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This commit is contained in:
Gabriele Cosmo
2018-06-29 10:58:11 +02:00
parent fe81a77428
commit 6aa23be517
1581 changed files with 124288 additions and 83758 deletions
Download Patch File Download Diff File Expand all files Collapse all files
source/processes/electromagnetic/dna/History
+11 -2
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@@ -14,13 +14,22 @@ committal in the CVS repository !
* Reverse chronological order (last date on top), please *
----------------------------------------------------------*
09-02-2018, M.Asai tag emdna-V10-03-31
22-06-2018, SI tag emdna-V10-04-04
- fixed warnings in lepts models
14-05-2018, SI tag emdna-V10-04-03
- chemistry update by Mathieu
01-05-2018, SI tag emdna-V10-04-02
- chemistry update by Mathieu
09-02-2018, M.Asai tag emdna-V10-04-01
- G4DNAMolecularMaterial.cc :
GetDensityTableFor() and GetNumMolPerVolTableFor() methods are accepted
at G4State_Init rather than G4State_Idle.
- Co-works with run-V10-04-01 and global-V10-04-01.
21-12-2017, G.Cosmo
21-12-2017, G.Cosmo tag emdna-V10-04-00
- Fixed self-consistency in headers (missing #include) in G4IosFlagsSaver,
G4KDNode, G4MoleculeIterator and G4LEPTSDiffXS.
Fixed spurious definition of G4IT namespace in G4ITMultiNavigator header.
source/processes/electromagnetic/dna/management/include/G4KDNode.hh
+1 -1
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@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4KDNode.hh 108498 2018-02-15 15:33:07Z gcosmo $
// $Id: G4KDNode.hh 108087 2017-12-21 09:00:58Z gcosmo $
//
// Author: Mathieu Karamitros
source/processes/electromagnetic/dna/management/include/G4KDTree.hh
+2 -2
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@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4KDTree.hh 102616 2017-02-10 07:57:14Z gcosmo $
// $Id: G4KDTree.hh 110873 2018-06-22 13:11:22Z gcosmo $
//
// Author: Mathieu Karamitros
@@ -271,7 +271,7 @@ protected:
int fNbActiveNodes;
G4KDMap* fKDMap;
G4ThreadLocalStatic G4Allocator<G4KDTree>* fgAllocator;
static G4Allocator<G4KDTree>*& fgAllocator();
};
#include "G4KDTree.icc"
source/processes/electromagnetic/dna/management/include/G4KDTreeResult.hh
+6 -6
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@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4KDTreeResult.hh 101354 2016-11-15 08:27:51Z gcosmo $
// $Id: G4KDTreeResult.hh 110873 2018-06-22 13:11:22Z gcosmo $
//
// Author: Mathieu Karamitros
@@ -120,20 +120,20 @@ public:
//------------------------------------------------------------------------------
#if defined G4EM_ALLOC_EXPORT
extern G4DLLEXPORT G4ThreadLocal G4Allocator<G4KDTreeResult> *aKDTreeAllocator;
extern G4DLLEXPORT G4Allocator<G4KDTreeResult>*& aKDTreeAllocator();
#else
extern G4DLLIMPORT G4ThreadLocal G4Allocator<G4KDTreeResult> *aKDTreeAllocator;
extern G4DLLIMPORT G4Allocator<G4KDTreeResult>*& aKDTreeAllocator();
#endif
inline void * G4KDTreeResult::operator new(size_t)
{
if (!aKDTreeAllocator) aKDTreeAllocator = new G4Allocator<G4KDTreeResult>;
return (void *) aKDTreeAllocator->MallocSingle();
if (!aKDTreeAllocator()) aKDTreeAllocator() = new G4Allocator<G4KDTreeResult>;
return (void *) aKDTreeAllocator()->MallocSingle();
}
inline void G4KDTreeResult::operator delete(void * object)
{
aKDTreeAllocator->FreeSingle((G4KDTreeResult *) object);
aKDTreeAllocator()->FreeSingle((G4KDTreeResult *) object);
}
//------------------------------------------------------------------------------
template<typename PointT>
source/processes/electromagnetic/dna/management/src/G4KDTree.cc
+8 -4
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@@ -43,7 +43,11 @@
using namespace std;
G4ThreadLocal G4Allocator<G4KDTree>* G4KDTree::fgAllocator(0);
G4Allocator<G4KDTree>*& G4KDTree::fgAllocator()
{
G4ThreadLocalStatic G4Allocator<G4KDTree>* _instance = nullptr;
return _instance;
}
//______________________________________________________________________
// KDTree methods
@@ -73,13 +77,13 @@ G4KDTree::~G4KDTree()
void* G4KDTree::operator new(size_t)
{
if (!fgAllocator) fgAllocator = new G4Allocator<G4KDTree>;
return (void *) fgAllocator->MallocSingle();
if (!fgAllocator()) fgAllocator() = new G4Allocator<G4KDTree>;
return (void *) fgAllocator()->MallocSingle();
}
void G4KDTree::operator delete(void *aNode)
{
fgAllocator->FreeSingle((G4KDTree*) aNode);
fgAllocator()->FreeSingle((G4KDTree*) aNode);
}
void G4KDTree::Print(std::ostream& out) const
source/processes/electromagnetic/dna/management/src/G4KDTreeResult.cc
+6 -2
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@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4KDTreeResult.cc 101354 2016-11-15 08:27:51Z gcosmo $
// $Id: G4KDTreeResult.cc 110873 2018-06-22 13:11:22Z gcosmo $
//
// Author: Mathieu Karamitros (kara (AT) cenbg . in2p3 . fr)
//
@@ -37,7 +37,11 @@
using namespace std;
G4ThreadLocal G4Allocator<G4KDTreeResult> *aKDTreeAllocator= 0;
G4Allocator<G4KDTreeResult>*& aKDTreeAllocator()
{
G4ThreadLocalStatic G4Allocator<G4KDTreeResult>* _instance = nullptr;
return _instance;
}
struct ResNode
{
source/processes/electromagnetic/dna/models/include/G4DNAOneStepThermalizationModel.hh
+40 -7
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@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4DNAOneStepThermalizationModel.hh 108498 2018-02-15 15:33:07Z gcosmo $
// $Id: G4DNAOneStepThermalizationModel.hh 110873 2018-06-22 13:11:22Z gcosmo $
//
// Author: Mathieu Karamitros
@@ -47,6 +47,7 @@
#ifndef G4DNAOneStepThermalizationModel_hh
#define G4DNAOneStepThermalizationModel_hh
#include <memory>
#include "G4VEmModel.hh"
class G4ITNavigator;
@@ -86,6 +87,21 @@ namespace DNA{
static const double gEnergies_T1990[11];
static const double gStdDev_T1990[11];
};
//-----------------------
/*
* Article: Ritchie RH, Hamm RN, Turner JE, Bolch WE (1994) Interaction of
* low-energy electrons with condensed matter: relevance for track
* structure.
* Computational approaches in molecular radiation biology, Plenum,
* New York, Vol. 63, pp. 155–166
* Note: also used in Ballarini et al., 2000
*/
struct Ritchie1994{
static void GetPenetration(G4double energy,
G4ThreeVector& displacement);
static double GetRmean(double energy);
};
}
}
@@ -102,7 +118,7 @@ class G4TDNAOneStepThermalizationModel : public G4VEmModel
public:
typedef MODEL Model;
G4TDNAOneStepThermalizationModel(const G4ParticleDefinition* p = 0,
const G4String& nam =
const G4String& nam =
"DNAOneStepThermalizationModel");
virtual ~G4TDNAOneStepThermalizationModel();
@@ -123,19 +139,19 @@ public:
inline void SetVerbose(int flag){
fVerboseLevel = flag;
}
void GetPenetration(G4double energy,
G4ThreeVector& displacement);
double GetRmean(double energy);
protected:
const std::vector<G4double>* fpWaterDensity;
G4ParticleChangeForGamma* fParticleChangeForGamma;
G4ParticleChangeForGamma* fpParticleChangeForGamma;
G4bool fIsInitialised;
G4int fVerboseLevel;
G4Navigator* fNavigator;
std::unique_ptr<G4Navigator> fpNavigator;
private:
G4TDNAOneStepThermalizationModel&
@@ -151,4 +167,21 @@ typedef G4TDNAOneStepThermalizationModel<DNA::Penetration::Meesungnoen2002> G4DN
// Note: if you use the above distribution, it would be
// better to follow the electrons down to 6 eV and only then apply
// the one step thermalization
class G4DNASolvationModelFactory
{
public:
/// @param penetrationType Available options:
/// Meesungnoen2002, Terrisol1990, Ritchie1994
static G4VEmModel* Create(const G4String& penetrationModel);
/// \brief One step thermalization model can be chosen via macro using
/// /process/dna/e-SolvationSubType Ritchie1994
/// \return Create the model defined via the command macro
/// /process/dna/e-SolvationSubType
/// In case the command is unused, it returns the default model set in
/// G4EmParameters.
static G4VEmModel* GetMacroDefinedModel();
};
#endif
source/processes/electromagnetic/dna/models/include/G4DNAOneStepThermalizationModel.hpp
+14 -19
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@@ -54,16 +54,15 @@
template<typename MODEL>
G4TDNAOneStepThermalizationModel<MODEL>::
G4TDNAOneStepThermalizationModel(const G4ParticleDefinition*,
const G4String& nam) :
const G4String& nam) :
G4VEmModel(nam), fIsInitialised(false)
{
fVerboseLevel = 0;
SetLowEnergyLimit(0.);
G4DNAWaterExcitationStructure exStructure;
SetHighEnergyLimit(exStructure.ExcitationEnergy(0));
fParticleChangeForGamma = 0;
fpParticleChangeForGamma = 0;
fpWaterDensity = 0;
fNavigator = 0;
}
//------------------------------------------------------------------------------
@@ -71,12 +70,8 @@ G4VEmModel(nam), fIsInitialised(false)
template<typename MODEL>
G4TDNAOneStepThermalizationModel<MODEL>::~G4TDNAOneStepThermalizationModel()
{
if(fNavigator)
{
// if(fNavigator->GetNavigatorState())
// delete fNavigator->GetNavigatorState();
delete fNavigator;
}
// if(fpNavigator && fpNavigator->GetNavigatorState())
// delete fpNavigator->GetNavigatorState();
}
//------------------------------------------------------------------------------
@@ -104,19 +99,19 @@ Initialise(const G4ParticleDefinition* particleDefinition,
if(!fIsInitialised)
{
fIsInitialised = true;
fParticleChangeForGamma = GetParticleChangeForGamma();
fpParticleChangeForGamma = GetParticleChangeForGamma();
}
G4Navigator* navigator =
G4TransportationManager::GetTransportationManager()->
GetNavigatorForTracking();
fNavigator = new G4Navigator();
fpNavigator.reset(new G4Navigator());
if(navigator){ // add these checks for testing mode
auto world=navigator->GetWorldVolume();
if(world){
fNavigator->SetWorldVolume(world);
fpNavigator->SetWorldVolume(world);
//fNavigator->NewNavigatorState();
}
}
@@ -188,8 +183,8 @@ SampleSecondaries(std::vector<G4DynamicParticle*>*,
if (k <= HighEnergyLimit())
{
fParticleChangeForGamma->ProposeTrackStatus(fStopAndKill);
fParticleChangeForGamma->ProposeLocalEnergyDeposit(k);
fpParticleChangeForGamma->ProposeTrackStatus(fStopAndKill);
fpParticleChangeForGamma->ProposeLocalEnergyDeposit(k);
if(G4DNAChemistryManager::IsActivated())
{
@@ -198,10 +193,10 @@ SampleSecondaries(std::vector<G4DynamicParticle*>*,
//______________________________________________________________
const G4Track * theIncomingTrack =
fParticleChangeForGamma->GetCurrentTrack();
fpParticleChangeForGamma->GetCurrentTrack();
G4ThreeVector finalPosition(theIncomingTrack->GetPosition()+displacement);
fNavigator->SetWorldVolume(theIncomingTrack->GetTouchable()->
fpNavigator->SetWorldVolume(theIncomingTrack->GetTouchable()->
GetVolume(theIncomingTrack->GetTouchable()->
GetHistoryDepth()));
@@ -229,12 +224,12 @@ SampleSecondaries(std::vector<G4DynamicParticle*>*,
// }
//--
fNavigator->ResetHierarchyAndLocate(theIncomingTrack->GetPosition(),
fpNavigator->ResetHierarchyAndLocate(theIncomingTrack->GetPosition(),
direction,
*((G4TouchableHistory*)
theIncomingTrack->GetTouchable()));
fNavigator->ComputeStep(theIncomingTrack->GetPosition(),
fpNavigator->ComputeStep(theIncomingTrack->GetPosition(),
displacement/displacementMag,
displacementMag,
safety);
@@ -248,7 +243,7 @@ SampleSecondaries(std::vector<G4DynamicParticle*>*,
G4DNAChemistryManager::Instance()->CreateSolvatedElectron(theIncomingTrack,
&finalPosition);
fParticleChangeForGamma->SetProposedKineticEnergy(25.e-3*eV);
fpParticleChangeForGamma->SetProposedKineticEnergy(25.e-3*eV);
}
}
}
source/processes/electromagnetic/dna/models/src/G4DNAOneStepThermalizationModel.cc
+212 -146
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4DNAOneStepThermalizationModel.cc 101807 2016-11-30 13:42:28Z gunter $
// $Id: G4DNAOneStepThermalizationModel.cc 110873 2018-06-22 13:11:22Z gcosmo $
//
// Author: Mathieu Karamitros
//
@@ -38,160 +38,226 @@
#include <algorithm>
#include "G4DNAOneStepThermalizationModel.hh"
#include "globals.hh"
#include "G4Exp.hh"
#include "G4RandomDirection.hh"
#include "G4Electron.hh"
#include "G4EmParameters.hh"
//------------------------------------------------------------------------------
namespace DNA{ namespace Penetration{
namespace DNA {
namespace Penetration {
const double
Meesungnoen2002::gCoeff[13] =
{ -4.06217193e-08, 3.06848412e-06, -9.93217814e-05,
1.80172797e-03, -2.01135480e-02, 1.42939448e-01,
-6.48348714e-01, 1.85227848e+00, -3.36450378e+00,
4.37785068e+00, -4.20557339e+00, 3.81679083e+00,
-2.34069784e-01 };
// fit from Meesungnoen, 2002
const double
Terrisol1990::gEnergies_T1990[11] =
{ 0.2, 0.5, 1, 2, 3, 4, 5, 6, 7,
// The two last are not in the dataset
8, 9}; // eV
const double
Terrisol1990::gStdDev_T1990[11] =
{ 17.68*CLHEP::angstrom,
22.3*CLHEP::angstrom,
28.49*CLHEP::angstrom,
45.35*CLHEP::angstrom,
70.03*CLHEP::angstrom,
98.05*CLHEP::angstrom,
120.56*CLHEP::angstrom,
132.73*CLHEP::angstrom,
142.60*CLHEP::angstrom,
// the above value as given in the paper's table does not match
// b=27.22 nm nor the mean value. 129.62*CLHEP::angstrom could be
// a better fit.
//
// The two last are made up
137.9*CLHEP::angstrom,
120.7*CLHEP::angstrom
}; // angstrom
//----------------------------------------------------------------------------
double Meesungnoen2002::GetRmean(double k){
G4double k_eV = k/eV;
if(k_eV>0.1){ // data until 0.2 eV
G4double r_mean = 0;
for(int8_t i=12; i!=-1 ; --i){
r_mean+=gCoeff[12-i]*std::pow(k_eV,i);
}
r_mean*=CLHEP::nanometer;
return r_mean;
}
return 0;
}
void Meesungnoen2002::GetPenetration(G4double k,
G4ThreeVector& displacement){
displacement=G4ThreeVector(0,0,0);
G4double k_eV = k/eV;
if(k_eV>0.1){ // data until 0.2 eV
G4double r_mean = 0;
for(int8_t i=12; i!=-1 ; --i){
r_mean+=gCoeff[12-i]*std::pow(k_eV,i);
}
r_mean*=nanometer;
//G4cout << "rmean = " << r_mean << G4endl;
static constexpr double r2s=0.62665706865775006; //sqrt(CLHEP::pi)/pow(2,3./2.)
// Use r_mean to build a 3D gaussian
double sigma3D = r_mean*r2s;
double x = G4RandGauss::shoot(0,sigma3D);
double y = G4RandGauss::shoot(0,sigma3D);
double z = G4RandGauss::shoot(0,sigma3D);
displacement=G4ThreeVector(x,y,z);
}
else{
displacement=G4RandomDirection()*(1e-3*CLHEP::nanometer);
// rare events:
// prevent H2O and secondary electron to be at the spot
}
}
//----------------------------------------------------------------------------
double Terrisol1990::Get3DStdDeviation(double energy){
G4double k_eV = energy/eV;
if(k_eV < 0.2) return 1e-3*CLHEP::nanometer;
// rare events:
// prevent H2O and secondary electron to be at the spot
if(k_eV == 9.) return gStdDev_T1990[10];
// TODO if k_eV > 9
const double
Meesungnoen2002::gCoeff[13] =
{ -4.06217193e-08, 3.06848412e-06, -9.93217814e-05,
1.80172797e-03, -2.01135480e-02, 1.42939448e-01,
-6.48348714e-01, 1.85227848e+00, -3.36450378e+00,
4.37785068e+00, -4.20557339e+00, 3.81679083e+00,
-2.34069784e-01 };
// fit from Meesungnoen, 2002
size_t lowBin, upBin;
if(k_eV >= 1.){
lowBin=std::floor(k_eV)+1;
upBin=std::min(lowBin+1, size_t(10));
const double
Terrisol1990::gEnergies_T1990[11] =
{ 0.2, 0.5, 1, 2, 3, 4, 5, 6, 7,
// The two last are not in the dataset
8, 9}; // eV
const double
Terrisol1990::gStdDev_T1990[11] =
{ 17.68*CLHEP::angstrom,
22.3*CLHEP::angstrom,
28.49*CLHEP::angstrom,
45.35*CLHEP::angstrom,
70.03*CLHEP::angstrom,
98.05*CLHEP::angstrom,
120.56*CLHEP::angstrom,
132.73*CLHEP::angstrom,
142.60*CLHEP::angstrom,
// the above value as given in the paper's table does not match
// b=27.22 nm nor the mean value. 129.62*CLHEP::angstrom could be
// a better fit.
//
// The two last are made up
137.9*CLHEP::angstrom,
120.7*CLHEP::angstrom
}; // angstrom
//----------------------------------------------------------------------------
double Meesungnoen2002::GetRmean(double k){
G4double k_eV = k/eV;
if(k_eV>0.1){ // data until 0.2 eV
G4double r_mean = 0;
for(int8_t i=12; i!=-1 ; --i){
r_mean+=gCoeff[12-i]*std::pow(k_eV,i);
}
else{
auto it=std::lower_bound(&gEnergies_T1990[0],
&gEnergies_T1990[2],
k_eV);
lowBin = it-&gEnergies_T1990[0];
upBin = lowBin+1;
}
double lowE = gEnergies_T1990[lowBin];
double upE = gEnergies_T1990[upBin];
// G4cout << lowE << " " << upE << G4endl;
double lowS = gStdDev_T1990[lowBin];
double upS = gStdDev_T1990[upBin];
double tanA = (lowS-upS)/(lowE-upE);
double sigma3D = lowS + (k_eV-lowE)*tanA;
return sigma3D;
}
double Terrisol1990::GetRmean(double energy){
double sigma3D=Get3DStdDeviation(energy);
static constexpr double s2r=1.595769121605731;
// pow(2,3./2.)/sqrt(CLHEP::pi)
double r_mean=sigma3D*s2r;
r_mean*=CLHEP::nanometer;
return r_mean;
}
void Terrisol1990::GetPenetration(G4double energy,
G4ThreeVector& displacement){
double sigma3D=Get3DStdDeviation(energy);
// G4cout << "sigma3D = " << sigma3D/CLHEP::nanometer << G4endl;
static constexpr double factor = 2.20496999539;
// 1./(3. - 8./CLHEP::pi);
double sigma1D = std::sqrt(std::pow(sigma3D, 2.)*factor);
// G4cout << "sigma1D = " << sigma1D/CLHEP::nanometer << G4endl;
return 0;
}
double x = G4RandGauss::shoot(0.,sigma1D);
double y = G4RandGauss::shoot(0.,sigma1D);
double z = G4RandGauss::shoot(0.,sigma1D);
displacement=G4ThreeVector(x,y,z);
// G4cout << "displacement[nm]: "
// << displacement.mag()/CLHEP::nanometer << G4endl;
void GetGaussianPenetrationFromRmean3D(G4double r_mean,
G4ThreeVector& displacement)
{
if(r_mean == 0)
{
// rare events:
// prevent H2O and secondary electron from being placed at the same position
displacement = G4RandomDirection() * (1e-3*CLHEP::nanometer);
return;
}
}}
static constexpr double convertRmean3DToSigma1D = 0.62665706865775006;
// = sqrt(CLHEP::pi)/pow(2,3./2.)
// Use r_mean to build a 3D gaussian
const double sigma1D = r_mean * convertRmean3DToSigma1D;
displacement = G4ThreeVector(G4RandGauss::shoot(0, sigma1D),
G4RandGauss::shoot(0, sigma1D),
G4RandGauss::shoot(0, sigma1D));
}
void Meesungnoen2002::GetPenetration(G4double k,
G4ThreeVector& displacement)
{
GetGaussianPenetrationFromRmean3D(GetRmean(k), displacement);
}
//----------------------------------------------------------------------------
void Ritchie1994::GetPenetration(G4double k,
G4ThreeVector& displacement)
{
GetGaussianPenetrationFromRmean3D(k/eV * 1.8 * nm, // r_mean
displacement);
}
//----------------------------------------------------------------------------
double Terrisol1990::Get3DStdDeviation(double energy){
G4double k_eV = energy/eV;
if(k_eV < 0.2){
// rare events:
// prevent H2O and secondary electron to be at the spot
return 1e-3*CLHEP::nanometer;
}
else if(k_eV == 9.){
return gStdDev_T1990[10];
}
else if(k_eV > 9.){
G4ExceptionDescription description;
description << "Terrisol1990 is not tabulated for energies greater than 9eV";
G4Exception("Terrisol1990::Get3DStdDeviation",
"INVALID_ARGUMENT",
FatalErrorInArgument,
description);
}
size_t lowBin, upBin;
if(k_eV >= 1.){
lowBin=std::floor(k_eV)+1;
upBin=std::min(lowBin+1, size_t(10));
}
else{
auto it=std::lower_bound(&gEnergies_T1990[0],
&gEnergies_T1990[2],
k_eV);
lowBin = it-&gEnergies_T1990[0];
upBin = lowBin+1;
}
double lowE = gEnergies_T1990[lowBin];
double upE = gEnergies_T1990[upBin];
double lowS = gStdDev_T1990[lowBin];
double upS = gStdDev_T1990[upBin];
double tanA = (lowS-upS)/(lowE-upE);
double sigma3D = lowS + (k_eV-lowE)*tanA;
return sigma3D;
}
double Terrisol1990::GetRmean(double energy){
double sigma3D=Get3DStdDeviation(energy);
static constexpr double s2r=1.595769121605731; // = pow(2,3./2.)/sqrt(CLHEP::pi)
double r_mean=sigma3D*s2r;
return r_mean;
}
void Terrisol1990::GetPenetration(G4double energy,
G4ThreeVector& displacement){
double sigma3D = Get3DStdDeviation(energy);
static constexpr double factor = 2.20496999539; // = 1./(3. - 8./CLHEP::pi);
double sigma1D = std::sqrt(std::pow(sigma3D, 2.)*factor);
displacement = G4ThreeVector(G4RandGauss::shoot(0, sigma1D),
G4RandGauss::shoot(0, sigma1D),
G4RandGauss::shoot(0, sigma1D));
}
} // Penetration
} // DNA
//------------------------------------------------------------------------------
G4VEmModel* G4DNASolvationModelFactory::Create(const G4String& penetrationModel)
{
G4String modelNamePrefix("DNAOneStepThermalizationModel_");
if(penetrationModel == "Terrisol1990")
{
return new G4TDNAOneStepThermalizationModel<DNA::Penetration::Terrisol1990>(G4Electron::Definition(), modelNamePrefix + penetrationModel);
}
else if(penetrationModel == "Meesungnoen2002")
{
return new G4TDNAOneStepThermalizationModel<DNA::Penetration::Meesungnoen2002>(G4Electron::Definition(), modelNamePrefix + penetrationModel);
}
else if(penetrationModel == "Ritchie1994")
{
return new G4TDNAOneStepThermalizationModel<DNA::Penetration::Ritchie1994>(G4Electron::Definition(), modelNamePrefix + penetrationModel);
}
else
{
G4ExceptionDescription description;
description << penetrationModel + " is not a valid model name.";
G4Exception("G4DNASolvationModelFactory::Create",
"INVALID_ARGUMENT",
FatalErrorInArgument,
description,
"Options are: Terrisol1990, Meesungnoen2002, Ritchie1994.");
}
return nullptr;
}
//------------------------------------------------------------------------------
G4VEmModel* G4DNASolvationModelFactory::GetMacroDefinedModel()
{
auto dnaSubType = G4EmParameters::Instance()->DNAeSolvationSubType();
switch(dnaSubType)
{
case fRitchie1994eSolvation:
return Create("Ritchie1994");
case fTerrisol1990eSolvation:
return Create("Terrisol1990");
case fMeesungnoen2002eSolvation:
case fDNAUnknownModel:
return Create("Meesungnoen2002");
default:
G4Exception("G4DNASolvationModelFactory::GetMacroDefinedModel",
"DnaSubType",
FatalErrorInArgument,
"The solvation parameter stored in G4EmParameters is unknown. Supported types are: fRitchie1994eSolvation, fTerrisol1990eSolvation, fMeesungnoen2002eSolvation.");
}
return nullptr;
}
source/processes/electromagnetic/dna/models/src/G4LEPTSDiffXS.cc
+5 -5
View File
@@ -68,7 +68,7 @@ void G4LEPTSDiffXS::readDXS( ) {
//G4cout << "Reading2 " << fileName << G4endl;
//NumAng = 181;
fscanf(fp, "%d %d %s", &NumAng, &NumEn, DXSTypeName);
(void) fscanf(fp, "%d %d %s", &NumAng, &NumEn, DXSTypeName);
if( !strcmp(DXSTypeName, "KTC") ) DXSType = 2; // read DXS & calculate KT
else if( !strcmp(DXSTypeName, "KT") ) DXSType = 1; // read DXS & KT
else DXSType = 0;
@@ -77,7 +77,7 @@ void G4LEPTSDiffXS::readDXS( ) {
// << "DXSType " << DXSTypeName << " " << DXSType << G4endl;
for (G4int eBin=1; eBin<=NumEn; eBin++){
fscanf(fp,"%f ",&data);
(void) fscanf(fp,"%f ",&data);
Eb[eBin] = (G4double)data;
}
@@ -87,10 +87,10 @@ void G4LEPTSDiffXS::readDXS( ) {
if(DXSType==1) {
G4cout << "DXSTYpe 1" << G4endl;
for (G4int aBin=0;aBin<NumAng;aBin++){
fscanf(fp,"%f ",&data);
(void) fscanf(fp,"%f ",&data);
DXS[0][aBin]=(G4double)data;
for (G4int eBin=1;eBin<=NumEn;eBin++){
fscanf(fp,"%f %f ",&data2, &data);
(void) fscanf(fp,"%f %f ",&data2, &data);
DXS[eBin][aBin]=(G4double)data;
KT[eBin][aBin]=(G4double)data2;
}
@@ -99,7 +99,7 @@ void G4LEPTSDiffXS::readDXS( ) {
else {
for(G4int aBin=0; aBin<NumAng; aBin++){
for(G4int eBin=0; eBin<=NumEn; eBin++){
fscanf(fp,"%f ",&data);
(void) fscanf(fp,"%f ",&data);
DXS[eBin][aBin] = (G4double)data;
}
}
source/processes/electromagnetic/dna/models/src/G4LEPTSElossDistr.cc
+5 -5
View File
@@ -52,21 +52,21 @@ void G4LEPTSElossDistr::ReadFile()
G4int nEnergies;
G4int nAngles;
G4int nData;
fscanf(fp,"%i \n",&nEnergies);
(void) fscanf(fp,"%i \n",&nEnergies);
for( G4int ie = 0; ie < nEnergies; ie++ ){
float energySep;
fscanf(fp,"%f \n",&energySep);
fscanf(fp,"%i \n",&nAngles);
(void) fscanf(fp,"%f \n",&energySep);
(void) fscanf(fp,"%i \n",&nAngles);
for( G4int ia = 0; ia < nAngles; ia++ ){
float angleSep;
fscanf(fp,"%f \n",&angleSep);
(void) fscanf(fp,"%f \n",&angleSep);
G4LEPTSDistribution* dist = new G4LEPTSDistribution();
theNDistributions ++;
mddist angleDist;
angleDist[angleSep] = dist;
theDistributions[energySep] = angleDist;
fscanf(fp,"%i \n",&nData);
(void) fscanf(fp,"%i \n",&nData);
if( dist->ReadFile( fp, nData ) ) {
G4Exception("G4LEPTSElossDistr",
"",
source/processes/electromagnetic/dna/molecules/management/include/G4Molecule.hh
+5 -5
View File
@@ -299,24 +299,24 @@ private:
};
#if defined G4EM_ALLOC_EXPORT
extern G4DLLEXPORT G4ThreadLocal G4Allocator<G4Molecule> *aMoleculeAllocator;
extern G4DLLEXPORT G4Allocator<G4Molecule>*& aMoleculeAllocator();
#else
extern G4DLLIMPORT G4ThreadLocal G4Allocator<G4Molecule> *aMoleculeAllocator;
extern G4DLLIMPORT G4Allocator<G4Molecule>*& aMoleculeAllocator();
#endif
//////////////////////////
inline void * G4Molecule::operator new(size_t)
//////////////////////////
{
if (!aMoleculeAllocator) aMoleculeAllocator = new G4Allocator<G4Molecule>;
return (void *) aMoleculeAllocator->MallocSingle();
if (!aMoleculeAllocator()) aMoleculeAllocator() = new G4Allocator<G4Molecule>;
return (void *) aMoleculeAllocator()->MallocSingle();
}
//////////////////////////
inline void G4Molecule::operator delete(void * aMolecule)
//////////////////////////
{
aMoleculeAllocator->FreeSingle((G4Molecule *) aMolecule);
aMoleculeAllocator()->FreeSingle((G4Molecule *) aMolecule);
}
#endif
source/processes/electromagnetic/dna/molecules/management/src/G4Molecule.cc
+6 -2
View File
@@ -22,7 +22,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4Molecule.cc 103042 2017-03-10 11:50:07Z gcosmo $
// $Id: G4Molecule.cc 110873 2018-06-22 13:11:22Z gcosmo $
//
// ---------------------------------------------------------------------
// GEANT 4 class header file
@@ -62,7 +62,11 @@ using namespace std;
ITImp(G4Molecule)
G4ThreadLocal G4Allocator<G4Molecule> *aMoleculeAllocator = 0;
G4Allocator<G4Molecule>*& aMoleculeAllocator()
{
G4ThreadLocalStatic G4Allocator<G4Molecule>* _instance = nullptr;
return _instance;
}
//______________________________________________________________________________
source/processes/electromagnetic/dna/processes/src/G4DNAElectronSolvation.cc
+1 -1
View File
@@ -66,7 +66,7 @@ void G4DNAElectronSolvation::InitialiseProcess(const G4ParticleDefinition*)
if(!EmModel())
{
SetEmModel(new G4DNAOneStepThermalizationModel);
SetEmModel(G4DNASolvationModelFactory::GetMacroDefinedModel());
}
AddEmModel(1, EmModel());
}
source/processes/electromagnetic/dna/utils/src/G4DNAMolecularMaterial.cc
+1 -1
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4DNAMolecularMaterial.cc 108498 2018-02-15 15:33:07Z gcosmo $
// $Id: G4DNAMolecularMaterial.cc 108397 2018-02-12 10:21:10Z gcosmo $
//
// Author: Mathieu Karamitros
//
source/processes/electromagnetic/highenergy/History
+9 -1
View File
@@ -1,4 +1,4 @@
$Id: History 107367 2017-11-09 10:56:09Z gcosmo $
$Id: History 109567 2018-05-02 07:04:10Z gcosmo $
-------------------------------------------------------------------
=========================================================
@@ -17,6 +17,14 @@ committal in the CVS repository !
* Reverse chronological order (last date on top), please *
----------------------------------------------------------
01 May 2018: V.Ivant (emhighenergy-V10-04-01)
- G4eeToHadronsMultiModel - cleanup of headers
- G4eeToHadronsModel, G4mplIonisationWithDeltaModel - minor cleanup
28 Feb 2018: V.Ivant (emhighenergy-V10-04-00)
- G4AnnihiToMuPair - H.Burkhardt added Coulomb correction to the
cross section at the threshold
08 Nov 2017: D.Sawkey (emhighenergy-V10-03-05)
- G4hBremsstrahlung, G4hPairProduction - update ProcessDescription text
source/processes/electromagnetic/highenergy/include/G4eeToHadronsMultiModel.hh
+3 -3
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4eeToHadronsMultiModel.hh 106715 2017-10-20 09:39:06Z gcosmo $
// $Id: G4eeToHadronsMultiModel.hh 109567 2018-05-02 07:04:10Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -54,8 +54,8 @@
#include "G4ParticleChangeForGamma.hh"
#include "G4TrackStatus.hh"
#include "Randomize.hh"
#include "CLHEP/Units/SystemOfUnits.h"
#include "CLHEP/Units/PhysicalConstants.h"
#include <CLHEP/Units/SystemOfUnits.h>
#include <CLHEP/Units/PhysicalConstants.h>
#include <vector>
class G4eeCrossSections;
source/processes/electromagnetic/highenergy/src/G4AnnihiToMuPair.cc
+9 -5
View File
@@ -24,7 +24,7 @@
// ********************************************************************
//
//
// $Id: G4AnnihiToMuPair.cc 97391 2016-06-02 10:08:45Z gcosmo $
// $Id: G4AnnihiToMuPair.cc 108750 2018-03-02 15:26:50Z gcosmo $
//
// ------------ G4AnnihiToMuPair physics process ------
// by H.Burkhardt, S. Kelner and R. Kokoulin, November 2002
@@ -35,6 +35,7 @@
// 27.01.03 : first implementation (hbu)
// 04.02.03 : cosmetic simplifications (mma)
// 25.10.04 : migrade to new interfaces of ParticleChange (vi)
// 28.02.18 : cross section now including SSS threshold factor
//
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
@@ -110,15 +111,18 @@ G4double G4AnnihiToMuPair::ComputeCrossSectionPerAtom(G4double Epos, G4double Z)
// It gives a good description from threshold to 1000 GeV
{
static const G4double Mmuon = G4MuonPlus::MuonPlus()->GetPDGMass();
static const G4double Rmuon = elm_coupling/Mmuon; //classical particle radius
static const G4double Sig0 = pi*Rmuon*Rmuon/3.; //constant in crossSection
static const G4double Rmuon = CLHEP::elm_coupling/Mmuon; //classical particle radius
static const G4double Sig0 = CLHEP::pi*Rmuon*Rmuon/3.; //constant in crossSection
static const G4double pia = CLHEP::pi * CLHEP::fine_structure_const; // pi * alphaQED
G4double CrossSection = 0.;
if (Epos < LowestEnergyLimit) return CrossSection;
G4double xi = LowestEnergyLimit/Epos;
G4double SigmaEl = Sig0*xi*(1.+xi/2.)*sqrt(1.-xi); // per electron
CrossSection = SigmaEl*Z; // number of electrons per atom
G4double piaxi = pia * sqrt(xi);
G4double SigmaEl = Sig0 * xi * (1.+xi/2.) * piaxi;
if( Epos>LowestEnergyLimit+1.e-5 ) SigmaEl /= (1.-std::exp( -piaxi/std::sqrt(1-xi) ));
CrossSection = SigmaEl*Z; // SigmaEl per electron * number of electrons per atom
return CrossSection;
}
source/processes/electromagnetic/highenergy/src/G4eeToHadronsModel.cc
+3 -7
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4eeToHadronsModel.cc 97391 2016-06-02 10:08:45Z gcosmo $
// $Id: G4eeToHadronsModel.cc 109567 2018-05-02 07:04:10Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -175,11 +175,7 @@ G4double G4eeToHadronsModel::ComputeCrossSectionPerElectron(
G4double energy,
G4double, G4double)
{
G4double cross = 0.0;
if(crossPerElectron) {
cross = crossPerElectron->Value(energy);
}
return cross;
return (crossPerElectron) ? crossPerElectron->Value(energy) : 0.0;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
@@ -226,7 +222,7 @@ void G4eeToHadronsModel::SampleSecondaries(std::vector<G4DynamicParticle*>* newp
gamma->Set4Momentum(gLv);
t -= gLv.e();
newp->push_back(gamma);
if(fabs(t) > MeV) {
if(std::abs(t) > MeV) {
G4cout << "G4eeToHadronsModel::SampleSecondaries: Ebalance(MeV)= "
<< t/MeV << " primary 4-momentum: " << inlv << G4endl;
}
source/processes/electromagnetic/highenergy/src/G4mplIonisationWithDeltaModel.cc
+2 -2
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4mplIonisationWithDeltaModel.cc 97391 2016-06-02 10:08:45Z gcosmo $
// $Id: G4mplIonisationWithDeltaModel.cc 109567 2018-05-02 07:04:10Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -80,7 +80,7 @@ G4mplIonisationWithDeltaModel::G4mplIonisationWithDeltaModel(G4double mCharge,
beta2lim(betalim*betalim),
bg2lim(beta2lim*(1.0 + beta2lim))
{
nmpl = G4lrint(std::fabs(magCharge) * 2 * fine_structure_const);
nmpl = G4lrint(std::abs(magCharge) * 2 * fine_structure_const);
if(nmpl > 6) { nmpl = 6; }
else if(nmpl < 1) { nmpl = 1; }
pi_hbarc2_over_mc2 = pi * hbarc * hbarc / electron_mass_c2;
source/processes/electromagnetic/lowenergy/History
+3 -3
View File
@@ -1,4 +1,4 @@
$Id: History 110113 2018-05-15 11:53:10Z gcosmo $
$Id: History 109509 2018-04-26 07:07:58Z gcosmo $
-------------------------------------------------------------------
=========================================================
@@ -17,11 +17,11 @@ committal in the CVS repository !
* Reverse chronological order (last date on top), please *
----------------------------------------------------------
25.04.2018 V.Ivanchenko, emlowen-V10-03-21
25.04.2018 V.Ivanchenko, emlowen-V10-04-01
- G4LivermorePhotoElectricModel - fixed double deletion of static members
happens when models defined per region (problem #2052)
19.12.2017 G.Cosmo, emlowen-V10-03-20
19.12.2017 G.Cosmo, emlowen-V10-04-00
- Fixed self-consistency in G4ecpssrFormFactorMixsModel header (missing #include).
Thanks to Raphael Isemann for reporting this.
source/processes/electromagnetic/lowenergy/src/G4LivermorePhotoElectricModel.cc
+1 -1
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4LivermorePhotoElectricModel.cc 110113 2018-05-15 11:53:10Z gcosmo $
// $Id: G4LivermorePhotoElectricModel.cc 109509 2018-04-26 07:07:58Z gcosmo $
//
//
// Author: Sebastien Incerti
source/processes/electromagnetic/muons/History
+12 -1
View File
@@ -1,4 +1,4 @@
$Id: History 107366 2017-11-09 10:55:20Z gcosmo $
$Id: History 110571 2018-05-30 13:06:17Z gcosmo $
-------------------------------------------------------------------
=========================================================
@@ -17,6 +17,17 @@ committal in the CVS repository !
* Reverse chronological order (last date on top), please *
----------------------------------------------------------
30 May 18: V.Ivant (emmuons-V10-04-02)
- G4MuPairProductionModel - added minor protection
25 April 18: V.Ivant (emmuons-V10-04-01)
- G4ePairProduction - fixed model name
12 February 18: V.Ivant (emmuons-V10-04-00)
- G4MuMultipleScattering, G4MuPairProduction, G4MuIonisation,
G4ePairProduction, G4MuBremsstrahlungModel, G4MuBremsstrahlung,
G4MuBetheBlochModel - use default destructor
08 November 17: D.Sawkey (emmuons-V10-03-06)
- G4MuMultipleScattering - modify ProcessDescription text
source/processes/electromagnetic/muons/include/G4MuBetheBlochModel.hh
+2 -4
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4MuBetheBlochModel.hh 97392 2016-06-02 10:10:32Z gcosmo $
// $Id: G4MuBetheBlochModel.hh 108424 2018-02-13 11:19:25Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -74,7 +74,7 @@ public:
explicit G4MuBetheBlochModel(const G4ParticleDefinition* p = nullptr,
const G4String& nam = "MuBetheBloch");
virtual ~G4MuBetheBlochModel();
~G4MuBetheBlochModel() = default;
virtual void Initialise(const G4ParticleDefinition*,
const G4DataVector&) override;
@@ -136,8 +136,6 @@ private:
G4double massSquare;
G4double ratio;
G4double twoln10;
//G4double bg2lim;
//G4double taulim;
G4double alphaprime;
static G4double xgi[8],wgi[8];
};
source/processes/electromagnetic/muons/include/G4MuBremsstrahlung.hh
+2 -2
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4MuBremsstrahlung.hh 106716 2017-10-20 09:40:09Z gcosmo $
// $Id: G4MuBremsstrahlung.hh 108424 2018-02-13 11:19:25Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -82,7 +82,7 @@ public:
explicit G4MuBremsstrahlung(const G4String& processName = "muBrems");
virtual ~G4MuBremsstrahlung();
~G4MuBremsstrahlung() = default;
virtual G4bool IsApplicable(const G4ParticleDefinition& p) override;
source/processes/electromagnetic/muons/include/G4MuBremsstrahlungModel.hh
+2 -2
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4MuBremsstrahlungModel.hh 103220 2017-03-22 11:35:04Z gcosmo $
// $Id: G4MuBremsstrahlungModel.hh 108424 2018-02-13 11:19:25Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -77,7 +77,7 @@ public:
explicit G4MuBremsstrahlungModel(const G4ParticleDefinition* p = nullptr,
const G4String& nam = "MuBrem");
virtual ~G4MuBremsstrahlungModel();
~G4MuBremsstrahlungModel() = default;
virtual void Initialise(const G4ParticleDefinition*,
const G4DataVector&) override;
source/processes/electromagnetic/muons/include/G4MuIonisation.hh
+2 -2
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4MuIonisation.hh 106716 2017-10-20 09:40:09Z gcosmo $
// $Id: G4MuIonisation.hh 108424 2018-02-13 11:19:25Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -89,7 +89,7 @@ public:
explicit G4MuIonisation(const G4String& name = "muIoni");
virtual ~G4MuIonisation();
~G4MuIonisation() = default;
virtual G4bool IsApplicable(const G4ParticleDefinition& p) override;
source/processes/electromagnetic/muons/include/G4MuMultipleScattering.hh
+2 -2
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4MuMultipleScattering.hh 107056 2017-11-01 14:52:32Z gcosmo $
// $Id: G4MuMultipleScattering.hh 108424 2018-02-13 11:19:25Z gcosmo $
//
// -----------------------------------------------------------------------------
//
@@ -64,7 +64,7 @@ public: // with description
explicit G4MuMultipleScattering(const G4String& processName="muMsc");
virtual ~G4MuMultipleScattering();
~G4MuMultipleScattering() = default;
// returns true for charged particles, false otherwise
G4bool IsApplicable (const G4ParticleDefinition& p) override;
source/processes/electromagnetic/muons/include/G4MuPairProduction.hh
+2 -2
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4MuPairProduction.hh 106716 2017-10-20 09:40:09Z gcosmo $
// $Id: G4MuPairProduction.hh 108424 2018-02-13 11:19:25Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -77,7 +77,7 @@ public:
explicit G4MuPairProduction(const G4String& processName = "muPairProd");
virtual ~G4MuPairProduction();
~G4MuPairProduction() = default;
virtual G4bool IsApplicable(const G4ParticleDefinition& p) override;
source/processes/electromagnetic/muons/include/G4ePairProduction.hh
+1 -1
View File
@@ -61,7 +61,7 @@ public:
explicit G4ePairProduction(const G4String& processName = "ePairProd");
virtual ~G4ePairProduction();
~G4ePairProduction() = default;
virtual G4bool IsApplicable(const G4ParticleDefinition& p) override;
source/processes/electromagnetic/muons/src/G4MuBetheBlochModel.cc
+1 -6
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4MuBetheBlochModel.cc 97392 2016-06-02 10:10:32Z gcosmo $
// $Id: G4MuBetheBlochModel.cc 108424 2018-02-13 11:19:25Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -100,11 +100,6 @@ G4MuBetheBlochModel::G4MuBetheBlochModel(const G4ParticleDefinition* p,
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4MuBetheBlochModel::~G4MuBetheBlochModel()
{}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4double G4MuBetheBlochModel::MinEnergyCut(const G4ParticleDefinition*,
const G4MaterialCutsCouple* couple)
{
source/processes/electromagnetic/muons/src/G4MuBremsstrahlung.cc
+1 -6
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4MuBremsstrahlung.cc 107056 2017-11-01 14:52:32Z gcosmo $
// $Id: G4MuBremsstrahlung.cc 108424 2018-02-13 11:19:25Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -85,11 +85,6 @@ G4MuBremsstrahlung::G4MuBremsstrahlung(const G4String& name)
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4MuBremsstrahlung::~G4MuBremsstrahlung()
{}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4bool G4MuBremsstrahlung::IsApplicable(const G4ParticleDefinition& p)
{
return (p.GetPDGCharge() != 0.0 && p.GetPDGMass() > 10.0*MeV);
source/processes/electromagnetic/muons/src/G4MuBremsstrahlungModel.cc
+1 -6
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4MuBremsstrahlungModel.cc 97392 2016-06-02 10:10:32Z gcosmo $
// $Id: G4MuBremsstrahlungModel.cc 108424 2018-02-13 11:19:25Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -123,11 +123,6 @@ G4MuBremsstrahlungModel::G4MuBremsstrahlungModel(const G4ParticleDefinition* p,
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4MuBremsstrahlungModel::~G4MuBremsstrahlungModel()
{}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4double G4MuBremsstrahlungModel::MinEnergyCut(const G4ParticleDefinition*,
const G4MaterialCutsCouple*)
{
source/processes/electromagnetic/muons/src/G4MuIonisation.cc
+1 -6
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4MuIonisation.cc 107056 2017-11-01 14:52:32Z gcosmo $
// $Id: G4MuIonisation.cc 108424 2018-02-13 11:19:25Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -109,11 +109,6 @@ G4MuIonisation::G4MuIonisation(const G4String& name)
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4MuIonisation::~G4MuIonisation()
{}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4bool G4MuIonisation::IsApplicable(const G4ParticleDefinition& p)
{
return (p.GetPDGCharge() != 0.0 && p.GetPDGMass() > 10.0*MeV);
source/processes/electromagnetic/muons/src/G4MuMultipleScattering.cc
+1 -6
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4MuMultipleScattering.cc 107366 2017-11-09 10:55:20Z gcosmo $
// $Id: G4MuMultipleScattering.cc 108424 2018-02-13 11:19:25Z gcosmo $
//
// -----------------------------------------------------------------------------
//
@@ -62,11 +62,6 @@ G4MuMultipleScattering::G4MuMultipleScattering(const G4String& pnam)
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4MuMultipleScattering::~G4MuMultipleScattering()
{}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4bool G4MuMultipleScattering::IsApplicable (const G4ParticleDefinition& p)
{
return (p.GetPDGCharge() != 0.0 && !p.IsShortLived());
source/processes/electromagnetic/muons/src/G4MuPairProduction.cc
+1 -6
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4MuPairProduction.cc 107056 2017-11-01 14:52:32Z gcosmo $
// $Id: G4MuPairProduction.cc 108424 2018-02-13 11:19:25Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -94,11 +94,6 @@ G4MuPairProduction::G4MuPairProduction(const G4String& name)
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4MuPairProduction::~G4MuPairProduction()
{}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4bool G4MuPairProduction::IsApplicable(const G4ParticleDefinition& p)
{
return (p.GetPDGCharge() != 0.0 && p.GetPDGMass() > 10.0*MeV);
source/processes/electromagnetic/muons/src/G4MuPairProductionModel.cc
+6 -6
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4MuPairProductionModel.cc 97392 2016-06-02 10:10:32Z gcosmo $
// $Id: G4MuPairProductionModel.cc 110571 2018-05-30 13:06:17Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -324,7 +324,7 @@ G4double G4MuPairProductionModel::ComputeDMicroscopicCrossSection(
G4double c3 = 0.75*sqrte*particleMass;
if (residEnergy <= c3*z13) { return cross; }
G4double c7 = 4.*CLHEP::electron_mass_c2;
static const G4double c7 = 4.*CLHEP::electron_mass_c2;
G4double c8 = 6.*particleMass*particleMass;
G4double alf = c7/pairEnergy;
G4double a3 = 1. - alf;
@@ -620,14 +620,14 @@ void G4MuPairProductionModel::SampleSecondaries(
// the angles of e- and e+ assumed to be the same as virtual gamma
// create G4DynamicParticle object for the particle1
G4double ekin = std::max(ElectronEnergy - electron_mass_c2,0.0);
G4DynamicParticle* aParticle1 =
new G4DynamicParticle(theElectron, gDirection,
ElectronEnergy - electron_mass_c2);
new G4DynamicParticle(theElectron, gDirection, ekin);
// create G4DynamicParticle object for the particle2
ekin = std::max(PositronEnergy - electron_mass_c2,0.0);
G4DynamicParticle* aParticle2 =
new G4DynamicParticle(thePositron, gDirection,
PositronEnergy - electron_mass_c2);
new G4DynamicParticle(thePositron, gDirection, ekin);
// primary change
kineticEnergy -= (ElectronEnergy + PositronEnergy);
source/processes/electromagnetic/muons/src/G4ePairProduction.cc
+1 -6
View File
@@ -70,11 +70,6 @@ G4ePairProduction::G4ePairProduction(const G4String& name)
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4ePairProduction::~G4ePairProduction()
{}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4bool G4ePairProduction::IsApplicable(const G4ParticleDefinition& p)
{
return (G4Electron::Electron() == &p || G4Positron::Positron() == &p);
@@ -100,7 +95,7 @@ void G4ePairProduction::InitialiseEnergyLossProcess(
theParticle = part;
G4MuPairProductionModel* mod = new G4MuPairProductionModel(part);
G4MuPairProductionModel* mod = new G4MuPairProductionModel(part, "ePairProd");
SetEmModel(mod);
lowestKinEnergy = std::max(lowestKinEnergy, part->GetPDGMass()*8.0);
source/processes/electromagnetic/polarisation/History
+12 -2
View File
@@ -1,4 +1,4 @@
$Id: History 108502 2018-02-15 15:41:45Z gcosmo $
$Id: History 109176 2018-04-03 06:53:39Z gcosmo $
-------------------------------------------------------------------
=========================================================
@@ -17,7 +17,17 @@ committal in the CVS repository !
