU,NNEU) KZ1=1 KZ2=KZI-KZ1 ATAR=AWRI*AN A1=AP A2=ATAR-AP Z1=ZP Z2=A2*9.31075E+08 MT=28 CALL NN2BOD(D,D,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) CALL PHOTON(D,D,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, +IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGNNP) RETURN 490 CONTINUE COMM=' COLISN; NO SECONDARY ENERGY DISTRIBUTION FOUND FOR MT-28' SIGREC=SIGTNS SUMREC=SUMS ISTOP=1 GO TO 560 500 SIGNNP=0.0 510 CONTINUE FSUMS = 1./SUMS GO TO 550 520 CONTINUE C REACTION TYPE IS (N,N"A) USING LR FLAG NMT22(MED)=NMT22(MED)+1 SIGNNA=SGNISD IF(ID.EQ.54)SIGNNA=SGNISC KZ1=2 KZ2=KZI-KZ1 ATAR=AWRI*AN A1=AA A2=ATAR-AA Z1=ZA Z2=A2*9.31075E+08 MT=22 CALL LR2BOD(D,D,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,QLRI,ID,MT) CALL PHOTON(D,D,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, +IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGNNA) RETURN 530 CONTINUE C REACTION TYPE IS (N,N"3A) USING LR FLAG C CARBON-12 IS CURRENTLY THE ONLY ELEMENT CONTAINING MT-23 NMT23(MED)=NMT23(MED)+1 SGNN3A=SGNISD IF(ID.EQ.54)SGNN3A=SGNISC KZ1=2 KZ2=KZI-KZ1 ATAR=AWRI*AN A1=AA A2=ATAR-AA Z1=ZA Z2=A2*9.31075E+08 C QBE8 IS THE MASS DIFFERENCE FOR A CARBON-ALPHA EMISSION MT=23 CALL LR2BOD(D,D,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,QBE8,ID,MT) KZ1=2 KZ2=KZ2-KZ1 ATAR=AWRI*AN A1=AA A2=A2-AA Z1=ZA Z2=A2*9.31075E+08 MT=23 CALL LR2BOD(D,D,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QBE8,QLRI,ID,MT) CALL PHOTON(D,D,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, +IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SGNN3A) RETURN 540 CONTINUE C REACTION TYPE IS (N,N"P) USING LR FLAG NMT28(MED)=NMT28(MED)+1 SIGNNP=SGNISD IF(ID.EQ.54)SIGNNP=SGNISC KZ1=1 KZ2=KZI-KZ1 ATAR=AWRI*AN A1=AP A2=ATAR-AP Z1=ZP Z2=A2*9.31075E+08 MT=28 CALL LR2BOD(D,D,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,QLRI,ID,MT) CALL PHOTON(D,D,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, +IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGNNP) RETURN 550 ITRY=ITRY+1 NSEI(IIN)=NSEI(IIN)-1 ISTOP = 1 IF((FSUMS.GT.0.1.AND.FSUMS.LE.10.0).AND. + (FSUMIS.GT.0.1.AND.FSUMIS.LE.10.0)) ISTOP = 0 IF(ISTOP.EQ.0.AND.ITRY.LE.5) GOTO 20 C A SCATTERING REACTION WAS NOT CHOSEN COMM=' COLISN: A SCATTERING REACTION TYPE WAS NOT CHOSEN ' SIGREC=SIGTNS SUMREC=SUMS GOTO 980 560 CONTINUE IF(ISTOP.EQ.1)GO TO 980 ITRY=0 GO TO 20 C THE REACTION TYPE IS AN ABSORPTION 570 NAEI(IIN)=NAEI(IIN)+1 R=FLTRNF(0) C DETERMINE THE FISSION CROSS SECTION (MT-18) C THE TREATMENT OF THE FISSION REACTION ASSUMES THE FISSION C CROSS SECTION IS STORED AS NUBAR*SIGF ID=10 L1=LDICT(ID,IIN) IF(L1.EQ.0)GO TO 640 LS1=IDICTS(ID,IIN)+LMOX2 LEN=L1/2 CALL TBSPLT(D(LS1),E,LEN,SIGNF) C DETERMINE THE AVERAGE