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authorstainer_t <thomas.stainer@oecd-nea.org>2025-09-08 13:48:49 +0200
committerstainer_t <thomas.stainer@oecd-nea.org>2025-09-08 13:48:49 +0200
commit7dfcc480ba1e19bd3232349fc733caef94034292 (patch)
tree03ee104eb8846d5cc1a981d267687a729185d3f3 /Dragon/src/SHISN3.f
Initial commit from Polytechnique Montreal
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+*DECK SHISN3
+ SUBROUTINE SHISN3 (IPLIB,IPTRK,IFTRAK,LEVEL,NGRO,NBISO,NBM,NREG,
+ 1 NUN,CDOOR,INRS,NBNRS,IMPX,ISONAM,MIX,DEN,SN,SB,LSHI,IPHASE,MAT,
+ 2 VOL,KEYFLX,LEAKSW,TITR,START,SIGT,SIGT3,NOCONV,BIEFF,LGC)
+*
+*-----------------------------------------------------------------------
+*
+*Purpose:
+* Perform one multidimensional self-shielding iteration using the
+* generalized Stamm'ler algorithm with Nordheim (PIC) approximation.
+*
+*Copyright:
+* Copyright (C) 2004 Ecole Polytechnique de Montreal
+* This library is free software; you can redistribute it and/or
+* modify it under the terms of the GNU Lesser General Public
+* License as published by the Free Software Foundation; either
+* version 2.1 of the License, or (at your option) any later version
+*
+*Author(s): A. Hebert
+*
+*Parameters: input
+* IPLIB pointer to the internal microscopic cross section library
+* (L_LIBRARY signature).
+* IPTRK pointer to the tracking (L_TRACK signature).
+* IFTRAK unit number of the sequential binary tracking file.
+* LEVEL type of self-shielding model (=1 original Stamm'ler model
+* with Nordheim approximation; =2 Stamm'ler model with Nordheim
+* approximation and Riemann integration method).
+* NGRO number of energy groups.
+* NBISO number of isotopes present in the calculation domain.
+* NBM number of mixtures in the macrolib.
+* NREG number of volumes.
+* NUN number of unknowns in the flux or source vector in one
+* energy group.
+* CDOOR name of the geometry/solution module.
+* INRS index of the resonant isotope under consideration.
+* NBNRS number of totaly correlated resonant regions.
+* IMPX print flag.
+* ISONAM alias name of isotopes.
+* MIX mix number of each isotope (can be zero).
+* DEN density of each isotope.
+* LSHI resonant region number associated with each isotope.
+* Infinite dilution will be assumed if LSHI(i)=0.
+* IPHASE type of flux solution (=1 use a native flux solution door;
+* =2 use collision probabilities).
+* MAT index-number of the mixture type assigned to each volume.
+* VOL volumes.
+* KEYFLX pointers of fluxes in unknown vector.
+* LEAKSW leakage flag (.TRUE. only if leakage is present on the outer
+* surface).
+* TITR title.
+* START beginning-of-iteration flag (.TRUE. if SHISN3 is called
+* for the first time).
+* SIGT3 transport correction.
+* NOCONV mixture convergence flag. (.TRUE. if mixture IBM
+* is not converged in group L).
+* BIEFF Livolant-Jeanpierre normalization flag (.TRUE. to
+* activate).
+* LGC Goldstein-Cohen approximation flag (.TRUE. to activate).
+*
+*Parameters: input/output
+* SN on input, estimate of the dilution cross section in each
+* energy group of each isotope. A value of 1.0e10 is used
+* for infinitedilution.
+* On output, computed dilution cross section in each energy
+* group of each isotope.
+* SIGT total macroscopic cross sections as modified by Shiba.
+*
+*Parameters: output
+* SB dilution cross section as used in Livolant-Jeanpierre
+* normalization.
+*
+*Reference:
+* A. Hebert, Revisiting the Stamm'ler Self-Shielding Method, Presented
+* at the 25th CNS annnual conference, June 6-9, Toronto, 2004.
