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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/SHISN2.f
Initial commit from Polytechnique Montreal
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+*DECK SHISN2
+ SUBROUTINE SHISN2 (IPLIB,IPTRK,IFTRAK,NGRO,NBISO,NBM,NREG,NUN,
+ 1 CDOOR,NRES,NBM2,IMPX,ISONAM,MIX,DEN,SN,SB,LSHI,IPHASE,MAT,VOL,
+ 2 KEYFLX,LEAKSW,TITR,START,SIGT,SIGT3,NOCONV,BIEFF,LGC,SIGE)
+*
+*-----------------------------------------------------------------------
+*
+*Purpose:
+* Perform one multidimensional self-shielding iteration using the
+* generalized Stamm'ler algorithm without Nordheim (PIC) approximation.
+*
+*Copyright:
+* Copyright (C) 2002 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.
+* 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.
+* NRES number of resonant mixtures.
+* NBM2 number of resonant isotopes.
+* 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 SHISN2 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: 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 infinite dilution.
+* 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.
+* SIGE computed macroscopic dilution cross section in each resonant
+* mixture and each energy group.
+*
+*Reference:
+* A. Hebert and G. Marleau, Generalization of the Stamm'ler Method
+* for the Self-Shielding of Resonant isotopes in Arbitrary Geometries,
+* Nucl. Sci. Eng. 108, 230 (1991).
+*
+*-----------------------------------------------------------------------
+*
+ USE GANLIB
+*----
+* SUBROUTINE ARGUMENTS
+*----
+ PARAMETER (NALPHA=5)
+ TYPE(C_PTR) IPLIB,IPTRK
+ INTEGER IFTRAK,NGRO,NBISO,NBM,NREG,NUN,NRES,NBM2,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),SIGE(NRES,NGRO)
+ CHARACTER CDOOR*12,TITR*72,CGRPNM*12
+ LOGICAL LEAKSW,START,NOCONV(NBM,NGRO),BIEFF,LGC
+*----
+* LOCAL VARIABLES
+*----
+ CHARACTER HSMG*131
+ LOGICAL LOGDO
+ COMPLEX COEF(3),DENOM(3),EAV
+ PARAMETER (NRAT=(NALPHA+1)/2)
+ TYPE(C_PTR) KPLIB
+ REAL FACT(NALPHA),SIGX(NALPHA)
+*----
+* ALLOCATABLE ARRAYS
+*----
+ INTEGER, ALLOCATABLE, DIMENSION(:) :: IRES,MIX2,IRNBM,NPSYS
+ REAL, ALLOCATABLE, DIMENSION(:) :: GAR,SIGRES,DILAV,FUN
+ REAL, ALLOCATABLE, DIMENSION(:,:) :: SIG0,SIG1,SIG3,TOTAL,SIGOLD,
+ 1 DILUT
+ LOGICAL, ALLOCATABLE, DIMENSION(:) :: MASKI
+ TYPE(C_PTR), ALLOCATABLE, DIMENSION(:) :: IPISO
+*----
+* DATA STATEMENTS
+*----
+ DATA FACT/0.01,0.1,1.0,10.0,100.0/
+*----
+* SCRATCH STORAGE ALLOCATION
+* SIG0 macroscopic xs of the resonant isotopes as interpolated.
+* SIG1 macroscopic xs of the resonant isotopes at various SIGX.
+* SIG3 macroscopic transport correction.
+*----
+ ALLOCATE(IRES(NBM),MIX2(NBISO),IRNBM(NBM),NPSYS(NGRO))
+ ALLOCATE(SIG0(NBM,NGRO),SIG1(NBM,NGRO),SIG3(NBM,NGRO),
+ 1 TOTAL(NGRO,NBM2),SIGOLD(NGRO,NBM2),GAR(NGRO),SIGRES(NBM),
+ 2 DILAV(NGRO),DILUT(NALPHA,NGRO))
+ ALLOCATE(MASKI(NBISO))
+ ALLOCATE(IPISO(NBISO))
+*----
+* SET THE LCM MICROLIB ISOTOPEWISE DIRECTORIES.
