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This commit is contained in:
Gabriele Cosmo
2016-06-08 16:03:00 +02:00
parent cfcb558cfe
commit 137e303ecc
2843 changed files with 37082 additions and 38426 deletions
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source/processes/electromagnetic/standard/include/G4ComptonScattering.hh
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// and all its terms.
//
// $Id: G4ComptonScattering.hh,v 1.4 1999/12/17 16:20:49 maire Exp $
// GEANT4 tag $Name: geant4-03-00 $
// GEANT4 tag $Name: geant4-03-01 $
//
// ------------ G4ComptonScattering physics process ------
// by Michel Maire, April 1996
source/processes/electromagnetic/standard/include/G4ComptonScattering.icc
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// and all its terms.
//
// $Id: G4ComptonScattering.icc,v 1.2 1999/12/15 14:51:45 gunter Exp $
// GEANT4 tag $Name: geant4-03-00 $
// GEANT4 tag $Name: geant4-03-01 $
//
//
// ---------------------------------------------------------------
source/processes/electromagnetic/standard/include/G4GammaConversion.hh
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@@ -6,7 +6,7 @@
// and all its terms.
//
// $Id: G4GammaConversion.hh,v 1.4 1999/12/17 18:26:11 maire Exp $
// GEANT4 tag $Name: geant4-03-00 $
// GEANT4 tag $Name: geant4-03-01 $
//
// ------------ G4GammaConversion physics process ------
// by Michel Maire, 24 May 1996
source/processes/electromagnetic/standard/include/G4GammaConversion.icc
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// and all its terms.
//
// $Id: G4GammaConversion.icc,v 1.2 1999/12/15 14:51:45 gunter Exp $
// GEANT4 tag $Name: geant4-03-00 $
// GEANT4 tag $Name: geant4-03-01 $
//
//
// ---------------------------------------------------------------
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
source/processes/electromagnetic/standard/include/G4IeBremsstrahlung.icc
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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.icc,v 1.3 1999/12/15 14:51:46 gunter Exp $
// GEANT4 tag $Name: geant4-03-00 $
//
// $Id:
// ---------------------------------------------------------------
// GEANT 4 class inlined methods file
//
// 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, 27 July 1996
// ***************************************************************
// 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
inline G4double G4IeBremsstrahlung::PostStepGetPhysicalInteractionLength(
const G4Track& track,
G4double previousStepSize,
G4ForceCondition* condition
)
{
const G4double Tfac=0.95,Tfac1=1.-Tfac,eps=1.e-2 ;
G4double nl,nll,nlold,range,rangeold,rangenext,
dEdx,KineticEnergyOld,KineticEnergyNext,value;
G4bool isOut;
const G4DynamicParticle* particle = track.GetDynamicParticle();
const G4ParticleDefinition* particletype = particle->GetDefinition() ;
G4double KineticEnergy = particle->GetKineticEnergy();
G4Material* material = track.GetMaterial();
const G4MaterialTable* theMaterialTable =
G4Material::GetMaterialTable();
G4int materialindex = material->GetIndex();
nl = (*theNlambdaTable)[materialindex]->
GetValue(KineticEnergy,isOut);
range = G4EnergyLossTables::GetPreciseRangeFromEnergy(particletype,
KineticEnergy,material) ;
if ( (previousStepSize <=0.0) || (theNumberOfInteractionLengthLeft<=0.0)) {
ResetNumberOfInteractionLengthLeft();
} else {
if(previousStepSize/range < eps)
{
nll = (*theNlambdaTable)[materialindex]->
GetValue(Tfac*KineticEnergy,isOut) ;
dEdx = G4EnergyLossTables::GetPreciseDEDX(particletype,
KineticEnergy,
material) ;
nlold = nl + dEdx*previousStepSize*(nl-nll)/
(Tfac1*KineticEnergy) ;
}
else
{
rangeold = range + previousStepSize ;
KineticEnergyOld = G4EnergyLossTables::GetPreciseEnergyFromRange(
particletype,
rangeold,material);
nlold = (*theNlambdaTable)[materialindex]->
GetValue(KineticEnergyOld,isOut);
if(nlold < nl)
{
if(verboseLevel>2)
{
G4cout << "G4IeBremsstrahlung PostStepGPIL : Nlambda has been" <<
" increased at update.Nlambda old/new :" << nlold <<
" " << nl << G4endl;
G4cout << "(theNumberOfInteractionLengthLeft has been increased!)"
<< G4endl;
G4cout << " correction : Nlambda old=new ........." << G4endl;
}
nlold = nl ;
}
}
theNumberOfInteractionLengthLeft -= nlold-nl ;
if(theNumberOfInteractionLengthLeft<perMillion)
theNumberOfInteractionLengthLeft=0.;
}
*condition = NotForced;
if(nl <= theNumberOfInteractionLengthLeft)
{
value = DBL_MAX ;
}
else
{
if(theNumberOfInteractionLengthLeft/nl < eps)
{
nll = (*theNlambdaTable)[materialindex]->
GetValue(Tfac*KineticEnergy,isOut) ;
dEdx = G4EnergyLossTables::GetPreciseDEDX(particletype,
KineticEnergy,
material) ;
value = theNumberOfInteractionLengthLeft*Tfac1
*KineticEnergy/(dEdx*(nl-nll)) ;
}
else
{
KineticEnergyNext = (*theInverseNlambdaTable)[materialindex]->
GetValue(nl-theNumberOfInteractionLengthLeft,isOut);
rangenext = G4EnergyLossTables::GetPreciseRangeFromEnergy(particletype,
KineticEnergyNext,material);
value = range - rangenext ;
if(range<rangenext)
{
if(verboseLevel>2)
{
G4cout << "G4IeBremsstrahlung PostStepGPIL: Step < 0.!, Step=" <<
value << G4endl;
G4cout << "range,rangenext:" << range << " " << rangenext << G4endl ;
G4cout << "correction : rangenext=range ....." << G4endl;
}
rangenext = range ;
value = range - rangenext ;
}
}
}
return value;
}
inline G4double G4IeBremsstrahlung::ScreenFunction1(G4double ScreenVariable)
// compute the value of the screening function 3*PHI1 - PHI2
{
G4double screenVal;
if (ScreenVariable > 1.)
screenVal = 42.24 - 8.368*log(ScreenVariable+0.952);
else
screenVal = 42.392 - ScreenVariable* (7.796 - 1.961*ScreenVariable);
return screenVal;
}
inline G4double G4IeBremsstrahlung::ScreenFunction2(G4double ScreenVariable)
// compute the value of the screening function 1.5*PHI1 - 0.5*PHI2
{
G4double screenVal;
if (ScreenVariable > 1.)
screenVal = 42.24 - 8.368*log(ScreenVariable+0.952);
else
screenVal = 41.734 - ScreenVariable* (6.484 - 1.250*ScreenVariable);
return screenVal;
}
inline G4double G4IeBremsstrahlung::ComputeMeanFreePath(
const G4ParticleDefinition* ParticleType,
G4double KineticEnergy,
const G4Material* aMaterial)
{
const G4ElementVector* theElementVector = aMaterial->GetElementVector() ;
const G4double* theAtomNumDensityVector =
aMaterial->GetAtomicNumDensityVector();
G4double GammaEnergyCut = (G4Gamma::GetCutsInEnergy())[aMaterial->GetIndex()];
G4double SIGMA = 0 ;
for ( G4int i=0 ; i < aMaterial->GetNumberOfElements() ; i++ )
{
SIGMA += theAtomNumDensityVector[i] *
ComputeMicroscopicCrossSection( ParticleType, KineticEnergy,
(*theElementVector)(i)->GetZ(),
GammaEnergyCut );
}
return SIGMA<=0.0 ? DBL_MAX : 1./SIGMA ;
}
inline G4bool G4IeBremsstrahlung::IsApplicable(
const G4ParticleDefinition& particle)
{
return( (&particle == (const G4ParticleDefinition *)theElectron)
||(&particle == (const G4ParticleDefinition *)thePositron)
) ;
}
inline G4double G4IeBremsstrahlung::GetNlambda(
G4double KineticEnergy,
G4Material* material)
{
G4bool isOut;
const G4MaterialTable* theMaterialTable =
G4Material::GetMaterialTable() ;
G4double lambda = (*theNlambdaTable)
[material->GetIndex()]->
GetValue(KineticEnergy,isOut);
return lambda;
}
source/processes/electromagnetic/standard/include/G4IeIonisation.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: G4IeIonisation.hh,v 1.4 2000/04/25 14:33:00 maire Exp $
// GEANT4 tag $Name: geant4-03-00 $
//
// $Id:
// ------------------------------------------------------------
// 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
// ---------- G4IeIonisation physics process -----------
// by Laszlo Urban, 23 June 1998
// ************************************************************
// It is the first implementation of the IONISATION
// PROCESS. ( delta rays + continuous energy loss)
// using an INTEGRAL APPROACH instead of the differential
// one used in the standard implementation .
