// // ******************************************************************** // * 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. * // ******************************************************************** // // // Author: Sebastien Incerti // 30 October 2008 // on base of G4LowEnergyPhotoElectric developed by A.Forti and M.G.Pia // // 15 Mar 2010 L. Pandola, removed methods to set explicitly fluorescence cuts. // Main cuts from G4ProductionCutsTable are always used // 30 May 2011 A Mantero & V Ivanchenko Migration to model design for deexcitation // 22 Oct 2012 A & V Ivanchenko Migration data structure to G4PhysicsVector // 1 June 2017 M Bandieramonte #ifndef G4LivermorePhotoElectricModel_h #define G4LivermorePhotoElectricModel_h 1 #include "G4ElementData.hh" #include "G4VEmModel.hh" #include class G4ParticleChangeForGamma; class G4VAtomDeexcitation; class G4PhysicsFreeVector; class G4LivermorePhotoElectricModel : public G4VEmModel { public: explicit G4LivermorePhotoElectricModel(const G4String& nam = "LivermorePhElectric"); ~G4LivermorePhotoElectricModel() override; void Initialise(const G4ParticleDefinition*, const G4DataVector&) override; G4double CrossSectionPerVolume(const G4Material*, const G4ParticleDefinition*, G4double energy, G4double cutEnergy = 0.0, G4double maxEnergy = DBL_MAX) override; G4double ComputeCrossSectionPerAtom(const G4ParticleDefinition*, G4double energy, G4double Z, G4double A = 0, G4double cut = 0, G4double emax = DBL_MAX) override; void SampleSecondaries(std::vector*, const G4MaterialCutsCouple*, const G4DynamicParticle*, G4double tmin, G4double maxEnergy) override; [[maybe_unused]] inline void SetLimitNumberOfShells(G4int n) { nShellLimit = n; }; G4double GetBindingEnergy(G4int Z, G4int shell); G4LivermorePhotoElectricModel& operator= (const G4LivermorePhotoElectricModel& right) = delete; G4LivermorePhotoElectricModel(const G4LivermorePhotoElectricModel&) = delete; protected: G4ParticleChangeForGamma* fParticleChange = nullptr; private: void ReadData(const G4int Z); void FindDirectoryPath(); void InitialiseOnFly(G4int Z); const G4ParticleDefinition* theGamma; const G4ParticleDefinition* theElectron; G4VAtomDeexcitation* fAtomDeexcitation{nullptr}; static constexpr G4int ZMAXPE{101}; // 101 because Z range is 1-100 static G4ElementData* fCrossSection; static G4ElementData* fCrossSectionLE; static std::vector* fParamHigh[ZMAXPE]; static std::vector* fParamLow[ZMAXPE]; static G4int fNShells[ZMAXPE]; static G4int fNShellsUsed[ZMAXPE]; static G4Material* fWater; static G4double fWaterEnergyLimit; static G4String fDataDirectory; std::vector fSandiaCof; G4double fCurrSection{0.0}; G4int verboseLevel; G4int nShellLimit{100}; G4bool fDeexcitationActive{false}; G4bool isInitializer{false}; }; //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... #endif