G4TheoFSGenerator.cc

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//
// G4TheoFSGenerator
//
// 20110307  M. Kelsey -- Add call to new theTransport->SetPrimaryProjectile()
//      to provide access to full initial state (for Bertini)
// 20110805  M. Kelsey -- Follow change to G4V3DNucleus::GetNucleons()
 
#include "G4DynamicParticle.hh"
#include "G4TheoFSGenerator.hh"
#include "G4ReactionProductVector.hh"
#include "G4ReactionProduct.hh"
#include "G4IonTable.hh"
#include "G4HadronicParameters.hh"
#include "G4CRCoalescence.hh"
#include "G4HadronicInteractionRegistry.hh"
 
G4TheoFSGenerator::G4TheoFSGenerator(const G4String& name)
    : G4HadronicInteraction(name)
    , theTransport(nullptr), theHighEnergyGenerator(nullptr)
    , theQuasielastic(nullptr)
    , theCosmicCoalescence(nullptr)
{
  theParticleChange = new G4HadFinalState;
}
 
G4TheoFSGenerator::~G4TheoFSGenerator()
{
  delete theParticleChange;
}
 
void G4TheoFSGenerator::ModelDescription(std::ostream& outFile) const
{
  outFile << GetModelName() <<" consists of a " << theHighEnergyGenerator->GetModelName()
      << " string model and a stage to de-excite the excited nuclear fragment.\n<p>"
      << "The string model simulates the interaction of\n"
          << "an incident hadron with a nucleus, forming \n"
          << "excited strings, decays these strings into hadrons,\n"
          << "and leaves an excited nucleus. \n"
          << "<p>The string model:\n";
  theHighEnergyGenerator->ModelDescription(outFile);
  outFile <<"\n<p>";
  theTransport->PropagateModelDescription(outFile);
}
 
G4HadFinalState * G4TheoFSGenerator::ApplyYourself(const G4HadProjectile & thePrimary, G4Nucleus &theNucleus)
{
  // init particle change
  theParticleChange->Clear();
  theParticleChange->SetStatusChange(stopAndKill);
  G4double timePrimary=thePrimary.GetGlobalTime();
 
  // Temporarily dummy treatment of heavy (charm and bottom) hadron projectiles at low energies.
  // Cascade models are currently not applicable for heavy hadrons and string models cannot
  // handle them properly at low energies - let's say safely below ~100 MeV.
  // In these cases, we return as final state the initial state unchanged.
  // For most applications, this is a safe simplification, giving that the nearly all
  // slowly moving charm and bottom hadrons decay before any hadronic interaction can occur.
  // Note that we prefer not to use G4HadronicParameters::GetMinEnergyTransitionFTF_Cascade()
  // (typicall ~3 GeV) because FTFP works reasonably well below such a value.
  const G4double energyThresholdForCharmAndBottomHadrons = 100.0*CLHEP::MeV;
  if ( thePrimary.GetKineticEnergy() < energyThresholdForCharmAndBottomHadrons  &&
       ( thePrimary.GetDefinition()->GetQuarkContent( 4 )     != 0  ||    // Has charm       constituent quark
     thePrimary.GetDefinition()->GetAntiQuarkContent( 4 ) != 0  ||    // Has anti-charm  constituent anti-quark
     thePrimary.GetDefinition()->GetQuarkContent( 5 )     != 0  ||    // Has bottom      constituent quark
     thePrimary.GetDefinition()->GetAntiQuarkContent( 5 ) != 0 ) ) {  // Has anti-bottom constituent anti-quark
    theParticleChange->SetStatusChange( isAlive );
    theParticleChange->SetEnergyChange( thePrimary.GetKineticEnergy() );
    theParticleChange->SetMomentumChange( thePrimary.Get4Momentum().vect().unit() );
    return theParticleChange;
  }
      
  // check if models have been registered, and use default, in case this is not true @@
  
  const G4DynamicParticle aPart(thePrimary.GetDefinition(),thePrimary.Get4Momentum().vect());
 
  if ( theQuasielastic ) 
  {
     if ( theQuasielastic->GetFraction(theNucleus, aPart) > G4UniformRand() )
     {
       //G4cout<<"___G4TheoFSGenerator: before Scatter (1) QE=" << theQuasielastic<<G4endl;
       G4KineticTrackVector *result= theQuasielastic->Scatter(theNucleus, aPart);
       //G4cout << "^^G4TheoFSGenerator: after Scatter (1) " << G4endl;
       if (result)
       {
        for(auto & ptr : *result)
        {
          G4DynamicParticle * aNew = 
         new G4DynamicParticle(ptr->GetDefinition(),
                                   ptr->Get4Momentum().e(),
                                   ptr->Get4Momentum().vect());
          theParticleChange->AddSecondary(aNew);
          delete ptr;
        }
        delete result;     
       } 
       else 
       {
        theParticleChange->SetStatusChange(isAlive);
        theParticleChange->SetEnergyChange(thePrimary.GetKineticEnergy());
        theParticleChange->SetMomentumChange(thePrimary.Get4Momentum().vect().unit());
 
       }
       return theParticleChange;
     } 
  }
 
  // get result from high energy model
  G4KineticTrackVector * theInitialResult =
               theHighEnergyGenerator->Scatter(theNucleus, aPart);
 
