| 1 | SUBROUTINE PIGEN1
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| 2 | C
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| 3 | C*********************************************************************
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| 4 | C DESIGN : D. HECK IK3 FZK KARLSRUHE
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| 5 | C DATE : JUL 31, 1989
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| 6 | C*********************************************************************
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| 7 | C THIS SUBROUTINE DESCRIBES THE PHOTONUCLEAR REACTION
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| 8 | C GAMMA + NUCLEON -----> PION + NUCLEON
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| 9 | C*********************************************************************
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| 10 | DOUBLE PRECISION BETA,DUMMY,ENUCL,ESQ,E3CM,GAMMA
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| 11 | DOUBLE PRECISION PEIG,PEOP,PT,PTRANS,P3CM,W0,W0I,W0S,W0SI
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| 12 | *KEEP,ELABCT.
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| 13 | COMMON /ELABCT/ ELCUT
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| 14 | DOUBLE PRECISION ELCUT(4)
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| 15 | *KEEP,PAM.
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| 16 | COMMON /PAM/ PAMA,SIGNUM
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| 17 | DOUBLE PRECISION PAMA(6000),SIGNUM(6000)
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| 18 | *KEEP,PARPAR.
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| 19 | COMMON /PARPAR/ CURPAR,SECPAR,PRMPAR,OUTPAR,C,
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| 20 | * E00,E00PN,PTOT0,PTOT0N,THICKH,ITYPE,LEVL
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| 21 | DOUBLE PRECISION CURPAR(14),SECPAR(14),PRMPAR(14),OUTPAR(14),
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| 22 | * C(50),E00,E00PN,PTOT0,PTOT0N,THICKH
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| 23 | INTEGER ITYPE,LEVL
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| 24 | *KEND.
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| 25 | DOUBLE PRECISION PI0MSQ
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| 26 | COMMON/PION/PI0MSQ,PITHR,PICMAS,PI0MAS,AMASK0,AMASKC,AMASPR,AMASNT
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| 27 | *
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| 28 | *KEEP,RANDPA.
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| 29 | COMMON /RANDPA/ FAC,U1,U2,RD,NSEQ,ISEED,KNOR
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| 30 | DOUBLE PRECISION FAC,U1,U2
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| 31 | REAL RD(3000)
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| 32 | INTEGER ISEED(103,10),NSEQ
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| 33 | LOGICAL KNOR
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| 34 | *KEEP,RUNPAR.
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| 35 | COMMON /RUNPAR/ FIXHEI,THICK0,HILOECM,HILOELB,
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| 36 | * STEPFC,NRRUN,NSHOW,PATAPE,MONIIN,
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| 37 | * MONIOU,MDEBUG,NUCNUC,
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| 38 | * CETAPE,
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| 39 | * SHOWNO,ISHW,NOPART,NRECS,NBLKS,MAXPRT,NDEBDL,
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| 40 | * N1STTR,MDBASE,
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| 41 | * DEBDEL,DEBUG,FDECAY,FEGS,FIRSTI,FIXINC,FIXTAR,
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| 42 | * FIX1I,FMUADD,FNKG,FPRINT,FDBASE
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| 43 | * ,GHEISH,GHESIG
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| 44 | COMMON /RUNPAC/ DSN,HOST,USER
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| 45 | DOUBLE PRECISION FIXHEI,THICK0,HILOECM,HILOELB
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| 46 | REAL STEPFC
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| 47 | INTEGER NRRUN,NSHOW,PATAPE,MONIIN,MONIOU,MDEBUG,NUCNUC,
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| 48 | * SHOWNO,ISHW,NOPART,NRECS,NBLKS,MAXPRT,NDEBDL,
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| 49 | * N1STTR,MDBASE
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| 50 | INTEGER CETAPE
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| 51 | CHARACTER*79 DSN
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| 52 | CHARACTER*20 HOST,USER
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| 53 |
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| 54 | LOGICAL DEBDEL,DEBUG,FDECAY,FEGS,FIRSTI,FIXINC,FIXTAR,
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| 55 | * FIX1I,FMUADD,FNKG,FPRINT,FDBASE
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| 56 | * ,GHEISH,GHESIG
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| 57 | *KEEP,STACKE.