// ************************************************************
// 27/10/98 : minor changes+cleanup , L.Urban
// ------------------------------------------------------------
#ifndef G4IeIonisation_h
#define G4IeIonisation_h 1
#include "G4ios.hh"
#include "g4std/iomanip"
#include "globals.hh"
#include "Randomize.hh"
#include "G4VIeEnergyLoss.hh"
#include "G4EnergyLossTables.hh"
#include "globals.hh"
#include "G4Track.hh"
#include "G4Step.hh"
#include "G4Electron.hh"
#include "G4Positron.hh"
#include "G4Gamma.hh"
#include "G4PhysicsLogVector.hh"
#include "G4PhysicsLinearVector.hh"
class G4IeIonisation : public G4VIeEnergyLoss
{
public:
G4IeIonisation(const G4String& processName = "IeIoni");
~G4IeIonisation();
G4bool IsApplicable(const G4ParticleDefinition&);
void SetPhysicsTableBining(G4double lowE, G4double highE, G4int nBins);
void BuildPhysicsTable(const G4ParticleDefinition& aParticleType);
void BuildLossTable(const G4ParticleDefinition& aParticleType);
void BuildLambdaTable(const G4ParticleDefinition& aParticleType);
void PrintInfoDefinition();
G4double PostStepGetPhysicalInteractionLength( const G4Track& track,
G4double previousStepSize,
G4ForceCondition* condition);
G4VParticleChange *PostStepDoIt(const G4Track& track,
const G4Step& Step ) ;
G4double GetNlambda(
G4double KineticEnergy,G4Material* material);
protected:
virtual G4double ComputeMicroscopicCrossSection(
const G4ParticleDefinition& aParticleType,
G4double KineticEnergy,
G4double AtomicNumber);
private:
// hide assignment operator
G4IeIonisation & operator=(const G4IeIonisation &right);
G4IeIonisation(const G4IeIonisation&);
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:
// private data members ...............................
G4PhysicsTable* theMeanFreePathTable;
G4PhysicsTable* theNlambdaTable;
G4PhysicsTable* theInverseNlambdaTable;
G4PhysicsTable* theCoeffATable;
G4PhysicsTable* theCoeffBTable;
G4PhysicsTable* theCoeffCTable;
G4double LowestKineticEnergy;
G4double HighestKineticEnergy;
G4int TotBin;
G4double RTable ;
// cut in range
G4double CutInRange ;
// particles , cuts in kinetic energy ........
const G4Electron* theElectron;
const G4Positron* thePositron;
const G4double* ParticleCutInKineticEnergy;
const G4double* DeltaCutInKineticEnergy ;
G4double ParticleCutInKineticEnergyNow ;
G4double DeltaKineticEnergyCutNow ;
G4int NumberOfBuildPhysicsTableCalls ;
};
#include "G4IeIonisation.icc"
#endif
source/processes/electromagnetic/standard/include/G4IeIonisation.icc
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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: G4IeIonisation.icc,v 1.3 1999/12/15 14:51:46 gunter Exp $
// GEANT4 tag $Name: geant4-03-00 $
//
// $Id:
// ---------------------------------------------------------------
// GEANT 4 class inlined methods file
//
// For information related to this code contact:
// CERN, IT Division, ASD group
// ------------ G4IeIonisation physics process ------------
// by Laszlo Urban, 23 June 1998
// ************************************************************
// It is the first implementation of the IONISATION
// PROCESS. ( delta rays + continuous energy loss)
// using an INTEGRAL APPROACH instead of the differential
// one used in the standard implementation .
// ************************************************************
// 27/10/98: minor changes , cleanup , L.Urban
// ------------------------------------------------------------
inline G4double G4IeIonisation::PostStepGetPhysicalInteractionLength(
const G4Track& track,
G4double previousStepSize,
G4ForceCondition* condition)
{
const G4double eps=1.e-2,Tfac=0.95,Tfac1=1.-Tfac ;
G4double nl,nll,nlold,range,rangeold,rangenext,
dEdx,KineticEnergyOld,KineticEnergyNext,value;
G4bool isOut;
const G4DynamicParticle* particle = track.GetDynamicParticle();
const G4ParticleDefinition* particletype = particle->GetDefinition() ;
G4double KineticEnergy = particle->GetKineticEnergy();
G4Material* material = track.GetMaterial();
const G4MaterialTable* theMaterialTable =
G4Material::GetMaterialTable();
G4int materialindex = material->GetIndex();
nl = (*theNlambdaTable)[materialindex]->
GetValue(KineticEnergy,isOut);
range = G4EnergyLossTables::GetPreciseRangeFromEnergy(particletype,
KineticEnergy,material) ;
if ( (previousStepSize <=0.0) || (theNumberOfInteractionLengthLeft<=0.0)) {
// beggining of tracking (or just after DoIt of this process)
ResetNumberOfInteractionLengthLeft();
} else {
if(previousStepSize/range < eps)
{
nll = (*theNlambdaTable)[materialindex]->
GetValue(Tfac*KineticEnergy,isOut) ;
dEdx = G4EnergyLossTables::GetPreciseDEDX(particletype,
KineticEnergy,
material) ;
nlold = nl + dEdx*previousStepSize*(nl-nll)/
(Tfac1*KineticEnergy) ;
}
else
{
rangeold = range + previousStepSize ;
KineticEnergyOld = G4EnergyLossTables::GetPreciseEnergyFromRange(
particletype,
rangeold,material);
nlold = (*theNlambdaTable)[materialindex]->
GetValue(KineticEnergyOld,isOut);
if(nlold < nl)
{
if(verboseLevel>2)
{
G4cout << "G4IeIonisation PostStepGPIL : Nlambda has been" <<
" increased at update.Nlambda old/new :" << nlold <<
" " << nl << G4endl;
G4cout << "(theNumberOfInteractionLengthLeft has been increased!)"
<< G4endl;
G4cout << " correction : Nlambda old=new ........." << G4endl;
}
nlold = nl ;
}
}
theNumberOfInteractionLengthLeft -= nlold-nl ;
if(theNumberOfInteractionLengthLeft<perMillion)
theNumberOfInteractionLengthLeft=0.;
}
// condition is set to "Not Forced"
*condition = NotForced;
if(nl <= theNumberOfInteractionLengthLeft)
{
value = DBL_MAX ;
}
else
{
if(theNumberOfInteractionLengthLeft/nl < eps)
{
nll = (*theNlambdaTable)[materialindex]->
GetValue(Tfac*KineticEnergy,isOut) ;
dEdx = G4EnergyLossTables::GetPreciseDEDX(particletype,
KineticEnergy,
material) ;
value = theNumberOfInteractionLengthLeft*Tfac1*
KineticEnergy/(dEdx*(nl-nll)) ;
}
else
{
KineticEnergyNext = (*theInverseNlambdaTable)[materialindex]->
GetValue(nl-theNumberOfInteractionLengthLeft,isOut);
rangenext = G4EnergyLossTables::GetPreciseRangeFromEnergy(particletype,
KineticEnergyNext,material);
value = range - rangenext ;
if(range<rangenext)
{
if(verboseLevel>2)
{
G4cout << "G4IeIonisation PostStepGPIL: Step < 0.!, Step="
<< value << G4endl;
G4cout << "range,rangenext:" << range << " " << rangenext << G4endl ;
G4cout << "correction : rangenext=range ....." << G4endl;
}
rangenext = range ;
value = range - rangenext ;
}
}
}
return value;
}
inline G4bool G4IeIonisation::IsApplicable(
const G4ParticleDefinition& particle)
{
return( (&particle == (const G4ParticleDefinition *)theElectron)
||(&particle == (const G4ParticleDefinition *)thePositron)
) ;
}
inline G4double G4IeIonisation::GetNlambda(
G4double KineticEnergy,
G4Material* material)
{
G4bool isOut;
const G4MaterialTable* theMaterialTable =
G4Material::GetMaterialTable() ;
G4double lambda = (*theNlambdaTable)
[material->GetIndex()]->
GetValue(KineticEnergy,isOut);
return lambda;
}
source/processes/electromagnetic/standard/include/G4IeplusAnnihilation.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: G4IeplusAnnihilation.hh,v 1.2 1999/12/15 14:51:46 gunter 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
// ------------ G4IeplusAnnihilation process ------
// by Michel Maire, 7 july 1996
// ************************************************************
// ************************************************************
// It is the first implementation of the
// eplusANNIHILATION PROCESS
// using an INTEGRAL APPROACH instead of the differential
// one used in the standard implementation .