NUMBER OF NEUTRONS EMITTED PER FISSION C EVENT (NUBAR) L1=LDICT(134,IIN) IF(L1.EQ.0)GO TO 630 LS1=IDICTS(134,IIN)+LMOX2 LEN=L1 CALL GETNU(D(LS1),D(LS1),EOLD,LEN,XNU) C EXTRACT THE FISSION CROSS SECTION FROM THE NUBAR*SIGF CROSS C SECTION STORED IN POSITION 10 OF THE DICTIONARY SIGNF=SIGNF/XNU SUMA=SIGNF/SIGTNA*FSUMA IF(R.GT.SUMA)GO TO 650 C THE REACTION TYPE IS (N,F) NMT18(MED)=NMT18(MED)+1 WATE = 0.0 C DETERMINE THE COSINE OF THE NEUTRON SCATTERING ANGLE IN THE C LABORATORY COORDINATE SYSTEM C changed in order to get N fission neutron CZ July 30,1992 C INEU is poisson distributed with mean XNU 580 CALL GPOISS(XNU,INEU,1) IF(INEU.GT.INT(4.*XNU)) GOTO 580 C check for maximum number of neutrons emitted IF(INEU.GT.INT(AWRI)-KZ(MED)) INEU = INT(AWRI) - KZ(MED) IF(INEU.GT.MAXNEU) INEU = MAXNEU L1=LDICT(74,IIN) IF(L1.EQ.0)GO TO 600 LS1=IDICTS(74,IIN)+LMOX2 LEN=L1 DO 590 KN=1,INEU CALL CANGLE(D(LS1),D(LS1),E,FM(KN),LEN) 590 CONTINUE GO TO 610 C ASSUME ISOTROPIC IN THE LABORATORY COORDINATE SYSTEM 600 CONTINUE LIFLAG=1 C DETERMINE THE EXIT NEUTRON ENERGY IN THE LABORATORY C COORDINATE SYSTEM 610 L1=LDICT(125,IIN) IF(L1.EQ.0)GO TO 620 LS1=IDICTS(125,IIN)+LMOX2 IF(INEU.GT.0) CALL GETENE(E,D(LS1),D(LS1),INEU) C DETERMINE THE EXIT NEUTRON WEIGHT FROM THE AVERAGE NUMBER C OF NEUTRONS EMITTED PER FISSION REACTION (NU) C changed CZ July 30,1992 CZ WATE=WATE*XNU C DETERMINE THE EXIT COLLISION PARAMETERS IN THE LABORATORY C COORDINATE SYSTEM QI=Q(ID,IIN) IF(INEU.GT.0) CALL LABNF(D,D,FM,AWRI,KZI,QI,LIFLAG) CALL PHOTON(D,D,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, +IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGNF) NPSCL(3)=NPSCL(3)+1 CALL BANKR(D,D,3) RETURN 620 CONTINUE COMM=' COLISN: NO SECONDARY ENERGY DISTRIBUTION FOUND FOR MT-18' SIGREC=SIGNF SUMREC=SUMA ISTOP=1 GO TO 970 630 CONTINUE COMM=' COLISN: NO NUMBER OF FISSION NEUTRON FOUND FOR MT-18' SIGREC=SIGNF SUMREC=SUMA ISTOP=1 GO TO 970 640 SIGNF=0.0 650 CONTINUE C DETERMINE (N,G) CROSS SECTION (MT-102) ID=55 L1=LDICT(ID,IIN) IF(L1.EQ.0)GO TO 660 LS1=IDICTS(ID,IIN)+LMOX2 LEN=L1/2 CALL TBSPLT(D(LS1),E,LEN,SIGNG) SUMA=SUMA+SIGNG/SIGTNA*FSUMA IF(R.GT.SUMA)GO TO 670 C THE REACTION TYPE IS (N,G) NMT102(MED)=NMT102(MED)+1 QI=Q(ID,IIN) CALL PHOTON(D,D,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, +IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGNG) MT=102 CALL NGHEVY(D,D,KZI,AWRI,QI,MT) WATE=0.0 RETURN 660 SIGNG=0.0 670 CONTINUE C DETERMINE (N,P) CROSS SECTION (MT-103) ID=56 L1=LDICT(ID,IIN) IF(L1.EQ.0)GO TO 690 LS1=IDICTS(ID,IIN)+LMOX2 LEN=L1/2 CALL TBSPLT(D(LS1),E,LEN,SIGNP) SUMA=SUMA+SIGNP/SIGTNA*FSUMA IF(R.GT.SUMA)GO TO 700 C THE REACTION TYPE IS (N,P) NMT103(MED)=NMT103(MED)+1 QI=Q(ID,IIN) KZ1=1 KZ2=KZI-KZ1 