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geant4/source/processes/electromagnetic/standard/include/G4IeBremsstrahlung.hh
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// This code implementation is the intellectual property of
// the GEANT4 collaboration.
//
// By copying, distributing or modifying the Program (or any work
// based on the Program) you indicate your acceptance of this statement,
// and all its terms.
//
// $Id: G4IeBremsstrahlung.hh,v 1.4 2000/04/25 14:33:00 maire Exp $
// GEANT4 tag $Name: geant4-03-00 $
//
// $Id:
// ------------------------------------------------------------
// GEANT 4 class header file
// CERN Geneva Switzerland
//
// For information related to this code contact:
// CERN, IT Division, ASD group
// History: first implementation, based on object model of
// 2nd December 1995, G.Cosmo
// ------------ G4IeBremsstrahlung physics process ------
// by Michel Maire, 24 July 1996
// ************************************************************
// 1-10-96 : new type G4OrderedTable; ComputePartialSumSigma()
// 20/03/97: new energy loss+ionisation+brems scheme, L.Urban
// ------------------------------------------------------------
// ************************************************************
// It is the first implementation of the BREMSSTRAHLUNG
// PROCESS. ( photons + continuous energy loss)
// using an INTEGRAL APPROACH instead of the differential
// one used in the standard implementation .
// ************************************************************
// by Laszlo Urban, 23 June 1998
// ------------------------------------------------------------
// 28/10/98: small changes, cleanup L.Urban
#ifndef G4IeBremsstrahlung_h
#define G4IeBremsstrahlung_h 1
#include "G4ios.hh"
#include "globals.hh"
#include "Randomize.hh"
#include "G4VIeEnergyLoss.hh"
#include "G4EnergyLossTables.hh"
#include "G4Track.hh"
#include "G4Step.hh"
#include "G4Gamma.hh"
#include "G4Electron.hh"
#include "G4Positron.hh"
#include "G4OrderedTable.hh"
#include "G4PhysicsTable.hh"
#include "G4PhysicsLogVector.hh"
class G4IeBremsstrahlung : public G4VIeEnergyLoss
{
public:
G4IeBremsstrahlung(const G4String& processName = "IeBrems");
~G4IeBremsstrahlung();
G4bool IsApplicable(const G4ParticleDefinition&);
void SetPhysicsTableBining(G4double lowE, G4double highE, G4int nBins);
void PrintInfoDefinition();
void BuildPhysicsTable(const G4ParticleDefinition& ParticleType);
void BuildLossTable(const G4ParticleDefinition& ParticleType);
void BuildLambdaTable(const G4ParticleDefinition& ParticleType);
G4double GetMeanFreePath(const G4Track& track,
G4double previousStepSize,
G4ForceCondition* condition );
G4VParticleChange *PostStepDoIt(const G4Track& track,
const G4Step& step);
G4double PostStepGetPhysicalInteractionLength( const G4Track& track,
G4double previousStepSize,
G4ForceCondition* condition);
G4double GetNlambda(
G4double KineticEnergy,G4Material* material);
protected:
inline G4double ComputeMeanFreePath(
const G4ParticleDefinition* ParticleType,
G4double KineticEnergy,
const G4Material* aMaterial);
void ComputePartialSumSigma( const G4ParticleDefinition* ParticleType,
G4double KineticEnergy,
const G4Material* aMaterial);
virtual G4double ComputeMicroscopicCrossSection(
const G4ParticleDefinition* ParticleType,
G4double KineticEnergy,
G4double AtomicNumber,
G4double GammaEnergyCut);
private:
G4IeBremsstrahlung & operator=(const G4IeBremsstrahlung &right);
G4IeBremsstrahlung(const G4IeBremsstrahlung&);
G4double ComputeBremLoss(G4double Z,G4double natom,G4double T,
G4double Cut,G4double x);
G4double ComputeXYPolynomial(G4double x,G4double y,G4int xSize,
G4int ySize,const G4double coeff[]);
G4double ComputePositronCorrFactorLoss( G4double AtomicNumber,
G4double KineticEnergy, G4double GammaEnergyCut);
G4double ComputePositronCorrFactorSigma( G4double AtomicNumber,
G4double KineticEnergy, G4double GammaEnergyCut);
G4Element* SelectRandomAtom(G4Material* aMaterial) const;
G4double ScreenFunction1(G4double ScreenVariable);
G4double ScreenFunction2(G4double ScreenVariable);
void BuildNlambdaTable(const G4ParticleDefinition& aParticleType) ;
void BuildNlambdaVector(const G4ParticleDefinition& aParticleType,
G4int materialIndex,
G4PhysicsLogVector* nlambdaVector) ;
void BuildInverseNlambdaTable(
const G4ParticleDefinition& aParticleType) ;
void InvertNlambdaVector(const G4ParticleDefinition& aParticleType,
G4int materialIndex,
G4PhysicsLogVector* nlambdaVector) ;
void BuildCoeffATable(const G4ParticleDefinition& aParticleType) ;
void BuildCoeffBTable(const G4ParticleDefinition& aParticleType) ;
void BuildCoeffCTable(const G4ParticleDefinition& aParticleType) ;
void TestOfInversion(const G4ParticleDefinition& aParticleType,
G4int printflag) ;
private:
G4PhysicsTable* theMeanFreePathTable ;
G4PhysicsTable* theNlambdaTable;
G4PhysicsTable* theInverseNlambdaTable;
G4PhysicsTable* theCoeffATable;
G4PhysicsTable* theCoeffBTable;
G4PhysicsTable* theCoeffCTable;
G4OrderedTable PartialSumSigma;
G4double LowestKineticEnergy;
G4double HighestKineticEnergy;
G4int TotBin;
G4double RTable ;
G4double CutInRange;
const G4Gamma* theGamma;
const G4Electron* theElectron;
const G4Positron* thePositron;
const G4double* GammaCutInKineticEnergy;
G4double GammaCutInKineticEnergyNow;
G4int NumberOfBuildPhysicsTableCalls ;
};
#include "G4IeBremsstrahlung.icc"
#endif