// ************************************************************
// by Laszlo Urban, 23 June 1998
// ----------------------------------------------------------
// 28/10/98: cleanup L. Urban
#ifndef G4IeplusAnnihilation_h
#define G4IeplusAnnihilation_h 1
#include "G4ios.hh"
#include "globals.hh"
#include "Randomize.hh"
#include "G4IVRestDiscreteProcess.hh"
#include "G4EnergyLossTables.hh"
#include "G4PhysicsTable.hh"
#include "G4PhysicsLogVector.hh"
#include "G4PhysicsLinearVector.hh"
#include "G4ElementTable.hh"
#include "G4Gamma.hh"
#include "G4Positron.hh"
#include "G4Step.hh"
class G4IeplusAnnihilation : public G4IVRestDiscreteProcess
{
public:
G4IeplusAnnihilation(const G4String& processName ="Iannihil");
~G4IeplusAnnihilation();
G4bool IsApplicable(const G4ParticleDefinition&);
void SetPhysicsTableBining(G4double lowE, G4double highE, G4int nBins);
void PrintInfoDefinition();
void BuildPhysicsTable(const G4ParticleDefinition& PositronType);
G4double PostStepGetPhysicalInteractionLength(const G4Track& track,
G4double previousStepSize,
G4ForceCondition* condition) ;
G4double GetMicroscopicCrossSection(G4DynamicParticle* aDynamicPositron,
G4Element* anElement);
G4VParticleChange* PostStepDoIt(const G4Track& aTrack,
const G4Step& aStep);
G4double GetMeanLifeTime(const G4Track& aTrack,
G4ForceCondition* condition);
G4VParticleChange* AtRestDoIt(const G4Track& aTrack,
const G4Step& aStep);
protected:
virtual G4double ComputeMicroscopicCrossSection(G4double PositKinEnergy,
G4double AtomicNumber);
virtual G4double ComputeMeanFreePath(G4double PositKinEnergy,
G4Material* aMaterial);
private:
// hide assignment operator as private
G4IeplusAnnihilation& operator=(const G4IeplusAnnihilation &right);
G4IeplusAnnihilation(const G4IeplusAnnihilation& );
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* theCrossSectionTable; // table for crossection
G4PhysicsTable* theMeanFreePathTable ;
G4PhysicsTable* theNlambdaTable;
G4PhysicsTable* theInverseNlambdaTable;
G4PhysicsTable* theCoeffATable;
G4PhysicsTable* theCoeffBTable;
G4PhysicsTable* theCoeffCTable;
G4double LowestEnergyLimit ; // low energy limit of the crossection formula
G4double HighestEnergyLimit ; // high energy limit of the crossection formula
G4int NumbBinTable ; // number of bins in the crossection table
G4int NumberOfBuildPhysicsTableCalls ;
G4double LowestKineticEnergy ;
G4double HighestKineticEnergy;
G4int TotBin ;
G4double RTable ;
};
#include "G4IeplusAnnihilation.icc"
#endif
source/processes/electromagnetic/standard/include/G4IeplusAnnihilation.icc
-197
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@@ -1,197 +0,0 @@
// 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: G4IeplusAnnihilation.icc,v 1.2 1999/12/15 14:51:46 gunter Exp $
// GEANT4 tag $Name: geant4-03-00 $
//
// $Id:
// ---------------------------------------------------------------
// GEANT 4 class inlined methods file
//
// For information related to this code contact:
// CERN, CN Division, ASD group
// History: first implementation, based on object model of
// 2nd December 1995, G.Cosmo
// ------------ G4IeplusAnnihilation process ---------
// by Michel Maire, 7 July 1996
// ***************************************************************
// ************************************************************
// It is the first implementation of the
// eplusANNIHILATION PROCESS
// using an INTEGRAL APPROACH instead of the differential
// one used in the standard implementation .
// ************************************************************
// by Laszlo Urban, 23 June 1998
// ---------------------------------------------------------
// 28/10/98: some cleanup , L.Urban
inline G4bool G4IeplusAnnihilation::IsApplicable(const G4ParticleDefinition& particle)
{
return ( &particle == G4Positron::Positron() );
}
inline G4double G4IeplusAnnihilation::GetMicroscopicCrossSection(
G4DynamicParticle* aDynamicPositron,
G4Element* anElement)
// gives the microscopic total cross section in GEANT4 internal units
{
G4double crossSection;
G4double PositronEnergy = aDynamicPositron->GetKineticEnergy();
G4bool isOutRange ;
if (PositronEnergy > HighestEnergyLimit)
crossSection = 0. ;
else {
if (PositronEnergy < LowestEnergyLimit) PositronEnergy = 1.01*LowestEnergyLimit;
crossSection = (*theCrossSectionTable)(anElement->GetIndex())->
GetValue( PositronEnergy, isOutRange );
}
return crossSection;
}
inline G4double G4IeplusAnnihilation::PostStepGetPhysicalInteractionLength(
const G4Track& track,
G4double previousStepSize,
G4ForceCondition* condition
)
{// get particle,particle type,kin.energy,material,mat.index
const G4double Tfac=0.95,Tfac1=1.-Tfac,eps=1.e-2 ;
G4double nl,nll,nlold,range,rangeold,rangenext,
dEdx,KineticEnergyOld,KineticEnergyNext,value;
G4bool isOut;
const G4DynamicParticle* particle = track.GetDynamicParticle();
const G4ParticleDefinition* particletype = particle->GetDefinition() ;
G4double KineticEnergy = particle->GetKineticEnergy();
G4Material* material = track.GetMaterial();
const G4MaterialTable* theMaterialTable =
G4Material::GetMaterialTable();
G4int materialindex = material->GetIndex();
nl = (*theNlambdaTable)[materialindex]->
GetValue(KineticEnergy,isOut);
range = G4EnergyLossTables::GetPreciseRangeFromEnergy(particletype,
KineticEnergy,material) ;
if ( (previousStepSize <=0.0) || (theNumberOfInteractionLengthLeft<=0.0)) {
ResetNumberOfInteractionLengthLeft();
} else {
if(previousStepSize/range < eps)
{
nll = (*theNlambdaTable)[materialindex]->
GetValue(Tfac*KineticEnergy,isOut) ;
dEdx = G4EnergyLossTables::GetPreciseDEDX(particletype,
KineticEnergy,
material) ;
nlold = nl + dEdx*previousStepSize*(nl-nll)/
(Tfac1*KineticEnergy) ;
}
else
{
rangeold = range + previousStepSize ;
KineticEnergyOld = G4EnergyLossTables::GetPreciseEnergyFromRange(
particletype,
rangeold,material);
nlold = (*theNlambdaTable)[materialindex]->
GetValue(KineticEnergyOld,isOut);
if(nlold < nl)
{
if(verboseLevel>2)
{
G4cout << "G4IeplusAnnihilation PostStepGPIL : Nlambda has been" <<
" increased at update.Nlambda old/new :" << nlold <<
" " << nl << G4endl;
G4cout << "(theNumberOfInteractionLengthLeft has been increased!)" << G4endl;
G4cout << " correction : Nlambda old=new ........." << G4endl;
}
nlold = nl ;
}
}
theNumberOfInteractionLengthLeft -= nlold-nl ;
if(theNumberOfInteractionLengthLeft<perMillion)
theNumberOfInteractionLengthLeft=0.;
}
// condition is set to "Not Forced"
*condition = NotForced;
if(nl <= theNumberOfInteractionLengthLeft)
{
value = DBL_MAX ;
}
else
{
if(theNumberOfInteractionLengthLeft/nl < eps)
{
nll = (*theNlambdaTable)[materialindex]->
GetValue(Tfac*KineticEnergy,isOut) ;
dEdx = G4EnergyLossTables::GetPreciseDEDX(particletype,
KineticEnergy,
material) ;
value = theNumberOfInteractionLengthLeft*Tfac1*KineticEnergy/(dEdx*(nl-nll)) ;
}
else
{
KineticEnergyNext = (*theInverseNlambdaTable)[materialindex]->
GetValue(nl-theNumberOfInteractionLengthLeft,isOut);
rangenext = G4EnergyLossTables::GetPreciseRangeFromEnergy(particletype,
KineticEnergyNext,material);
value = range - rangenext ;
if(range<rangenext)
{
if(verboseLevel>2)
{
G4cout << "G4IeplusAnnihilation PostStepGPIL: Step < 0.!, Step=" <<
value << G4endl;
G4cout << "range,rangenext:" << range << " " << rangenext << G4endl ;
G4cout << "correction : rangenext=range ....." << G4endl;
}
rangenext = range ;