* Reverse chronological order (last date on top), please *
----------------------------------------------------------
12 February 18: V.Ivanchenko (empolar-V10-03-02)
01 April 18: V.Ivanchenko (empolar-V10-04-02)
- G4PolarizedCompton, G4PolarizedPhotoElectricEffect,
G4PolarizedGammaConversion, G4ePolarizedBremsstrahlung,
G4ePolarizedIonisation - cleanup process classes, moved virtual
methods to source, removed unused headers and methods
01 April 18: V.Ivanchenko (empolar-V10-04-01)
- G4PolarizedAnnihilationModel - implemented sampling of final
state AtRest
12 February 18: V.Ivanchenko (empolar-V10-04-00)
- G4StokesVector - moved static inline method to the source
05 August 17: V.Ivanchenko (empolar-V10-03-01)
source/processes/electromagnetic/polarisation/include/G4PolarizedAnnihilationModel.hh
+9 -10
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4PolarizedAnnihilationModel.hh 96114 2016-03-16 18:51:33Z gcosmo $
// $Id: G4PolarizedAnnihilationModel.hh 109176 2018-04-03 06:53:39Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -71,12 +71,11 @@ public:
virtual ~G4PolarizedAnnihilationModel();
virtual void Initialise(const G4ParticleDefinition*,
const G4DataVector&) override;
virtual G4double ComputeCrossSectionPerElectron(
const G4ParticleDefinition*,
G4double kinEnergy,
G4double cut,
G4double emax) override;
const G4DataVector&) final;
virtual G4double
ComputeCrossSectionPerElectron(G4double kinEnergy) final;
void ComputeAsymmetriesPerElectron(G4double gammaEnergy,
G4double & valueX,
G4double & valueA,
@@ -86,7 +85,7 @@ public:
const G4MaterialCutsCouple*,
const G4DynamicParticle*,
G4double tmin,
G4double maxEnergy) override;
G4double maxEnergy) final;
// polarized routines
inline void SetTargetPolarization(const G4ThreeVector & pTarget);
@@ -95,11 +94,12 @@ public:
inline const G4ThreeVector & GetBeamPolarization() const;
inline const G4ThreeVector & GetFinalGamma1Polarization() const;
inline const G4ThreeVector & GetFinalGamma2Polarization() const;
private:
// hide assignment operator
G4PolarizedAnnihilationModel &
operator=(const G4PolarizedAnnihilationModel &right) = delete;
operator=(const G4PolarizedAnnihilationModel &right) = delete;
G4PolarizedAnnihilationModel(const G4PolarizedAnnihilationModel&) = delete;
G4PolarizedAnnihilationCrossSection * crossSectionCalculator;
@@ -113,7 +113,6 @@ private:
G4int verboseLevel;
G4ParticleChangeForGamma* gParticleChange;
G4bool gIsInitialised;
};
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
source/processes/electromagnetic/polarisation/include/G4PolarizedGammaConversion.hh
+1 -10
View File
@@ -24,7 +24,7 @@
// ********************************************************************
//
//
// $Id: G4PolarizedGammaConversion.hh 96114 2016-03-16 18:51:33Z gcosmo $
// $Id: G4PolarizedGammaConversion.hh 109176 2018-04-03 06:53:39Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -89,15 +89,6 @@ private:
G4bool isInitialised;
};
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
inline G4bool G4PolarizedGammaConversion::IsApplicable(const G4ParticleDefinition& p)
{
return (&p == G4Gamma::Gamma());
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
#endif
source/processes/electromagnetic/polarisation/include/G4PolarizedPhotoElectricEffect.hh
+2 -21
View File
@@ -24,7 +24,7 @@
// ********************************************************************
//
//
// $Id: G4PolarizedPhotoElectricEffect.hh 96114 2016-03-16 18:51:33Z gcosmo $
// $Id: G4PolarizedPhotoElectricEffect.hh 109176 2018-04-03 06:53:39Z gcosmo $
//
//
//------------------ G4PolarizedPhotoElectricEffect physics process ------------------
@@ -63,24 +63,16 @@
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
#ifdef NOIONIZATIONAS
#define G4PolarizedPhotoElectricEffect_h 1
#endif
#ifndef G4PolarizedPhotoElectricEffect_h
#define G4PolarizedPhotoElectricEffect_h 1
#include "globals.hh"
#include "G4VEmProcess.hh"
#include "G4Gamma.hh"
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
class G4ParticleDefinition;
class G4VEmModel;
class G4MaterialCutsCouple;
class G4DynamicParticle;
class G4PolarizedPhotoElectricEffect : public G4VEmProcess
@@ -88,7 +80,7 @@ class G4PolarizedPhotoElectricEffect : public G4VEmProcess
public: // with description
explicit G4PolarizedPhotoElectricEffect(const G4String& processName ="pol-phot",
G4ProcessType type = fElectromagnetic);
G4ProcessType type = fElectromagnetic);
virtual ~G4PolarizedPhotoElectricEffect();
@@ -107,16 +99,5 @@ private:
G4bool isInitialised;
};
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
inline
G4bool G4PolarizedPhotoElectricEffect::IsApplicable(const G4ParticleDefinition& p)
{
return (&p == G4Gamma::Gamma());
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
#endif
source/processes/electromagnetic/polarisation/include/G4StokesVector.hh
+1 -1
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4StokesVector.hh 108502 2018-02-15 15:41:45Z gcosmo $
// $Id: G4StokesVector.hh 108422 2018-02-13 11:17:20Z gcosmo $
//
// GEANT4 Class header file
//
source/processes/electromagnetic/polarisation/include/G4ePolarizedIonisation.hh
+1 -5
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4ePolarizedIonisation.hh 96114 2016-03-16 18:51:33Z gcosmo $
// $Id: G4ePolarizedIonisation.hh 109176 2018-04-03 06:53:39Z gcosmo $
// -------------------------------------------------------------------
//
// GEANT4 Class header file
@@ -97,10 +97,6 @@ protected:
virtual void BuildPhysicsTable(const G4ParticleDefinition&) override;
protected:
const G4ParticleDefinition* DefineBaseParticle(const G4ParticleDefinition* p);
private:
void CleanTables();
source/processes/electromagnetic/polarisation/include/G4eplusPolarizedAnnihilation.hh
+2 -2
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4eplusPolarizedAnnihilation.hh 96114 2016-03-16 18:51:33Z gcosmo $
// $Id: G4eplusPolarizedAnnihilation.hh 109176 2018-04-03 06:53:39Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -106,7 +106,7 @@ private:
G4PolarizedAnnihilationModel* emModel;
G4ThreeVector theTargetPolarization;
G4PhysicsTable* theAsymmetryTable; // table for cross section assym.
G4PhysicsTable* theAsymmetryTable; // table for cross section assym.
G4PhysicsTable* theTransverseAsymmetryTable; // table for transverse cross section assym.
};
source/processes/electromagnetic/polarisation/src/G4PolarizedAnnihilationModel.cc
+17 -26
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4PolarizedAnnihilationModel.cc 96114 2016-03-16 18:51:33Z gcosmo $
// $Id: G4PolarizedAnnihilationModel.cc 109176 2018-04-03 06:53:39Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -66,37 +66,32 @@ G4PolarizedAnnihilationModel::G4PolarizedAnnihilationModel(const G4ParticleDefin
: G4eeToTwoGammaModel(p,nam),
crossSectionCalculator(nullptr),
verboseLevel(0),
gParticleChange(nullptr),
gIsInitialised(false)
gParticleChange(nullptr)
{
crossSectionCalculator=new G4PolarizedAnnihilationCrossSection();
crossSectionCalculator = new G4PolarizedAnnihilationCrossSection();
}
G4PolarizedAnnihilationModel::~G4PolarizedAnnihilationModel()
{
if (crossSectionCalculator) delete crossSectionCalculator;
delete crossSectionCalculator;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4PolarizedAnnihilationModel::Initialise(const G4ParticleDefinition*,
const G4DataVector&)
void G4PolarizedAnnihilationModel::Initialise(const G4ParticleDefinition* part,
const G4DataVector& dv)
{
// G4eeToTwoGammaModel::Initialise(part,dv);
if(gIsInitialised) return;
G4eeToTwoGammaModel::Initialise(part, dv);
if(gParticleChange) { return; }
gParticleChange = GetParticleChangeForGamma();
gIsInitialised = true;
}
G4double G4PolarizedAnnihilationModel::ComputeCrossSectionPerElectron(
const G4ParticleDefinition* pd,
G4double kinEnergy,
G4double cut,
G4double emax)
G4double
G4PolarizedAnnihilationModel::ComputeCrossSectionPerElectron(G4double kinEnergy)
{
G4double xs = G4eeToTwoGammaModel::ComputeCrossSectionPerElectron(pd,kinEnergy,
cut,emax);
// cross section from base model
G4double xs = G4eeToTwoGammaModel::ComputeCrossSectionPerElectron(kinEnergy);
G4double polzz = theBeamPolarization.z()*theTargetPolarization.z();
G4double poltt = theBeamPolarization.x()*theTargetPolarization.x()
@@ -138,24 +133,20 @@ void G4PolarizedAnnihilationModel::ComputeAsymmetriesPerElectron(G4double ene,
if ( (valueA < -1) || (1 < valueA)) {
G4cout<< " ERROR PolarizedAnnihilationPS::ComputeAsymmetries \n";
G4cout<< " something wrong in total cross section calculation (valueA)\n";
G4cout<<"*********** LONG "<<valueX<<"\t"<<valueA<<"\t"<<valueT<<" energy = "<<gam<<G4endl;
G4cout<< " LONG: "<<valueX<<"\t"<<valueA<<"\t"<<valueT<<" energy = "<<gam<<G4endl;
}
if ( (valueT < -1) || (1 < valueT)) {
G4cout<< " ERROR PolarizedAnnihilationPS::ComputeAsymmetries \n";
G4cout<< " something wrong in total cross section calculation (valueT)\n";
G4cout<<"****** TRAN "<<valueX<<"\t"<<valueA<<"\t"<<valueT<<" energy = "<<gam<<G4endl;
G4cout<< " TRAN: "<<valueX<<"\t"<<valueA<<"\t"<<valueT<<" energy = "<<gam<<G4endl;
}
}
void G4PolarizedAnnihilationModel::SampleSecondaries(std::vector<G4DynamicParticle*>* fvect,
const G4MaterialCutsCouple* /*couple*/,
const G4MaterialCutsCouple*,
const G4DynamicParticle* dp,
G4double /*tmin*/,
G4double /*maxEnergy*/)
G4double, G4double)
{
// G4ParticleChangeForGamma* gParticleChange
// = dynamic_cast<G4ParticleChangeForGamma*>(pParticleChange);
const G4Track * aTrack = gParticleChange->GetCurrentTrack();
// kill primary
@@ -165,7 +156,7 @@ void G4PolarizedAnnihilationModel::SampleSecondaries(std::vector<G4DynamicPartic
// V.Ivanchenko add protection against zero kin energy
G4double PositKinEnergy = dp->GetKineticEnergy();
if(PositKinEnergy < DBL_MIN) {
if(PositKinEnergy == 0.0) {
G4double cosTeta = 2.*G4UniformRand()-1.;
G4double sinTeta = std::sqrt((1.0 - cosTeta)*(1.0 + cosTeta));
source/processes/electromagnetic/polarisation/src/G4PolarizedCompton.cc
+2 -2
View File
@@ -24,7 +24,7 @@
// ********************************************************************
//
//
// $Id: G4PolarizedCompton.cc 105740 2017-08-16 13:05:44Z gcosmo $
// $Id: G4PolarizedCompton.cc 109176 2018-04-03 06:53:39Z gcosmo $
//
//
// File name: G4PolarizedCompton
@@ -123,7 +123,7 @@ void G4PolarizedCompton::InitialiseProcess(const G4ParticleDefinition*)
if(!EmModel(0)) { SetEmModel(new G4KleinNishinaCompton()); }
} else {
emModel = new G4PolarizedComptonModel();
SetEmModel(emModel, 1);
SetEmModel(emModel);
}
G4EmParameters* param = G4EmParameters::Instance();
EmModel(0)->SetLowEnergyLimit(param->MinKinEnergy());
source/processes/electromagnetic/polarisation/src/G4PolarizedGammaConversion.cc
+8 -1
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4PolarizedGammaConversion.cc 105740 2017-08-16 13:05:44Z gcosmo $
// $Id: G4PolarizedGammaConversion.cc 109176 2018-04-03 06:53:39Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -68,6 +68,13 @@ G4PolarizedGammaConversion::~G4PolarizedGammaConversion()
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4bool G4PolarizedGammaConversion::IsApplicable(const G4ParticleDefinition& p)
{
return (&p == G4Gamma::Gamma());
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4PolarizedGammaConversion::InitialiseProcess(const G4ParticleDefinition*)
{
if(!isInitialised) {
source/processes/electromagnetic/polarisation/src/G4PolarizedPhotoElectricEffect.cc
+17 -9
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4PolarizedPhotoElectricEffect.cc 85018 2014-10-23 09:51:37Z gcosmo $
// $Id: G4PolarizedPhotoElectricEffect.cc 109176 2018-04-03 06:53:39Z gcosmo $
//
//
//------------------ G4PolarizedPhotoElectricEffect physics process --
@@ -31,20 +31,19 @@
//
// -----------------------------------------------------------------------------
#ifndef NOIONIZATIONAS
#include "G4PolarizedPhotoElectricEffect.hh"
#include "G4PolarizedPEEffectModel.hh"
#include "G4Electron.hh"
#include "G4Gamma.hh"
#include "G4EmParameters.hh"
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
using namespace std;
G4PolarizedPhotoElectricEffect::G4PolarizedPhotoElectricEffect(const G4String& processName,
G4ProcessType type):G4VEmProcess (processName, type),
isInitialised(false)
G4PolarizedPhotoElectricEffect::G4PolarizedPhotoElectricEffect(
const G4String& processName, G4ProcessType type)
: G4VEmProcess (processName, type), isInitialised(false)
{
SetBuildTableFlag(false);
SetSecondaryParticle(G4Electron::Electron());
@@ -58,11 +57,20 @@ G4PolarizedPhotoElectricEffect::~G4PolarizedPhotoElectricEffect()
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
void G4PolarizedPhotoElectricEffect::InitialiseProcess(const G4ParticleDefinition*)
G4bool
G4PolarizedPhotoElectricEffect::IsApplicable(const G4ParticleDefinition& p)
{
return (&p == G4Gamma::Gamma());
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
void
G4PolarizedPhotoElectricEffect::InitialiseProcess(const G4ParticleDefinition*)
{
if(!isInitialised) {
isInitialised = true;
if(!EmModel()) SetEmModel(new G4PolarizedPEEffectModel);
if(!EmModel()) { SetEmModel(new G4PolarizedPEEffectModel); }
G4EmParameters* param = G4EmParameters::Instance();
EmModel()->SetLowEnergyLimit(param->MinKinEnergy());
EmModel()->SetHighEnergyLimit(param->MaxKinEnergy());
@@ -76,4 +84,4 @@ void G4PolarizedPhotoElectricEffect::PrintInfo()
{}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
#endif // NOIONIZATIONAS
source/processes/electromagnetic/polarisation/src/G4StokesVector.cc
+1 -1
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4StokesVector.cc 108502 2018-02-15 15:41:45Z gcosmo $
// $Id: G4StokesVector.cc 108422 2018-02-13 11:17:20Z gcosmo $
//
// GEANT4 Class file
//
source/processes/electromagnetic/polarisation/src/G4ePolarizedBremsstrahlung.cc
+8 -4
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4ePolarizedBremsstrahlung.cc 96114 2016-03-16 18:51:33Z gcosmo $
// $Id: G4ePolarizedBremsstrahlung.cc 109176 2018-04-03 06:53:39Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -62,6 +62,8 @@ G4ePolarizedBremsstrahlung::G4ePolarizedBremsstrahlung(const G4String& name):
G4eBremsstrahlung(name)
{}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4ePolarizedBremsstrahlung::InitialiseEnergyLossProcess(
const G4ParticleDefinition*,
const G4ParticleDefinition*)
@@ -72,11 +74,13 @@ void G4ePolarizedBremsstrahlung::InitialiseEnergyLossProcess(
SetIonisation(false);
G4VEmFluctuationModel* fm = nullptr;
//G4VEmFluctuationModel* fm = new G4UniversalFluctuation();
G4VEmModel* em = new G4ePolarizedBremsstrahlungModel;
em->SetLowEnergyLimit(0.1*keV);
em->SetHighEnergyLimit(100.0*TeV);
G4EmParameters* param = G4EmParameters::Instance();
em->SetLowEnergyLimit(param->MinKinEnergy());
em->SetHighEnergyLimit(param->MaxKinEnergy());
AddEmModel(1, em, fm);
}
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
source/processes/electromagnetic/polarisation/src/G4ePolarizedIonisation.cc
+2 -2
View File
@@ -24,7 +24,7 @@
// ********************************************************************
//
//
// $Id: G4ePolarizedIonisation.cc 105740 2017-08-16 13:05:44Z gcosmo $
// $Id: G4ePolarizedIonisation.cc 109176 2018-04-03 06:53:39Z gcosmo $
// -------------------------------------------------------------------
//
// GEANT4 Class file
@@ -127,7 +127,7 @@ G4bool G4ePolarizedIonisation::IsApplicable(const G4ParticleDefinition& p)
void G4ePolarizedIonisation::InitialiseEnergyLossProcess(
const G4ParticleDefinition* part,
const G4ParticleDefinition* /*part2*/)
const G4ParticleDefinition*)
{
if(!isInitialised) {
source/processes/electromagnetic/standard/History
+104 -2
View File
@@ -1,4 +1,4 @@
$Id: History 108504 2018-02-15 15:46:37Z gcosmo $
$Id: History 110934 2018-06-26 08:11:04Z gcosmo $
-------------------------------------------------------------------
=========================================================
@@ -18,7 +18,109 @@ committal in the CVS repository !
----------------------------------------------------------
09 December 17: V.Ivanchenko (emstand-V10-03-52)
25 June 18: V.Ivanchenko (emstand-V10-04-29)
- G4LindhardSorensenData - fixed Coverity warnings on read beyond
the array boundary
15 June 18: V.Ivanchenko (emstand-V10-04-28)
- G4AtimaEnergyLossModel, G4LindhardSorensenData - fixed Coverity warnings
on read/write out of the array boundary
11 June 18: M.Novak (emstand-V10-04-27)
- G4PairProductionRelModel, G4BetheHeitler5DModel - fixed computation of cross
section in the new version of the high energy model. Fixed triplet production
below treshold in the 5D model by I. Semeniouk.
11 June 18: V.Ivanchenko (emstand-V10-04-26)
- G4AtimaEnergyLossModel, G4AtimaFluctuations - fixed data handling in the
new ion ionisation, which were identified by Coverity code analysis
04 June 18: M. Novak (emstand-V10-04-25)
- G4BetheHeitler5DModel - optimization of the final state sampling (M. Novak)
28 May 18: M. Novak (emstand-V10-04-24)
- G4GoudsmitSaundersonTable - fix gcc-8 warnings regarding.
28 May 18: M. Novak (emstand-V10-04-23)
- G4BetheHeitlerModel, G4PairProductionRelModel, G4BetheHeitler5DModel - new
versions of G4BetheHeitlerModel, G4PairProductionRelModel with improved
screening function approximation, improved LPM function apporximation,
efficiency, documentation and cleanup. Corrected call to selecting target
atom in final state sampling. Follow up changes in the derived
G4BetheHeitler5DModel.
23 May 18: V.Ivanchenko (emstand-V10-04-22)
- G4BetheHeitlerModel - use G4ModifiedTsai angular generator
22 May 18: V.Ivanchenko (emstand-V10-04-21)
- G4DipBustGenerator, G4ModifiedTsai - implement new interface for
directions of e+e- pair
- G4PairProductionRelModel - use G4ModifiedTsai angular generator
- G4BetheHeitlerModel - use G4DipBustGenerator angular generator
- G4UrbanMscModel - use more fast lateral displacement by default
04 May 18: V.Ivanchenko (emstand-V10-04-20)
- G4AtimaEnergyLossModel, G4AtimaFluctuations - new ion ionisation
model developed by J.L.R. Sanchez
- G4WentzelOKandVIxSection - improved Mott corrections to e+-
- G4LindhardSorensenData - fixed Coverity warning
02 May 18: V.Ivanchenko (emstand-V10-04-17)
- G4ScreeningMottCrossSection - added extra method for more effective
computation of the Mott correction
- G4WentzelOKandVIxSection - added Mott corrections to e+-
- G4NISTStoppingData - cleanup header
24 April 18: V.Ivanchenko (emstand-V10-04-16)
- G4LindhardSorensenIonModel,G4LindhardSorensenData - new relativistic ion
ionisation model
- G4BetheBlochModel - minor cleanup
18 April 18: V.Ivanchenko (emstand-V10-04-15)
- G4LindhardSorensenIonModel - new ion ionisation model
- G4UrbanMscModel - use second type of parameterisation in all EM physics
- G4BetheHeitler5DModel - D.Bernard added detailed description of the model
05 April 18: V.Ivanchenko (emstand-V10-04-14)
- G4BetheHeitler5DModel - fixed Coverity warning
01 April 18: V.Ivanchenko (emstand-V10-04-13)
- G4eplusAnnihilation - moved sampling of final state from AtRestDoIt()
method to the SamplingSecondaries() model of a model
- G4eeToTwoGammaModel - cleanup
- G4eplusTo2GammaOKVIModel, G4eplusTo3GammaOKVIModel - new models
23 March 18: V.Ivanchenko (emstand-V10-04-12)
- G4BetheHeitlerModel, G4BetheHeitler5DModel - Igor Semeniouk cleanup the code
07 March 18: V.Ivanchenko (emstand-V10-04-11)
07 March 18: V.Ivanchenko (emstand-V10-04-09)
- G4BetheBlochModel - fixed non-reproducibility introduced in early tag
05 March 18: V.Ivanchenko (emstand-V10-04-08)
05 March 18: V.Ivanchenko (emstand-V10-04-05)
- G4UrbanMscModel - (L.Urban) new lateral displacement algorithm
- G4BetheHeitlerModel, G4BetheHeitler5DModel - Igor Semeniouk and Denis Bernard
added new 5D model
09 February 18: V.Ivanchenko (emstand-V10-04-04)
- G4eBremsstrahlungRelModel, G4PairProductionRelModel, G4PAIySection,
G4PAIxSection, G4ICRU73QOModel - inline method which use static constants
are moved to source, improved formatting of the code
02 February 18: M.Novak (emstand-V10-04-03)
- G4GoudsmitSaundersonMscModel - implemented interface method for macroscopic
1st trans. x-section computation CrossSectionPerVolume (used only for testing)
- G4GSMottCorrection, G4GSPWACorrections - fixed initialization of 1st moment
correction factor
21 December 17: V.Ivanchenko (emstand-V10-04-02)
- G4WentzelOKandVIxSection - fixed formfactor for proton
- G4BetheBlochModel - use formfactor for projectile ion in
formulation of NIM A 488 (2002) 282; this is needed further
evalution, so the tag is not proposed
09 December 17: V.Ivanchenko (emstand-V10-04-01)
- G4PairProductionRelModel - fixed misuse of G4Pow (A13(..) should
be used instead of Z13(..)), add initialisation of an element
cache before sampling of final state (partly fix problem #2017)
source/processes/electromagnetic/standard/include/G4AtimaEnergyLossModel.hh
+222
View File
@@ -0,0 +1,222 @@
//
// ********************************************************************
// * License and Disclaimer *
// * *
// * The Geant4 software is copyright of the Copyright Holders of *
// * the Geant4 Collaboration. It is provided under the terms and *
// * conditions of the Geant4 Software License, included in the file *
// * LICENSE and available at http://cern.ch/geant4/license . These *
// * include a list of copyright holders. *
// * *
// * Neither the authors of this software system, nor their employing *
// * institutes,nor the agencies providing financial support for this *
// * work make any representation or warranty, express or implied, *
// * regarding this software system or assume any liability for its *
// * use. Please see the license in the file LICENSE and URL above *
// * for the full disclaimer and the limitation of liability. *
// * *
// * This code implementation is the result of the scientific and *
// * technical work of the GEANT4 collaboration. *
// * By using, copying, modifying or distributing the software (or *
// * any work based on the software) you agree to acknowledge its *
// * use in resulting scientific publications, and indicate your *
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
//
// GEANT4 Class header file
//
// File name: G4AtimaEnergyLossModel
//
// Author: Jose Luis Rodriguez Sanchez on base of ATIMA code
//
// Creation date: 16.01.2018
//
// Modifications:
//
//
// Class Description:
//
// Implementation of ATIMA model of energy loss
// by heavy charged particles
// -------------------------------------------------------------------
//
#ifndef G4AtimaEnergyLossModel_h
#define G4AtimaEnergyLossModel_h 1
#include <CLHEP/Units/SystemOfUnits.h>
#include "G4VEmModel.hh"
#include "G4NistManager.hh"
class G4EmCorrections;
class G4ParticleChangeForLoss;
class G4AtimaEnergyLossModel : public G4VEmModel
{
public:
explicit G4AtimaEnergyLossModel(const G4ParticleDefinition* p = nullptr,
const G4String& nam = "Atima");
virtual ~G4AtimaEnergyLossModel();
virtual void Initialise(const G4ParticleDefinition*,
const G4DataVector&) override;
virtual G4double MinEnergyCut(const G4ParticleDefinition*,
const G4MaterialCutsCouple* couple) override;
virtual G4double ComputeCrossSectionPerElectron(
const G4ParticleDefinition*,
G4double kineticEnergy,
G4double cutEnergy,
G4double maxEnergy);
virtual G4double ComputeCrossSectionPerAtom(
const G4ParticleDefinition*,
G4double kineticEnergy,
G4double Z, G4double A,
G4double cutEnergy,
G4double maxEnergy) override;
virtual G4double CrossSectionPerVolume(const G4Material*,
const G4ParticleDefinition*,
G4double kineticEnergy,
G4double cutEnergy,
G4double maxEnergy) override;
virtual G4double ComputeDEDXPerVolume(const G4Material*,
const G4ParticleDefinition*,
G4double kineticEnergy,
G4double) override;
virtual G4double GetChargeSquareRatio(const G4ParticleDefinition* p,
const G4Material* mat,
G4double kineticEnergy) override;
virtual G4double GetParticleCharge(const G4ParticleDefinition* p,
const G4Material* mat,
G4double kineticEnergy) override;
virtual void CorrectionsAlongStep(const G4MaterialCutsCouple*,
const G4DynamicParticle*,
G4double&,
G4double&,
G4double) override;
virtual void SampleSecondaries(std::vector<G4DynamicParticle*>*,
const G4MaterialCutsCouple*,
const G4DynamicParticle*,
G4double tmin,
G4double maxEnergy) override;
protected:
virtual G4double MaxSecondaryEnergy(const G4ParticleDefinition*,
G4double kinEnergy) override;
inline G4double GetChargeSquareRatio() const;
inline void SetChargeSquareRatio(G4double val);
private:
void SetupParameters();
inline void SetParticle(const G4ParticleDefinition* p);
inline void SetGenericIon(const G4ParticleDefinition* p);
G4double StoppingPower(G4double ap, G4double zp, G4double ep, G4double at, G4double zt);
G4double Bethek_dedx_e(G4double ap,G4double zp,G4double ep,G4double at,G4double zt);
G4double dedx_n(const G4double ap, const G4double zp, const G4double ep, const G4double at, const G4double zt);
G4double sezi_dedx_e(const G4double zp, const G4double ep, const G4double at, const G4double zt);
G4double sezi_p_se(const G4double energy, const G4double at, const G4double zt);
G4double EnergyTable_interpolate(G4double xval, const G4double* y);
// hide assignment operator
G4AtimaEnergyLossModel & operator=(const G4AtimaEnergyLossModel &right) = delete;
G4AtimaEnergyLossModel(const G4AtimaEnergyLossModel&) = delete;
const G4ParticleDefinition* particle;
G4ParticleDefinition* theElectron;
G4EmCorrections* corr;
G4ParticleChangeForLoss* fParticleChange;
G4NistManager* nist;
G4Pow* g4calc;
G4double mass;
G4double tlimit;
G4double spin;
G4double magMoment2;
G4double chargeSquare;
G4double ratio;
G4double formfact;
G4double corrFactor;
G4bool isIon;
G4double MLN10;
G4double atomic_mass_unit;
G4double dedx_constant;
G4double electron_mass;
G4double fine_structure;
G4double domega2dx_constant;
static G4double stepE;
static G4double tableE[200];
static const G4double element_atomic_weights[110];
static const G4double ls_coefficients_a[110][200];
static const G4double ls_coefficients_ahi[110][200];
static const G4double proton_stopping_coef[92][8];
static const G4double ionisation_potentials_z[121];
static const G4double atima_vfermi[92];
static const G4double atima_lambda_screening[92];
static const G4double x0[92];
static const G4double x1[92];
static const G4double afermi[92];
static const G4double c[92];
static const G4double m0[92];
static const G4double del_0[92];
};
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
inline void G4AtimaEnergyLossModel::SetParticle(const G4ParticleDefinition* p)
{
if(particle != p) {
particle = p;
if(p->GetBaryonNumber() > 3 || p->GetPDGCharge() > CLHEP::eplus)
{ isIon = true; }
SetupParameters();
}
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
inline void G4AtimaEnergyLossModel::SetGenericIon(const G4ParticleDefinition* p)
{
if(p && p->GetParticleName() == "GenericIon") { isIon = true; }
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
inline G4double G4AtimaEnergyLossModel::GetChargeSquareRatio() const
{
return chargeSquare;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
inline void G4AtimaEnergyLossModel::SetChargeSquareRatio(G4double val)
{
chargeSquare = val;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
#endif
source/processes/electromagnetic/standard/include/G4AtimaFluctuations.hh
+129
View File
@@ -0,0 +1,129 @@
//
// ********************************************************************
// * License and Disclaimer *
// * *
// * The Geant4 software is copyright of the Copyright Holders of *
// * the Geant4 Collaboration. It is provided under the terms and *
// * conditions of the Geant4 Software License, included in the file *
// * LICENSE and available at http://cern.ch/geant4/license . These *
// * include a list of copyright holders. *
// * *
// * Neither the authors of this software system, nor their employing *
// * institutes,nor the agencies providing financial support for this *
// * work make any representation or warranty, express or implied, *
// * regarding this software system or assume any liability for its *
// * use. Please see the license in the file LICENSE and URL above *
// * for the full disclaimer and the limitation of liability. *
// * *
// * This code implementation is the result of the scientific and *
// * technical work of the GEANT4 collaboration. *
// * By using, copying, modifying or distributing the software (or *
// * any work based on the software) you agree to acknowledge its *
// * use in resulting scientific publications, and indicate your *
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4AtimaFluctuations.hh $
//
// -------------------------------------------------------------------
//
// GEANT4 Class header file
//
//
// File name: G4AtimaFluctuations
//
// Author: Jose Luis Rodriguez Sanchez on base of ATIMA code
//
// Creation date: 16.01.2018
//
// Modifications:
//
//
// Class Description:
//
// Implementation of ion energy loss fluctuations
//
// -------------------------------------------------------------------
//
#ifndef G4AtimaFluctuations_h
#define G4AtimaFluctuations_h 1
#include "G4VEmFluctuationModel.hh"
#include "G4ParticleDefinition.hh"
#include "G4UniversalFluctuation.hh"
class G4Pow;
class G4AtimaFluctuations : public G4VEmFluctuationModel
{
public:
explicit G4AtimaFluctuations(const G4String& nam = "IonFlucAtima");
virtual ~G4AtimaFluctuations();
// Sample fluctuations
virtual G4double SampleFluctuations(const G4MaterialCutsCouple*,
const G4DynamicParticle*,
G4double tmax,
G4double length,
G4double meanLoss) override;
// Compute dispertion
virtual G4double Dispersion(const G4Material*,
const G4DynamicParticle*,
G4double tmax,
G4double length) override;
// Initialisation prerun
virtual void InitialiseMe(const G4ParticleDefinition*) override;
// Initialisation prestep
virtual void SetParticleAndCharge(const G4ParticleDefinition*,
G4double q2) override;
private:
G4double EnergyTable_interpolate(const G4double* table,G4double xval, const G4double* y);
// hide assignment operator
G4AtimaFluctuations & operator=(const G4AtimaFluctuations &right) = delete;
G4AtimaFluctuations(const G4AtimaFluctuations&) = delete;
G4UniversalFluctuation uniFluct;
const G4ParticleDefinition* particle;
G4Pow* g4calc;
G4double particleMass;
G4double charge;
G4double chargeSquare;
G4double effChargeSquare;
G4double MLN10;
G4double atomic_mass_unit;
G4double dedx_constant;
G4double electron_mass;
G4double fine_structure;
G4double domega2dx_constant;
static G4double stepE;
static G4double tableE[200];
static const G4double ls_X_coefficients_a[110][200];
static const G4double ls_X_coefficients_ahi[110][200];
static const G4double element_atomic_weights[110];
// data members to speed up the fluctuation calculation
G4double minLoss;
// cash
G4double kineticEnergy;
G4double beta2;
};
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
#endif
source/processes/electromagnetic/standard/include/G4BetheBlochModel.hh
+3 -5
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4BetheBlochModel.hh 96934 2016-05-18 09:10:41Z gcosmo $
// $Id: G4BetheBlochModel.hh 108810 2018-03-08 15:04:30Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -175,7 +175,7 @@ inline void G4BetheBlochModel::SetParticle(const G4ParticleDefinition* p)
if(particle != p) {
particle = p;
if(p->GetBaryonNumber() > 3 || p->GetPDGCharge() > CLHEP::eplus)
{ isIon = true; }
{ isIon = true; }
SetupParameters();
}
}
@@ -184,9 +184,7 @@ inline void G4BetheBlochModel::SetParticle(const G4ParticleDefinition* p)
inline void G4BetheBlochModel::SetGenericIon(const G4ParticleDefinition* p)
{
if(p && particle != p) {
if(p->GetParticleName() == "GenericIon") { isIon = true; }
}
if(p && p->GetParticleName() == "GenericIon") { isIon = true; }
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
source/processes/electromagnetic/standard/include/G4BetheHeitler5DModel.hh
+102
View File
@@ -0,0 +1,102 @@
//
// ********************************************************************
// * License and Disclaimer *
// * *
// * The Geant4 software is copyright of the Copyright Holders of *
// * the Geant4 Collaboration. It is provided under the terms and *
// * conditions of the Geant4 Software License, included in the file *
// * LICENSE and available at http://cern.ch/geant4/license . These *
// * include a list of copyright holders. *
// * *
// * Neither the authors of this software system, nor their employing *
// * institutes,nor the agencies providing financial support for this *
// * work make any representation or warranty, express or implied, *
// * regarding this software system or assume any liability for its *
// * use. Please see the license in the file LICENSE and URL above *
// * for the full disclaimer and the limitation of liability. *
// * *
// * This code implementation is the result of the scientific and *
// * technical work of the GEANT4 collaboration. *
// * By using, copying, modifying or distributing the software (or *
// * any work based on the software) you agree to acknowledge its *
// * use in resulting scientific publications, and indicate your *
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: $
//
// -------------------------------------------------------------------
//
// GEANT4 Class header file
//
//
// File name: G4BetheHeitler5DModel
//
// Authors:
// Igor Semeniouk and Denis Bernard,
// LLR, Ecole polytechnique & CNRS/IN2P3, 91128 Palaiseau, France
//
// Modifications:
// 27-10-17 New class (IgS)
// 19-01-18 version that calculates the pdf in the same way as in the fortran
// version (Denis Bernard)
// 04-06-18 Performance optimization of the final state sampling (M. Novak)
//
// Class Description:
//
// Implementation of gamma convertion to e+e- in the field of a nucleus
//
// -------------------------------------------------------------------
//
#ifndef G4BetheHeitler5DModel_h
#define G4BetheHeitler5DModel_h 1
#include "G4BetheHeitlerModel.hh"
class G4IonTable;
class G4BetheHeitler5DModel : public G4BetheHeitlerModel
{
public:
explicit G4BetheHeitler5DModel(const G4ParticleDefinition* p = nullptr,
const G4String& nam = "BetheHeitler5D");
virtual ~G4BetheHeitler5DModel();
virtual void Initialise(const G4ParticleDefinition*,
const G4DataVector&) final;
void SampleSecondaries(std::vector<G4DynamicParticle*>* fvect,
const G4MaterialCutsCouple* couple,
const G4DynamicParticle* aDynamicGamma,
G4double, G4double) final;
inline void SetVerbose(G4int val) { fVerbose = val; }
private:
// hide assignment operator
G4BetheHeitler5DModel& operator=(const G4BetheHeitler5DModel& right) = delete;
G4BetheHeitler5DModel(const G4BetheHeitler5DModel&) = delete;
void BoostG4LorentzVector(const G4LorentzVector& p, const G4LorentzVector& q,
G4LorentzVector& res) const;
void BoostG4LorentzVector(const G4LorentzVector& p, const G4double qz,
const G4double qt, const G4double lffac,
const G4double imass, G4LorentzVector& res) const;
G4double MaxDiffCrossSection(const G4double* par, G4double eZ,
G4double e, G4double loge) const;
G4IonTable* theIonTable;
G4int fVerbose;
G4int fConversionType;
G4bool iraw;
};
#endif
source/processes/electromagnetic/standard/include/G4BetheHeitlerModel.hh
+80 -37
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4BetheHeitlerModel.hh 106628 2017-10-17 06:25:38Z gcosmo $
// $Id: G4BetheHeitlerModel.hh 110527 2018-05-29 06:09:58Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -38,6 +38,8 @@
//
// Modifications:
// 02-02-06 Remove InitialiseCrossSectionPerAtom();
// 28-05-18 New version with improved screening function approximation, improved
// efficiency, documentation and cleanup (M. Novak)
//
// Class Description:
//
@@ -54,6 +56,8 @@
#include "G4PhysicsTable.hh"
#include "G4Log.hh"
#include <vector>
class G4ParticleChangeForGamma;
class G4Pow;
@@ -63,70 +67,109 @@ class G4BetheHeitlerModel : public G4VEmModel
public:
explicit G4BetheHeitlerModel(const G4ParticleDefinition* p = 0,
const G4String& nam = "BetheHeitler");
const G4String& nam = "BetheHeitler");
virtual ~G4BetheHeitlerModel();
virtual void Initialise(const G4ParticleDefinition*,
const G4DataVector&) override;
const G4DataVector&) override;
virtual void InitialiseLocal(const G4ParticleDefinition*,
G4VEmModel* masterModel) override;
G4VEmModel* masterModel) override;
virtual G4double ComputeCrossSectionPerAtom(
const G4ParticleDefinition*,
G4double kinEnergy,
G4double Z,
G4double A=0.,
G4double cut=0.,
G4double emax=DBL_MAX) override;
virtual G4double ComputeCrossSectionPerAtom(const G4ParticleDefinition*,
G4double kinEnergy,
G4double Z,
G4double A=0.,
G4double cut=0.,
G4double emax=DBL_MAX) override;
virtual void SampleSecondaries(std::vector<G4DynamicParticle*>*,
const G4MaterialCutsCouple*,
const G4DynamicParticle*,
G4double tmin,
G4double maxEnergy) override;
const G4MaterialCutsCouple*,
const G4DynamicParticle*,
G4double tmin,
G4double maxEnergy) override;
protected:
inline G4double ScreenFunction1(const G4double delta);
inline G4double ScreenFunction2(const G4double delta);
inline void ScreenFunction12(const G4double delta, G4double &f1, G4double &f2);
void InitialiseElementData();
struct ElementData {
G4double fDeltaMaxLow;
G4double fDeltaMaxHigh;
};
private:
G4double ScreenFunction1(G4double ScreenVariable);
G4double ScreenFunction2(G4double ScreenVariable);
// hide assignment operator
G4BetheHeitlerModel & operator=(const G4BetheHeitlerModel &right) = delete;
G4BetheHeitlerModel(const G4BetheHeitlerModel&) = delete;
protected:
static const G4int gMaxZet;
G4Pow* fG4Calc;
G4ParticleDefinition* fTheGamma;
G4ParticleDefinition* fTheElectron;
G4ParticleDefinition* fThePositron;
G4ParticleChangeForGamma* fParticleChange;
G4Pow* g4calc;
G4ParticleDefinition* theGamma;
G4ParticleDefinition* theElectron;
G4ParticleDefinition* thePositron;
G4ParticleChangeForGamma* fParticleChange;
static std::vector<ElementData*> gElementData;
};
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
inline G4double G4BetheHeitlerModel::ScreenFunction1(G4double ScreenVariable)
//
// Bethe screening functions for the elastic (coherent) scattering:
// Bethe's phi1, phi2 coherent screening functions were computed numerically
// by using (the universal) atomic form factors computed based on the Thomas-
// Fermi model of the atom (using numerical solution of the Thomas-Fermi
// screening function instead of Moliere's analytical approximation). The
// numerical results can be well approximated (better than Butcher & Messel
// especially near the delta=1 limit) by:
// ## if delta <= 1.4
// phi1(delta) = 20.806 - delta*(3.190 - 0.5710*delta)
// phi2(delta) = 20.234 - delta*(2.126 - 0.0903*delta)
// ## if delta > 1.4
// phi1(delta) = phi2(delta) = 21.0190 - 4.145*ln(delta + 0.958)
// with delta = 136mc^2kZ^{-1/3}/[E(Eg-E)] = 136Z^{-1/3}eps0/[eps(1-eps)] where
// Eg is the initial photon energy, E is the total energy transferred to one of
// the e-/e+ pair, eps0 = mc^2/Eg and eps = E/Eg.
// compute the value of the screening function 3*PHI1 - PHI2
// Compute the value of the screening function 3*PHI1(delta) - PHI2(delta):
inline G4double G4BetheHeitlerModel::ScreenFunction1(const G4double delta)
{
return (ScreenVariable > 1.)
? 42.24 - 8.368*G4Log(ScreenVariable+0.952)
: 42.392 - ScreenVariable*(7.796 - 1.961*ScreenVariable);
return (delta > 1.4) ? 42.038 - 8.29*G4Log(delta + 0.958)
: 42.184 - delta*(7.444 - 1.623*delta);
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
inline G4double G4BetheHeitlerModel::ScreenFunction2(G4double ScreenVariable)
// compute the value of the screening function 1.5*PHI1 - 0.5*PHI2
// Compute the value of the screening function 1.5*PHI1(delta) +0.5*PHI2(delta):
inline G4double G4BetheHeitlerModel::ScreenFunction2(const G4double delta)
{
return (ScreenVariable > 1.)
? 42.24 - 8.368*G4Log(ScreenVariable+0.952)
: 41.405 - ScreenVariable*(5.828 - 0.8945*ScreenVariable);
return (delta > 1.4) ? 42.038 - 8.29*G4Log(delta + 0.958)
: 41.326 - delta*(5.848 - 0.902*delta);
}
// Same as ScreenFunction1 and ScreenFunction2 but computes them at once
inline void G4BetheHeitlerModel::ScreenFunction12(const G4double delta,
G4double &f1, G4double &f2)
{
if (delta > 1.4) {
f1 = 42.038 - 8.29*G4Log(delta + 0.958);
f2 = f1;
} else {
f1 = 42.184 - delta*(7.444 - 1.623*delta);
f2 = 41.326 - delta*(5.848 - 0.902*delta);
}
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
#endif
source/processes/electromagnetic/standard/include/G4DipBustGenerator.hh
+14 -4
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4DipBustGenerator.hh 96934 2016-05-18 09:10:41Z gcosmo $
// $Id: G4DipBustGenerator.hh 110415 2018-05-23 06:44:31Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -65,14 +65,24 @@ public:
G4double out_energy, G4int Z,
const G4Material* mat = nullptr) final;
G4double PolarAngle(const G4double initial_energy,
const G4double final_energy,
const G4int Z);
virtual void SamplePairDirections(const G4DynamicParticle* dp,
G4double elecKinEnergy,
G4double posiKinEnergy,
G4ThreeVector& dirElectron,
G4ThreeVector& dirPositron,
G4int Z = 0,
const G4Material* mat = nullptr) final;
G4double PolarAngle(G4double initial_energy,
G4double final_energy,
G4int Z);
virtual void PrintGeneratorInformation() const final;
private:
G4double SampleCosTheta(G4double kinEnergy);
// hide assignment operator
G4DipBustGenerator & operator=(const G4DipBustGenerator &right) = delete;
G4DipBustGenerator(const G4DipBustGenerator&) = delete;
source/processes/electromagnetic/standard/include/G4GoudsmitSaundersonMscModel.hh
+7 -1
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4GoudsmitSaundersonMscModel.hh 106953 2017-10-31 08:30:13Z gcosmo $
// $Id: G4GoudsmitSaundersonMscModel.hh 108305 2018-02-02 13:08:43Z gcosmo $
//
// ----------------------------------------------------------------------------
//
@@ -98,6 +98,7 @@
// Unlike the default GS, the Mott-corrected angular distributions are particle type
// (different for e- and e+ <= the DCS_{Mott} and the screening correction) and target
// (Z and material) dependent.