ATAR=AWRI*AN A1=AP A2=ATAR+AN-AP Z1=ZP Z2=A2*9.31075E+08 MT=103 IF(KZI.EQ.6)GO TO 680 CALL TWOBOD(D,D,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) CALL PHOTON(D,D,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, +IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGNP) WATE=0.0 RETURN 680 CALL GRNDST(D,D,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) WATE=0.0 RETURN 690 SIGNP=0.0 700 CONTINUE C DETERMINE (N,D) CROSS SECTION (MT-104) ID=57 L1=LDICT(ID,IIN) IF(L1.EQ.0)GO TO 720 LS1=IDICTS(ID,IIN)+LMOX2 LEN=L1/2 CALL TBSPLT(D(LS1),E,LEN,SIGND) SUMA=SUMA+SIGND/SIGTNA*FSUMA IF(R.GT.SUMA)GO TO 730 C THE REACTION TYPE IS (N,D) NMT104(MED)=NMT104(MED)+1 QI=Q(ID,IIN) KZ1=1 KZ2=KZI-KZ1 ATAR=AWRI*AN A1=AD A2=ATAR+AN-AD Z1=ZD Z2=A2*9.31075E+08 MT=104 IF((KZI.EQ.5).OR.(KZI.EQ.6))GO TO 710 IF((KZI.EQ.8).OR.(KZI.EQ.13))GO TO 710 IF((KZI.EQ.14).OR.(KZI.EQ.20))GO TO 710 CALL TWOBOD(D,D,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) CALL PHOTON(D,D,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, +IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGND) WATE=0.0 RETURN 710 CALL GRNDST(D,D,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) WATE=0.0 RETURN 720 SIGND=0.0 730 CONTINUE C DETERMINE (N,T) CROSS SECTION (MT-105) ID=58 L1=LDICT(ID,IIN) IF(L1.EQ.0)GO TO 750 LS1=IDICTS(ID,IIN)+LMOX2 LEN=L1/2 CALL TBSPLT(D(LS1),E,LEN,SIGNT) SUMA=SUMA+SIGNT/SIGTNA*FSUMA IF(R.GT.SUMA)GO TO 760 C THE REACTION TYPE IS (N,T) NMT105(MED)=NMT105(MED)+1 QI=Q(ID,IIN) KZ1=1 KZ2=KZI-KZ1 ATAR=AWRI*AN A1=AT A2=ATAR+AN-AT Z1=ZT Z2=A2*9.31075E+08 MT=105 IF((KZI.EQ.5).OR.(KZI.EQ.13))GO TO 740 IF(KZI.EQ.20)GO TO 740 CALL TWOBOD(D,D,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) CALL PHOTON(D,D,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, +IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGNT) WATE=0.0 RETURN 740 CALL GRNDST(D,D,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) WATE=0.0 RETURN 750 SIGNT=0.0 760 CONTINUE C DETERMINE (N,3HE) CROSS SECTION (MT-106) ID=59 L1=LDICT(ID,IIN) IF(L1.EQ.0)GO TO 780 LS1=IDICTS(ID,IIN)+LMOX2 LEN=L1/2 CALL TBSPLT(D(LS1),E,LEN,SGN3HE) SUMA=SUMA+SGN3HE/SIGTNA*FSUMA IF(R.GT.SUMA)GO TO 790 C THE REACTION TYPE IS (N,3HE) NMT106(MED)=NMT106(MED)+1 QI=Q(ID,IIN) KZ1=2 KZ2=KZI-KZ1 ATAR=AWRI*AN A1=AHE3 A2=ATAR+AN-AHE3 Z1=ZHE3 Z2=A2*9.31075E+08 MT=106 IF(KZI.EQ.20)GO TO 770 CALL TWOBOD(D,D,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) CALL PHOTON(D,D,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, +IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SGN3HE) WATE=0.0 RETURN 770 CALL GRNDST(D,D,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) WATE=0.0 RETURN 780 SGN3HE=0.0 790 CONTINUE C DETERMINE (N,A) CROSS SECTION (MT-107) ID=60 L1=LDICT(ID,IIN) IF(L1.EQ.0)GO TO 810 LS1=IDICTS(ID,IIN)+LMOX2 LEN=L1/2 CALL TBSPLT(D(LS1),E,LEN,SIGNA) SUMA=SUMA+SIGNA/SIGTNA*FSUMA IF(R.GT.SUMA)GO TO 820 C THE REACTION TYPE IS (N,A) NMT107(MED)=NMT107(MED)+1 QI=Q(ID,IIN) KZ1=2 KZ2=KZI-KZ1 ATAR=AWRI*AN A1=AA A2=ATAR+AN-AA Z1=ZA Z2=A2*9.31075E+08 MT=107 IF((KZI.EQ.6).OR.