value = range - rangenext ;
}
}
}
return value;
}
inline G4double G4IeplusAnnihilation::ComputeMeanFreePath(G4double PositKinEnergy,
G4Material* aMaterial)
// returns the positron mean free path in GEANT4 internal units
{
const G4ElementVector* theElementVector = aMaterial->GetElementVector() ;
const G4double* theAtomNumDensityVector = aMaterial->GetAtomicNumDensityVector();
G4double SIGMA = 0 ;
for ( G4int i=0 ; i < aMaterial->GetNumberOfElements() ; i++ )
{
SIGMA += theAtomNumDensityVector[i] *
ComputeMicroscopicCrossSection( PositKinEnergy,
(*theElementVector)(i)->GetZ() );
}
return SIGMA<=0.0 ? DBL_MAX : 1./SIGMA ;
}
inline G4double G4IeplusAnnihilation::GetMeanLifeTime(const G4Track&,
G4ForceCondition*)
// returns the annihilation mean life time in GEANT4 internal units
{
return 0.0;
}
source/processes/electromagnetic/standard/include/G4IhIonisation.hh
-144
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@@ -1,144 +0,0 @@
// 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: G4IhIonisation.hh,v 1.4 2000/04/25 14:33:01 maire 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
// ---------- G4IhIonisation 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
// 28/10/98: some cleanup , L.Urban
// ------------------------------------------------------------
#ifndef G4IhIonisation_h
#define G4IhIonisation_h 1
#include "G4ios.hh"
#include "globals.hh"
#include "Randomize.hh"
#include "G4VIhEnergyLoss.hh"
#include "G4EnergyLossTables.hh"
#include "globals.hh"
#include "G4Track.hh"
#include "G4Step.hh"
#include "G4Electron.hh"
#include "G4Proton.hh"
#include "G4AntiProton.hh"
#include "G4PhysicsLogVector.hh"
#include "G4PhysicsLinearVector.hh"
class G4IhIonisation : public G4VIhEnergyLoss
{
public:
G4IhIonisation(const G4String& processName = "IhIoni");
~G4IhIonisation();
G4bool IsApplicable(const G4ParticleDefinition&);
void SetPhysicsTableBining(G4double lowE, G4double highE, G4int nBins);
void BuildPhysicsTable(const G4ParticleDefinition& aParticleType);
void BuildLossTable(const G4ParticleDefinition& aParticleType);
void BuildLambdaTable(const G4ParticleDefinition& aParticleType);
void PrintInfoDefinition();
G4double PostStepGetPhysicalInteractionLength(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);
private:
// hide assignment operator
G4IhIonisation & operator=(const G4IhIonisation &right);
G4IhIonisation(const G4IhIonisation&);
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:
// private data members ...............................
G4PhysicsTable* theMeanFreePathTable;
G4PhysicsTable* theNlambdaTable;
G4PhysicsTable* theInverseNlambdaTable;
G4PhysicsTable* theCoeffATable;
G4PhysicsTable* theCoeffBTable;
G4PhysicsTable* theCoeffCTable;
const G4Electron* theElectron;
const G4Proton* theProton;
const G4AntiProton* theAntiProton;
const G4double* ParticleCutInKineticEnergy;
const G4double* DeltaCutInKineticEnergy ;
G4double ParticleCutInKineticEnergyNow ;
G4double DeltaCutInKineticEnergyNow ;
G4int NumberOfBuildPhysicsTableCalls ;
};
#include "G4IhIonisation.icc"
#endif
source/processes/electromagnetic/standard/include/G4IhIonisation.icc
-145
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@@ -1,145 +0,0 @@
// 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: G4IhIonisation.icc,v 1.2 1999/12/15 14:51:47 gunter Exp $
// GEANT4 tag $Name: geant4-03-00 $
//
//
// ---------------------------------------------------------------
// GEANT 4 class inlined methods file
//
// For information related to this code contact:
// CERN, IT Division, ASD group
// ------------ G4IhIonisation physics process ------------
// by Laszlo Urban, 30 May 1997
// ***************************************************************
// It is the first implementation of the NEW IONISATION PROCESS.
// It calculates the ionisation of charged hadrons.
// ***************************************************************
// 24/09/97: corrected by L.Urban
// 20/11/97: correction on MeanFreePath for KineticEnergy > HighestLimit
// 29/10/98: some cleanup + small changes , L.Urban
// ---------------------------------------------------------------
inline G4double G4IhIonisation::PostStepGetPhysicalInteractionLength(
const G4Track& track,
G4double previousStepSize,
G4ForceCondition* condition)
{// get particle,particle type,kin.energy,material,mat.index
const G4double Tfac=0.95,Tfac1=1.-Tfac,eps=1.e-2 ;
G4double nl,nll,nlold,range,rangeold,rangenext,
dEdx,KineticEnergyOld,KineticEnergyNext,value;
G4bool isOut;
const G4DynamicParticle* particle = track.GetDynamicParticle();
const G4ParticleDefinition* particletype = particle->GetDefinition() ;
G4double KineticEnergy = particle->GetKineticEnergy();
G4Material* material = track.GetMaterial();
const G4MaterialTable* theMaterialTable =
G4Material::GetMaterialTable();
G4int materialindex = material->GetIndex();
nl = (*theNlambdaTable)[materialindex]->
GetValue(KineticEnergy,isOut);
range = G4EnergyLossTables::GetPreciseRangeFromEnergy(particletype,
KineticEnergy,material) ;
if ( (previousStepSize <=0.0) || (theNumberOfInteractionLengthLeft<=0.0)) {
ResetNumberOfInteractionLengthLeft();
} else {
if(previousStepSize/range < eps)
{
nll = (*theNlambdaTable)[materialindex]->
GetValue(Tfac*KineticEnergy,isOut) ;
dEdx = G4EnergyLossTables::GetPreciseDEDX(particletype,
KineticEnergy,
material) ;
nlold = nl + dEdx*previousStepSize*(nl-nll)/
(Tfac1*KineticEnergy) ;
}
else
{
rangeold = range + previousStepSize ;
KineticEnergyOld = G4EnergyLossTables::GetPreciseEnergyFromRange(
particletype,
rangeold,material);
nlold = (*theNlambdaTable)[materialindex]->
GetValue(KineticEnergyOld,isOut);
if(nlold < nl)
{
if(verboseLevel>2)
{
G4cout << "G4IhIonisation PostStepGPIL : Nlambda has been" <<
" increased at update.Nlambda old/new :" << nlold <<
" " << nl << G4endl;
G4cout << "(theNumberOfInteractionLengthLeft has been increased!)"
<< G4endl;
G4cout << " correction : Nlambda old=new ........." << G4endl;
}
nlold = nl ;
}
}
theNumberOfInteractionLengthLeft -= nlold-nl ;
if(theNumberOfInteractionLengthLeft<perMillion)
theNumberOfInteractionLengthLeft=0.;
}
// condition is set to "Not Forced"
*condition = NotForced;
if(nl <= theNumberOfInteractionLengthLeft)
{
value = DBL_MAX ;
}
else
{
if(theNumberOfInteractionLengthLeft/nl < eps)
{
nll = (*theNlambdaTable)[materialindex]->
GetValue(Tfac*KineticEnergy,isOut) ;
dEdx = G4EnergyLossTables::GetPreciseDEDX(particletype,
KineticEnergy,
material) ;
value = theNumberOfInteractionLengthLeft*Tfac1*KineticEnergy/
(dEdx*(nl-nll));
}
else
{
KineticEnergyNext = (*theInverseNlambdaTable)[materialindex]->
GetValue(nl-theNumberOfInteractionLengthLeft,isOut);
rangenext = G4EnergyLossTables::GetPreciseRangeFromEnergy(particletype,
KineticEnergyNext,material);
value = range - rangenext ;
if(range<rangenext)
{
if(verboseLevel>2)
{
G4cout << "G4IhIonisation PostStepGPIL: Step < 0.!, Step="
<< value << G4endl;
G4cout << "range,rangenext:" << range << " " << rangenext << G4endl ;
G4cout << "correction : rangenext=range ....." << G4endl;
}
rangenext = range ;
value = range - rangenext ;
}
}
}
return value;
}
inline G4bool G4IhIonisation::IsApplicable(
const G4ParticleDefinition& particle)
{
return(particle.GetPDGCharge() != 0.);
}
source/processes/electromagnetic/standard/include/G4PAIonisation.hh
+1 -1
View File
@@ -6,7 +6,7 @@
// and all its terms.