+*----
+ CALL LIBIPS(IPLIB,NBISO,IPISO)
+*----
+* UNLOAD MICROSCOPIC X-S FROM LCM TO SCRATCH STORAGE
+*----
+ IBM=0
+ DO 20 ISO=1,NBISO
+ MIX2(ISO)=0
+ IF(LSHI(ISO).GT.0) THEN
+ IBM=IBM+1
+ MIX2(ISO)=IBM
+ KPLIB=IPISO(ISO) ! set ISO-th isotope
+ CALL LCMGET(KPLIB,'NTOT0',TOTAL(1,IBM))
+ CALL LCMLEN(KPLIB,'NGOLD',LENGT,ITYLCM)
+ IF((LENGT.EQ.NGRO).AND.(.NOT.START).AND.LGC) THEN
+ IF(IMPX.GE.5) WRITE (6,390) (ISONAM(I0,ISO),I0=1,3)
+ CALL LCMGET(KPLIB,'SIGS00',SIGOLD(1,IBM))
+ CALL LCMGET(KPLIB,'NGOLD',GAR)
+ DO 10 LLL=1,NGRO
+ SIGOLD(LLL,IBM)=(1.0-GAR(LLL))*SIGOLD(LLL,IBM)
+ 10 CONTINUE
+ ELSE
+ SIGOLD(:NGRO,IBM)=0.0
+ ENDIF
+ ENDIF
+ 20 CONTINUE
+*----
+* LOOP OVER RESONANT REGIONS. THE CP ARE STORED ON DIRECTORY SHIBA
+*----
+ CALL LCMSIX(IPLIB,'SHIBA',1)
+ DO 260 INRS=1,NRES
+*----
+* FIND THE RESONANT MIXTURE NUMBERS (IRNBM) ASSOCIATED WITH REGION INRS
+*----
+ NBNRS=0
+ DO 50 IBM=1,NBM
+ IRES(IBM)=0
+ DO 40 ISO=1,NBISO
+ IF((MIX(ISO).EQ.IBM).AND.(LSHI(ISO).EQ.INRS)) THEN
+ NBNRS=NBNRS+1
+ IRNBM(NBNRS)=IBM
+ IRES(IBM)=1
+ GO TO 50
+ ENDIF
+ 40 CONTINUE
+ 50 CONTINUE
+ IF(NBNRS.EQ.0) THEN
+ IF(START.AND.(IMPX.GE.1)) WRITE(6,385) 'SHISN2',INRS
+ GO TO 260
+ ELSE IF(START.AND.(NBNRS.GT.1).AND.(IMPX.GE.5)) THEN
+ WRITE (6,380) NBNRS,INRS
+ ENDIF
+*
+ NPSYS(:NGRO)=0
+ DO 120 LLL=1,NGRO
+ LOGDO=.FALSE.
+ DO 60 I=1,NBNRS
+ LOGDO=LOGDO.OR.NOCONV(IRNBM(I),LLL)
+ 60 CONTINUE
+ IF(LOGDO) THEN
+ NPSYS(LLL)=LLL
+*
+* COMPUTE THE LIGHT AND RESONANT COMPONENTS OF THE MACROSCOPIC
+* CROSS SECTIONS IN EACH RESONANT MIXTURE.
+ DO 80 I=1,NBNRS
+ SIGRES(I)=0.0
+ DO 70 ISO=1,NBISO
+ IF((MIX(ISO).EQ.IRNBM(I)).AND.(LSHI(ISO).EQ.INRS)) THEN
+ SIGRES(I)=SIGRES(I)+TOTAL(LLL,MIX2(ISO))*DEN(ISO)
+ ENDIF
+ 70 CONTINUE
+ SIGT(IRNBM(I),LLL)=SIGT(IRNBM(I),LLL)-SIGRES(I)
+ 80 CONTINUE
+ DO 90 IBM=1,NBM
+ SIG0(IBM,LLL)=0.0
+ SIG1(IBM,LLL)=0.0
+ SIG3(IBM,LLL)=SIGT3(IBM,LLL)
+ 90 CONTINUE
+ DO 110 I=1,NBNRS
+ SIG0(IRNBM(I),LLL)=SIGRES(I)
+ SIG3(IRNBM(I),LLL)=0.0
+ 110 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
+ 120 CONTINUE
+*----
+* SET UP VECTORS DILUT AND SIGX.
