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geant4/source/parameterisations/channeling/include/G4CoherentPairProduction.hh
2024-12-06 11:11:40 +01:00

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C++

//
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//
// Author: Alexei Sytov
// Co-author: Gianfranco Paterno (testing)
// Using the key points of G4BaierKatkov and developments of V.V. Tikhomirov,
// partially described in L. Bandiera et al. Eur. Phys. J. C 82, 699 (2022)
#ifndef G4CoherentPairProduction_h
#define G4CoherentPairProduction_h 1
#include "G4VDiscreteProcess.hh"
#include <vector>
#include <CLHEP/Units/SystemOfUnits.h>
#include <CLHEP/Units/PhysicalConstants.h>
#include <CLHEP/Vector/TwoVector.h>
#include "G4ChannelingFastSimCrystalData.hh"
#include "G4LogicalVolume.hh"
#include "G4ParticleTable.hh"
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
class G4CoherentPairProduction : public G4VDiscreteProcess
{
public:
G4CoherentPairProduction(const G4String& processName = "cpp",
G4ProcessType aType = fElectromagnetic);
~G4CoherentPairProduction() = default;
G4VParticleChange* PostStepDoIt(const G4Track&, const G4Step&) override;
G4bool IsApplicable(const G4ParticleDefinition& aPD) override
{
return(aPD.GetParticleName() == "gamma");
}
// print documentation in html format
void ProcessDescription(std::ostream&) const override;
///special functions
void Input(const G4Material* crystal,
const G4String &lattice)
{Input(crystal,lattice,"");}
void Input(const G4Material* crystal,
const G4String &lattice,
const G4String &filePath);
// an option to use crystal data already created outside this class
void Input(const G4ChannelingFastSimCrystalData* crystalData);
///activate incoherent scattering
///(standard gamma conversion should be switched off in physics list)
void ActivateIncoherentScattering(){fIncoherentScattering = true;}
G4ChannelingFastSimCrystalData* GetCrystalData() {return fCrystalData;}
///get cuts
// minimal energy for non-zero cross section
G4double ModelMinPrimaryEnergy() { return fLowEnergyLimit;}
G4double GetHighAngleLimit() {return fHighAngleLimit;}
G4double GetPPKineticEnergyCut() {return fPPKineticEnergyCut;}
/// get the number of pairs in sampling of Baier-Katkov Integral
/// (MC integration by e+- energy and angles <=> e+- momentum)
G4int GetSamplingPairsNumber(){return fNMCPairs;}
/// get the number of particle angles 1/gamma in pair production
/// defining the width of the angular distribution of pair sampling
/// in the Baier-Katkov Integral
G4double GetChargeParticleAngleFactor(){return fChargeParticleAngleFactor;}
/// get number of trajectory steps of a single particle (e- or e+)
G4double GetNTrajectorySteps(){return fNTrajectorySteps;}
/// get effective radiation length
/// (due to coherent process of pair production)
/// simulated for the current photon
G4double GetEffectiveLrad(){return fEffectiveLrad;}
///get the name of G4Region in which the model is applicable
G4String GetG4RegionName() {return fG4RegionName;}
///set cuts
void SetLowEnergyLimit(G4double energy){fLowEnergyLimit=energy;}
void SetHighAngleLimit(G4double angle) {fHighAngleLimit=angle;}
void SetPPKineticEnergyCut(G4double kineticEnergyCut) {fPPKineticEnergyCut=kineticEnergyCut;}
/// set the number of pairs in sampling of Baier-Katkov Integral
/// (MC integration by e+- energy and angles <=> e+- momentum)
void SetSamplingPairsNumber(G4int nPairs){fNMCPairs = nPairs;}
/// set the number of particle angles 1/gamma in pair production
/// defining the width of the angular distribution of pair sampling
/// in the Baier-Katkov Integral
void SetChargeParticleAngleFactor(G4double chargeParticleAngleFactor)
{fChargeParticleAngleFactor = chargeParticleAngleFactor;}
/// set number of trajectory steps of a single particle (e- or e+)
void SetNTrajectorySteps(G4int nTrajectorySteps)
{fNTrajectorySteps = nTrajectorySteps;}
///set the name of G4Region in which the model is applicable
void SetG4RegionName(const G4String& nameG4Region){fG4RegionName=nameG4Region;}
G4double GetMeanFreePath(const G4Track& aTrack,
G4double,
G4ForceCondition* condition) override;
private:
G4int FindVectorIndex(std::vector<G4double> &myvector, G4double value);
G4ChannelingFastSimCrystalData* fCrystalData{nullptr};
//collection of etotal
std::vector <CLHEP::Hep2Vector> fullVectorEtotal;
//collection of x
std::vector <CLHEP::Hep2Vector> fullVectorX;
//collection of y
std::vector <CLHEP::Hep2Vector> fullVectorY;
//collection of tx
std::vector <CLHEP::Hep2Vector> fullVectorTX;
//collection of tx
std::vector <CLHEP::Hep2Vector> fullVectorTY;
//the vector of the discrete CDF of the production of sampling e+e- pairs
//(in reality per distance along the photon direction)
std::vector <G4double> fPairProductionCDFdz;
G4double fLowEnergyLimit = 1*CLHEP::GeV;
G4double fHighAngleLimit = 50*CLHEP::mrad;
///minimal kinetic energy of a charged particle produced
G4double fPPKineticEnergyCut = 1*CLHEP::MeV;
///Monte Carlo statistics of e+- pair sampling in Baier-Katkov for 1 photon
G4int fNMCPairs = 150;
G4double fChargeParticleAngleFactor = 4; // number of particle angles 1/gamma:
// more fChargeParticleAngleFactor => higher paramParticleAngle
///number of trajectory steps of a single particle (e- or e+)
G4int fNTrajectorySteps=250;
///effective radiation length (due to coherent process of pair production)
G4double fEffectiveLrad = 0.;
///the name of G4Region in which the model is applicable
G4String fG4RegionName = "Crystal";
///charged particle mass
const G4double fMass = CLHEP::electron_mass_c2;
///flag of simulation of incoherent scattering
G4bool fIncoherentScattering = false;
};
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
#endif