//
// $Id: G4PAIonisation.hh,v 1.7 2000/09/22 14:44:07 grichine Exp $
// GEANT4 tag $Name: geant4-03-00 $
// GEANT4 tag $Name: geant4-03-01 $
//
//
// ------------------------------------------------------------
source/processes/electromagnetic/standard/include/G4PAIonisation.icc
+9 -3
View File
@@ -86,7 +86,7 @@ GetMeanFreePath( const G4Track& trackData,
// G4cout<<"G4PAIonisation::GetMeanFreePath is called"<<G4endl ;
G4int iTkin, iPlace ;
G4double charge, charge2, massRatio, kinE, scaledE, meanFreePath ;
G4double charge, charge2, mass, massRatio, kinE, gamma, scaledE, meanFreePath ;
G4double E1, E2, W, W1, W2, primaryIon ;
*condition = NotForced ;
@@ -98,9 +98,14 @@ GetMeanFreePath( const G4Track& trackData,
{
const G4DynamicParticle* aParticle = trackData.GetDynamicParticle() ;
kinE = aParticle->GetKineticEnergy() ;
mass = aParticle->GetDefinition()->GetPDGMass() ;
gamma = 1.0 + kinE/mass ;
if(gamma < 1.2) return meanFreePath = DBL_MAX ;
charge = aParticle->GetDefinition()->GetPDGCharge() ;
charge2 = charge*charge ;
massRatio = proton_mass_c2/aParticle->GetDefinition()->GetPDGMass() ;
massRatio = proton_mass_c2/mass ;
scaledE = kinE*massRatio ;
for(iTkin=0;iTkin<G4PAIonisation::GetBinNumber();iTkin++)
@@ -235,7 +240,8 @@ GetdEdx( G4double scaledTkin, G4double charge2 )
inline G4bool G4PAIonisation::IsApplicable(
const G4ParticleDefinition& particle)
{
return(particle.GetPDGCharge() != 0.);
return( particle.GetPDGCharge() != 0. &&
particle.GetPDGMass() > 0. );
}
//////////////////////////////////////////////////////////////////////////
source/processes/electromagnetic/standard/include/G4PAIxSection.hh
+1 -1
View File
@@ -6,7 +6,7 @@
// and all its terms.
//
// $Id: G4PAIxSection.hh,v 1.4 1999/12/15 14:51:47 gunter Exp $
// GEANT4 tag $Name: geant4-03-00 $
// GEANT4 tag $Name: geant4-03-01 $
//
//
// G4PAIxSection.hh -- header file
source/processes/electromagnetic/standard/include/G4PhotoElectricEffect.hh
+5 -5
View File
@@ -5,11 +5,10 @@
// based on the Program) you indicate your acceptance of this statement,
// and all its terms.
//
// $Id: G4PhotoElectricEffect.hh,v 1.5 1999/12/17 18:26:12 maire Exp $
// GEANT4 tag $Name: geant4-03-00 $
// $Id: G4PhotoElectricEffect.hh,v 1.6 2001/02/22 16:05:42 maire Exp $
// GEANT4 tag $Name: geant4-03-01 $
//
// ------------ G4PhotoElectricEffect physics process ------
// by Michel Maire, April 1996
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
//
// 12-06-96, Added SelectRandomAtom() method and new data member
// for cumulative total cross section, by M.Maire
@@ -21,7 +20,8 @@
// 13-08-98, new methods SetBining() PrintInfo()
// 17-11-98, use table of atomic shells in PostStepDoIt, mma
// 06-01-99, Sandia crossSection below 50 keV, V.Grichine mma
// ------------------------------------------------------------
//
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
// class description
//
source/processes/electromagnetic/standard/include/G4PhotoElectricEffect.icc
+5 -14
View File
@@ -5,20 +5,11 @@
// based on the Program) you indicate your acceptance of this statement,
// and all its terms.
//
// $Id: G4PhotoElectricEffect.icc,v 1.3 1999/12/15 14:51:48 gunter Exp $
// GEANT4 tag $Name: geant4-03-00 $
// $Id: G4PhotoElectricEffect.icc,v 1.4 2001/02/22 16:05:43 maire Exp $
// GEANT4 tag $Name: geant4-03-01 $
//
//
// ---------------------------------------------------------------
// GEANT 4 class inlined methods file
//
// For information related to this code contact:
// CERN, CN Division, ASD group
// History: first implementation, based on object model of
// 2nd December 1995, G.Cosmo
// ------------ G4PhotoElectricEffect physics process ---------
// by Michel Maire, April 1996
// ***************************************************************
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
// 12-06-96, update by M.Maire
// 17-09-96, PartialSumSigma(i)
// split ComputeBinbingEnergy(), M.Maire
@@ -27,8 +18,8 @@
// 20-11-97, change for lowest energy limit default action
// 17-11-98, use table of atomic shells in PostStepDoIt, mma
// 06-01-99, use Sandia crossSection, V.Grichine mma
// ---------------------------------------------------------------
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
inline G4bool G4PhotoElectricEffect::IsApplicable(const G4ParticleDefinition& particle)
source/processes/electromagnetic/standard/include/G4PolarizedComptonScattering.hh
+1 -1
View File
@@ -6,7 +6,7 @@
// and all its terms.
//
// $Id: G4PolarizedComptonScattering.hh,v 1.4 2000/11/17 15:03:16 maire Exp $
// GEANT4 tag $Name: geant4-03-00 $
// GEANT4 tag $Name: geant4-03-01 $
//
// --------- G4PolarizedComptonScattering physics process -----
// by Vicente Lara, March 1998
source/processes/electromagnetic/standard/include/G4SynchrotronRadiation.hh
+2 -3
View File
@@ -5,8 +5,8 @@
// based on the Program) you indicate your acceptance of this statement,
// and all its terms.
//
// $Id: G4SynchrotronRadiation.hh,v 1.3 2000/11/01 15:30:46 gcosmo Exp $
// GEANT4 tag $Name: geant4-03-00 $
// $Id: G4SynchrotronRadiation.hh,v 1.4 2001/02/05 17:53:51 gcosmo Exp $
// GEANT4 tag $Name: geant4-03-01 $
//
// ------------------------------------------------------------
// GEANT 4 class header file
@@ -43,7 +43,6 @@
#include "G4Positron.hh"
#include "G4OrderedTable.hh"
#include "G4PhysicsTable.hh"
#include "G4PhysicsLogVector.hh"
source/processes/electromagnetic/standard/include/G4VIeEnergyLoss.hh
-243
View File
@@ -1,243 +0,0 @@
// 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: G4VIeEnergyLoss.hh,v 1.3 2000/08/15 09:42:14 urban Exp $
// GEANT4 tag $Name: geant4-03-00 $
//
// $Id:
// ------------------------------------------------------------
// GEANT 4 class header file
//
// 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
// ---------- G4VIeEnergyLoss physics process -----------
// by Laszlo Urban, 20 March 1997
// ************************************************************
// It is the first implementation of the new unified Energy Loss process.
// It calculates the continuous energy loss for e+/e-.
// Processes giving contribution to the continuous loss :
// ionisation (= cont.ion.loss + delta ray production)
// bremsstrahlung (= cont.loss due to sooft brems+discrete bremsstrahlung)
// can be added more easily ..........
// This class creates static dE/dx and range tables for e+ and e-,
// which tables can be used by other processes.
