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geant4/source/processes/hadronic/models/de_excitation/fission/src/G4FissionParameters.cc
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2019-12-06 15:12:28 +01:00

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// Hadronic Process: Nuclear De-excitations
// by V. Lara (Oct 1998)
//
//J. M. Quesada (May 2009): sigma_sym (SigmaS) tuned for spallation data.
//J. M. Quesada (30.10.09): retuning for IAEA spallation data
#include "G4FissionParameters.hh"
#include "G4SystemOfUnits.hh"
G4FissionParameters::G4FissionParameters()
: A1(134),A2(141),A3((A1 + A2)*0.5),As(0.0),Sigma1(0.0),Sigma2(0.0),
SigmaS(0.),w(0.0)
{}
G4FissionParameters::~G4FissionParameters()
{}
void G4FissionParameters::DefineParameters(G4int A, G4int Z, G4double ExEnergy,
G4double FissionBarrier)
{
// to avoid usage of units
G4double U = std::min(200., ExEnergy/CLHEP::MeV);
As = A*0.5;
if (A <= 235) { Sigma2 = 5.6; }
else { Sigma2 = 5.6 + 0.096*(A-235); }
Sigma1 = 0.5*Sigma2;
//JMQ 310509
// if (SigmaS > 20.0) SigmaS = 20.0;
// SigmaS*=1.3;
//JMQ 301009: retuning (after CEM transition prob.have been chosen as default)
SigmaS = 0.8*G4Exp(0.00553*U + 2.1386);
G4double wa = 0.0;
w = 0.0;
if (Z >= 90) {
if (U <= 16.25) { wa = G4Exp(0.5385*U-9.9564); }
else { wa = G4Exp(0.09197*U-2.7003); }
} else if (Z == 89) {
wa = G4Exp(0.09197*U-1.0808);
} else if (Z >= 82) {
G4double X = std::max(0.0, FissionBarrier/CLHEP::MeV - 7.5);
wa = G4Exp(0.09197*(U-X) - 1.0808);
} else { // Z < 82
w = 1001.0;
}
if (Z >= 82) {
G4double x1 = (A1-As)/Sigma1;
G4double x2 = (A2-As)/Sigma2;
G4double FasymAsym = 2*LocalExp(x2) + LocalExp(x1);
G4double x3 = (As-A3)/SigmaS;
G4double FsymA1A2 = LocalExp(x3);
G4double w1 = std::max(1.03*wa - FasymAsym, 0.0001);
G4double w2 = std::max(1.0 - FsymA1A2*wa, 0.0001);
w = w1/w2;
if (A < 227) { w *= G4Exp(0.3*(227-A)); }
}
}