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| 58 | COMMON/STACKE/ E,TIME,X,Y,Z,U,V,W,DNEAR,IQ,IGEN,IR,IOBS,LPCTE,NP
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| 59 | DOUBLE PRECISION E(60),TIME(60)
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| 60 | REAL X(60),Y(60),Z(60),U(60),V(60),W(60),DNEAR(60)
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| 61 | INTEGER IQ(60),IGEN(60),IR(60),IOBS(60),LPCTE(60),NP
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| 62 | *KEND.
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| 63 | COMMON/UPHIOT/THETA,SINTHE,COSTHE,SINPHI, COSPHI,PI,TWOPI,PI5D2
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| 64 | COMMON/ACLOCK/NCLOCK,JCLOCK
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| 65 | C_____IF (NCLOCK.GT.JCLOCK) THEN
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| 66 | C______WRITE(MDEBUG,* )' PIGEN1:NP=',NP,' IR=',IR(NP),' IOBS=',IOBS(NP)
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| 67 | C______CALL AUSGB2
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| 68 | C_____END IF
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| 69 | IF(DEBUG)WRITE(MDEBUG,*)'PIGEN1: E=',E(NP)
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| 70 | PEIG=E(NP)
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| 71 | C*** NUMBERS AT THE VARIABLES MEAN :
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| 72 | C*** 1 INCOMING GAMMA RAY
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| 73 | C*** 2 HIT NUCLEON
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| 74 | C*** 3 PRODUCED PION
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| 75 | C*** 4 RECOILING NUCLEON
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| 76 | C*** LOOK WHICH TYPE OF REACTION
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| 77 | CALL RMMAR(RD,2,2)
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| 78 | RNNO91=RD(1)
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| 79 | RNNO92=RD(2)
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| 80 | C*** 0.49923 IS THE FRACTION OF PROTONS IN AIR
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| 81 | IF (RNNO91.LE.0.49923) THEN
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| 82 | C *** HIT NUCLEON IS PROTON
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| 83 | AMASS2=AMASPR
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| 84 | C *** 33% CHANCE FOR CHARGE EXCHANGE
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| 85 | IF (RNNO92.LE.0.333333) THEN
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| 86 | C *** PI(+) + NEUTRON PRODUCED
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| 87 | IQ(NP)=8
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| 88 | IQ(NP+1)=13
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| 89 | ELSE
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| 90 | C *** PI(0) + PROTON PRODUCED
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| 91 | IQ(NP)=7
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| 92 | IQ(NP+1)=14
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| 93 | END IF
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| 94 | ELSE
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| 95 | C *** HIT NUCLEON IS NEUTRON
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| 96 | AMASS2=AMASNT
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| 97 | C *** 33% CHANCE FOR CHARGE EXCHANGE
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| 98 | IF (RNNO92.LE.0.333333) THEN
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| 99 | C *** PI(-) + PROTON PRODUCED
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| 100 | IQ(NP)=9
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| 101 | IQ(NP+1)=14
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| 102 | ELSE
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| 103 | C *** PI(0) + NEUTRON PRODUCED
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| 104 | IQ(NP)=7
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| 105 | IQ(NP+1)=13
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| 106 | END IF
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| 107 | END IF
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| 108 | AMAS2I=1./AMASS2
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| 109 | C*** NOTE: THE ENERGIES IN EGS ARE IN MEV, IN CORSIKA IN GEV
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| 110 | AMASS3=PAMA(IQ(NP))*1.D3
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| 111 | AMASS4=PAMA(IQ(NP+1))*1.D3
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| 112 | C*** TOTAL LABORATORY ENERGY AND ITS INVERSE
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| 113 | W0 =PEIG+AMASS2
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| 114 | W0I=1.D0/W0
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| 115 | C*** TOTAL.C.M. ENERGY AND INVERSE OF TOTAL C.M.ENERGY
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| 116 | W0S = SQRT(AMASS2*(AMASS2+2.D0*PEIG))
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| 117 | W0SI=1.D0/W0S
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| 118 | C*** THRESHOLD ENERGY
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| 119 | ETH=0.5*((AMASS3+AMASS4)**2-AMASS2**2)*AMAS2I
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| 120 | C*** BETA,GAMMA, ESQ, BRATIO, G3 ARE AUXILIARY QUANTITIES
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| 121 | BETA=PEIG*W0I
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| 122 | GAMMA=W0*W0SI
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| 123 | ED =0.5*((AMASS3-AMASS4)**2-AMASS2**2)*AMAS2I
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| 124 | ESQ = SQRT((PEIG-ETH)*(PEIG-ED))
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| 125 | BRATIO = PEIG/ESQ
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| 126 | G3 = W0I*BRATIO*(PEIG-ETH+AMASS3*AMAS2I*(AMASS3+AMASS4))
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| 127 | C*** C.M. ENERGY OF PION
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| 128 | E3CM=G3*AMASS2*GAMMA/BRATIO
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| 129 | C*** C.M. PION MOMENTUM
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| 130 | P3CM=AMASS2*W0SI*ESQ
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| 131 | B3CM2=P3CM**2/(P3CM**2+AMASS3**2)
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| 132 | B3CM=SQRT(B3CM2)
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| 133 | C*** DETERMINE THETA IN C.M. SYSTEM BY CHANCE.