+*
+*-----------------------------------------------------------------------
+*
+ USE GANLIB
+*----
+* SUBROUTINE ARGUMENTS
+*----
+ PARAMETER (NALPHA=9,NRAT=(NALPHA+1)/2)
+ TYPE(C_PTR) IPLIB,IPTRK
+ INTEGER IFTRAK,LEVEL,NGRO,NBISO,NBM,NREG,NUN,INRS,NBNRS,IMPX,
+ 1 ISONAM(3,NBISO),MIX(NBISO),LSHI(NBISO),IPHASE,MAT(NREG),
+ 2 KEYFLX(NREG)
+ REAL DEN(NBISO),SN(NGRO,NBISO),SB(NGRO,NBISO),VOL(NREG),
+ 1 SIGT(NBM,NGRO),SIGT3(NBM,NGRO)
+ CHARACTER CDOOR*12,TITR*72
+ LOGICAL LEAKSW,START,NOCONV(NBM,NGRO),BIEFF,LGC
+*----
+* LOCAL VARIABLES
+*----
+ TYPE(C_PTR) KPLIB
+ CHARACTER HSMG*131,CGRPNM*12
+ LOGICAL LOGDO
+ REAL FACT(NALPHA),SIGX(NALPHA)
+ COMPLEX SUM
+*----
+* ALLOCATABLE ARRAYS
+*----
+ INTEGER, ALLOCATABLE, DIMENSION(:) :: IRES,ISONR,NPSYS
+ REAL, ALLOCATABLE, DIMENSION(:) :: GAR,GAS,SIGE,VST,DIST,FUN,DILG
+ REAL, ALLOCATABLE, DIMENSION(:,:) :: SIG0,SIG3,TOTAL,DILUT,GC
+ DOUBLE PRECISION, ALLOCATABLE, DIMENSION(:,:,:) :: PICX
+ LOGICAL, ALLOCATABLE, DIMENSION(:) :: MASKI
+ COMPLEX, ALLOCATABLE, DIMENSION(:,:) :: COEF,DENOM
+ COMPLEX*16, ALLOCATABLE, DIMENSION(:,:,:) :: XCOEF,XDENO
+ TYPE(C_PTR), ALLOCATABLE, DIMENSION(:) :: IPISO
+*----
+* DATA STATEMENTS
+*----
+ DATA FACT/0.01,0.03162278,0.1,0.3162278,1.0,3.162278,10.0,
+ 1 31.62278,100.0/
+*----
+* SCRATCH STORAGE ALLOCATION
+* SIG0 macroscopic xs of the resonant isotopes as interpolated.
+* SIG3 macroscopic transport correction.
+*----
+ ALLOCATE(IRES(NBM),ISONR(NBNRS),NPSYS(NGRO))
+ ALLOCATE(SIG0(NBM,NGRO),SIG3(NBM,NGRO),TOTAL(NGRO,NBNRS),
+ 1 GAR(NGRO),GAS(NGRO),SIGE(NGRO),DILUT(NALPHA,NGRO),
+ 2 GC(NGRO,NBNRS),VST(NBNRS),DIST(NBNRS))
+ ALLOCATE(PICX(NALPHA,NBNRS,NGRO))
+ ALLOCATE(MASKI(NBISO))
+ ALLOCATE(COEF(NRAT,NGRO),DENOM(NRAT,NGRO))
+ ALLOCATE(XCOEF(NRAT,NBNRS,NGRO),XDENO(NRAT,NBNRS,NGRO))
+ ALLOCATE(IPISO(NBISO))
+*----
+* FIND THE RESONANT MIXTURE NUMBERS AND THE CORRELATED ISOTOPES
+* ASSOCIATED WITH REGION INRS
+*----
+ IRS=0
+ DO 30 IBM=1,NBM
+ LOGDO=.FALSE.
+ DO 10 I=1,NREG
+ LOGDO=LOGDO.OR.(MAT(I).EQ.IBM)
+ 10 CONTINUE
+ IF(.NOT.LOGDO) GO TO 30
+ DO 20 ISO=1,NBISO
+ IF((MIX(ISO).EQ.IBM).AND.(LSHI(ISO).EQ.INRS)) THEN
+ IRS=IRS+1
+ ISONR(IRS)=ISO
+ GO TO 30
+ ENDIF
+ 20 CONTINUE
+ 30 CONTINUE
+ IF(IRS.NE.NBNRS) CALL XABORT('SHISN3: INVALID VALUE OF NBNRS.')
+ IRES(:NBM)=0
+ DO 40 IRS=1,NBNRS
+ ISO=ISONR(IRS)
+ IRES(MIX(ISO))=IRS
+ 40 CONTINUE
+*----
+* SET THE LCM MICROLIB ISOTOPEWISE DIRECTORIES.
