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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: G4AdjointhIonisationModel.cc,v 1.3 2009/12/16 17:50:07 gunter Exp $ // GEANT4 tag $Name: geant4-09-03 $ // #include "G4AdjointhIonisationModel.hh" #include "G4AdjointCSManager.hh" #include "G4Integrator.hh" #include "G4TrackStatus.hh" #include "G4ParticleChange.hh" #include "G4AdjointElectron.hh" #include "G4AdjointProton.hh" #include "G4AdjointInterpolator.hh" #include "G4BetheBlochModel.hh" #include "G4BraggModel.hh" #include "G4Proton.hh" #include "G4NistManager.hh" //////////////////////////////////////////////////////////////////////////////// // G4AdjointhIonisationModel::G4AdjointhIonisationModel(G4ParticleDefinition* projectileDefinition): G4VEmAdjointModel("Adjoint_hIonisation") { UseMatrix =true; UseMatrixPerElement = true; ApplyCutInRange = true; UseOnlyOneMatrixForAllElements = true; CS_biasing_factor =1.; second_part_of_same_type =false; //The direct EM Modfel is taken has BetheBloch it is only used for the computation // of the differential cross section. //The Bragg model could be used as an alternative as it offers the same differential cross section theDirectEMModel = new G4BetheBlochModel(projectileDefinition); theBraggDirectEMModel = new G4BraggModel(projectileDefinition); theAdjEquivOfDirectSecondPartDef=G4AdjointElectron::AdjointElectron(); theDirectPrimaryPartDef = projectileDefinition; if (projectileDefinition == G4Proton::Proton()) { theAdjEquivOfDirectPrimPartDef = G4AdjointProton::AdjointProton(); } DefineProjectileProperty(); } //////////////////////////////////////////////////////////////////////////////// // G4AdjointhIonisationModel::~G4AdjointhIonisationModel() {;} //////////////////////////////////////////////////////////////////////////////// // void G4AdjointhIonisationModel::SampleSecondaries(const G4Track& aTrack, G4bool IsScatProjToProjCase, G4ParticleChange* fParticleChange) { if (!UseMatrix) return RapidSampleSecondaries(aTrack,IsScatProjToProjCase,fParticleChange); const G4DynamicParticle* theAdjointPrimary =aTrack.GetDynamicParticle(); //Elastic inverse scattering //--------------------------------------------------------- G4double adjointPrimKinEnergy = theAdjointPrimary->GetKineticEnergy(); G4double adjointPrimP =theAdjointPrimary->GetTotalMomentum(); if (adjointPrimKinEnergy>HighEnergyLimit*0.999){ return; } //Sample secondary energy //----------------------- G4double projectileKinEnergy = SampleAdjSecEnergyFromCSMatrix(adjointPrimKinEnergy, IsScatProjToProjCase); CorrectPostStepWeight(fParticleChange, aTrack.GetWeight(), adjointPrimKinEnergy, projectileKinEnergy, IsScatProjToProjCase); //Caution !!!this weight correction should be always applied //Kinematic: //we consider a two body elastic scattering for the forward processes where the projectile knock on an e- at rest and gives // him part of its energy //---------------------------------------------------------------------------------------- G4double projectileM0 = theAdjEquivOfDirectPrimPartDef->GetPDGMass(); G4double projectileTotalEnergy = projectileM0+projectileKinEnergy; G4double projectileP2 = projectileTotalEnergy*projectileTotalEnergy - projectileM0*projectileM0; //Companion //----------- G4double companionM0 = theAdjEquivOfDirectPrimPartDef->GetPDGMass(); if (IsScatProjToProjCase) { companionM0=theAdjEquivOfDirectSecondPartDef->GetPDGMass(); } G4double companionTotalEnergy =companionM0+ projectileKinEnergy-adjointPrimKinEnergy; G4double companionP2 = companionTotalEnergy*companionTotalEnergy - companionM0*companionM0; //Projectile momentum //-------------------- G4double P_parallel = (adjointPrimP*adjointPrimP + projectileP2 - companionP2)/(2.