(KZI.EQ.13))GO TO 800 CALL TWOBOD(D,D,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) CALL PHOTON(D,D,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, +IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGNA) WATE=0.0 RETURN 800 CALL GRNDST(D,D,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) WATE=0.0 RETURN 810 SIGNA=0.0 820 CONTINUE C DETERMINE (N,2A) CROSS SECTION (MT-108) ID=61 L1=LDICT(ID,IIN) IF(L1.EQ.0)GO TO 840 LS1=IDICTS(ID,IIN)+LMOX2 LEN=L1/2 CALL TBSPLT(D(LS1),E,LEN,SIGN2A) SUMA=SUMA+SIGN2A/SIGTNA*FSUMA IF(R.GT.SUMA)GO TO 850 C THE REACTION TYPE IS (N,2A) NMT108(MED)=NMT108(MED)+1 QI=Q(ID,IIN) KZ1=2 KZ2=KZI-2*KZ1 ATAR=AWRI*AN A1=AA A2=ATAR+AN-AA Z1=ZA Z2=A2*9.31075E+08 MT=108 C USE THE ONE PARTICLE EMISSION MODEL AND MULTIPLY THE C WEIGHT BY TWO IF((KZI.EQ.7).OR.(KZI.EQ.20))GO TO 830 CALL TWOBOD(D,D,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) CALL PHOTON(D,D,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, +IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGN2A) WATE=0.0 RETURN 830 CALL GRNDST(D,D,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) WATE=0.0 RETURN 840 SIGN2A=0.0 850 CONTINUE C DETERMINE (N,3A) CROSS SECTION (MT-109) ID=62 L1=LDICT(ID,IIN) IF(L1.EQ.0)GO TO 860 LS1=IDICTS(ID,IIN)+LMOX2 LEN=L1/2 CALL TBSPLT(D(LS1),E,LEN,SIGN3A) SUMA=SUMA+SIGN3A/SIGTNA*FSUMA IF(R.GT.SUMA)GO TO 870 C THE REACTION TYPE IS (N,3A) NMT109(MED)=NMT109(MED)+1 QI=Q(ID,IIN) KZ1=2 KZ2=KZI-3*KZ1 ATAR=AWRI*AN A1=AA A2=ATAR+AN-AA Z1=ZA Z2=A2*9.31075E+08 MT=109 C USE THE ONE PARTICLE EMISSION MODEL AND MULTIPLY THE C WEIGHT BY THREE CALL TWOBOD(D,D,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) CALL PHOTON(D,D,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, +IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGN3A) WATE=0.0 RETURN 860 SIGN3A=0.0 870 CONTINUE C DETERMINE (N,2P) CROSS SECTION (MT-111) ID=63 L1=LDICT(ID,IIN) IF(L1.EQ.0)GO TO 890 LS1=IDICTS(ID,IIN)+LMOX2 LEN=L1/2 CALL TBSPLT(D(LS1),E,LEN,SIGN2P) SUMA=SUMA+SIGN2P/SIGTNA*FSUMA IF(R.GT.SUMA)GO TO 900 C THE REACTION TYPE IS (N,2P) NMT111(MED)=NMT111(MED)+1 QI=Q(ID,IIN) KZ1=1 KZ2=KZI-2*KZ1 ATAR=AWRI*AN A1=AP A2=ATAR+AN-AP Z1=ZP Z2=A2*9.31075E+08 MT=111 C USE THE ONE PARTICLE EMISSION MODEL AND MULTIPLY THE C WEIGHT BY TWO IF(KZI.EQ.20)GO TO 880 CALL TWOBOD(D,D,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) CALL