+*----
+ CALL LIBIPS(IPLIB,NBISO,IPISO)
+*----
+* UNLOAD MICROSCOPIC X-S FROM LCM TO SCRATCH STORAGE. SET THE
+* GOLDSTEIN-COHEN TO ONE IN LEVEL 2 CALCULATIONS.
+*----
+ DO 50 IRS=1,NBNRS
+ ISO=ISONR(IRS)
+ KPLIB=IPISO(ISO) ! set ISO-th isotope
+ CALL LCMGET(KPLIB,'NTOT0',TOTAL(1,IRS))
+ GC(:NGRO,IRS)=1.0
+ 50 CONTINUE
+*
+ VST(:NBNRS)=0.0
+ DO 60 I=1,NREG
+ IF(MAT(I).EQ.0) GO TO 60
+ IND=IRES(MAT(I))
+ IF(IND.GT.0) VST(IND)=VST(IND)+VOL(I)
+ 60 CONTINUE
+*
+ NPSYS(:NGRO)=0
+ DO 110 LLL=1,NGRO
+ LOGDO=.FALSE.
+ DO 70 IRS=1,NBNRS
+ LOGDO=LOGDO.OR.NOCONV(MIX(ISONR(IRS)),LLL)
+ 70 CONTINUE
+ IF(LOGDO) THEN
+ NPSYS(LLL)=LLL
+*
+* COMPUTE THE LIGHT AND RESONANT COMPONENTS OF THE MACROSCOPIC
+* CROSS SECTIONS IN EACH RESONANT MIXTURE.
+ DO 80 IRS=1,NBNRS
+ ISO=ISONR(IRS)
+ IBM=MIX(ISO)
+ SIGT(IBM,LLL)=SIGT(IBM,LLL)-TOTAL(LLL,IRS)*DEN(ISO)
+ 80 CONTINUE
+ DO 90 IBM=1,NBM
+ SIG0(IBM,LLL)=0.0
+ SIG3(IBM,LLL)=SIGT3(IBM,LLL)
+ 90 CONTINUE
+ DO 100 IRS=1,NBNRS
+ ISO=ISONR(IRS)
+ SIG0(MIX(ISO),LLL)=TOTAL(LLL,IRS)*DEN(ISO)
+ SIG3(MIX(ISO),LLL)=0.0
+ 100 CONTINUE
+ IF(IMPX.GE.10) THEN
+ WRITE (6,400) LLL,(SIG0(I,LLL),I=1,NBM)
+ WRITE (6,410) LLL,(SIGT(I,LLL),I=1,NBM)
+ WRITE (6,420) LLL,(SIGT3(I,LLL),I=1,NBM)
+ ENDIF
+ ENDIF
+ 110 CONTINUE
+*----
+* SET UP VECTORS SIGE AND SB.
+*----
+ CALL LCMSIX(IPLIB,'SHIBA',1)
+*
+ SIGE(:NGRO)=0.0
+ ALLOCATE(FUN(NUN*NGRO))
+ CALL LCMSIX(IPLIB,'--AVERAGE--',1)
+ CALL SHIDST(IPLIB,NPSYS,IPTRK,IFTRAK,CDOOR,IMPX,NBM,NREG,NUN,
+ 1 NGRO,IPHASE,MAT,VOL,KEYFLX,LEAKSW,IRES,SIG0,SIGT,SIGT3(1,1),
+ 2 TITR,FUN,SIGE)
+ CALL LCMSIX(IPLIB,' ',2)
+ DO 130 LLL=1,NGRO
+ IF(NPSYS(LLL).NE.0) THEN
+ DO 120 I=1,NREG
+ IBM=MAT(I)
+ IF(IBM.EQ.0) GO TO 120
+ IND=IRES(IBM)
+ IF(IND.GT.0) THEN
+ IOF=(LLL-1)*NUN+KEYFLX(I)
+ ISO=ISONR(IND)
+ IF(NOCONV(IBM,LLL)) SB(LLL,ISO)=FUN(IOF)/
+ 1 SIG0(IBM,LLL)
+ ENDIF
+ 120 CONTINUE
+ ENDIF
+ 130 CONTINUE
+ DEALLOCATE(FUN)
+*----
+* SET UP VECTORS DILUT AND SIGX.
