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geant4/source/processes/electromagnetic/standard/include/G4hIonisation.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: G4hIonisation.hh,v 1.10 2000/10/30 06:56:19 urban Exp $
// GEANT4 tag $Name: geant4-03-00 $
//
//
// ------------------------------------------------------------
// GEANT 4 class header file
//
// For information related to this code contact:
// CERN, IT Division, ASD group
// History: based on object model of
// 2nd December 1995, G.Cosmo
// ---------- G4hIonisation physics process -----------
// by Laszlo Urban, 30 May 1997
// ************************************************************
// It is the first implementation of the NEW IONISATION
// PROCESS. ( delta rays + continuous energy loss)
// It calculates the ionisation for charged hadrons.
// ************************************************************
// corrected by L.Urban on 24/09/97
// corrected by L.Urban on 13/01/98
// bugs fixed by L.Urban on 02/02/99
// 10/02/00 modifications , new e.m. structure, L.Urban
// ------------------------------------------------------------
#ifndef G4hIonisation_h
#define G4hIonisation_h 1
#include "G4ios.hh"
#include "globals.hh"
#include "Randomize.hh"
#include "G4VhEnergyLoss.hh"
#include "globals.hh"
#include "G4Track.hh"
#include "G4Step.hh"
#include "G4Electron.hh"
#include "G4PhysicsLogVector.hh"
#include "G4PhysicsLinearVector.hh"
class G4hIonisation : public G4VhEnergyLoss
{
public:
G4hIonisation(const G4String& processName = "hIoni");
~G4hIonisation();
G4bool IsApplicable(const G4ParticleDefinition&);
void BuildPhysicsTable(const G4ParticleDefinition& aParticleType);
virtual void BuildLossTable(const G4ParticleDefinition& aParticleType);
void BuildLambdaTable(const G4ParticleDefinition& aParticleType);
virtual void PrintInfoDefinition();
G4double GetMeanFreePath(
const G4Track& track,
G4double previousStepSize,
G4ForceCondition* condition ) ;
G4VParticleChange *PostStepDoIt(const G4Track& track,
const G4Step& Step ) ;
protected:
virtual G4double ComputeMicroscopicCrossSection(
const G4ParticleDefinition& aParticleType,
G4double KineticEnergy,
G4double AtomicNumber);
G4PhysicsTable* theMeanFreePathTable;
private:
// hide assignment operator
G4hIonisation & operator=(const G4hIonisation &right);
G4hIonisation(const G4hIonisation&);
private:
// private data members ...............................
// G4PhysicsTable* theMeanFreePathTable;
// particles , cuts in kinetic energy ........
const G4Electron* theElectron;
const G4Proton* theProton;
const G4AntiProton* theAntiProton;
const G4double* DeltaCutInKineticEnergy ;
G4double DeltaCutInKineticEnergyNow ;
static G4double Tmincut ;
static G4double LowerBoundLambda ; // bining for lambda table
static G4double UpperBoundLambda ;
static G4int NbinLambda ;
G4double LowestKineticEnergy,HighestKineticEnergy ;
G4int TotBin ;
public:
static void SetLowerBoundLambda(G4double val) {LowerBoundLambda = val;};
static void SetUpperBoundLambda(G4double val) {UpperBoundLambda = val;};
static void SetNbinLambda(G4int n) {NbinLambda = n;};
static G4double GetLowerBoundLambda() { return LowerBoundLambda;};
static G4double GetUpperBoundLambda() { return UpperBoundLambda;};
static G4int GetNbinLambda() {return NbinLambda;};
};
#include "G4hIonisation.icc"
#endif