// 02.02.2018 M. Novak: implemented CrossSectionPerVolume interface method (used only for testing)
//
// Class description:
// Kawrakow-Bielajew Goudsmit-Saunderson MSC model based on the screened Rutherford DCS
@@ -156,6 +157,11 @@ public:
virtual G4double ComputeTrueStepLength(G4double geomStepLength);
// method to compute first transport cross section per Volume (i.e. macroscropic first transport cross section; this
// method is used only for testing and not during a normal simulation)
virtual G4double CrossSectionPerVolume(const G4Material*, const G4ParticleDefinition*, G4double kineticEnergy,
G4double cutEnergy = 0.0, G4double maxEnergy = DBL_MAX);
void StartTracking(G4Track*);
void SampleMSC();
source/processes/electromagnetic/standard/include/G4ICRU73QOModel.hh
+47 -90
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4ICRU73QOModel.hh 96934 2016-05-18 09:10:41Z gcosmo $
// $Id: G4ICRU73QOModel.hh 108737 2018-03-02 13:49:56Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -74,54 +74,54 @@ class G4ICRU73QOModel : public G4VEmModel
public:
explicit G4ICRU73QOModel(const G4ParticleDefinition* p = 0,
const G4String& nam = "ICRU73QO");
const G4String& nam = "ICRU73QO");
virtual ~G4ICRU73QOModel();
~G4ICRU73QOModel() = default;
virtual void Initialise(const G4ParticleDefinition*,
const G4DataVector&) override;
const G4DataVector&) override;
virtual G4double ComputeCrossSectionPerElectron(
const G4ParticleDefinition*,
G4double kineticEnergy,
G4double cutEnergy,
G4double maxEnergy) final;
const G4ParticleDefinition*,
G4double kineticEnergy,
G4double cutEnergy,
G4double maxEnergy) final;
virtual G4double ComputeCrossSectionPerAtom(
const G4ParticleDefinition*,
G4double kineticEnergy,
G4double Z, G4double A,
G4double cutEnergy,
G4double maxEnergy) override;
const G4ParticleDefinition*,
G4double kineticEnergy,
G4double Z, G4double A,
G4double cutEnergy,
G4double maxEnergy) override;
virtual G4double CrossSectionPerVolume(const G4Material*,
const G4ParticleDefinition*,
G4double kineticEnergy,
G4double cutEnergy,
G4double maxEnergy) override;
const G4ParticleDefinition*,
G4double kineticEnergy,
G4double cutEnergy,
G4double maxEnergy) override;
virtual G4double ComputeDEDXPerVolume(const G4Material*,
const G4ParticleDefinition*,
G4double kineticEnergy,
G4double) override;
const G4ParticleDefinition*,
G4double kineticEnergy,
G4double) override;
virtual void SampleSecondaries(std::vector<G4DynamicParticle*>*,
const G4MaterialCutsCouple*,
const G4DynamicParticle*,
G4double tmin,
G4double maxEnergy) override;
const G4MaterialCutsCouple*,
const G4DynamicParticle*,
G4double tmin,
G4double maxEnergy) override;
// add correction to energy loss and compute non-ionizing energy loss
virtual void CorrectionsAlongStep(const G4MaterialCutsCouple*,
const G4DynamicParticle*,
G4double& eloss,
G4double& niel,
G4double length) override;
const G4DynamicParticle*,
G4double& eloss,
G4double& niel,
G4double length) override;
protected:
virtual G4double MaxSecondaryEnergy(const G4ParticleDefinition*,
G4double kinEnergy) final;
G4double kinEnergy) final;
private:
@@ -132,6 +132,21 @@ private:
G4double DEDXPerElement(G4int Z, G4double kineticEnergy);
// get number of shell, energy and oscillator strenghts for material
G4int GetNumberOfShells(G4int Z) const;
G4double GetShellEnergy(G4int Z, G4int nbOfTheShell) const;
G4double GetOscillatorEnergy(G4int Z, G4int nbOfTheShell) const;
G4double GetShellStrength(G4int Z, G4int nbOfTheShell) const;
// calculate stopping number for L's term
G4double GetL0(G4double normEnergy) const;
// terms in Z^2
G4double GetL1(G4double normEnergy) const;
// terms in Z^3
G4double GetL2(G4double normEnergy) const;
// terms in Z^4
// hide assignment operator
G4ICRU73QOModel & operator=(const G4ICRU73QOModel &right) = delete;
G4ICRU73QOModel(const G4ICRU73QOModel&) = delete;
@@ -150,22 +165,6 @@ private:
G4bool isInitialised;
// get number of shell, energy and oscillator strenghts for material
G4int GetNumberOfShells(G4int Z) const;
G4double GetShellEnergy(G4int Z, G4int nbOfTheShell) const;
G4double GetOscillatorEnergy(G4int Z, G4int nbOfTheShell) const;
G4double GetShellStrength(G4int Z, G4int nbOfTheShell) const;
// calculate stopping number for L's term
G4double GetL0(G4double normEnergy) const;
// terms in Z^2
G4double GetL1(G4double normEnergy) const;
// terms in Z^3
G4double GetL2(G4double normEnergy) const;
// terms in Z^4
// Z of element at now avaliable for the model
static const G4int NQOELEM = 26;
static const G4int NQODATA = 130;
@@ -207,48 +206,6 @@ inline void G4ICRU73QOModel::SetParticle(const G4ParticleDefinition* p)
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
inline G4int G4ICRU73QOModel::GetNumberOfShells(G4int Z) const
{
G4int nShell = 0;
if(indexZ[Z] >= 0) { nShell = nbofShellsForElement[indexZ[Z]];
} else { nShell = G4AtomicShells::GetNumberOfShells(Z); }
return nShell;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
inline G4double
G4ICRU73QOModel::GetShellEnergy(G4int Z, G4int nbOfTheShell) const
{
G4double shellEnergy = 0.;
G4int idx = indexZ[Z];
if(idx >= 0) { shellEnergy = ShellEnergy[startElemIndex[idx] + nbOfTheShell]*CLHEP::eV;
} else { shellEnergy = GetOscillatorEnergy(Z, nbOfTheShell); }
return shellEnergy;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
inline G4double
G4ICRU73QOModel::GetShellStrength(G4int Z, G4int nbOfTheShell) const
{
G4double shellStrength = 0.;
G4int idx = indexZ[Z];
if(idx >= 0) { shellStrength = SubShellOccupation[startElemIndex[idx] + nbOfTheShell] / Z;
} else { shellStrength = G4double(G4AtomicShells::GetNumberOfElectrons(Z,nbOfTheShell))/Z; }
return shellStrength;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
inline void G4ICRU73QOModel::SetLowestKinEnergy(G4double val)
{
lowestKinEnergy = val;
source/processes/electromagnetic/standard/include/G4LindhardSorensenData.hh
+83
View File
@@ -0,0 +1,83 @@
//
// ********************************************************************
// * License and Disclaimer *
// * *
// * The Geant4 software is copyright of the Copyright Holders of *
// * the Geant4 Collaboration. It is provided under the terms and *
// * conditions of the Geant4 Software License, included in the file *
// * LICENSE and available at http://cern.ch/geant4/license . These *
// * include a list of copyright holders. *
// * *
// * Neither the authors of this software system, nor their employing *
// * institutes,nor the agencies providing financial support for this *
// * work make any representation or warranty, express or implied, *
// * regarding this software system or assume any liability for its *
// * use. Please see the license in the file LICENSE and URL above *
// * for the full disclaimer and the limitation of liability. *
// * *
// * This code implementation is the result of the scientific and *
// * technical work of the GEANT4 collaboration. *
// * By using, copying, modifying or distributing the software (or *
// * any work based on the software) you agree to acknowledge its *
// * use in resulting scientific publications, and indicate your *
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4LindhardSorensenData.hh 96909 2016-05-17 10:16:09Z vnivanch $
#ifndef G4LindhardSorensenData_h
#define G4LindhardSorensenData_h 1
//---------------------------------------------------------------------------
//
// ClassName: G4LindhardSorensenData
//
// Description: Data on stopping power
//
// Author: Alexander Bagulya & Vladimir Ivanchenko
//
// Creation date: 16.04.2018
//
// Class Description:
//
// Parameterised data on corrections to ion stopping power
//
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
#include "globals.hh"
class G4PhysicsVector;
class G4Pow;
class G4LindhardSorensenData
{
public:
explicit G4LindhardSorensenData();
~G4LindhardSorensenData();
G4double GetDeltaL(G4int Z, G4double gamma) const;
private:
void InitialiseData();
G4double ComputeDeltaL(G4int Z, G4double x) const;
// hide assignment operator
G4LindhardSorensenData & operator=
(const G4LindhardSorensenData &right) = delete;
G4LindhardSorensenData(const G4LindhardSorensenData&) = delete;
G4double xmin;
G4double xmax;
G4PhysicsVector* data[9];
G4Pow* g4calc;
};
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
#endif
source/processes/electromagnetic/standard/include/G4LindhardSorensenIonModel.hh
+188
View File
@@ -0,0 +1,188 @@
//
// ********************************************************************
// * License and Disclaimer *
// * *
// * The Geant4 software is copyright of the Copyright Holders of *
// * the Geant4 Collaboration. It is provided under the terms and *
// * conditions of the Geant4 Software License, included in the file *
// * LICENSE and available at http://cern.ch/geant4/license . These *
// * include a list of copyright holders. *
// * *
// * Neither the authors of this software system, nor their employing *
// * institutes,nor the agencies providing financial support for this *
// * work make any representation or warranty, express or implied, *
// * regarding this software system or assume any liability for its *
// * use. Please see the license in the file LICENSE and URL above *
// * for the full disclaimer and the limitation of liability. *
// * *
// * This code implementation is the result of the scientific and *
// * technical work of the GEANT4 collaboration. *
// * By using, copying, modifying or distributing the software (or *
// * any work based on the software) you agree to acknowledge its *
// * use in resulting scientific publications, and indicate your *
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4LindhardSorensenIonModel.hh 108808 2018-03-08 09:45:40Z vnivanch $
//
// -------------------------------------------------------------------
//
// GEANT4 Class header file
//
//
// File name: G4LindhardSorensenIonModel
//
// Author: Alexander Bagulya & Vladimir Ivanchenko
//
// Creation date: 16.04.2018
//
//
// Class Description:
//
// Implementation of ion ionisation energy loss and delta-electron
// production by heavy charged particles according to
// J. Lindhard & A.H. Sorensen, Phys. Rev. A 53 (1996) 2443-2455
// -------------------------------------------------------------------
//
#ifndef G4LindhardSorensenIonModel_h
#define G4LindhardSorensenIonModel_h 1
#include <CLHEP/Units/SystemOfUnits.h>
#include "G4VEmModel.hh"
#include "G4NistManager.hh"
class G4EmCorrections;
class G4ParticleChangeForLoss;
class G4LindhardSorensenData;
class G4LindhardSorensenIonModel : public G4VEmModel
{
public:
explicit G4LindhardSorensenIonModel(const G4ParticleDefinition* p = nullptr,
const G4String& nam = "LindhardSorensen");
virtual ~G4LindhardSorensenIonModel();
virtual void Initialise(const G4ParticleDefinition*,
const G4DataVector&) override;
virtual G4double MinEnergyCut(const G4ParticleDefinition*,
const G4MaterialCutsCouple* couple) override;
virtual G4double ComputeCrossSectionPerElectron(
const G4ParticleDefinition*,
G4double kineticEnergy,
G4double cutEnergy,
G4double maxEnergy);
virtual G4double ComputeCrossSectionPerAtom(
const G4ParticleDefinition*,
G4double kineticEnergy,
G4double Z, G4double A,
G4double cutEnergy,
G4double maxEnergy) override;
virtual G4double CrossSectionPerVolume(const G4Material*,
const G4ParticleDefinition*,
G4double kineticEnergy,
G4double cutEnergy,
G4double maxEnergy) override;
virtual G4double ComputeDEDXPerVolume(const G4Material*,
const G4ParticleDefinition*,
G4double kineticEnergy,
G4double cutEnergy) override;
virtual G4double GetChargeSquareRatio(const G4ParticleDefinition* p,
const G4Material* mat,
G4double kineticEnergy) override;
virtual G4double GetParticleCharge(const G4ParticleDefinition* p,
const G4Material* mat,
G4double kineticEnergy) override;
virtual void CorrectionsAlongStep(const G4MaterialCutsCouple* couple,
const G4DynamicParticle* dp,
G4double& eloss,
G4double&,
G4double length) override;
virtual void SampleSecondaries(std::vector<G4DynamicParticle*>*,
const G4MaterialCutsCouple*,
const G4DynamicParticle*,
G4double tmin,
G4double maxEnergy) override;
protected:
virtual G4double MaxSecondaryEnergy(const G4ParticleDefinition*,
G4double kinEnergy) override;
inline G4double GetChargeSquareRatio() const;
inline void SetChargeSquareRatio(G4double val);
private:
void SetupParameters();
inline void SetParticle(const G4ParticleDefinition* p);
// hide assignment operator
G4LindhardSorensenIonModel & operator=
(const G4LindhardSorensenIonModel &right) = delete;
G4LindhardSorensenIonModel(const G4LindhardSorensenIonModel&) = delete;
static G4LindhardSorensenData* lsdata;
const G4ParticleDefinition* particle;
G4ParticleDefinition* theElectron;
G4EmCorrections* corr;
G4ParticleChangeForLoss* fParticleChange;
G4NistManager* nist;
G4int Zin;
G4double mass;
G4double tlimit;
G4double spin;
G4double magMoment2;
G4double chargeSquare;
G4double charge;
G4double ratio;
G4double formfact;
G4double twoln10;
};
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
inline void
G4LindhardSorensenIonModel::SetParticle(const G4ParticleDefinition* p)
{
if(particle != p) {
particle = p;
SetupParameters();
}
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
inline G4double G4LindhardSorensenIonModel::GetChargeSquareRatio() const
{
return chargeSquare;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
inline void G4LindhardSorensenIonModel::SetChargeSquareRatio(G4double val)
{
chargeSquare = val;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
#endif
source/processes/electromagnetic/standard/include/G4ModifiedTsai.hh
+11 -1
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4ModifiedTsai.hh 96934 2016-05-18 09:10:41Z gcosmo $
// $Id: G4ModifiedTsai.hh 110415 2018-05-23 06:44:31Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -73,10 +73,20 @@ public:
G4double out_energy, G4int Z,
const G4Material* mat = nullptr) final;
virtual void SamplePairDirections(const G4DynamicParticle* dp,
G4double elecKinEnergy,
G4double posiKinEnergy,
G4ThreeVector& dirElectron,
G4ThreeVector& dirPositron,
G4int Z = 0,
const G4Material* mat = nullptr) final;
virtual void PrintGeneratorInformation() const final;
private:
G4double SampleCosTheta(G4double kinEnergy);
// hide assignment operator
G4ModifiedTsai & operator=(const G4ModifiedTsai &right) = delete;
G4ModifiedTsai(const G4ModifiedTsai&) = delete;
source/processes/electromagnetic/standard/include/G4NISTStoppingData.hh
+1 -1
View File
@@ -47,7 +47,7 @@
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
#include "globals.hh"
#include "CLHEP/Units/SystemOfUnits.h"
#include <CLHEP/Units/SystemOfUnits.h>
static const G4String nameNIST[74] = {
"G4_A-150_TISSUE", "G4_ACETYLENE","G4_ADIPOSE_TISSUE_ICRP","G4_Ag","G4_AIR",
source/processes/electromagnetic/standard/include/G4PAIxSection.hh
+7 -11
View File
@@ -24,7 +24,7 @@
// ********************************************************************
//
//
// $Id: G4PAIxSection.hh 96934 2016-05-18 09:10:41Z gcosmo $
// $Id: G4PAIxSection.hh 108737 2018-03-02 13:49:56Z gcosmo $
//
//
// G4PAIxSection.hh -- header file
@@ -194,12 +194,13 @@ public:
G4double GetLowEnergyCof() const { return fLowEnergyCof; }
void SetVerbose(G4int v){fVerbose=v;};
inline G4double GetPAItable(G4int i,G4int j) const;
G4double GetLorentzFactor(G4int i) const;
inline void SetVerbose(G4int v) { fVerbose=v; };
inline G4double GetLorentzFactor(G4int i) const;
inline G4double GetPAItable(G4int i,G4int j) const;
inline G4double GetSplineEnergy(G4int i) const;
inline G4double GetIntegralPAIxSection(G4int i) const;
@@ -283,11 +284,6 @@ inline G4double G4PAIxSection::GetPAItable(G4int i, G4int j) const
return fPAItable[i][j];
}
inline G4double G4PAIxSection::GetLorentzFactor(G4int j) const
{
return fLorentzFactor[j];
}
inline G4double G4PAIxSection::GetSplineEnergy(G4int i) const
{
if(i < 1 || i > fSplineNumber) { CallError(i, "GetSplineEnergy"); }
source/processes/electromagnetic/standard/include/G4PAIySection.hh
+24 -29
View File
@@ -24,7 +24,7 @@
// ********************************************************************
//
//
// $Id: G4PAIySection.hh 96934 2016-05-18 09:10:41Z gcosmo $
// $Id: G4PAIySection.hh 108737 2018-03-02 13:49:56Z gcosmo $
//
//
// G4PAIySection.hh -- header file
@@ -54,11 +54,11 @@ class G4PAIySection
public:
explicit G4PAIySection();
~G4PAIySection();
~G4PAIySection() = default;
void Initialize(const G4Material* material, G4double maxEnergyTransfer,
G4double betaGammaSq, G4SandiaTable*);
G4double betaGammaSq, G4SandiaTable*);
void ComputeLowEnergyCof(const G4Material* material);
@@ -67,25 +67,25 @@ public:
void NormShift( G4double betaGammaSq );
void SplainPAI( G4double betaGammaSq );
// Physical methods
G4double RutherfordIntegral( G4int intervalNumber,
G4double limitLow,
G4double limitHigh );
G4double limitLow,
G4double limitHigh );
G4double ImPartDielectricConst( G4int intervalNumber,
G4double energy );
G4double energy );
G4double RePartDielectricConst(G4double energy);
G4double DifPAIySection( G4int intervalNumber,
G4double betaGammaSq );
G4double betaGammaSq );
G4double PAIdNdxCerenkov( G4int intervalNumber,
G4double betaGammaSq );
G4double betaGammaSq );
G4double PAIdNdxPlasmon( G4int intervalNumber,
G4double betaGammaSq );
G4double betaGammaSq );
void IntegralPAIySection();
void IntegralCerenkov();
@@ -97,24 +97,26 @@ public:
G4double SumOverInterPlasmon(G4int intervalNumber);
G4double SumOverBorder( G4int intervalNumber,
G4double energy );
G4double energy );
G4double SumOverBorderdEdx( G4int intervalNumber,
G4double energy );
G4double energy );
G4double SumOverBordCerenkov( G4int intervalNumber,
G4double energy );
G4double energy );
G4double SumOverBordPlasmon( G4int intervalNumber,
G4double energy );
G4double energy );
G4double GetStepEnergyLoss( G4double step );
G4double GetStepCerenkovLoss( G4double step );
G4double GetStepPlasmonLoss( G4double step );
G4double GetLorentzFactor(G4int j) const;
// Inline access functions
inline G4int GetNumberOfGammas() const { return fNumberOfGammas; }
inline G4int GetSplineSize() const { return fSplineNumber; }
inline G4int GetIntervalNumber() const { return fIntervalNumber; }
inline G4double GetEnergyInterval(G4int i){ return fEnergyInterval[i]; }
@@ -122,7 +124,7 @@ public:
inline G4double GetDifPAIySection(G4int i){ return fDifPAIySection[i]; }
inline G4double GetPAIdNdxCrenkov(G4int i){ return fdNdxCerenkov[i]; }
inline G4double GetPAIdNdxPlasmon(G4int i){ return fdNdxPlasmon[i]; }
inline G4double GetMeanEnergyLoss() const {return fIntegralPAIySection[0]; }
inline G4double GetMeanCerenkovLoss() const {return fIntegralCerenkov[0]; }
inline G4double GetMeanPlasmonLoss() const {return fIntegralPlasmon[0]; }
@@ -130,11 +132,9 @@ public:
inline G4double GetNormalizationCof() const { return fNormalizationCof; }
inline G4double GetPAItable(G4int i,G4int j) const;
inline G4double GetLorentzFactor(G4int i) const;
inline G4double GetSplineEnergy(G4int i) const;
inline G4double GetIntegralPAIySection(G4int i) const;
inline G4double GetIntegralPAIdEdx(G4int i) const;
inline G4double GetIntegralCerenkov(G4int i) const;
@@ -201,17 +201,12 @@ inline G4double G4PAIySection::GetPAItable(G4int i, G4int j) const
return fPAItable[i][j];
}
inline G4double G4PAIySection::GetLorentzFactor(G4int j) const
{
return fLorentzFactor[j];
}
inline G4double G4PAIySection::GetSplineEnergy(G4int i) const
{
if(i < 1 || i > fSplineNumber) { CallError(i, "GetSplineEnergy"); }
return fSplineEnergy[i];
}
inline G4double G4PAIySection::GetIntegralPAIySection(G4int i) const
{
if(i < 1 || i > fSplineNumber) { CallError(i, "GetIntegralPAIySection"); }
source/processes/electromagnetic/standard/include/G4PairProductionRelModel.hh
+141 -158
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4PairProductionRelModel.hh 106628 2017-10-17 06:25:38Z gcosmo $
// $Id: G4PairProductionRelModel.hh 110527 2018-05-29 06:09:58Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -37,6 +37,10 @@
// Creation date: 02.04.2009
//
// Modifications:
// 28-05-18 New version with improved screening function approximation, improved
// LPM function approximation, efficiency, documentation and cleanup.
// Corrected call to selecting target atom in the final state sampling.
// (M. Novak)
//
// Class Description:
//
@@ -53,11 +57,12 @@
#include <CLHEP/Units/PhysicalConstants.h>
#include "G4VEmModel.hh"
#include "G4PhysicsTable.hh"
#include "G4Log.hh"
#include "G4Exp.hh"
#include "G4Pow.hh"
#include <vector>
class G4ParticleChangeForGamma;
class G4PairProductionRelModel : public G4VEmModel
@@ -66,15 +71,15 @@ class G4PairProductionRelModel : public G4VEmModel
public:
explicit G4PairProductionRelModel(const G4ParticleDefinition* p = nullptr,
const G4String& nam = "BetheHeitlerLPM");
const G4String& nam = "BetheHeitlerLPM");
virtual ~G4PairProductionRelModel();
virtual void Initialise(const G4ParticleDefinition*,
const G4DataVector&) override;
const G4DataVector&) override;
virtual void InitialiseLocal(const G4ParticleDefinition*,
G4VEmModel* masterModel) override;
G4VEmModel* masterModel) override;
virtual G4double ComputeCrossSectionPerAtom(
const G4ParticleDefinition*,
@@ -85,182 +90,160 @@ public:
G4double emax=DBL_MAX) override;
virtual void SampleSecondaries(std::vector<G4DynamicParticle*>*,
const G4MaterialCutsCouple*,
const G4DynamicParticle*,
G4double tmin,
G4double maxEnergy) override;
const G4MaterialCutsCouple*,
const G4DynamicParticle*,
G4double tmin,
G4double maxEnergy) override;
virtual void SetupForMaterial(const G4ParticleDefinition*,
const G4Material*,G4double) override;
// * fast inline functions *
inline void SetCurrentElement(G4double Z);
// set / get methods
inline void SetLPMconstant(G4double val);
inline G4double LPMconstant() const;
inline void SetLPMflag(G4bool);
inline G4bool LPMflag() const;
inline void SetLPMflag(G4bool val) { fIsUseLPMCorrection = val; }
inline G4bool LPMflag() const { return fIsUseLPMCorrection; }
protected:
// screening functions
inline G4double Phi1(G4double delta) const;
inline G4double Phi2(G4double delta) const;
inline G4double ScreenFunction1(G4double ScreenVariable);
inline G4double ScreenFunction2(G4double ScreenVariable);
inline G4double DeltaMax() const;
inline G4double DeltaMin(G4double) const;
// for evaluating screening related functions
inline void ComputePhi12(const G4double delta, G4double &phi1, G4double &phi2);
inline G4double ScreenFunction1(const G4double delta);
inline G4double ScreenFunction2(const G4double delta);
inline void ScreenFunction12(const G4double delta, G4double &f1, G4double &f2);
// helper methods for cross-section computation under different approximations
G4double ComputeXSectionPerAtom(G4double gammaEnergy, G4double Z);
G4double ComputeDXSectionPerAtom(G4double eplusEnergy, G4double gammaEnergy,
G4double Z);
G4double ComputeRelDXSectionPerAtom(G4double eplusEnergy, G4double gammaEnergy,
G4double Z);
// lpm functions
void CalcLPMFunctions(G4double k, G4double eplus);
G4double ComputeXSectionPerAtom(G4double totalEnergy, G4double Z);
private:
G4double ComputeDXSectionPerAtom(G4double eplusEnergy, G4double totalEnergy, G4double Z);
G4double ComputeRelDXSectionPerAtom(G4double eplusEnergy, G4double totalEnergy, G4double Z);
// for creating some data structure per Z with often used comp. intensive data
void InitialiseElementData();
struct ElementData {
G4double fLogZ13;
G4double fCoulomb;
G4double fLradEl;
G4double fDeltaFactor;
G4double fDeltaMax;
G4double fEtaValue;
G4double fLPMVarS1Cond;
G4double fLPMILVarS1Cond;
};
// for precomputing comp. intensive parts of LPM suppression functions and
// using them at run-time
void InitLPMFunctions();
void ComputeLPMGsPhis(G4double &funcGS, G4double &funcPhiS,
const G4double varShat);
void GetLPMFunctions(G4double &lpmGs, G4double &lpmPhis, const G4double sval);
void ComputeLPMfunctions(G4double &fXiS, G4double &fGS, G4double &fPhiS,
const G4double eps, const G4double egamma,
const G4int izet);
struct LPMFuncs {
LPMFuncs() : fIsInitialized(false), fISDelta(100.), fSLimit(2.) {}
G4bool fIsInitialized;
G4double fISDelta;
G4double fSLimit;
std::vector<G4double> fLPMFuncG;
std::vector<G4double> fLPMFuncPhi;
};
private:
// hide assignment operator
G4PairProductionRelModel & operator=
(const G4PairProductionRelModel &right) = delete;
G4PairProductionRelModel(const G4PairProductionRelModel&) = delete;
G4Pow* g4calc;
G4ParticleDefinition* theGamma;
G4ParticleDefinition* theElectron;
G4ParticleDefinition* thePositron;
G4ParticleChangeForGamma* fParticleChange;
G4double fLPMconstant;
G4bool fLPMflag;
// cash
G4double z13, z23, lnZ;
G4double Fel, Finel, fCoulomb;
G4double currentZ;
// LPM effect
G4double lpmEnergy;
G4double xiLPM, phiLPM, gLPM;
// consts
G4bool use_completescreening;
static const G4double xgi[8], wgi[8];
static const G4double Fel_light[5];
static const G4double Finel_light[5];
static const G4double facFel;
static const G4double facFinel;
static const G4double preS1, logTwo, xsfactor, Egsmall, Eghigh;
protected:
static const G4int gMaxZet;
//
static const G4double gLPMconstant;
//
static const G4double gXGL[8];
static const G4double gWGL[8];
static const G4double gFelLowZet[8];
static const G4double gFinelLowZet[8];
//
static const G4double gXSecFactor;
static const G4double gEgLPMActivation;
//
static std::vector<ElementData*> gElementData;
static LPMFuncs gLPMFuncs;
//
G4bool fIsUseLPMCorrection;
G4bool fIsUseCompleteScreening;
//
G4double fLPMEnergy;
//
G4Pow* fG4Calc;
G4ParticleDefinition* fTheGamma;
G4ParticleDefinition* fTheElectron;
G4ParticleDefinition* fThePositron;
G4ParticleChangeForGamma* fParticleChange;
};
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
//
// Bethe screening functions for the elastic (coherent) scattering:
// Bethe's phi1, phi2 coherent screening functions were computed numerically
// by using (the universal) atomic form factors computed based on the Thomas-
// Fermi model of the atom (using numerical solution of the Thomas-Fermi
// screening function instead of Moliere's analytical approximation). The
// numerical results can be well approximated (better than Butcher & Messel
// especially near the delta=1 limit) by:
// ## if delta <= 1.4
// phi1(delta) = 20.806 - delta*(3.190 - 0.5710*delta)
// phi2(delta) = 20.234 - delta*(2.126 - 0.0903*delta)
// ## if delta > 1.4
// phi1(delta) = phi2(delta) = 21.0190 - 4.145*ln(delta + 0.958)
// with delta = 136mc^2kZ^{-1/3}/[E(Eg-E)] = 136Z^{-1/3}eps0/[eps(1-eps)] where
// Eg is the initial photon energy, E is the total energy transferred to one of
// the e-/e+ pair, eps0 = mc^2/Eg and eps = E/Eg.
inline
void G4PairProductionRelModel::SetLPMconstant(G4double val)
void G4PairProductionRelModel::ComputePhi12(const G4double delta, G4double &phi1,
G4double &phi2)
{
fLPMconstant = val;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
inline
G4double G4PairProductionRelModel::LPMconstant() const
{
return fLPMconstant;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
inline
void G4PairProductionRelModel::SetLPMflag(G4bool val)
{
fLPMflag = val;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
inline
G4bool G4PairProductionRelModel::LPMflag() const
{
return fLPMflag;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
inline void G4PairProductionRelModel::SetCurrentElement(G4double Z)
{
if(Z != currentZ) {
currentZ = Z;
G4int iz = G4lrint(Z);
z13 = g4calc->Z13(iz);
z23 = z13*z13;
lnZ = g4calc->logZ(iz);
if (iz <= 4) {
Fel = Fel_light[iz];
Finel = Finel_light[iz] ;
if (delta > 1.4) {
phi1 = 21.0190 - 4.145*G4Log(delta + 0.958);
phi2 = phi1;
} else {
phi1 = 20.806 - delta*(3.190 - 0.5710*delta);
phi2 = 20.234 - delta*(2.126 - 0.0903*delta);
}
else {
Fel = facFel - lnZ/3. ;
Finel = facFinel - 2.*lnZ/3. ;
}
fCoulomb=GetCurrentElement()->GetfCoulomb();
}
// Compute the value of the screening function 3*PHI1(delta) - PHI2(delta):
inline G4double G4PairProductionRelModel::ScreenFunction1(const G4double delta)
{
return (delta > 1.4) ? 42.038 - 8.29*G4Log(delta + 0.958)
: 42.184 - delta*(7.444 - 1.623*delta);
}
// Compute the value of the screening function 1.5*PHI1(delta) +0.5*PHI2(delta):
inline G4double G4PairProductionRelModel::ScreenFunction2(const G4double delta)
{
return (delta > 1.4) ? 42.038 - 8.29*G4Log(delta + 0.958)
: 41.326 - delta*(5.848 - 0.902*delta);
}
// Same as ScreenFunction1 and ScreenFunction2 but computes them at once
inline void G4PairProductionRelModel::ScreenFunction12(const G4double delta,
G4double &f1, G4double &f2)
{
if (delta > 1.4) {
f1 = 42.038 - 8.29*G4Log(delta + 0.958);
f2 = f1;
} else {
f1 = 42.184 - delta*(7.444 - 1.623*delta);
f2 = 41.326 - delta*(5.848 - 0.902*delta);
}
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
inline G4double G4PairProductionRelModel::Phi1(G4double delta) const
{
return (delta > 1.)
? 21.12 - 4.184*G4Log(delta+0.952)
: 20.868 - delta*(3.242 - 0.625*delta);
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
inline G4double G4PairProductionRelModel::Phi2(G4double delta) const
{
return (delta > 1.)
? 21.12 - 4.184*G4Log(delta+0.952)
: 20.209 - delta*(1.930 + 0.086*delta);
}
inline G4double G4PairProductionRelModel::ScreenFunction1(G4double ScreenVariable)
// compute the value of the screening function 3*PHI1 - PHI2
{
return (ScreenVariable > 1.)
? 42.24 - 8.368*G4Log(ScreenVariable+0.952)
: 42.392 - ScreenVariable*(7.796 - 1.961*ScreenVariable);
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
inline G4double G4PairProductionRelModel::ScreenFunction2(G4double ScreenVariable)
// compute the value of the screening function 1.5*PHI1 + 0.5*PHI2
{
return (ScreenVariable > 1.)
? 42.24 - 8.368*G4Log(ScreenVariable+0.952)
: 41.405 - ScreenVariable*(5.828 - 0.8945*ScreenVariable);
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
inline G4double G4PairProductionRelModel::DeltaMax() const
{
// k > 50 MeV
G4double FZ = 8.*(lnZ/3. + fCoulomb);
return G4Exp( (42.24-FZ)/8.368 ) + 0.952;
}
inline G4double G4PairProductionRelModel::DeltaMin(G4double k) const
{
return 544.*CLHEP::electron_mass_c2/(z13*k);
}
#endif
source/processes/electromagnetic/standard/include/G4ScreeningMottCrossSection.hh
+1
View File
@@ -113,6 +113,7 @@ public:
G4double McFcorrection(G4double);
G4double RatioMottRutherford(G4double);
G4double RatioMottRutherfordCosT(G4double);
G4double FormFactor2ExpHof(G4double);
G4double FormFactor2Gauss(G4double);
G4double FormFactor2UniformHelm(G4double);
source/processes/electromagnetic/standard/include/G4WentzelOKandVIxSection.hh
+7 -3
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4WentzelOKandVIxSection.hh 104307 2017-05-24 09:01:45Z gcosmo $
// $Id: G4WentzelOKandVIxSection.hh 109683 2018-05-08 10:36:32Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -67,6 +67,7 @@
#include "G4Threading.hh"
class G4ParticleDefinition;
class G4ScreeningMottCrossSection;
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
@@ -126,6 +127,8 @@ protected:
G4NistManager* fNistManager;
G4Pow* fG4pow;
G4ScreeningMottCrossSection* fMottXSection;
G4ThreeVector temp;
G4double numlimit;
@@ -170,6 +173,7 @@ protected:
G4double factB;
G4double factB1;
G4double factD;
G4double fMottFactor;
G4double gam0pcmp;
G4double pcmp2;
@@ -223,7 +227,7 @@ inline G4double
G4WentzelOKandVIxSection::ComputeNuclearCrossSection(G4double cosTMin,
G4double cosTMax)
{
return targetZ*kinFactor*(cosTMin - cosTMax)/
return targetZ*kinFactor*fMottFactor*(cosTMin - cosTMax)/
((1.0 - cosTMin + screenZ)*(1.0 - cosTMax + screenZ));
}
@@ -235,7 +239,7 @@ G4WentzelOKandVIxSection::ComputeElectronCrossSection(G4double cosTMin,
{
G4double cost1 = std::max(cosTMin,cosTetMaxElec);
G4double cost2 = std::max(cosTMax,cosTetMaxElec);
return (cost1 <= cost2) ? 0.0 : kinFactor*(cost1 - cost2)/
return (cost1 <= cost2) ? 0.0 : kinFactor*fMottFactor*(cost1 - cost2)/
((1.0 - cost1 + screenZ)*(1.0 - cost2 + screenZ));
}
source/processes/electromagnetic/standard/include/G4eBremsstrahlungRelModel.hh
+19 -47
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4eBremsstrahlungRelModel.hh 104373 2017-05-29 09:56:39Z gcosmo $
// $Id: G4eBremsstrahlungRelModel.hh 108737 2018-03-02 13:49:56Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -65,38 +65,38 @@ class G4eBremsstrahlungRelModel : public G4VEmModel
public:
explicit G4eBremsstrahlungRelModel(const G4ParticleDefinition* p = 0,
const G4String& nam = "eBremLPM");
const G4String& nam = "eBremLPM");
virtual ~G4eBremsstrahlungRelModel();
~G4eBremsstrahlungRelModel() = default;
virtual void Initialise(const G4ParticleDefinition*, const G4DataVector&) override;
virtual void InitialiseLocal(const G4ParticleDefinition*,
G4VEmModel* masterModel) override;
G4VEmModel* masterModel) override;
virtual G4double ComputeDEDXPerVolume(const G4Material*,
const G4ParticleDefinition*,
G4double kineticEnergy,
G4double cutEnergy) override;
const G4ParticleDefinition*,
G4double kineticEnergy,
G4double cutEnergy) override;
virtual G4double ComputeCrossSectionPerAtom(const G4ParticleDefinition*,
G4double tkin,
G4double Z, G4double,
G4double cutEnergy,
G4double maxEnergy = DBL_MAX) override;
G4double tkin,
G4double Z, G4double,
G4double cutEnergy,
G4double maxEnergy = DBL_MAX) override;
virtual void SampleSecondaries(std::vector<G4DynamicParticle*>*,
const G4MaterialCutsCouple*,
const G4DynamicParticle*,
G4double cutEnergy,
G4double maxEnergy) override;
const G4MaterialCutsCouple*,
const G4DynamicParticle*,
G4double cutEnergy,
G4double maxEnergy) override;
virtual void SetupForMaterial(const G4ParticleDefinition*,
const G4Material*,G4double) override;
virtual G4double MinPrimaryEnergy(const G4Material*,
const G4ParticleDefinition*,
G4double cut) override;
const G4ParticleDefinition*,
G4double cut) override;
inline void SetLPMconstant(G4double val);
inline G4double LPMconstant() const;
@@ -109,8 +109,7 @@ protected:
virtual G4double ComputeDXSectionPerAtom(G4double gammaEnergy);
// * fast inline functions *
inline void SetCurrentElement(G4int);
void SetCurrentElement(G4int);
private:
@@ -190,33 +189,6 @@ private:
};
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
inline void G4eBremsstrahlungRelModel::SetCurrentElement(G4int Z)
{
if(Z != currentZ) {
currentZ = Z;
z13 = nist->GetZ13(Z);
z23 = z13*z13;
lnZ = nist->GetLOGZ(Z);
if (Z <= 4) {
Fel = Fel_light[Z];
Finel = Finel_light[Z] ;
}
else {
G4double lnzt = lnZ/3.;
Fel = facFel - lnzt;
Finel = facFinel - 2*lnzt;
}
fCoulomb = GetCurrentElement()->GetfCoulomb();
G4double xz = 1.0/(G4double)Z;
fMax = Fel-fCoulomb + Finel*xz + (1. + xz)/12.;
}
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
source/processes/electromagnetic/standard/include/G4eeToTwoGammaModel.hh
+5 -10
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4eeToTwoGammaModel.hh 96934 2016-05-18 09:10:41Z gcosmo $
// $Id: G4eeToTwoGammaModel.hh 109177 2018-04-03 06:55:14Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -70,11 +70,7 @@ public:
virtual void Initialise(const G4ParticleDefinition*,
const G4DataVector&) override;
virtual G4double ComputeCrossSectionPerElectron(
const G4ParticleDefinition*,
G4double kinEnergy,
G4double cutEnergy = 0.,
G4double maxEnergy = DBL_MAX);
virtual G4double ComputeCrossSectionPerElectron(G4double kinEnergy);
virtual G4double ComputeCrossSectionPerAtom(
const G4ParticleDefinition*,
@@ -82,13 +78,13 @@ public:
G4double Z,
G4double A = 0.,
G4double cutEnergy = 0.,
G4double maxEnergy = DBL_MAX) final;
G4double maxEnergy = DBL_MAX) override;
virtual G4double CrossSectionPerVolume(const G4Material*,
const G4ParticleDefinition*,
G4double kineticEnergy,
G4double cutEnergy,
G4double maxEnergy) final;
G4double cutEnergy = 0.0,
G4double maxEnergy = DBL_MAX) override;
virtual void SampleSecondaries(std::vector<G4DynamicParticle*>*,
const G4MaterialCutsCouple*,
@@ -105,7 +101,6 @@ private:
G4double pi_rcl2;
G4ParticleDefinition* theGamma;
G4ParticleChangeForGamma* fParticleChange;
G4bool isInitialised;
};
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
source/processes/electromagnetic/standard/include/G4eplusTo2GammaOKVIModel.hh
+110
View File
@@ -0,0 +1,110 @@
//
// ********************************************************************
// * License and Disclaimer *
// * *
// * The Geant4 software is copyright of the Copyright Holders of *
// * the Geant4 Collaboration. It is provided under the terms and *
// * conditions of the Geant4 Software License, included in the file *
// * LICENSE and available at http://cern.ch/geant4/license . These *
// * include a list of copyright holders. *
// * *
// * Neither the authors of this software system, nor their employing *
// * institutes,nor the agencies providing financial support for this *
// * work make any representation or warranty, express or implied, *
// * regarding this software system or assume any liability for its *
// * use. Please see the license in the file LICENSE and URL above *
// * for the full disclaimer and the limitation of liability. *
// * *
// * This code implementation is the result of the scientific and *
// * technical work of the GEANT4 collaboration. *
// * By using, copying, modifying or distributing the software (or *
// * any work based on the software) you agree to acknowledge its *
// * use in resulting scientific publications, and indicate your *
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4eplusTo2GammaOKVIModel.hh 96909 2016-05-17 10:16:09Z vnivanch $
//
// -------------------------------------------------------------------
//
// GEANT4 Class header file
//
//
// File name: G4eplusTo2GammaOKVIModel
//
// Author: Vladimir Ivanchenko and Omrane Kadri
//
// Creation date: 29.03.2018
//
//
// Class Description:
//
// Implementation of e+ annihilation into 2 gamma
// -------------------------------------------------------------------
//
#ifndef G4eplusTo2GammaOKVIModel_h
#define G4eplusTo2GammaOKVIModel_h 1
#include "G4VEmModel.hh"
class G4eplusTo3GammaOKVIModel;
class G4ParticleChangeForGamma;
class G4PhysicsVector;
class G4eplusTo2GammaOKVIModel : public G4VEmModel
{
public:
explicit G4eplusTo2GammaOKVIModel(const G4ParticleDefinition* p = nullptr,
const G4String& nam = "eplus2ggOKVI");
virtual ~G4eplusTo2GammaOKVIModel();
virtual void Initialise(const G4ParticleDefinition*,
const G4DataVector&) override;
G4double ComputeCrossSectionPerElectron(G4double kinEnergy);
virtual G4double ComputeCrossSectionPerAtom(
const G4ParticleDefinition*,
G4double kinEnergy,
G4double Z,
G4double A = 0.,
G4double cutEnergy = 0.,
G4double maxEnergy = DBL_MAX) final;
virtual G4double CrossSectionPerVolume(const G4Material*,
const G4ParticleDefinition*,
G4double kineticEnergy,
G4double cutEnergy = 0.0,
G4double maxEnergy = DBL_MAX) final;
virtual void SampleSecondaries(std::vector<G4DynamicParticle*>*,
const G4MaterialCutsCouple*,
const G4DynamicParticle*,
G4double tmin = 0.0,
G4double maxEnergy = DBL_MAX) final;
private:
// hide assignment operator
G4eplusTo2GammaOKVIModel & operator=
(const G4eplusTo2GammaOKVIModel &right) = delete;
G4eplusTo2GammaOKVIModel(const G4eplusTo2GammaOKVIModel&) = delete;
G4double pi_rcl2;
G4double energyTh;
G4ParticleDefinition* theGamma;
G4ParticleChangeForGamma* fParticleChange;
G4eplusTo3GammaOKVIModel* f3GModel;
static G4PhysicsVector* fCrossSection;
static G4PhysicsVector* f3GProbability;
};
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
#endif
source/processes/electromagnetic/standard/include/G4eplusTo3GammaOKVIModel.hh
+104
View File
@@ -0,0 +1,104 @@
//
// ********************************************************************
// * License and Disclaimer *
// * *
// * The Geant4 software is copyright of the Copyright Holders of *
// * the Geant4 Collaboration. It is provided under the terms and *
// * conditions of the Geant4 Software License, included in the file *
// * LICENSE and available at http://cern.ch/geant4/license . These *
// * include a list of copyright holders. *
// * *
// * Neither the authors of this software system, nor their employing *
// * institutes,nor the agencies providing financial support for this *
// * work make any representation or warranty, express or implied, *
// * regarding this software system or assume any liability for its *
// * use. Please see the license in the file LICENSE and URL above *
// * for the full disclaimer and the limitation of liability. *
// * *
// * This code implementation is the result of the scientific and *
// * technical work of the GEANT4 collaboration. *
// * By using, copying, modifying or distributing the software (or *
// * any work based on the software) you agree to acknowledge its *
// * use in resulting scientific publications, and indicate your *
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4eplusTo3GammaOKVIModel.hh 96909 2016-05-17 10:16:09Z vnivanch $
//
// -------------------------------------------------------------------
//
// GEANT4 Class header file
//
//
// File name: G4eplusTo3GammaOKVIModel
//
// Author: Vladimir Ivanchenko and Omrane Kadri
//
// Creation date: 29.03.2018
//
//
// Class Description:
//
// Implementation of e+ annihilation into 2 gamma
// -------------------------------------------------------------------
//
#ifndef G4eplusTo3GammaOKVIModel_h
#define G4eplusTo3GammaOKVIModel_h 1
#include "G4VEmModel.hh"
class G4ParticleChangeForGamma;
class G4eplusTo3GammaOKVIModel : public G4VEmModel
{
public:
explicit G4eplusTo3GammaOKVIModel(const G4ParticleDefinition* p = nullptr,
const G4String& nam = "eplus3ggOKVI");
virtual ~G4eplusTo3GammaOKVIModel();
virtual void Initialise(const G4ParticleDefinition*,
const G4DataVector&) final;
G4double ComputeCrossSectionPerElectron(G4double kinEnergy);
virtual G4double ComputeCrossSectionPerAtom(
const G4ParticleDefinition*,
G4double kinEnergy,
G4double Z,
G4double A = 0.,
G4double cutEnergy = 0.,
G4double maxEnergy = DBL_MAX) final;
virtual G4double CrossSectionPerVolume(const G4Material*,
const G4ParticleDefinition*,
G4double kineticEnergy,
G4double cutEnergy = 0.0,
G4double maxEnergy = DBL_MAX) final;
virtual void SampleSecondaries(std::vector<G4DynamicParticle*>*,
const G4MaterialCutsCouple*,
const G4DynamicParticle*,
G4double tmin = 0.0,
G4double maxEnergy = DBL_MAX) final;
private:
// hide assignment operator
G4eplusTo3GammaOKVIModel & operator=
(const G4eplusTo3GammaOKVIModel &right) = delete;
G4eplusTo3GammaOKVIModel(const G4eplusTo3GammaOKVIModel&) = delete;
G4double pi_rcl2;
G4double energyTh;
G4ParticleDefinition* theGamma;
G4ParticleChangeForGamma* fParticleChange;
};
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
#endif
source/processes/electromagnetic/standard/sources.cmake
+15 -1
View File
@@ -11,7 +11,7 @@
#
# Generated on : 24/9/2010
#
# $Id: sources.cmake 106953 2017-10-31 08:30:13Z gcosmo $
# $Id: sources.cmake 109620 2018-05-03 13:01:04Z gcosmo $
#
#------------------------------------------------------------------------------
@@ -46,9 +46,12 @@ include(Geant4MacroDefineModule)
GEANT4_DEFINE_MODULE(NAME G4emstandard
HEADERS
G4ASTARStopping.hh
G4AtimaEnergyLossModel.hh
G4AtimaFluctuations.hh
G4BetheBlochIonGasModel.hh
G4BetheBlochModel.hh
G4BetheHeitlerModel.hh
G4BetheHeitler5DModel.hh
G4BohrFluctuations.hh
G4BraggIonGasModel.hh
G4BraggIonModel.hh
@@ -73,6 +76,8 @@ GEANT4_DEFINE_MODULE(NAME G4emstandard
G4IonFluctuations.hh
G4KleinNishinaCompton.hh
G4KleinNishinaModel.hh
G4LindhardSorensenData.hh
G4LindhardSorensenIonModel.hh
G4ModifiedTsai.hh
G4MollerBhabhaModel.hh
G4MottCoefficients.hh
@@ -109,15 +114,20 @@ GEANT4_DEFINE_MODULE(NAME G4emstandard
G4eSingleCoulombScatteringModel.hh
G4eeToTwoGammaModel.hh
G4eplusAnnihilation.hh
G4eplusTo2GammaOKVIModel.hh
G4eplusTo3GammaOKVIModel.hh
G4hCoulombScatteringModel.hh
G4hIonisation.hh
G4hMultipleScattering.hh
G4ionIonisation.hh
SOURCES
G4ASTARStopping.cc
G4AtimaEnergyLossModel.cc
G4AtimaFluctuations.cc
G4BetheBlochIonGasModel.cc
G4BetheBlochModel.cc
G4BetheHeitlerModel.cc
G4BetheHeitler5DModel.cc
G4BohrFluctuations.cc
G4BraggIonGasModel.cc
G4BraggIonModel.cc
@@ -142,6 +152,8 @@ GEANT4_DEFINE_MODULE(NAME G4emstandard
G4IonFluctuations.cc
G4KleinNishinaCompton.cc
G4KleinNishinaModel.cc
G4LindhardSorensenData.cc
G4LindhardSorensenIonModel.cc
G4ModifiedTsai.cc
G4MollerBhabhaModel.cc
G4MottCoefficients.cc
@@ -177,6 +189,8 @@ GEANT4_DEFINE_MODULE(NAME G4emstandard
G4eSingleCoulombScatteringModel.cc
G4eeToTwoGammaModel.cc
G4eplusAnnihilation.cc
G4eplusTo2GammaOKVIModel.cc
G4eplusTo3GammaOKVIModel.cc
G4hCoulombScatteringModel.cc
G4hIonisation.cc
G4hMultipleScattering.cc
source/processes/electromagnetic/standard/src/G4AtimaEnergyLossModel.cc
+1506
View File
File diff suppressed because it is too large Load Diff
source/processes/electromagnetic/standard/src/G4AtimaFluctuations.cc
+572
View File
@@ -0,0 +1,572 @@
//
// ********************************************************************
// * License and Disclaimer *
// * *
// * The Geant4 software is copyright of the Copyright Holders of *
// * the Geant4 Collaboration. It is provided under the terms and *
// * conditions of the Geant4 Software License, included in the file *
// * LICENSE and available at http://cern.ch/geant4/license . These *
// * include a list of copyright holders. *
// * *
// * Neither the authors of this software system, nor their employing *
// * institutes,nor the agencies providing financial support for this *
// * work make any representation or warranty, express or implied, *
// * regarding this software system or assume any liability for its *
// * use. Please see the license in the file LICENSE and URL above *
// * for the full disclaimer and the limitation of liability. *
// * *
// * This code implementation is the result of the scientific and *
// * technical work of the GEANT4 collaboration. *
// * By using, copying, modifying or distributing the software (or *
// * any work based on the software) you agree to acknowledge its *
// * use in resulting scientific publications, and indicate your *
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// GEANT4 Class header file
//
//
// File name: G4AtimaFluctuations
//
// Author: Jose Luis Rodriguez Sanchez on base of ATIMA code
//
// Creation date: 16.01.2018
//
// Modifications:
//
//
//
// Class Description:
//
// This model calculates the energy-loss fluctuations according to ATIMA code
// developed at GSI, Darmstadt, Germany.