+*----
+ IF(START) THEN
+* USE A VERY CHEAP APPROXIMATION TO START ITERATIONS.
+ DO 145 LLL=1,NGRO
+ DO 140 IALP=1,NALPHA
+ SIGX(IALP)=0.0
+ DILUT(IALP,LLL)=SIGE(LLL)
+ 140 CONTINUE
+ 145 CONTINUE
+ ELSE
+ AVDEN=0.0
+ VOLTOT=0.0
+ DO 150 IRS=1,NBNRS
+ AVDEN=AVDEN+DEN(ISONR(IRS))*VST(IRS)
+ VOLTOT=VOLTOT+VST(IRS)
+ 150 CONTINUE
+ AVDEN=AVDEN/VOLTOT
+ DO 160 IRS=1,NBNRS
+ ISO=ISONR(IRS)
+ DIST(IRS)=DEN(ISO)/AVDEN
+ 160 CONTINUE
+ DO 220 IALP=1,NALPHA
+ DO 190 LLL=1,NGRO
+ IF(NPSYS(LLL).NE.0) THEN
+ SIGX(IALP)=FACT(IALP)*SIGE(LLL)
+ DO 170 IBM=1,NBM
+ SIG0(IBM,LLL)=0.0
+ SIG3(IBM,LLL)=SIGT3(IBM,LLL)
+ 170 CONTINUE
+ DO 180 IRS=1,NBNRS
+ ISO=ISONR(IRS)
+ SIG0(MIX(ISO),LLL)=SIGX(IALP)*DIST(IRS)
+ SIG3(MIX(ISO),LLL)=0.0
+ 180 CONTINUE
+ ENDIF
+ 190 CONTINUE
+ ALLOCATE(DILG(NGRO),FUN(NUN*NGRO))
+ WRITE(CGRPNM,'(8H--BAND--,I4.4)') IALP
+ CALL LCMSIX(IPLIB,CGRPNM,1)
+ CALL SHIDST(IPLIB,NPSYS,IPTRK,IFTRAK,CDOOR,IMPX,NBM,NREG,NUN,
+ 1 NGRO,IPHASE,MAT,VOL,KEYFLX,LEAKSW,IRES,SIG0,SIGT,SIG3(1,1),
+ 2 TITR,FUN,DILG)
+ CALL LCMSIX(IPLIB,' ',2)
+ DO 210 LLL=1,NGRO
+ IF(NPSYS(LLL).NE.0) THEN
+ DILUT(IALP,LLL)=DILG(LLL)
+ DO 200 I=1,NREG
+ IBM=MAT(I)
+ IF(IBM.EQ.0) GO TO 200
+ IND=IRES(IBM)
+ IF(IND.GT.0) THEN
+ IOF=(LLL-1)*NUN+KEYFLX(I)
+ PICX(IALP,IND,LLL)=FUN(IOF)/SIG0(IBM,LLL)
+ ENDIF
+ 200 CONTINUE
+ ENDIF
+ 210 CONTINUE
+ DEALLOCATE(FUN,DILG)
+ 220 CONTINUE
+ ENDIF
+ CALL LCMSIX(IPLIB,' ',2)
+*----
+* COMPUTE AVERAGE MACROSCOPIC DILUTION X-S USING A N-TERM RATIONAL
+* APPROXIMATION.