+*----
+ DILAV(:NGRO)=0.0
+ IF(START) THEN
+* USE A VERY CHEAP APPROXIMATION TO START ITERATIONS.
+ ALLOCATE(FUN(NUN*NGRO))
+ CALL LCMSIX(IPLIB,'--AVERAGE--',1)
+ CALL SHIDST (IPLIB,NPSYS,IPTRK,IFTRAK,CDOOR,IMPX,NBM,NREG,
+ 1 NUN,NGRO,IPHASE,MAT,VOL,KEYFLX,LEAKSW,IRES,SIG0,SIGT,
+ 2 SIGT3(1,1),TITR,FUN,DILAV)
+ CALL LCMSIX(IPLIB,' ',2)
+ DEALLOCATE(FUN)
+ DO 135 LLL=1,NGRO
+ DO 130 IALP=1,NALPHA
+ DILUT(IALP,LLL)=DILAV(LLL)
+ 130 CONTINUE
+ 135 CONTINUE
+ ELSE
+ DO 165 IALP=1,NALPHA
+ DO 150 LLL=1,NGRO
+ IF(NPSYS(LLL).NE.0) THEN
+ DO 140 I=1,NBNRS
+ SIG1(IRNBM(I),LLL)=FACT(IALP)*SIGE(INRS,LLL)
+ 140 CONTINUE
+ ENDIF
+ 150 CONTINUE
+ ALLOCATE(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,
+ 1 NUN,NGRO,IPHASE,MAT,VOL,KEYFLX,LEAKSW,IRES,SIG1,SIGT,
+ 2 SIG3(1,1),TITR,FUN,DILAV)
+ CALL LCMSIX(IPLIB,' ',2)
+ DEALLOCATE(FUN)
+ DO 160 LLL=1,NGRO
+ DILUT(IALP,LLL)=DILAV(LLL)
+ 160 CONTINUE
+ 165 CONTINUE
+ ENDIF
+*----
+* COMPUTE AVERAGE MACROSCOPIC DILUTION X-S (SIGE) USING A THREE-TERM
+* RATIONAL APPROXIMATION.
+*----
+ DO 200 LLL=1,NGRO
+ IF(NPSYS(LLL).NE.0) THEN
+ DO 170 IALP=1,NALPHA
+ SIGX(IALP)=FACT(IALP)*SIGE(INRS,LLL)
+ 170 CONTINUE
+ IMPX2=IMPX
+ IF(START) IMPX2=MAX(0,IMPX-10)
+* **********************************************************
+ CALL SHIRAT(IMPX2,NRAT,SIGX,DILUT(1,LLL),LLL,A,COEF,DENOM)
+* **********************************************************
+ EAV=(COEF(1)*SQRT(DENOM(1))+COEF(2)*SQRT(DENOM(2))+
+ 1 COEF(3)*SQRT(DENOM(3)))**2
+ SIGE(INRS,LLL)=REAL(EAV)
+ IF((.NOT.START).AND.(BIEFF).AND.(NBNRS.EQ.1)) THEN
+* COMPUTE DILAV FOR THE L-J NORMALIZATION.
+ SIGXX=SIG0(IRNBM(1),LLL)
+ PXX=REAL(COEF(1)/(SIGXX+DENOM(1))+COEF(2)/(SIGXX+DENOM(2))
+ 1 +COEF(3)/(SIGXX+DENOM(3)))
+ DILAV(LLL)=1.0/PXX-SIGXX
+ ENDIF
+*----
+* COMPUTE THE ISOTOPE DILUTION MICROSCOPIC CROSS SECTIONS (SN) USED
+* FOR LIBRARY INTERPOLATION.
+*----
+ DO 190 ISO=1,NBISO
+ IF((LSHI(ISO).EQ.INRS).AND.(IRES(MIX(ISO)).EQ.1).AND.
+ 1 (DEN(ISO).NE.0.)) THEN
+ SUM=0.0
+ DO 180 JSO=1,NBISO
+ IBM=MIX(JSO)
+ IF((LSHI(JSO).EQ.INRS).AND.(IBM.EQ.MIX(ISO)).AND.