*adjointPrimP); G4double P_perp = std::sqrt( projectileP2 - P_parallel*P_parallel); G4ThreeVector dir_parallel=theAdjointPrimary->GetMomentumDirection(); G4double phi =G4UniformRand()*2.*3.1415926; G4ThreeVector projectileMomentum = G4ThreeVector(P_perp*std::cos(phi),P_perp*std::sin(phi),P_parallel); projectileMomentum.rotateUz(dir_parallel); if (!IsScatProjToProjCase ){ //kill the primary and add a secondary fParticleChange->ProposeTrackStatus(fStopAndKill); fParticleChange->AddSecondary(new G4DynamicParticle(theAdjEquivOfDirectPrimPartDef,projectileMomentum)); //G4cout<<"projectileMomentum "<ProposeEnergy(projectileKinEnergy); fParticleChange->ProposeMomentumDirection(projectileMomentum.unit()); } } //////////////////////////////////////////////////////////////////////////////// // void G4AdjointhIonisationModel::RapidSampleSecondaries(const G4Track& aTrack, G4bool IsScatProjToProjCase, G4ParticleChange* fParticleChange) { const G4DynamicParticle* theAdjointPrimary =aTrack.GetDynamicParticle(); DefineCurrentMaterial(aTrack.GetMaterialCutsCouple()); G4double adjointPrimKinEnergy = theAdjointPrimary->GetKineticEnergy(); G4double adjointPrimP =theAdjointPrimary->GetTotalMomentum(); if (adjointPrimKinEnergy>HighEnergyLimit*0.999){ return; } G4double projectileKinEnergy =0.; G4double eEnergy=0.; G4double newCS=currentMaterial->GetElectronDensity()*twopi_mc2_rcl2*mass; if (!IsScatProjToProjCase){//1/E^2 distribution eEnergy=adjointPrimKinEnergy; G4double Emax = GetSecondAdjEnergyMaxForProdToProjCase(adjointPrimKinEnergy); G4double Emin= GetSecondAdjEnergyMinForProdToProjCase(adjointPrimKinEnergy); if (Emin>=Emax) return; G4double a=1./Emax; G4double b=1./Emin; newCS=newCS*(b-a)/eEnergy; projectileKinEnergy =1./(b- (b-a)*G4UniformRand()); } else { G4double Emax = GetSecondAdjEnergyMaxForScatProjToProjCase(adjointPrimKinEnergy); G4double Emin = GetSecondAdjEnergyMinForScatProjToProjCase(adjointPrimKinEnergy,currentTcutForDirectSecond); if (Emin>=Emax) return; G4double diff1=Emin-adjointPrimKinEnergy; G4double diff2=Emax-adjointPrimKinEnergy; G4double t1=adjointPrimKinEnergy*(1./diff1-1./diff2); G4double t2=adjointPrimKinEnergy*(1./Emin-1./Emax); G4double f31=diff1/Emin; G4double f32=diff2/Emax/f31; G4double t3=2.*std::log(f32); G4double sum_t=t1+t2+t3; newCS=newCS*sum_t/adjointPrimKinEnergy/adjointPrimKinEnergy; G4double t=G4UniformRand()*sum_t; if (t <=t1 ){ G4double q= G4UniformRand()*t1/adjointPrimKinEnergy ; projectileKinEnergy =adjointPrimKinEnergy +1./(1./diff1-q); } else if (t <=t2 ) { G4double q= G4UniformRand()*t2/adjointPrimKinEnergy; projectileKinEnergy =1./(1./Emin-q); } else { projectileKinEnergy=adjointPrimKinEnergy/(1.