Import Geant4 9.2.0 source tree
This commit is contained in:
@@ -23,8 +23,8 @@
|
||||
// * acceptance of all terms of the Geant4 Software license. *
|
||||
// ********************************************************************
|
||||
//
|
||||
// $Id: G4MuBremsstrahlungModel.cc,v 1.24 2007/11/08 11:48:28 vnivanch Exp $
|
||||
// GEANT4 tag $Name: geant4-09-01 $
|
||||
// $Id: G4MuBremsstrahlungModel.cc,v 1.32 2008/07/22 16:11:34 vnivanch Exp $
|
||||
// GEANT4 tag $Name: geant4-09-02 $
|
||||
//
|
||||
// -------------------------------------------------------------------
|
||||
//
|
||||
@@ -45,11 +45,12 @@
|
||||
// 27-01-03 Make models region aware (V.Ivanchenko)
|
||||
// 13-02-03 Add name (V.Ivanchenko)
|
||||
// 10-02-04 Add lowestKinEnergy (V.Ivanchenko)
|
||||
// 08-04-05 Major optimisation of internal interfaces (V.Ivantchenko)
|
||||
// 03-08-05 Angular correlations according to PRM (V.Ivantchenko)
|
||||
// 08-04-05 Major optimisation of internal interfaces (V.Ivanchenko)
|
||||
// 03-08-05 Angular correlations according to PRM (V.Ivanchenko)
|
||||
// 13-02-06 add ComputeCrossSectionPerAtom (mma)
|
||||
// 21-03-06 Fix problem of initialisation in case when cuts are not defined (VI)
|
||||
// 07-11-07 Improve sampling of final state (A.Bogdanov)
|
||||
// 28-02-08 Use precomputed Z^1/3 and Log(A) (V.Ivanchenko)
|
||||
//
|
||||
|
||||
//
|
||||
@@ -73,14 +74,6 @@
|
||||
#include "G4ParticleChangeForLoss.hh"
|
||||
|
||||
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
|
||||
|
||||
// static members
|
||||
//
|
||||
G4double G4MuBremsstrahlungModel::zdat[]={1., 4., 13., 29., 92.};
|
||||
G4double G4MuBremsstrahlungModel::adat[]={1.01, 9.01, 26.98, 63.55, 238.03};
|
||||
G4double G4MuBremsstrahlungModel::tdat[]={1.e3, 1.e4, 1.e5, 1.e6, 1.e7, 1.e8,
|
||||
1.e9, 1.e10};
|
||||
|
||||
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
|
||||
|
||||
using namespace std;
|
||||
@@ -89,16 +82,17 @@ G4MuBremsstrahlungModel::G4MuBremsstrahlungModel(const G4ParticleDefinition* p,
|
||||
const G4String& nam)
|
||||
: G4VEmModel(nam),
|
||||
particle(0),
|
||||
sqrte(sqrt(exp(1.))),
|
||||
bh(202.4),
|
||||
bh1(446.),
|
||||
btf(183.),
|
||||
btf1(1429.),
|
||||
fParticleChange(0),
|
||||
lowestKinEnergy(1.0*GeV),
|
||||
minThreshold(1.0*keV),
|
||||
nzdat(5),
|
||||
ntdat(8),
|
||||
NBIN(1000),
|
||||
cutFixed(0.98*keV),
|
||||
ignoreCut(false),
|
||||
samplingTablesAreFilled(false)
|
||||
minThreshold(1.0*keV)
|
||||
{
|
||||
theGamma = G4Gamma::Gamma();
|
||||
nist = G4NistManager::Instance();
|
||||
if(p) SetParticle(p);
|
||||
}
|
||||
|
||||
@@ -116,24 +110,6 @@ G4MuBremsstrahlungModel::~G4MuBremsstrahlungModel()
|
||||
|
||||
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
|
||||
|
||||
G4double G4MuBremsstrahlungModel::MinEnergyCut(const G4ParticleDefinition*,
|
||||
const G4MaterialCutsCouple*)
|
||||
{
|
||||
return minThreshold;
|
||||
}
|
||||
|
||||
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
|
||||
|
||||
void G4MuBremsstrahlungModel::SetParticle(const G4ParticleDefinition* p)
|
||||
{
|
||||
if(!particle) {
|
||||
particle = p;
|
||||
mass = particle->GetPDGMass();
|
||||
}
|
||||
}
|
||||
|
||||
