Import Geant4 9.3.0 source tree
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@@ -23,8 +23,8 @@
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// * acceptance of all terms of the Geant4 Software license. *
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// ********************************************************************
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//
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// $Id: G4eCoulombScatteringModel.cc,v 1.59 2008/10/22 18:39:29 vnivanch Exp $
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// GEANT4 tag $Name: geant4-09-02 $
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// $Id: G4eCoulombScatteringModel.cc,v 1.78 2009/10/28 10:14:13 vnivanch Exp $
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// GEANT4 tag $Name: geant4-09-03 $
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//
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// -------------------------------------------------------------------
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//
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@@ -38,12 +38,15 @@
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// Creation date: 22.08.2005
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//
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// Modifications:
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//
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// 01.08.06 V.Ivanchenko extend upper limit of table to TeV and review the
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// logic of building - only elements from G4ElementTable
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// 08.08.06 V.Ivanchenko build internal table in ekin scale, introduce faclim
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// 19.08.06 V.Ivanchenko add inline function ScreeningParameter
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// 09.10.07 V.Ivanchenko reorganized methods, add cut dependence in scattering off e-
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// 09.06.08 V.Ivanchenko add SelectIsotope and sampling of the recoil ion
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// 16.06.09 C.Consolandi fixed computation of effective mass
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//
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//
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// Class Description:
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//
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@@ -62,9 +65,14 @@
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#include "G4Positron.hh"
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#include "G4Proton.hh"
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#include "G4ParticleTable.hh"
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#include "G4ProductionCutsTable.hh"
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#include "G4NucleiProperties.hh"
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//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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G4double G4eCoulombScatteringModel::ScreenRSquare[] = {0.0};
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G4double G4eCoulombScatteringModel::FormFactor[] = {0.0};
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using namespace std;
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G4eCoulombScatteringModel::G4eCoulombScatteringModel(const G4String& nam)
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@@ -83,19 +91,31 @@ G4eCoulombScatteringModel::G4eCoulombScatteringModel(const G4String& nam)
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theProton = G4Proton::Proton();
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currentMaterial = 0;
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currentElement = 0;
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a0 = alpha2*electron_mass_c2*electron_mass_c2/(0.885*0.885);
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lowEnergyLimit = 0.1*keV;
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G4double p0 = electron_mass_c2*classic_electr_radius;
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coeff = twopi*p0*p0;
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constn = 6.937e-6/(MeV*MeV);
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tkin = targetZ = mom2 = DBL_MIN;
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elecXSection = nucXSection = 0.0;
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recoilThreshold = DBL_MAX;
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recoilThreshold = 0.*keV;
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ecut = DBL_MAX;
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particle = 0;
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currentCouple = 0;
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for(size_t j=0; j<100; j++) {
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FF[j] = 0.0;
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}
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// Thomas-Fermi screening radii
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// Formfactors from A.V. Butkevich et al., NIM A 488 (2002) 282
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if(0.0 == ScreenRSquare[0]) {
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G4double a0 = electron_mass_c2/0.88534;
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G4double constn = 6.937e-6/(MeV*MeV);
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ScreenRSquare[0] = alpha2*a0*a0;
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for(G4int j=1; j<100; j++) {
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G4double x = a0*fNistManager->GetZ13(j);
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ScreenRSquare[j] = alpha2*x*x;
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x = fNistManager->GetA27(j);
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FormFactor[j] = constn*x*x;
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}
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}
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}
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//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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@@ -114,18 +134,14 @@ void G4eCoulombScatteringModel::Initialise(const G4ParticleDefinition* p,
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tkin = targetZ = mom2 = DBL_MIN;
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ecut = etag = DBL_MAX;
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cosThetaMin = cos(PolarAngleLimit());
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currentCuts = &cuts;
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pCuts = G4ProductionCutsTable::GetProductionCutsTable()->GetEnergyCutsVector(3);
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//G4cout << "!!! G4eCoulombScatteringModel::Initialise for "
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// << p->GetParticleName() << " cos(TetMin)= " << cosThetaMin
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// << " cos(TetMax)= " << cosThetaMax <<G4endl;
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// G4cout << "cut0= " << cuts[0] << " cut1= " << cuts[1] << G4endl;
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if(!isInitialised) {
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isInitialised = true;
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if(pParticleChange)
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fParticleChange =
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reinterpret_cast<G4ParticleChangeForGamma*>(pParticleChange);
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else
