// // ******************************************************************** // * License and Disclaimer * // * * // * The Geant4 software is copyright of the Copyright Holders of * // * the Geant4 Collaboration. It is provided under the terms and * // * conditions of the Geant4 Software License, included in the file * // * LICENSE and available at http://cern.ch/geant4/license . These * // * include a list of copyright holders. * // * * // * Neither the authors of this software system, nor their employing * // * institutes,nor the agencies providing financial support for this * // * work make any representation or warranty, express or implied, * // * regarding this software system or assume any liability for its * // * use. Please see the license in the file LICENSE and URL above * // * for the full disclaimer and the limitation of liability. * // * * // * This code implementation is the result of the scientific and * // * technical work of the GEANT4 collaboration. * // * By using, copying, modifying or distributing the software (or * // * any work based on the software) you agree to acknowledge its * // * use in resulting scientific publications, and indicate your * // * acceptance of all terms of the Geant4 Software license. * // ******************************************************************** // // // $Id: G4CompetitiveFission.hh 107060 2017-11-01 15:00:04Z gcosmo $ // // Hadronic Process: Nuclear De-excitations // by V. Lara (Oct 1998) #ifndef G4CompetitiveFission_h #define G4CompetitiveFission_h 1 #include "G4VEvaporationChannel.hh" #include "G4Fragment.hh" #include "G4VFissionBarrier.hh" #include "G4FissionBarrier.hh" #include "G4VEmissionProbability.hh" #include "G4FissionProbability.hh" #include "G4VLevelDensityParameter.hh" #include "G4FissionLevelDensityParameter.hh" #include "G4FissionParameters.hh" #include "Randomize.hh" #include class G4CompetitiveFission : public G4VEvaporationChannel { public: explicit G4CompetitiveFission(); virtual ~G4CompetitiveFission(); virtual G4Fragment* EmittedFragment(G4Fragment* theNucleus); virtual G4double GetEmissionProbability(G4Fragment* theNucleus); inline void SetFissionBarrier(G4VFissionBarrier * aBarrier); inline void SetEmissionStrategy(G4VEmissionProbability * aFissionProb); inline void SetLevelDensityParameter(G4VLevelDensityParameter * aLevelDensity); inline G4double GetFissionBarrier(void) const; inline G4double GetLevelDensityParameter(void) const; inline G4double GetMaximalKineticEnergy(void) const; 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); inline G4double SymmetricRatio(G4int A, G4double A11); inline G4double AsymmetricRatio(G4int A, G4double A11); 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; // Maximal Kinetic Energy that can be carried by fragment G4double MaximalKineticEnergy; // For Fission barrier G4VFissionBarrier * theFissionBarrierPtr; G4double FissionBarrier; G4bool MyOwnFissionBarrier; // For Fission probability emission G4VEmissionProbability * theFissionProbabilityPtr; G4double FissionProbability; G4bool MyOwnFissionProbability; // For Level Density calculation G4bool MyOwnLevelDensity; G4VLevelDensityParameter * theLevelDensityPtr; G4double LevelDensityParameter; G4PairingCorrection* pairingCorrection; G4FissionParameters theParam; }; inline void G4CompetitiveFission::SetFissionBarrier(G4VFissionBarrier * aBarrier) { if (MyOwnFissionBarrier) delete theFissionBarrierPtr; theFissionBarrierPtr = aBarrier; MyOwnFissionBarrier = false; } inline void G4CompetitiveFission::SetEmissionStrategy(G4VEmissionProbability * aFissionProb) { if (MyOwnFissionProbability) delete theFissionProbabilityPtr; theFissionProbabilityPtr = aFissionProb; MyOwnFissionProbability = false; } inline void G4CompetitiveFission::SetLevelDensityParameter(G4VLevelDensityParameter* aLevelDensity) { if (MyOwnLevelDensity) delete theLevelDensityPtr; theLevelDensityPtr = aLevelDensity; MyOwnLevelDensity = false; } inline G4double G4CompetitiveFission::GetFissionBarrier(void) const { return FissionBarrier; } inline G4double G4CompetitiveFission::GetLevelDensityParameter(void) const { return LevelDensityParameter; } inline G4double G4CompetitiveFission::GetMaximalKineticEnergy(void) const { return MaximalKineticEnergy; } inline G4double G4CompetitiveFission::Ratio(G4double A, G4double A11, G4double B1, G4double A00) { 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) { return Ratio(G4double(A),A11,23.5,134.0); } inline G4double G4CompetitiveFission::SymmetricRatio(G4int A, G4double A11) { G4double A0 = G4double(A); return Ratio(A0,A11,5.32,A0*0.5); } #endif