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
|
||||
|
||||
void G4MuBremsstrahlungModel::Initialise(const G4ParticleDefinition* p,
|
||||
const G4DataVector& cuts)
|
||||
{
|
||||
@@ -141,13 +117,15 @@ void G4MuBremsstrahlungModel::Initialise(const G4ParticleDefinition* p,
|
||||
|
||||
highKinEnergy = HighEnergyLimit();
|
||||
|
||||
// partial cross section is computed for fixed energy
|
||||
G4double fixedEnergy = 0.5*highKinEnergy;
|
||||
|
||||
const G4ProductionCutsTable* theCoupleTable=
|
||||
G4ProductionCutsTable::GetProductionCutsTable();
|
||||
if(theCoupleTable) {
|
||||
G4int numOfCouples = theCoupleTable->GetTableSize();
|
||||
|
||||
|
||||
// clear old data
|
||||
G4int nn = partialSumSigma.size();
|
||||
G4int nc = cuts.size();
|
||||
if(nn > 0) {
|
||||
@@ -157,11 +135,14 @@ void G4MuBremsstrahlungModel::Initialise(const G4ParticleDefinition* p,
|
||||
}
|
||||
partialSumSigma.clear();
|
||||
}
|
||||
// fill new data
|
||||
if (numOfCouples>0) {
|
||||
for (G4int i=0; i<numOfCouples; i++) {
|
||||
G4double cute = DBL_MAX;
|
||||
|
||||
// protection for usage with extrapolator
|
||||
if(i < nc) cute = cuts[i];
|
||||
if(cute < cutFixed || ignoreCut) cute = cutFixed;
|
||||
|
||||
const G4MaterialCutsCouple* couple =
|
||||
theCoupleTable->GetMaterialCutsCouple(i);
|
||||
const G4Material* material = couple->GetMaterial();
|
||||
@@ -170,12 +151,15 @@ void G4MuBremsstrahlungModel::Initialise(const G4ParticleDefinition* p,
|
||||
}
|
||||
}
|
||||
}
|
||||
if(!samplingTablesAreFilled) MakeSamplingTables();
|
||||
if(pParticleChange)
|
||||
fParticleChange =
|
||||
reinterpret_cast<G4ParticleChangeForLoss*>(pParticleChange);
|
||||
else
|
||||
fParticleChange = new G4ParticleChangeForLoss();
|
||||
|
||||
// define pointer to G4ParticleChange
|
||||
if(!fParticleChange) {
|
||||
if(pParticleChange)
|
||||
fParticleChange =
|
||||
reinterpret_cast<G4ParticleChangeForLoss*>(pParticleChange);
|
||||
else
|
||||
fParticleChange = new G4ParticleChangeForLoss();
|
||||
}
|
||||
}
|
||||
|
||||
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
|
||||
@@ -187,33 +171,32 @@ G4double G4MuBremsstrahlungModel::ComputeDEDXPerVolume(
|
||||
G4double cutEnergy)
|
||||
{
|
||||
G4double dedx = 0.0;
|
||||
if (kineticEnergy <= lowestKinEnergy || ignoreCut) return dedx;
|
||||
if (kineticEnergy <= lowestKinEnergy) return dedx;
|
||||
|
||||
G4double tmax = kineticEnergy;
|
||||
G4double cut = min(cutEnergy,tmax);
|
||||
if(cut < cutFixed) cut = cutFixed;
|
||||
G4double cut = std::min(cutEnergy,tmax);
|
||||
if(cut < minThreshold) cut = minThreshold;
|
||||
|
||||
const G4ElementVector* theElementVector = material->GetElementVector();
|
||||
const G4double* theAtomicNumDensityVector =
|
||||
material->GetAtomicNumDensityVector();
|
||||
material->GetAtomicNumDensityVector();
|
||||
|
||||
// loop for elements in the material
|
||||
for (size_t i=0; i<material->GetNumberOfElements(); i++) {
|
||||
|
||||
G4double Z = (*theElementVector)[i]->GetZ();
|
||||
G4double A = (*theElementVector)[i]->GetA()/(g/mole) ;
|
||||
|
||||
G4double loss = ComputMuBremLoss(Z, A, kineticEnergy, cut);
|
||||
G4double loss =
|
||||
ComputMuBremLoss((*theElementVector)[i]->GetZ(), kineticEnergy, cut);
