// // ******************************************************************** // * DISCLAIMER * // * * // * The following disclaimer summarizes all the specific disclaimers * // * of contributors to this software. The specific disclaimers,which * // * govern, are listed with their locations in: * // * http://cern.ch/geant4/license * // * * // * 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. * // * * // * This code implementation is the intellectual property of the * // * GEANT4 collaboration. * // * By copying, distributing or modifying the Program (or any work * // * based on the Program) you indicate your acceptance of this * // * statement, and all its terms. * // ******************************************************************** // // // // Hadronic Process: Inelastic Interaction // original by H.P. Wellisch // modified by J.L. Chuma, TRIUMF, 22-Nov-1996 // Last modified: 27-Mar-1997 // J.P. Wellisch: 23-Apr-97: G4Exception removed // J.P. Wellisch: 24-Apr-97: correction for SetUpPions // Modified by J.L. Chuma, 30-Apr-97: added originalTarget to CalculateMomenta // since TwoBody needed to reset the target particle // J.L. Chuma, 20-Jun-97: Modified CalculateMomenta to correct the decision process // for whether to use GenerateXandPt or TwoCluster // J.L. Chuma, 06-Aug-97: added original incident particle, before Fermi motion and // evaporation effects are included, needed for calculating // self absorption and corrections for single particle spectra // HPW removed misunderstanding of LocalEnergyDeposit, 11.04.98. #include "G4InelasticInteraction.hh" #include "Randomize.hh" G4double G4InelasticInteraction::Pmltpc( // used in Cascade functions G4int np, G4int nm, G4int nz, G4int n, G4double b, G4double c ) { const G4double expxu = 82.; // upper bound for arg. of exp const G4double expxl = -expxu; // lower bound for arg. of exp G4double npf = 0.0; G4double nmf = 0.0; G4double nzf = 0.0; G4int i; for( i=2; i<=np; i++ )npf += log((double)i); for( i=2; i<=nm; i++ )nmf += log((double)i); for( i=2; i<=nz; i++ )nzf += log((double)i); G4double r; r = G4std::min( expxu, G4std::max( expxl, -(np-nm+nz+b)*(np-nm+nz+b)/(2*c*c*n*n)-npf-nmf-nzf ) ); return exp(r); } G4bool G4InelasticInteraction::MarkLeadingStrangeParticle( const G4ReactionProduct ¤tParticle, const G4ReactionProduct &targetParticle, G4ReactionProduct &leadParticle ) { // the following was in GenerateXandPt and TwoCluster // add a parameter to the GenerateXandPt function telling it about the strange particle // // assumes that the original particle was a strange particle // G4bool lead = false; if( (currentParticle.GetMass() >= G4KaonPlus::KaonPlus()->GetPDGMass()) && (currentParticle.GetDefinition() != G4Proton::Proton()) && (currentParticle.GetDefinition() != G4Neutron::Neutron()) ) { lead = true; leadParticle = currentParticle; // set lead to the incident particle } else if( (targetParticle.GetMass() >= G4KaonPlus::KaonPlus()->GetPDGMass()) && (targetParticle.GetDefinition() != G4Proton::Proton()) && (targetParticle.GetDefinition() != G4Neutron::Neutron()) ) { lead = true; leadParticle = targetParticle; // set lead to the target particle } return lead; } void G4InelasticInteraction::SetUpPions( const G4int np, const G4int nm, const G4int nz, G4FastVector &vec, G4int &vecLen ) { if( np+nm+nz == 0 )return; G4int i; G4ReactionProduct *p; for( i=0; iSetDefinition( G4PionPlus::PionPlus() ); (G4UniformRand() < 0.5) ? p->SetSide( -1 ) : p->SetSide( 1 ); vec.SetElement( vecLen++, p ); } for( i=np; iSetDefinition( G4PionMinus::PionMinus() ); (G4UniformRand() < 0.5) ? p->SetSide( -1 ) : p->SetSide( 1 ); vec.SetElement( vecLen++, p ); } for( i=np+nm; iSetDefinition( G4PionZero::PionZero() ); (G4UniformRand() < 0.5) ? p->SetSide( -1 ) : p->SetSide( 1 ); vec.SetElement( vecLen++, p ); } } void