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fParticleChange = new G4ParticleChangeForGamma();
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fParticleChange = GetParticleChangeForGamma();
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}
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if(mass < GeV && particle->GetParticleType() != "nucleus") {
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InitialiseElementSelectors(p,cuts);
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@@ -156,7 +172,8 @@ void G4eCoulombScatteringModel::ComputeMaxElectronScattering(G4double cutEnergy)
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G4double mom22 = t1*(t1 + 2.0*mass);
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G4double ctm = (mom2 + mom22 - mom21)*0.5/sqrt(mom2*mom22);
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//G4cout << "ctm= " << ctm << G4endl;
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if(ctm < 1.0) cosTetMaxElec = ctm;
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if(ctm < 1.0) cosTetMaxElec = ctm;
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if(ctm < -1.0) cosTetMaxElec = -1.0;
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}
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}
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}
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@@ -173,10 +190,10 @@ G4double G4eCoulombScatteringModel::ComputeCrossSectionPerAtom(
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// << p->GetParticleName()<<" Z= "<<Z<<" e(MeV)= "<< kinEnergy/MeV << G4endl;
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G4double xsec = 0.0;
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SetupParticle(p);
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G4double ekin = std::max(lowEnergyLimit, kinEnergy);
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SetupKinematic(ekin, cutEnergy);
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if(kinEnergy < lowEnergyLimit) return xsec;
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SetupKinematic(kinEnergy, cutEnergy);
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if(cosTetMaxNuc < cosTetMinNuc) {
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SetupTarget(Z, ekin);
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SetupTarget(Z, kinEnergy);
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xsec = CrossSectionPerAtom();
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}
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/*
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@@ -184,8 +201,7 @@ G4double G4eCoulombScatteringModel::ComputeCrossSectionPerAtom(
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<< " cosTetMaxNuc= " << cosTetMaxNuc
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<< " cosTetMaxElec= " << cosTetMaxElec
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<< " screenZ= " << screenZ
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<< " formfactA= " << formfactA
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<< " cosTetMaxHad= " << cosTetMaxHad << G4endl;
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<< " formfactA= " << formfactA << G4endl;
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*/
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return xsec;
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}
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@@ -195,8 +211,11 @@ G4double G4eCoulombScatteringModel::ComputeCrossSectionPerAtom(
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G4double G4eCoulombScatteringModel::CrossSectionPerAtom()
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{
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// This method needs initialisation before be called
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//G4double fac = coeff*targetZ*chargeSquare*invbeta2/mom2;
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G4double meff = targetMass/(mass+targetMass);
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G4double fac = coeff*targetZ*chargeSquare*invbeta2/(mom2*meff*meff);
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G4double fac = coeff*targetZ*chargeSquare*invbeta2/mom2;
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elecXSection = 0.0;
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nucXSection = 0.0;
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@@ -215,7 +234,8 @@ G4double G4eCoulombScatteringModel::CrossSectionPerAtom()
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if(cosTetMaxNuc2 < cosTetMinNuc) {
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G4double s = screenZ*formfactA;
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G4double z1 = 1.0 - cosTetMaxNuc2 + screenZ;
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G4double d = (1.0 - s)/formfactA;
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G4double s1 = 1.0 - s;
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G4double d = s1/formfactA;
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//G4cout <<"x1= "<<x1<<" z1= " <<z1<<" s= "<<s << " d= " <<d <<G4endl;
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if(d < 0.2*x1) {
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G4double x2 = x1*x1;
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@@ -225,12 +245,10 @@ G4double G4eCoulombScatteringModel::CrossSectionPerAtom()
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} else {
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G4double x2 = x1 + d;
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G4double z2 = z1 + d;
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x = (1.0 + 2.0*s)*((cosTetMinNuc - cosTetMaxNuc2)*(1.0/(x1*z1) + 1.0/(x2*z2)) -
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2.0*log(z1*x2/(z2*x1))/d);
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x = (1.0/x1 - 1.0/z1 + 1.0/x2 - 1.0/z2 - 2.0*log(z1*x2/(z2*x1))/d)/(s1*s1);
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}
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nucXSection += fac*targetZ*x;
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}
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//G4cout<<" cross(bn)= "<<nucXSection/barn<<" xsElec(bn)= "<<elecXSection/barn
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// << " Asc= " << screenZ << G4endl;
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@@ -247,18 +265,23 @@ void G4eCoulombScatteringModel::SampleSecondaries(
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G4double)
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{
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G4double kinEnergy = dp->GetKineticEnergy();
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if(kinEnergy <= DBL_MIN) return;
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if(kinEnergy < lowEnergyLimit) return;
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DefineMaterial(couple);
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SetupParticle(dp->GetDefinition());
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G4double ekin = std::max(lowEnergyLimit, kinEnergy);
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SetupKinematic(ekin, cutEnergy);
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SetupKinematic(kinEnergy, cutEnergy);
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//G4cout << "G4eCoulombScatteringModel::SampleSecondaries e(MeV)= "
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// << kinEnergy << " " << particle->GetParticleName() << G4endl;
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// << kinEnergy << " " << particle->GetParticleName()
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// << " cut= " << cutEnergy<< G4endl;
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// Choose nucleus
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currentElement = SelectRandomAtom(couple,particle,ekin,cutEnergy,ekin);