|
||||
|
||||
dedx += loss*theAtomicNumDensityVector[i];
|
||||
}
|
||||
// G4cout << "BR e= " << kineticEnergy << " dedx= " << dedx << G4endl;
|
||||
if(dedx < 0.) dedx = 0.;
|
||||
return dedx;
|
||||
}
|
||||
|
||||
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
|
||||
|
||||
G4double G4MuBremsstrahlungModel::ComputMuBremLoss(G4double Z, G4double A,
|
||||
G4double G4MuBremsstrahlungModel::ComputMuBremLoss(G4double Z,
|
||||
G4double tkin, G4double cut)
|
||||
{
|
||||
G4double totalEnergy = mass + tkin;
|
||||
@@ -238,7 +221,7 @@ G4double G4MuBremsstrahlungModel::ComputMuBremLoss(G4double Z, G4double A,
|
||||
for(G4int i=0; i<6; i++)
|
||||
{
|
||||
G4double ep = (aa + xgi[i]*hhh)*totalEnergy;
|
||||
loss += ep*wgi[i]*ComputeDMicroscopicCrossSection(tkin, Z, A, ep);
|
||||
loss += ep*wgi[i]*ComputeDMicroscopicCrossSection(tkin, Z, ep);
|
||||
}
|
||||
aa += hhh;
|
||||
}
|
||||
@@ -253,7 +236,6 @@ G4double G4MuBremsstrahlungModel::ComputMuBremLoss(G4double Z, G4double A,
|
||||
G4double G4MuBremsstrahlungModel::ComputeMicroscopicCrossSection(
|
||||
G4double tkin,
|
||||
G4double Z,
|
||||
G4double A,
|
||||
G4double cut)
|
||||
{
|
||||
G4double totalEnergy = tkin + mass;
|
||||
@@ -271,7 +253,7 @@ G4double G4MuBremsstrahlungModel::ComputeMicroscopicCrossSection(
|
||||
G4double aaa = log(vcut);
|
||||
G4double bbb = log(vmax);
|
||||
G4int kkk = (G4int)((bbb-aaa)/ak1)+k2 ;
|
||||
G4double hhh = (bbb-aaa)/float(kkk);
|
||||
G4double hhh = (bbb-aaa)/G4double(kkk);
|
||||
|
||||
G4double aa = aaa;
|
||||
|
||||
@@ -280,13 +262,15 @@ G4double G4MuBremsstrahlungModel::ComputeMicroscopicCrossSection(
|
||||
for(G4int i=0; i<6; i++)
|
||||
{
|
||||
G4double ep = exp(aa + xgi[i]*hhh)*totalEnergy;
|
||||
cross += ep*wgi[i]*ComputeDMicroscopicCrossSection(tkin, Z, A, ep);
|
||||
cross += ep*wgi[i]*ComputeDMicroscopicCrossSection(tkin, Z, ep);
|
||||
}
|
||||
aa += hhh;
|
||||
}
|
||||
|
||||
cross *=hhh;
|
||||
|
||||
//G4cout << "BR e= " << tkin<< " cross= " << cross/barn << G4endl;
|
||||
|
||||
return cross;
|
||||
}
|
||||
|
||||
@@ -295,16 +279,9 @@ G4double G4MuBremsstrahlungModel::ComputeMicroscopicCrossSection(
|
||||
G4double G4MuBremsstrahlungModel::ComputeDMicroscopicCrossSection(
|
||||
G4double tkin,
|
||||
G4double Z,
|
||||
G4double A,
|
||||
G4double gammaEnergy)
|
||||
// differential cross section
|
||||
{
|
||||
static const G4double sqrte=sqrt(exp(1.)) ;
|
||||
static const G4double bh=202.4,bh1=446.,btf=183.,btf1=1429. ;
|
||||
static const G4double rmass=mass/electron_mass_c2 ;
|
||||
static const G4double cc=classic_electr_radius/rmass ;
|
||||
static const G4double coeff= 16.*fine_structure_const*cc*cc/3. ;
|
||||
|
||||
G4double dxsection = 0.;
|
||||
|
||||
if( gammaEnergy > tkin) return dxsection ;
|
||||
@@ -314,22 +291,25 @@ G4double G4MuBremsstrahlungModel::ComputeDMicroscopicCrossSection(
|
||||
G4double delta = 0.5*mass*mass*v/(E-gammaEnergy) ;
|
||||
G4double rab0=delta*sqrte ;
|
||||
|
||||
G4double z13 = exp(-log(Z)/3.) ;
|
||||
G4double dn = 1.54*exp(0.27*log(A)) ;
|
||||
G4int iz = G4int(Z);
|
||||
if(iz < 1) iz = 1;
|
||||
|
||||
G4double z13 = 1.0/nist->GetZ13(iz);
|
||||
G4double dn = 1.54*nist->GetA27(iz);