// http://web-docs.gsi.de/~weick/atima/
//
// -------------------------------------------------------------------
//
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
#include "G4AtimaFluctuations.hh"
#include "G4PhysicalConstants.hh"
#include "G4SystemOfUnits.hh"
#include "Randomize.hh"
#include "G4Poisson.hh"
#include "G4MaterialCutsCouple.hh"
#include "G4Material.hh"
#include "G4NistManager.hh"
#include "G4DynamicParticle.hh"
#include "G4Log.hh"
#include "G4Exp.hh"
#include "G4Pow.hh"
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
using namespace std;
G4double G4AtimaFluctuations::stepE = 0.0;
G4double G4AtimaFluctuations::tableE[] = {0.0};
G4AtimaFluctuations::G4AtimaFluctuations(const G4String& nam)
: G4VEmFluctuationModel(nam),
particle(0),
particleMass(CLHEP::proton_mass_c2),
charge(1.0),
chargeSquare(1.0),
effChargeSquare(1.0),
minLoss(0.001*CLHEP::eV)
{
g4calc = G4Pow::GetInstance();
kineticEnergy = 0.0;
beta2 = 0.0;
MLN10 = 2.30258509299;
atomic_mass_unit = 931.4940954; // MeV/c^2
dedx_constant = 0.3070749187; //4*pi*Na*me*c^2*r_e^2 //MeV cm^2
electron_mass = 0.510998928; // MeV/c^2
fine_structure = 1.0/137.035999139;
domega2dx_constant = dedx_constant*electron_mass; //4*pi*Na*me*c^2*r_e^2 //MeV^2 cm^2
if(tableE[0] == 0.0) {
G4double logmin = 0.;
G4double logmax = 5.;
stepE = (logmax-logmin)/(G4double)(199);
for(G4int i=0; i<200; ++i){
tableE[i] = G4Exp(MLN10*(logmin + ((G4double)i)*stepE));
}
}
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4AtimaFluctuations::~G4AtimaFluctuations()
{}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4AtimaFluctuations::InitialiseMe(const G4ParticleDefinition* part)
{
particle = part;
particleMass = part->GetPDGMass();
charge = part->GetPDGCharge()/eplus;
chargeSquare = charge*charge;
effChargeSquare= chargeSquare;
uniFluct.InitialiseMe(part);
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4double
G4AtimaFluctuations::SampleFluctuations(const G4MaterialCutsCouple* couple,
const G4DynamicParticle* dp,
G4double tmax,
G4double length,
G4double meanLoss)
{
// G4cout << "### meanLoss= " << meanLoss << G4endl;
if(meanLoss <= minLoss) return meanLoss;
// G4cout << "G4AtimaFluctuations::SampleFluctuations E(MeV)= "
// << dp->GetKineticEnergy()
// << " Elim(MeV)= " << parameter*charge*particleMass
// << " " << parameter << " " << charge << " " << particleMass << G4endl;
const G4Material* material = couple->GetMaterial();
G4double siga = Dispersion(material,dp,tmax,length);
CLHEP::HepRandomEngine* rndmEngine = G4Random::getTheEngine();
//G4cout << "meanLoss= " << meanLoss << " loss= " << siga << G4endl;
return G4RandGauss::shoot(rndmEngine,meanLoss,std::sqrt(siga));
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4double G4AtimaFluctuations::Dispersion(const G4Material* mat,
const G4DynamicParticle* dp,
G4double,
G4double length)
{
kineticEnergy = dp->GetKineticEnergy();
const G4ParticleDefinition* p = dp->GetDefinition();
G4double ap = p->GetPDGMass()/atomic_mass_unit;
G4double zp = p->GetPDGCharge();
G4double ep = kineticEnergy/ap;// ep in MeV/u
G4double zt = mat->GetIonisation()->GetZeffective();
G4double at = G4NistManager::Instance()->GetAtomicMassAmu(G4lrint(zt));
G4int z = G4lrint(zp);
if(z > 109) { z = 109; }
G4double gamma=1.0 + ep/atomic_mass_unit;
beta2=1.0-1.0/(gamma*gamma);
G4double beta = std::sqrt(beta2);
//z_eff_Pierce_Blann(Z, beta);
G4double zp_eff = zp*(1.0-G4Exp(-0.95*137.035999139*beta/g4calc->Z23(z)));
//
G4double f = domega2dx_constant*zp_eff*zp_eff*zt/at;
//
G4double cor =
24.89 * g4calc->powA(zt,1.2324)/(electron_mass*1e6 * beta2)*
G4Log( 2.0*electron_mass*1e6*beta2/(33.05*g4calc->powA(zt,1.6364)));
cor = std::max(cor, 0.0 );
//Lindhard corrections
if(ep<tableE[0])ep = tableE[0];
G4double da = (ap - element_atomic_weights[z])/element_atomic_weights[z];
G4double v3 = EnergyTable_interpolate(tableE,ep,ls_X_coefficients_a[z-1]);
G4double v4 = EnergyTable_interpolate(tableE,ep,ls_X_coefficients_ahi[z-1]);
G4double dif = v4 - v3;
G4double X = v3+(dif*da/0.05);
X *= gamma*gamma;
//
G4double sse = 0.;
if(ep<30.0){
//Energy straggling Firsov
G4double factor = 4.8184e-3*g4calc->powA(zp+zt,8.0/3.0)/at;
sse = std::min(f*(X+cor), factor*beta2/fine_structure/fine_structure);
}else{
sse = f*(X+cor);
}
//
return sse*length/(cm)*mat->GetDensity()/(g/cm3);
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4AtimaFluctuations::SetParticleAndCharge(const G4ParticleDefinition* part,
G4double q2)
{
if(part != particle) {
particle = part;
particleMass = part->GetPDGMass();
charge = part->GetPDGCharge()/eplus;
chargeSquare = charge*charge;
}
effChargeSquare = q2;
uniFluct.SetParticleAndCharge(part, q2);
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4double G4AtimaFluctuations::EnergyTable_interpolate(const G4double* table, G4double xval,const G4double* y){
G4double r;
G4int num=200;
G4double lxval = G4Log(xval)/MLN10;
if(xval<table[0] || xval>table[num-1])return 0.0;
if(xval==table[num-1])return y[num-1];
G4int i = (G4int)(lxval/stepE);
i = std::min(std::max(i, 0), num-2);
G4double linstep = table[i+1] - table[i];
G4double x = 1.0 - ((xval - table[i])/linstep);
r = (x*y[i]) + ((1-x)*y[i+1]);
return r;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
const G4double G4AtimaFluctuations::element_atomic_weights[110]={
0.0,
1.00794, //H
4.0026, //He
6.941, //Li
9.01218, //Be
10.811, //B
12.0107, //C
14.0067, //N
15.9994, //O
18.9984, //F
20.1797, //Ne
22.9898, //Na
24.305, //Mg
26.9815, //Al
28.0855, //Si
30.9738, //P
32.065, //S
35.453, //Cl
39.948, //Ar
39.0983, //K
40.078, //Ca
44.9559, //Sc
47.867, //Ti
50.9415, //V
51.9961, //Cr
54.938, //Mn
55.845, //Fe
58.9332, //Co
58.6934, //Ni
63.546, //Cu
65.409, //Zn
69.723, //Ga
72.64, //Ge
74.9216, //As
78.96, //Se
79.904, //Br
83.798, //Kr
85.4678, //Rb
87.62, //Sr
88.9059, //Y
91.224, //Zr
92.9064, //Nb
95.94, //Mo
97.9072, //Tc
101.07, //Ru
102.906, //Rh
106.42, //Pd
107.868, //Ag
112.411, //Cd
114.818, //In
118.71, //Sn
121.76, //Sb
127.6, //Te
126.904, //I
131.293, //Xe
132.905, //Cs
137.327, //Ba
138.905, //La
140.116, //Ce
140.908, //Pr
144.24, //Nd
144.913, //Pm
150.36, //Sm
151.964, //Eu
157.25, //Gd
158.925, //Tb
162.5, //Dy
164.93, //Ho
167.259, //Er
168.934, //Tm
173.04, //Yb
174.967, //Lu
178.49, //Hf
180.948, //Ta
183.84, //W
186.207, //Re
190.23, //Os
192.217, //Ir
195.078, //Pt
196.967, //Au
200.59, //Hg
204.383, //Tl
207.2, //Pb
208.98, //Bi
208.982, //Po
209.987, //At
222.018, //Rn
223.02, //Fr
226.025, //Ra
227.028, //Ac
232.038, //Th
231.036, //Pa
238.029, //U
237.048, //Np
244.064, //Pu
243.061, //Am
247.07, //Cm
247.07, //Bk
251.08, //Cf
252.083, //Es
257.095, //Fm
258.098, //Md
259.101, //No
262.11, //Lr
261.109, //Rf
262.114, //Db
266.122, //Sg
264.125, //Bh
269.134, //Hs
268.139 //Mt
};
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
//arrays dimensions are [z][energy], z=1 starts from index=0
//LS X coefficient (dE straggling) for A=atomic weight
const G4double G4AtimaFluctuations::ls_X_coefficients_a[110][200]=
{
{0.999182,0.999124,0.999062,0.998995,0.998925,0.998851,0.998772,0.998688,0.998598,0.998504,0.998404,0.998297,0.998184,0.998064,0.997937,0.997802,0.997659,0.997507,0.997346,0.997175,0.996994,0.996802,0.996598,0.996382,0.996153,0.99591,0.995653,0.995381,0.995092,0.994785,0.994461,0.994117,0.993753,0.993367,0.992958,0.992526,0.992067,0.991582,0.991068,0.990524,0.989948,0.989338,0.988693,0.988011,0.987289,0.986525,0.985717,0.984863,0.98396,0.983005,0.981996,0.98093,0.979804,0.978614,0.977358,0.976032,0.974632,0.973155,0.971597,0.969955,0.968223,0.966397,0.964474,0.962449,0.960317,0.958074,0.955714,0.953233,0.950626,0.947887,0.945012,0.941995,0.938832,0.935516,0.932044,0.928409,0.924608,0.920635,0.916485,0.912155,0.90764,0.902937,0.898042,0.892953,0.887666,0.88218,0.876495,0.870608,0.864522,0.858236,0.851752,0.845074,0.838206,0.831151,0.823917,0.81651,0.808938,0.801211,0.79334,0.785335,0.77721,0.768979,0.760656,0.752258,0.7438,0.735302,0.72678,0.718255,0.709744,0.701267,0.692844,0.684494,0.676236,0.668089,0.660071,0.6522,0.644492,0.636962,0.629625,0.622494,0.61558,0.608894,0.602443,0.596236,0.590278,0.584573,0.579123,0.573929,0.568991,0.564308,0.559877,0.555692,0.55175,0.548044,0.544568,0.541314,0.538274,0.535439,0.532801,0.53035,0.528078,0.525974,0.52403,0.522236,0.520584,0.519064,0.517667,0.516386,0.515211,0.514137,0.513154,0.512256,0.511437,0.510689,0.510008,0.509387,0.508822,0.508306,0.507837,0.507408,0.507018,0.50666,0.506333,0.506032,0.505756,0.5055,0.505262,0.50504,0.504831,0.504632,0.504442,0.504258,0.504078,0.503901,0.503723,0.503542,0.503357,0.503165,0.502964,0.50275,0.502522,0.502277,0.502011,0.501721,0.501403,0.501053,0.500667,0.500239,0.499764,0.499237,0.49865,0.497996,0.497267,0.496453,0.495544,0.494529,0.493396,0.492131,0.490717,0.489139},
{0.999599,0.999546,0.999489,0.999428,0.999363,0.999294,0.999221,0.999143,0.99906,0.998971,0.998877,0.998778,0.998671,0.998558,0.998438,0.998311,0.998175,0.998031,0.997878,0.997716,0.997543,0.99736,0.997165,0.996959,0.99674,0.996507,0.99626,0.995998,0.99572,0.995425,0.995112,0.99478,0.994428,0.994054,0.993659,0.993239,0.992795,0.992323,0.991824,0.991295,0.990734,0.990141,0.989512,0.988846,0.988141,0.987395,0.986606,0.98577,0.984886,0.983951,0.982962,0.981917,0.980812,0.979645,0.978411,0.977108,0.975732,0.974279,0.972746,0.971129,0.969423,0.967625,0.965729,0.963732,0.961629,0.959416,0.957086,0.954636,0.952061,0.949354,0.946512,0.943529,0.940401,0.93712,0.933684,0.930086,0.926322,0.922387,0.918276,0.913985,0.90951,0.904848,0.899994,0.894946,0.889702,0.884259,0.878617,0.872775,0.866733,0.860491,0.854053,0.847421,0.840598,0.833589,0.826401,0.81904,0.811515,0.803834,0.796008,0.78805,0.779971,0.771785,0.763507,0.755154,0.746741,0.738286,0.729807,0.721324,0.712855,0.704419,0.696036,0.687725,0.679505,0.671396,0.663414,0.655578,0.647903,0.640406,0.6331,0.625999,0.619114,0.612455,0.606031,0.599849,0.593915,0.588232,0.582803,0.577629,0.57271,0.568044,0.563629,0.559459,0.555531,0.551838,0.548373,0.54513,0.542099,0.539272,0.536641,0.534197,0.531929,0.52983,0.527889,0.526097,0.524445,0.522924,0.521526,0.520242,0.519064,0.517984,0.516995,0.516089,0.51526,0.514501,0.513807,0.513171,0.512587,0.512052,0.511559,0.511105,0.510685,0.510295,0.509931,0.509589,0.509265,0.508957,0.508661,0.508372,0.508089,0.507808,0.507525,0.507238,0.506942,0.506634,0.50631,0.505967,0.505599,0.505203,0.504773,0.504304,0.503789,0.503224,0.502599,0.501908,0.501142,0.500292,0.499346,0.498293,0.497121,0.495814,0.494358,0.492735,0.490925,0.488909,0.486663,0.484161,0.481378,0.478282,0.474842,0.471024},
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{1.01181,1.01255,1.01332,1.01414,1.015,1.01591,1.01686,1.01787,1.01893,1.02005,1.02123,1.02247,1.02379,1.02517,1.02663,1.02817,1.0298,1.03151,1.03332,1.03523,1.03724,1.03936,1.0416,1.04396,1.04646,1.04908,1.05186,1.05478,1.05786,1.0611,1.06452,1.06813,1.07193,1.07592,1.08014,1.08457,1.08924,1.09415,1.09931,1.10474,1.11045,1.11644,1.12274,1.12935,1.13629,1.14356,1.15119,1.15918,1.16754,1.1763,1.18545,1.19502,1.20501,1.21543,1.2263,1.23762,1.24941,1.26166,1.2744,1.28762,1.30132,1.31552,1.33021,1.34539,1.36106,1.37722,1.39386,1.41098,1.42855,1.44658,1.46504,1.48393,1.50321,1.52286,1.54287,1.56321,1.58384,1.60473,1.62585,1.64715,1.66861,1.69018,1.71181,1.73346,1.75508,1.77663,1.79805,1.81929,1.84031,1.86106,1.88147,1.90151,1.92113,1.94027,1.9589,1.97697,1.99444,2.01127,2.02743,2.04288,2.05761,2.07159,2.08479,2.09722,2.10884,2.11967,2.1297,2.13893,2.14738,2.15504,2.16194,2.1681,2.17353,2.17826,2.18232,2.18573,2.18852,2.19072,2.19236,2.19346,2.19407,2.19419,2.19387,2.19312,2.19198,2.19045,2.18855,2.18631,2.18374,2.18084,2.17763,2.1741,2.17027,2.16612,2.16166,2.15688,2.15178,2.14633,2.14053,2.13435,2.12779,2.12082,2.11341,2.10555,2.09719,2.08832,2.07891,2.06891,2.05829,2.04701,2.03505,2.02234,2.00886,1.99455,1.97938,1.96329,1.94623,1.92816,1.90903,1.88877,1.86736,1.84472,1.82082,1.79559,1.76901,1.74101,1.71157,1.68063,1.64817,1.61417,1.5786,1.54146,1.50275,1.46248,1.42069,1.3774,1.3327,1.28666,1.23938,1.191,1.14165,1.09151,1.04079,0.989695,0.938475,0.887385,0.836697,0.786688,0.737636,0.689807,0.643452,0.598791,0.556011,0.515254,0.476615,0.440142,0.405835,0.373654,0.343529,0.315373},
{1.01163,1.01236,1.01312,1.01393,1.01478,1.01567,1.01662,1.01761,1.01866,1.01976,1.02093,1.02215,1.02345,1.02481,1.02626,1.02778,1.02938,1.03107,1.03286,1.03474,1.03673,1.03882,1.04104,1.04337,1.04583,1.04843,1.05116,1.05405,1.0571,1.0603,1.06369,1.06725,1.07101,1.07497,1.07914,1.08353,1.08815,1.09301,1.09813,1.10352,1.10918,1.11513,1.12138,1.12795,1.13484,1.14207,1.14966,1.15761,1.16594,1.17466,1.18379,1.19333,1.2033,1.21371,1.22457,1.2359,1.24769,1.25997,1.27273,1.28599,1.29975,1.31401,1.32878,1.34405,1.35984,1.37612,1.39291,1.41019,1.42795,1.44619,1.46488,1.48401,1.50357,1.52353,1.54387,1.56456,1.58556,1.60686,1.62841,1.65018,1.67212,1.69421,1.71638,1.7386,1.76081,1.78298,1.80504,1.82695,1.84866,1.87011,1.89126,1.91205,1.93242,1.95234,1.97176,1.99062,2.00889,2.02653,2.0435,2.05977,2.0753,2.09008,2.10409,2.1173,2.1297,2.14129,2.15207,2.16203,2.17118,2.17954,2.1871,2.1939,2.19995,2.20527,2.2099,2.21384,2.21714,2.21981,2.2219,2.22342,2.22441,2.2249,2.22491,2.22446,2.22358,2.22229,2.22061,2.21856,2.21614,2.21337,2.21026,2.20681,2.20303,2.19891,2.19445,2.18965,2.1845,2.17898,2.17308,2.1668,2.1601,2.15296,2.14537,2.1373,2.12873,2.11961,2.10992,2.09963,2.0887,2.0771,2.06478,2.0517,2.03782,2.0231,2.00749,1.99094,1.9734,1.95483,1.93517,1.91438,1.8924,1.86918,1.84467,1.81883,1.7916,1.76294,1.73281,1.70117,1.668,1.63326,1.59695,1.55905,1.51956,1.47851,1.43593,1.39186,1.34636,1.29953,1.25147,1.20231,1.15221,1.10134,1.0499,0.998117,0.946241,0.89453,0.843259,0.792708,0.743155,0.694867,0.648094,0.603053,0.559929,0.518859,0.479935,0.443201,0.40865,0.376241,0.345902,0.317543},
{1.01145,1.01216,1.01292,1.01372,1.01455,1.01544,1.01637,1.01735,1.01838,1.01947,1.02062,1.02183,1.0231,1.02445,1.02587,1.02737,1.02895,1.03062,1.03238,1.03424,1.0362,1.03827,1.04045,1.04275,1.04518,1.04775,1.05045,1.0533,1.05631,1.05948,1.06282,1.06634,1.07006,1.07397,1.07809,1.08244,1.08701,1.09183,1.0969,1.10223,1.10784,1.11374,1.11994,1.12646,1.1333,1.14048,1.14802,1.15593,1.16421,1.1729,1.18198,1.19149,1.20144,1.21182,1.22267,1.23398,1.24578,1.25806,1.27084,1.28412,1.29792,1.31223,1.32707,1.34242,1.3583,1.3747,1.39162,1.40905,1.42698,1.4454,1.46431,1.48368,1.5035,1.52374,1.54439,1.56542,1.58679,1.60848,1.63045,1.65266,1.67508,1.69767,1.72037,1.74315,1.76595,1.78872,1.81142,1.834,1.85639,1.87854,1.90041,1.92194,1.94308,1.96378,1.98398,2.00364,2.02272,2.04117,2.05896,2.07604,2.0924,2.10799,2.1228,2.13681,2.15,2.16237,2.17391,2.18461,2.19449,2.20354,2.21179,2.21924,2.22592,2.23185,2.23704,2.24153,2.24535,2.24851,2.25105,2.253,2.25439,2.25524,2.25558,2.25543,2.25482,2.25378,2.25231,2.25044,2.24817,2.24553,2.24251,2.23913,2.23539,2.23128,2.22681,2.22197,2.21675,2.21115,2.20513,2.19871,2.19184,2.18452,2.17672,2.16841,2.15957,2.15017,2.14017,2.12955,2.11827,2.10628,2.09356,2.08006,2.06573,2.05053,2.03442,2.01735,1.99927,1.98013,1.95987,1.93846,1.91584,1.89195,1.86675,1.84019,1.81223,1.78281,1.7519,1.71947,1.68547,1.6499,1.61274,1.57397,1.53362,1.49169,1.44822,1.40327,1.35689,1.30919,1.26028,1.21028,1.15937,1.10772,1.05554,1.00307,0.950546,0.898241,0.846433,0.795403,0.745431,0.696782,0.649704,0.604409,0.561076,0.519837,0.480774,0.443923,0.409272,0.376775,0.346354,0.317918},
{1.01126,1.01197,1.01271,1.0135,1.01432,1.01519,1.01611,1.01707,1.01809,1.01916,1.0203,1.02149,1.02275,1.02407,1.02547,1.02695,1.02851,1.03016,1.03189,1.03372,1.03565,1.03769,1.03985,1.04212,1.04451,1.04704,1.0497,1.05252,1.05548,1.05861,1.06191,1.06539,1.06906,1.07292,1.077,1.08129,1.08581,1.09058,1.09559,1.10087,1.10642,1.11227,1.11841,1.12487,1.13166,1.13879,1.14627,1.15412,1.16236,1.17099,1.18003,1.1895,1.19941,1.20976,1.22058,1.23187,1.24365,1.25593,1.26871,1.28201,1.29583,1.31018,1.32507,1.34049,1.35645,1.37294,1.38998,1.40754,1.42563,1.44423,1.46333,1.48293,1.50299,1.52351,1.54445,1.5658,1.58752,1.60959,1.63197,1.65462,1.67751,1.70059,1.72382,1.74714,1.77053,1.79391,1.81725,1.84048,1.86356,1.88642,1.90902,1.9313,1.95321,1.97469,1.9957,2.01617,2.03607,2.05535,2.07398,2.0919,2.10909,2.12552,2.14117,2.156,2.17001,2.18318,2.1955,2.20698,2.21761,2.2274,2.23636,2.2445,2.25184,2.2584,2.26421,2.26928,2.27365,2.27733,2.28037,2.28278,2.28459,2.28584,2.28655,2.28675,2.28645,2.28568,2.28446,2.28281,2.28074,2.27826,2.27538,2.27211,2.26845,2.26441,2.25997,2.25514,2.24991,2.24426,2.23819,2.23168,2.22472,2.21727,2.20932,2.20085,2.19183,2.18222,2.172,2.16113,2.14959,2.13732,2.1243,2.11048,2.09581,2.08026,2.06378,2.04632,2.02783,2.00826,1.98756,1.96569,1.94259,1.91821,1.89249,1.8654,1.83689,1.8069,1.77541,1.74238,1.70778,1.67158,1.63377,1.59435,1.55332,1.51071,1.46656,1.4209,1.37383,1.32542,1.27579,1.22509,1.17347,1.12112,1.06825,1.01509,0.961903,0.90895,0.856513,0.804876,0.75432,0.705112,0.6575,0.611697,0.56788,0.526181,0.486681,0.449415,0.41437,0.381498,0.350721,0.321949},
{1.01107,1.01176,1.0125,1.01327,1.01409,1.01494,1.01585,1.0168,1.0178,1.01886,1.01997,1.02115,1.02238,1.02369,1.02507,1.02653,1.02806,1.02968,1.03139,1.03319,1.0351,1.03711,1.03922,1.04146,1.04382,1.04631,1.04894,1.05171,1.05464,1.05772,1.06098,1.06441,1.06803,1.07184,1.07586,1.0801,1.08457,1.08928,1.09423,1.09945,1.10495,1.11073,1.11681,1.12321,1.12993,1.137,1.14442,1.15221,1.16039,1.16896,1.17795,1.18736,1.19722,1.20753,1.21831,1.22957,1.24132,1.25358,1.26635,1.27965,1.29348,1.30785,1.32277,1.33824,1.35426,1.37084,1.38797,1.40565,1.42387,1.44263,1.46191,1.48171,1.502,1.52277,1.54399,1.56564,1.5877,1.61012,1.63289,1.65596,1.6793,1.70285,1.72658,1.75045,1.7744,1.79837,1.82233,1.84621,1.86996,1.89352,1.91684,1.93986,1.96253,1.98479,2.00659,2.02787,2.04859,2.0687,2.08816,2.10692,2.12495,2.14222,2.15869,2.17435,2.18918,2.20315,2.21627,2.22852,2.23991,2.25043,2.26011,2.26894,2.27695,2.28415,2.29056,2.29622,2.30113,2.30534,2.30886,2.31173,2.31397,2.31561,2.31668,2.3172,2.3172,2.3167,2.31571,2.31426,2.31235,2.31001,2.30724,2.30405,2.30044,2.29642,2.29198,2.28711,2.28182,2.27608,2.2699,2.26325,2.25611,2.24847,2.24031,2.23159,2.2223,2.2124,2.20186,2.19065,2.17874,2.16609,2.15265,2.13838,2.12325,2.10721,2.09022,2.07222,2.05316,2.033,2.01169,1.98918,1.96541,1.94034,1.91391,1.88608,1.8568,1.82603,1.79374,1.75988,1.72442,1.68736,1.64867,1.60835,1.56642,1.5229,1.47783,1.43126,1.38328,1.33398,1.28348,1.23192,1.17948,1.12635,1.07273,1.01888,0.965058,0.911526,0.858573,0.806486,0.755544,0.706013,0.658139,0.612127,0.568149,0.526327,0.486735,0.449399,0.414298,0.38138,0.350562,0.321751}
};
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
//LS X coefficient for A=atomic weight * 1.05
const G4double G4AtimaFluctuations::ls_X_coefficients_ahi[110][200]=
{
{0.999182,0.999124,0.999062,0.998995,0.998925,0.998851,0.998772,0.998688,0.998598,0.998504,0.998404,0.998297,0.998184,0.998064,0.997937,0.997802,0.997659,0.997507,0.997346,0.997175,0.996994,0.996802,0.996598,0.996382,0.996153,0.99591,0.995653,0.995381,0.995092,0.994785,0.994461,0.994117,0.993753,0.993367,0.992958,0.992526,0.992067,0.991582,0.991068,0.990524,0.989948,0.989338,0.988693,0.988011,0.987289,0.986525,0.985717,0.984863,0.98396,0.983005,0.981996,0.98093,0.979804,0.978614,0.977358,0.976032,0.974632,0.973155,0.971597,0.969955,0.968223,0.966397,0.964474,0.962449,0.960317,0.958074,0.955714,0.953233,0.950626,0.947887,0.945012,0.941995,0.938832,0.935516,0.932044,0.928409,0.924608,0.920635,0.916485,0.912155,0.90764,0.902937,0.898042,0.892952,0.887666,0.88218,0.876495,0.870608,0.864522,0.858236,0.851752,0.845074,0.838206,0.831151,0.823917,0.81651,0.808938,0.801211,0.79334,0.785335,0.77721,0.768979,0.760656,0.752258,0.7438,0.735302,0.72678,0.718255,0.709743,0.701267,0.692844,0.684494,0.676236,0.668089,0.660071,0.6522,0.644492,0.636962,0.629625,0.622494,0.61558,0.608893,0.602443,0.596236,0.590278,0.584572,0.579122,0.573929,0.568991,0.564308,0.559876,0.555692,0.55175,0.548044,0.544568,0.541314,0.538273,0.535438,0.5328,0.53035,0.528077,0.525973,0.524029,0.522235,0.520583,0.519062,0.517665,0.516384,0.515209,0.514135,0.513152,0.512254,0.511434,0.510686,0.510005,0.509383,0.508817,0.508302,0.507831,0.507403,0.507011,0.506653,0.506325,0.506024,0.505746,0.505489,0.50525,0.505026,0.504815,0.504615,0.504423,0.504237,0.504055,0.503874,0.503693,0.503509,0.50332,0.503124,0.502918,0.502699,0.502465,0.502213,0.501939,0.501641,0.501313,0.500953,0.500554,0.500113,0.499624,0.49908,0.498474,0.4978,0.497047,0.496207,0.495269,0.494222,0.493052,0.491747,0.490288,0.48866},
{0.999599,0.999546,0.999489,0.999428,0.999363,0.999294,0.999221,0.999143,0.99906,0.998971,0.998877,0.998778,0.998671,0.998558,0.998438,0.998311,0.998175,0.998031,0.997878,0.997716,0.997543,0.99736,0.997165,0.996959,0.99674,0.996507,0.99626,0.995998,0.99572,0.995425,0.995112,0.99478,0.994428,0.994054,0.993659,0.993239,0.992795,0.992323,0.991824,0.991295,0.990734,0.990141,0.989512,0.988846,0.988141,0.987395,0.986605,0.98577,0.984886,0.983951,0.982962,0.981917,0.980812,0.979644,0.978411,0.977108,0.975732,0.974279,0.972746,0.971129,0.969423,0.967625,0.965729,0.963732,0.961629,0.959416,0.957086,0.954636,0.95206,0.949354,0.946512,0.943529,0.9404,0.93712,0.933684,0.930086,0.926322,0.922387,0.918276,0.913985,0.90951,0.904848,0.899994,0.894946,0.889702,0.884259,0.878617,0.872775,0.866732,0.860491,0.854053,0.847421,0.840598,0.833589,0.826401,0.81904,0.811514,0.803834,0.796008,0.78805,0.77997,0.771785,0.763507,0.755153,0.74674,0.738286,0.729807,0.721324,0.712855,0.704419,0.696036,0.687725,0.679505,0.671395,0.663414,0.655577,0.647903,0.640406,0.6331,0.625999,0.619114,0.612455,0.606031,0.599848,0.593914,0.588231,0.582802,0.577628,0.572709,0.568043,0.563628,0.559458,0.55553,0.551837,0.548372,0.545128,0.542097,0.539271,0.536639,0.534195,0.531927,0.529827,0.527886,0.526094,0.524442,0.522921,0.521522,0.520238,0.519059,0.517979,0.516989,0.516083,0.515253,0.514493,0.513798,0.513161,0.512576,0.51204,0.511546,0.51109,0.510669,0.510277,0.50991,0.509566,0.50924,0.508929,0.508629,0.508337,0.50805,0.507765,0.507477,0.507184,0.506881,0.506566,0.506235,0.505883,0.505505,0.505098,0.504656,0.504173,0.503643,0.50306,0.502417,0.501704,0.500915,0.500037,0.499061,0.497975,0.496766,0.495418,0.493916,0.492242,0.490376,0.488297,0.485981,0.483402,0.480533,0.477343,0.4738,0.469868},
{1.00017,1.00012,1.00007,1.00002,0.999959,0.999897,0.99983,0.999759,0.999682,0.999601,0.999514,0.999421,0.999322,0.999217,0.999104,0.998984,0.998857,0.998721,0.998576,0.998422,0.998258,0.998083,0.997898,0.997701,0.997491,0.997268,0.997031,0.996779,0.996512,0.996228,0.995926,0.995606,0.995266,0.994905,0.994522,0.994115,0.993684,0.993226,0.992741,0.992226,0.991681,0.991103,0.99049,0.98984,0.989152,0.988423,0.987652,0.986834,0.985969,0.985054,0.984085,0.98306,0.981976,0.98083,0.979618,0.978338,0.976985,0.975557,0.974048,0.972456,0.970776,0.969004,0.967136,0.965167,0.963092,0.960907,0.958608,0.956188,0.953644,0.95097,0.94816,0.945211,0.942116,0.938871,0.935469,0.931908,0.92818,0.924283,0.92021,0.915958,0.911523,0.9069,0.902087,0.897081,0.891878,0.886478,0.880878,0.875079,0.869081,0.862884,0.85649,0.849902,0.843124,0.836161,0.829018,0.821702,0.814222,0.806587,0.798807,0.790893,0.782859,0.774718,0.766485,0.758175,0.749806,0.741394,0.732958,0.724516,0.716087,0.707692,0.699348,0.691075,0.682893,0.67482,0.666873,0.659071,0.65143,0.643965,0.63669,0.629618,0.622761,0.616129,0.609731,0.603573,0.597662,0.592001,0.586593,0.581439,0.576538,0.571889,0.56749,0.563335,0.559421,0.55574,0.552287,0.549053,0.546032,0.543214,0.54059,0.538152,0.53589,0.533794,0.531857,0.530067,0.528417,0.526896,0.525498,0.524212,0.523031,0.521947,0.520952,0.520039,0.519202,0.518434,0.517728,0.517079,0.51648,0.515928,0.515415,0.514939,0.514494,0.514075,0.513679,0.513301,0.512937,0.512583,0.512236,0.511891,0.511544,0.511191,0.510828,0.510451,0.510054,0.509634,0.509185,0.508701,0.508176,0.507604,0.506978,0.506289,0.50553,0.50469,0.50376,0.502728,0.501582,0.500307,0.498889,0.49731,0.495552,0.493595,0.491416,0.488992,0.486294,0.483295,0.479964,0.476266,0.472165,0.467623,0.4626,0.457054},
{1.00086,1.00082,1.00078,1.00073,1.00069,1.00063,1.00058,1.00051,1.00045,1.00038,1.0003,1.00021,1.00012,1.00003,0.999924,0.999813,0.999695,0.999568,0.999433,0.999288,0.999134,0.998969,0.998793,0.998606,0.998406,0.998193,0.997967,0.997726,0.997469,0.997196,0.996906,0.996598,0.996269,0.995921,0.99555,0.995157,0.994739,0.994295,0.993823,0.993323,0.992793,0.99223,0.991632,0.990999,0.990327,0.989615,0.988861,0.988062,0.987215,0.986318,0.985369,0.984364,0.983301,0.982176,0.980986,0.979728,0.978398,0.976993,0.975508,0.973941,0.972286,0.97054,0.968699,0.966757,0.96471,0.962554,0.960284,0.957895,0.955381,0.952738,0.949961,0.947044,0.943983,0.940771,0.937405,0.933879,0.930188,0.926327,0.922292,0.918078,0.913682,0.909099,0.904325,0.899359,0.894198,0.888839,0.883282,0.877525,0.87157,0.865416,0.859066,0.852522,0.845788,0.838869,0.831771,0.8245,0.817065,0.809474,0.801738,0.793869,0.785879,0.777782,0.769592,0.761326,0.752999,0.744629,0.736235,0.727834,0.719445,0.711089,0.702784,0.694549,0.686403,0.678365,0.670453,0.662685,0.655076,0.647642,0.640397,0.633354,0.626525,0.61992,0.613547,0.607413,0.601525,0.595886,0.590498,0.585363,0.580481,0.575849,0.571465,0.567325,0.563425,0.559757,0.556315,0.553093,0.550081,0.547272,0.544656,0.542225,0.539969,0.537879,0.535946,0.53416,0.532512,0.530994,0.529596,0.528311,0.527129,0.526044,0.525047,0.524131,0.52329,0.522516,0.521804,0.521147,0.520539,0.519976,0.519452,0.518962,0.518501,0.518064,0.517648,0.517247,0.516857,0.516475,0.516095,0.515713,0.515325,0.514927,0.514513,0.514078,0.513618,0.513126,0.512597,0.512023,0.511399,0.510715,0.509964,0.509136,0.508222,0.507209,0.506086,0.504839,0.503454,0.501913,0.500199,0.498292,0.49617,0.493809,0.491184,0.488265,0.485024,0.481427,0.477438,0.473019,0.468131,0.462732,0.456779,0.450227},
{1.00162,1.0016,1.00157,1.00154,1.00151,1.00147,1.00143,1.00138,1.00132,1.00127,1.0012,1.00113,1.00105,1.00097,1.00088,1.00078,1.00067,1.00056,1.00043,1.0003,1.00016,1,0.99984,0.999664,0.999476,0.999275,0.99906,0.998831,0.998587,0.998326,0.998048,0.997752,0.997436,0.997101,0.996743,0.996363,0.995959,0.995529,0.995072,0.994586,0.99407,0.993523,0.992941,0.992324,0.991668,0.990973,0.990236,0.989455,0.988626,0.987748,0.986818,0.985833,0.98479,0.983685,0.982517,0.981281,0.979973,0.978591,0.977131,0.975587,0.973958,0.972237,0.970422,0.968507,0.966488,0.96436,0.962118,0.959758,0.957275,0.954663,0.951917,0.949033,0.946004,0.942827,0.939495,0.936003,0.932348,0.928523,0.924525,0.920349,0.91599,0.911446,0.906712,0.901786,0.896665,0.891347,0.885831,0.880116,0.874203,0.868092,0.861784,0.855284,0.848593,0.841718,0.834663,0.827436,0.820045,0.812498,0.804806,0.79698,0.789033,0.780979,0.772832,0.764608,0.756323,0.747994,0.73964,0.731279,0.72293,0.714612,0.706344,0.698146,0.690036,0.682033,0.674155,0.66642,0.658842,0.651439,0.644223,0.637209,0.630407,0.623827,0.617479,0.611369,0.605503,0.599885,0.594517,0.589401,0.584536,0.579921,0.575553,0.571428,0.567541,0.563885,0.560455,0.557243,0.554241,0.551441,0.548833,0.546409,0.544159,0.542074,0.540146,0.538364,0.536719,0.535203,0.533807,0.532522,0.531341,0.530255,0.529256,0.528337,0.527493,0.526714,0.525996,0.525333,0.524718,0.524145,0.52361,0.523108,0.522633,0.522181,0.521747,0.521326,0.520914,0.520506,0.520098,0.519685,0.519261,0.518823,0.518364,0.517879,0.517363,0.516808,0.516209,0.515557,0.514845,0.514064,0.513204,0.512255,0.511206,0.510043,0.508752,0.507319,0.505727,0.503956,0.501987,0.499797,0.497363,0.494656,0.49165,0.488312,0.484609,0.480505,0.475962,0.47094,0.465395,0.459285,0.452567,0.445192},
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{1.01181,1.01255,1.01333,1.01414,1.015,1.01591,1.01687,1.01787,1.01893,1.02005,1.02123,1.02248,1.02379,1.02517,1.02663,1.02817,1.0298,1.03151,1.03332,1.03523,1.03724,1.03937,1.04161,1.04397,1.04646,1.04909,1.05186,1.05478,1.05786,1.06111,1.06453,1.06814,1.07193,1.07593,1.08014,1.08458,1.08924,1.09415,1.09932,1.10475,1.11046,1.11645,1.12275,1.12936,1.1363,1.14357,1.1512,1.15919,1.16755,1.17631,1.18546,1.19503,1.20502,1.21544,1.22631,1.23763,1.24941,1.26167,1.2744,1.28762,1.30132,1.31552,1.33021,1.34539,1.36106,1.37721,1.39385,1.41096,1.42854,1.44656,1.46502,1.4839,1.50317,1.52283,1.54283,1.56316,1.58378,1.60467,1.62578,1.64708,1.66853,1.69009,1.71171,1.73335,1.75496,1.7765,1.79791,1.81914,1.84015,1.86088,1.88128,1.90131,1.92091,1.94004,1.95866,1.97671,1.99416,2.01097,2.02712,2.04256,2.05726,2.07122,2.08441,2.09681,2.10842,2.11923,2.12923,2.13844,2.14686,2.1545,2.16138,2.16751,2.17291,2.17762,2.18164,2.18502,2.18778,2.18994,2.19155,2.19262,2.19318,2.19327,2.1929,2.19211,2.19092,2.18934,2.18739,2.18509,2.18246,2.1795,2.17622,2.17263,2.16872,2.16449,2.15995,2.15509,2.14988,2.14434,2.13843,2.13215,2.12547,2.11837,2.11083,2.10282,2.09432,2.08529,2.07571,2.06553,2.05472,2.04325,2.03107,2.01815,2.00443,1.98988,1.97445,1.95809,1.94075,1.92238,1.90293,1.88236,1.8606,1.83761,1.81334,1.78774,1.76076,1.73237,1.70251,1.67115,1.63827,1.60383,1.56783,1.53025,1.49111,1.45041,1.4082,1.36453,1.31945,1.27306,1.22547,1.17682,1.12724,1.07694,1.0261,0.974969,0.923777,0.872791,0.822286,0.772538,0.723823,0.676404,0.630523,0.586392,0.544186,0.504034,0.466016,0.430168,0.396476,0.364894,0.335341,0.30773},
{1.01163,1.01236,1.01313,1.01393,1.01478,1.01568,1.01662,1.01761,1.01866,1.01976,1.02093,1.02216,1.02345,1.02482,1.02626,1.02778,1.02938,1.03108,1.03286,1.03474,1.03673,1.03883,1.04104,1.04337,1.04584,1.04843,1.05117,1.05406,1.0571,1.06031,1.06369,1.06726,1.07102,1.07498,1.07915,1.08354,1.08816,1.09302,1.09814,1.10353,1.10919,1.11514,1.12139,1.12796,1.13485,1.14208,1.14967,1.15762,1.16595,1.17467,1.1838,1.19334,1.20331,1.21372,1.22458,1.23591,1.2477,1.25998,1.27274,1.28599,1.29975,1.31401,1.32878,1.34405,1.35983,1.37612,1.3929,1.41018,1.42794,1.44617,1.46486,1.48399,1.50354,1.5235,1.54383,1.56451,1.58551,1.6068,1.62835,1.65011,1.67204,1.69412,1.71628,1.73849,1.76069,1.78285,1.8049,1.8268,1.8485,1.86994,1.89107,1.91184,1.9322,1.95211,1.9715,1.99035,2.00861,2.02623,2.04318,2.05943,2.07494,2.0897,2.10369,2.11687,2.12926,2.14083,2.15158,2.16151,2.17064,2.17897,2.18651,2.19328,2.1993,2.2046,2.20918,2.2131,2.21636,2.219,2.22105,2.22254,2.22349,2.22393,2.22389,2.2234,2.22247,2.22113,2.2194,2.21728,2.2148,2.21197,2.20879,2.20527,2.20141,2.19721,2.19267,2.18778,2.18253,2.17691,2.17091,2.1645,2.15768,2.15042,2.14269,2.13448,2.12575,2.11647,2.10661,2.09614,2.08502,2.07321,2.06067,2.04737,2.03325,2.01828,2.00241,1.98558,1.96776,1.94889,1.92891,1.90779,1.88546,1.86189,1.83701,1.81078,1.78315,1.75409,1.72354,1.69148,1.65787,1.6227,1.58595,1.54761,1.50769,1.46621,1.42322,1.37875,1.33288,1.28571,1.23734,1.18791,1.13759,1.08655,1.03501,0.983198,0.931361,0.879765,0.828689,0.778411,0.729207,0.68134,0.635053,0.590552,0.548011,0.507555,0.469259,0.433155,0.399225,0.367419,0.337656,0.309845},
{1.01145,1.01217,1.01292,1.01372,1.01456,1.01544,1.01637,1.01735,1.01838,1.01947,1.02062,1.02183,1.02311,1.02445,1.02588,1.02737,1.02896,1.03063,1.03239,1.03425,1.03621,1.03827,1.04046,1.04276,1.04519,1.04775,1.05046,1.05331,1.05631,1.05948,1.06283,1.06635,1.07007,1.07398,1.0781,1.08245,1.08702,1.09184,1.09691,1.10224,1.10785,1.11375,1.11995,1.12647,1.13331,1.1405,1.14804,1.15594,1.16423,1.17291,1.182,1.19151,1.20145,1.21184,1.22268,1.234,1.24579,1.25807,1.27085,1.28413,1.29793,1.31224,1.32707,1.34243,1.3583,1.3747,1.39161,1.40904,1.42697,1.44539,1.46429,1.48366,1.50347,1.52371,1.54436,1.56537,1.58674,1.60842,1.63038,1.65259,1.675,1.69758,1.72027,1.74304,1.76583,1.78859,1.81128,1.83384,1.85622,1.87836,1.90022,1.92173,1.94286,1.96353,1.98372,2.00337,2.02243,2.04086,2.05863,2.07569,2.09202,2.1076,2.12238,2.13637,2.14954,2.16188,2.17339,2.18407,2.19392,2.20295,2.21117,2.21859,2.22524,2.23113,2.2363,2.24075,2.24453,2.24766,2.25016,2.25207,2.25341,2.25422,2.25451,2.25432,2.25366,2.25256,2.25103,2.2491,2.24677,2.24406,2.24097,2.23752,2.2337,2.22951,2.22495,2.22001,2.2147,2.20898,2.20286,2.19631,2.18932,2.18187,2.17392,2.16547,2.15647,2.1469,2.13673,2.12592,2.11444,2.10225,2.08931,2.07557,2.061,2.04555,2.02917,2.01182,1.99344,1.97399,1.95342,1.93167,1.9087,1.88445,1.85887,1.83192,1.80356,1.77373,1.7424,1.70953,1.6751,1.63909,1.60148,1.56228,1.52149,1.47913,1.43525,1.3899,1.34316,1.29512,1.2459,1.19565,1.14452,1.09272,1.04045,0.987958,0.93549,0.883316,0.831719,0.78098,0.731374,0.683162,0.636585,0.591845,0.549107,0.50849,0.470063,0.433848,0.399821,0.367928,0.338085,0.310199},
{1.01126,1.01197,1.01271,1.0135,1.01432,1.01519,1.01611,1.01708,1.01809,1.01917,1.0203,1.02149,1.02275,1.02408,1.02548,1.02696,1.02852,1.03016,1.0319,1.03373,1.03566,1.0377,1.03985,1.04212,1.04452,1.04705,1.04971,1.05253,1.05549,1.05862,1.06192,1.0654,1.06907,1.07294,1.07701,1.0813,1.08583,1.09059,1.0956,1.10088,1.10644,1.11228,1.11843,1.12489,1.13167,1.1388,1.14629,1.15414,1.16238,1.17101,1.18005,1.18952,1.19942,1.20978,1.22059,1.23189,1.24367,1.25594,1.26872,1.28202,1.29584,1.31019,1.32507,1.34049,1.35645,1.37295,1.38998,1.40754,1.42562,1.44422,1.46332,1.48291,1.50297,1.52348,1.54442,1.56576,1.58748,1.60954,1.63191,1.65455,1.67743,1.7005,1.72372,1.74704,1.77041,1.79378,1.8171,1.84033,1.86339,1.88624,1.90883,1.93109,1.95298,1.97445,1.99543,2.01589,2.03577,2.05503,2.07364,2.09154,2.10871,2.12512,2.14074,2.15555,2.16953,2.18267,2.19497,2.20642,2.21702,2.22679,2.23571,2.24383,2.25114,2.25766,2.26343,2.26847,2.2728,2.27645,2.27944,2.28181,2.28358,2.28479,2.28545,2.28559,2.28524,2.28442,2.28314,2.28142,2.27929,2.27674,2.27379,2.27044,2.2667,2.26257,2.25804,2.25312,2.24778,2.24203,2.23584,2.22921,2.22211,2.21453,2.20644,2.19782,2.18863,2.17886,2.16846,2.1574,2.14565,2.13318,2.11993,2.10588,2.09096,2.07516,2.0584,2.04065,2.02187,2.00199,1.98096,1.95875,1.93529,1.91054,1.88445,1.85697,1.82805,1.79765,1.76573,1.73227,1.69722,1.66058,1.62232,1.58246,1.54099,1.49795,1.45338,1.40733,1.35989,1.31114,1.26121,1.21025,1.15842,1.10592,1.05296,0.999789,0.946659,0.893843,0.841623,0.790283,0.7401,0.691337,0.644234,0.598992,0.555777,0.514707,0.475849,0.439226,0.404811,0.372549,0.342355,0.314138},
{1.01107,1.01177,1.0125,1.01328,1.01409,1.01495,1.01585,1.0168,1.0178,1.01886,1.01997,1.02115,1.02239,1.0237,1.02508,1.02653,1.02807,1.02969,1.0314,1.0332,1.0351,1.03711,1.03923,1.04147,1.04383,1.04632,1.04895,1.05172,1.05465,1.05773,1.06099,1.06442,1.06804,1.07185,1.07588,1.08012,1.08458,1.08929,1.09425,1.09947,1.10496,1.11074,1.11683,1.12322,1.12995,1.13702,1.14444,1.15223,1.16041,1.16898,1.17797,1.18738,1.19724,1.20755,1.21833,1.22959,1.24134,1.2536,1.26637,1.27967,1.2935,1.30787,1.32279,1.33825,1.35427,1.37085,1.38798,1.40565,1.42387,1.44263,1.4619,1.48169,1.50198,1.52274,1.54396,1.5656,1.58765,1.61007,1.63283,1.6559,1.67922,1.70277,1.72649,1.75034,1.77428,1.79824,1.82219,1.84605,1.86979,1.89334,1.91664,1.93965,1.9623,1.98454,2.00632,2.02758,2.04828,2.06837,2.0878,2.10654,2.12455,2.14179,2.15824,2.17388,2.18868,2.20263,2.21572,2.22794,2.2393,2.24979,2.25944,2.26824,2.27621,2.28338,2.28975,2.29537,2.30025,2.30441,2.30789,2.31071,2.31291,2.3145,2.31552,2.31599,2.31593,2.31537,2.31432,2.3128,2.31083,2.30842,2.30558,2.3023,2.29861,2.2945,2.28996,2.285,2.27959,2.27375,2.26745,2.26067,2.2534,2.24562,2.23731,2.22844,2.21898,2.20891,2.19819,2.18678,2.17467,2.16179,2.14813,2.13362,2.11824,2.10194,2.08466,2.06637,2.04701,2.02654,2.00489,1.98203,1.9579,1.93246,1.90564,1.87741,1.84773,1.81654,1.78381,1.74951,1.71361,1.6761,1.63696,1.5962,1.55383,1.50987,1.46439,1.41743,1.36908,1.31944,1.26864,1.21684,1.1642,1.11092,1.05724,1.00339,0.94964,0.896264,0.843547,0.791776,0.741226,0.692157,0.644807,0.599371,0.556007,0.514825,0.475882,0.439192,0.404725,0.372418,0.342184,0.31393}
};
source/processes/electromagnetic/standard/src/G4BetheBlochModel.cc
+17 -20
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4BetheBlochModel.cc 96934 2016-05-18 09:10:41Z gcosmo $
// $Id: G4BetheBlochModel.cc 109480 2018-04-24 14:46:36Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -72,7 +72,7 @@
using namespace std;
G4BetheBlochModel::G4BetheBlochModel(const G4ParticleDefinition* p,
G4BetheBlochModel::G4BetheBlochModel(const G4ParticleDefinition*,
const G4String& nam)
: G4VEmModel(nam),
particle(nullptr),
@@ -82,12 +82,7 @@ G4BetheBlochModel::G4BetheBlochModel(const G4ParticleDefinition* p,
{
fParticleChange = nullptr;
theElectron = G4Electron::Electron();
if(p) {
SetGenericIon(p);
SetParticle(p);
} else {
SetParticle(theElectron);
}
SetParticle(theElectron);
corr = G4LossTableManager::Instance()->EmCorrections();
nist = G4NistManager::Instance();
SetLowEnergyLimit(2.0*MeV);
@@ -151,23 +146,25 @@ void G4BetheBlochModel::SetupParameters()
{
mass = particle->GetPDGMass();
spin = particle->GetPDGSpin();
G4double q = particle->GetPDGCharge()/eplus;
G4double q = particle->GetPDGCharge()*inveplus;
chargeSquare = q*q;
corrFactor = chargeSquare;
ratio = electron_mass_c2/mass;
G4double magmom =
particle->GetPDGMagneticMoment()*mass/(0.5*eplus*hbar_Planck*c_squared);
static const G4double aMag = 1./(0.5*eplus*hbar_Planck*c_squared);
G4double magmom = particle->GetPDGMagneticMoment()*mass*aMag;
magMoment2 = magmom*magmom - 1.0;
formfact = 0.0;
tlimit = DBL_MAX;
if(particle->GetLeptonNumber() == 0) {
G4double x = 0.8426*GeV;
if(spin == 0.0 && mass < GeV) {x = 0.736*GeV;}
else if(mass > GeV) {
x /= nist->GetZ13(mass/proton_mass_c2);
// tlimit = 51.2*GeV*A13[iz]*A13[iz];
G4int iz = G4lrint(q);
if(iz <= 1) {
formfact = (spin == 0.0 && mass < GeV) ? 1.181e-6 : 1.548e-6;
} else {
G4double x = nist->GetA27(iz);
formfact = 3.969e-6*x*x;
}
formfact = 2.0*electron_mass_c2/(x*x);
tlimit = 2.0/formfact;
tlimit = std::sqrt(0.414/formfact +
electron_mass_c2*electron_mass_c2) - electron_mass_c2;
}
}
@@ -189,7 +186,7 @@ G4BetheBlochModel::ComputeCrossSectionPerElectron(const G4ParticleDefinition* p,
{
G4double cross = 0.0;
G4double tmax = MaxSecondaryEnergy(p, kineticEnergy);
G4double maxEnergy = min(tmax,maxKinEnergy);
G4double maxEnergy = std::min(tmax,maxKinEnergy);
if(cutEnergy < maxEnergy) {
G4double totEnergy = kineticEnergy + mass;
@@ -370,7 +367,7 @@ void G4BetheBlochModel::SampleSecondaries(vector<G4DynamicParticle*>* vdp,
// projectile formfactor - suppresion of high energy
// delta-electron production at high energy
G4double x = formfact*deltaKinEnergy;
G4double x = formfact*deltaKinEnergy*(deltaKinEnergy + 2*electron_mass_c2);
if(x > 1.e-6) {
G4double x1 = 1.0 + x;
source/processes/electromagnetic/standard/src/G4BetheHeitler5DModel.cc
+616
View File
@@ -0,0 +1,616 @@
//
// ********************************************************************
// * License and Disclaimer *
// * *
// * The Geant4 software is copyright of the Copyright Holders of *
// * the Geant4 Collaboration. It is provided under the terms and *
// * conditions of the Geant4 Software License, included in the file *
// * LICENSE and available at http://cern.ch/geant4/license . These *
// * include a list of copyright holders. *
// * *
// * Neither the authors of this software system, nor their employing *
// * institutes,nor the agencies providing financial support for this *
// * work make any representation or warranty, express or implied, *
// * regarding this software system or assume any liability for its *
// * use. Please see the license in the file LICENSE and URL above *
// * for the full disclaimer and the limitation of liability. *
// * *
// * This code implementation is the result of the scientific and *
// * technical work of the GEANT4 collaboration. *
// * By using, copying, modifying or distributing the software (or *
// * any work based on the software) you agree to acknowledge its *
// * use in resulting scientific publications, and indicate your *
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4BetheHeitler5DModel.cc $
//
// -------------------------------------------------------------------
//
// GEANT4 Class file
//
//
// File name: G4BetheHeitler5DModel
//
// Authors:
// Igor Semeniouk and Denis Bernard,
// LLR, Ecole polytechnique & CNRS/IN2P3, 91128 Palaiseau, France
//
// Acknowledgement of the support of the French National Research Agency
// (ANR-13-BS05-0002).