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| 134 | IF (PEIG.LE.900.D0) THEN
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| 135 | C *** PHOTON ENERGY IS BELOW 900 MEV
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| 136 | 210 CONTINUE
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| 137 | CALL RMMAR(RD,2,2)
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| 138 | RNNO93=RD(1)
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| 139 | RNNO94=RD(2)
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| 140 | IF (IQ(NP).EQ.7) THEN
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| 141 | C *** NEUTRAL PION EMITTED, TAKE PURE
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| 142 | C *** DIPOLE RADIATION: W(COSTH) = 1-3/5*COSTH**2
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| 143 | COSTE3 = 2.*RNNO93-1.
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| 144 | IF((RNNO94 .GT. 1.-0.6*COSTE3**2))GOTO 210
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| 145 | ELSE
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| 146 | C *** CHARGED PION EMITTED, TAKE MODIFIED DIPOLE RADIATION
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| 147 | C *** WITH ASYMMETRY TERM 1/(1-BETACM*COSTE3)**2
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| 148 | COSTE3 = 1./B3CM-1./(RNNO93*2.*B3CM2/(1.-B3CM2)+B3CM/(1.+B3CM))
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| 149 | IF((RNNO94*2.5 .GT. 1.+COSTE3*(-1.8+COSTE3*(.65+COSTE3*(.34 -.18
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| 150 | * *COSTE3 )))))GOTO 210
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| 151 | END IF
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| 152 | ELSE IF(PEIG.LE.1300.D0) THEN
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| 153 | C *** PHOTON ENERGY BETWEEN 900 AND 1300 MEV
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| 154 | 220 CONTINUE
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| 155 | CALL RMMAR(RD,2,2)
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| 156 | RNNO93=RD(1)
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| 157 | RNNO94=RD(2)
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| 158 | IF (IQ(NP).EQ.7) THEN
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| 159 | C *** NEUTRAL PION EMITTED, TAKE PURE QUADRUPOLE
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| 160 | C *** RADIATION: W(COSTH) = 1+6*COSTH**2-5*COSTH**4
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| 161 | COSTE3 = 2.*RNNO93-1.