|
||||
|
||||
G4double b,b1,dnstar ;
|
||||
|
||||
if(Z<1.5)
|
||||
if(1 == iz)
|
||||
{
|
||||
b=bh;
|
||||
b1=bh1;
|
||||
dnstar=dn ;
|
||||
b = bh;
|
||||
b1 = bh1;
|
||||
dnstar = dn;
|
||||
}
|
||||
else
|
||||
{
|
||||
b=btf;
|
||||
b1=btf1;
|
||||
dnstar = exp((1.-1./Z)*log(dn)) ;
|
||||
b = btf;
|
||||
b1 = btf1;
|
||||
dnstar = dn/std::pow(dn, 1./Z);
|
||||
}
|
||||
|
||||
// nucleus contribution logarithm
|
||||
@@ -358,50 +338,21 @@ G4double G4MuBremsstrahlungModel::ComputeDMicroscopicCrossSection(
|
||||
G4double G4MuBremsstrahlungModel::ComputeCrossSectionPerAtom(
|
||||
const G4ParticleDefinition*,
|
||||
G4double kineticEnergy,
|
||||
G4double Z, G4double A,
|
||||
G4double Z, G4double,
|
||||
G4double cutEnergy,
|
||||
G4double)
|
||||
{
|
||||
G4double cut = min(cutEnergy, kineticEnergy);
|
||||
if(cut < cutFixed || ignoreCut) cut = cutFixed;
|
||||
G4double cross =
|
||||
ComputeMicroscopicCrossSection (kineticEnergy, Z, A/(g/mole), cut);
|
||||
return cross;
|
||||
}
|
||||
|
||||
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
|
||||
|
||||
G4double G4MuBremsstrahlungModel::CrossSectionPerVolume(
|
||||
const G4Material* material,
|
||||
const G4ParticleDefinition*,
|
||||
G4double kineticEnergy,
|
||||
G4double cutEnergy,
|
||||
G4double maxEnergy)
|
||||
G4double maxEnergy)
|
||||
{
|
||||
G4double cross = 0.0;
|
||||
if (cutEnergy >= maxEnergy || kineticEnergy <= lowestKinEnergy) return cross;
|
||||
|
||||
G4double tmax = min(maxEnergy, kineticEnergy);
|
||||
G4double cut = min(cutEnergy, tmax);
|
||||
if(cut < cutFixed || ignoreCut) cut = cutFixed;
|
||||
if (kineticEnergy <= lowestKinEnergy) return cross;
|
||||
G4double tmax = std::min(maxEnergy, kineticEnergy);
|
||||
G4double cut = std::min(cutEnergy, kineticEnergy);
|
||||
if(cut < minThreshold) cut = minThreshold;
|
||||
if (cut >= tmax) return cross;
|
||||
|
||||
const G4ElementVector* theElementVector = material->GetElementVector();
|
||||
const G4double* theAtomNumDensityVector =
|
||||
material->GetAtomicNumDensityVector();
|
||||
|
||||
for (size_t i=0; i<material->GetNumberOfElements(); i++) {
|
||||
|
||||
G4double Z = (*theElementVector)[i]->GetZ();
|
||||
G4double A = (*theElementVector)[i]->GetA()/(g/mole);
|
||||
|
||||
G4double cr = ComputeMicroscopicCrossSection(kineticEnergy, Z, A, cut);
|
||||
|
||||
if(tmax < kineticEnergy) {
|
||||
cr -= ComputeMicroscopicCrossSection(kineticEnergy, Z, A, tmax);
|
||||
}
|
||||
cross += theAtomNumDensityVector[i] * cr;
|
||||
cross = ComputeMicroscopicCrossSection (kineticEnergy, Z, cut);
|
||||
if(tmax < kineticEnergy) {
|
||||
cross -= ComputeMicroscopicCrossSection(kineticEnergy, Z, tmax);
|
||||
}
|
||||
|
||||
return cross;
|
||||
}
|
||||
|
||||
@@ -409,27 +360,26 @@ G4double G4MuBremsstrahlungModel::CrossSectionPerVolume(
|
||||
|
||||
G4DataVector* G4MuBremsstrahlungModel::ComputePartialSumSigma(
|
||||
const G4Material* material,
|
||||
G4double kineticEnergy,
|
||||
G4double cut)
|
||||
G4double kineticEnergy,
|
||||
G4double cut)
|
||||
|
||||
// Build the table of cross section per element. The table is built for MATERIAL
|
||||
// This table is used by DoIt to select randomly an element in the material.