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currentElement = SelectRandomAtom(couple,particle,
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kinEnergy,cutEnergy,kinEnergy);
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SetupTarget(currentElement->GetZ(),ekin);
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SetupTarget(currentElement->GetZ(),kinEnergy);
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G4int ia = SelectIsotopeNumber(currentElement);
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targetMass = G4NucleiProperties::GetNuclearMass(ia, iz);
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G4double cost = SampleCosineTheta();
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G4double z1 = 1.0 - cost;
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@@ -266,7 +289,7 @@ void G4eCoulombScatteringModel::SampleSecondaries(
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G4double sint = sqrt(z1*(1.0 + cost));
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//G4cout<<"## Sampled sint= " << sint << " Z= " << targetZ
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//G4cout<<"## Sampled sint= " << sint << " Z= " << targetZ << " A= " << ia
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// << " screenZ= " << screenZ << " cn= " << formfactA << G4endl;
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G4double phi = twopi * G4UniformRand();
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@@ -279,24 +302,28 @@ void G4eCoulombScatteringModel::SampleSecondaries(
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// recoil sampling assuming a small recoil
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// and first order correction to primary 4-momentum
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if(lowEnergyLimit < kinEnergy) {
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G4int ia = SelectIsotopeNumber(currentElement);
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G4double Trec = z1*mom2/(amu_c2*G4double(ia));
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G4double th =
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std::min(recoilThreshold,
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targetZ*currentElement->GetIonisation()->GetMeanExcitationEnergy());
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G4double q2 = 2*z1*mom2;
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G4double trec = q2/(sqrt(targetMass*targetMass + q2) + targetMass);
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G4double finalT = kinEnergy - trec;
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//G4cout<<"G4eCoulombScatteringModel: finalT= "<<finalT<<" Trec= "<<trec<<G4endl;
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if(finalT <= lowEnergyLimit) {
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trec = kinEnergy;
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finalT = 0.0;
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}
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if(Trec > th) {
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G4int iz = G4int(targetZ);
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G4ParticleDefinition* ion = theParticleTable->FindIon(iz, ia, 0, iz);
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Trec = z1*mom2/ion->GetPDGMass();
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if(Trec < kinEnergy) {
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G4ThreeVector dir = (direction - newDirection).unit();
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G4DynamicParticle* newdp = new G4DynamicParticle(ion, dir, Trec);
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fvect->push_back(newdp);
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fParticleChange->SetProposedKineticEnergy(kinEnergy - Trec);
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}
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}
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fParticleChange->SetProposedKineticEnergy(finalT);
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G4double tcut = recoilThreshold;
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if(pCuts) { tcut= std::max(tcut,(*pCuts)[currentMaterialIndex]); }
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if(trec > tcut) {
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G4ParticleDefinition* ion = theParticleTable->FindIon(iz, ia, 0, iz);
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G4ThreeVector dir = (direction*sqrt(mom2) -
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newDirection*sqrt(finalT*(2*mass + finalT))).unit();
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G4DynamicParticle* newdp = new G4DynamicParticle(ion, dir, trec);
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fvect->push_back(newdp);
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} else {
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fParticleChange->ProposeLocalEnergyDeposit(trec);
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fParticleChange->ProposeNonIonizingEnergyDeposit(trec);
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}
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return;
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@@ -318,14 +345,14 @@ G4double G4eCoulombScatteringModel::SampleCosineTheta()
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formf = 0.0;
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}
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/*
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/*
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G4cout << "SampleCost: e(MeV)= " << tkin
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<< " ctmin= " << cosThetaMin
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<< " ctmaxN= " << cosTetMaxNuc
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<< " ctmax= " << costm
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<< " Z= " << targetZ << " A= " << targetA
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<< " 1-ctmaxN= " << 1. - cosTetMinNuc
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<< " 1-ctmax= " << 1. - costm
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<< " Z= " << targetZ
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<< G4endl;
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*/
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if(costm >= cosTetMinNuc) return 2.0;
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G4double x1 = 1. - cosTetMinNuc + screenZ;
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@@ -337,8 +364,13 @@ G4double G4eCoulombScatteringModel::SampleCosineTheta()
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grej = 1.0/(1.0 + formf*z1);
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} while ( G4UniformRand() > grej*grej );
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//G4cout << "z= " << z1 << " cross= " << nucXSection/barn
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// << " crossE= " << elecXSection/barn << G4endl;
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if(mass > MeV) {
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if(G4UniformRand() > (1. - z1*0.5)/(1.0 + z1*sqrt(mom2)/targetMass)) {
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return 2.0;
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}
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}
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//G4cout << "z1= " << z1 << " cross= " << nucXSection/barn
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// << " crossE= " << elecXSection/barn << G4endl;
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return 1.0 - z1;
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}
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