G4InelasticInteraction::GetNormalizationConstant( const G4double energy, // MeV, <0 means annihilation channels G4double &n, G4double &anpn ) { const G4double expxu = 82.; // upper bound for arg. of exp const G4double expxl = -expxu; // lower bound for arg. of exp const G4int numSec = 60; // // the only difference between the calculation for annihilation channels // and normal is the starting value, iBegin, for the loop below // G4int iBegin = 1; G4double en = energy; if( energy < 0.0 ) { iBegin = 2; en *= -1.0; } // // number of total particles vs. centre of mass Energy - 2*proton mass // G4double aleab = log(en/GeV); n = 3.62567 + aleab*(0.665843 + aleab*(0.336514 + aleab*(0.117712 + 0.0136912*aleab))); n -= 2.0; // // normalization constant for kno-distribution // anpn = 0.0; G4double test, temp; for( G4int i=iBegin; i<=numSec; ++i ) { temp = pi*i/(2.0*n*n); test = exp( G4std::min( expxu, G4std::max( expxl, -(pi/4.0)*(i*i)/(n*n) ) ) ); if( temp < 1.0 ) { if( test >= 1.0e-10 )anpn += temp*test; } else anpn += temp*test; } } void G4InelasticInteraction::CalculateMomenta( G4FastVector &vec, G4int &vecLen, const G4DynamicParticle *originalIncident, // the original incident particle const G4DynamicParticle *originalTarget, G4ReactionProduct &modifiedOriginal, // Fermi motion and evap. effects included G4Nucleus &targetNucleus, G4ReactionProduct ¤tParticle, G4ReactionProduct &targetParticle, G4bool &incidentHasChanged, G4bool &targetHasChanged, G4bool quasiElastic ) { what = originalIncident->GetMomentum(); theReactionDynamics.ProduceStrangeParticlePairs( vec, vecLen, modifiedOriginal, originalTarget, currentParticle, targetParticle, incidentHasChanged, targetHasChanged ); if( quasiElastic ) { theReactionDynamics.TwoBody( vec, vecLen, modifiedOriginal, originalTarget, currentParticle, targetParticle, targetNucleus, targetHasChanged ); return; } G4ReactionProduct leadingStrangeParticle; G4bool leadFlag = MarkLeadingStrangeParticle( currentParticle, targetParticle, leadingStrangeParticle ); // // Note: the number of secondaries can be reduced in GenerateXandPt and TwoCluster // G4bool finishedGenXPt = false; G4bool annihilation = false; if( originalIncident->GetDefinition()->GetPDGEncoding() < 0 && currentParticle.GetMass() == 0.0 && targetParticle.GetMass() == 0.0 ) { // original was an anti-particle and annihilation has taken place annihilation = true; G4double ekcor = 1.0; G4double ek = originalIncident->GetKineticEnergy(); G4double ekOrg = ek; const G4double tarmas = originalTarget->GetDefinition()->GetPDGMass(); if( ek > 1.0*GeV )ekcor = 1./(ek/GeV); const G4double atomicWeight = targetNucleus.GetN(); ek = 2*tarmas + ek*(1.+ekcor/atomicWeight); G4double tkin = targetNucleus.Cinema( ek ); ek += tkin; ekOrg += tkin; modifiedOriginal.SetKineticEnergy( ekOrg ); // // evaporation -- re-calculate black track energies // this was Done already just before the cascade // tkin = targetNucleus.EvaporationEffects( ek ); ekOrg -= tkin; ekOrg = G4std::max( 0.0001*GeV, ekOrg ); modifiedOriginal.SetKineticEnergy( ekOrg ); G4double amas = originalIncident->GetDefinition()->GetPDGMass(); G4double et = ekOrg + amas; G4double p = sqrt( abs(et*et-amas*amas) ); G4double pp = modifiedOriginal.GetMomentum().mag(); if( pp > 0.0 ) { G4ThreeVector momentum = modifiedOriginal.GetMomentum(); modifiedOriginal.SetMomentum( momentum * (p/pp) ); } if( ekOrg <= 0.0001 ) { modifiedOriginal.SetKineticEnergy( 0.0 ); modifiedOriginal.SetMomentum( 0.0, 0.0, 0.0 ); } } const G4double twsup[] = { 1.0, 0.7, 0.5, 0.3, 0.2, 0.1 }; G4double rand1 = G4UniformRand(); G4double rand2 = G4UniformRand(); if( annihilation || (vecLen >= 6) || (modifiedOriginal.GetKineticEnergy()/GeV >= 