|
||||
// Build the table of cross section per element.
|
||||
// The table is built for material
|
||||
// This table is used to select randomly an element in the material.
|
||||
{
|
||||
G4int nElements = material->GetNumberOfElements();
|
||||
const G4ElementVector* theElementVector = material->GetElementVector();
|
||||
const G4double* theAtomNumDensityVector =
|
||||
material->GetAtomicNumDensityVector();
|
||||
material->GetAtomicNumDensityVector();
|
||||
|
||||
G4DataVector* dv = new G4DataVector();
|
||||
|
||||
G4double cross = 0.0;
|
||||
|
||||
for (G4int i=0; i<nElements; i++ ) {
|
||||
|
||||
G4double Z = (*theElementVector)[i]->GetZ();
|
||||
G4double A = (*theElementVector)[i]->GetA()/(g/mole) ;
|
||||
cross += theAtomNumDensityVector[i]
|
||||
* ComputeMicroscopicCrossSection(kineticEnergy, Z, A, cut);
|
||||
* ComputeMicroscopicCrossSection(kineticEnergy,
|
||||
(*theElementVector)[i]->GetZ(), cut);
|
||||
dv->push_back(cross);
|
||||
}
|
||||
return dv;
|
||||
@@ -437,126 +387,52 @@ G4DataVector* G4MuBremsstrahlungModel::ComputePartialSumSigma(
|
||||
|
||||
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
|
||||
|
||||
void G4MuBremsstrahlungModel::MakeSamplingTables()
|
||||
{
|
||||
|
||||
G4double AtomicNumber,AtomicWeight,KineticEnergy,
|
||||
TotalEnergy,Maxep;
|
||||
|
||||
for (G4int iz=0; iz<nzdat; iz++)
|
||||
{
|
||||
AtomicNumber = zdat[iz];
|
||||
AtomicWeight = adat[iz]*g/mole ;
|
||||
|
||||
for (G4int it=0; it<ntdat; it++)
|
||||
{
|
||||
KineticEnergy = tdat[it];
|
||||
TotalEnergy = KineticEnergy + mass;
|
||||
Maxep = KineticEnergy ;
|
||||
|
||||
G4double CrossSection = 0.0 ;
|
||||
|
||||
// calculate the differential cross section
|
||||
// numerical integration in
|
||||
// log ...............
|
||||
G4double c = log(Maxep/cutFixed) ;
|
||||
G4double ymin = -5. ;
|
||||
G4double ymax = 0. ;
|
||||
G4double dy = (ymax-ymin)/NBIN ;
|
||||
|
||||
G4double y = ymin - 0.5*dy ;
|
||||
G4double yy = ymin - dy ;
|
||||
G4double x = exp(y);
|
||||
G4double fac = exp(dy);
|
||||
G4double dx = exp(yy)*(fac - 1.0);
|
||||
|
||||
for (G4int i=0 ; i<NBIN; i++)
|
||||
{
|
||||
y += dy ;
|
||||
x *= fac;
|
||||
dx*= fac;
|
||||
G4double ep = cutFixed*exp(c*x) ;
|
||||
|
||||
CrossSection += ep*dx*ComputeDMicroscopicCrossSection(
|
||||
KineticEnergy,AtomicNumber,
|
||||
AtomicWeight,ep) ;
|
||||
ya[i]=y ;
|
||||
proba[iz][it][i] = CrossSection ;
|
||||
|
||||
}
|
||||
|
||||
proba[iz][it][NBIN] = CrossSection ;
|
||||
ya[NBIN] = 0. ; // !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!
|
||||
|
||||
if(CrossSection > 0.)
