Geant4 11.1.1
Toolkit for the simulation of the passage of particles through matter
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G4FissionParameters.cc
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28// Hadronic Process: Nuclear De-excitations
29// by V. Lara (Oct 1998)
30//
31//J. M. Quesada (May 2009): sigma_sym (SigmaS) tuned for spallation data.
32//J. M. Quesada (30.10.09): retuning for IAEA spallation data
33
35#include "G4SystemOfUnits.hh"
36
38 : A1(134),A2(141),A3((A1 + A2)*0.5),As(0.0),Sigma1(0.0),Sigma2(0.0),
39 SigmaS(0.),w(0.0)
40{}
41
43{}
44
46 G4double FissionBarrier)
47{
48 // to avoid usage of units
49 G4double U = std::min(200., ExEnergy/CLHEP::MeV);
50
51 As = A*0.5;
52
53 if (A <= 235) { Sigma2 = 5.6; }
54 else { Sigma2 = 5.6 + 0.096*(A-235); }
55
56 Sigma1 = 0.5*Sigma2;
57
58 //JMQ 310509
59 // if (SigmaS > 20.0) SigmaS = 20.0;
60 // SigmaS*=1.3;
61 //JMQ 301009: retuning (after CEM transition prob.have been chosen as default)
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-9.9564); }
68 else { wa = G4Exp(0.09197*U-2.7003); }
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/CLHEP::MeV - 7.5);
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) + LocalExp(x1);
82
83 G4double x3 = (As-A3)/SigmaS;
84 G4double FsymA1A2 = LocalExp(x3);
85
86 G4double w1 = std::max(1.03*wa - FasymAsym, 0.0001);
87 G4double w2 = std::max(1.0 - FsymA1A2*wa, 0.0001);
88
89 w = w1/w2;
90
91 if (A < 227) { w *= G4Exp(0.3*(227-A)); }
92 }
93}
94
95
G4double G4Exp(G4double initial_x)
Exponential Function double precision.
Definition: G4Exp.hh:180
double G4double
Definition: G4Types.hh:83
int G4int
Definition: G4Types.hh:85
const G4int Z[17]
const G4double A[17]
void DefineParameters(G4int A, G4int Z, G4double ExEnergy, G4double FissionBarrier)