1.0) && (((originalIncident->GetDefinition() == G4KaonPlus::KaonPlus() || originalIncident->GetDefinition() == G4KaonMinus::KaonMinus() || originalIncident->GetDefinition() == G4KaonZeroLong::KaonZeroLong() || originalIncident->GetDefinition() == G4KaonZeroShort::KaonZeroShort()) && rand1 < 0.5) || rand2 > twsup[vecLen]) ) finishedGenXPt = theReactionDynamics.GenerateXandPt( vec, vecLen, modifiedOriginal, originalIncident, currentParticle, targetParticle, targetNucleus, incidentHasChanged, targetHasChanged, leadFlag, leadingStrangeParticle ); if( finishedGenXPt ) { Rotate(vec, vecLen); return; } G4bool finishedTwoClu = false; if( modifiedOriginal.GetTotalMomentum()/MeV < 1.0 ) { for(G4int i=0; i= 1.5) // && !(incidentHasChanged || targetHasChanged) // && (targetNucleus.GetPNBlackTrackEnergy()/MeV <= pnCutOff) // && (targetNucleus.GetDTABlackTrackEnergy()/MeV <= dtaCutOff) ) //{ // the atomic weight of the target nucleus is >= 1.5 AND // neither the incident nor the target particles have changed AND // there is no kinetic energy available for either proton/neutron // or for deuteron/triton/alpha black track particles // For diffraction scattering on heavy nuclei use elastic routines instead //G4cerr << "*** Error in G4InelasticInteraction::CalculateMomenta" << G4endl; //G4cerr << "*** the elastic scattering would be better here ***" < &vec, G4int &vecLen) { G4double rotation = 2.*pi*G4UniformRand(); cache = rotation; G4int i; for( i=0; iGetMomentum(); momentum = momentum.rotate(rotation, what); vec[i]->SetMomentum(momentum); } } void G4InelasticInteraction::SetUpChange( G4FastVector &vec, G4int &vecLen, G4ReactionProduct ¤tParticle, G4ReactionProduct &targetParticle, G4bool &incidentHasChanged ) { G4ParticleDefinition *aKaonZL = G4KaonZeroLong::KaonZeroLong(); G4ParticleDefinition *aKaonZS = G4KaonZeroShort::KaonZeroShort(); G4int i; if( currentParticle.GetDefinition() == aKaonZL ) { if( G4UniformRand() <= 0.5 ) { currentParticle.SetDefinition( aKaonZS ); incidentHasChanged = true; } } else if( currentParticle.GetDefinition() == aKaonZS ) { if( G4UniformRand() > 0.5 ) { currentParticle.SetDefinition( aKaonZL ); incidentHasChanged = true; } } if( targetParticle.GetDefinition() == aKaonZL ) { if( G4UniformRand() <= 0.5 )targetParticle.SetDefinition( aKaonZS ); } else if( targetParticle.GetDefinition() == aKaonZS ) { if( G4UniformRand() > 0.5 )targetParticle.SetDefinition( aKaonZL ); } for( i=0; iGetDefinition() == aKaonZL ) { if( G4UniformRand() <= 0.5 )vec[i]->SetDefinition( aKaonZS ); } else if( vec[i]->GetDefinition() == aKaonZS ) { if( G4UniformRand() > 0.5 )vec[i]->SetDefinition( aKaonZL ); } } if( incidentHasChanged ) { theParticleChange.SetNumberOfSecondaries( vecLen+2 ); G4DynamicParticle* p0 = new G4DynamicParticle; p0->SetDefinition( currentParticle.GetDefinition() ); p0->SetMomentum( currentParticle.GetMomentum() ); theParticleChange.AddSecondary( p0 ); theParticleChange.SetStatusChange( fStopAndKill ); theParticleChange.SetEnergyChange( 0.0 ); } else { theParticleChange.SetNumberOfSecondaries( vecLen+1 ); G4double p = currentParticle.GetMomentum().mag()/MeV; G4ThreeVector m = currentParticle.GetMomentum(); if( p > DBL_MIN ) theParticleChange.SetMomentumChange( m.x()/p, m.y()/p, m.z()/p ); else theParticleChange.SetMomentumChange( 0.0, 0.0, 0.0 ); theParticleChange.SetEnergyChange( currentParticle.GetKineticEnergy() ); } if( targetParticle.GetMass() > 0.0 ) // targetParticle can be eliminated in TwoBody { G4DynamicParticle *p1 = new G4DynamicParticle; p1->SetDefinition( targetParticle.GetDefinition() ); G4ThreeVector momentum = targetParticle.GetMomentum(); momentum = momentum.rotate(cache, what); p1->SetMomentum( momentum ); theParticleChange.AddSecondary( p1 ); } G4DynamicParticle *p; for( i=0; iSetDefinition( vec[i]->GetDefinition() ); p->SetMomentum( vec[i]->GetMomentum() ); theParticleChange.AddSecondary( p ); delete vec[i]; } } /* end of file */