+*----
+ DO 260 LLL=1,NGRO
+ IF(NPSYS(LLL).NE.0) THEN
+ DO 230 IALP=1,NALPHA
+ SIGX(IALP)=FACT(IALP)*SIGE(LLL)
+ 230 CONTINUE
+* **********************************************************
+ CALL SHIRAT(IMPX,NRAT,SIGX,DILUT(1,LLL),LLL,A,COEF(1,LLL),
+ 1 DENOM(1,LLL))
+* **********************************************************
+*
+* COMPUTE THE PIC BASE POINTS FOR A N-TERM RATIONAL APPROXIMATION
+ IF(START) THEN
+ DO 245 IRS=1,NBNRS
+ DO 240 I=1,NRAT
+ XCOEF(I,IRS,LLL)=COEF(I,LLL)
+ XDENO(I,IRS,LLL)=DENOM(I,LLL)
+ 240 CONTINUE
+ 245 CONTINUE
+ ELSE
+ CALL SHIDIL(NRAT,NALPHA,NBNRS,COEF(1,LLL),DENOM(1,LLL),
+ 1 DILUT(1,LLL),PICX(1,1,LLL),SIGX,DIST,VST,IMPX,LLL,
+ 2 XCOEF(1,1,LLL),XDENO(1,1,LLL))
+ ENDIF
+ IF(.NOT.START.AND.BIEFF) THEN
+ DO 255 IRS=1,NBNRS
+ ISO=ISONR(IRS)
+ IF(NOCONV(MIX(ISO),LLL)) THEN
+ SIGRES=TOTAL(LLL,IRS)*DEN(ISO)
+ IF(NBNRS.EQ.1) THEN
+ SUM=0.0
+ DO 250 I=1,NRAT
+ SUM=SUM+COEF(I,LLL)/(SIGRES+DENOM(I,LLL))
+ 250 CONTINUE
+ PX0=REAL(SUM)
+ ELSE
+ PX0=SB(LLL,ISO)
+ ENDIF
+ SB(LLL,ISO)=(1.0/PX0-SIGRES)/DEN(ISO)
+ IF(SB(LLL,ISO).LT.0.0) THEN
+ WRITE (HSMG,515) (ISONAM(I0,ISO),I0=1,3),SB(LLL,ISO),
+ 1 LLL
+ CALL XABORT(HSMG)
+ ENDIF
+ ENDIF
+ 255 CONTINUE
+ ENDIF
+ ENDIF
+ 260 CONTINUE
+*----
+* APPLY A GOLDSTEIN-COHEN CORRECTION SIMILAR TO THE CORRECTION USED
+* IN SHISN2.
+*----
+ IF((.NOT.START).AND.LGC) THEN
+ DO 295 IRS=1,NBNRS
+ ISO=ISONR(IRS)
+ KPLIB=IPISO(ISO) ! set ISO-th isotope
+ CALL LCMLEN(KPLIB,'NGOLD',LENGT,ITYLCM)
+ IF(LENGT.EQ.NGRO) THEN
+ IF(IMPX.GE.5) WRITE (6,390) (ISONAM(I0,ISO),I0=1,3)
+ CALL LCMGET(KPLIB,'NGOLD',GC(1,IRS))
+ ENDIF
+ IF(LEVEL.EQ.2) GO TO 295
+ DO 290 JSO=1,NBISO
+ IF((MIX(JSO).EQ.MIX(ISO)).AND.(JSO.NE.ISO).AND.
+ 1 (LSHI(JSO).NE.0)) THEN
+ KPLIB=IPISO(JSO) ! set JSO-th isotope
+ CALL LCMLEN(KPLIB,'NGOLD',LENGT,ITYLCM)
+ IF(LENGT.EQ.NGRO) THEN
+ CALL LCMGET(KPLIB,'SIGS00',GAS)
+ CALL LCMGET(KPLIB,'NGOLD',GAR)
+ DO 280 LLL=1,NGRO
+ IF((NOCONV(MIX(JSO),LLL)).AND.(GAR(LLL).NE.1.0)) THEN
+ DDD=(1.0-GAR(LLL))*GAS(LLL)*DEN(JSO)
+ DO 270 I=1,NRAT
+ XDENO(I,IRS,LLL)=XDENO(I,IRS,LLL)-DDD
+ 270 CONTINUE
+ ENDIF
+ 280 CONTINUE
+ ENDIF
+ ENDIF
+ 290 CONTINUE
+ 295 CONTINUE
+ ENDIF
+*----
+* COMPUTE THE DILUTION PARAMETERS (BARN) FOR EACH RESONANT ISOTOPE IN
+* RESONANT MIXTURE INRS
+*----
+ CALL SHIEQU(IPLIB,LEVEL,NGRO,NBISO,NBM,NBNRS,NRAT,MIX,ISONAM,
+ 1 NOCONV,ISONR,GC,COEF,DENOM,XCOEF,XDENO,DEN,IMPX,SN)
+*
+ DO 320 LLL=1,NGRO
+ LOGDO=.FALSE.