// ------------------------------------------------------------
//
// 27.05.98 OldGetRange removed + other corrs , L.Urban
// 26.10.98 revision , L.Urban
// ------------------------------------------------------------
#ifndef G4VIeEnergyLoss_h
#define G4VIeEnergyLoss_h 1
#include "G4ios.hh"
#include "globals.hh"
#include "Randomize.hh"
#include "G4IVContinuousDiscreteProcess.hh"
#include "G4Material.hh"
#include "G4Element.hh"
#include "G4VParticleChange.hh"
#include "globals.hh"
#include "G4Track.hh"
#include "G4Step.hh"
#include "G4Electron.hh"
#include "G4Positron.hh"
#include "G4PhysicsLogVector.hh"
#include "G4PhysicsLinearVector.hh"
class G4EnergyLossMessenger;
class G4VIeEnergyLoss : public G4IVContinuousDiscreteProcess
{
public:
G4VIeEnergyLoss(const G4String& );
virtual ~G4VIeEnergyLoss();
G4bool IsApplicable(const G4ParticleDefinition&);
public:
void BuildDEDXTable(const G4ParticleDefinition& aParticleType);
G4double GetContinuousStepLimit(const G4Track& track,
G4double previousStepSize,
G4double currentMinimumStep,
G4double& currentSafety);
G4VParticleChange* AlongStepDoIt(const G4Track& track,
const G4Step& Step) ;
virtual G4VParticleChange* PostStepDoIt(const G4Track& track,
const G4Step& Step) = 0;
private:
void BuildRangeTable(const G4ParticleDefinition& aParticleType);
void BuildInverseRangeTable(const G4ParticleDefinition& aParticleType);
void BuildTimeTables(const G4ParticleDefinition& aParticleType);
void BuildRangeVector(G4int materialIndex,
G4PhysicsLogVector* rangeVector);
void BuildLabTimeVector(G4int materialIndex,
G4PhysicsLogVector* rangeVector);
void BuildProperTimeVector(G4int materialIndex,
G4PhysicsLogVector* rangeVector);
void InvertRangeVector(G4int materialIndex,
G4PhysicsLogVector* rangeVector);
G4double RangeIntLin(G4PhysicsVector* physicsVector,G4int nbin);
G4double RangeIntLog(G4PhysicsVector* physicsVector,G4int nbin);
G4double LabTimeIntLog(G4PhysicsVector* physicsVector,G4int nbin);
G4double ProperTimeIntLog(G4PhysicsVector* physicsVector,G4int nbin);
void BuildRangeCoeffATable(const G4ParticleDefinition& aParticleType);
void BuildRangeCoeffBTable(const G4ParticleDefinition& aParticleType);
void BuildRangeCoeffCTable(const G4ParticleDefinition& aParticleType);
G4double GetConstraints(const G4DynamicParticle* aParticle,
G4Material* aMaterial);
G4double GetLossWithFluct(const G4DynamicParticle* aParticle,
G4Material* aMaterial,
G4double ChargeSquare,
G4double MeanLoss,
G4double step) ;
// hide assignment operator
G4VIeEnergyLoss (G4VIeEnergyLoss &);
G4VIeEnergyLoss & operator=(const G4VIeEnergyLoss &right);
protected:
G4PhysicsTable* theLossTable;
G4double ParticleMass; // heavily used
private:
G4PhysicsTable* theDEDXTable;
G4PhysicsTable* theRangeTable;
G4PhysicsTable* theInverseRangeTable;
G4PhysicsTable* theLabTimeTable ;
G4PhysicsTable* theProperTimeTable ;
G4int CounterOfProcess;
G4PhysicsTable** RecorderOfProcess;
G4double fdEdx; // computed in GetConstraints
G4double fRangeNow; // computed in GetConstraints
G4int EnergyBinNumber; // computed in GetConstraints
// (needed to compute range)
G4int TotBin; // number of bins in table,
// calculated in BuildPhysicTable
G4double LowestKineticEnergy;
G4double HighestKineticEnergy;
G4double RTable,LOGRTable; // LOGRTable=log(HighestKineticEnergy-
// LowestKineticEnergy)/TotBin
// RTable = exp(LOGRTable)
G4PhysicsTable* theRangeCoeffATable;
G4PhysicsTable* theRangeCoeffBTable;
G4PhysicsTable* theRangeCoeffCTable;
// variables for the integration routines
G4double taulow,tauhigh,ltaulow,ltauhigh;
// data members to speed up the fluctuation calculation
G4Material* lastMaterial;
G4int imat;
G4double f1Fluct,f2Fluct,e1Fluct,e2Fluct,rateFluct,ipotFluct;
G4double e1LogFluct,e2LogFluct,ipotLogFluct;
const G4double MaxExcitationNumber ;
const G4double probLimFluct ;
const long nmaxDirectFluct,nmaxCont1,nmaxCont2 ;
//
// static part of the class
//
protected:
//basic DEDX and Range tables
static G4PhysicsTable* theDEDXElectronTable ;
static G4PhysicsTable* theDEDXPositronTable ;
static G4PhysicsTable* theRangeElectronTable ;
static G4PhysicsTable* theRangePositronTable ;
//inverse tables of the range tables
static G4PhysicsTable* theInverseRangeElectronTable;
static G4PhysicsTable* theInverseRangePositronTable;
// lab and proper time tables
static G4PhysicsTable* theLabTimeElectronTable ;
static G4PhysicsTable* theLabTimePositronTable ;
static G4PhysicsTable* theProperTimeElectronTable ;
static G4PhysicsTable* theProperTimePositronTable ;
//processes inherited from G4VIeEnergyLoss
//register themselves in the static array Recorder
//for electrons/positrons separately
//nb of contributing processes = NbOfProcesses
static G4int NbOfProcesses;
static G4int CounterOfElectronProcess;
static G4int CounterOfPositronProcess ;
static G4PhysicsTable** RecorderOfElectronProcess;
static G4PhysicsTable** RecorderOfPositronProcess;
private:
//for interpolation within the tables
static G4PhysicsTable* theeRangeCoeffATable;
static G4PhysicsTable* theeRangeCoeffBTable;
static G4PhysicsTable* theeRangeCoeffCTable;
static G4PhysicsTable* thepRangeCoeffATable;
static G4PhysicsTable* thepRangeCoeffBTable;
static G4PhysicsTable* thepRangeCoeffCTable;
static G4double dRoverRange; // dRoverRange is the maximum allowed
// deltarange/range in one Step
static G4double finalRange; // final step before stopping
static G4bool rndmStepFlag; // control the randomization of the step
static G4bool EnlossFlucFlag; // control the energy loss fluctuation
static G4EnergyLossMessenger* eLossMessenger;
public:
static void SetNbOfProcesses(G4int nb) {NbOfProcesses=nb;};
static void PlusNbOfProcesses() {NbOfProcesses++ ;};
static void MinusNbOfProcesses() {NbOfProcesses-- ;};
static G4int GetNbOfProcesses() {return NbOfProcesses;};
static void SetRndmStep (G4bool value) {rndmStepFlag = value;}
static void SetEnlossFluc (G4bool value) {EnlossFlucFlag = value;}
static void SetStepFunction (G4double c1, G4double c2)
{dRoverRange = c1; finalRange = c2;}
};
#include "G4VIeEnergyLoss.icc"
#endif
source/processes/electromagnetic/standard/include/G4VIeEnergyLoss.icc
-55
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@@ -1,55 +0,0 @@
// 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: G4VIeEnergyLoss.icc,v 1.1 2000/04/25 14:33:02 maire Exp $
// GEANT4 tag $Name: geant4-03-00 $
//
// $Id:
// ---------------------------------------------------------------
// GEANT 4 class inlined methods file
//
// For information related to this code contact:
// CERN, IT Division, ASD group
// History: based on object model of
// 2nd December 1995, G.Cosmo
// ------------ G4VIeEnergyLoss physics process ------------
// by Laszlo Urban, 20 March 1997
// ***************************************************************
// It is the first implementation of the NEW UNIFIED ENERGY LOSS PROCESS.
// It calculates the energy loss of e+/e-.
// -------------------------------------------------------------
//
// 27-05-98: new randomization of the Step limit , new extrapolations for
// high/low energies. L.Urban
// 26-10-98: cleanup , L.Urban
// ---------------------------------------------------------------
inline G4bool G4VIeEnergyLoss::IsApplicable(const G4ParticleDefinition&
particle)
{
return( (&particle == G4Electron::Electron())
||(&particle == G4Positron::Positron()) );
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
inline G4double G4VIeEnergyLoss::GetContinuousStepLimit(
const G4Track& track,
G4double,
G4double currentMinimumStep,
G4double&)
{
G4double Step =
GetConstraints(track.GetDynamicParticle(),track.GetMaterial());
if ((Step>0.0)&&(Step<currentMinimumStep)) currentMinimumStep = Step;
return Step ;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
source/processes/electromagnetic/standard/include/G4VIhEnergyLoss.hh
-295
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@@ -1,295 +0,0 @@
// 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: G4VIhEnergyLoss.hh,v 1.3 2000/08/15 09:42:14 urban Exp $
// GEANT4 tag $Name: geant4-03-00 $
//
// $Id:
// ------------------------------------------------------------
// GEANT 4 class header file
//
// 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
// ---------- G4VIhEnergyLoss physics process -----------
// by Laszlo Urban, 30 May 1997
//
// ************************************************************
// It is the first implementation of the NEW UNIFIED ENERGY LOSS PROCESS.
// It calculates the continuous energy loss for charged hadrons.
// Processes giving contribution to the continuous loss :
// ionisation (= cont.ion.loss + delta ray production)
// can be added more easily ..........
