G4LivermorePolarizedPhotoElectricModel.hh

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//
// 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
//
 
 
#ifndef G4LivermorePolarizedPhotoElectricModel_h
#define G4LivermorePolarizedPhotoElectricModel_h 1
 
#include "G4VEmModel.hh"
#include "G4ElementData.hh"
#include <vector>
 
class G4ParticleChangeForGamma;
class G4VAtomDeexcitation;
class G4LPhysicsFreeVector;
 
class G4LivermorePolarizedPhotoElectricModel : public G4VEmModel
{
 
public:
 
  G4LivermorePolarizedPhotoElectricModel(const G4String& nam = "LivermorePolarizedPhotoElectric");
 
  virtual ~G4LivermorePolarizedPhotoElectricModel();
 
  virtual void Initialise(const G4ParticleDefinition*, const G4DataVector&);
 
  virtual G4double CrossSectionPerVolume(const G4Material*,
                                         const G4ParticleDefinition*,
                                         G4double energy,
                                         G4double cutEnergy = 0.0,
                                         G4double maxEnergy = DBL_MAX);
 
  virtual G4double ComputeCrossSectionPerAtom(
                                const G4ParticleDefinition*,
                                      G4double energy, 
                                      G4double Z, 
                                      G4double A=0, 
                                      G4double cut=0,
                                      G4double emax=DBL_MAX);
 
  virtual void SampleSecondaries(std::vector<G4DynamicParticle*>*,
                 const G4MaterialCutsCouple*,
                 const G4DynamicParticle*,
                 G4double tmin,
                 G4double maxEnergy);
 
 
  virtual void InitialiseForElement(const G4ParticleDefinition*, G4int Z);
 
  inline void SetLimitNumberOfShells(G4int);
 
protected:
 
  G4ParticleChangeForGamma* fParticleChange;
 
private:
 
  void ReadData(G4int Z, const char* path = 0);
 
  G4LivermorePolarizedPhotoElectricModel & operator=(const G4LivermorePolarizedPhotoElectricModel &right);
  G4LivermorePolarizedPhotoElectricModel(const G4LivermorePolarizedPhotoElectricModel&);
 
  G4ParticleDefinition*   theGamma;
  G4ParticleDefinition*   theElectron;
 
  G4int                   verboseLevel;
  G4int                   maxZ;
  G4int                   nShellLimit;
  G4bool                  fDeexcitationActive;
  G4bool                  isInitialised;
 
  static G4LPhysicsFreeVector*   fCrossSection[99];
  static G4LPhysicsFreeVector*   fCrossSectionLE[99];
  static std::vector<G4double>*  fParam[99];
  static G4int                   fNShells[99];
  static G4int                   fNShellsUsed[99];
  static G4ElementData*          fShellCrossSection;
  static G4Material*             fWater;
  static G4double                fWaterEnergyLimit;
 
  G4VAtomDeexcitation*    fAtomDeexcitation;
 
  G4double                fCurrSection;
  std::vector<G4double>   fSandiaCof;
};
 
inline 
void G4LivermorePolarizedPhotoElectricModel::SetLimitNumberOfShells(G4int n)
{
  nShellLimit = n;
}
 
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#endif