PHOTON(D,D,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, +IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGN2P) WATE=0.0 RETURN 880 CALL GRNDST(D,D,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) WATE=0.0 RETURN 890 SIGN2P=0.0 900 CONTINUE C DETERMINE (N,PA) CROSS SECTION (MT-112) ID=64 L1=LDICT(ID,IIN) IF(L1.EQ.0)GO TO 910 LS1=IDICTS(ID,IIN)+LMOX2 LEN=L1/2 CALL TBSPLT(D(LS1),E,LEN,SIGNPA) SUMA=SUMA+SIGNPA/SIGTNA*FSUMA IF(R.GT.SUMA)GO TO 920 C THE REACTION TYPE IS (N,PA) NMT112(MED)=NMT112(MED)+1 QI=Q(ID,IIN) KZ1=1 KZ2=2 KZ3=KZI-KZ1-KZ2 ATAR=AWRI*AN A1=AP A2=AA A3=ATAR+AN-A1 Z1=ZP Z2=ZA Z3=A3*9.31075E+08 MT=112 CZ July 30,1992 Three-Body process added ---- CALL TREBOD(D,D,KZ1,KZ2,KZ3,A1,A2,A3,Z1,Z2,Z3,ATAR,QI,MT) CALL PHOTON(D,D,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, +IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGNPA) WATE=0.0 RETURN 910 SIGNPA=0.0 920 CONTINUE C DETERMINE (N,T2A) CROSS SECTION (MT-113) ID=65 L1=LDICT(ID,IIN) IF(L1.EQ.0)GO TO 930 LS1=IDICTS(ID,IIN)+LMOX2 LEN=L1/2 CALL TBSPLT(D(LS1),E,LEN,SGNT2A) SUMA=SUMA+SGNT2A/SIGTNA*FSUMA IF(R.GT.SUMA)GO TO 940 C THE REACTION TYPE IS (N,T2A) NMT113(MED)=NMT113(MED)+1 QI=Q(ID,IIN) KZ1=1 KZ2=2 KZ3=KZI-KZ1-2*KZ2 ATAR=AWRI*AN A1=AT A2=AA A3=ATAR+AN-A1 Z1=ZT Z2=ZA Z3=A3*9.31075E+08 MT=113 CZ July 30,1992 Three-Body process added ---- CALL TREBOD(D,D,KZ1,KZ2,KZ3,A1,A2,A3,Z1,Z2,Z3,ATAR,QI,MT) CALL PHOTON(D,D,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, +IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SGNT2A) WATE=0.0 RETURN 930 SGNT2A=0.0 940 CONTINUE C DETERMINE (N,D2A) CROSS SECTION (MT-114) ID=66 L1=LDICT(ID,IIN) IF(L1.EQ.0)GO TO 950 LS1=IDICTS(ID,IIN)+LMOX2 LEN=L1/2 CALL TBSPLT(D(LS1),E,LEN,SGND2A) SUMA=SUMA+SGND2A/SIGTNA*FSUMA IF(R.GT.SUMA)GO TO 960 C THE REACTION TYPE IS (N,D2A) NMT114(MED)=NMT114(MED)+1 QI=Q(ID,IIN) KZ1=1 KZ2=2 KZ3=KZI-KZ1-2*KZ2 ATAR=AWRI*AN A1=AD A2=AA A3=ATAR+AN-A1 Z1=ZD Z2=ZA Z3=A3*9.31075E+08 MT=114 CZ July 30,1992 Three-Body process added ---- CALL TREBOD(D,D,KZ1,KZ2,KZ3,A1,A2,A3,Z1,Z2,Z3,ATAR,QI,MT) CALL PHOTON(D,D,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, +IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SGND2A) WATE=0.0 RETURN 950 SGND2A=0.0 960 CONTINUE FSUMA = 1./SUMA ITRY=ITRY+1 ISTOP=1 IF(FSUMA.GT.0.1.AND.FSUMA.LE.10.0) ISTOP=0 NAEI(IIN)=NAEI(IIN)-1 IF(ISTOP.EQ.0.AND.ITRY.LE.5)GO TO 20 C AN ABSORPTION REACTION WAS NOT CHOSEN COMM=' COLISN:AN ABSORPTION REACTION TYPE WAS NOT CHOSEN ' SIGREC = SIGTNA SUMREC = SUMA GOTO 980 970 CONTINUE IF(ISTOP.EQ.1)GO TO 980 ITRY=0 GO TO 20 980 CONTINUE WRITE(IOUT,'(A80,/,I5,F7.1,I4,/,G18.7,I5,3G10.4)') COMM, + NMED,AWR(IIN),KZ(IIM), + E,MT, + SIGT,SIGREC,SUMREC RETURN END