//
// Reference: arXiv:1802.08253 [hep-ph]
//
// Class Description:
//
// Generates the conversion of a high-energy photon to an e+e- pair, either in the field of an
// atomic electron (triplet) or nucleus (nuclear).
// Samples the five-dimensional (5D) differential cross-section analytical expression:
// . Non polarized conversion:
// H.A. Bethe, W. Heitler, Proc. R. Soc. Lond. Ser. A 146 (1934) 83.
// . Polarized conversion:
// T. H. Berlin and L. Madansky, Phys. Rev. 78 (1950) 623,
// M. M. May, Phys. Rev. 84 (1951) 265,
// J. M. Jauch and F. Rohrlich, The theory of photons and electrons, 1976.
//
// All the above expressions are named "Bethe-Heitler" here.
//
// Bethe & Heitler, put in Feynman diagram parlance, compute only the two dominant diagrams of
// the first order Born development, which is an excellent approximation for nuclear conversion
// and for high-energy triplet conversion.
//
// Only the linear polarisation of the incoming photon takes part in these expressions.
// The circular polarisation of the incoming photon does not (take part) and no polarisation
// is transfered to the final leptons.
//
// In case conversion takes place in the field of an isolated nucleus or electron, the bare
// Bethe-Heitler expression is used.
//
// In case the nucleus or the electron are part of an atom, the screening of the target field
// by the other electrons of the atom is described by a simple form factor, function of q2:
// . nuclear: N.F. Mott, H.S.W. Massey, The Theory of Atomic Collisions, 1934.
// . triplet: J.A. Wheeler and W.E. Lamb, Phys. Rev. 55 (1939) 858.
//
// The nuclear form factor that affects the probability of very large-q2 events, is not considered.
//
// In principle the code is valid from threshold, that is from 2 * m_e c^2 for nuclear and from
// 4 * m_e c^2 for triplet, up to infinity, while in pratice the divergence of the differential
// cross section at small q2 and, at high-energy, at small polar angle, make it break down at
// some point that depends on machine precision.
//
// Very-high-energy LPM suppression effects in the normalized differential cross-section
// are not considered.
//
// The 5D differential cross section is sampled without any high-energy nor small
// angle approximation(s).
// The generation is strictly energy-momentum conserving when all particles in the final state
// are taken into account, that is, including the recoiling target.
// (In contrast with the BH expressions taken at face values, for which the electron energy is
// taken to be EMinus = GammaEnergy - EPlus)
//
// Tests include the examination of 1D distributions: see TestEm15
//
// Total cross sections are not computed (we inherit from other classes).
// We just convert a photon on a target when asked to do so.
//
// Pure nuclear, pure triplet and 1/Z triplet/nuclear mixture can be generated.
//
// -------------------------------------------------------------------
#include "G4BetheHeitler5DModel.hh"
#include "G4EmParameters.hh"
#include "G4PhysicalConstants.hh"
#include "G4SystemOfUnits.hh"
#include "G4Electron.hh"
#include "G4Positron.hh"
#include "G4Gamma.hh"
#include "G4IonTable.hh"
#include "G4NucleiProperties.hh"
#include "Randomize.hh"
#include "G4ParticleChangeForGamma.hh"
#include "G4Pow.hh"
#include "G4Log.hh"
#include "G4Exp.hh"
#include "G4LorentzVector.hh"
#include "G4ThreeVector.hh"
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4BetheHeitler5DModel::G4BetheHeitler5DModel(const G4ParticleDefinition* pd,
const G4String& nam)
: G4BetheHeitlerModel(pd, nam), fVerbose(1), fConversionType(0), iraw(false)
{
theIonTable = G4IonTable::GetIonTable();
// Verbosity levels: ( Can redefine as needed, but some consideration )
// 0 = nothing
// > 2 print results
// > 4 print photon direction & polarisation
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4BetheHeitler5DModel::~G4BetheHeitler5DModel()
{}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4BetheHeitler5DModel::Initialise(const G4ParticleDefinition* part,
const G4DataVector& vec)
{
G4BetheHeitlerModel::Initialise(part, vec);
G4EmParameters* theManager = G4EmParameters::Instance();
// place to initialise model parameters
fVerbose = theManager->Verbose();
fConversionType = theManager->GetConversionType();
//////////////////////////////////////////////////////////////
// iraw :
// true : isolated electron or nucleus.
// false : inside atom -> screening form factor
iraw = theManager->OnIsolated();
// G4cout << "BH5DModel::Initialise verbose " << fVerbose
// << " isolated " << iraw << " ctype "<< fConversionType << G4endl;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void
G4BetheHeitler5DModel::BoostG4LorentzVector(const G4LorentzVector& p,
const G4LorentzVector& q,
G4LorentzVector& res) const
{
// p : 4-vector which will be boosted
// q : 4-vector of new origin in the old coordinates
const G4double pq = p.x()*q.x() + p.y()*q.y() + p.z()*q.z();
const G4double qq = q.x()*q.x() + q.y()*q.y() + q.z()*q.z();
const G4double mass = std::sqrt(q.t()*q.t()-qq);
const G4double lf = ((q.t()-mass)*pq/qq+p.t())/mass;
res.setX(p.x()+q.x()*lf);
res.setY(p.y()+q.y()*lf);
res.setZ(p.z()+q.z()*lf);
res.setT((p.t()*q.t()+pq)/mass);
}
// assuming that q.x=q.y=0.0
void
G4BetheHeitler5DModel::BoostG4LorentzVector(const G4LorentzVector& p,
const G4double qz,
const G4double qt,
const G4double lffac,
const G4double imass,
G4LorentzVector& res) const
{
// p : 4-vector which will be boosted
// q : 4-vector of new origin in the old coordinates
const G4double pq = p.z()*qz;
const G4double lf = (lffac*pq+p.t())*imass;
res.setZ(p.z()+qz*lf);
res.setT((p.t()*qt+pq)*imass);
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4double G4BetheHeitler5DModel::MaxDiffCrossSection(const G4double* par,
G4double Z,
G4double e,
G4double loge) const
{
const G4double Q = e/par[9];
return par[0] * G4Exp((par[2]+loge*par[4])*loge)
/ (par[1]+ G4Exp(par[3]*loge)+G4Exp(par[5]*loge))
* (1+par[7]*G4Exp(par[8]*G4Log(Z))*Q/(1+Q));
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void
G4BetheHeitler5DModel::SampleSecondaries(std::vector<G4DynamicParticle*>* fvect,
const G4MaterialCutsCouple* couple,
const G4DynamicParticle* aDynamicGamma,
G4double, G4double)
{
// MeV
static const G4double ElectronMass = CLHEP::electron_mass_c2;
static const G4double ElectronMass2 = ElectronMass*ElectronMass;
static const G4double alpha0 = CLHEP::fine_structure_const;
// mm
static const G4double r0 = CLHEP::classic_electr_radius;
// mbarn
static const G4double r02 = r0*r0*1.e+25;
static const G4double twoPi = CLHEP::twopi;
static const G4double factor = alpha0 * r02 / (twoPi*twoPi);
static const G4double factor1 = 2.66134007899/(8.*alpha0*ElectronMass);
//
static const G4double PairInvMassMin = 2.*ElectronMass;
//
static const G4double nu[10] = { 0.0227436, 0.0582046, 3.0322675, 2.8275065,
-0.0034004, 1.1212766, 1.8989468, 68.3492750,
0.0211186, 14.4 };
static const G4double tr[10] = { 0.0332350, 4.3942537, 2.8515925, 2.6351695,
-0.0031510, 1.5737305, 1.8104647, 20.6434021,
-0.0272586, 28.9};
//
static const G4double para[3][2] = { {11., -16.},{-1.17, -2.95},{-2., -0.5} };
//
static const G4double correctionIndex = 1.4;
//
const G4double GammaEnergy = aDynamicGamma->GetKineticEnergy();
const G4double GammaEnergy2 = GammaEnergy*GammaEnergy;
// do nothing below the threshold
if ( GammaEnergy <= LowEnergyLimit()) { return; }
// Will not be true tot cross section = 0
if ( GammaEnergy <= 2.0*ElectronMass) { return; }
//
const G4ParticleMomentum GammaDirection = aDynamicGamma->GetMomentumDirection();
G4ThreeVector GammaPolarization = aDynamicGamma->GetPolarization();
// The protection polarization perpendicular to the direction vector,
// as it done in G4LivermorePolarizedGammaConversionModel,
// assuming Direction is unitary vector
// (projection to plane) p_proj = p - (p o d)/(d o d) x d
if ( GammaPolarization.howOrthogonal(GammaDirection) != 0) {
GammaPolarization -= GammaPolarization.dot(GammaDirection) * GammaDirection;
}
// End of Protection
//
const G4double GammaPolarizationMag = GammaPolarization.mag();
//////////////////////////////////////////////////////////////
// target element
// select randomly one element constituting the material
const G4Element* anElement = SelectRandomAtom(couple, fTheGamma, GammaEnergy);
// Atomic number
const G4int Z = anElement->GetZasInt();
const G4int A = SelectIsotopeNumber(anElement);
const G4double iZ13 = 1./anElement->GetIonisation()->GetZ3();
const G4double targetMass = G4NucleiProperties::GetNuclearMass(A, Z);
//
CLHEP::HepRandomEngine* rndmEngine = G4Random::getTheEngine();
//
// itriplet : true -- triplet, false -- nuclear.
G4bool itriplet = false;
if (fConversionType == 1) {
itriplet = false;
} else if (fConversionType == 2) {
itriplet = true;
if ( GammaEnergy <= 4.0*ElectronMass ) return;
} else if ( GammaEnergy > 4.0*ElectronMass ) {
// choose triplet or nuclear from a triplet/nuclear=1/Z
// total cross section ratio.
// approximate at low energies !
if(rndmEngine->flat()*(Z+1) < 1.) {
itriplet = true;
}
}
//
const G4double RecoilMass = itriplet ? ElectronMass : targetMass;
const G4double RecoilMass2 = RecoilMass*RecoilMass;
const G4double sCMS = 2.*RecoilMass*GammaEnergy + RecoilMass2;
const G4double sCMSPlusRM2 = sCMS + RecoilMass2;
const G4double sqrts = std::sqrt(sCMS);
const G4double isqrts2 = 1./(2.*sqrts);
//
const G4double PairInvMassMax = sqrts-RecoilMass;
const G4double PairInvMassRange = PairInvMassMax/PairInvMassMin;
// use exact expression:
const G4double lnPairInvMassRange = G4Log(PairInvMassRange);
// initial state. Defines z axis of "0" frame as along photon propagation.
// create 4-vectors: gamma0 + target0 and CMS=gamma0+target0
// Since CMS(0., 0., GammaEnergy, GammaEnergy+RecoilMass) set some constants
// for the special boost that makes use of the form of CMS 4-vector
const G4double CMSqz = GammaEnergy;
const G4double CMSt = GammaEnergy+RecoilMass;
const G4double iCMSmass = 1./std::sqrt(RecoilMass*(RecoilMass+2.*GammaEnergy));
const G4double CMSfact = (CMSt-1./iCMSmass)/(CMSqz*CMSqz);
// maximum value of pdf
const G4double EffectiveZ = iraw ? 0.5 : Z;
const G4double Threshold = itriplet ? 4.*ElectronMass : 2.*ElectronMass;
const G4double AvailableEnergy = GammaEnergy - Threshold;
const G4double LogAvailableEnergy = G4Log(AvailableEnergy);
//
const G4double MaxDiffCross = itriplet
? MaxDiffCrossSection(tr, EffectiveZ, AvailableEnergy, LogAvailableEnergy)
: MaxDiffCrossSection(nu, EffectiveZ, AvailableEnergy, LogAvailableEnergy);
//
// 50% safety marging factor
const G4double ymax = 1.5 * MaxDiffCross;
// x1 bounds
const G4double xu1 = (LogAvailableEnergy > para[2][0])
? para[0][0] + para[1][0]*LogAvailableEnergy
: para[0][0] + para[2][0]*para[1][0];
const G4double xl1 = (LogAvailableEnergy > para[2][1])
? para[0][1] + para[1][1]*LogAvailableEnergy
: para[0][1] + para[2][1]*para[1][1];
//
G4LorentzVector Recoil0;
G4LorentzVector Positron0;
G4LorentzVector Electron0;
G4LorentzVector Recoil1;
G4LorentzVector Positron1;
G4LorentzVector Electron1;
G4LorentzVector Positron2;
G4LorentzVector Electron2;
G4LorentzVector Pair1;
G4double pdf = 0.;
// START Sampling
do {
G4double X1;
G4double rndmv2[2];
G4double cond1;
do {
rndmEngine->flatArray(2, rndmv2);
X1 = rndmv2[0];
cond1 = G4Exp(correctionIndex*G4Log(X1));
} while (cond1 < rndmv2[1]);
const G4double x0 = G4Exp(xl1 + (xu1 - xl1)*rndmEngine->flat());
const G4double dum0 = 1./(1.+x0);
const G4double cosTheta = (x0-1.)*dum0;
const G4double sinTheta = std::sqrt(4.*x0)*dum0;
const G4double PairInvMass = PairInvMassMin*G4Exp(X1*X1*lnPairInvMassRange);
G4double rndmv3[3];
rndmEngine->flatArray(3, rndmv3);
//--------------------------------------------------------------------------
// const G4double ThetaLept = pi*rndmv3[0];
// const G4double cosThetaLept = std::cos(ThetaLept);
// const G4double sinThetaLept = std::sin(ThetaLept);
//
// const G4double PhiLept = twoPi*rndmv3[1]-pi;
// const G4double cosPhiLept = std::cos(PhiLept);
// const G4double sinPhiLept = std::sin(PhiLept);
//
// const G4double Phi = twoPi*rndmv3[2]-pi;
// const G4double cosPhi = std::cos(Phi);
// const G4double sinPhi = std::sin(Phi);
//---------------------------------------------------------------------------
// cos and sin theta-lepton
const G4double cosThetaLept = std::cos(pi*rndmv3[0]);
// sin(ThetaLept) is always in [0,+1] if ThetaLept is in [0,pi]
const G4double sinThetaLept = std::sqrt((1.-cosThetaLept)*(1.+cosThetaLept));
// cos and sin phi-lepton
const G4double cosPhiLept = std::cos(twoPi*rndmv3[1]-pi);
const G4double dumx0 = std::sqrt((1.-cosPhiLept)*(1.+cosPhiLept));
// sin(PhiLept) is in [-1,0] if PhiLept in [-pi,0) and
// is in [0,+1] if PhiLept in [0,+pi]
const G4double sinPhiLept = (rndmv3[1]<0.5) ? -1.*dumx0 : dumx0;
// cos and sin phi
const G4double cosPhi = std::cos(twoPi*rndmv3[2]-pi);
const G4double dumx1 = std::sqrt((1.-cosPhi)*(1.+cosPhi));
const G4double sinPhi = (rndmv3[2]<0.5) ? -1.*dumx1 : dumx1;
// frames:
// 0 : the laboratory Lorentz frame, axes along photon direction and polarisation
// 1 : the center-of-mass Lorentz frame
// 2 : the pair Lorentz frame
// 3 : the laboratory Lorentz frame, Geant4 axes definition
// in the center-of-mass frame
const G4double RecEnergyCMS = (sCMSPlusRM2-PairInvMass*PairInvMass)*isqrts2;
const G4double LeptonEnergy2 = PairInvMass*0.5;
const G4double thePRecoil = std::sqrt( (RecEnergyCMS-RecoilMass)
*(RecEnergyCMS+RecoilMass));
Recoil1.setX( thePRecoil*sinTheta*cosPhi);
Recoil1.setY( thePRecoil*sinTheta*sinPhi);
Recoil1.setZ( thePRecoil*cosTheta);
Recoil1.setT( RecEnergyCMS);
Pair1.setX (-Recoil1.x());
Pair1.setY (-Recoil1.y());
Pair1.setZ (-Recoil1.z());
Pair1.setT ( RecEnergyCMS);
// in the pair frame
const G4double thePLepton = std::sqrt( (LeptonEnergy2-ElectronMass)
*(LeptonEnergy2+ElectronMass));
Positron2.setX( thePLepton*sinThetaLept*cosPhiLept);
Positron2.setY( thePLepton*sinThetaLept*sinPhiLept);
Positron2.setZ( thePLepton*cosThetaLept);
Positron2.setT( LeptonEnergy2);
Electron2.setX(-Positron2.x());
Electron2.setY(-Positron2.y());
Electron2.setZ(-Positron2.z());
Electron2.setT( LeptonEnergy2);
// back to the center-of-mass frame
Pair1.setT(sqrts-RecEnergyCMS);
// Normalisation of final state phase space:
// Section 47 of Particle Data Group, Chin. Phys. C, 40, 100001 (2016)
const G4double Norme = Recoil1.vect().mag() * Positron2.vect().mag();
//
BoostG4LorentzVector(Positron2, Pair1, Positron1);
BoostG4LorentzVector(Electron2, Pair1, Electron1);
//
// back to the laboratory frame (make use of the CMS(0,0,Eg,Eg+RM)) form
Recoil0.setX(Recoil1.x());
Recoil0.setY(Recoil1.y());
BoostG4LorentzVector(Recoil1 , CMSqz, CMSt, CMSfact, iCMSmass, Recoil0);
//
Positron0.setX(Positron1.x());
Positron0.setY(Positron1.y());
BoostG4LorentzVector(Positron1, CMSqz, CMSt, CMSfact, iCMSmass, Positron0);
//
Electron0.setX(Electron1.x());
Electron0.setY(Electron1.y());
BoostG4LorentzVector(Electron1, CMSqz, CMSt, CMSfact, iCMSmass, Electron0);
//
// Jacobian factors
const G4double Jacob0 = x0*dum0*dum0;
const G4double Jacob1 = 2.*X1*lnPairInvMassRange*PairInvMass;
const G4double Jacob2 = std::abs(sinThetaLept);
// Normalisation of final state phase space:
// Section 47 of Particle Data Group, Chin. Phys. C, 40, 100001 (2016)
// G4double Norme = Recoil1.vect().mag() * Positron2.vect().mag();
const G4double EPlus = Positron0.t();
const G4double PPlus = Positron0.vect().mag();
const G4double sinThetaPlus = Positron0.vect().perp()/PPlus;
const G4double cosThetaPlus = Positron0.vect().cosTheta();
const G4double pPX = Positron0.x();
const G4double pPY = Positron0.y();
const G4double dum1 = 1./std::sqrt( pPX*pPX + pPY*pPY );
const G4double cosPhiPlus = pPX*dum1;
const G4double sinPhiPlus = pPY*dum1;
// denominators:
// the two cancelling leading terms for forward emission at high energy, removed
const G4double elMassCTP = ElectronMass*cosThetaPlus;
const G4double ePlusSTP = EPlus*sinThetaPlus;
const G4double DPlus = (elMassCTP*elMassCTP + ePlusSTP*ePlusSTP)
/(EPlus + PPlus*cosThetaPlus);
const G4double EMinus = Electron0.t();
const G4double PMinus = Electron0.vect().mag();
const G4double sinThetaMinus = Electron0.vect().perp()/PMinus;
const G4double cosThetaMinus = Electron0.vect().cosTheta();
const G4double ePX = Electron0.x();
const G4double ePY = Electron0.y();
const G4double dum2 = 1./std::sqrt( ePX*ePX + ePY*ePY );
const G4double cosPhiMinus = ePX*dum2;
const G4double sinPhiMinus = ePY*dum2;
const G4double elMassCTM = ElectronMass*cosThetaMinus;
const G4double eMinSTM = EMinus*sinThetaMinus;
const G4double DMinus = (elMassCTM*elMassCTM + eMinSTM*eMinSTM)
/(EMinus + PMinus*cosThetaMinus);
// cos(phiMinus-PhiPlus)
const G4double cosdPhi = cosPhiPlus*cosPhiMinus + sinPhiPlus*sinPhiMinus;
const G4double PRec = Recoil0.vect().mag();
const G4double q2 = PRec*PRec;
const G4double BigPhi = -ElectronMass2 / (GammaEnergy*GammaEnergy2 * q2*q2);
G4double FormFactor = 1.;
if (!iraw) {
if (itriplet) {
const G4double qun = factor1*iZ13*iZ13;
const G4double nun = qun * PRec;
if (nun < 1.) {
FormFactor = (nun < 0.01) ? (13.8-55.4*std::sqrt(nun))*nun
: std::sqrt(1-(nun-1)*(nun-1));
} // else FormFactor = 1 by default
} else {
const G4double dum3 = 217.*PRec*iZ13;
const G4double AFF = 1./(1. + dum3*dum3);
FormFactor = (1.-AFF)*(1-AFF);
}
} // else FormFactor = 1 by default
//
G4double betheheitler;
if (GammaPolarizationMag==0.) {
const G4double pPlusSTP = PPlus*sinThetaPlus;
const G4double pMinusSTM = PMinus*sinThetaMinus;
const G4double pPlusSTPperDP = pPlusSTP/DPlus;
const G4double pMinusSTMperDM = pMinusSTM/DMinus;
const G4double dunpol = BigPhi*(
pPlusSTPperDP *pPlusSTPperDP *(4.*EMinus*EMinus-q2)
+ pMinusSTMperDM*pMinusSTMperDM*(4.*EPlus*EPlus - q2)
+ 2.*pPlusSTPperDP*pMinusSTMperDM*cosdPhi
*(4.*EPlus*EMinus + q2 - 2.*GammaEnergy2)
- 2.*GammaEnergy2*(pPlusSTP*pPlusSTP+pMinusSTM*pMinusSTM)/(DMinus*DPlus));
betheheitler = dunpol * factor;
} else {
const G4double pPlusSTP = PPlus*sinThetaPlus;
const G4double pMinusSTM = PMinus*sinThetaMinus;
const G4double pPlusSTPCPPperDP = pPlusSTP*cosPhiPlus/DPlus;
const G4double pMinusSTMCPMperDM = pMinusSTM*cosPhiMinus/DMinus;
const G4double caa = 2.*(EPlus*pMinusSTMCPMperDM+EMinus*pPlusSTPCPPperDP);
const G4double cbb = pMinusSTMCPMperDM-pPlusSTPCPPperDP;
const G4double ccc = (pPlusSTP*pPlusSTP + pMinusSTM*pMinusSTM
+2.*pPlusSTP*pMinusSTM*cosdPhi)/ (DMinus*DPlus);
const G4double dtot= 2.*BigPhi*( caa*caa - q2*cbb*cbb - GammaEnergy2*ccc);
betheheitler = dtot * factor;
}
//
const G4double cross = Norme * Jacob0 * Jacob1 * Jacob2 * betheheitler
* FormFactor * RecoilMass / sqrts;
pdf = cross * (xu1 - xl1) / cond1;
} while ( pdf < ymax * rndmEngine->flat() );
// END of Sampling
//
if ( fVerbose > 2 ) {
G4double recul = std::sqrt(Recoil0.x()*Recoil0.x()+Recoil0.y()*Recoil0.y()
+Recoil0.z()*Recoil0.z());
G4cout << "BetheHeitler5DModel GammaEnergy= " << GammaEnergy
<< " PDF= " << pdf << " ymax= " << ymax
<< " recul= " << recul << G4endl;
}
// back to Geant4 system
if ( fVerbose > 4 ) {
G4cout << "BetheHeitler5DModel GammaDirection " << GammaDirection << G4endl;
G4cout << "BetheHeitler5DModel GammaPolarization " << GammaPolarization << G4endl;
}
//
if (GammaPolarizationMag == 0.0) {
G4ThreeVector axis(1.,0.,0.);
G4ThreeVector perp = GammaDirection.cross(axis);
if (perp.mag() == 0) {
axis.set(0.,1.,0.);
perp = GammaDirection.cross(axis);
}
perp = perp / perp.mag();
G4ThreeVector perperp = GammaDirection.cross(perp);
perperp = perperp / perperp.mag();
// rotation
G4ThreeVector Rot = Recoil0.x()*perp + Recoil0.y()*perperp
+ Recoil0.z()*GammaDirection;
Recoil0.setVect(Rot);
Rot = Positron0.x()*perp + Positron0.y()*perperp
+ Positron0.z()*GammaDirection;
Positron0.setVect(Rot);
Rot = Electron0.x()*perp + Electron0.y()*perperp
+ Electron0.z()*GammaDirection;
Electron0.setVect(Rot);
} else {
// The unit norm vector that is orthogonal to the two others
G4ThreeVector yGrec = GammaDirection.cross(GammaPolarization);
// rotation
G4ThreeVector Rot = Recoil0.x()*GammaPolarization + Recoil0.y()*yGrec
+ Recoil0.z()*GammaDirection;
Recoil0.setVect(Rot);
Rot = Positron0.x()*GammaPolarization + Positron0.y()*yGrec
+ Positron0.z()*GammaDirection;
Positron0.setVect(Rot);
Rot = Electron0.x()*GammaPolarization + Electron0.y()*yGrec
+ Electron0.z()*GammaDirection;
Electron0.setVect(Rot);
}
//
if ( fVerbose > 2 ) {
G4cout << "BetheHeitler5DModel Recoil0 " << Recoil0.x() << " " << Recoil0.y() << " " << Recoil0.z()
<< " " << Recoil0.t() << " " << G4endl;
G4cout << "BetheHeitler5DModel Positron0 " << Positron0.x() << " " << Positron0.y() << " "
<< Positron0.z() << " " << Positron0.t() << " " << G4endl;
G4cout << "BetheHeitler5DModel Electron0 " << Electron0.x() << " " << Electron0.y() << " "
<< Electron0.z() << " " << Electron0.t() << " " << G4endl;
}
//
// create G4DynamicParticle object for the particle1 (electron)
G4DynamicParticle* aParticle1 = new G4DynamicParticle(fTheElectron,Electron0);
// create G4DynamicParticle object for the particle2 (positron)
G4DynamicParticle* aParticle2 = new G4DynamicParticle(fThePositron,Positron0);
// create G4DynamicParticle object for the particle3 ( recoil )
G4DynamicParticle* aParticle3;
G4ParticleDefinition* RecoilPart;
if (itriplet) {
// triplet
RecoilPart = fTheElectron;
} else{
RecoilPart = theIonTable->GetIon(Z, A, 0);
}
aParticle3 = new G4DynamicParticle(RecoilPart,Recoil0);
// Fill output vector
fvect->push_back(aParticle1);
fvect->push_back(aParticle2);
fvect->push_back(aParticle3);
// kill incident photon
fParticleChange->SetProposedKineticEnergy(0.);
fParticleChange->ProposeTrackStatus(fStopAndKill);
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
source/processes/electromagnetic/standard/src/G4BetheHeitlerModel.cc
+213 -185
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4BetheHeitlerModel.cc 104555 2017-06-06 07:31:32Z gcosmo $
// $Id: G4BetheHeitlerModel.cc 110939 2018-06-27 12:02:21Z gunter $
//
// -------------------------------------------------------------------
//
@@ -44,13 +44,14 @@
// 20-02-07 SelectRandomElement is called for any initial gamma energy
// in order to have selected element for polarized model (VI)
// 25-10-10 Removed unused table, added element selector (VI)
// 28-05-18 New version with improved screening function approximation, improved
// efficiency, documentation and cleanup. Corrected call to selecting
// target atom in the final state sampling. (M. Novak)
//
// Class Description:
//
// -------------------------------------------------------------------
//
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
#include "G4BetheHeitlerModel.hh"
#include "G4PhysicalConstants.hh"
@@ -61,104 +62,128 @@
#include "Randomize.hh"
#include "G4ParticleChangeForGamma.hh"
#include "G4Pow.hh"
#include "G4Exp.hh"
#include "G4ModifiedTsai.hh"
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
using namespace std;
const G4int G4BetheHeitlerModel::gMaxZet = 120;
std::vector<G4BetheHeitlerModel::ElementData*> G4BetheHeitlerModel::gElementData;
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4BetheHeitlerModel::G4BetheHeitlerModel(const G4ParticleDefinition*,
const G4String& nam)
: G4VEmModel(nam)
G4BetheHeitlerModel::G4BetheHeitlerModel(const G4ParticleDefinition*,
const G4String& nam)
: G4VEmModel(nam),
fG4Calc(G4Pow::GetInstance()), fTheGamma(G4Gamma::Gamma()),
fTheElectron(G4Electron::Electron()), fThePositron(G4Positron::Positron()),
fParticleChange(nullptr)
{
fParticleChange = nullptr;
theGamma = G4Gamma::Gamma();
thePositron = G4Positron::Positron();
theElectron = G4Electron::Electron();
g4calc = G4Pow::GetInstance();
SetAngularDistribution(new G4ModifiedTsai());
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4BetheHeitlerModel::~G4BetheHeitlerModel()
{}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4BetheHeitlerModel::Initialise(const G4ParticleDefinition* p,
const G4DataVector& cuts)
{
if(!fParticleChange) { fParticleChange = GetParticleChangeForGamma(); }
if(IsMaster()) { InitialiseElementSelectors(p, cuts); }
if (IsMaster()) {
// clear ElementData container
for (size_t iz = 0; iz < gElementData.size(); ++iz) {
if (gElementData[iz]) delete gElementData[iz];
}
gElementData.clear();
}
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4BetheHeitlerModel::InitialiseLocal(const G4ParticleDefinition*,
G4VEmModel* masterModel)
void G4BetheHeitlerModel::Initialise(const G4ParticleDefinition* p,
const G4DataVector& cuts)
{
if (IsMaster()) {
InitialiseElementData();
}
if (!fParticleChange) { fParticleChange = GetParticleChangeForGamma(); }
if (IsMaster()) {
InitialiseElementSelectors(p, cuts);
}
}
void G4BetheHeitlerModel::InitialiseLocal(const G4ParticleDefinition*,
G4VEmModel* masterModel)
{
SetElementSelectors(masterModel->GetElementSelectors());
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4double
G4BetheHeitlerModel::ComputeCrossSectionPerAtom(const G4ParticleDefinition*,
G4double GammaEnergy, G4double Z,
G4double, G4double, G4double)
// Calculates the microscopic cross section in GEANT4 internal units.
// A parametrized formula from L. Urban is used to estimate
// the total cross section.
// It gives a good description of the data from 1.5 MeV to 100 GeV.
// below 1.5 MeV: sigma=sigma(1.5MeV)*(GammaEnergy-2electronmass)
// *(GammaEnergy-2electronmass)
G4double
G4BetheHeitlerModel::ComputeCrossSectionPerAtom(const G4ParticleDefinition*,
G4double gammaEnergy, G4double Z,
G4double, G4double, G4double)
{
G4double xSection = 0.0 ;
if ( Z < 0.9 || GammaEnergy <= 2.0*electron_mass_c2 ) { return xSection; }
static const G4double GammaEnergyLimit = 1.5*MeV;
static const G4double
a0= 8.7842e+2*microbarn, a1=-1.9625e+3*microbarn, a2= 1.2949e+3*microbarn,
a3=-2.0028e+2*microbarn, a4= 1.2575e+1*microbarn, a5=-2.8333e-1*microbarn;
static const G4double
b0=-1.0342e+1*microbarn, b1= 1.7692e+1*microbarn, b2=-8.2381 *microbarn,
b3= 1.3063 *microbarn, b4=-9.0815e-2*microbarn, b5= 2.3586e-3*microbarn;
static const G4double
c0=-4.5263e+2*microbarn, c1= 1.1161e+3*microbarn, c2=-8.6749e+2*microbarn,
c3= 2.1773e+2*microbarn, c4=-2.0467e+1*microbarn, c5= 6.5372e-1*microbarn;
G4double GammaEnergySave = GammaEnergy;
if (GammaEnergy < GammaEnergyLimit) { GammaEnergy = GammaEnergyLimit; }
G4double X=G4Log(GammaEnergy/electron_mass_c2), X2=X*X, X3=X2*X, X4=X3*X, X5=X4*X;
G4double F1 = a0 + a1*X + a2*X2 + a3*X3 + a4*X4 + a5*X5,
F2 = b0 + b1*X + b2*X2 + b3*X3 + b4*X4 + b5*X5,
F3 = c0 + c1*X + c2*X2 + c3*X3 + c4*X4 + c5*X5;
// short versions
static const G4double kMC2 = CLHEP::electron_mass_c2;
// zero cross section below the kinematical limit: Eg<2mc^2
if (Z < 0.9 || gammaEnergy <= 2.0*kMC2) { return xSection; }
//
static const G4double gammaEnergyLimit = 1.5*CLHEP::MeV;
// set coefficients a, b c
static const G4double a0 = 8.7842e+2*CLHEP::microbarn;
static const G4double a1 = -1.9625e+3*CLHEP::microbarn;
static const G4double a2 = 1.2949e+3*CLHEP::microbarn;
static const G4double a3 = -2.0028e+2*CLHEP::microbarn;
static const G4double a4 = 1.2575e+1*CLHEP::microbarn;
static const G4double a5 = -2.8333e-1*CLHEP::microbarn;
static const G4double b0 = -1.0342e+1*CLHEP::microbarn;
static const G4double b1 = 1.7692e+1*CLHEP::microbarn;
static const G4double b2 = -8.2381 *CLHEP::microbarn;
static const G4double b3 = 1.3063 *CLHEP::microbarn;
static const G4double b4 = -9.0815e-2*CLHEP::microbarn;
static const G4double b5 = 2.3586e-3*CLHEP::microbarn;
static const G4double c0 = -4.5263e+2*CLHEP::microbarn;
static const G4double c1 = 1.1161e+3*CLHEP::microbarn;
static const G4double c2 = -8.6749e+2*CLHEP::microbarn;
static const G4double c3 = 2.1773e+2*CLHEP::microbarn;
static const G4double c4 = -2.0467e+1*CLHEP::microbarn;
static const G4double c5 = 6.5372e-1*CLHEP::microbarn;
// check low energy limit of the approximation (1.5 MeV)
G4double gammaEnergyOrg = gammaEnergy;
if (gammaEnergy < gammaEnergyLimit) { gammaEnergy = gammaEnergyLimit; }
// compute gamma energy variables
const G4double x = G4Log(gammaEnergy/kMC2);
const G4double x2 = x *x;
const G4double x3 = x2*x;
const G4double x4 = x3*x;
const G4double x5 = x4*x;
//
const G4double F1 = a0 + a1*x + a2*x2 + a3*x3 + a4*x4 + a5*x5;
const G4double F2 = b0 + b1*x + b2*x2 + b3*x3 + b4*x4 + b5*x5;
const G4double F3 = c0 + c1*x + c2*x2 + c3*x3 + c4*x4 + c5*x5;
// compute the approximated cross section
xSection = (Z + 1.)*(F1*Z + F2*Z*Z + F3);
if (GammaEnergySave < GammaEnergyLimit) {
X = (GammaEnergySave - 2.*electron_mass_c2)
/ (GammaEnergyLimit - 2.*electron_mass_c2);
xSection *= X*X;
// check if we are below the limit of the approximation and apply correction
if (gammaEnergyOrg < gammaEnergyLimit) {
const G4double dum = (gammaEnergyOrg-2.*kMC2)/(gammaEnergyLimit-2.*kMC2);
xSection *= dum*dum;
}
// make sure that the cross section is never negative
xSection = std::max(xSection, 0.);
return xSection;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4BetheHeitlerModel::SampleSecondaries(std::vector<G4DynamicParticle*>* fvect,
const G4MaterialCutsCouple* couple,
const G4DynamicParticle* aDynamicGamma,
G4double,
G4double)
// The secondaries e+e- energies are sampled using the Bethe - Heitler
// cross sections with Coulomb correction.
// A modified version of the random number techniques of Butcher & Messel
@@ -171,146 +196,149 @@ void G4BetheHeitlerModel::SampleSecondaries(std::vector<G4DynamicParticle*>* fve
// Note 2 : The differential cross section implicitly takes account of
// pair creation in both nuclear and atomic electron fields.
// However triplet prodution is not generated.
void G4BetheHeitlerModel::SampleSecondaries(std::vector<G4DynamicParticle*>* fvect,
const G4MaterialCutsCouple* couple,
const G4DynamicParticle* aDynamicGamma,
G4double, G4double)
{
const G4Material* aMaterial = couple->GetMaterial();
G4double GammaEnergy = aDynamicGamma->GetKineticEnergy();
G4ParticleMomentum GammaDirection = aDynamicGamma->GetMomentumDirection();
G4double epsil ;
G4double epsil0 = electron_mass_c2/GammaEnergy;
if(epsil0 > 1.0) { return; }
// do it fast if GammaEnergy < Egsmall
// select randomly one element constituing the material
const G4Element* anElement =
SelectRandomAtom(aMaterial, theGamma, GammaEnergy);
// set some constant values
const G4double gammaEnergy = aDynamicGamma->GetKineticEnergy();
const G4double eps0 = CLHEP::electron_mass_c2/gammaEnergy;
//
// check kinematical limit: gamma energy(Eg) must be at least 2 e- rest mass
if (eps0 > 0.5) { return; }
//
// select target element of the material (probs. are based on partial x-secs)
const G4Element* anElement = SelectRandomAtom(couple,fTheGamma,gammaEnergy);
//
// get the random engine
CLHEP::HepRandomEngine* rndmEngine = G4Random::getTheEngine();
static const G4double Egsmall=2.*CLHEP::MeV;
if (GammaEnergy < Egsmall) {
epsil = epsil0 + (0.5-epsil0)*rndmEngine->flat();
//
// 'eps' is the total energy transferred to one of the e-/e+ pair in initial
// gamma energy units Eg. Since the corresponding DCS is symmetric on eps=0.5,
// the kinematical limits for eps0=mc^2/Eg <= eps <= 0.5
// 1. 'eps' is sampled uniformly on the [eps0, 0.5] inteval if Eg<Egsmall
// 2. otherwise, on the [eps_min, 0.5] interval according to the DCS (case 2.)
G4double eps;
// case 1.
static const G4double Egsmall = 2.*CLHEP::MeV;
if (gammaEnergy < Egsmall) {
eps = eps0 + (0.5-eps0)*rndmEngine->flat();
} else {
// now comes the case with GammaEnergy >= 2. MeV
// Extract Coulomb factor for this Element
G4double FZ = 8.*(anElement->GetIonisation()->GetlogZ3());
// case 2.
// get the Coulomb factor for the target element (Z) and gamma energy (Eg)
// F(Z) = 8*ln(Z)/3 if Eg <= 50 [MeV] => no Coulomb correction
// F(Z) = 8*ln(Z)/3 + 8*fc(Z) if Eg > 50 [MeV] => fc(Z) is the Coulomb cor.
//
// The screening variable 'delta(eps)' = 136*Z^{-1/3}*eps0/[eps(1-eps)]
// Due to the Coulomb correction, the DCS can go below zero even at
// kinematicaly allowed eps > eps0 values. In order to exclude this eps
// range with negative DCS, the minimum eps value will be set to eps_min =
// max[eps0, epsp] with epsp is the solution of SF(delta(epsp)) - F(Z)/2 = 0
// with SF being the screening function (SF1=SF2 at high value of delta).
// The solution is epsp = 0.5 - 0.5*sqrt[ 1 - 4*136*Z^{-1/3}eps0/deltap]
// with deltap = Exp[(42.038-F(Z))/8.29]-0.958. So the limits are:
// - when eps=eps_max = 0.5 => delta_min = 136*Z^{-1/3}*eps0/4
// - epsp = 0.5 - 0.5*sqrt[ 1 - delta_min/deltap]
// - and eps_min = max[eps0, epsp]
static const G4double midEnergy = 50.*CLHEP::MeV;
if (GammaEnergy > midEnergy) { FZ += 8.*(anElement->GetfCoulomb()); }
// limits of the screening variable
G4double screenfac = 136.*epsil0/(anElement->GetIonisation()->GetZ3());
G4double screenmax = G4Exp ((42.24 - FZ)/8.368) + 0.952 ;
G4double screenmin = std::min(4.*screenfac, screenmax);
// limits of the energy sampling
G4double epsil1 = 0.5 - 0.5*sqrt(1. - screenmin/screenmax) ;
G4double epsilmin = std::max(epsil0,epsil1);
G4double epsilrange = 0.5 - epsilmin;
const G4int iZet = std::min(gMaxZet, anElement->GetZasInt());
const G4double deltaFactor = 136.*eps0/anElement->GetIonisation()->GetZ3();
G4double deltaMax = gElementData[iZet]->fDeltaMaxLow;
G4double FZ = 8.*anElement->GetIonisation()->GetlogZ3();
if (gammaEnergy > midEnergy) {
FZ += 8.*(anElement->GetfCoulomb());
deltaMax = gElementData[iZet]->fDeltaMaxHigh;
}
const G4double deltaMin = 4.*deltaFactor;
//
// compute the limits of eps
const G4double epsp = 0.5 - 0.5*std::sqrt(1. - deltaMin/deltaMax) ;
const G4double epsMin = std::max(eps0,epsp);
const G4double epsRange = 0.5 - epsMin;
//
// sample the energy rate of the created electron (or positron)
//
//G4double epsil, screenvar, greject ;
G4double screenvar, greject ;
G4double F10 = ScreenFunction1(screenmin) - FZ;
G4double F20 = ScreenFunction2(screenmin) - FZ;
G4double NormF1 = std::max(F10*epsilrange*epsilrange, 0.);
G4double NormF2 = std::max(1.5*F20, 0.);
// sample the energy rate (eps) of the created electron (or positron)
G4double F10, F20;
ScreenFunction12(deltaMin, F10, F20);
F10 -= FZ;
F20 -= FZ;
const G4double NormF1 = std::max(F10 * epsRange * epsRange, 0.);
const G4double NormF2 = std::max(1.5 * F20 , 0.);
const G4double NormCond = NormF1/(NormF1 + NormF2);
// we will need 3 uniform random number for each trial of sampling
G4double rndmv[3];
G4double greject = 0.;
do {
if ( NormF1/(NormF1+NormF2) > rndmEngine->flat()) {
epsil = 0.5 - epsilrange*g4calc->A13(rndmEngine->flat());
screenvar = screenfac/(epsil*(1-epsil));
greject = (ScreenFunction1(screenvar) - FZ)/F10;
rndmEngine->flatArray(3, rndmv);
if (NormCond > rndmv[0]) {
eps = 0.5 - epsRange * fG4Calc->A13(rndmv[1]);
const G4double delta = deltaFactor/(eps*(1.-eps));
greject = (ScreenFunction1(delta)-FZ)/F10;
} else {
epsil = epsilmin + epsilrange*rndmEngine->flat();
screenvar = screenfac/(epsil*(1-epsil));
greject = (ScreenFunction2(screenvar) - FZ)/F20;
eps = epsMin + epsRange*rndmv[1];
const G4double delta = deltaFactor/(eps*(1.-eps));
greject = (ScreenFunction2(delta)-FZ)/F20;
}
// Loop checking, 03-Aug-2015, Vladimir Ivanchenko
} while( greject < rndmEngine->flat());
} // end of epsil sampling
} while (greject < rndmv[2]);
} // end of eps sampling
//
// fixe charges randomly
//
G4double ElectTotEnergy, PositTotEnergy;
// select charges randomly
G4double eTotEnergy, pTotEnergy;
if (rndmEngine->flat() > 0.5) {
ElectTotEnergy = (1.-epsil)*GammaEnergy;
PositTotEnergy = epsil*GammaEnergy;
eTotEnergy = (1.-eps)*gammaEnergy;
pTotEnergy = eps*gammaEnergy;
} else {
PositTotEnergy = (1.-epsil)*GammaEnergy;
ElectTotEnergy = epsil*GammaEnergy;
pTotEnergy = (1.-eps)*gammaEnergy;
eTotEnergy = eps*gammaEnergy;
}
//
// scattered electron (positron) angles. ( Z - axis along the parent photon)
// sample pair kinematics
const G4double eKinEnergy = std::max(0.,eTotEnergy - CLHEP::electron_mass_c2);
const G4double pKinEnergy = std::max(0.,pTotEnergy - CLHEP::electron_mass_c2);
//
// universal distribution suggested by L. Urban
// (Geant3 manual (1993) Phys211),
// derived from Tsai distribution (Rev Mod Phys 49,421(1977))
static const G4double a1 = 1.6;
static const G4double a2 = a1/3.;
G4double uu = -G4Log(rndmEngine->flat()*rndmEngine->flat());
G4double u = (0.25 > rndmEngine->flat()) ? uu*a1 : uu*a2;
G4double thetaEle = u*electron_mass_c2/ElectTotEnergy;
G4double sinte = std::sin(thetaEle);
G4double coste = std::cos(thetaEle);
G4double thetaPos = u*electron_mass_c2/PositTotEnergy;
G4double sintp = std::sin(thetaPos);
G4double costp = std::cos(thetaPos);
G4double phi = twopi * rndmEngine->flat();
G4double sinp = std::sin(phi);
G4double cosp = std::cos(phi);
G4ThreeVector eDirection, pDirection;
//
// kinematic of the created pair
//
// the electron and positron are assumed to have a symetric
// angular distribution with respect to the Z axis along the parent photon.
G4double ElectKineEnergy = std::max(0.,ElectTotEnergy - electron_mass_c2);
G4ThreeVector ElectDirection (sinte*cosp, sinte*sinp, coste);
ElectDirection.rotateUz(GammaDirection);
// create G4DynamicParticle object for the particle1
GetAngularDistribution()->SamplePairDirections(aDynamicGamma,
eKinEnergy, pKinEnergy,
eDirection, pDirection);
// create G4DynamicParticle object for the particle1
G4DynamicParticle* aParticle1= new G4DynamicParticle(
theElectron,ElectDirection,ElectKineEnergy);
// the e+ is always created (even with Ekine=0) for further annihilation.
G4double PositKineEnergy = std::max(0.,PositTotEnergy - electron_mass_c2);
G4ThreeVector PositDirection (-sintp*cosp, -sintp*sinp, costp);
PositDirection.rotateUz(GammaDirection);
// create G4DynamicParticle object for the particle2
fTheElectron,eDirection,eKinEnergy);
// create G4DynamicParticle object for the particle2
G4DynamicParticle* aParticle2= new G4DynamicParticle(
thePositron,PositDirection,PositKineEnergy);
fThePositron,pDirection,pKinEnergy);
// Fill output vector
fvect->push_back(aParticle1);
fvect->push_back(aParticle2);
// kill incident photon
fParticleChange->SetProposedKineticEnergy(0.);
fParticleChange->ProposeTrackStatus(fStopAndKill);
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
// should be called only by the master and at initialisation
void G4BetheHeitlerModel::InitialiseElementData()
{
G4int size = gElementData.size();
if (size < gMaxZet+1) {
gElementData.resize(gMaxZet+1, nullptr);
}
// create for all elements that are in the detector
const G4ElementTable* elemTable = G4Element::GetElementTable();
size_t numElems = (*elemTable).size();
for (size_t ie = 0; ie < numElems; ++ie) {
const G4Element* elem = (*elemTable)[ie];
const G4int iz = std::min(gMaxZet, elem->GetZasInt());
if (!gElementData[iz]) { // create it if doesn't exist yet
G4double FZLow = 8.*elem->GetIonisation()->GetlogZ3();
G4double FZHigh = FZLow + 8.*elem->GetfCoulomb();
ElementData* elD = new ElementData();
elD->fDeltaMaxLow = G4Exp((42.038 - FZLow )/8.29) - 0.958;
elD->fDeltaMaxHigh = G4Exp((42.038 - FZHigh)/8.29) - 0.958;
gElementData[iz] = elD;
}
}
}
source/processes/electromagnetic/standard/src/G4DipBustGenerator.cc
+63 -60
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4DipBustGenerator.cc 74581 2013-10-15 12:03:25Z gcosmo $
// $Id: G4DipBustGenerator.cc 110415 2018-05-23 06:44:31Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -51,94 +51,95 @@
//
#include "G4DipBustGenerator.hh"
#include "G4PhysicalConstants.hh"
#include "Randomize.hh"
#include "G4Log.hh"
#include "G4Exp.hh"
#include <CLHEP/Units/PhysicalConstants.h>
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4DipBustGenerator::G4DipBustGenerator(const G4String&)
: G4VEmAngularDistribution("DipBustGen")
{}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4DipBustGenerator::~G4DipBustGenerator()
{}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4double G4DipBustGenerator::SampleCosTheta(G4double kinEnergy)
{
G4double c = 4. - 8.*G4UniformRand();
G4double delta = 0.5*(std::sqrt(c*c+4.) + std::abs(c));
G4double signc = (c < 0.) ? -1.0 : 1.0;
G4double cofA = -signc*G4Exp(G4Log(delta)/3.0);
G4double cosTheta = cofA - 1./cofA;
G4double tau = kinEnergy/CLHEP::electron_mass_c2;
G4double beta = std::sqrt(tau*(tau + 2.))/(tau + 1.);
return (cosTheta + beta)/(1 + cosTheta*beta);
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4ThreeVector&
G4DipBustGenerator::SampleDirection(const G4DynamicParticle* dp,
G4double, G4int, const G4Material*)
{
G4double a, c, cosTheta, delta, cofA, signc = 1.;
G4double eTkin = dp->GetKineticEnergy();
c = 4. - 8.*G4UniformRand();
a = c;
if( c < 0. )
{
signc = -1.;
a = -c;
}
delta = std::sqrt(a*a+4.);
delta += a;
delta *= 0.5;
cofA = -signc*G4Exp(G4Log(delta)/3.0);
cosTheta = cofA - 1./cofA;
G4double tau = eTkin/electron_mass_c2;
G4double beta = std::sqrt(tau*(tau + 2.))/(tau + 1.);
cosTheta = (cosTheta + beta)/(1 + cosTheta*beta);
G4double cosTheta = SampleCosTheta(dp->GetKineticEnergy());
G4double sinTheta = std::sqrt((1 - cosTheta)*(1 + cosTheta));
G4double phi = twopi*G4UniformRand();
G4double phi = CLHEP::twopi*G4UniformRand();
fLocalDirection.set(sinTheta*std::cos(phi), sinTheta*std::sin(phi),cosTheta);
fLocalDirection.rotateUz(dp->GetMomentumDirection());
return fLocalDirection;
}
G4double G4DipBustGenerator::PolarAngle(const G4double eTkin,
const G4double, // final_energy
const G4int ) // Z
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4double G4DipBustGenerator::PolarAngle(G4double eTkin,
G4double, // final_energy
G4int ) // Z
{
G4double c, cosTheta, delta, cofA, signc = 1., a;
G4double gamma, beta, theta;
c = 4. - 8.*G4UniformRand();
a = c;
if( c < 0. )
{
signc = -1.;
a = -c;
}
delta = std::sqrt(a*a+4.);
delta += a;
delta *= 0.5;
cofA = -signc*G4Exp(G4Log(delta)/3.0);
cosTheta = cofA - 1./cofA;
gamma = 1. + eTkin/electron_mass_c2;
beta = std::sqrt(1. - 1./gamma/gamma);
cosTheta = (cosTheta + beta)/(1 + cosTheta*beta);
theta = std::acos(cosTheta);
if( theta < 0. ) theta = 0.;
if( theta > pi ) theta = pi;
// G4cout <<"theta = "<<theta<<"; ";
G4double cosTheta = SampleCosTheta(eTkin);
G4double theta = std::acos(cosTheta);
theta = std::min(std::max(theta, 0.), CLHEP::pi);
return theta;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4DipBustGenerator::SamplePairDirections(const G4DynamicParticle* dp,
G4double elecKinEnergy,
G4double posiKinEnergy,
G4ThreeVector& dirElectron,
G4ThreeVector& dirPositron,
G4int, const G4Material*)
{
G4double phi = CLHEP::twopi * G4UniformRand();
G4double sinp = std::sin(phi);
G4double cosp = std::cos(phi);
G4double cost = SampleCosTheta(elecKinEnergy);
G4double sint = std::sqrt((1. - cost)*(1. + cost));
dirElectron.set(sint*cosp, sint*sinp, cost);
dirElectron.rotateUz(dp->GetMomentumDirection());
cost = SampleCosTheta(posiKinEnergy);
sint = std::sqrt((1. - cost)*(1. + cost));
dirPositron.set(-sint*cosp, -sint*sinp, cost);
dirPositron.rotateUz(dp->GetMomentumDirection());
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4DipBustGenerator::PrintGeneratorInformation() const
{
G4cout << "\n" << G4endl;
@@ -146,3 +147,5 @@ void G4DipBustGenerator::PrintGeneratorInformation() const
G4cout << "J.D. Jackson, Classical Electrodynamics, Wiley, New York 1975"
<< G4endl;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
source/processes/electromagnetic/standard/src/G4GSMottCorrection.cc
+2 -1
View File
@@ -35,6 +35,7 @@
// Creation date: 23.08.2017
//
// Modifications:
// 02.02.2018 M.Novak: fixed initialization of first moment correction.