// This class creates static proton/antiproton dE/dx and range tables ,
// which tables can be used by other processes.
// The energy loss for other charged hadrons is calculated from the p/pbar
// tables with scaled kinetic energy.
//
// ****************************************************************************
// It is assumed that the cut in range is the same for all the charged hadrons!
// ****************************************************************************
//
// 7/10/98 some bugs fixed + some cleanup , L.Urban
// 26/10/98 cleanup , L.Urban
//
#ifndef G4VIhEnergyLoss_h
#define G4VIhEnergyLoss_h 1
#include "G4ios.hh"
#include "globals.hh"
#include "Randomize.hh"
#include "G4IVContinuousDiscreteProcess.hh"
#include "G4Material.hh"
#include "G4Element.hh"
#include "G4Proton.hh"
#include "G4AntiProton.hh"
#include "G4Electron.hh"
#include "G4VParticleChange.hh"
#include "G4Track.hh"
#include "G4Step.hh"
#include "G4PhysicsLogVector.hh"
#include "G4PhysicsLinearVector.hh"
class G4EnergyLossMessenger;
class G4VIhEnergyLoss : public G4IVContinuousDiscreteProcess
{
public:
G4VIhEnergyLoss(const G4String& );
virtual ~G4VIhEnergyLoss();
G4bool IsApplicable(const G4ParticleDefinition&);
G4double GetContinuousStepLimit(
const G4Track& track,
G4double previousStepSize,
G4double currentMinimumStep,
G4double& currentSafety) ;
G4VParticleChange* AlongStepDoIt(const G4Track& track ,const G4Step& Step) ;
virtual G4VParticleChange* PostStepDoIt(const G4Track& track,
const G4Step& Step) = 0 ;
protected:
private:
// hide assignment operator
G4VIhEnergyLoss(G4VIhEnergyLoss &);
G4VIhEnergyLoss & operator=(const G4VIhEnergyLoss &right);
G4double GetConstraints(const G4DynamicParticle *aParticle,
G4Material *aMaterial);
G4double GetLossWithFluct(const G4DynamicParticle *aParticle,
G4Material *aMaterial,
G4double ChargeSquare,
G4double MeanLoss,
G4double Step) ;
// =====================================================================
public:
protected:
G4PhysicsTable* theLossTable ;
private:
G4double fdEdx; // computed in GetContraints
G4double fRangeNow ; // computed in GetContraints
G4int EnergyBinNumber ;
G4double RangeCoeffA,RangeCoeffB,RangeCoeffC ;
// variables for the integration routines
static G4double Mass,taulow,tauhigh,ltaulow,ltauhigh;
// data members to speed up the fluctuation calculation
G4Material *lastMaterial ;
G4int imat ;
G4double f1Fluct,f2Fluct,e1Fluct,e2Fluct,rateFluct,ipotFluct;
G4double e1LogFluct,e2LogFluct,ipotLogFluct;
const G4double MaxExcitationNumber ;
const G4double probLimFluct ;
const long nmaxDirectFluct,nmaxCont1,nmaxCont2 ;
// ====================================================================
// static part of the class
public:
// get the number of processes contributing to the cont.energy loss
static G4int GetNumberOfProcesses() { return NumberOfProcesses; };
// set the number of processes contributing to the cont.energy loss
static void SetNumberOfProcesses(G4int number)
{NumberOfProcesses=number ; };
// Increment the number of processes contributing to the cont.energy loss
static void PlusNumberOfProcesses()
{ NumberOfProcesses++ ; };
// decrement the number of processes contributing to the cont.energy loss
static void MinusNumberOfProcesses()
{ NumberOfProcesses-- ; };
static void SetdRoverRange(G4double value) {dRoverRange = value;}
static void SetRndmStep (G4bool value) {rndmStepFlag = value;}
static void SetEnlossFluc (G4bool value) {EnlossFlucFlag = value;}
static void SetStepFunction (G4double c1, G4double c2)
{dRoverRange = c1; finalRange = c2;}
protected:
static void BuildDEDXTable(const G4ParticleDefinition& aParticleType);
private:
static void BuildRangeTable(const G4ParticleDefinition& aParticleType);
static void BuildInverseRangeTable(
const G4ParticleDefinition& aParticleType);
static void BuildTimeTables(const G4ParticleDefinition& aParticleType);
static void BuildLabTimeVector(G4int materialIndex,
G4PhysicsLogVector* rangeVector);
static void BuildProperTimeVector(G4int materialIndex,
G4PhysicsLogVector* rangeVector);
static void InvertRangeVector(G4int materialIndex,
G4PhysicsLogVector* rangeVector);
static void BuildRangeVector(G4int materialIndex,
G4PhysicsLogVector* rangeVector);
static G4double LabTimeIntLog(G4PhysicsVector* physicsVector
,G4int nbin);
static G4double ProperTimeIntLog(G4PhysicsVector* physicsVector,
G4int nbin);
static G4double RangeIntLin(G4PhysicsVector* physicsVector
,G4int nbin);
static G4double RangeIntLog(G4PhysicsVector* physicsVector
,G4int nbin);
static void BuildRangeCoeffATable(
const G4ParticleDefinition& aParticleType);
static void BuildRangeCoeffBTable(
const G4ParticleDefinition& aParticleType);
static void BuildRangeCoeffCTable(
const G4ParticleDefinition& aParticleType);
// ====================================================================
public:
protected:
static G4PhysicsTable* theDEDXpTable ;
static G4PhysicsTable* theDEDXpbarTable ;
static G4PhysicsTable* theRangepTable ;
static G4PhysicsTable* theRangepbarTable ;
//inverse of the range tables
static G4PhysicsTable* theInverseRangepTable ;
static G4PhysicsTable* theInverseRangepbarTable ;
//lab and proper time tables
static G4PhysicsTable* theLabTimepTable ;
static G4PhysicsTable* theLabTimepbarTable ;
static G4PhysicsTable* theProperTimepTable ;
static G4PhysicsTable* theProperTimepbarTable ;
// processes inherited from G4VIhEnergyLoss
// register themselves in the static array Recorder
static G4PhysicsTable** RecorderOfpProcess;
static G4PhysicsTable** RecorderOfpbarProcess;
static G4int CounterOfpProcess ;
static G4int CounterOfpbarProcess ;
// particle mass
static G4double ParticleMass ;
static const G4Proton* theProton ;
static const G4AntiProton* theAntiProton ;
// cut in range
static G4double CutInRange;
static G4double LowestKineticEnergy;
static G4double HighestKineticEnergy;
static G4int TotBin; // number of bins in table,
// calculated in BuildPhysicsTable
static G4double RTable,LOGRTable; // LOGRTable=log(HighestKineticEnergy
// /LowestKineticEnergy)/TotBin
// RTable = exp(LOGRTable)
private:
static G4PhysicsTable* theDEDXTable;
static G4PhysicsTable* theRangeTable;
static G4PhysicsTable* theInverseRangeTable;
static G4PhysicsTable* theLabTimeTable;
static G4PhysicsTable* theProperTimeTable;
static G4PhysicsTable** RecorderOfProcess;
static G4int CounterOfProcess;
static G4PhysicsTable* thepRangeCoeffATable;
static G4PhysicsTable* thepRangeCoeffBTable;
static G4PhysicsTable* thepRangeCoeffCTable;
static G4PhysicsTable* thepbarRangeCoeffATable;
static G4PhysicsTable* thepbarRangeCoeffBTable;
static G4PhysicsTable* thepbarRangeCoeffCTable;
static G4PhysicsTable* theRangeCoeffATable;
static G4PhysicsTable* theRangeCoeffBTable;
static G4PhysicsTable* theRangeCoeffCTable;
static G4double dRoverRange ; // maximum allowed deltarange/range
// in one step
static G4double finalRange ; // last step before stop
static G4bool rndmStepFlag ;
static G4bool EnlossFlucFlag ;
static G4int NumberOfProcesses ;
};
#include "G4VIhEnergyLoss.icc"
#endif
source/processes/electromagnetic/standard/include/G4VIhEnergyLoss.icc
-49
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@@ -1,49 +0,0 @@
// 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: G4VIhEnergyLoss.icc,v 1.1 2000/04/25 14:33:02 maire Exp $
// GEANT4 tag $Name: geant4-03-00 $
//
// $Id:
// ---------------------------------------------------------------
// GEANT 4 class inlined methods file
//
// For information related to this code contact:
// CERN, IT Division, ASD group
// History: based on object model of
// 2nd December 1995, G.Cosmo
// ------------ G4VIhEnergyLoss physics process ------------
// by Laszlo Urban, 30 May 1997
// ***************************************************************
// It is the first implementation of the NEW UNIFIED ENERGY LOSS PROCESS.