-f31*std::pow(f32,G4UniformRand())); } eEnergy=projectileKinEnergy-adjointPrimKinEnergy; } G4double diffCS_perAtom_Used=twopi_mc2_rcl2*mass*adjointPrimKinEnergy/projectileKinEnergy/projectileKinEnergy/eEnergy/eEnergy; //Weight correction //----------------------- //First w_corr is set to the ratio between adjoint total CS and fwd total CS G4double w_corr=G4AdjointCSManager::GetAdjointCSManager()->GetPostStepWeightCorrection(); //G4cout<SetParentWeightByProcess(false); fParticleChange->SetSecondaryWeightByProcess(false); fParticleChange->ProposeParentWeight(new_weight); //Kinematic: //we consider a two body elastic scattering for the forward processes where the projectile knock on an e- at rest and gives // him part of its energy //---------------------------------------------------------------------------------------- G4double projectileM0 = theAdjEquivOfDirectPrimPartDef->GetPDGMass(); G4double projectileTotalEnergy = projectileM0+projectileKinEnergy; G4double projectileP2 = projectileTotalEnergy*projectileTotalEnergy - projectileM0*projectileM0; //Companion //----------- G4double companionM0 = theAdjEquivOfDirectPrimPartDef->GetPDGMass(); if (IsScatProjToProjCase) { companionM0=theAdjEquivOfDirectSecondPartDef->GetPDGMass(); } G4double companionTotalEnergy =companionM0+ projectileKinEnergy-adjointPrimKinEnergy; G4double companionP2 = companionTotalEnergy*companionTotalEnergy - companionM0*companionM0; //Projectile momentum //-------------------- G4double P_parallel = (adjointPrimP*adjointPrimP + projectileP2 - companionP2)/(2.*adjointPrimP); G4double P_perp = std::sqrt( projectileP2 - P_parallel*P_parallel); G4ThreeVector dir_parallel=theAdjointPrimary->GetMomentumDirection(); G4double phi =G4UniformRand()*2.*3.1415926; G4ThreeVector projectileMomentum = G4ThreeVector(P_perp*std::cos(phi),P_perp*std::sin(phi),P_parallel); projectileMomentum.rotateUz(dir_parallel); if (!IsScatProjToProjCase ){ //kill the primary and add a secondary fParticleChange->ProposeTrackStatus(fStopAndKill); fParticleChange->AddSecondary(new G4DynamicParticle(theAdjEquivOfDirectPrimPartDef,projectileMomentum)); //G4cout<<"projectileMomentum "<ProposeEnergy(projectileKinEnergy); fParticleChange->ProposeMomentumDirection(projectileMomentum.unit()); } } //////////////////////////////////////////////////////////////////////////////// // G4double G4AdjointhIonisationModel::DiffCrossSectionPerAtomPrimToSecond( G4double kinEnergyProj, G4double kinEnergyProd, G4double Z, G4double A) {//Probably that here the Bragg Model should be also used for kinEnergyProj/nuc<2MeV G4double dSigmadEprod=0; G4double Emax_proj = GetSecondAdjEnergyMaxForProdToProjCase(kinEnergyProd); G4double Emin_proj = GetSecondAdjEnergyMinForProdToProjCase(kinEnergyProd); if (kinEnergyProj>Emin_proj && kinEnergyProj<=Emax_proj){ //the produced particle should have a kinetic energy smaller than the projectile G4double Tmax=kinEnergyProj; G4double E1=kinEnergyProd; G4double E2=kinEnergyProd*1.000001; G4double dE=(E2-E1); G4double sigma1,sigma2; if (kinEnergyProj >2.*MeV){ sigma1=theDirectEMModel->ComputeCrossSectionPerAtom(theDirectPrimaryPartDef,kinEnergyProj,Z,A ,E1,1.e20); sigma2=theDirectEMModel->ComputeCrossSectionPerAtom(theDirectPrimaryPartDef,kinEnergyProj,Z,A ,E2,1.e20); } else { sigma1=theBraggDirectEMModel->ComputeCrossSectionPerAtom(theDirectPrimaryPartDef,kinEnergyProj,Z,A ,E1,1.e20); sigma2=theBraggDirectEMModel->ComputeCrossSectionPerAtom(theDirectPrimaryPartDef,kinEnergyProj,Z,A ,E2,1.e20); } dSigmadEprod=(sigma1-sigma2)/dE; if (dSigmadEprod>1.) { G4cout<<"sigma1 "< 1.e-6) { G4double totEnergy = kinEnergyProj + mass; G4double etot2 = totEnergy*totEnergy; G4double beta2 = kinEnergyProj*(kinEnergyProj + 2.0*mass)/etot2; G4double f; G4double f1 = 0.0; f = 1.0 - beta2*deltaKinEnergy/Tmax; if( 0.5 == spin ) { f1 = 0.5*deltaKinEnergy*deltaKinEnergy/etot2; f += f1; } G4double x1 = 1.0 + x; G4double g = 1.0/(x1*x1); if( 