//
// Class description: see the header file.
//
@@ -472,7 +473,7 @@ void G4GSMottCorrection::InitMCDataMaterial(const G4Material *mat) {
// screening parameter (= (mc^2)^\alpha^2/(4(pc)^2C_{TF}^2) dumScr
G4double scrCorTed = constFactor*dumScr/(4.*pt2);
G4double dum0 = G4Log(1.+1./scrCorTed);
perMatPerEkin->fMCFirstMoment = perMatPerEkin->fMCFirstMoment/(zs*(dum0-1./(1.-scrCorTed)));
perMatPerEkin->fMCFirstMoment = perMatPerEkin->fMCFirstMoment/(zs*(dum0-1./(1.+scrCorTed)));
//
// 3. the remaining part of the second moment correction and divide by the one computed by using the corrected
// screening parameter
source/processes/electromagnetic/standard/src/G4GSPWACorrections.cc
+2 -1
View File
@@ -35,6 +35,7 @@
// Creation date: 17.10.2017
//
// Modifications:
// 02.02.2018 M.Novak: fixed initialization of first moment correction.
//
// Class description: see the header file.
//
@@ -329,7 +330,7 @@ void G4GSPWACorrections::InitDataMaterial(const G4Material *mat) {
// screening parameter (= (mc^2)^\alpha^2/(4(pc)^2C_{TF}^2) dumScr
G4double scrCorTed = constFactor*dumScr/(4.*pt2);
G4double dum0 = G4Log(1.+1./scrCorTed);
perMat->fCorFirstMoment[iek] = perMat->fCorFirstMoment[iek]/(zs*(dum0-1./(1.-scrCorTed)));
perMat->fCorFirstMoment[iek] = perMat->fCorFirstMoment[iek]/(zs*(dum0-1./(1.+scrCorTed)));
//
// 3. the remaining part of the second moment correction and divide by the one computed by using the corrected
// screening parameter
source/processes/electromagnetic/standard/src/G4GoudsmitSaundersonMscModel.cc
+60 -3
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4GoudsmitSaundersonMscModel.cc 106953 2017-10-31 08:30:13Z gcosmo $
// $Id: G4GoudsmitSaundersonMscModel.cc 108305 2018-02-02 13:08:43Z gcosmo $
//
// ----------------------------------------------------------------------------
//
@@ -105,6 +105,7 @@
// # fUseSafety corresponds to Urban's fUseSafety
// # fUseDistanceToBoundary corresponds to Urban's fUseDistanceToBoundary
// # fUseSafetyPlus corresponds to the error-free stepping algorithm
// 02.02.2018 M. Novak: implemented CrossSectionPerVolume interface method (used only for testing)
//
// Class description:
// Kawrakow-Bielajew Goudsmit-Saunderson MSC model based on the screened Rutherford DCS
@@ -253,7 +254,6 @@ G4GoudsmitSaundersonMscModel::~G4GoudsmitSaundersonMscModel() {
void G4GoudsmitSaundersonMscModel::Initialise(const G4ParticleDefinition* p, const G4DataVector&) {
SetParticle(p);
fParticleChange = GetParticleChangeForMSC(p);
// -create GoudsmitSaundersonTable and init its Mott-correction member if
// Mott-correction was required
if (IsMaster()) {
@@ -292,10 +292,11 @@ void G4GoudsmitSaundersonMscModel::Initialise(const G4ParticleDefinition* p, con
fGSTable->Initialise(LowEnergyLimit(),HighEnergyLimit());
// create PWA corrections table if it was requested (and not disactivated because active Mott-correction)
if (fIsUsePWACorrection) {
fPWACorrection = new G4GSPWACorrections();
fPWACorrection = new G4GSPWACorrections(isElectron);
fPWACorrection->Initialise();
}
}
fParticleChange = GetParticleChangeForMSC(p);
}
@@ -307,6 +308,62 @@ void G4GoudsmitSaundersonMscModel::InitialiseLocal(const G4ParticleDefinition*,
}
// computes macroscopic first transport cross section: used only in testing not during mc transport
G4double G4GoudsmitSaundersonMscModel::CrossSectionPerVolume(const G4Material* mat,
const G4ParticleDefinition*,
G4double kineticEnergy,
G4double,
G4double) {
G4double xsecTr1 = 0.; // cross section per volume i.e. macroscopic 1st transport cross section
G4double efEnergy = kineticEnergy;
//
fLambda0 = 0.0; // elastic mean free path
fLambda1 = 0.0; // first transport mean free path
fScrA = 0.0; // screening parameter
fG1 = 0.0; // first transport coef.
// use Moliere's screening (with Mott-corretion if it was requested)
if (efEnergy<10.*CLHEP::eV) efEnergy = 10.*CLHEP::eV;
// total mometum square
G4double pt2 = efEnergy*(efEnergy+2.0*electron_mass_c2);
// beta square
G4double beta2 = pt2/(pt2+electron_mass_c2*electron_mass_c2);
// current material index
G4int matindx = mat->GetIndex();
// Moliere's b_c
G4double bc = fGSTable->GetMoliereBc(matindx);
// get the Mott-correcton factors if Mott-correcton was requested by the user
fMCtoScrA = 1.0;
fMCtoQ1 = 1.0;
fMCtoG2PerG1 = 1.0;
G4double scpCor = 1.0;
if (fIsUseMottCorrection) {
fGSTable->GetMottCorrectionFactors(G4Log(efEnergy), beta2, matindx, fMCtoScrA, fMCtoQ1, fMCtoG2PerG1);
// ! no scattering power correction since the current couple is not set before this interface method is called
// scpCor = fGSTable->ComputeScatteringPowerCorrection(currentCouple, efEnergy);
} else if (fIsUsePWACorrection) {
fPWACorrection->GetPWACorrectionFactors(G4Log(efEnergy), beta2, matindx, fMCtoScrA, fMCtoQ1, fMCtoG2PerG1);
// scpCor = fGSTable->ComputeScatteringPowerCorrection(currentCouple, efEnergy);
}
// screening parameter:
// - if Mott-corretioncorrection: the Screened-Rutherford times Mott-corretion DCS with this
// screening parameter gives back the (elsepa) PWA first transport cross section
// - if PWA correction: he Screened-Rutherford DCS with this screening parameter
// gives back the (elsepa) PWA first transport cross section
fScrA = fGSTable->GetMoliereXc2(matindx)/(4.0*pt2*bc)*fMCtoScrA;
// elastic mean free path in Geant4 internal lenght units: the neglected (1+screening parameter) term is corrected
// (if Mott-corretion: the corrected screening parameter is used for this (1+A) correction + Moliere b_c is also
// corrected with the screening parameter correction)
fLambda0 = beta2*(1.+fScrA)*fMCtoScrA/bc/scpCor;
// first transport coefficient (if Mott-corretion: the corrected screening parameter is used (it will be fully
// consistent with the one used during the pre-computation of the Mott-correted GS angular distributions))
fG1 = 2.0*fScrA*((1.0+fScrA)*G4Log(1.0/fScrA+1.0)-1.0);
// first transport mean free path
fLambda1 = fLambda0/fG1;
xsecTr1 = 1./fLambda1;
return xsecTr1;
}
// gives back the first transport mean free path in internal G4 units
G4double
G4GoudsmitSaundersonMscModel::GetTransportMeanFreePath(const G4ParticleDefinition* /*partdef*/,
source/processes/electromagnetic/standard/src/G4GoudsmitSaundersonTable.cc
+11 -11
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4GoudsmitSaundersonTable.cc 107234 2017-11-06 11:53:54Z gcosmo $
// $Id: G4GoudsmitSaundersonTable.cc 110527 2018-05-29 06:09:58Z gcosmo $
//
// -----------------------------------------------------------------------------
//
@@ -89,6 +89,8 @@
#include "G4MaterialCutsCouple.hh"
#include "G4ProductionCutsTable.hh"
#include "G4String.hh"
#include <fstream>
#include <cstdlib>
#include <cmath>
@@ -443,15 +445,14 @@ void G4GoudsmitSaundersonTable::LoadMSCData() {
}
//
gGSMSCAngularDistributions1.resize(gLAMBNUM*gQNUM1,nullptr);
const G4String str1 = G4String(path) + "/msc_GS/GSGrid_1/gsDistr_";
for (G4int il=0; il<gLAMBNUM; ++il) {
char fname[512];
sprintf(fname,"%s/msc_GS/GSGrid_1/gsDistr_%d",path,il);
G4String fname = str1 + std::to_string(il);
std::ifstream infile(fname,std::ios::in);
if (!infile.is_open()) {
char msgc[512];
sprintf(msgc,"Cannot open file: %s .",fname);
G4String msgc = "Cannot open file: " + fname;
G4Exception("G4GoudsmitSaundersonTable::LoadMSCData()","em0006",
FatalException, msgc);
FatalException, msgc.c_str());
return;
}
for (G4int iq=0; iq<gQNUM1; ++iq) {
@@ -474,15 +475,14 @@ void G4GoudsmitSaundersonTable::LoadMSCData() {
//
// second grid
gGSMSCAngularDistributions2.resize(gLAMBNUM*gQNUM2,nullptr);
const G4String str2 = G4String(path) + "/msc_GS/GSGrid_2/gsDistr_";
for (G4int il=0; il<gLAMBNUM; ++il) {
char fname[512];
sprintf(fname,"%s/msc_GS/GSGrid_2/gsDistr_%d",path,il);
G4String fname = str2 + std::to_string(il);
std::ifstream infile(fname,std::ios::in);
if (!infile.is_open()) {
char msgc[512];
sprintf(msgc,"Cannot open file: %s .",fname);
G4String msgc = "Cannot open file: " + fname;
G4Exception("G4GoudsmitSaundersonTable::LoadMSCData()","em0006",
FatalException, msgc);
FatalException, msgc.c_str());
return;
}
for (G4int iq=0; iq<gQNUM2; ++iq) {
source/processes/electromagnetic/standard/src/G4ICRU73QOModel.cc
+52 -11
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4ICRU73QOModel.cc 96934 2016-05-18 09:10:41Z gcosmo $
// $Id: G4ICRU73QOModel.cc 108737 2018-03-02 13:49:56Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -97,11 +97,6 @@ G4ICRU73QOModel::G4ICRU73QOModel(const G4ParticleDefinition* p, const G4String&
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4ICRU73QOModel::~G4ICRU73QOModel()
{}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
void G4ICRU73QOModel::Initialise(const G4ParticleDefinition* p,
const G4DataVector&)
{
@@ -226,7 +221,7 @@ G4double G4ICRU73QOModel::DEDX(const G4Material* material,
{
const G4Element* element = (*theElementVector)[i] ;
eloss += DEDXPerElement(element->GetZasInt(), kineticEnergy)
* theAtomicNumDensityVector[i] * element->GetZ();
* theAtomicNumDensityVector[i] * element->GetZ();
}
return eloss;
}
@@ -236,10 +231,8 @@ G4double G4ICRU73QOModel::DEDX(const G4Material* material,
G4double G4ICRU73QOModel::DEDXPerElement(G4int AtomicNumber,
G4double kineticEnergy)
{
G4int Z = AtomicNumber;
if(Z > 97) { Z = 97; }
G4int nbOfShells = GetNumberOfShells(Z);
if(nbOfShells < 1) { nbOfShells = 1; }
G4int Z = std::min(AtomicNumber, 97);
G4int nbOfShells = std::max(GetNumberOfShells(Z), 1);
G4double v = CLHEP::c_light * std::sqrt( 2.0*kineticEnergy/proton_mass_c2 );
@@ -303,6 +296,54 @@ G4double G4ICRU73QOModel::GetOscillatorEnergy(G4int Z,
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4int G4ICRU73QOModel::GetNumberOfShells(G4int Z) const
{
G4int nShell = 0;
if(indexZ[Z] >= 0) {
nShell = nbofShellsForElement[indexZ[Z]];
} else {
nShell = G4AtomicShells::GetNumberOfShells(Z);
}
return nShell;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4double G4ICRU73QOModel::GetShellEnergy(G4int Z, G4int nbOfTheShell) const
{
G4double shellEnergy = 0.;
G4int idx = indexZ[Z];
if(idx >= 0) {
shellEnergy = ShellEnergy[startElemIndex[idx] + nbOfTheShell]*CLHEP::eV;
} else {
shellEnergy = GetOscillatorEnergy(Z, nbOfTheShell);
}
return shellEnergy;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4double G4ICRU73QOModel::GetShellStrength(G4int Z, G4int nbOfTheShell) const
{
G4double shellStrength = 0.;
G4int idx = indexZ[Z];
if(idx >= 0) {
shellStrength = SubShellOccupation[startElemIndex[idx] + nbOfTheShell] / Z;
} else {
shellStrength = G4double(G4AtomicShells::GetNumberOfElectrons(Z,nbOfTheShell))/Z;
}
return shellStrength;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4double G4ICRU73QOModel::GetL0(G4double normEnergy) const
{
G4int n;
source/processes/electromagnetic/standard/src/G4LindhardSorensenData.cc
+211
View File
@@ -0,0 +1,211 @@
//
// ********************************************************************
// * License and Disclaimer *
// * *
// * The Geant4 software is copyright of the Copyright Holders of *
// * the Geant4 Collaboration. It is provided under the terms and *
// * conditions of the Geant4 Software License, included in the file *
// * LICENSE and available at http://cern.ch/geant4/license . These *
// * include a list of copyright holders. *
// * *
// * Neither the authors of this software system, nor their employing *
// * institutes,nor the agencies providing financial support for this *
// * work make any representation or warranty, express or implied, *
// * regarding this software system or assume any liability for its *
// * use. Please see the license in the file LICENSE and URL above *
// * for the full disclaimer and the limitation of liability. *
// * *
// * This code implementation is the result of the scientific and *
// * technical work of the GEANT4 collaboration. *
// * By using, copying, modifying or distributing the software (or *
// * any work based on the software) you agree to acknowledge its *
// * use in resulting scientific publications, and indicate your *
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4LindhardSorensenData.cc 95413 2016-02-10 11:45:48Z vnivanch $
//
//---------------------------------------------------------------------------
//
// GEANT4 Class file
//
// Description: Data on stopping power
//
// Description: Data on stopping power
//
// Author: Alexander Bagulya & Vladimir Ivanchenko
//
// Creation date: 23.04.2018
//
//----------------------------------------------------------------------------
//
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
#include "G4LindhardSorensenData.hh"
#include "G4PhysicsVector.hh"
#include "G4PhysicsLinearVector.hh"
#include "G4Log.hh"
#include "G4Pow.hh"
const G4int zlist[9] = {1, 10, 18, 36, 54, 66, 79, 92, 109};
const G4int LVECT = 8;
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4LindhardSorensenData::G4LindhardSorensenData()
{
g4calc = G4Pow::GetInstance();
InitialiseData();
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4LindhardSorensenData::~G4LindhardSorensenData()
{
for(G4int i=0; i<=LVECT; ++i) { delete data[i]; }
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4double G4LindhardSorensenData::GetDeltaL(G4int Z, G4double gamma) const
{
G4int idx = 0;
for(; idx<LVECT; ++idx) {
if(Z < zlist[idx+1]) { break; }
}
idx = std::min(idx, LVECT);
G4double x = G4Log(gamma - 1.0);
G4double y = ComputeDeltaL(idx, x);
// interpolation over Z if needed
if(idx < LVECT && Z > zlist[idx]) {
G4double y1 = ComputeDeltaL(idx+1, x);
y += (y1 - y)*(Z - zlist[idx])/(G4double)(zlist[idx+1] - zlist[idx]);
}
y *= g4calc->Z23(Z);
return y;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4double G4LindhardSorensenData::ComputeDeltaL(G4int idx, G4double x) const
{
G4double y(0.0);
if(x < xmin) {
G4double x1 = (data[idx])->Energy(2);
G4double ymin = (*(data[idx]))[0];
G4double y1 = (*(data[idx]))[2];
y = ymin + (y1 - ymin)*(x - xmin)/(x1 - xmin);
} else if(x > xmax) {
G4double x1 = (data[idx])->Energy(LVECT-2);
G4double ymax = (*(data[idx]))[LVECT];
G4double y1 = (*(data[idx]))[LVECT-2];
y = y1 + (ymax - y1)*(x - x1)/(xmax - x1);
} else {
y = (data[idx])->Value(x);
}
return y;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
void G4LindhardSorensenData::InitialiseData()
{
xmin = G4Log(0.02);
xmax = 2.5*g4calc->logZ(10);
const G4int NPOINT = 41;
const G4double lsdata[9][NPOINT] = {
{0.0036181621,
0.0042618872, 0.0040786701, 0.0039097273, 0.0041240731, 0.0044311195, // 0-5
0.0059858073, 0.0079655897, 0.0089669217, 0.010091248, 0.0096319233, // 5-10
0.0085344428, 0.0087326058, 0.009780094, 0.010617094, 0.011277997, // 10-15
0.01185287, 0.012242278, 0.012507042, 0.012369698, 0.012202436, // 15-20
0.012016446, 0.011793182, 0.011612196, 0.011375017, 0.010624408, // 20-25
0.0096685612, 0.0093765113, 0.0091152632, 0.0087458522, 0.0082645153, // 25-30
0.0068625676, 0.0046558921, 0.0021660968, -0.00072760644, -0.0062653709, // 30-35
-0.015834368, -0.03224412, -0.062296044, -0.10327705, -0.16545368},
{-0.024837796,
-0.018943357, -0.013251703, -0.007646936, -0.003751624, 7.4932758e-05, // 0-5
0.0027996278, 0.0057534909, 0.0078441157, 0.010341958, 0.012419648, // 5-10
0.01491866, 0.016403769, 0.018106955, 0.019249728, 0.020704966, // 10-15
0.021636244, 0.022526456, 0.023429501, 0.024251631, 0.024727856, // 15-20
0.024997337, 0.025225657, 0.025335138, 0.025474553, 0.025306356, // 20-25
0.025048151, 0.02467553, 0.02416496, 0.023519917, 0.022699646, // 25-30
0.020902526, 0.017645158, 0.013219058, 0.0059989118, -0.0042559395, // 30-35
-0.020223315, -0.044480728, -0.074942757, -0.11185084, -0.15264337},
{-0.04948514,
-0.039259418, -0.029641846, -0.022112859, -0.0152972, -0.0077213168, // 0-5
-0.0031032447, 0.0023506153, 0.0058573025, 0.0097554723, 0.012692892, // 5-10
0.016404575, 0.018642388, 0.021492082, 0.023328047, 0.025358859, // 10-15
0.026839018, 0.028169751, 0.029240668, 0.030035325, 0.030689491, // 15-20
0.031113343, 0.031518392, 0.031657748, 0.031794607, 0.031672646, // 20-25
0.031507453, 0.031024952, 0.030410522, 0.029266343, 0.027729316, // 25-30
0.025132583, 0.02141173, 0.016127626, 0.008039769, -0.0046793613, // 30-35
-0.02196456, -0.043877567, -0.070852217, -0.09979099, -0.13187648},
{-0.07502957,
-0.063927817, -0.053895181, -0.043621797, -0.033329203, -0.024765223, // 0-5
-0.015996122, -0.0084995741, -0.00017499271, 0.0064195209, 0.01117532, // 5-10
0.016956954, 0.02155737, 0.025213602, 0.029869549, 0.031980316, // 10-15
0.034664781, 0.036995048, 0.038244843, 0.039836367, 0.040930356, // 15-20
0.041677336, 0.042211864, 0.042472572, 0.042617755, 0.042393662, // 20-25
0.042049893, 0.041341375, 0.040408112, 0.03867031, 0.036457345, // 25-30
0.032742289, 0.027897265, 0.020305954, 0.0099602019, -0.0036658833, // 30-35
-0.020344557, -0.039700638, -0.059781744, -0.080649004, -0.10263347},
{-0.081885964,
-0.072049323, -0.06299877, -0.053400445, -0.043830227, -0.03415406, // 0-5
-0.024723298, -0.015706543, -0.0070305988, 0.0016621818, 0.0093560784, // 5-10
0.017338568, 0.023286722, 0.028930541, 0.034048359, 0.037750635, // 10-15
0.041512165, 0.04362858, 0.046323682, 0.048044285, 0.049379817, // 15-20
0.050501289, 0.050963981, 0.051463496, 0.051292532, 0.051074821, // 20-25
0.050350498, 0.049370817, 0.047660517, 0.045247985, 0.04188952, // 25-30
0.037009647, 0.030171627, 0.021186013, 0.0092064517, -0.0051358689, // 30-35
-0.01977885, -0.036354277, -0.053187271, -0.069851489, -0.087776477},
{-0.083068958,
-0.074302116, -0.065040071, -0.056500699, -0.047189921, -0.03781489, // 0-5
-0.028666422, -0.0192974, -0.0097949279, -0.0011649946, 0.0071301285, // 5-10
0.01548354, 0.023483416, 0.030515545, 0.036162102, 0.040602642, // 10-15
0.045011738, 0.048259036, 0.051136495, 0.053524791, 0.054971064, // 15-20
0.056247898, 0.056729496, 0.057135059, 0.056923775, 0.05657171, // 20-25
0.055504504, 0.054134086, 0.051812977, 0.048857213, 0.044525663, // 25-30
0.038593442, 0.03027527, 0.020452704, 0.0082978722, -0.0045556908, // 30-35
-0.018750622, -0.033642805, -0.048788529, -0.064509221, -0.080215679},
{-0.083061344,
-0.075180377, -0.066735793, -0.059067728, -0.049303999, -0.040618218, // 0-5
-0.031608369, -0.022553882, -0.012699373, -0.0033434259, 0.0051129584, // 5-10
0.013817276, 0.023132109, 0.030886148, 0.037688311, 0.043478106, // 10-15
0.048602814, 0.052502168, 0.055969817, 0.058142903, 0.060860174, // 15-20
0.061732795, 0.062844014, 0.062911637, 0.06278651, 0.061898673, // 20-25
0.060500452, 0.058323088, 0.055297604, 0.051242701, 0.04596475, // 25-30
0.038863441, 0.030302781, 0.019055839, 0.0072837125, -0.0047516889, // 30-35
-0.017733076, -0.031547911, -0.04523347, -0.059727542, -0.074202114},
{-0.082449782,
-0.07492693, -0.067041495, -0.059614338, -0.051061455, -0.042587329, // 0-5
-0.034242658, -0.025296495, -0.016157818, -0.0064198954, 0.0033148315, // 5-10
0.012927383, 0.021914897, 0.03053429, 0.03854699, 0.045293871, // 10-15
0.05141546, 0.056473799, 0.060050334, 0.063292547, 0.065215264, // 15-20
0.066961692, 0.067369593, 0.067623539, 0.066825274, 0.065740573, // 20-25
0.063673411, 0.061033708, 0.057399807, 0.052544441, 0.04583072, // 25-30
0.037931379, 0.028569029, 0.017544895, 0.0068751554, -0.0038105519, // 30-35
-0.015233268, -0.026956839, -0.038981068, -0.05091927, -0.064344384},
{-0.081232852,
-0.074976912, -0.068421001, -0.060951614, -0.053624488, -0.045755024, // 0-5
-0.037708151, -0.029246587, -0.02018635, -0.01073862, -0.00085387172, // 5-10
0.0090831897, 0.018970381, 0.02761289, 0.036215831, 0.044355404, // 10-15
0.051067631, 0.057143777, 0.061348214, 0.065462308, 0.06715594, // 15-20
0.069155687, 0.069845259, 0.069828188, 0.069170195, 0.067585183, // 20-25
0.065486015, 0.062437523, 0.058111347, 0.052410482, 0.045597673, // 25-30
0.037571853, 0.028019555, 0.016564385, 0.0060254421, -0.0043254115, // 30-35
-0.015675051, -0.027353574, -0.03931666, -0.050325729, -0.06174447}};
for(G4int i=0; i<=LVECT; ++i) {
data[i] = new G4PhysicsLinearVector(xmin, xmax, NPOINT-1);
for(size_t j=0; j<NPOINT; ++j) {
data[i]->PutValue(j, lsdata[i][j]);
}
}
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
source/processes/electromagnetic/standard/src/G4LindhardSorensenIonModel.cc
+440
View File
@@ -0,0 +1,440 @@
//
// ********************************************************************
// * License and Disclaimer *
// * *
// * The Geant4 software is copyright of the Copyright Holders of *
// * the Geant4 Collaboration. It is provided under the terms and *
// * conditions of the Geant4 Software License, included in the file *
// * LICENSE and available at http://cern.ch/geant4/license . These *
// * include a list of copyright holders. *
// * *
// * Neither the authors of this software system, nor their employing *
// * institutes,nor the agencies providing financial support for this *
// * work make any representation or warranty, express or implied, *
// * regarding this software system or assume any liability for its *
// * use. Please see the license in the file LICENSE and URL above *
// * for the full disclaimer and the limitation of liability. *
// * *
// * This code implementation is the result of the scientific and *
// * technical work of the GEANT4 collaboration. *
// * By using, copying, modifying or distributing the software (or *
// * any work based on the software) you agree to acknowledge its *
// * use in resulting scientific publications, and indicate your *
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4LindhardSorensenIonModel.cc 108805 2018-03-07 18:58:45Z vnivanch $
//
// -------------------------------------------------------------------
//
// GEANT4 Class header file
//
//
// File name: G4LindhardSorensenIonModel
//
// Author: Alexander Bagulya & Vladimir Ivanchenko
//
// Creation date: 16.04.2018
//
//
// -------------------------------------------------------------------
//
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
#include "G4LindhardSorensenIonModel.hh"
#include "Randomize.hh"
#include "G4PhysicalConstants.hh"
#include "G4SystemOfUnits.hh"
#include "G4Electron.hh"
#include "G4LossTableManager.hh"
#include "G4EmCorrections.hh"
#include "G4ParticleChangeForLoss.hh"
#include "G4Log.hh"
#include "G4DeltaAngle.hh"
#include "G4LindhardSorensenData.hh"
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
using namespace std;
G4LindhardSorensenData* G4LindhardSorensenIonModel::lsdata = nullptr;
G4LindhardSorensenIonModel::G4LindhardSorensenIonModel(const G4ParticleDefinition*,
const G4String& nam)
: G4VEmModel(nam),
particle(nullptr),
tlimit(DBL_MAX),
twoln10(2.0*G4Log(10.0))
{
fParticleChange = nullptr;
theElectron = G4Electron::Electron();
SetParticle(theElectron);
corr = G4LossTableManager::Instance()->EmCorrections();
nist = G4NistManager::Instance();
SetLowEnergyLimit(2.0*MeV);
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4LindhardSorensenIonModel::~G4LindhardSorensenIonModel()
{}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
void G4LindhardSorensenIonModel::Initialise(const G4ParticleDefinition* p,
const G4DataVector&)
{
SetParticle(p);
//G4cout << "G4LindhardSorensenIonModel::Initialise for " << p->GetParticleName()
// << G4endl;
// always false before the run
SetDeexcitationFlag(false);
if(nullptr == fParticleChange) {
fParticleChange = GetParticleChangeForLoss();
if(UseAngularGeneratorFlag() && !GetAngularDistribution()) {
SetAngularDistribution(new G4DeltaAngle());
}
}
if(IsMaster() && !lsdata) {
lsdata = new G4LindhardSorensenData();
}
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4double
G4LindhardSorensenIonModel::GetChargeSquareRatio(const G4ParticleDefinition*,
const G4Material*,
G4double)
{
return chargeSquare;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4double
G4LindhardSorensenIonModel::GetParticleCharge(const G4ParticleDefinition*,
const G4Material*,
G4double)
{
return charge;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4LindhardSorensenIonModel::SetupParameters()
{
mass = particle->GetPDGMass();
spin = particle->GetPDGSpin();
charge = particle->GetPDGCharge()*inveplus;
Zin = G4lrint(charge);
chargeSquare = charge*charge;
ratio = electron_mass_c2/mass;
static const G4double aMag = 1./(0.5*eplus*hbar_Planck*c_squared);
G4double magmom = particle->GetPDGMagneticMoment()*mass*aMag;
magMoment2 = magmom*magmom - 1.0;
if(Zin <= 1) {
formfact = (spin == 0.0 && mass < GeV) ? 1.181e-6 : 1.548e-6;
} else {
G4double x = nist->GetA27(Zin);
formfact = 3.969e-6*x*x;
}
tlimit = std::sqrt(0.414/formfact +
electron_mass_c2*electron_mass_c2) - electron_mass_c2;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4double G4LindhardSorensenIonModel::MinEnergyCut(const G4ParticleDefinition*,
const G4MaterialCutsCouple* couple)
{
return couple->GetMaterial()->GetIonisation()->GetMeanExcitationEnergy();
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4double
G4LindhardSorensenIonModel::ComputeCrossSectionPerElectron(
const G4ParticleDefinition* p,
G4double kineticEnergy,
G4double cutEnergy,
G4double maxKinEnergy)
{
G4double cross = 0.0;
G4double tmax = MaxSecondaryEnergy(p, kineticEnergy);
G4double maxEnergy = std::min(tmax,maxKinEnergy);
if(cutEnergy < maxEnergy) {
G4double totEnergy = kineticEnergy + mass;
G4double energy2 = totEnergy*totEnergy;
G4double beta2 = kineticEnergy*(kineticEnergy + 2.0*mass)/energy2;
cross = (maxEnergy - cutEnergy)/(cutEnergy*maxEnergy)
- beta2*G4Log(maxEnergy/cutEnergy)/tmax;
// +term for spin=1/2 particle
if( 0.0 < spin ) { cross += 0.5*(maxEnergy - cutEnergy)/energy2; }
cross *= twopi_mc2_rcl2*chargeSquare/beta2;
}
// G4cout << "BB: e= " << kineticEnergy << " tmin= " << cutEnergy
// << " tmax= " << tmax << " cross= " << cross << G4endl;
return cross;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4double G4LindhardSorensenIonModel::ComputeCrossSectionPerAtom(
const G4ParticleDefinition* p,
G4double kineticEnergy,
G4double Z, G4double,
G4double cutEnergy,
G4double maxEnergy)
{
G4double cross = Z*ComputeCrossSectionPerElectron
(p,kineticEnergy,cutEnergy,maxEnergy);
return cross;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4double G4LindhardSorensenIonModel::CrossSectionPerVolume(
const G4Material* material,
const G4ParticleDefinition* p,
G4double kineticEnergy,
G4double cutEnergy,
G4double maxEnergy)
{
G4double eDensity = material->GetElectronDensity();
G4double cross = eDensity*ComputeCrossSectionPerElectron
(p,kineticEnergy,cutEnergy,maxEnergy);
return cross;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4double
G4LindhardSorensenIonModel::ComputeDEDXPerVolume(const G4Material* material,
const G4ParticleDefinition* p,
G4double kineticEnergy,
G4double cut)
{
G4double tmax = MaxSecondaryEnergy(p, kineticEnergy);
G4double cutEnergy = std::min(cut,tmax);
G4double tau = kineticEnergy/mass;
G4double gam = tau + 1.0;
G4double bg2 = tau * (tau+2.0);
G4double beta2 = bg2/(gam*gam);
G4double eexc = material->GetIonisation()->GetMeanExcitationEnergy();
G4double eexc2 = eexc*eexc;
G4double eDensity = material->GetElectronDensity();
G4double dedx = G4Log(2.0*electron_mass_c2*bg2*cutEnergy/eexc2)
- (1.0 + cutEnergy/tmax)*beta2;
if(0.0 < spin) {
G4double del = 0.5*cutEnergy/(kineticEnergy + mass);
dedx += del*del;
}
// density correction
G4double x = G4Log(bg2)/twoln10;
dedx -= material->GetIonisation()->DensityCorrection(x);
// shell correction
dedx -= 2.0*corr->ShellCorrection(p,material,kineticEnergy);
//High order correction different for hadrons and ions
dedx += 2.0*corr->BarkasCorrection(p,material,kineticEnergy);
dedx = std::max(dedx, 0.0);
// now compute the total ionization loss
dedx *= twopi_mc2_rcl2*chargeSquare*eDensity/beta2;
//G4cout << "E(MeV)= " << kineticEnergy/MeV << " dedx= " << dedx
// << " " << material->GetName() << G4endl;
return dedx;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
void
G4LindhardSorensenIonModel::CorrectionsAlongStep(const G4MaterialCutsCouple* couple,
const G4DynamicParticle* dp,
G4double& eloss,
G4double&,
G4double length)
{
const G4ParticleDefinition* p = dp->GetDefinition();
SetParticle(p);
G4double eDensity = couple->GetMaterial()->GetElectronDensity();
G4double preKinEnergy = dp->GetKineticEnergy();
G4double e = preKinEnergy - eloss*0.5;
GetModelOfFluctuations()->SetParticleAndCharge(p, chargeSquare);
G4double tau = e/mass;
G4double gam = tau + 1.0;
G4double beta2 = tau * (tau+2.0)/(gam*gam);
G4double deltaL0 =
2.0*corr->BarkasCorrection (p, couple->GetMaterial(), e)*(charge-1.)/charge;
G4double deltaL = lsdata->GetDeltaL(Zin, tau);
G4double elossnew =
eloss + twopi_mc2_rcl2*chargeSquare*eDensity*(deltaL+deltaL0)*length/beta2;
/*
G4cout << "G4LindhardSorensenIonModel::CorrectionsAlongStep: E(GeV)= "
<< preKinEnergy/GeV << " eloss(MeV)= " << eloss
<< " L= " << eloss*beta2/(twopi_mc2_rcl2*chargeSquare*eDensity*length)
<< " dL0= " << deltaL0
<< " dL= " << deltaL << G4endl;
*/
if(elossnew > preKinEnergy) { elossnew = preKinEnergy; }
else if(elossnew < 0.0) { elossnew = eloss*0.5; }
eloss = elossnew;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
void G4LindhardSorensenIonModel::SampleSecondaries(
vector<G4DynamicParticle*>* vdp,
const G4MaterialCutsCouple* couple,
const G4DynamicParticle* dp,
G4double minKinEnergy,
G4double maxEnergy)
{
G4double kineticEnergy = dp->GetKineticEnergy();
G4double tmax = MaxSecondaryEnergy(dp->GetDefinition(),kineticEnergy);
G4double maxKinEnergy = std::min(maxEnergy,tmax);
if(minKinEnergy >= maxKinEnergy) { return; }
//G4cout << "G4LindhardSorensenIonModel::SampleSecondaries Emin= " << minKinEnergy
// << " Emax= " << maxKinEnergy << G4endl;
G4double totEnergy = kineticEnergy + mass;
G4double etot2 = totEnergy*totEnergy;
G4double beta2 = kineticEnergy*(kineticEnergy + 2.0*mass)/etot2;
G4double deltaKinEnergy, f;
G4double f1 = 0.0;
G4double fmax = 1.0;
if( 0.0 < spin ) { fmax += 0.5*maxKinEnergy*maxKinEnergy/etot2; }
CLHEP::HepRandomEngine* rndmEngineMod = G4Random::getTheEngine();
G4double rndm[2];
// sampling without nuclear size effect
do {
rndmEngineMod->flatArray(2, rndm);
deltaKinEnergy = minKinEnergy*maxKinEnergy
/(minKinEnergy*(1.0 - rndm[0]) + maxKinEnergy*rndm[0]);
f = 1.0 - beta2*deltaKinEnergy/tmax;
if( 0.0 < spin ) {
f1 = 0.5*deltaKinEnergy*deltaKinEnergy/etot2;
f += f1;
}
// Loop checking, 03-Aug-2015, Vladimir Ivanchenko
} while( fmax*rndm[1] > f);
// projectile formfactor - suppresion of high energy
// delta-electron production at high energy
G4double x = formfact*deltaKinEnergy*(deltaKinEnergy + 2*electron_mass_c2);
if(x > 1.e-6) {
G4double x1 = 1.0 + x;
G4double grej = 1.0/(x1*x1);
if( 0.0 < spin ) {
G4double x2 = 0.5*electron_mass_c2*deltaKinEnergy/(mass*mass);
grej *= (1.0 + magMoment2*(x2 - f1/f)/(1.0 + x2));
}
if(grej > 1.1) {
G4cout << "### G4LindhardSorensenIonModel WARNING: grej= " << grej
<< " " << dp->GetDefinition()->GetParticleName()
<< " Ekin(MeV)= " << kineticEnergy
<< " delEkin(MeV)= " << deltaKinEnergy
<< G4endl;
}
if(rndmEngineMod->flat() > grej) { return; }
}
G4ThreeVector deltaDirection;
if(UseAngularGeneratorFlag()) {
const G4Material* mat = couple->GetMaterial();
G4int Z = SelectRandomAtomNumber(mat);
deltaDirection =
GetAngularDistribution()->SampleDirection(dp, deltaKinEnergy, Z, mat);
} else {
G4double deltaMomentum =
sqrt(deltaKinEnergy * (deltaKinEnergy + 2.0*electron_mass_c2));
G4double cost = deltaKinEnergy * (totEnergy + electron_mass_c2) /
(deltaMomentum * dp->GetTotalMomentum());
if(cost > 1.0) { cost = 1.0; }
G4double sint = sqrt((1.0 - cost)*(1.0 + cost));
G4double phi = twopi*rndmEngineMod->flat();
deltaDirection.set(sint*cos(phi),sint*sin(phi), cost) ;
deltaDirection.rotateUz(dp->GetMomentumDirection());
}
/*
G4cout << "### G4LindhardSorensenIonModel "
<< dp->GetDefinition()->GetParticleName()
<< " Ekin(MeV)= " << kineticEnergy
<< " delEkin(MeV)= " << deltaKinEnergy
<< " tmin(MeV)= " << minKinEnergy
<< " tmax(MeV)= " << maxKinEnergy
<< " dir= " << dp->GetMomentumDirection()
<< " dirDelta= " << deltaDirection
<< G4endl;
*/
// create G4DynamicParticle object for delta ray
G4DynamicParticle* delta =
new G4DynamicParticle(theElectron,deltaDirection,deltaKinEnergy);
vdp->push_back(delta);
// Change kinematics of primary particle
kineticEnergy -= deltaKinEnergy;
G4ThreeVector finalP = dp->GetMomentum() - delta->GetMomentum();
finalP = finalP.unit();
fParticleChange->SetProposedKineticEnergy(kineticEnergy);
fParticleChange->SetProposedMomentumDirection(finalP);
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4double
G4LindhardSorensenIonModel::MaxSecondaryEnergy(const G4ParticleDefinition* pd,
G4double kinEnergy)
{
// here particle type is checked for any method
SetParticle(pd);
G4double tau = kinEnergy/mass;
G4double tmax = 2.0*electron_mass_c2*tau*(tau + 2.) /
(1. + 2.0*(tau + 1.)*ratio + ratio*ratio);
return std::min(tmax,tlimit);
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
source/processes/electromagnetic/standard/src/G4ModifiedTsai.cc
+64 -22
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4ModifiedTsai.cc 91726 2015-08-03 15:41:36Z gcosmo $
// $Id: G4ModifiedTsai.cc 110415 2018-05-23 06:44:31Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -57,42 +57,29 @@
//
#include "G4ModifiedTsai.hh"
#include "G4PhysicalConstants.hh"
#include "Randomize.hh"
#include "G4Log.hh"
#include <CLHEP/Units/PhysicalConstants.h>
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4ModifiedTsai::G4ModifiedTsai(const G4String&)
: G4VEmAngularDistribution("AngularGenUrban")
{}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4ModifiedTsai::~G4ModifiedTsai()
{}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4ThreeVector&
G4ModifiedTsai::SampleDirection(const G4DynamicParticle* dp,
G4double, G4int, const G4Material*)
{
// Sample gamma angle (Z - axis along the parent particle).
// Universal distribution suggested by L. Urban (Geant3 manual (1993)
// Phys211) derived from Tsai distribution (Rev Mod Phys 49,421(1977))
G4double uMax = 2*(1. + dp->GetKineticEnergy()/electron_mass_c2);
static const G4double a1 = 0.625;
static const G4double a2 = 1.875;
static const G4double border = 0.25;
G4double u;
do {
u = - G4Log(G4UniformRand()*G4UniformRand());
if ( border > G4UniformRand() ) { u /= a1; }
else { u /= a2; }
// Loop checking, 03-Aug-2015, Vladimir Ivanchenko
} while(u > uMax);
G4double cost = 1.0 - 2*u*u/(uMax*uMax);
G4double cost = SampleCosTheta(dp->GetKineticEnergy());
G4double sint = std::sqrt((1 - cost)*(1 + cost));
G4double phi = CLHEP::twopi*G4UniformRand();
@@ -102,6 +89,59 @@ G4ModifiedTsai::SampleDirection(const G4DynamicParticle* dp,
return fLocalDirection;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4double G4ModifiedTsai::SampleCosTheta(G4double kinEnergy)
{
// Universal distribution suggested by L. Urban (Geant3 manual (1993)
// Phys211) derived from Tsai distribution (Rev Mod Phys 49,421(1977))
G4double uMax = 2*(1. + kinEnergy/CLHEP::electron_mass_c2);
static const G4double a1 = 1.6;
static const G4double a2 = a1/3.;
static const G4double border = 0.25;
G4double u;
CLHEP::HepRandomEngine* rndmEngine = G4Random::getTheEngine();
do {
G4double uu = -G4Log(rndmEngine->flat()*rndmEngine->flat());
u = (border > rndmEngine->flat()) ? uu*a1 : uu*a2;
// Loop checking, 03-Aug-2015, Vladimir Ivanchenko
} while(u > uMax);
return 1.0 - 2.0*u*u/(uMax*uMax);
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4ModifiedTsai::SamplePairDirections(const G4DynamicParticle* dp,
G4double elecKinEnergy,
G4double posiKinEnergy,
G4ThreeVector& dirElectron,
G4ThreeVector& dirPositron,
G4int, const G4Material*)
{
G4double phi = CLHEP::twopi * G4UniformRand();
G4double sinp = std::sin(phi);
G4double cosp = std::cos(phi);
G4double cost = SampleCosTheta(elecKinEnergy);
G4double sint = std::sqrt((1. - cost)*(1. + cost));
dirElectron.set(sint*cosp, sint*sinp, cost);
dirElectron.rotateUz(dp->GetMomentumDirection());
cost = SampleCosTheta(posiKinEnergy);
sint = std::sqrt((1. - cost)*(1. + cost));
dirPositron.set(-sint*cosp, -sint*sinp, cost);
dirPositron.rotateUz(dp->GetMomentumDirection());
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4ModifiedTsai::PrintGeneratorInformation() const
{
G4cout << "\n" << G4endl;
@@ -111,3 +151,5 @@ void G4ModifiedTsai::PrintGeneratorInformation() const
G4cout << "Derived from Tsai distribution (Rev Mod Phys 49,421(1977)) \n"
<< G4endl;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
source/processes/electromagnetic/standard/src/G4PAIxSection.cc
+5 -3
View File
@@ -24,7 +24,7 @@
// ********************************************************************
//
//
// $Id: G4PAIxSection.cc 106442 2017-10-10 08:00:30Z gcosmo $
// $Id: G4PAIxSection.cc 108737 2018-03-02 13:49:56Z gcosmo $
// GEANT4 tag $Name: geant4-09-03-ref-06 $
//
//
@@ -596,8 +596,10 @@ G4PAIxSection::~G4PAIxSection()
delete fMatSandiaMatrix;
}
G4double G4PAIxSection::GetLorentzFactor(G4int j) const
{
return fLorentzFactor[j];
}
////////////////////////////////////////////////////////////////////////
//
source/processes/electromagnetic/standard/src/G4PAIySection.cc
+12 -10
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4PAIySection.cc 96934 2016-05-18 09:10:41Z gcosmo $
// $Id: G4PAIySection.cc 108737 2018-03-02 13:49:56Z gcosmo $
//
//
// G4PAIySection.cc -- class implementation file
@@ -105,10 +105,12 @@ G4PAIySection::G4PAIySection()
////////////////////////////////////////////////////////////////////////////
//
// Destructor
//
G4PAIySection::~G4PAIySection()
{}
G4double G4PAIySection::GetLorentzFactor(G4int j) const
{
return fLorentzFactor[j];
}
////////////////////////////////////////////////////////////////////////
//
@@ -297,7 +299,7 @@ void G4PAIySection::InitPAI()
}
fPAItable[0][0] = fSplineNumber;
for( G4int j = 1; j < 112; j++) // for other gammas
for( G4int j = 1; j < 112; ++j) // for other gammas
{
if( j == fRefGammaNumber ) continue;
@@ -329,9 +331,9 @@ void G4PAIySection::NormShift(G4double betaGammaSq)
{
G4int i, j;
for( i = 1; i <= fIntervalNumber-1; i++ )
for( i = 1; i <= fIntervalNumber-1; ++i)
{
for( j = 1; j <= 2; j++ )
for( j = 1; j <= 2; ++j)
{
fSplineNumber = (i-1)*2 + j;
@@ -373,9 +375,9 @@ void G4PAIySection::NormShift(G4double betaGammaSq)
// Calculation of PAI differrential cross-section (1/(keV*cm))
// in the energy points near borders of energy intervals
for(G4int k=1;k<=fIntervalNumber-1;k++)
for(G4int k=1; k<=fIntervalNumber-1; ++k)
{
for(j=1;j<=2;j++)
for(j=1; j<=2; ++j)
{
i = (k-1)*2 + j;
fImPartDielectricConst[i] = fNormalizationCof*
@@ -462,7 +464,7 @@ void G4PAIySection::SplainPAI(G4double betaGammaSq)
G4double x = 2*(fDifPAIySection[i+1] - y)/(fDifPAIySection[i+1] + y);
G4double delta = 2.*(fSplineEnergy[i+1]-fSplineEnergy[i])
/(fSplineEnergy[i+1]+fSplineEnergy[i]);
/(fSplineEnergy[i+1]+fSplineEnergy[i]);
if( x < 0 )
{
source/processes/electromagnetic/standard/src/G4PairProductionRelModel.cc
+479 -345
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4PairProductionRelModel.cc 108504 2018-02-15 15:46:37Z gcosmo $
// $Id: G4PairProductionRelModel.cc 110939 2018-06-27 12:02:21Z gunter $
//
// -------------------------------------------------------------------
//
@@ -37,11 +37,14 @@
// Creation date: 02.04.2009
//
// Modifications:
//
// 20.03.17 change LPMconstant such that it gives suppression variable 's'
// that consistent to Migdal's one; fix a small bug in 'logTS1'
// computation; suppression is consistent now with the one in the
// brem. model (F.Hariri)
// 20.03.17 Change LPMconstant such that it gives suppression variable 's'
// that consistent to Migdal's one; fix a small bug in 'logTS1'
// computation; suppression is consistent now with the one in the
// brem. model (F.Hariri)
// 28-05-18 New version with improved screening function approximation, improved
// LPM function approximation, efficiency, documentation and cleanup.
// Corrected call to selecting target atom in the final state sampling.
// (M. Novak)
//
// Class Description:
//
@@ -53,9 +56,6 @@
// Wiley, 1972.
//
// -------------------------------------------------------------------
//
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
#include "G4PairProductionRelModel.hh"
#include "G4PhysicalConstants.hh"
@@ -65,264 +65,291 @@
#include "G4Positron.hh"
#include "G4ParticleChangeForGamma.hh"
#include "G4LossTableManager.hh"
#include "G4ModifiedTsai.hh"
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
using namespace std;
const G4int G4PairProductionRelModel::gMaxZet = 120;
const G4double G4PairProductionRelModel::facFel = G4Log(184.15);
const G4double G4PairProductionRelModel::facFinel = G4Log(1194.); // 1440.
