Geant4 9.6.0
Toolkit for the simulation of the passage of particles through matter
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G4FissionParameters.cc
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27// $Id$
28//
29// Hadronic Process: Nuclear De-excitations
30// by V. Lara (Oct 1998)
31//
32//J. M. Quesada (May 2009): sigma_sym (SigmaS) tuned for spallation data.
33//J. M. Quesada (30.10.09): retuning for IAEA spallation data
34
36#include "G4SystemOfUnits.hh"
38
39
40const G4double G4FissionParameters::A1 = 134.0;
41const G4double G4FissionParameters::A2 = 141.0;
42
44 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
57 //JMQ 310509
58 // if (SigmaS > 20.0) SigmaS = 20.0;
59 // SigmaS*=1.3;
60 //JMQ 301009: retuning (after CEM transition prob.have been chosen as default)
61 SigmaS*=0.8;
62 //
63
64 G4double FasymAsym = 2.0*std::exp(-((A2-As)*(A2-As))/(2.0*Sigma2*Sigma2)) +
65 std::exp(-((A1-As)*(A1-As))/(2.0*Sigma1*Sigma1));
66
67 G4double FsymA1A2 = std::exp(-((As-(A1+A2)/2.0)*(As-(A1+A2)/2.0))
68 /(2.0*SigmaS*SigmaS));
69
70
71 G4double wa = 0.0;
72 w = 0.0;
73 if (Z >= 90) { // Z >= 90
74 if (U <= 16.25) wa = std::exp(0.5385*U/MeV-9.9564); // U <= 16.25 MeV
75 else wa = std::exp(0.09197*U/MeV-2.7003); // U > 16.25 MeV
76 } else if (Z == 89) { // Z == 89
77 wa = std::exp(0.09197*U-1.0808);
78 } else if (Z >= 82) { // 82 <= Z <= 88
79 G4double X = FissionBarrier - 7.5*MeV;
80 if (X < 0.0) X = 0.0;
81 wa = std::exp(0.09197*(U-X)/MeV-1.0808);
82 } else { // Z < 82
83 w = 1001.0;
84 }
85
86 if (w == 0.0) {
87 G4double w1 = std::max(1.03*wa - FasymAsym, 0.0001);
88 G4double w2 = std::max(1.0 - FsymA1A2*wa, 0.0001);
89
90 w = w1/w2;
91
92 if (82 <= Z && Z < 89 && A < 227) w *= std::exp(0.3*(227-A));
93 }
94
95}
96
98{}
99
double G4double
Definition: G4Types.hh:64
int G4int
Definition: G4Types.hh:66
G4FissionParameters(G4int A, G4int Z, G4double ExEnergy, G4double FissionBarrier)