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// Hadronic Process: Nuclear De-excitations
// by V. Lara (Oct 1998)
#ifndef G4CompetitiveFission_h
#define G4CompetitiveFission_h 1
#include "G4VEvaporationChannel.hh"
#include "G4Fragment.hh"
#include "G4VEmissionProbability.hh"
#include "G4FissionParameters.hh"
#include <CLHEP/Units/SystemOfUnits.h>
#include "G4Exp.hh"
class G4VFissionBarrier;
class G4VEmissionProbability;
class G4VLevelDensityParameter;
class G4PairingCorrection;
class G4CompetitiveFission : public G4VEvaporationChannel
{
public:
G4CompetitiveFission();
~G4CompetitiveFission() override;
void Initialise() override;
G4Fragment* EmittedFragment(G4Fragment* theNucleus) override;
G4double GetEmissionProbability(G4Fragment* theNucleus) override;
void SetFissionBarrier(G4VFissionBarrier * aBarrier);
void SetEmissionStrategy(G4VEmissionProbability * aFissionProb);
void SetLevelDensityParameter(G4VLevelDensityParameter * aLevelDensity);
inline G4double GetFissionBarrier(void) const;
inline G4double GetLevelDensityParameter(void) const;
inline G4double GetMaximalKineticEnergy(void) const;
G4CompetitiveFission(const G4CompetitiveFission &right) = delete;
const G4CompetitiveFission & operator=(const G4CompetitiveFission &right) = delete;
G4bool operator==(const G4CompetitiveFission &right) const = delete;
G4bool operator!=(const G4CompetitiveFission &right) const = delete;
private:
// Sample AtomicNumber of Fission products
G4int FissionAtomicNumber(G4int A);
G4double MassDistribution(G4double x, G4int A);
// Sample Charge of fission products
G4int FissionCharge(G4int A, G4int Z, G4double Af);
// Sample Kinetic energy of fission products
G4double FissionKineticEnergy(G4int A, G4int Z,
G4int Af1, G4int Zf1,
G4int Af2, G4int Zf2,
G4double U, G4double Tmax);
inline G4double Ratio(G4double A, G4double A11,
G4double B1, G4double A00) const;
inline G4double SymmetricRatio(G4int A, G4double A11) const;
inline G4double AsymmetricRatio(G4int A, G4double A11) const;
inline G4double LocalExp(G4double x) const;
// Maximal Kinetic Energy that can be carried by fragment
G4double maxKineticEnergy{0.0};
G4double fissionBarrier{0.0};
G4double fissionProbability{0.0};
G4double fFactor{1.0};
// For Fission barrier
G4VFissionBarrier* theFissionBarrierPtr;
// For Fission probability emission
G4VEmissionProbability* theFissionProbabilityPtr;
// For Level Density calculation
G4VLevelDensityParameter* theLevelDensityPtr;
G4PairingCorrection* pairingCorrection;
G4bool myOwnFissionProbability{true};
G4bool myOwnFissionBarrier{true};
G4bool myOwnLevelDensity{true};
G4FissionParameters theParam;
G4int theSecID; // Creator model ID for the secondaries created by this model
G4bool isInitialised{false};
};
inline G4double G4CompetitiveFission::GetFissionBarrier(void) const
{
return fissionBarrier;
}
inline G4double G4CompetitiveFission::GetMaximalKineticEnergy(void) const
{
return maxKineticEnergy;
}
inline
G4double G4CompetitiveFission::Ratio(G4double A, G4double A11,
G4double B1, G4double A00) const
{
G4double res;
if (A11 >= A*0.5 && A11 <= (A00+10.0)) {
G4double x = (A11-A00)/A;
res = 1.0 - B1*x*x;
} else {
G4double x = 10.0/A;
res = 1.0 - B1*x*x - 2.0*x*B1*(A11-A00-10.0)/A;
}
return res;
}
inline
G4double G4CompetitiveFission::AsymmetricRatio(G4int A, G4double A11) const
{
return Ratio(G4double(A),A11,23.5,134.0);
}
inline
G4double G4CompetitiveFission::SymmetricRatio(G4int A, G4double A11) const
{
G4double A0 = G4double(A);
return Ratio(A0,A11,5.32,A0*0.5);
}
inline G4double G4CompetitiveFission::LocalExp(G4double x) const
{
return (std::abs(x) < 8.) ? G4Exp(-0.5*x*x) : 0.0;
}
#endif