// LPM constant: \alpha(mc^2)^2/(4\pi*\hbar c)
const G4double G4PairProductionRelModel::gLPMconstant =
CLHEP::fine_structure_const*CLHEP::electron_mass_c2*CLHEP::electron_mass_c2
/(4.*CLHEP::pi*CLHEP::hbarc);
const G4double G4PairProductionRelModel::preS1 = 1./(184.15*184.15);
const G4double G4PairProductionRelModel::logTwo = G4Log(2.);
// abscissas and weights of an 8 point Gauss-Legendre quadrature
// for numerical integration on [0,1]
const G4double G4PairProductionRelModel::gXGL[] = {
1.98550718e-02, 1.01666761e-01, 2.37233795e-01, 4.08282679e-01,
5.91717321e-01, 7.62766205e-01, 8.98333239e-01, 9.80144928e-01
};
const G4double G4PairProductionRelModel::gWGL[] = {
5.06142681e-02, 1.11190517e-01, 1.56853323e-01, 1.81341892e-01,
1.81341892e-01, 1.56853323e-01, 1.11190517e-01, 5.06142681e-02
};
const G4double G4PairProductionRelModel::xgi[]={ 0.0199, 0.1017, 0.2372, 0.4083,
0.5917, 0.7628, 0.8983, 0.9801 };
const G4double G4PairProductionRelModel::wgi[]={ 0.0506, 0.1112, 0.1569, 0.1813,
0.1813, 0.1569, 0.1112, 0.0506 };
const G4double G4PairProductionRelModel::Fel_light[] = {0., 5.31 , 4.79 , 4.74 , 4.71};
const G4double G4PairProductionRelModel::Finel_light[] = {0., 6.144 , 5.621 , 5.805 , 5.924};
// elastic and inelatic radiation logarithms for light elements (where the
// Thomas-Fermi model doesn't work): computed by using Dirac-Fock model of atom.
const G4double G4PairProductionRelModel::gFelLowZet [] = {
0.0, 5.3104, 4.7935, 4.7402, 4.7112, 4.6694, 4.6134, 4.5520
};
const G4double G4PairProductionRelModel::gFinelLowZet[] = {
0.0, 5.9173, 5.6125, 5.5377, 5.4728, 5.4174, 5.3688, 5.3236
};
const G4double G4PairProductionRelModel::xsfactor =
4*CLHEP::fine_structure_const*CLHEP::classic_electr_radius*CLHEP::classic_electr_radius;
const G4double G4PairProductionRelModel::Egsmall = 2.*CLHEP::MeV;
const G4double G4PairProductionRelModel::Eghigh = 100.*CLHEP::GeV;
// constant cross section factor
const G4double G4PairProductionRelModel::gXSecFactor =
4.*CLHEP::fine_structure_const*CLHEP::classic_electr_radius
*CLHEP::classic_electr_radius;
// gamma energy limit above which LPM suppression will be applied (if the
// fIsUseLPMCorrection flag is true)
const G4double G4PairProductionRelModel::gEgLPMActivation = 100.*CLHEP::GeV;
// special data structure per element i.e. per Z
std::vector<G4PairProductionRelModel::ElementData*> G4PairProductionRelModel::gElementData;
// LPM supression functions evaluated at initialisation time
G4PairProductionRelModel::LPMFuncs G4PairProductionRelModel::gLPMFuncs;
// CTR
G4PairProductionRelModel::G4PairProductionRelModel(const G4ParticleDefinition*,
const G4String& nam)
: G4VEmModel(nam),
fLPMconstant(CLHEP::fine_structure_const*CLHEP::electron_mass_c2*CLHEP::electron_mass_c2/
(4.*CLHEP::pi*CLHEP::hbarc)),
fLPMflag(true),
lpmEnergy(0.),
use_completescreening(false)
const G4String& nam)
: G4VEmModel(nam), fIsUseLPMCorrection(true), fIsUseCompleteScreening(false),
fLPMEnergy(0.), fG4Calc(G4Pow::GetInstance()), fTheGamma(G4Gamma::Gamma()),
fTheElectron(G4Electron::Electron()), fThePositron(G4Positron::Positron()),
fParticleChange(nullptr)
{
fParticleChange = nullptr;
theGamma = G4Gamma::Gamma();
thePositron = G4Positron::Positron();
theElectron = G4Electron::Electron();
g4calc = G4Pow::GetInstance();
currentZ = z13 = z23 = lnZ = Fel = Finel = fCoulomb = phiLPM = gLPM = xiLPM = 0;
SetAngularDistribution(new G4ModifiedTsai());
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
// DTR
G4PairProductionRelModel::~G4PairProductionRelModel()
{}
{
if (IsMaster()) {
// clear ElementData container
for (size_t iz = 0; iz < gElementData.size(); ++iz) {
if (gElementData[iz]) delete gElementData[iz];
}
gElementData.clear();
// clear LPMFunctions (if any)
if (fIsUseLPMCorrection) {
gLPMFuncs.fLPMFuncG.clear();
gLPMFuncs.fLPMFuncPhi.clear();
}
}
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4PairProductionRelModel::Initialise(const G4ParticleDefinition* p,
const G4DataVector& cuts)
const G4DataVector& cuts)
{
if (IsMaster()) {
// init element data and LPM funcs
if (IsMaster()) {
InitialiseElementData();
if (fIsUseLPMCorrection) {
InitLPMFunctions();
}
}
}
if(!fParticleChange) { fParticleChange = GetParticleChangeForGamma(); }
if(IsMaster() && LowEnergyLimit() < HighEnergyLimit()) {
InitialiseElementSelectors(p, cuts);
}
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4PairProductionRelModel::InitialiseLocal(const G4ParticleDefinition*,
G4VEmModel* masterModel)
G4VEmModel* masterModel)
{
if(LowEnergyLimit() < HighEnergyLimit()) {
SetElementSelectors(masterModel->GetElementSelectors());
}
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4double G4PairProductionRelModel::ComputeXSectionPerAtom(G4double totalEnergy, G4double Z)
G4double G4PairProductionRelModel::ComputeXSectionPerAtom(G4double gammaEnergy,
G4double Z)
{
G4double cross = 0.0;
// number of intervals and integration step
G4double vcut = electron_mass_c2/totalEnergy ;
// limits by the screening variable
G4double dmax = DeltaMax();
G4double dmin = std::min(DeltaMin(totalEnergy),dmax);
G4double vcut1 = 0.5 - 0.5*sqrt(1. - dmin/dmax);
vcut = max(vcut, vcut1);
G4double vmax = 0.5;
G4int n = 1; // needs optimisation
G4double delta = (vmax - vcut)*totalEnergy/G4double(n);
G4double e0 = vcut*totalEnergy;
// simple integration
for(G4int l=0; l<n; ++l) {
e0 += delta;
for(G4int i=0; i<8; ++i) {
G4double eg = (e0 + xgi[i]*delta);
G4double xs = (fLPMflag && totalEnergy > Eghigh)
? ComputeRelDXSectionPerAtom(eg,totalEnergy,Z)
: ComputeDXSectionPerAtom(eg,totalEnergy,Z);
cross += wgi[i]*xs;
G4double xSection = 0.0;
// check if LPM suppression needs to be used
const G4bool isLPM = (fIsUseLPMCorrection && gammaEnergy>gEgLPMActivation);
// determine the kinematical limits (taken into account the correction due to
// the way in which the Coulomb correction is applied i.e. avoid negative DCS)
const G4int iz = std::min(gMaxZet, G4lrint(Z));
const G4double eps0 = CLHEP::electron_mass_c2/gammaEnergy;
const G4double dmax = gElementData[iz]->fDeltaMax;
const G4double dmin = 4.*eps0*gElementData[iz]->fDeltaFactor;
const G4double eps1 = 0.5 - 0.5*std::sqrt(1.-dmin/dmax);
const G4double epsMin = std::max(eps0, eps1);
const G4double epsMax = 0.5; // DCS is symmetric around eps=0.5
// let Et be the total energy transferred to the e- or to the e+
// the [Et-min, Et-max] interval will be divided into i=1,2,..,n subintervals
// with width of dInterv = (Et-max - Et-min)/n and numerical integration will
// be done in each sub-inteval using the xi = (Et - Et_i-min)/dInterv variable
// that is in [0,1]. The 8-point GL q. is used for the integration on [0,1].
const G4int numSub = 2;
const G4double dInterv= (epsMax - epsMin)*gammaEnergy/G4double(numSub);
G4double minEti = epsMin*gammaEnergy; // Et-min i.e. Et_0-min
for (G4int i = 0; i < numSub; ++i) {
for (G4int ngl = 0; ngl < 8; ++ngl) {
const G4double Et = (minEti + gXGL[ngl]*dInterv);
const G4double xs = isLPM ? ComputeRelDXSectionPerAtom(Et, gammaEnergy, Z)
: ComputeDXSectionPerAtom(Et, gammaEnergy, Z);
xSection += gWGL[ngl]*xs;
}
// update minimum Et of the sub-inteval
minEti += dInterv;
}
cross *= delta*2.;
return cross;
// apply corrections of variable transformation and half interval integration
xSection = std::max(2.*xSection*dInterv, 0.);
return xSection;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4double
G4PairProductionRelModel::ComputeDXSectionPerAtom(G4double eplusEnergy,
G4double totalEnergy,
G4double /*Z*/)
// DCS WITHOUT LPM SUPPRESSION
// Computes DCS value for a given target element (Z), initial gamma energy (Eg),
// total energy transferred to one of the e-/e+ pair(Et) WITHOUT LPM suppression
// The constant factor 4 \alpha r_0^2 Z (Z +\eta(Z)) is not included here and
// the returned value will be differential in total energy transfer instead of
// the eps=Et/Eg. The computed part of the DCS
// NORMAL CASE: DEFAULT STTING (i.e. fIsUseCompleteScreening = FALSE)
// ds/deps(Et,Eg,Z) = ds/deps(eps,Z) = (eps^2+(1-eps)^2)*[phi1(d)/4-ln(Z)/3-fc]
// + 2*eps(1-eps)*[phi2(d)/4-ln(Z)/3-fc]/3 where the universal (in the TF model)
// screening variable d=d(eps)=136Z^(-1/3)eps0/[eps*(1-eps)] with eps0=mc^2/Eg.
// COMPLETE SCREENING (when d(eps) approx-equal-to 0) : NEED TO BE SET BY USER
// ds/deps(Et,Eg,Z) = ds/deps(eps,Z) = (eps^2+(1-eps)^2+eps*(1-eps)/3)*[Lel-fc]
// -eps(1-eps)/9 where Lel=phi1(0)/4-ln(Z)/3 is the elastic(coherent) radiation
// logarithm, fc is the Coulomb correction and the relation phi2(0)/4-ln(Z)/3 =
// phi1(0)/4-1/6-ln(Z)/3 = Lel-1/6 (due to phi2(0)=phi1(0)-2/3) was used.
G4double G4PairProductionRelModel::ComputeDXSectionPerAtom(G4double pEnergy,
G4double gammaEnergy,
G4double Z)
{
// most simple case - complete screening:
// dsig/dE+ = 4 * alpha * Z**2 * r0**2 / k
// * [ (y**2 + (1-y**2) + 2/3*y*(1-y) ) * ( log (183 * Z**-1/3) + 1/9 * y*(1-y) ]
// y = E+/k
G4double yp=eplusEnergy/totalEnergy;
G4double ym=1.-yp;
G4double cross = 0.;
if (use_completescreening)
cross = (yp*yp + ym*ym + 2./3.*ym*yp)*(Fel - fCoulomb) + yp*ym/9.;
else {
G4double delta = 0.25*DeltaMin(totalEnergy)/(yp*ym);
cross = (yp*yp + ym*ym)*(0.25*Phi1(delta) - lnZ/3. - fCoulomb)
+ 2./3.*ym*yp*(0.25*Phi2(delta) - lnZ/3. - fCoulomb);
G4double xSection = 0.;
const G4int iz = std::min(gMaxZet, G4lrint(Z));
const G4double eps = pEnergy/gammaEnergy;
const G4double epsm = 1.-eps;
const G4double dum = eps*epsm;
if (fIsUseCompleteScreening) {
// complete screening:
const G4double Lel = gElementData[iz]->fLradEl;
const G4double fc = gElementData[iz]->fCoulomb;
xSection = (eps*eps + epsm*epsm + 2.*dum/3.)*(Lel-fc) - dum/9.;
} else {
// normal case:
const G4double eps0 = CLHEP::electron_mass_c2/gammaEnergy;
const G4double fc = gElementData[iz]->fCoulomb;
const G4double lnZ13 = gElementData[iz]->fLogZ13;
const G4double delta = gElementData[iz]->fDeltaFactor*eps0/dum;
G4double phi1, phi2;
ComputePhi12(delta, phi1, phi2);
xSection = (eps*eps + epsm*epsm)*(0.25*phi1-lnZ13-fc)
+ 2.*dum*(0.25*phi2-lnZ13-fc)/3.;
}
return cross/totalEnergy;
// non-const. part of the DCS differential in total energy transfer not in eps
// ds/dEt=ds/deps deps/dEt with deps/dEt=1/Eg
return std::max(xSection, 0.0)/gammaEnergy;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4double
G4PairProductionRelModel::ComputeRelDXSectionPerAtom(G4double eplusEnergy,
G4double totalEnergy,
G4double /*Z*/)
// DCS WITH POSSIBLE LPM SUPPRESSION
// Computes DCS value for a given target element (Z), initial gamma energy (Eg),
// total energy transferred to one of the e-/e+ pair(Et) WITH LPM suppression.
// For a given Z, the LPM suppression will depend on the material through the
// LMP-Energy. This will determine the suppression variable s and the LPM sup-
// pression functions xi(s), fi(s) and G(s).
// The constant factor 4 \alpha r_0^2 Z (Z +\eta(Z)) is not included here and
// the returned value will be differential in total energy transfer instead of
// the eps=Et/Eg. The computed part of the DCS
// NORMAL CASE: DEFAULT STTING (i.e. fIsUseCompleteScreening = FALSE)
// ds/deps(Et,Eg,Z)=ds/deps(eps,Z) = xi(s)*{ (eps^2+(1-eps)^2)*[2fi(s)/3+G(s)/3]
// *[phi1(d)/4-ln(Z)/3-fc] + 2*eps(1-eps)*G(s)*[phi2(d)/4-ln(Z)/3-fc]/3 } where
// the universal (in the TF model) screening variable d=d(eps)=136Z^(-1/3)eps0
// /[eps*(1-eps)] with eps0=mc^2/Eg.
// COMPLETE SCREENING (when d(eps) approx-equal-to 0) : NEED TO BE SET BY USER
// ds/deps(Et,Eg,Z) = ds/deps(eps,Z) = xi(s)*{ [Lel-fc]*[ (eps^2+(1-eps)^2+eps
// *(1-eps)/3)*2fi(s)/3 + G(s)/3] - eps(1-eps)*G(s)/9 }
// Note, that when the LPM suppression is absent i.e. xi(s)=fi(s)=G(s)=1, both
// the normal and the complete screening DCS give back the NO-LMP case above.
G4double G4PairProductionRelModel::ComputeRelDXSectionPerAtom(G4double pEnergy,
G4double gammaEnergy,
G4double Z)
{
// most simple case - complete screening:
// dsig/dE+ = 4 * alpha * Z**2 * r0**2 / k
// * [ (y**2 + (1-y**2) + 2/3*y*(1-y) ) * ( log (183 * Z**-1/3) + 1/9 * y*(1-y) ]
// y = E+/k
G4double yp=eplusEnergy/totalEnergy;
G4double ym=1.-yp;
CalcLPMFunctions(totalEnergy,eplusEnergy); // gamma
G4double cross = 0.;
if (use_completescreening)
cross = xiLPM*(2./3.*phiLPM*(yp*yp + ym*ym) + gLPM)*(Fel - fCoulomb);
else {
G4double delta = 0.25*DeltaMin(totalEnergy)/(yp*ym);
cross = (1./3.*gLPM + 2./3.*phiLPM)*(yp*yp + ym*ym)
*(0.25*Phi1(delta) - lnZ/3. - fCoulomb)
+ 2./3.*gLPM*ym*yp*(0.25*Phi2(delta) - lnZ/3. - fCoulomb);
cross *= xiLPM;
G4double xSection = 0.;
const G4int iz = std::min(gMaxZet, G4lrint(Z));
const G4double eps = pEnergy/gammaEnergy;
const G4double epsm = 1.-eps;
const G4double dum = eps*epsm;
// evaluate LPM suppression functions
G4double fXiS, fGS, fPhiS;
ComputeLPMfunctions(fXiS, fGS, fPhiS, eps, gammaEnergy, iz);
if (fIsUseCompleteScreening) {
// complete screening:
const G4double Lel = gElementData[iz]->fLradEl;
const G4double fc = gElementData[iz]->fCoulomb;
xSection = (Lel-fc)*((eps*eps+epsm*epsm)*2.*fPhiS + fGS)/3. - dum*fGS/9.;
} else {
// normal case:
const G4double eps0 = CLHEP::electron_mass_c2/gammaEnergy;
const G4double fc = gElementData[iz]->fCoulomb;
const G4double lnZ13 = gElementData[iz]->fLogZ13;
const G4double delta = gElementData[iz]->fDeltaFactor*eps0/dum;
G4double phi1, phi2;
ComputePhi12(delta, phi1, phi2);
xSection = (eps*eps + epsm*epsm)*(2.*fPhiS+fGS)*(0.25*phi1-lnZ13-fc)/3.
+ 2.*dum*fGS*(0.25*phi2-lnZ13-fc)/3.;
}
return cross/totalEnergy;
// non-const. part of the DCS differential in total energy transfer not in eps
// ds/dEt=ds/deps deps/dEt with deps/dEt=1/Eg
return std::max(fXiS*xSection, 0.0)/gammaEnergy;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void
G4PairProductionRelModel::CalcLPMFunctions(G4double k, G4double eplusEnergy)
{
// *** calculate lpm variable s & sprime ***
// Klein eqs. (78) & (79)
G4double sprime = sqrt(0.125*k*lpmEnergy/(eplusEnergy*(k-eplusEnergy)));
G4double s1 = preS1*z23;
G4double logS1 = 2./3.*lnZ-2.*facFel;
G4double logTS1 = 0.5*logTwo+logS1;
xiLPM = 2.;
if (sprime>1)
xiLPM = 1.;
else if (sprime>sqrt(2.)*s1) {
G4double h = G4Log(sprime)/logTS1;
xiLPM = 1+h-0.08*(1-h)*(1-sqr(1-h))/logTS1;
}
G4double s0 = sprime/sqrt(xiLPM);
// G4cout<<"k="<<k<<" y="<<eplusEnergy/k<<G4endl;
// G4cout<<"s0="<<s0<<G4endl;
// *** calculate supression functions phi and G ***
// Klein eqs. (77)
G4double s2=s0*s0;
G4double s3=s0*s2;
G4double s4=s2*s2;
if (s0<0.1) {
// high suppression limit
phiLPM = 6.*s0 - 18.84955592153876*s2 + 39.47841760435743*s3
- 57.69873135166053*s4;
gLPM = 37.69911184307752*s2 - 236.8705056261446*s3 + 807.7822389*s4;
}
else if (s0<1.9516) {
// intermediate suppression
// using eq.77 approxim. valid s0<2.
phiLPM = 1.-G4Exp(-6.*s0*(1.+(3.-pi)*s0)
+s3/(0.623+0.795*s0+0.658*s2));
if (s0<0.415827397755) {
// using eq.77 approxim. valid 0.07<s<2
G4double psiLPM = 1-G4Exp(-4*s0-8*s2/(1+3.936*s0+4.97*s2-0.05*s3+7.50*s4));
gLPM = 3*psiLPM-2*phiLPM;
}
else {
// using alternative parametrisiation
G4double pre = -0.16072300849123999 + s0*3.7550300067531581 + s2*-1.7981383069010097
+ s3*0.67282686077812381 + s4*-0.1207722909879257;
gLPM = std::tanh(pre);
}
}
else {
// low suppression limit valid s>2.
phiLPM = 1. - 0.0119048/s4;
gLPM = 1. - 0.0230655/s4;
}
// *** make sure suppression is smaller than 1 ***
// *** caused by Migdal approximation in xi ***
if (xiLPM*phiLPM>1. || s0>0.57) { xiLPM=1./phiLPM; }
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4double
G4PairProductionRelModel::ComputeCrossSectionPerAtom(const G4ParticleDefinition*,
G4double gammaEnergy, G4double Z, G4double, G4double, G4double)
{
G4double crossSection = 0.0 ;
// check kinematical limit
if ( gammaEnergy <= 2.0*electron_mass_c2 ) { return crossSection; }
SetCurrentElement(Z);
// choose calculator according to parameters and switches
// in the moment only one calculator:
crossSection=ComputeXSectionPerAtom(gammaEnergy,Z);
G4double xi = Finel/(Fel - fCoulomb); // inelastic contribution
crossSection *= xsfactor*Z*(Z+xi);
return crossSection;
// Computes the cross section with or without LPM suppression depending on
// settings (by default with if the gamma energy is above a given threshold)
// and using or not using complete sreening approximation (by default not).
// Only the dependent part is computed in the numerical integration of the DCS
// i.e. the result must be multiplied here with 4 \alpha r_0^2 Z(Z+\eta(Z))
crossSection = ComputeXSectionPerAtom(gammaEnergy, Z);
// apply the constant factors:
// - eta(Z) is a correction to account interaction in the field of e-
// - gXSecFactor = 4 \alpha r_0^2
const G4int iz = std::min(gMaxZet, G4lrint(Z));
const G4double eta = gElementData[iz]->fEtaValue;
crossSection *= gXSecFactor*Z*(Z+eta);
// final protection
return std::max(crossSection, 0.);
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4PairProductionRelModel::SetupForMaterial(const G4ParticleDefinition*,
const G4Material* mat, G4double)
{
fLPMEnergy = mat->GetRadlen()*gLPMconstant;
}
void
G4PairProductionRelModel::SampleSecondaries(std::vector<G4DynamicParticle*>* fvect,
const G4MaterialCutsCouple* couple,
const G4DynamicParticle* aDynamicGamma,
G4double,
G4double)
const G4MaterialCutsCouple* couple,
const G4DynamicParticle* aDynamicGamma,
G4double,
G4double)
// The secondaries e+e- energies are sampled using the Bethe - Heitler
// cross sections with Coulomb correction.
// A modified version of the random number techniques of Butcher & Messel
@@ -336,169 +363,276 @@ G4PairProductionRelModel::SampleSecondaries(std::vector<G4DynamicParticle*>* fve
// pair creation in both nuclear and atomic electron fields.
// However triplet prodution is not generated.
{
const G4Material* aMaterial = couple->GetMaterial();
G4double GammaEnergy = aDynamicGamma->GetKineticEnergy();
G4ParticleMomentum GammaDirection = aDynamicGamma->GetMomentumDirection();
G4double epsil ;
G4double epsil0 = electron_mass_c2/GammaEnergy ;
if(epsil0 > 1.0) { return; }
SetupForMaterial(theGamma, aMaterial, GammaEnergy);
// select randomly one element constituing the material
const G4Element* anElement =
SelectRandomAtom(aMaterial, theGamma, GammaEnergy);
SetCurrentElement(anElement->GetZasInt());
const G4Material* mat = couple->GetMaterial();
const G4double gammaEnergy = aDynamicGamma->GetKineticEnergy();
const G4double eps0 = CLHEP::electron_mass_c2/gammaEnergy ;
//
// check kinematical limit: gamma energy(Eg) must be at least 2 e- rest mass
// (but the model should be used at higher energies above 100 MeV)
if (eps0 > 0.5) { return; }
//
// select target atom of the material
const G4Element* anElement = SelectRandomAtom(couple, fTheGamma, gammaEnergy);
CLHEP::HepRandomEngine* rndmEngine = G4Random::getTheEngine();
// do it fast if GammaEnergy < 2. MeV
if (GammaEnergy < Egsmall) {
epsil = epsil0 + (0.5-epsil0)*rndmEngine->flat();
} else {
// now comes the case with GammaEnergy >= 2. MeV
// Extract Coulomb factor for this Element
G4double FZ = 8.*(anElement->GetIonisation()->GetlogZ3());
static const G4double midEnergy = 50.*CLHEP::MeV;
if (GammaEnergy > midEnergy) { FZ += 8.*(anElement->GetfCoulomb()); }
// limits of the screening variable
G4double screenfac = 136.*epsil0/(anElement->GetIonisation()->GetZ3());
//F.Hariri : correct sign of last term
G4double screenmax = G4Exp ((42.24 - FZ)/8.368) + 0.952 ;
G4double screenmin = std::min(4.*screenfac, screenmax);
// limits of the energy sampling
G4double epsil1 = 0.5 - 0.5*sqrt(1. - screenmin/screenmax) ;
G4double epsilmin = std::max(epsil0, epsil1);
G4double epsilrange = 0.5 - epsilmin;
//
// sample the energy rate of the created electron (or positron)
//
//G4double epsil, screenvar, greject ;
G4double screenvar, greject ;
G4double F10 = ScreenFunction1(screenmin) - FZ;
G4double F20 = ScreenFunction2(screenmin) - FZ;
G4double NormF1 = std::max(F10*epsilrange*epsilrange,0.);
G4double NormF2 = std::max(1.5*F20,0.);
do {
if ( NormF1/(NormF1+NormF2) > rndmEngine->flat() ) {
epsil = 0.5 - epsilrange*g4calc->A13(rndmEngine->flat());
screenvar = screenfac/(epsil*(1-epsil));
if (fLPMflag && GammaEnergy > Eghigh) {
CalcLPMFunctions(GammaEnergy,GammaEnergy*epsil);
greject = xiLPM*((gLPM+2.*phiLPM)*Phi1(screenvar) -
gLPM*Phi2(screenvar) - phiLPM*FZ)/F10;
}
else {
greject = (ScreenFunction1(screenvar) - FZ)/F10;
}
//
// 'eps' is the total energy transferred to one of the e-/e+ pair in initial
// gamma energy units Eg. Since the corresponding DCS is symmetric on eps=0.5,
// the kinematical limits for eps0=mc^2/Eg <= eps <= 0.5
//
// The Coulomb factor for the target element (Z) (Eg>50 MeV is assumed)
// F(Z) = 8*ln(Z)/3 + 8*fc(Z)
//
// The screening variable 'delta(eps)' = 136*Z^{-1/3}*eps0/[eps(1-eps)]
// Due to the Coulomb correction, the DCS can go below zero even at
// kinematicaly allowed eps > eps0 values. In order to exclude this eps
// range with negative DCS, the minimum eps value will be set to eps_min =
// max[eps0, epsp] with epsp is the solution of SF(delta(epsp)) - F(Z)/2 = 0
// with SF being the screening function (SF1=SF2 at high value of delta).
// The solution is epsp = 0.5 - 0.5*sqrt[ 1 - 4*136*Z^{-1/3}eps0/deltap]
// with deltap = Exp[(42.038-F(Z))/8.29]-0.958. So the limits are:
// - when eps=eps_max = 0.5 => delta_min = 136*Z^{-1/3}*eps0/4
// - epsp = 0.5 - 0.5*sqrt[ 1 - delta_min/deltap]
// - and eps_min = max[eps0, epsp]
const G4int iZet = std::min(gMaxZet, anElement->GetZasInt());
const G4double deltaFactor = gElementData[iZet]->fDeltaFactor*eps0;
const G4double deltaMin = 4.*deltaFactor;
const G4double deltaMax = gElementData[iZet]->fDeltaMax;
// compute the limits of eps
const G4double epsp = 0.5 - 0.5*std::sqrt(1. - deltaMin/deltaMax) ;
const G4double epsMin = std::max(eps0,epsp);
const G4double epsRange = 0.5 - epsMin;
const G4double FZ = 8.*(gElementData[iZet]->fLogZ13 +
gElementData[iZet]->fCoulomb);
//
// sample the energy rate (eps) of the created electron (or positron)
G4double F10, F20;
ScreenFunction12(deltaMin, F10, F20);
F10 -= FZ;
F20 -= FZ;
const G4double NormF1 = std::max(F10 * epsRange * epsRange, 0.);
const G4double NormF2 = std::max(1.5 * F20 , 0.);
const G4double NormCond = NormF1/(NormF1 + NormF2);
// check if LPM correction is active
const G4bool isLPM = (fIsUseLPMCorrection && gammaEnergy>gEgLPMActivation);
fLPMEnergy = mat->GetRadlen()*gLPMconstant;
// we will need 3 uniform random number for each trial of sampling
G4double rndmv[3];
G4double greject = 0.;
G4double eps;
do {
rndmEngine->flatArray(3, rndmv);
if (NormCond > rndmv[0]) {
eps = 0.5 - epsRange * fG4Calc->A13(rndmv[1]);
const G4double delta = deltaFactor/(eps*(1.-eps));
if (isLPM) {
G4double lpmXiS, lpmGS, lpmPhiS, phi1, phi2;
ComputePhi12(delta, phi1, phi2);
ComputeLPMfunctions(lpmXiS, lpmGS, lpmPhiS, eps, gammaEnergy, iZet);
greject = lpmXiS*((2.*lpmPhiS+lpmGS)*phi1-lpmGS*phi2-lpmPhiS*FZ)/F10;
} else {
epsil = epsilmin + epsilrange*rndmEngine->flat();
screenvar = screenfac/(epsil*(1-epsil));
if (fLPMflag && GammaEnergy > Eghigh) {
CalcLPMFunctions(GammaEnergy,GammaEnergy*epsil);
greject = xiLPM*((0.5*gLPM+phiLPM)*Phi1(screenvar) +
0.5*gLPM*Phi2(screenvar) - 0.5*(gLPM+phiLPM)*FZ)/F20;
}
else {
greject = (ScreenFunction2(screenvar) - FZ)/F20;
}
greject = (ScreenFunction1(delta)-FZ)/F10;
}
// Loop checking, 03-Aug-2015, Vladimir Ivanchenko
} while( greject < rndmEngine->flat());
} // end of epsil sampling
} else {
eps = epsMin + epsRange*rndmv[1];
const G4double delta = deltaFactor/(eps*(1.-eps));
if (isLPM) {
G4double lpmXiS, lpmGS, lpmPhiS, phi1, phi2;
ComputePhi12(delta, phi1, phi2);
ComputeLPMfunctions(lpmXiS, lpmGS, lpmPhiS, eps, gammaEnergy, iZet);
greject = lpmXiS*( (lpmPhiS+0.5*lpmGS)*phi1 + 0.5*lpmGS*phi2
-0.5*(lpmGS+lpmPhiS)*FZ )/F20;
} else {
greject = (ScreenFunction2(delta)-FZ)/F20;
}
}
// Loop checking, 03-Aug-2015, Vladimir Ivanchenko
} while (greject < rndmv[2]);
// end of eps sampling
//
// fixe charges randomly
//
G4double ElectTotEnergy, PositTotEnergy;
// select charges randomly
G4double eTotEnergy, pTotEnergy;
if (rndmEngine->flat() > 0.5) {
ElectTotEnergy = (1.-epsil)*GammaEnergy;
PositTotEnergy = epsil*GammaEnergy;
eTotEnergy = (1.-eps)*gammaEnergy;
pTotEnergy = eps*gammaEnergy;
} else {
PositTotEnergy = (1.-epsil)*GammaEnergy;
ElectTotEnergy = epsil*GammaEnergy;
pTotEnergy = (1.-eps)*gammaEnergy;
eTotEnergy = eps*gammaEnergy;
}
//
// scattered electron (positron) angles. ( Z - axis along the parent photon)
// sample pair kinematics
//
const G4double eKinEnergy = std::max(0.,eTotEnergy - CLHEP::electron_mass_c2);
const G4double pKinEnergy = std::max(0.,pTotEnergy - CLHEP::electron_mass_c2);
//
// universal distribution suggested by L. Urban
// (Geant3 manual (1993) Phys211),
// derived from Tsai distribution (Rev Mod Phys 49,421(1977))
static const G4double a1 = 1.6;
static const G4double a2 = a1/3.;
G4double uu = -G4Log(rndmEngine->flat()*rndmEngine->flat());
G4double u = (0.25 > rndmEngine->flat()) ? uu*a1 : uu*a2;
G4double thetaEle = u*electron_mass_c2/ElectTotEnergy;
G4double sinte = std::sin(thetaEle);
G4double coste = std::cos(thetaEle);
G4double thetaPos = u*electron_mass_c2/PositTotEnergy;
G4double sintp = std::sin(thetaPos);
G4double costp = std::cos(thetaPos);
G4double phi = twopi * rndmEngine->flat();
G4double sinp = std::sin(phi);
G4double cosp = std::cos(phi);
G4ThreeVector eDirection, pDirection;
//
// kinematic of the created pair
//
// the electron and positron are assumed to have a symetric
// angular distribution with respect to the Z axis along the parent photon.
G4double ElectKineEnergy = max(0.,ElectTotEnergy - electron_mass_c2);
G4ThreeVector ElectDirection (sinte*cosp, sinte*sinp, coste);
ElectDirection.rotateUz(GammaDirection);
GetAngularDistribution()->SamplePairDirections(aDynamicGamma,
eKinEnergy, pKinEnergy,
eDirection, pDirection);
// create G4DynamicParticle object for the particle1
G4DynamicParticle* aParticle1= new G4DynamicParticle(
theElectron,ElectDirection,ElectKineEnergy);
// the e+ is always created (even with Ekine=0) for further annihilation.
G4double PositKineEnergy = std::max(0.,PositTotEnergy - electron_mass_c2);
G4ThreeVector PositDirection (-sintp*cosp, -sintp*sinp, costp);
PositDirection.rotateUz(GammaDirection);
fTheElectron,eDirection,eKinEnergy);
// create G4DynamicParticle object for the particle2
G4DynamicParticle* aParticle2= new G4DynamicParticle(
thePositron,PositDirection,PositKineEnergy);
fThePositron,pDirection,pKinEnergy);
// Fill output vector
fvect->push_back(aParticle1);
fvect->push_back(aParticle2);
// kill incident photon
fParticleChange->SetProposedKineticEnergy(0.);
fParticleChange->ProposeTrackStatus(fStopAndKill);
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
void G4PairProductionRelModel::SetupForMaterial(const G4ParticleDefinition*,
const G4Material* mat, G4double)
// should be called only by the master and at initialisation
void G4PairProductionRelModel::InitialiseElementData()
{
lpmEnergy = mat->GetRadlen()*fLPMconstant;
// G4cout<<" lpmEnergy="<<lpmEnergy<<G4endl;
G4int size = gElementData.size();
if (size < gMaxZet+1) {
gElementData.resize(gMaxZet+1, nullptr);
}
// create for all elements that are in the detector
const G4ElementTable* elemTable = G4Element::GetElementTable();
size_t numElems = (*elemTable).size();
for (size_t ie = 0; ie < numElems; ++ie) {
const G4Element* elem = (*elemTable)[ie];
const G4int iz = std::min(gMaxZet, elem->GetZasInt());
if (!gElementData[iz]) { // create it if doesn't exist yet
const G4double logZ13 = elem->GetIonisation()->GetlogZ3();
const G4double Z13 = elem->GetIonisation()->GetZ3();
const G4double fc = elem->GetfCoulomb();
const G4double FZ = 8.*(logZ13 + fc);
G4double Fel;
G4double Finel;
if (iz<5) { // use data from Dirac-Fock atomic model
Fel = gFelLowZet[iz];
Finel = gFinelLowZet[iz];
} else { // use the results of the Thomas-Fermi-Moliere model
Fel = G4Log(184.) - logZ13;
Finel = G4Log(1194.) - 2.*logZ13;
}
ElementData* elD = new ElementData();
elD->fLogZ13 = logZ13;
elD->fCoulomb = fc;
elD->fLradEl = Fel;
elD->fDeltaFactor = 136./Z13;
elD->fDeltaMax = G4Exp((42.038 - FZ)/8.29) - 0.958;
elD->fEtaValue = Finel/(Fel-fc);
elD->fLPMVarS1Cond = std::sqrt(2.)*Z13*Z13/(184.*184.);
elD->fLPMILVarS1Cond = 1./G4Log(elD->fLPMVarS1Cond);
gElementData[iz] = elD;
}
}
}
// s goes up to 2 with ds = 0.01 be default
void G4PairProductionRelModel::InitLPMFunctions() {
if (!gLPMFuncs.fIsInitialized) {
const G4int num = gLPMFuncs.fSLimit*gLPMFuncs.fISDelta+1;
gLPMFuncs.fLPMFuncG.resize(num);
gLPMFuncs.fLPMFuncPhi.resize(num);
for (G4int i=0; i<num; ++i) {
const G4double sval = i/gLPMFuncs.fISDelta;
ComputeLPMGsPhis(gLPMFuncs.fLPMFuncG[i],gLPMFuncs.fLPMFuncPhi[i],sval);
}
gLPMFuncs.fIsInitialized = true;
}
}
// used only at initialisation time
void G4PairProductionRelModel::ComputeLPMGsPhis(G4double &funcGS, G4double &funcPhiS, const G4double varShat) {
if (varShat < 0.01) {
funcPhiS = 6.0*varShat*(1.0-CLHEP::pi*varShat);
funcGS = 12.0*varShat-2.0*funcPhiS;
} else {
const G4double varShat2 = varShat*varShat;
const G4double varShat3 = varShat*varShat2;
const G4double varShat4 = varShat2*varShat2;
if (varShat < 0.415827397755) { // Stanev ap.: for \psi(s) and compute G(s)
funcPhiS = 1.0-G4Exp( -6.0*varShat*(1.0+varShat*(3.0-CLHEP::pi))
+ varShat3/(0.623+0.796*varShat+0.658*varShat2));
// 1-\exp \left\{-4s-\frac{8s^2}{1+3.936s+4.97s^2-0.05s^3+7.5s^4} \right\}
const G4double funcPsiS = 1.0-G4Exp( -4.0*varShat - 8.0*varShat2/(1.0
+ 3.936*varShat+4.97*varShat2-0.05*varShat3+7.5*varShat4));
// G(s) = 3 \psi(s) - 2 \phi(s)
funcGS = 3.0*funcPsiS - 2.0*funcPhiS;
} else if (varShat < 1.55) {
funcPhiS = 1.0-G4Exp( -6.0*varShat*(1.0+varShat*(3.0-CLHEP::pi))
+ varShat3/(0.623+0.796*varShat+0.658*varShat2));
const G4double dum0 = -0.16072300849123999+3.7550300067531581*varShat
-1.7981383069010097 *varShat2
+0.67282686077812381*varShat3
-0.1207722909879257 *varShat4;
funcGS = std::tanh(dum0);
} else {
funcPhiS = 1.0-0.01190476/varShat4;
if (varShat < 1.9156) {
const G4double dum0 = -0.16072300849123999+3.7550300067531581*varShat
-1.7981383069010097 *varShat2
+0.67282686077812381*varShat3
-0.1207722909879257 *varShat4;
funcGS = std::tanh(dum0);
} else {
funcGS = 1.0-0.0230655/varShat4;
}
}
}
}
// used at run-time to get some pre-computed LPM function values
void G4PairProductionRelModel::GetLPMFunctions(G4double &lpmGs,
G4double &lpmPhis,
const G4double sval) {
if (sval < gLPMFuncs.fSLimit) {
G4double val = sval*gLPMFuncs.fISDelta;
const G4int ilow = (G4int)val;
val -= ilow;
lpmGs = (gLPMFuncs.fLPMFuncG[ilow+1]-gLPMFuncs.fLPMFuncG[ilow])*val
+ gLPMFuncs.fLPMFuncG[ilow];
lpmPhis = (gLPMFuncs.fLPMFuncPhi[ilow+1]-gLPMFuncs.fLPMFuncPhi[ilow])*val
+ gLPMFuncs.fLPMFuncPhi[ilow];
} else {
G4double ss = sval*sval;
ss *= ss;
lpmPhis = 1.0-0.01190476/ss;
lpmGs = 1.0-0.0230655/ss;
}
}
void G4PairProductionRelModel::ComputeLPMfunctions(G4double &funcXiS,
G4double &funcGS, G4double &funcPhiS, const G4double eps,
const G4double egamma, const G4int izet)
{
// 1. y = E_+/E_{\gamma} with E_+ being the total energy transfered
// to one of the e-/e+ pair
// s' = \sqrt{ \frac{1}{8} \frac{1}{y(1-y)} \frac{E^{KL}_{LPM}}{E_{\gamma}} }
const G4double varSprime = std::sqrt(0.125*fLPMEnergy/(eps*egamma*(1.0-eps)));
const G4double condition = gElementData[izet]->fLPMVarS1Cond;
funcXiS = 2.0;
if (varSprime > 1.0) {
funcXiS = 1.0;
} else if (varSprime > condition) {
const G4double dum = gElementData[izet]->fLPMILVarS1Cond;
const G4double funcHSprime = G4Log(varSprime)*dum;
funcXiS = 1.0 + funcHSprime
- 0.08*(1.0-funcHSprime)*funcHSprime*(2.0-funcHSprime)*dum;
}
// 2. s=\frac{s'}{\sqrt{\xi(s')}}
const G4double varShat = varSprime / std::sqrt(funcXiS);
GetLPMFunctions(funcGS, funcPhiS, varShat);
// MAKE SURE SUPPRESSION IS SMALLER THAN 1: due to Migdal's approximation on xi
if (funcXiS * funcPhiS > 1. || varShat > 0.57) {
funcXiS = 1. / funcPhiS;
}
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
source/processes/electromagnetic/standard/src/G4ScreeningMottCrossSection.cc
+6 -1
View File
@@ -307,9 +307,14 @@ G4double G4ScreeningMottCrossSection::McFcorrection(G4double angles )
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4double G4ScreeningMottCrossSection::RatioMottRutherford(G4double angles)
{
return RatioMottRutherfordCosT(std::sqrt(1. -cos(angles)));
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4double G4ScreeningMottCrossSection::RatioMottRutherfordCosT(G4double fcost)
{
G4double R=0;
G4double fcost=std::sqrt((1. -cos(angles)));
G4double a[5];
static const G4double shift=0.7181228;
G4double beta0= beta -shift;
source/processes/electromagnetic/standard/src/G4UrbanMscModel.cc
+99 -96
View File
@@ -926,13 +926,14 @@ G4double G4UrbanMscModel::SampleCosineTheta(G4double trueStepLength,
if (tau >= taubig) { cth = -1.+2.*rndmEngineMod->flat(); }
else if (tau >= tausmall) {
static const G4double numlim = 0.01;
static const G4double onethird = 1./3.;
G4double xmeanth, x2meanth;
if(tau < numlim) {
xmeanth = 1.0 - tau*(1.0 - 0.5*tau);
x2meanth= 1.0 - tau*(5.0 - 6.25*tau)/3.;
x2meanth= 1.0 - tau*(5.0 - 6.25*tau)*onethird;
} else {
xmeanth = G4Exp(-tau);
x2meanth = (1.+2.*G4Exp(-2.5*tau))/3.;
x2meanth = (1.+2.*G4Exp(-2.5*tau))*onethird;
}
// too large step of low-energy particle
@@ -952,7 +953,8 @@ G4double G4UrbanMscModel::SampleCosineTheta(G4double trueStepLength,
extremesmallstep = true ;
}
static const G4double theta0max = CLHEP::pi/6.;
static const G4double onesixth = 1./6.;
static const G4double theta0max = CLHEP::pi*onesixth;
//G4cout << "Theta0= " << theta0 << " theta0max= " << theta0max
// << " sqrt(tausmall)= " << sqrt(tausmall) << G4endl;
@@ -973,13 +975,14 @@ G4double G4UrbanMscModel::SampleCosineTheta(G4double trueStepLength,
// parameter for tail
G4double ltau= G4Log(tau);
G4double u = G4Exp(ltau/6.);
if(extremesmallstep) { u = G4Exp(G4Log(tsmall/lambda0)/6.); }
G4double u = extremesmallstep
? G4Exp(G4Log(tsmall/lambda0)*onesixth)
: G4Exp(ltau*onesixth);
G4double xx = G4Log(lambdaeff/currentRadLength);
G4double xsi = coeffc1+u*(coeffc2+coeffc3*u)+coeffc4*xx;
// tail should not be too big
if(xsi < 1.9) {
xsi = std::max(xsi, 1.9);
/*
if(KineticEnergy > 20*MeV && xsi < 1.6) {
G4cout << "G4UrbanMscModel::SampleCosineTheta: E(GeV)= "
@@ -990,8 +993,6 @@ G4double G4UrbanMscModel::SampleCosineTheta(G4double trueStepLength,
<< " tau= " << tau << G4endl;
}
*/
xsi = 1.9;
}
G4double c = xsi;
@@ -1128,53 +1129,44 @@ G4double G4UrbanMscModel::ComputeTheta0(G4double trueStepLength,
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
void G4UrbanMscModel::SampleDisplacement(G4double sth, G4double phi)
{
void G4UrbanMscModel::SampleDisplacement(G4double , G4double phi)
{
//simple distribution for u=r/rmax
// based on single scattering results
// ~(u/u0)**p1 for u < u0
// ~((1-u)/(1-u0))**p2 for u >= u0
G4double rmax = sqrt((tPathLength-zPathLength)*(tPathLength+zPathLength));
G4double r = 0.;
if(rmax > 0.)
{
static const G4double su0 = 0.851549;
static const G4double sp1 = 3.02549;
static const G4double sp2 = 1.84108;
static const G4double su1 = 1-su0;
static const G4double sp11 = sp1+1;
static const G4double sp21 = sp2+1;
static const G4double sweight = 0.802110;
G4double u;
static const G4double third = 1./3.;
G4double r = rmax*G4Exp(G4Log(rndmEngineMod->flat())*third);
/*
G4cout << "G4UrbanMscModel::SampleSecondaries: e(MeV)= " << kineticEnergy
<< " sinTheta= " << sth << " r(mm)= " << r
<< " trueStep(mm)= " << tPathLength
<< " geomStep(mm)= " << zPathLength
<< G4endl;
*/
if(r > 0.) {
static const G4double kappa = 2.5;
static const G4double kappami1 = 1.5;
G4double latcorr = 0.;
if((currentTau >= tausmall) && !insideskin) {
if(currentTau < taulim) {
latcorr = lambdaeff*kappa*currentTau*currentTau*
(1.-(kappa+1.)*currentTau*third)*third;
} else {
G4double etau = (currentTau < taubig) ? G4Exp(-currentTau) : 0.;
latcorr = -kappa*currentTau;
latcorr = G4Exp(latcorr)/kappami1;
latcorr += 1.-kappa*etau/kappami1 ;
latcorr *= 2.*lambdaeff*third;
}
}
latcorr = std::min(latcorr, r);
// sample direction of lateral displacement
// compute it from the lateral correlation
G4double Phi;
if(std::abs(r*sth) < latcorr) {
Phi = twopi*rndmEngineMod->flat();
if(rndmEngineMod->flat() < sweight) {
u = su0*G4Exp(G4Log(rndmEngineMod->flat())/sp11);
} else {
//G4cout << "latcorr= " << latcorr << " r*sth= " << r*sth
// << " ratio= " << latcorr/(r*sth) << G4endl;
G4double psi = std::acos(latcorr/(r*sth));
G4double rdm = rndmEngineMod->flat();
Phi = (rdm < 0.5) ? phi+psi : phi-psi;
u = 1-su1*G4Exp(G4Log(1-rndmEngineMod->flat())/sp21);
}
r = rmax*u ;
}
//simple distribution for v=Phi-phi=psi ~exp(-beta*v)
// alpha determined from the requirement that distribution should give
// the same mean value than that obtained from the ss simulation
if(r > 0.)
{
static const G4double cbeta = 1.933 ;
static const G4double cbeta1 = 1.-exp(-cbeta*CLHEP::pi);
G4double psi = -G4Log(1.-rndmEngineMod->flat()*cbeta1)/cbeta;
G4double Phi = (rndmEngineMod->flat() < 0.5) ? phi+psi : phi-psi;
fDisplacement.set(r*std::cos(Phi),r*std::sin(Phi),0.0);
}
}
@@ -1186,62 +1178,73 @@ void G4UrbanMscModel::SampleDisplacementNew(G4double , G4double phi)
//sample displacement r
G4double rmax = sqrt((tPathLength-zPathLength)*(tPathLength+zPathLength));
// u = (r/rmax)**2 , v=1-u
// paramerization from ss simulation
// f(u) = p0*exp(p1*log(v)-p2*v)+v*(p3+p4*v)
G4double u ,v , rej;
G4int count = 0;
G4double r = 0.;
G4double u = r/rmax;
if(rmax > 0.)
{
G4double rej;
G4int count = 0;
static const G4double reps = 1.e-6;
static const G4double rp0 = 2.2747e+4;
static const G4double rp1 = 4.5980e+0;
static const G4double rp2 = 1.5580e+1;
static const G4double rp3 = 7.1287e-1;
static const G4double rp4 =-5.7069e-1;
static const G4double reps = 1.e-6;
static const G4double rp1 = 1.61385e+1;
static const G4double rp2 = 3.26646e+0;
static const G4double rp3 =-3.35702e+0;
static const G4double rp4 = 7.38037e+1;
static const G4double rp5 =-1.12829e+2;
static const G4double rp6 = 4.63974e+1;
static const G4double ymax = 2.88900e+1;
do {
u = reps+(1.-2.*reps)*rndmEngineMod->flat();
v = 1.-u ;
rej = rp0*G4Exp(rp1*G4Log(v)-rp2*v) + v*(rp3+rp4*v);
do {
u = reps+(1.-2.*reps)*rndmEngineMod->flat();
G4double v = 1.-u ;
G4double v2= v*v;
G4double v4= v2*v2;
G4double v6= v4*v2;
G4double v8= v6*v2;
rej = G4Exp(rp1*u*u+rp2*G4Log(v))*u*v*(1+rp3*v2+rp4*v4+rp5*v6+rp6*v8);
}
// Loop checking, 15-Sept-2015, Vladimir Ivanchenko
while (ymax*rndmEngineMod->flat() > rej && ++count < 1000);
r = rmax*u;
}
// Loop checking, 15-Sept-2015, Vladimir Ivanchenko
while (rndmEngineMod->flat() > rej && ++count < 1000);
G4double r = rmax*sqrt(u);
if(r > 0.)