+ DO 300 IRS=1,NBNRS
+ LOGDO=LOGDO.OR.NOCONV(MIX(ISONR(IRS)),LLL)
+ 300 CONTINUE
+ IF(LOGDO) THEN
+ DO 310 IRS=1,NBNRS
+ ISO=ISONR(IRS)
+ IBM=MIX(ISO)
+ IF(START.OR.(.NOT.BIEFF)) THEN
+ SB(LLL,ISO)=SN(LLL,ISO)
+ ELSE IF(SB(LLL,ISO).LT.0.97*SN(LLL,ISO)) THEN
+ WRITE (6,520)(ISONAM(I0,ISO),I0=1,3),SB(LLL,ISO)/
+ 1 SN(LLL,ISO),0.97,LLL
+ SB(LLL,ISO)=0.97*SN(LLL,ISO)
+ ENDIF
+ SIGT(IBM,LLL)=SIGT(IBM,LLL)+TOTAL(LLL,IRS)*DEN(ISO)
+ 310 CONTINUE
+ ENDIF
+ 320 CONTINUE
+*----
+* SAVE THE GROUP- AND ISOTOPE-DEPENDENT DILUTIONS
+*----
+ CALL LCMPUT(IPLIB,'ISOTOPESDSB',NBISO*NGRO,2,SB)
+ CALL LCMPUT(IPLIB,'ISOTOPESDSN',NBISO*NGRO,2,SN)
+*----
+* COMPUTE THE SELF-SHIELDED MICROSCOPIC CROSS SECTIONS AND UPDATE
+* VECTOR SIGT
+*----
+ DO 330 ISO=1,NBISO
+ LOGDO=START.OR.(DEN(ISO).NE.0.)
+ MASKI(ISO)=(LSHI(ISO).EQ.INRS).AND.LOGDO
+ 330 CONTINUE
+ IMPX2=MAX(0,IMPX-1)
+ CALL LIBLIB (IPLIB,NBISO,MASKI,IMPX2)
+ DO 345 IRS=1,NBNRS
+ ISO=ISONR(IRS)
+ IBM=MIX(ISO)
+ KPLIB=IPISO(ISO) ! set ISO-th isotope
+ CALL LCMGET(KPLIB,'NTOT0',GAR)
+ DO 340 LLL=1,NGRO
+ TOTAL(LLL,IRS)=TOTAL(LLL,IRS)-GAR(LLL)
+ SIGT(IBM,LLL)=SIGT(IBM,LLL)-DEN(ISO)*TOTAL(LLL,IRS)
+ 340 CONTINUE
+ 345 CONTINUE
+*----
+* SCRATCH STORAGE DEALLOCATION
+*----
+ DEALLOCATE(IPISO)
+ DEALLOCATE(XDENO,XCOEF)
+ DEALLOCATE(DENOM,COEF)
+ DEALLOCATE(MASKI)
+ DEALLOCATE(PICX)
+ DEALLOCATE(DIST,VST,GC,DILUT,SIGE,GAS,GAR,TOTAL,SIG3,SIG0)
+ DEALLOCATE(NPSYS,ISONR,IRES)
+ RETURN
+*
+ 390 FORMAT(/53H SHISN3: GOLDSTEIN AND COHEN APPROXIMATION USED FOR I,
+ 1 8HSOTOPE ',3A4,2H'.)
+ 400 FORMAT(//51H TOTAL MACROSCOPIC CROSS SECTIONS OF THE RESONANT M,
+ 1 31HATERIALS IN EACH MIXTURE (GROUP,I5,2H):/(1X,1P,11E11.3))
+ 410 FORMAT(//51H TOTAL MACROSCOPIC CROSS SECTIONS OF THE OTHER MATE,
+ 1 28HRIALS IN EACH MIXTURE (GROUP,I5,2H):/(1X,1P,11E11.3))
+ 420 FORMAT(//1X,'TRANSPORT CORRECTION CROSS SECTIONS OF THE OTHER ',
+ 1'MATERIALS IN EACH MIXTURE (GROUP',I5,'):'/(1X,1P,11E11.3))
+ 515 FORMAT(30HSHISN3: THE RESONANT ISOTOPE ',3A4,14H' HAS A NEGATI,
+ 1 22HVE L-J CROSS-SECTION (,1P,E14.4,0P,10H) IN GROUP,I4,1H.)
+ 520 FORMAT(54H SHISN3: THE L-J EQUIVALENCE FACTOR OF RESONANT ISOTOP,
+ 1 3HE ',3A4,18H' WAS CHANGED FROM,F6.3,3H TO,F5.2,9H IN GROUP,I4,
+ 2 1H.)
+ END