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Lara (Oct 1998) 31 // by V. Lara (Oct 1998) 30 // 32 // 31 //J. M. Quesada (May 2009): sigma_sym (SigmaS) << 33 32 //J. M. Quesada (30.10.09): retuning for IAEA << 33 34 34 #include "G4FissionParameters.hh" 35 #include "G4FissionParameters.hh" 35 #include "G4SystemOfUnits.hh" << 36 #include "G4HadronicException.hh" 36 37 37 G4FissionParameters::G4FissionParameters() << 38 : A1(134),A2(141),A3((A1 + A2)*0.5),As(0.0), << 39 SigmaS(0.),w(0.0) << 40 {} << 41 38 42 G4FissionParameters::~G4FissionParameters() << 39 const G4double G4FissionParameters::A1 = 134.0; 43 {} << 40 const G4double G4FissionParameters::A2 = 141.0; 44 41 45 void G4FissionParameters::DefineParameters(G4i << 46 G4double FissionBarrier) << 47 { << 48 // to avoid usage of units << 49 G4double U = std::min(200., ExEnergy/CLHEP:: << 50 42 51 As = A*0.5; << 43 G4FissionParameters::G4FissionParameters(const G4int A, const G4int Z, const G4double ExEnergy, >> 44 const G4double FissionBarrier) >> 45 { >> 46 G4double U = ExEnergy; >> 47 >> 48 As = A/2.0; >> 49 >> 50 if (A <= 235) Sigma2 = 5.6; // MeV >> 51 else Sigma2 = 5.6 + 0.096*(A-235); // MeV >> 52 >> 53 Sigma1 = 0.5*Sigma2; // MeV >> 54 >> 55 SigmaS = std::exp(0.00553*U/MeV + 2.1386); // MeV >> 56 if (SigmaS > 20.0) SigmaS = 20.0; >> 57 >> 58 G4double FasymAsym = 2.0*std::exp(-((A2-As)*(A2-As))/(2.0*Sigma2*Sigma2)) + >> 59 std::exp(-((A1-As)*(A1-As))/(2.0*Sigma1*Sigma1)); >> 60 >> 61 G4double FsymA1A2 = std::exp(-((As-(A1+A2)/2.0)*(As-(A1+A2)/2.0))/(2.0*SigmaS*SigmaS)); >> 62 >> 63 >> 64 G4double wa = 0.0; >> 65 w = 0.0; >> 66 if (Z >= 90) { // Z >= 90 >> 67 if (U <= 16.25) wa = std::exp(0.5385*U/MeV-9.9564); // U <= 16.25 MeV >> 68 else wa = std::exp(0.09197*U/MeV-2.7003); // U > 16.25 MeV >> 69 } else if (Z == 89) { // Z == 89 >> 70 wa = std::exp(0.09197*U-1.0808); >> 71 } else if (Z >= 82) { // 82 <= Z <= 88 >> 72 G4double X = FissionBarrier - 7.5*MeV; >> 73 if (X < 0.0) X = 0.0; >> 74 wa = std::exp(0.09197*(U-X)/MeV-1.0808); >> 75 } else { // Z < 82 >> 76 w = 1001.0; >> 77 } >> 78 >> 79 if (w == 0.0) { >> 80 G4double w1 = std::max(1.03*wa - FasymAsym, 0.0001); >> 81 G4double w2 = std::max(1.0 - FsymA1A2*wa, 0.0001); 52 82 53 if (A <= 235) { Sigma2 = 5.6; } << 83 w = w1/w2; 54 else { Sigma2 = 5.6 + 0.096*(A-235) << 55 84 56 Sigma1 = 0.5*Sigma2; << 85 if (82 <= Z && Z < 89 && A < 227) w *= std::exp(0.3*(227-A)); 57 << 86 } 58 //JMQ 310509 << 87 59 // if (SigmaS > 20.0) SigmaS = 20.0; << 88 } 60 // SigmaS*=1.3; << 61 //JMQ 301009: retuning (after CEM transition << 62 SigmaS = 0.8*G4Exp(0.00553*U + 2.1386); << 63 << 64 G4double wa = 0.0; << 65 w = 0.0; << 66 if (Z >= 90) { << 67 if (U <= 16.25) { wa = G4Exp(0.5385*U-9.95 << 68 else { wa = G4Exp(0.09197*U-2.7 << 69 } else if (Z == 89) { << 70 wa = G4Exp(0.09197*U-1.0808); << 71 } else if (Z >= 82) { << 72 G4double X = std::max(0.0, FissionBarrier/ << 73 wa = G4Exp(0.09197*(U-X) - 1.0808); << 74 } else { // Z < 82 << 75 w = 1001.0; << 76 } << 77 << 78 if (Z >= 82) { << 79 G4double x1 = (A1-As)/Sigma1; << 80 G4double x2 = (A2-As)/Sigma2; << 81 G4double FasymAsym = 2*LocalExp(x2) + Loca << 82 << 83 G4double x3 = (As-A3)/SigmaS; << 84 G4double FsymA1A2 = LocalExp(x3); << 85 89 86 G4double w1 = std::max(1.03*wa - FasymAsym << 90 87 G4double w2 = std::max(1.0 - FsymA1A2*wa, << 91 G4FissionParameters::G4FissionParameters(const G4FissionParameters &) 88 << 92 { 89 w = w1/w2; << 93 throw G4HadronicException(__FILE__, __LINE__, "G4FissionParameters::copy_constructor meant to not be accessable"); 90 << 94 } 91 if (A < 227) { w *= G4Exp(0.3*(227-A)); } << 95 92 } << 96 >> 97 const G4FissionParameters & G4FissionParameters::operator=(const G4FissionParameters &) >> 98 { >> 99 throw G4HadronicException(__FILE__, __LINE__, "G4FissionParameters::operator= meant to not be accessable"); >> 100 return *this; >> 101 } >> 102 >> 103 >> 104 G4bool G4FissionParameters::operator==(const G4FissionParameters &) const >> 105 { >> 106 return false; >> 107 } >> 108 >> 109 G4bool G4FissionParameters::operator!=(const G4FissionParameters &) const >> 110 { >> 111 return true; 93 } 112 } 94 113 95 114 96 115