{
// sample Phi using lateral correlation
// and r/rmax - (Phi-phi) correlation
// v = Phi-phi = acos(latcorr/(r*sth))
// v has a universal distribution which can be parametrized from ss
// simulation as
// f(v) = 1.49e-2*exp(-v**2/(2*0.320))+2.50e-2*exp(-31.0*log(1.+6.30e-2*v))+
// 1.96e-5*exp(8.42e-1*log(1.+1.45e1*v))
static const G4double probv1 = 0.305533;
static const G4double probv2 = 0.955176;
static const G4double vhigh = 3.15;
static const G4double w2v = 1./G4Exp(30.*G4Log(1. + 6.30e-2*vhigh));
static const G4double w3v = 1./G4Exp(-1.842*G4Log(1. + 1.45e1*vhigh));
// from SS simulation f(v) = a0*exp(-a1*v)+a2
G4double v, rej;
G4int count(0);
G4double Phi;
G4double random = rndmEngineMod->flat();
if(random < probv1) {
do {
v = G4RandGauss::shoot(rndmEngineMod,0.,0.320);
}
// Loop checking, 15-Sept-2015, Vladimir Ivanchenko
while (std::abs(v) >= vhigh);
Phi = phi + v;
static const G4double a1phi[10] = {4.508e-1,6.132e-1,1.180e+0,1.357e+0,1.582e+0,
1.863e+0,2.217e+0,2.739e+0,3.652e+0,5.149e+0};
static const G4double a2phi[10] = {1.556e+0,3.571e-1,6.480e-2,3.964e-2,2.733e-2,
1.571e-2,8.546e-3,3.308e-3,6.464e-4,4.194e-5};
static const G4double a3phi[10] = {3.631e-2,1.300e-1,8.899e-1,8.396e-1,7.362e-1,
6.782e-1,5.613e-1,4.568e-1,4.296e-1,4.067e-1};
static const G4double gmphi[10] = {3.8455,1.5860,2.0190,1.4924,1.1711,
1.0158,1.0086,1.0034,1.0007,1.0001};
} else {
G4int iphi = u*10.;
if(iphi < 0) { iphi = 0; }
else if(iphi > 9) { iphi = 9; }
G4double a1 = a1phi[iphi];
G4double a2 = a2phi[iphi];
G4double a3 = a3phi[iphi];
G4double rejmax = gmphi[iphi];
G4double wphi = 1-G4Exp(-0.5*a1*CLHEP::pi);
G4double rnd = rndmEngineMod->flat();
v = (random < probv2)
? (-1.+1./G4Exp(G4Log(1.-rnd*(1.-w2v))/30.))/6.30e-2
: (-1.+1./G4Exp(G4Log(1.-rnd*(1.-w3v))/-1.842))/1.45e1;
rnd = rndmEngineMod->flat();
Phi = (rnd < 0.5) ? phi+v : phi-v;
do {
v = -2*G4Log(1-wphi*rndmEngineMod->flat())/a1;
G4double exav = G4Exp(-0.5*a1*v);
rej = (1+G4Exp(a3*G4Log(v)))*(exav*exav+a2)/(exav*rejmax);
}
// Loop checking, 5-March-2018, Vladimir Ivanchenko
while (rndmEngineMod->flat() > rej && ++count < 1000);
G4double Phi = (rndmEngineMod->flat() < 0.5) ? phi+v : phi-v;
fDisplacement.set(r*std::cos(Phi),r*std::sin(Phi),0.0);
}
}
source/processes/electromagnetic/standard/src/G4WentzelOKandVIxSection.cc
+27 -7
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4WentzelOKandVIxSection.cc 105734 2017-08-16 12:58:28Z gcosmo $
// $Id: G4WentzelOKandVIxSection.cc 109683 2018-05-08 10:36:32Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -45,6 +45,7 @@
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
#include "G4WentzelOKandVIxSection.hh"
#include "G4ScreeningMottCrossSection.hh"
#include "G4PhysicalConstants.hh"
#include "G4SystemOfUnits.hh"
#include "Randomize.hh"
@@ -78,9 +79,12 @@ G4WentzelOKandVIxSection::G4WentzelOKandVIxSection(G4bool comb) :
{
fNistManager = G4NistManager::Instance();
fG4pow = G4Pow::GetInstance();
fMottXSection = nullptr;
theElectron = G4Electron::Electron();
thePositron = G4Positron::Positron();
theProton = G4Proton::Proton();
lowEnergyLimit = 1.0*eV;
G4double p0 = electron_mass_c2*classic_electr_radius;
coeff = twopi*p0*p0;
@@ -90,7 +94,8 @@ G4WentzelOKandVIxSection::G4WentzelOKandVIxSection(G4bool comb) :
currentMaterial = nullptr;
factB = factD = formfactA = screenZ = 0.0;
cosTetMaxElec = cosTetMaxNuc = invbeta2 = kinFactor = gam0pcmp = pcmp2 = 1.0;
cosTetMaxElec = cosTetMaxNuc = invbeta2 = kinFactor = fMottFactor
= gam0pcmp = pcmp2 = 1.0;
factB1= 0.5*CLHEP::pi*fine_structure_const;
@@ -125,6 +130,12 @@ void G4WentzelOKandVIxSection::Initialise(const G4ParticleDefinition* p,
fNucFormfactor = G4EmParameters::Instance()->NuclearFormfactorType();
if(0.0 == ScreenRSquare[0]) { InitialiseA(); }
// Mott corrections
if((p == theElectron || p == thePositron) && !fMottXSection) {
fMottXSection = new G4ScreeningMottCrossSection();
fMottXSection->Initialise(p, 1.0);
}
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
@@ -145,7 +156,7 @@ void G4WentzelOKandVIxSection::InitialiseA()
ScreenRSquare[0] = afact;
ScreenRSquare[1] = afact;
ScreenRSquareElec[1] = afact;
FormFactor[1] = constn;
FormFactor[1] = 3.097e-6/(MeV*MeV);
for(G4int j=2; j<100; ++j) {
G4double x = fG4pow->Z13(j);
@@ -218,6 +229,9 @@ G4WentzelOKandVIxSection::SetupTarget(G4int Z, G4double cut)
SetTargetMass(massT);
kinFactor = coeff*Z*chargeSquare*invbeta2/mom2;
if(particle == theElectron && fMottXSection) {
fMottFactor = (1.0 + 2.0e-4*Z*Z);
}
if(1 == Z) {
screenZ = ScreenRSquare[targetZ]/mom2;
@@ -369,11 +383,17 @@ G4WentzelOKandVIxSection::SampleSingleScattering(G4double cosTMin,
fm *= FlatFormfactor(x*0.6
*fG4pow->A13(fNistManager->GetAtomicMassAmu(targetZ)));
}
G4double grej = (1. - z1*factB + factB1*targetZ*sqrt(z1*factB)*(2. - z1))
G4double grej;
if(fMottXSection) {
fMottXSection->SetupKinematic(tkin, (G4double)targetZ);
grej = fMottXSection->RatioMottRutherfordCosT(std::sqrt(z1))*fm*fm;
} else {
grej = (1. - z1*factB + factB1*targetZ*sqrt(z1*factB)*(2. - z1))
*fm*fm/(1.0 + z1*factD);
if(rndmEngineMod->flat() <= grej ) {
}
//G4cout << "SampleSingleScattering: E= " << tkin << " z1= "
// << z1 << " grej= " << grej << G4endl;
if(fMottFactor*rndmEngineMod->flat() <= grej ) {
// exclude "false" scattering due to formfactor and spin effect
G4double cost = 1.0 - z1;
if(cost > 1.0) { cost = 1.0; }
source/processes/electromagnetic/standard/src/G4eBremsstrahlungRelModel.cc
+64 -45
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4eBremsstrahlungRelModel.cc 104456 2017-05-31 15:51:40Z gcosmo $
// $Id: G4eBremsstrahlungRelModel.cc 108737 2018-03-02 13:49:56Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -76,10 +76,10 @@
const G4double
G4eBremsstrahlungRelModel::xgi[]={ 0.0199, 0.1017, 0.2372, 0.4083,
0.5917, 0.7628, 0.8983, 0.9801 };
0.5917, 0.7628, 0.8983, 0.9801 };
const G4double
G4eBremsstrahlungRelModel::wgi[]={ 0.0506, 0.1112, 0.1569, 0.1813,
0.1813, 0.1569, 0.1112, 0.0506 };
0.1813, 0.1569, 0.1112, 0.0506 };
const G4double
G4eBremsstrahlungRelModel::Fel_light[] = {0., 5.31 , 4.79 , 4.74 , 4.71};
const G4double
@@ -107,7 +107,6 @@ G4eBremsstrahlungRelModel::G4eBremsstrahlungRelModel(
nist = G4NistManager::Instance();
SetLPMFlag(true);
//SetAngularDistribution(new G4ModifiedTsai());
SetAngularDistribution(new G4DipBustGenerator());
particleMass = kinEnergy = totalEnergy = z13 = z23 = lnZ = Fel
@@ -133,25 +132,18 @@ void G4eBremsstrahlungRelModel::InitialiseConstants()
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4eBremsstrahlungRelModel::~G4eBremsstrahlungRelModel()
{
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4eBremsstrahlungRelModel::SetParticle(const G4ParticleDefinition* p)
{
particle = p;
particleMass = p->GetPDGMass();
if(p == G4Electron::Electron()) { isElectron = true; }
else { isElectron = false;}
isElectron = (p == G4Electron::Electron()) ? true : false;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4eBremsstrahlungRelModel::SetupForMaterial(const G4ParticleDefinition*,
const G4Material* mat,
G4double kineticEnergy)
const G4Material* mat,
G4double kineticEnergy)
{
densityFactor = mat->GetElectronDensity()*fMigdalConstant;
lpmEnergy = mat->GetRadlen()*fLPMconstant;
@@ -172,10 +164,37 @@ void G4eBremsstrahlungRelModel::SetupForMaterial(const G4ParticleDefinition*,
kp=sqrt(densityCorr);
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
void G4eBremsstrahlungRelModel::SetCurrentElement(G4int Z)
{
if(Z != currentZ) {
currentZ = Z;
z13 = nist->GetZ13(Z);
z23 = z13*z13;
lnZ = nist->GetLOGZ(Z);
if (Z <= 4) {
Fel = Fel_light[Z];
Finel = Finel_light[Z] ;
}
else {
G4double lnzt = lnZ/3.;
Fel = facFel - lnzt;
Finel = facFinel - 2*lnzt;
}
fCoulomb = GetCurrentElement()->GetfCoulomb();
G4double xz = 1.0/(G4double)Z;
fMax = Fel-fCoulomb + Finel*xz + (1. + xz)/12.;
}
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4eBremsstrahlungRelModel::Initialise(const G4ParticleDefinition* p,
const G4DataVector& cuts)
const G4DataVector& cuts)
{
if(p) { SetParticle(p); }
@@ -195,7 +214,7 @@ void G4eBremsstrahlungRelModel::Initialise(const G4ParticleDefinition* p,
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4eBremsstrahlungRelModel::InitialiseLocal(const G4ParticleDefinition*,
G4VEmModel* masterModel)
G4VEmModel* masterModel)
{
if(LowEnergyLimit() < HighEnergyLimit()) {
SetElementSelectors(masterModel->GetElementSelectors());
@@ -206,8 +225,8 @@ void G4eBremsstrahlungRelModel::InitialiseLocal(const G4ParticleDefinition*,
G4double
G4eBremsstrahlungRelModel::MinPrimaryEnergy(const G4Material*,
const G4ParticleDefinition*,
G4double cut)
const G4ParticleDefinition*,
G4double cut)
{
return std::max(lowestKinEnergy, cut);
}
@@ -215,7 +234,7 @@ G4eBremsstrahlungRelModel::MinPrimaryEnergy(const G4Material*,
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4double G4eBremsstrahlungRelModel::ComputeDEDXPerVolume(
const G4Material* material,
const G4Material* material,
const G4ParticleDefinition* p,
G4double kineticEnergy,
G4double cutEnergy)
@@ -268,9 +287,9 @@ G4double G4eBremsstrahlungRelModel::ComputeBremLoss(G4double cut)
G4double eg = (e0 + xgi[i]*delta)*totalEnergy;
if(totalEnergy > energyThresholdLPM) {
xs = ComputeRelDXSectionPerAtom(eg);
xs = ComputeRelDXSectionPerAtom(eg);
} else {
xs = ComputeDXSectionPerAtom(eg);
xs = ComputeDXSectionPerAtom(eg);
}
loss += wgi[i]*xs/(1.0 + densityCorr/(eg*eg));
}
@@ -286,10 +305,10 @@ G4double G4eBremsstrahlungRelModel::ComputeBremLoss(G4double cut)
G4double G4eBremsstrahlungRelModel::ComputeCrossSectionPerAtom(
const G4ParticleDefinition* p,
G4double kineticEnergy,
G4double Z, G4double,
G4double cutEnergy,
G4double maxEnergy)
G4double kineticEnergy,
G4double Z, G4double,
G4double cutEnergy,
G4double maxEnergy)
{
if(!particle) { SetParticle(p); }
if(kineticEnergy < LowEnergyLimit()) { return 0.0; }
@@ -335,9 +354,9 @@ G4double G4eBremsstrahlungRelModel::ComputeXSectionPerAtom(G4double cut)
G4double eg = G4Exp(e0 + xgi[i]*delta)*totalEnergy;
if(totalEnergy > energyThresholdLPM) {
xs = ComputeRelDXSectionPerAtom(eg);
xs = ComputeRelDXSectionPerAtom(eg);
} else {
xs = ComputeDXSectionPerAtom(eg);
xs = ComputeDXSectionPerAtom(eg);
}
cross += wgi[i]*xs/(1.0 + densityCorr/(eg*eg));
}
@@ -400,7 +419,7 @@ void G4eBremsstrahlungRelModel::CalcLPMFunctions(G4double k)
// intermediate suppression
// using eq.77 approxim. valid s<2.
phiLPM = 1.-G4Exp(-6.*s0*(1.+(3.-pi)*s0)
+s3/(0.623+0.795*s0+0.658*s2));
+s3/(0.623+0.795*s0+0.658*s2));
if (s0<0.415827397755) {
// using eq.77 approxim. valid 0.07<s<2
G4double psiLPM = 1-G4Exp(-4*s0-8*s2/(1+3.936*s0+4.97*s2-0.05*s3+7.50*s4));
@@ -409,7 +428,7 @@ void G4eBremsstrahlungRelModel::CalcLPMFunctions(G4double k)
else {
// using alternative parametrisiation
G4double pre = -0.16072300849123999 + s0*3.7550300067531581 + s2*-1.7981383069010097
+ s3*0.67282686077812381 + s4*-0.1207722909879257;
+ s3*0.67282686077812381 + s4*-0.1207722909879257;
gLPM = tanh(pre);
}
}
@@ -503,11 +522,11 @@ G4double G4eBremsstrahlungRelModel::ComputeDXSectionPerAtom(G4double gammaEnergy
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4eBremsstrahlungRelModel::SampleSecondaries(
std::vector<G4DynamicParticle*>* vdp,
const G4MaterialCutsCouple* couple,
const G4DynamicParticle* dp,
G4double cutEnergy,
G4double maxEnergy)
std::vector<G4DynamicParticle*>* vdp,
const G4MaterialCutsCouple* couple,
const G4DynamicParticle* dp,
G4double cutEnergy,
G4double maxEnergy)
{
G4double kineticEnergy = dp->GetKineticEnergy();
if(kineticEnergy < LowEnergyLimit()) { return; }
@@ -543,11 +562,11 @@ void G4eBremsstrahlungRelModel::SampleSecondaries(
if ( f > fMax ) {
G4cout << "### G4eBremsstrahlungRelModel Warning: Majoranta exceeded! "
<< f << " > " << fMax
<< " Egamma(MeV)= " << gammaEnergy
<< " Ee(MeV)= " << kineticEnergy
<< " " << GetName()
<< G4endl;
<< f << " > " << fMax
<< " Egamma(MeV)= " << gammaEnergy
<< " Ee(MeV)= " << kineticEnergy
<< " " << GetName()
<< G4endl;
}
// Loop checking, 03-Aug-2015, Vladimir Ivanchenko
@@ -556,7 +575,7 @@ void G4eBremsstrahlungRelModel::SampleSecondaries(
// scattering off nucleus or off e- by triplet model
if(scatOffElectron && G4UniformRand()*sumTerm > nucTerm) {
GetTripletModel()->SampleSecondaries(vdp, couple, dp,
cutEnergy, maxEnergy);
cutEnergy, maxEnergy);
return;
}
@@ -567,17 +586,17 @@ void G4eBremsstrahlungRelModel::SampleSecondaries(
G4ThreeVector gammaDirection =
GetAngularDistribution()->SampleDirection(dp, totalEnergy-gammaEnergy,
currentZ,
couple->GetMaterial());
currentZ,
couple->GetMaterial());
// create G4DynamicParticle object for the Gamma
G4DynamicParticle* gamma = new G4DynamicParticle(theGamma,gammaDirection,
gammaEnergy);
gammaEnergy);
vdp->push_back(gamma);
G4double totMomentum = sqrt(kineticEnergy*(totalEnergy + electron_mass_c2));
G4ThreeVector direction = (totMomentum*dp->GetMomentumDirection()
- gammaEnergy*gammaDirection).unit();
- gammaEnergy*gammaDirection).unit();
// energy of primary
G4double finalE = kineticEnergy - gammaEnergy;
@@ -588,7 +607,7 @@ void G4eBremsstrahlungRelModel::SampleSecondaries(
fParticleChange->SetProposedKineticEnergy(0.0);
G4DynamicParticle* el =
new G4DynamicParticle(const_cast<G4ParticleDefinition*>(particle),
direction, finalE);
direction, finalE);
vdp->push_back(el);
// continue tracking
source/processes/electromagnetic/standard/src/G4eeToTwoGammaModel.cc
+44 -43
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4eeToTwoGammaModel.cc 101198 2016-11-09 09:34:52Z gcosmo $
// $Id: G4eeToTwoGammaModel.cc 109177 2018-04-03 06:55:14Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -87,8 +87,7 @@ using namespace std;
G4eeToTwoGammaModel::G4eeToTwoGammaModel(const G4ParticleDefinition*,
const G4String& nam)
: G4VEmModel(nam),
pi_rcl2(pi*classic_electr_radius*classic_electr_radius),
isInitialised(false)
pi_rcl2(pi*classic_electr_radius*classic_electr_radius)
{
theGamma = G4Gamma::Gamma();
fParticleChange = nullptr;
@@ -104,17 +103,14 @@ G4eeToTwoGammaModel::~G4eeToTwoGammaModel()
void G4eeToTwoGammaModel::Initialise(const G4ParticleDefinition*,
const G4DataVector&)
{
if(isInitialised) { return; }
if(fParticleChange) { return; }
fParticleChange = GetParticleChangeForGamma();
isInitialised = true;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4double G4eeToTwoGammaModel::ComputeCrossSectionPerElectron(
const G4ParticleDefinition*,
G4double kineticEnergy,
G4double, G4double)
G4double
G4eeToTwoGammaModel::ComputeCrossSectionPerElectron(G4double kineticEnergy)
{
// Calculates the cross section per electron of annihilation into two photons
// from the Heilter formula.
@@ -135,13 +131,13 @@ G4double G4eeToTwoGammaModel::ComputeCrossSectionPerElectron(
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4double G4eeToTwoGammaModel::ComputeCrossSectionPerAtom(
const G4ParticleDefinition* p,
const G4ParticleDefinition*,
G4double kineticEnergy, G4double Z,
G4double, G4double, G4double)
{
// Calculates the cross section per atom of annihilation into two photons
G4double cross = Z*ComputeCrossSectionPerElectron(p,kineticEnergy);
G4double cross = Z*ComputeCrossSectionPerElectron(kineticEnergy);
return cross;
}
@@ -149,14 +145,14 @@ G4double G4eeToTwoGammaModel::ComputeCrossSectionPerAtom(
G4double G4eeToTwoGammaModel::CrossSectionPerVolume(
const G4Material* material,
const G4ParticleDefinition* p,
const G4ParticleDefinition*,
G4double kineticEnergy,
G4double, G4double)
{
// Calculates the cross section per volume of annihilation into two photons
G4double eDensity = material->GetElectronDensity();
G4double cross = eDensity*ComputeCrossSectionPerElectron(p,kineticEnergy);
G4double cross = eDensity*ComputeCrossSectionPerElectron(kineticEnergy);
return cross;
}
@@ -171,13 +167,13 @@ void G4eeToTwoGammaModel::SampleSecondaries(vector<G4DynamicParticle*>* vdp,
G4double,
G4double)
{
G4double PositKinEnergy = dp->GetKineticEnergy();
G4double posiKinEnergy = dp->GetKineticEnergy();
G4DynamicParticle *aGamma1, *aGamma2;
CLHEP::HepRandomEngine* rndmEngine = G4Random::getTheEngine();
// Case at rest
if(PositKinEnergy == 0.0) {
if(posiKinEnergy == 0.0) {
G4double cost = 2.*rndmEngine->flat()-1.;
G4double sint = sqrt((1. - cost)*(1. + cost));
G4double phi = twopi * rndmEngine->flat();
@@ -193,12 +189,15 @@ void G4eeToTwoGammaModel::SampleSecondaries(vector<G4DynamicParticle*>* vdp,
pol.set(-sinphi, cosphi, 0.0);
pol.rotateUz(dir);
aGamma2->SetPolarization(pol.x(),pol.y(),pol.z());
/*
G4cout << "Annihilation at rest fly: e0= " << " dir= " << dir
<< G4endl;
*/
} else {
G4ThreeVector PositDirection = dp->GetMomentumDirection();
G4ThreeVector posiDirection = dp->GetMomentumDirection();
G4double tau = PositKinEnergy/electron_mass_c2;
G4double tau = posiKinEnergy/electron_mass_c2;
G4double gam = tau + 1.0;
G4double tau2 = tau + 2.0;
G4double sqgrate = sqrt(tau/tau2)*0.5;
@@ -227,7 +226,7 @@ void G4eeToTwoGammaModel::SampleSecondaries(vector<G4DynamicParticle*>* vdp,
G4double cost = (epsil*tau2-1.)/(epsil*sqg2m1);
if(std::abs(cost) > 1.0) {
G4cout << "### G4eeToTwoGammaModel WARNING cost= " << cost
<< " positron Ekin(MeV)= " << PositKinEnergy
<< " positron Ekin(MeV)= " << posiKinEnergy
<< " gamma epsil= " << epsil
<< G4endl;
if(cost > 1.0) cost = 1.0;
@@ -240,47 +239,49 @@ void G4eeToTwoGammaModel::SampleSecondaries(vector<G4DynamicParticle*>* vdp,
// kinematic of the created pair
//
G4double TotalAvailableEnergy = PositKinEnergy + 2.0*electron_mass_c2;
G4double Phot1Energy = epsil*TotalAvailableEnergy;
G4double totalEnergy = posiKinEnergy + 2.0*electron_mass_c2;
G4double phot1Energy = epsil*totalEnergy;
G4ThreeVector Phot1Direction(sint*cos(phi), sint*sin(phi), cost);
Phot1Direction.rotateUz(PositDirection);
aGamma1 = new G4DynamicParticle (theGamma,Phot1Direction, Phot1Energy);
G4ThreeVector phot1Direction(sint*cos(phi), sint*sin(phi), cost);
phot1Direction.rotateUz(posiDirection);
aGamma1 = new G4DynamicParticle (theGamma,phot1Direction, phot1Energy);
phi = twopi * rndmEngine->flat();
G4double cosphi = cos(phi);
G4double sinphi = sin(phi);
G4ThreeVector pol(cosphi, sinphi, 0.0);
pol.rotateUz(Phot1Direction);
pol.rotateUz(phot1Direction);
aGamma1->SetPolarization(pol.x(),pol.y(),pol.z());
G4double Phot2Energy =(1.-epsil)*TotalAvailableEnergy;
G4double PositP= sqrt(PositKinEnergy*(PositKinEnergy+2.*electron_mass_c2));
G4ThreeVector dir = PositDirection*PositP - Phot1Direction*Phot1Energy;
G4ThreeVector Phot2Direction = dir.unit();
G4double phot2Energy =(1.-epsil)*totalEnergy;
G4double posiP= sqrt(posiKinEnergy*(posiKinEnergy+2.*electron_mass_c2));
G4ThreeVector dir = posiDirection*posiP - phot1Direction*phot1Energy;
G4ThreeVector phot2Direction = dir.unit();
// create G4DynamicParticle object for the particle2
aGamma2 = new G4DynamicParticle (theGamma,Phot2Direction, Phot2Energy);
aGamma2 = new G4DynamicParticle (theGamma, phot2Direction, phot2Energy);
//!!! likely problematic direction to be checked
pol.set(-sinphi, cosphi, 0.0);
pol.rotateUz(Phot1Direction);
cost = pol*Phot2Direction;
pol -= cost*Phot2Direction;
pol.rotateUz(phot1Direction);
cost = pol*phot2Direction;
pol -= cost*phot2Direction;
pol = pol.unit();
aGamma2->SetPolarization(pol.x(),pol.y(),pol.z());
}
/*
G4cout << "Annihilation in fly: e0= " << PositKinEnergy
<< " m= " << electron_mass_c2
<< " e1= " << Phot1Energy
<< " e2= " << Phot2Energy << " dir= " << dir
<< " -> " << Phot1Direction << " "
<< Phot2Direction << G4endl;
*/
/*
G4cout << "Annihilation on fly: e0= " << posiKinEnergy
<< " m= " << electron_mass_c2
<< " e1= " << phot1Energy
<< " e2= " << phot2Energy << " dir= " << dir
<< " -> " << phot1Direction << " "
<< phot2Direction << G4endl;
*/
}
vdp->push_back(aGamma1);
vdp->push_back(aGamma2);
fParticleChange->SetProposedKineticEnergy(0.);
// kill primary positron
fParticleChange->SetProposedKineticEnergy(0.0);
fParticleChange->ProposeTrackStatus(fStopAndKill);
}
source/processes/electromagnetic/standard/src/G4eplusAnnihilation.cc
+82 -43
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4eplusAnnihilation.cc 107058 2017-11-01 14:54:12Z gcosmo $
// $Id: G4eplusAnnihilation.cc 109177 2018-04-03 06:55:14Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -59,6 +59,7 @@
#include "G4Gamma.hh"
#include "G4Positron.hh"
#include "G4eeToTwoGammaModel.hh"
#include "G4EmBiasingManager.hh"
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
@@ -74,6 +75,7 @@ G4eplusAnnihilation::G4eplusAnnihilation(const G4String& name)
SetSecondaryParticle(theGamma);
SetProcessSubType(fAnnihilation);
enableAtRestDoIt = true;
mainSecondaries = 2;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
@@ -118,55 +120,92 @@ void G4eplusAnnihilation::StreamProcessInfo(std::ostream&,
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4VParticleChange* G4eplusAnnihilation::AtRestDoIt(const G4Track& aTrack,
const G4Step& )
//
G4VParticleChange* G4eplusAnnihilation::AtRestDoIt(const G4Track& track,
const G4Step& step)
// Performs the e+ e- annihilation when both particles are assumed at rest.
// It generates two back to back photons with energy = electron_mass.
// The angular distribution is isotropic.
// GEANT4 internal units
//
// Note : Effects due to binding of atomic electrons are negliged.
{
fParticleChange.InitializeForPostStep(aTrack);
CLHEP::HepRandomEngine* rndmEngine = G4Random::getTheEngine();
fParticleChange.InitializeForPostStep(track);
size_t idx = CurrentMaterialCutsCoupleIndex();
G4double ene(0.0);
G4VEmModel* model = SelectModel(ene, idx);
G4double cosTeta = 2.*rndmEngine->flat()-1.;
G4double sinTeta = sqrt((1.-cosTeta)*(1.0 + cosTeta));
G4double phi = twopi * rndmEngine->flat();
G4ThreeVector dir(sinTeta*cos(phi), sinTeta*sin(phi), cosTeta);
phi = twopi * rndmEngine->flat();
G4double cosphi = cos(phi);
G4double sinphi = sin(phi);
G4ThreeVector pol(cosphi, sinphi, 0.0);
pol.rotateUz(dir);
// define new weight for primary and secondaries
G4double weight = fParticleChange.GetParentWeight();
// e+ parameters
G4double weight = aTrack.GetWeight();
G4double time = aTrack.GetGlobalTime();
// sample secondaries
secParticles.clear();
G4double gammaCut = GetGammaEnergyCut();
model->SampleSecondaries(&secParticles, MaterialCutsCouple(),
track.GetDynamicParticle(), gammaCut);
G4int num0 = secParticles.size();
// add gammas
fParticleChange.SetNumberOfSecondaries(2);
G4DynamicParticle* dp =
new G4DynamicParticle(theGamma, dir, electron_mass_c2);
dp->SetPolarization(pol.x(),pol.y(),pol.z());
G4Track* track = new G4Track(dp, time, aTrack.GetPosition());
track->SetTouchableHandle(aTrack.GetTouchableHandle());
track->SetWeight(weight);
pParticleChange->AddSecondary(track);
// splitting or Russian roulette
if(biasManager) {
if(biasManager->SecondaryBiasingRegion(idx)) {
G4double eloss = 0.0;
weight *= biasManager->ApplySecondaryBiasing(
secParticles, track, model, &fParticleChange, eloss,
idx, gammaCut, step.GetPostStepPoint()->GetSafety());
if(eloss > 0.0) {
eloss += fParticleChange.GetLocalEnergyDeposit();
fParticleChange.ProposeLocalEnergyDeposit(eloss);
}
}
}
// save secondaries
G4int num = secParticles.size();
if(num > 0) {
dp = new G4DynamicParticle(theGamma,-dir, electron_mass_c2);
pol.set(-sinphi, cosphi, 0.0);
pol.rotateUz(dir);
dp->SetPolarization(pol.x(),pol.y(),pol.z());
track = new G4Track(dp, time, aTrack.GetPosition());
track->SetTouchableHandle(aTrack.GetTouchableHandle());
track->SetWeight(weight);
pParticleChange->AddSecondary(track);
fParticleChange.SetNumberOfSecondaries(num);
G4double edep = fParticleChange.GetLocalEnergyDeposit();
G4double time = track.GetGlobalTime();
for (G4int i=0; i<num; ++i) {
if (secParticles[i]) {
G4DynamicParticle* dp = secParticles[i];
const G4ParticleDefinition* p = dp->GetParticleDefinition();
G4double e = dp->GetKineticEnergy();
G4bool good = true;
if(ApplyCuts()) {
if (p == theGamma) {
if (e < gammaCut) { good = false; }
} else if (p == theElectron) {
if (e < GetElectronEnergyCut()) { good = false; }
}
// added secondary if it is good
}
if (good) {
G4Track* t = new G4Track(dp, time, track.GetPosition());
t->SetTouchableHandle(track.GetTouchableHandle());
t->SetWeight(weight);
pParticleChange->AddSecondary(t);
// Kill the incident positron
//
fParticleChange.ProposeTrackStatus(fStopAndKill);
// define type of secondary
if(i < mainSecondaries) { t->SetCreatorModelIndex(secID); }
else if(i < num0) {
if(p == theGamma) {
t->SetCreatorModelIndex(fluoID);
} else {
t->SetCreatorModelIndex(augerID);
}
} else {
t->SetCreatorModelIndex(biasID);
}
/*
G4cout << "Secondary(post step) has weight " << t->GetWeight()
<< ", Ekin= " << t->GetKineticEnergy()/MeV << " MeV "
<< GetProcessName() << " fluoID= " << fluoID
<< " augerID= " << augerID <<G4endl;
*/
} else {
delete dp;
edep += e;
}
}
}
fParticleChange.ProposeLocalEnergyDeposit(edep);
}
return &fParticleChange;
}
source/processes/electromagnetic/standard/src/G4eplusTo2GammaOKVIModel.cc
+295
View File
@@ -0,0 +1,295 @@
//
// ********************************************************************
// * License and Disclaimer *
// * *
// * The Geant4 software is copyright of the Copyright Holders of *
// * the Geant4 Collaboration. It is provided under the terms and *
// * conditions of the Geant4 Software License, included in the file *
// * LICENSE and available at http://cern.ch/geant4/license . These *
// * include a list of copyright holders. *
// * *
// * Neither the authors of this software system, nor their employing *
// * institutes,nor the agencies providing financial support for this *
// * work make any representation or warranty, express or implied, *
// * regarding this software system or assume any liability for its *
// * use. Please see the license in the file LICENSE and URL above *
// * for the full disclaimer and the limitation of liability. *
// * *
// * This code implementation is the result of the scientific and *
// * technical work of the GEANT4 collaboration. *
// * By using, copying, modifying or distributing the software (or *
// * any work based on the software) you agree to acknowledge its *
// * use in resulting scientific publications, and indicate your *
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4eplusTo2GammaOKVIModel.cc 101193 2016-11-08 18:02:50Z vnivanch $
//
// -------------------------------------------------------------------
//
// GEANT4 Class file
//
//
// File name: G4eplusTo2GammaOKVIModel
//
// Author: Vladimir Ivanchenko and Omrame Kadri
//
// Creation date: 29.03.2018
//
// -------------------------------------------------------------------
//
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
#include "G4eplusTo2GammaOKVIModel.hh"
#include "G4eplusTo3GammaOKVIModel.hh"
#include "G4PhysicalConstants.hh"
#include "G4SystemOfUnits.hh"
#include "G4EmParameters.hh"
#include "G4TrackStatus.hh"
#include "G4Electron.hh"
#include "G4Positron.hh"
#include "G4Gamma.hh"
#include "G4PhysicsVector.hh"
#include "G4PhysicsLogVector.hh"
#include "Randomize.hh"
#include "G4ParticleChangeForGamma.hh"
#include "G4Log.hh"
#include "G4Exp.hh"
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
using namespace std;
G4PhysicsVector* G4eplusTo2GammaOKVIModel::fCrossSection = nullptr;
G4PhysicsVector* G4eplusTo2GammaOKVIModel::f3GProbability= nullptr;
G4eplusTo2GammaOKVIModel::G4eplusTo2GammaOKVIModel(const G4ParticleDefinition*,
const G4String& nam)
: G4VEmModel(nam),
pi_rcl2(pi*classic_electr_radius*classic_electr_radius),
energyTh(10*MeV)
{
theGamma = G4Gamma::Gamma();
fParticleChange = nullptr;
f3GModel = new G4eplusTo3GammaOKVIModel();
SetTripletModel(f3GModel);
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4eplusTo2GammaOKVIModel::~G4eplusTo2GammaOKVIModel()
{}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4eplusTo2GammaOKVIModel::Initialise(const G4ParticleDefinition* p,
const G4DataVector& cuts)
{
energyTh = G4EmParameters::Instance()->LowestTripletEnergy();
f3GModel->Initialise(p, cuts);
if(IsMaster()) {
if(!fCrossSection) {
G4double emin = 10*eV;
G4double emax = 100*TeV;
G4int nbins = 20*G4lrint(std::log10(emax/emin));
fCrossSection = new G4PhysicsLogVector(emin, emax, nbins);
f3GProbability= new G4PhysicsLogVector(emin, emax, nbins);
fCrossSection->SetSpline(true);
f3GProbability->SetSpline(true);
for(G4int i=0; i<= nbins; ++i) {
G4double e = fCrossSection->Energy(i);
G4double cs2 = ComputeCrossSectionPerElectron(e);
G4double cs3 = f3GModel->ComputeCrossSectionPerElectron(e);
cs2 += cs3;
fCrossSection->PutValue(i, cs2);
f3GProbability->PutValue(i, cs3/cs2);
}
}
}
// here particle change is set for the triplet model
if(fParticleChange) { return; }
fParticleChange = GetParticleChangeForGamma();
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4double
G4eplusTo2GammaOKVIModel::ComputeCrossSectionPerElectron(G4double kineticEnergy)
{
// Calculates the cross section per electron of annihilation into two photons
// from the Heilter formula.
G4double ekin = std::max(eV,kineticEnergy);
G4double tau = ekin/electron_mass_c2;
G4double gam = tau + 1.0;
G4double gamma2= gam*gam;
G4double bg2 = tau * (tau+2.0);
G4double bg = sqrt(bg2);
G4double cross = pi_rcl2*((gamma2+4*gam+1.)*G4Log(gam+bg) - (gam+3.)*bg)
/ (bg2*(gam+1.));
return cross;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4double G4eplusTo2GammaOKVIModel::ComputeCrossSectionPerAtom(
const G4ParticleDefinition*,
G4double kineticEnergy, G4double Z,
G4double, G4double, G4double)
{
// Calculates the cross section per atom of annihilation into two photons
G4double cross = Z*fCrossSection->Value(kineticEnergy);
return cross;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4double G4eplusTo2GammaOKVIModel::CrossSectionPerVolume(
const G4Material* material,
const G4ParticleDefinition*,
G4double kineticEnergy,
G4double, G4double)
{
// Calculates the cross section per volume of annihilation into two photons
G4double eDensity = material->GetElectronDensity();
G4double cross = eDensity*fCrossSection->Value(kineticEnergy);
return cross;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
// Polarisation of gamma according to M.H.L.Pryce and J.C.Ward,
// Nature 4065 (1947) 435.
void
G4eplusTo2GammaOKVIModel::SampleSecondaries(vector<G4DynamicParticle*>* vdp,
const G4MaterialCutsCouple* mcc,
const G4DynamicParticle* dp,
G4double, G4double)
{
G4double posiKinEnergy = dp->GetKineticEnergy();
CLHEP::HepRandomEngine* rndmEngine = G4Random::getTheEngine();
if(rndmEngine->flat() < f3GProbability->Value(posiKinEnergy)) {
f3GModel->SampleSecondaries(vdp, mcc, dp);
return;
}
G4DynamicParticle *aGamma1, *aGamma2;
// Case at rest
if(posiKinEnergy == 0.0) {
G4double cost = 2.*rndmEngine->flat()-1.;
G4double sint = sqrt((1. - cost)*(1. + cost));
G4double phi = twopi * rndmEngine->flat();
G4ThreeVector dir(sint*cos(phi), sint*sin(phi), cost);
phi = twopi * rndmEngine->flat();
G4double cosphi = cos(phi);
G4double sinphi = sin(phi);
G4ThreeVector pol(cosphi, sinphi, 0.0);
pol.rotateUz(dir);
aGamma1 = new G4DynamicParticle(theGamma, dir, electron_mass_c2);
aGamma1->SetPolarization(pol.x(),pol.y(),pol.z());
aGamma2 = new G4DynamicParticle(theGamma,-dir, electron_mass_c2);
pol.set(-sinphi, cosphi, 0.0);
pol.rotateUz(dir);
aGamma2->SetPolarization(pol.x(),pol.y(),pol.z());
} else {
G4ThreeVector posiDirection = dp->GetMomentumDirection();
G4double tau = posiKinEnergy/electron_mass_c2;
G4double gam = tau + 1.0;
G4double tau2 = tau + 2.0;
G4double sqgrate = sqrt(tau/tau2)*0.5;
G4double sqg2m1 = sqrt(tau*tau2);
// limits of the energy sampling
G4double epsilmin = 0.5 - sqgrate;
G4double epsilmax = 0.5 + sqgrate;
G4double epsilqot = epsilmax/epsilmin;
//
// sample the energy rate of the created gammas
//
G4double epsil, greject;
do {
epsil = epsilmin*G4Exp(G4Log(epsilqot)*rndmEngine->flat());
greject = 1. - epsil + (2.*gam*epsil-1.)/(epsil*tau2*tau2);
// Loop checking, 03-Aug-2015, Vladimir Ivanchenko
} while( greject < rndmEngine->flat());
//
// scattered Gamma angles. ( Z - axis along the parent positron)
//
G4double cost = (epsil*tau2-1.)/(epsil*sqg2m1);
if(std::abs(cost) > 1.0) {
G4cout << "### G4eplusTo2GammaOKVIModel WARNING cost= " << cost
<< " positron Ekin(MeV)= " << posiKinEnergy
<< " gamma epsil= " << epsil
<< G4endl;
if(cost > 1.0) cost = 1.0;
else cost = -1.0;
}
G4double sint = sqrt((1.+cost)*(1.-cost));
G4double phi = twopi * rndmEngine->flat();
//
// kinematic of the created pair
//
G4double TotalAvailableEnergy = posiKinEnergy + 2.0*electron_mass_c2;
G4double phot1Energy = epsil*TotalAvailableEnergy;
G4ThreeVector phot1Direction(sint*cos(phi), sint*sin(phi), cost);
phot1Direction.rotateUz(posiDirection);
aGamma1 = new G4DynamicParticle (theGamma,phot1Direction, phot1Energy);
phi = twopi * rndmEngine->flat();
G4double cosphi = cos(phi);
G4double sinphi = sin(phi);
G4ThreeVector pol(cosphi, sinphi, 0.0);
pol.rotateUz(phot1Direction);
aGamma1->SetPolarization(pol.x(),pol.y(),pol.z());
G4double phot2Energy =(1.-epsil)*TotalAvailableEnergy;
G4double posiP= sqrt(posiKinEnergy*(posiKinEnergy+2.*electron_mass_c2));
G4ThreeVector dir = posiDirection*posiP - phot1Direction*phot1Energy;
G4ThreeVector phot2Direction = dir.unit();
// create G4DynamicParticle object for the particle2
aGamma2 = new G4DynamicParticle (theGamma,phot2Direction, phot2Energy);
//!!! likely problematic direction to be checked
pol.set(-sinphi, cosphi, 0.0);
pol.rotateUz(phot1Direction);
cost = pol*phot2Direction;
pol -= cost*phot2Direction;
pol = pol.unit();
aGamma2->SetPolarization(pol.x(),pol.y(),pol.z());
}
/*
G4cout << "Annihilation in fly: e0= " << posiKinEnergy
<< " m= " << electron_mass_c2
<< " e1= " << phot1Energy
<< " e2= " << phot2Energy << " dir= " << dir
<< " -> " << phot1Direction << " "
<< phot2Direction << G4endl;
*/
vdp->push_back(aGamma1);
vdp->push_back(aGamma2);
// kill primary positron
fParticleChange->SetProposedKineticEnergy(0.0);
fParticleChange->ProposeTrackStatus(fStopAndKill);
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
source/processes/electromagnetic/standard/src/G4eplusTo3GammaOKVIModel.cc
+260
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@@ -0,0 +1,260 @@
//
// ********************************************************************
// * License and Disclaimer *
// * *
// * The Geant4 software is copyright of the Copyright Holders of *
// * the Geant4 Collaboration. It is provided under the terms and *
// * conditions of the Geant4 Software License, included in the file *
// * LICENSE and available at http://cern.ch/geant4/license . These *
// * include a list of copyright holders. *
// * *
// * Neither the authors of this software system, nor their employing *
// * institutes,nor the agencies providing financial support for this *
// * work make any representation or warranty, express or implied, *
// * regarding this software system or assume any liability for its *
// * use. Please see the license in the file LICENSE and URL above *
// * for the full disclaimer and the limitation of liability. *
// * *
// * This code implementation is the result of the scientific and *
// * technical work of the GEANT4 collaboration. *
// * By using, copying, modifying or distributing the software (or *
// * any work based on the software) you agree to acknowledge its *
// * use in resulting scientific publications, and indicate your *
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4eplusTo3GammaOKVIModel.cc 101193 2016-11-08 18:02:50Z vnivanch $
//
// -------------------------------------------------------------------
//
// GEANT4 Class file
//
//
// File name: G4eplusTo3GammaOKVIModel
//
// Author: Vladimir Ivanchenko and Omrame Kadri
//
// Creation date: 29.03.2018
//
// -------------------------------------------------------------------
//
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
#include "G4eplusTo3GammaOKVIModel.hh"
#include "G4PhysicalConstants.hh"
#include "G4SystemOfUnits.hh"
#include "G4EmParameters.hh"
#include "G4TrackStatus.hh"
#include "G4Electron.hh"
#include "G4Positron.hh"
#include "G4Gamma.hh"
#include "Randomize.hh"
#include "G4ParticleChangeForGamma.hh"
#include "G4Log.hh"
#include "G4Exp.hh"
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
using namespace std;
G4eplusTo3GammaOKVIModel::G4eplusTo3GammaOKVIModel(const G4ParticleDefinition*,
const G4String& nam)
: G4VEmModel(nam),
pi_rcl2(pi*classic_electr_radius*classic_electr_radius),
energyTh(10*MeV)
{
theGamma = G4Gamma::Gamma();
fParticleChange = nullptr;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4eplusTo3GammaOKVIModel::~G4eplusTo3GammaOKVIModel()
{}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4eplusTo3GammaOKVIModel::Initialise(const G4ParticleDefinition*,
const G4DataVector&)
{
energyTh = G4EmParameters::Instance()->LowestTripletEnergy();
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4double
G4eplusTo3GammaOKVIModel::ComputeCrossSectionPerElectron(G4double kineticEnergy)
{
// Calculates the cross section per electron of annihilation into two photons
// from the Heilter formula.
G4double ekin = std::max(eV,kineticEnergy);
G4double tau = ekin/electron_mass_c2;
G4double gam = tau + 1.0;
G4double gamma2= gam*gam;
G4double bg2 = tau * (tau+2.0);
G4double bg = sqrt(bg2);
G4double cross = pi_rcl2*((gamma2+4*gam+1.)*G4Log(gam+bg) - (gam+3.)*bg)
/ (bg2*(gam+1.));
return cross;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4double G4eplusTo3GammaOKVIModel::ComputeCrossSectionPerAtom(
const G4ParticleDefinition*,
G4double kineticEnergy, G4double Z,
G4double, G4double, G4double)
{
// Calculates the cross section per atom of annihilation into two photons
G4double cross = Z*ComputeCrossSectionPerElectron(kineticEnergy);
return cross;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4double G4eplusTo3GammaOKVIModel::CrossSectionPerVolume(
const G4Material* material,
const G4ParticleDefinition*,
G4double kineticEnergy,
G4double, G4double)
{
// Calculates the cross section per volume of annihilation into two photons
G4double eDensity = material->GetElectronDensity();
G4double cross = eDensity*ComputeCrossSectionPerElectron(kineticEnergy);
return cross;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
// Polarisation of gamma according to M.H.L.Pryce and J.C.Ward,
// Nature 4065 (1947) 435.
void
G4eplusTo3GammaOKVIModel::SampleSecondaries(vector<G4DynamicParticle*>* vdp,
const G4MaterialCutsCouple*,
const G4DynamicParticle* dp,
G4double, G4double)
{
G4double posiKinEnergy = dp->GetKineticEnergy();
G4DynamicParticle *aGamma1, *aGamma2, *aGamma3;
CLHEP::HepRandomEngine* rndmEngine = G4Random::getTheEngine();
// Case at rest
if(posiKinEnergy == 0.0) {
G4double cost = 2.*rndmEngine->flat()-1.;
G4double sint = sqrt((1. - cost)*(1. + cost));
G4double phi = twopi * rndmEngine->flat();
G4ThreeVector dir(sint*cos(phi), sint*sin(phi), cost);
phi = twopi * rndmEngine->flat();
G4double cosphi = cos(phi);
G4double sinphi = sin(phi);
G4ThreeVector pol(cosphi, sinphi, 0.0);
pol.rotateUz(dir);
aGamma1 = new G4DynamicParticle(theGamma, dir, electron_mass_c2);
aGamma1->SetPolarization(pol.x(),pol.y(),pol.z());
aGamma2 = new G4DynamicParticle(theGamma,-dir, electron_mass_c2);
pol.set(-sinphi, cosphi, 0.0);
pol.rotateUz(dir);
aGamma2->SetPolarization(pol.x(),pol.y(),pol.z());
} else {
G4ThreeVector posiDirection = dp->GetMomentumDirection();
G4double tau = posiKinEnergy/electron_mass_c2;
G4double gam = tau + 1.0;
G4double tau2 = tau + 2.0;
G4double sqgrate = sqrt(tau/tau2)*0.5;
G4double sqg2m1 = sqrt(tau*tau2);
// limits of the energy sampling
G4double epsilmin = 0.5 - sqgrate;
G4double epsilmax = 0.5 + sqgrate;
G4double epsilqot = epsilmax/epsilmin;
//
// sample the energy rate of the created gammas
//
G4double epsil, greject;
do {
epsil = epsilmin*G4Exp(G4Log(epsilqot)*rndmEngine->flat());
greject = 1. - epsil + (2.*gam*epsil-1.)/(epsil*tau2*tau2);
// Loop checking, 03-Aug-2015, Vladimir Ivanchenko
} while( greject < rndmEngine->flat());
//
// scattered Gamma angles. ( Z - axis along the parent positron)
//
G4double cost = (epsil*tau2-1.)/(epsil*sqg2m1);
if(std::abs(cost) > 1.0) {
G4cout << "### G4eplusTo3GammaOKVIModel WARNING cost= " << cost
<< " positron Ekin(MeV)= " << posiKinEnergy
<< " gamma epsil= " << epsil
<< G4endl;
if(cost > 1.0) cost = 1.0;
else cost = -1.0;
}
G4double sint = sqrt((1.+cost)*(1.-cost));
G4double phi = twopi * rndmEngine->flat();
//
// kinematic of the created pair
//
G4double TotalAvailableEnergy = posiKinEnergy + 2.0*electron_mass_c2;
G4double phot1Energy = epsil*TotalAvailableEnergy;
G4ThreeVector phot1Direction(sint*cos(phi), sint*sin(phi), cost);
phot1Direction.rotateUz(posiDirection);
aGamma1 = new G4DynamicParticle (theGamma,phot1Direction, phot1Energy);
phi = twopi * rndmEngine->flat();
G4double cosphi = cos(phi);
G4double sinphi = sin(phi);
G4ThreeVector pol(cosphi, sinphi, 0.0);
pol.rotateUz(phot1Direction);
aGamma1->SetPolarization(pol.x(),pol.y(),pol.z());
G4double phot2Energy =(1.-epsil)*TotalAvailableEnergy;
G4double posiP= sqrt(posiKinEnergy*(posiKinEnergy+2.*electron_mass_c2));
G4ThreeVector dir = posiDirection*posiP - phot1Direction*phot1Energy;
G4ThreeVector phot2Direction = dir.unit();
// create G4DynamicParticle object for the particle2
aGamma2 = new G4DynamicParticle (theGamma,phot2Direction, phot2Energy);
//!!! likely problematic direction to be checked
pol.set(-sinphi, cosphi, 0.0);
pol.rotateUz(phot1Direction);
cost = pol*phot2Direction;
pol -= cost*phot2Direction;
pol = pol.unit();
aGamma2->SetPolarization(pol.x(),pol.y(),pol.z());
}
/*
G4cout << "Annihilation in fly: e0= " << posiKinEnergy
<< " m= " << electron_mass_c2
<< " e1= " << phot1Energy
<< " e2= " << phot2Energy << " dir= " << dir
<< " -> " << phot1Direction << " "
<< phot2Direction << G4endl;
*/
vdp->push_back(aGamma1);
vdp->push_back(aGamma2);
vdp->push_back(aGamma3);
// kill primary positron
fParticleChange->SetProposedKineticEnergy(0.0);
fParticleChange->ProposeTrackStatus(fStopAndKill);
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....

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