Files
geant4/source/processes/electromagnetic/lowenergy/include/G4LivermorePhotoElectricModel.hh
2025-06-26 09:17:29 +02:00

114 lines
4.4 KiB
C++

//
// ********************************************************************
// * 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 <vector>
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<G4DynamicParticle*>*,
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<G4double>* fParamHigh[ZMAXPE];
static std::vector<G4double>* fParamLow[ZMAXPE];
static G4int fNShells[ZMAXPE];
static G4int fNShellsUsed[ZMAXPE];
static G4Material* fWater;
static G4double fWaterEnergyLimit;
static G4String fDataDirectory;
std::vector<G4double> fSandiaCof;
G4double fCurrSection{0.0};
G4int verboseLevel;
G4int nShellLimit{100};
G4bool fDeexcitationActive{false};
G4bool isInitializer{false};
};
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
#endif