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| 162 | IF((2.8*RNNO94 .GT. 1.+6.*COSTE3**2-5.*COSTE3**4))GOTO 220
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| 163 | ELSE
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| 164 | C *** CHARGED PION EMITTED, TAKE MODIFIED QUADRUPOLE
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| 165 | C *** RADIATION WITH ASYMMETRY TERM: 1/(1-BETACM*COSTE3)**2
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| 166 | COSTE3 = 1./B3CM-1./(RNNO93*2.*B3CM2/(1.-B3CM2)+B3CM/(1.+B3CM))
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| 167 | IF((13.2*RNNO94 .GT. 1.+COSTE3*(-2.18+COSTE3*(7.20+COSTE3*(-2.55
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| 168 | * +COSTE3*(-15.39+COSTE3*(6.36+COSTE3*(13.80-COSTE3*8.235))))))))
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| 169 | * GOTO 220
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| 170 | END IF
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| 171 | ELSE
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| 172 | C *** ABOVE 1300 MEV THE ANGULAR DISTRIBUTION IS DETERMINED
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| 173 | C *** BY THE TRANSVERSE MOMENTUM OF THE PION
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| 174 | PT=1.D3*PTRANS(DUMMY)
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| 175 | COSTE3=SQRT(MAX(0.D0,P3CM**2-PT**2))/P3CM
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| 176 | END IF
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| 177 | C*** PRECISE ENERGY OUTGOING PION = PEOP
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| 178 | PEOP =GAMMA*(E3CM+BETA*P3CM*COSTE3)
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| 179 | C*** ENERGY OF OUTGOING PION IN STACK POSITION NP
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| 180 | E(NP)=PEOP
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| 181 | C*** MOMENTUM OF OUTGOING PION = AMOM3
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| 182 | C*** COSTHE AND SINTHE ARE ANGLES IN LAB SYSTEM FOR PARTICLE 3 (PION)
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| 183 | C*** SEE SLAC-265, P. 52
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| 184 | AMOM3=SQRT(MAX(0.D0,PEOP**2-AMASS3**2))
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| 185 | IF (AMOM3.GT.0.) THEN
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| 186 | COSTHE=(AMASS4**2-AMASS2**2-AMASS3**2+2.*PEOP*W0-2.*PEIG*AMASS2)
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| 187 | * /(2.*PEIG* AMOM3)
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| 188 | ELSE
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| 189 | COSTHE=1.
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| 190 | END IF
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| 191 | SINTHE= SQRT(MAX(0.0,1.-COSTHE**2))
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| 192 | CALL UPHI(2,1)
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| 193 | C*** TOTAL ENERGY OF RECOILING NUCLEON = ENUCL
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| 194 | ENUCL=W0-PEOP
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| 195 | IF ((ENUCL-AMASS4).GT.ELCUT(1)*1000.D0) THEN
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| 196 | C *** RECOIL ENERGY IS TOO LARGE, MUST TREAT THE NUCLEON
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| 197 | NP=NP+1
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| 198 | E(NP)=ENUCL
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| 199 | C *** MOMENTUM OF RECOIL NUCLEON
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| 200 | AMOM4=SQRT(ENUCL**2-AMASS4**2)
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| 201 | C *** COSTHE AND SINTHE ARE ANGLES IN LAB SYSTEM FOR RECOIL NUCLEON
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| 202 | C *** SEE SLAC-265, P. 52
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| 203 | COSTHE=(AMASS3**2-AMASS2**2-AMASS4**2+2.*ENUCL*W0-2.*PEIG*AMASS2)
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| 204 | * / (2. * PEIG*AMOM4)
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| 205 | SINTHE=-SQRT(MAX(0.0,1.-COSTHE**2))
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| 206 | CALL UPHI(3,2)
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| 207 | IF (W(NP).GT.C(29)) THEN
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| 208 | C *** ANGLE WITH RESPECT TO X AXIS
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| 209 | IF (U(NP)**2+V(NP)**2.GT.3.E-38) THEN
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| 210 | ANGLEX = -ATAN2(V(NP),U(NP))
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| 211 | ELSE
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| 212 | ANGLEX = 0.
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| 213 | END IF
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| 214 | C *** ADD NUCLEON TO CORSIKA STACK
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| 215 | SECPAR(1)=IQ(NP)
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| 216 | SECPAR(2)=E(NP)/AMASS4
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| 217 | SECPAR(3)=W(NP)
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| 218 | SECPAR(4)=ANGLEX
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| 219 | SECPAR(5)=-Z(NP)
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| 220 | SECPAR(6)=TIME(NP)
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| 221 | SECPAR(7)=X(NP)
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| 222 | SECPAR(8)=-Y(NP)
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| 223 | SECPAR(11)=1.D0
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| 224 | SECPAR(12)=0.D0
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| 225 | CALL TSTOUT
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| 226 | END IF
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| 227 | C *** ELIMINATE NUCLEON FROM EGS-STACK
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| 228 | NP=NP-1
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| 229 | END IF
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| 230 | C*** END OF RECOIL NUCLEON TREATEMENT CASE
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| 231 | RETURN
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| 232 | END
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