// // ******************************************************************** // * 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. * // ******************************************************************** // // $Id$ // // 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 explicitely 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 // #ifndef G4LivermorePhotoElectricModel_h #define G4LivermorePhotoElectricModel_h 1 #include "G4VEmModel.hh" #include "G4ElementData.hh" #include class G4ParticleChangeForGamma; class G4VAtomDeexcitation; class G4LPhysicsFreeVector; class G4LivermorePhotoElectricModel : public G4VEmModel { public: G4LivermorePhotoElectricModel(const G4String& nam = "LivermorePhElectric"); virtual ~G4LivermorePhotoElectricModel(); virtual void Initialise(const G4ParticleDefinition*, const G4DataVector&); virtual G4double ComputeCrossSectionPerAtom( const G4ParticleDefinition*, G4double kinEnergy, G4double Z, G4double A=0, G4double cut=0, G4double emax=DBL_MAX); virtual void SampleSecondaries(std::vector*, const G4MaterialCutsCouple*, const G4DynamicParticle*, G4double tmin, G4double maxEnergy); inline void SetLimitNumberOfShells(G4int); protected: G4ParticleChangeForGamma* fParticleChange; private: void ReadData(G4int Z, const char* path = 0); G4LivermorePhotoElectricModel & operator=(const G4LivermorePhotoElectricModel &right); G4LivermorePhotoElectricModel(const G4LivermorePhotoElectricModel&); G4ParticleDefinition* theGamma; G4ParticleDefinition* theElectron; G4int verboseLevel; G4int maxZ; G4int nShellLimit; G4bool fDeexcitationActive; G4bool isInitialised; G4LPhysicsFreeVector* fCrossSection[99]; G4LPhysicsFreeVector* fCrossSectionLE[99]; std::vector fParam[99]; G4int fNShells[99]; G4int fNShellsUsed[99]; G4ElementData fShellCrossSection; G4VAtomDeexcitation* fAtomDeexcitation; }; inline void G4LivermorePhotoElectricModel::SetLimitNumberOfShells(G4int n) { nShellLimit = n; } //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... #endif