|
||||
{
|
||||
for(G4int ib=0; ib<=NBIN; ib++)
|
||||
{
|
||||
proba[iz][it][ib] /= CrossSection ;
|
||||
}
|
||||
}
|
||||
}
|
||||
}
|
||||
samplingTablesAreFilled = true;
|
||||
}
|
||||
|
||||
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
|
||||
|
||||
void G4MuBremsstrahlungModel::SampleSecondaries(std::vector<G4DynamicParticle*>* vdp,
|
||||
const G4MaterialCutsCouple* couple,
|
||||
const G4DynamicParticle* dp,
|
||||
G4double minEnergy,
|
||||
G4double maxEnergy)
|
||||
void G4MuBremsstrahlungModel::SampleSecondaries(
|
||||
std::vector<G4DynamicParticle*>* vdp,
|
||||
const G4MaterialCutsCouple* couple,
|
||||
const G4DynamicParticle* dp,
|
||||
G4double minEnergy,
|
||||
G4double maxEnergy)
|
||||
{
|
||||
G4double kineticEnergy = dp->GetKineticEnergy();
|
||||
// check against insufficient energy
|
||||
G4double tmax = min(kineticEnergy, maxEnergy);
|
||||
G4double tmin = min(kineticEnergy, minEnergy);
|
||||
if(tmin < cutFixed || ignoreCut) tmin = cutFixed;
|
||||
G4double tmax = std::min(kineticEnergy, maxEnergy);
|
||||
G4double tmin = std::min(kineticEnergy, minEnergy);
|
||||
if(tmin < minThreshold) tmin = minThreshold;
|
||||
if(tmin >= tmax) return;
|
||||
|
||||
// ===== the begining of a new code ======
|
||||
// ===== sampling of energy transfer ======
|
||||
|
||||
G4ParticleMomentum partDirection = dp->GetMomentumDirection();
|
||||
|
||||
// select randomly one element constituing the material
|
||||
const G4Element* anElement = SelectRandomAtom(couple);
|
||||
G4double Z = anElement->GetZ();
|
||||
|
||||
G4double totalEnergy = kineticEnergy + mass;
|
||||
G4double totalMomentum = sqrt(kineticEnergy*(kineticEnergy + 2.0*mass));
|
||||
|
||||
G4double AtomicNumber = anElement->GetZ();
|
||||
G4double AtomicWeight = anElement->GetA()/(g/mole);
|
||||
|
||||
G4double func1 = tmin*ComputeDMicroscopicCrossSection(
|
||||
kineticEnergy,AtomicNumber,
|
||||
AtomicWeight,tmin);
|
||||
G4double func1 = tmin*
|
||||
ComputeDMicroscopicCrossSection(kineticEnergy,Z,tmin);
|
||||
|
||||
G4double lnepksi, epksi;
|
||||
G4double func2;
|
||||
G4double ksi2;
|
||||
|
||||
do {
|
||||
lnepksi = log(tmin) + G4UniformRand()*log(kineticEnergy/tmin);
|
||||
epksi = exp(lnepksi);
|
||||
func2 = epksi*ComputeDMicroscopicCrossSection(
|
||||
kineticEnergy,AtomicNumber,
|
||||
AtomicWeight,epksi);
|
||||
ksi2 = G4UniformRand();
|
||||
func2 = epksi*ComputeDMicroscopicCrossSection(kineticEnergy,Z,epksi);
|
||||
|
||||
} while(func2/func1 < ksi2);
|
||||
} while(func2 < func1*G4UniformRand());
|
||||
|
||||
// ===== the end of a new code =====
|
||||
|
||||
// create G4DynamicParticle object for the Gamma
|
||||
G4double gEnergy = epksi;
|
||||
|
||||
// sample angle
|
||||
// ===== sample angle =====
|
||||
|
||||
G4double gam = totalEnergy/mass;
|
||||
G4double rmax = gam*min(1.0, totalEnergy/gEnergy - 1.0);
|
||||
rmax *= rmax;
|
||||
G4double x = G4UniformRand()*rmax/(1.0 + rmax);
|
||||
G4double rmax = gam*std::min(1.0, totalEnergy/gEnergy - 1.0);
|
||||
G4double rmax2= rmax*rmax;
|
||||
G4double x = G4UniformRand()*rmax2/(1.0 + rmax2);
|
||||
|
||||
G4double theta = sqrt(x/(1.0 - x))/gam;
|
||||
G4double sint = sin(theta);
|
||||
@@ -576,7 +452,8 @@ void G4MuBremsstrahlungModel::SampleSecondaries(std::vector<G4DynamicParticle*>*
|
||||
fParticleChange->SetProposedMomentumDirection(partDirection);
|
||||
|
||||
// save secondary
|
||||
G4DynamicParticle* aGamma = new G4DynamicParticle(theGamma,gDirection,gEnergy);
|
||||
G4DynamicParticle* aGamma =
|
||||
new G4DynamicParticle(theGamma,gDirection,gEnergy);
|
||||
vdp->push_back(aGamma);
|
||||
}
|
||||
|
||||
|
||||
Reference in New Issue
Block a user