// // ******************************************************************** // * 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. * // ******************************************************************** // // // ------------------------------------------------------------------- // // GEANT4 Class header file // // // File name: G4eplusTo2or3GammaModel // // Author: Vladimir Ivanchenko and Omrane Kadri // // Creation date: 29.03.2018 // // // Class Description: // // Implementation of e+ annihilation into 2 or 3 gamma on fly // Annihilation at rest is sampled by G4VPositronAtRestModel // Implementation of 3-gamma annihilation is performed by // G4eplusTo3GammaOKVIModel. Cross section of both models // depend on cut parameter fDelta, which defines relative low-energy // limit on 3d gamma energy. For computation of the cross section // next to leading order radiative corrections are taken into account, // atomic effects at low-energy are not considered. // // V.N.Baier, V.S. Fadin, V.A. Khose, E.A. Kuraev, // Physics Reports 78 (1981) 293-393. // // ------------------------------------------------------------------- // #ifndef G4eplusTo2or3GammaModel_h #define G4eplusTo2or3GammaModel_h 1 #include "G4VEmModel.hh" class G4eplusTo3GammaOKVIModel; class G4ParticleChangeForGamma; class G4PhysicsVector; class G4DataVector; class G4eplusTo2or3GammaModel : public G4VEmModel { public: G4eplusTo2or3GammaModel(); ~G4eplusTo2or3GammaModel() override; void Initialise(const G4ParticleDefinition*, const G4DataVector&) override; G4double ComputeCrossSectionPerElectron(G4double kinEnergy); G4double ComputeCrossSectionPerAtom( const G4ParticleDefinition*, G4double kinEnergy, G4double Z, G4double A = 0., G4double cutEnergy = 0., G4double maxEnergy = DBL_MAX) override; G4double CrossSectionPerVolume(const G4Material*, const G4ParticleDefinition*, G4double kineticEnergy, G4double cutEnergy = 0.0, G4double maxEnergy = DBL_MAX) override; void SampleSecondaries(std::vector*, const G4MaterialCutsCouple*, const G4DynamicParticle*, G4double tmin = 0.0, G4double maxEnergy = DBL_MAX) override; void SetDelta(G4double val) { if(val > 0.0) { fDeltaMin = val; } }; // hide assignment operator G4eplusTo2or3GammaModel & operator= (const G4eplusTo2or3GammaModel &right) = delete; G4eplusTo2or3GammaModel(const G4eplusTo2or3GammaModel&) = delete; private: const G4ParticleDefinition* theGamma; G4ParticleChangeForGamma* fParticleChange; G4eplusTo3GammaOKVIModel* f3GModel; G4double fDeltaMin; // fixed minimal relative limit G4double fDelta; // running limit - function of energy G4double fGammaTh; // 3-gamma annihilation low-energy limit static G4PhysicsVector* fCrossSection; static G4PhysicsVector* f3GProbability; }; //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... #endif