// It calculates the energy loss of charged hadrons.
// ***************************************************************
// 26/10/98: cleanup , L.Urban
// ---------------------------------------------------------------
inline G4bool G4VIhEnergyLoss::IsApplicable(const G4ParticleDefinition&
particle)
{
return(particle.GetPDGCharge()!= 0.);
}
inline G4double G4VIhEnergyLoss::GetContinuousStepLimit(
const G4Track& track,
G4double,
G4double currentMinimumStep,
G4double&)
{
G4double Step =
GetConstraints(track.GetDynamicParticle(),track.GetMaterial()) ;
if((Step>0.0)&&(Step<currentMinimumStep))
currentMinimumStep = Step ;
return Step ;
}
source/processes/electromagnetic/standard/include/G4VPAIenergyLoss.hh
+1 -1
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@@ -6,7 +6,7 @@
// and all its terms.
//
// $Id: G4VPAIenergyLoss.hh,v 1.2 2000/06/07 17:00:48 maire Exp $
// GEANT4 tag $Name: geant4-03-00 $
// GEANT4 tag $Name: geant4-03-01 $
//
// ------------------------------------------------------------
// GEANT 4 class header file
source/processes/electromagnetic/standard/include/G4VeEnergyLoss.hh
+1 -1
View File
@@ -6,7 +6,7 @@
// and all its terms.
//
// $Id: G4VeEnergyLoss.hh,v 1.5 2000/10/30 06:56:19 urban Exp $
// GEANT4 tag $Name: geant4-03-00 $
// GEANT4 tag $Name: geant4-03-01 $
//
// ---------------------------------------------------------------
source/processes/electromagnetic/standard/include/G4VeEnergyLoss.icc
+1 -1
View File
@@ -6,7 +6,7 @@
// and all its terms.
//
// $Id: G4VeEnergyLoss.icc,v 1.2 2000/05/23 14:39:26 urban Exp $
// GEANT4 tag $Name: geant4-03-00 $
// GEANT4 tag $Name: geant4-03-01 $
//
// ---------------------------------------------------------------
// GEANT 4 class inlined methods file
source/processes/electromagnetic/standard/include/G4VhEnergyLoss.hh
+1 -1
View File
@@ -6,7 +6,7 @@
// and all its terms.
//
// $Id: G4VhEnergyLoss.hh,v 1.7 2000/10/30 06:56:19 urban Exp $
// GEANT4 tag $Name: geant4-03-00 $
// GEANT4 tag $Name: geant4-03-01 $
//
// ------------------------------------------------------------
// GEANT 4 class header file
source/processes/electromagnetic/standard/include/G4VhEnergyLoss.icc
+1 -1
View File
@@ -6,7 +6,7 @@
// and all its terms.
//
// $Id: G4VhEnergyLoss.icc,v 1.2 2000/05/23 14:39:27 urban Exp $
// GEANT4 tag $Name: geant4-03-00 $
// GEANT4 tag $Name: geant4-03-01 $
//
// ---------------------------------------------------------------
// GEANT 4 class inlined methods file
source/processes/electromagnetic/standard/include/G4eBremsstrahlung.hh
+2 -5
View File
@@ -5,8 +5,8 @@
// based on the Program) you indicate your acceptance of this statement,
// and all its terms.
//
// $Id: G4eBremsstrahlung.hh,v 1.7 2000/08/08 10:26:19 urban Exp $
// GEANT4 tag $Name: geant4-03-00 $
// $Id: G4eBremsstrahlung.hh,v 1.8 2001/01/11 10:39:48 urban Exp $
// GEANT4 tag $Name: geant4-03-01 $
//
//
// ------------------------------------------------------------
@@ -93,9 +93,6 @@ class G4eBremsstrahlung : public G4VeEnergyLoss
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);
source/processes/electromagnetic/standard/include/G4eBremsstrahlung.icc
+1 -1
View File
@@ -6,7 +6,7 @@
// and all its terms.
//
// $Id: G4eBremsstrahlung.icc,v 1.3 2000/05/23 15:44:07 maire Exp $
// GEANT4 tag $Name: geant4-03-00 $
// GEANT4 tag $Name: geant4-03-01 $
//
//
// ---------------------------------------------------------------
source/processes/electromagnetic/standard/include/G4eIonisation.hh
+1 -1
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@@ -6,7 +6,7 @@
// and all its terms.
//
// $Id: G4eIonisation.hh,v 1.7 2000/10/30 06:56:19 urban Exp $
// GEANT4 tag $Name: geant4-03-00 $
// GEANT4 tag $Name: geant4-03-01 $
//
//
// ------------------------------------------------------------
source/processes/electromagnetic/standard/include/G4eIonisation.icc
+1 -1
View File
@@ -6,7 +6,7 @@
// and all its terms.
//
// $Id: G4eIonisation.icc,v 1.3 1999/12/15 14:51:49 gunter Exp $
// GEANT4 tag $Name: geant4-03-00 $
// GEANT4 tag $Name: geant4-03-01 $
//
//
// ---------------------------------------------------------------
source/processes/electromagnetic/standard/include/G4eplusAnnihilation.hh
+6 -6
View File
@@ -5,16 +5,16 @@
// based on the Program) you indicate your acceptance of this statement,
// and all its terms.
//
// $Id: G4eplusAnnihilation.hh,v 1.3 1999/12/17 18:26:12 maire Exp $
// GEANT4 tag $Name: geant4-03-00 $
//
// ------------ G4eplusAnnihilation process ------
// by Michel Maire, 7 july 1996
// $Id: G4eplusAnnihilation.hh,v 1.4 2001/02/22 18:26:07 maire Exp $
// GEANT4 tag $Name: geant4-03-01 $
//
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
// 10-01-97, crossection table + meanfreepath table, M.Maire
// 17-03-97, merge 'in fly' and 'at rest', M.Maire
// 31-08-98, new methods SetBining() and PrintInfo()
// ------------------------------------------------------------
//
// class description
//
source/processes/electromagnetic/standard/include/G4eplusAnnihilation.icc
+6 -15
View File
@@ -5,24 +5,15 @@
// based on the Program) you indicate your acceptance of this statement,
// and all its terms.
//
// $Id: G4eplusAnnihilation.icc,v 1.2 1999/12/15 14:51:49 gunter Exp $
// GEANT4 tag $Name: geant4-03-00 $
// $Id: G4eplusAnnihilation.icc,v 1.3 2001/02/22 18:26:08 maire Exp $
// GEANT4 tag $Name: geant4-03-01 $
//
//
// ---------------------------------------------------------------
// GEANT 4 class inlined methods file
//
// For information related to this code contact:
// CERN, CN Division, ASD group
// History: first implementation, based on object model of
// 2nd December 1995, G.Cosmo
// ------------ G4eplusAnnihilation process ---------
// by Michel Maire, 7 July 1996
// ***************************************************************
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
// 10-01-97, crossection table + meanfreepath table, M.Maire
// 17-03-97, merge 'in fly' and 'at rest', M.Maire
// ---------------------------------------------------------------
//
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
inline G4bool G4eplusAnnihilation::IsApplicable(const G4ParticleDefinition& particle)
source/processes/electromagnetic/standard/include/G4hIonisation.hh
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@@ -6,7 +6,7 @@
// and all its terms.
//
// $Id: G4hIonisation.hh,v 1.10 2000/10/30 06:56:19 urban Exp $
// GEANT4 tag $Name: geant4-03-00 $
// GEANT4 tag $Name: geant4-03-01 $
//
//
// ------------------------------------------------------------
source/processes/electromagnetic/standard/include/G4hIonisation.icc
+1 -1
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@@ -6,7 +6,7 @@
// and all its terms.
//
// $Id: G4hIonisation.icc,v 1.3 1999/12/15 14:51:49 gunter Exp $
// GEANT4 tag $Name: geant4-03-00 $
// GEANT4 tag $Name: geant4-03-01 $
//
//
// ---------------------------------------------------------------
source/processes/electromagnetic/standard/include/lof
-10
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@@ -1,10 +0,0 @@
G4IMultipleScattering.hh
G4IMultipleScattering.icc
G4IeBremsstrahlung.hh
G4IeBremsstrahlung.icc
G4IeEnergyLoss.hh
G4IeEnergyLoss.icc
G4IeIonisation.hh
G4IeIonisation.icc
G4IeplusAnnihilation.hh
G4IeplusAnnihilation.icc