  //#define DEBUG_initial_result
  #ifdef DEBUG_initial_result
      G4double E_out(0);
      G4IonTable * ionTable=G4ParticleTable::GetParticleTable()->GetIonTable();
      for(auto & ptr : *theInitialResult)
      {
         //G4cout << "TheoFS secondary, mom " << ptr->GetDefinition()->GetParticleName() 
             //         << " " << ptr->Get4Momentum() << G4endl;
         E_out += ptr->Get4Momentum().e();
      }
      G4double init_mass= ionTable->GetIonMass(theNucleus.GetZ_asInt(),theNucleus.GetA_asInt());
          G4double init_E=aPart.Get4Momentum().e();
      // residual nucleus
 
      const std::vector<G4Nucleon> & thy = theHighEnergyGenerator->GetWoundedNucleus()->GetNucleons();
 
      G4int resZ(0),resA(0);
      G4double delta_m(0);
      for(auto & nuc : thy)
      {
         if(nuc.AreYouHit()) {
           ++resA;
           if ( nuc.GetDefinition() == G4Proton::Proton() ) {
             ++resZ;
         delta_m += CLHEP::proton_mass_c2;
           } else {
         delta_m += CLHEP::neutron_mass_c2;
           }  
         }
      }
 
      G4double final_mass(0);
      if ( theNucleus.GetA_asInt() ) {
       final_mass=ionTable->GetIonMass(theNucleus.GetZ_asInt()-resZ,theNucleus.GetA_asInt()- resA);
      }
      G4double E_excit=init_mass + init_E - final_mass - E_out;
      G4cout << " Corrected delta mass " << init_mass - final_mass - delta_m << G4endl;
      G4cout << "initial E, mass = " << init_E << ", " << init_mass << G4endl;
      G4cout << "  final E, mass = " << E_out <<", " << final_mass << "  excitation_E " << E_excit << G4endl;
  #endif
 
  G4ReactionProductVector * theTransportResult = nullptr;
 
  // Uzhi Nov. 2012 for nucleus-nucleus collision
  G4V3DNucleus* theProjectileNucleus = theHighEnergyGenerator->GetProjectileNucleus(); 
  if(theProjectileNucleus == nullptr)
  {
    G4int hitCount = 0;
    const std::vector<G4Nucleon>& they = theHighEnergyGenerator->GetWoundedNucleus()->GetNucleons();
    for(auto & nuc : they)
    {
      if(nuc.AreYouHit()) ++hitCount;
    }
    if(hitCount != theHighEnergyGenerator->GetWoundedNucleus()->GetMassNumber() )
    {
      theTransport->SetPrimaryProjectile(thePrimary);   // For Bertini Cascade
      theTransportResult = 
        theTransport->Propagate(theInitialResult, 
                                theHighEnergyGenerator->GetWoundedNucleus());
      if ( !theTransportResult ) {
        G4cout << "G4TheoFSGenerator: null ptr from transport propagate " << G4endl;
        throw G4HadronicException(__FILE__, __LINE__, "Null ptr from transport propagate");
      }
    }
    else
    {
      theTransportResult = theDecay.Propagate(theInitialResult, 
                                 theHighEnergyGenerator->GetWoundedNucleus());
      if ( theTransportResult == nullptr ) {
         G4cout << "G4TheoFSGenerator: null ptr from decay propagate " << G4endl;
         throw G4HadronicException(__FILE__, __LINE__, "Null ptr from decay propagate");
      }   
    }
  } 
  else 
  { 
    theTransport->SetPrimaryProjectile(thePrimary);
    theTransportResult = theTransport->PropagateNuclNucl(theInitialResult, 
                            theHighEnergyGenerator->GetWoundedNucleus(),
                            theProjectileNucleus);
    if ( !theTransportResult ) {
       G4cout << "G4TheoFSGenerator: null ptr from transport propagate " << G4endl;
       throw G4HadronicException(__FILE__, __LINE__, "Null ptr from transport propagate");
    } 
  }
 
  // If enabled, apply the Cosmic Rays (CR) coalescence to the list of secondaries produced so far.
  // This algorithm can form deuterons and antideuterons by coalescence of, respectively,
  // proton-neutron and antiproton-antineutron pairs close in momentum space.
  // This can be useful in particular for Cosmic Ray applications.
  if ( G4HadronicParameters::Instance()->EnableCRCoalescence() ) {
    if(nullptr == theCosmicCoalescence) {
      theCosmicCoalescence = (G4CRCoalescence*)
        G4HadronicInteractionRegistry::Instance()->FindModel("G4CRCoalescence");
      if(nullptr == theCosmicCoalescence) { 
    theCosmicCoalescence = new G4CRCoalescence();
      }
    }
    theCosmicCoalescence->SetP0Coalescence( thePrimary, theHighEnergyGenerator->GetModelName() );
    theCosmicCoalescence->GenerateDeuterons( theTransportResult );
  }
    
  // Fill particle change
  for(auto & ptr : *theTransportResult)
  {
    G4DynamicParticle * aNewDP =
       new G4DynamicParticle(ptr->GetDefinition(),
                             ptr->GetTotalEnergy(),
                             ptr->GetMomentum());
    G4HadSecondary aNew = G4HadSecondary(aNewDP);
    G4double time = std::max(ptr->GetFormationTime(), 0.0);
    aNew.SetTime(timePrimary + time);
    aNew.SetCreatorModelType(ptr->GetCreatorModel());
    theParticleChange->AddSecondary(aNew);
    delete ptr;
  }
  
  // some garbage collection
  delete theTransportResult;
  
  // Done
  return theParticleChange;
}
 
std::pair<G4double, G4double> G4TheoFSGenerator::GetEnergyMomentumCheckLevels() const
{
  if ( theHighEnergyGenerator ) {
     return theHighEnergyGenerator->GetEnergyMomentumCheckLevels();
  } else {
     return std::pair<G4double, G4double>(DBL_MAX, DBL_MAX);
  }
}