+ 1 (ISO.NE.JSO)) SUM=SUM+(TOTAL(LLL,MIX2(JSO))-
+ 2 SIGOLD(LLL,MIX2(JSO)))*DEN(JSO)
+ 180 CONTINUE
+ SN(LLL,ISO)=REAL(COEF(1)*SQRT(DENOM(1)+SUM)+COEF(2)*
+ 1 SQRT(DENOM(2)+SUM)+COEF(3)*SQRT(DENOM(3)+SUM))**2/DEN(ISO)
+ IF(SN(LLL,ISO).LE.0.0) THEN
+ WRITE (HSMG,510) (ISONAM(I0,ISO),I0=1,3),SN(LLL,ISO),LLL
+ CALL XABORT(HSMG)
+ ENDIF
+ ELSE IF((LSHI(ISO).EQ.INRS).AND.(IRES(MIX(ISO)).EQ.1).AND.
+ 1 (DEN(ISO).EQ.0.)) THEN
+ SN(LLL,ISO)=1.0E10
+ ENDIF
+ 190 CONTINUE
+ IF((.NOT.START).AND.(IMPX.GE.10)) THEN
+ DO 195 I=1,NBNRS
+ PP=A-SIGT(IRNBM(I),LLL)
+ QQ=SIGE(INRS,LLL)-SIGT(IRNBM(I),LLL)
+ IF(ABS(PP).GT.1.0E-4*SIGT(IRNBM(I),LLL)) THEN
+ BEL=QQ/PP
+ ELSE
+ BEL=0.0
+ ENDIF
+ WRITE (6,610) I,SIGE(INRS,LLL),BEL
+ 195 CONTINUE
+ ENDIF
+ ENDIF
+ 200 CONTINUE
+*----
+* COMPUTE THE ISOTOPE DILUTION MICROSCOPIC CROSS SECTIONS (SB) USED
+* IN L-J NORMALIZATION.
+*----
+ IF((.NOT.START).AND.(BIEFF).AND.(NBNRS.GT.1)) THEN
+* COMPUTE DILAV FOR THE L-J NORMALIZATION.
+ ALLOCATE(FUN(NUN*NGRO))
+ CALL LCMSIX(IPLIB,'--AVERAGE--',1)
+ CALL SHIDST (IPLIB,NPSYS,IPTRK,IFTRAK,CDOOR,IMPX,NBM,NREG,
+ 1 NUN,NGRO,IPHASE,MAT,VOL,KEYFLX,LEAKSW,IRES,SIG0,SIGT,
+ 2 SIGT3(1,1),TITR,FUN,DILAV)
+ CALL LCMSIX(IPLIB,' ',2)
+ DEALLOCATE(FUN)
+ ENDIF
+ DO 250 LLL=1,NGRO
+ IF(NPSYS(LLL).NE.0) THEN
+ DO 220 ISO=1,NBISO
+ IF((LSHI(ISO).EQ.INRS).AND.(IRES(MIX(ISO)).EQ.1).AND.
+ 1 (DEN(ISO).NE.0.)) THEN
+ SUM=0.0
+ DO 210 JSO=1,NBISO
+ IBM=MIX(JSO)
+ IF((LSHI(JSO).EQ.INRS).AND.(IBM.EQ.MIX(ISO)).AND.
+ 1 (ISO.NE.JSO)) SUM=SUM+TOTAL(LLL,MIX2(JSO))*DEN(JSO)
+ 210 CONTINUE
+ IF(START.OR.(.NOT.BIEFF)) THEN
+ SB(LLL,ISO)=SN(LLL,ISO)
+ ELSE
+ SB(LLL,ISO)=(DILAV(LLL)+SUM)/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)
+ ELSE IF(SB(LLL,ISO).LT.SN(LLL,ISO)) THEN
+ IF(SB(LLL,ISO).LT.0.99*SN(LLL,ISO)) WRITE (6,520)
+ 1 (ISONAM(I0,ISO),I0=1,3),SB(LLL,ISO)/SN(LLL,ISO),LLL
+ SB(LLL,ISO)=SN(LLL,ISO)
+ ENDIF
+ ENDIF
+ ELSE IF((LSHI(ISO).EQ.INRS).AND.(IRES(MIX(ISO)).EQ.1).AND.
