// // ******************************************************************** // * 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: G4AdjointeIonisationModel.cc,v 1.2 2009/11/20 10:31:20 ldesorgh Exp $ // GEANT4 tag $Name: geant4-09-03-cand-01 $ // #include "G4AdjointeIonisationModel.hh" #include "G4AdjointCSManager.hh" #include "G4Integrator.hh" #include "G4TrackStatus.hh" #include "G4ParticleChange.hh" #include "G4AdjointElectron.hh" #include "G4Gamma.hh" #include "G4AdjointGamma.hh" //////////////////////////////////////////////////////////////////////////////// // G4AdjointeIonisationModel::G4AdjointeIonisationModel(): G4VEmAdjointModel("Inv_eIon_model") { UseMatrix =true; UseMatrixPerElement = true; ApplyCutInRange = true; UseOnlyOneMatrixForAllElements = true; CS_biasing_factor =1.; WithRapidSampling = false; theAdjEquivOfDirectPrimPartDef =G4AdjointElectron::AdjointElectron(); theAdjEquivOfDirectSecondPartDef=G4AdjointElectron::AdjointElectron(); theDirectPrimaryPartDef=G4Electron::Electron(); second_part_of_same_type=true; } //////////////////////////////////////////////////////////////////////////////// // G4AdjointeIonisationModel::~G4AdjointeIonisationModel() {;} //////////////////////////////////////////////////////////////////////////////// // void G4AdjointeIonisationModel::SampleSecondaries(const G4Track& aTrack, G4bool IsScatProjToProjCase, G4ParticleChange* 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; if (!WithRapidSampling ) { //used by default projectileKinEnergy = SampleAdjSecEnergyFromCSMatrix(adjointPrimKinEnergy, IsScatProjToProjCase); CorrectPostStepWeight(fParticleChange, aTrack.GetWeight(), adjointPrimKinEnergy, projectileKinEnergy, IsScatProjToProjCase); //Caution !!!this weight correction should be always applied } else { //only for test at the moment G4double Emin,Emax; if (IsScatProjToProjCase) { Emin=GetSecondAdjEnergyMinForScatProjToProjCase(adjointPrimKinEnergy,currentTcutForDirectSecond); Emax=GetSecondAdjEnergyMaxForScatProjToProjCase(adjointPrimKinEnergy); } else { Emin=GetSecondAdjEnergyMinForProdToProjCase(adjointPrimKinEnergy); Emax=GetSecondAdjEnergyMaxForProdToProjCase(adjointPrimKinEnergy); } projectileKinEnergy = Emin*std::pow(Emax/Emin,G4UniformRand()); lastCS=lastAdjointCSForScatProjToProjCase; if ( !IsScatProjToProjCase) lastCS=lastAdjointCSForProdToProjCase; G4double new_weight=aTrack.GetWeight(); G4double used_diffCS=lastCS*std::log(Emax/Emin)/projectileKinEnergy; G4double needed_diffCS=adjointPrimKinEnergy/projectileKinEnergy; if (!IsScatProjToProjCase) needed_diffCS *=DiffCrossSectionPerVolumePrimToSecond(currentMaterial,projectileKinEnergy,adjointPrimKinEnergy); else needed_diffCS *=DiffCrossSectionPerVolumePrimToScatPrim(currentMaterial,projectileKinEnergy,adjointPrimKinEnergy); new_weight*=needed_diffCS/used_diffCS; fParticleChange->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()); } } //////////////////////////////////////////////////////////////////////////////// // //The implementation here is correct for energy loss process, for the photoelectric and compton scattering the method should be redefine G4double G4AdjointeIonisationModel::DiffCrossSectionPerAtomPrimToSecond( G4double kinEnergyProj, G4double kinEnergyProd, G4double Z, G4double ) { 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 dSigmadEprod=Z*DiffCrossSectionMoller(kinEnergyProj,kinEnergyProd); } return dSigmadEprod; } ////////////////////////////////////////////////////////////////////////////// // G4double G4AdjointeIonisationModel::DiffCrossSectionMoller(G4double kinEnergyProj,G4double kinEnergyProd){ G4double electron_mass_c2=0.51099906*MeV; G4double energy = kinEnergyProj + electron_mass_c2; G4double x = kinEnergyProd/kinEnergyProj; G4double gam = energy/electron_mass_c2; G4double gamma2 = gam*gam; G4double beta2 = 1.0 - 1.0/gamma2; G4double g = (2.0*gam - 1.0)/gamma2; G4double y = 1.0 - x; G4double fac=twopi_mc2_rcl2/electron_mass_c2; G4double dCS = fac*( 1.-g + ((1.0 - g*x)/(x*x)) + ((1.0 - g*y)/(y*y)))/(beta2*(gam-1)); return dCS/kinEnergyProj; }