0.5 == spin ) { G4double x2 = 0.5*electron_mass_c2*deltaKinEnergy/(mass*mass); g *= (1.0 + magMoment2*(x2 - f1/f)/(1.0 + x2)); } if(g > 1.0) { G4cout << "### G4BetheBlochModel in Adjoint Sim WARNING: g= " << g << G4endl; g=1.; } //G4cout<<"g"<GetParticleName(); if (theDirectPrimaryPartDef->GetParticleType() == "nucleus" && pname != "deuteron" && pname != "triton") { isIon = true; } mass = theDirectPrimaryPartDef->GetPDGMass(); spin = theDirectPrimaryPartDef->GetPDGSpin(); G4double q = theDirectPrimaryPartDef->GetPDGCharge()/eplus; chargeSquare = q*q; ratio = electron_mass_c2/mass; ratio2 = ratio*ratio; one_plus_ratio_2=(1+ratio)*(1+ratio); one_minus_ratio_2=(1-ratio)*(1-ratio); G4double magmom = theDirectPrimaryPartDef->GetPDGMagneticMoment() *mass/(0.5*eplus*hbar_Planck*c_squared); magMoment2 = magmom*magmom - 1.0; formfact = 0.0; if(theDirectPrimaryPartDef->GetLeptonNumber() == 0) { G4double x = 0.8426*GeV; if(spin == 0.0 && mass < GeV) {x = 0.736*GeV;} else if(mass > GeV) { x /= G4NistManager::Instance()->GetZ13(mass/proton_mass_c2); // tlimit = 51.2*GeV*A13[iz]*A13[iz]; } formfact = 2.0*electron_mass_c2/(x*x); tlimit = 2.0/formfact; } } //////////////////////////////////////////////////////////////////////////////// // G4double G4AdjointhIonisationModel::AdjointCrossSection(const G4MaterialCutsCouple* aCouple, G4double primEnergy, G4bool IsScatProjToProjCase) { if (UseMatrix) return G4VEmAdjointModel::AdjointCrossSection(aCouple,primEnergy,IsScatProjToProjCase); DefineCurrentMaterial(aCouple); G4double Cross=currentMaterial->GetElectronDensity()*twopi_mc2_rcl2*mass; if (!IsScatProjToProjCase ){ G4double Emax_proj = GetSecondAdjEnergyMaxForProdToProjCase(primEnergy); G4double Emin_proj = GetSecondAdjEnergyMinForProdToProjCase(primEnergy); if (Emax_proj>Emin_proj && primEnergy > currentTcutForDirectSecond) { Cross*=(1./Emin_proj -1./Emax_proj)/primEnergy; } else Cross=0.; } else { G4double Emax_proj = GetSecondAdjEnergyMaxForScatProjToProjCase(primEnergy); G4double Emin_proj = GetSecondAdjEnergyMinForScatProjToProjCase(primEnergy,currentTcutForDirectSecond); G4double diff1=Emin_proj-primEnergy; G4double diff2=Emax_proj-primEnergy; G4double t1=(1./diff1+1./Emin_proj-1./diff2-1./Emax_proj)/primEnergy; G4double t2=2.*std::log(diff2*Emin_proj/Emax_proj/diff1)/primEnergy/primEnergy; Cross*=(t1+t2); } lastCS =Cross; return Cross; } ////////////////////////////////////////////////////////////////////////////// // G4double G4AdjointhIonisationModel::GetSecondAdjEnergyMaxForScatProjToProjCase(G4double PrimAdjEnergy) { G4double Tmax=PrimAdjEnergy*one_plus_ratio_2/(one_minus_ratio_2-2.*ratio*PrimAdjEnergy/mass); return Tmax; } ////////////////////////////////////////////////////////////////////////////// // G4double G4AdjointhIonisationModel::GetSecondAdjEnergyMinForScatProjToProjCase(G4double PrimAdjEnergy,G4double Tcut) { return PrimAdjEnergy+Tcut; } ////////////////////////////////////////////////////////////////////////////// // G4double G4AdjointhIonisationModel::GetSecondAdjEnergyMaxForProdToProjCase(G4double ) { return HighEnergyLimit; } ////////////////////////////////////////////////////////////////////////////// // G4double G4AdjointhIonisationModel::GetSecondAdjEnergyMinForProdToProjCase(G4double PrimAdjEnergy) { G4double Tmin= (2*PrimAdjEnergy-4*mass + std::sqrt(4.*PrimAdjEnergy*PrimAdjEnergy +16.*mass*mass + 8.*PrimAdjEnergy*mass*(1/ratio +ratio)))/4.; return Tmin; }