+ 1 (DEN(ISO).EQ.0.)) THEN
+ SB(LLL,ISO)=1.0E10
+ ENDIF
+ 220 CONTINUE
+*
+* RESTORE SIGT ARRAY.
+ DO 240 I=1,NBNRS
+ SIGRES(I)=0.0
+ DO 230 ISO=1,NBISO
+ IF((MIX(ISO).EQ.IRNBM(I)).AND.(LSHI(ISO).EQ.INRS)) THEN
+ SIGRES(I)=SIGRES(I)+TOTAL(LLL,MIX2(ISO))*DEN(ISO)
+ ENDIF
+ 230 CONTINUE
+ SIGT(IRNBM(I),LLL)=SIGT(IRNBM(I),LLL)+SIGRES(I)
+ 240 CONTINUE
+ ENDIF
+ 250 CONTINUE
+ 260 CONTINUE
+ CALL LCMSIX(IPLIB,' ',2)
+*----
+* 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 290 ISO=1,NBISO
+ LOGDO=START.OR.(DEN(ISO).NE.0.)
+ MASKI(ISO)=(LSHI(ISO).GT.0).AND.LOGDO
+ 290 CONTINUE
+ IMPX2=MAX(0,IMPX-1)
+ CALL LIBLIB (IPLIB,NBISO,MASKI,IMPX2)
+ DO 320 ISO=1,NBISO
+ IBM=MIX(ISO)
+ IF((LSHI(ISO).GT.0).AND.(IBM.GT.0).AND.(DEN(ISO).NE.0.)) THEN
+ KPLIB=IPISO(ISO) ! set ISO-th isotope
+ CALL LCMGET(KPLIB,'NTOT0',GAR)
+ DO 300 LLL=1,NGRO
+ TOTAL(LLL,MIX2(ISO))=TOTAL(LLL,MIX2(ISO))-GAR(LLL)
+ 300 CONTINUE
+ DO 310 LLL=1,NGRO
+ IF(NOCONV(IBM,LLL)) SIGT(IBM,LLL)=SIGT(IBM,LLL)-DEN(ISO)*
+ 1 TOTAL(LLL,MIX2(ISO))
+ 310 CONTINUE
+ ENDIF
+ 320 CONTINUE
+*----
+* SCRATCH STORAGE DEALLOCATION
+*----
+ DEALLOCATE(IPISO)
+ DEALLOCATE(MASKI)
+ DEALLOCATE(DILUT,DILAV,SIGRES,GAR,SIGOLD,TOTAL,SIG3,SIG1,SIG0)
+ DEALLOCATE(NPSYS,IRNBM,MIX2,IRES)
+ RETURN
+*
+ 380 FORMAT(/16H SHISN2: MERGING,I3,30H RESONANT MIXTURES IN RESONANT,
+ 1 14H REGION NUMBER,I3,1H.)
+ 385 FORMAT(A6,1X,': RESONANT REGION =',I10,1X,'NOT USED.')
+ 390 FORMAT(/53H SHISN2: GOLDSTEIN AND COHEN APPROXIMATION USED FOR I,
+ 1 8HSOTOPE ',3A4,2H'.)
+ 400 FORMAT(1X,'TOTAL MACROSCOPIC CROSS SECTIONS OF THE RESONANT ',
+ 1'MATERIALS IN EACH MIXTURE (GROUP',I5,'):'/(1X,1P,11E11.3))
+ 410 FORMAT(1X,'TOTAL MACROSCOPIC CROSS SECTIONS OF THE OTHER ',
+ 1'MATERIALS IN EACH MIXTURE (GROUP',I5,'):'/(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))
+ 510 FORMAT(30HSHISN2: THE RESONANT ISOTOPE ',3A4,14H' HAS A NEGATI,
+ 1 27HVE DILUTION CROSS-SECTION (,1P,E14.4,0P,10H) IN GROUP,I4,1H.)
+ 515 FORMAT(30HSHISN2: 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 SHISN2: THE L-J EQUIVALENCE FACTOR OF RESONANT ISOTOP,
+ 1 3HE ',3A4,18H' WAS CHANGED FROM,F6.3,16H TO 1.0 IN GROUP,I4,1H.)
+ 610 FORMAT(8X,8HAVERAGE(,I2,1H),1P,E13.5/8X,11HBELL FACTOR,E13.5)
+ END