G4INCLXXInterface Class Reference

INCL++ intra-nuclear cascade. More...

#include <G4INCLXXInterface.hh>

Inheritance diagram for G4INCLXXInterface:

Collaboration diagram for G4INCLXXInterface:

Public Member Functions
	G4INCLXXInterface (G4VPreCompoundModel *const aPreCompound=0)
	~G4INCLXXInterface ()
G4int	operator== (G4INCLXXInterface &right)
G4int	operator!= (G4INCLXXInterface &right)
G4ReactionProductVector *	Propagate (G4KineticTrackVector *theSecondaries, G4V3DNucleus *theNucleus)
G4HadFinalState *	ApplyYourself (const G4HadProjectile &aTrack, G4Nucleus &theNucleus)
void	DeleteModel ()
virtual void	ModelDescription (std::ostream &outFile) const
G4String const &	GetDeExcitationModelName () const
Public Member Functions inherited from G4VIntraNuclearTransportModel
	G4VIntraNuclearTransportModel (const G4String &mName="CascadeModel", G4VPreCompoundModel *ptr=nullptr)
virtual	~G4VIntraNuclearTransportModel ()
virtual G4ReactionProductVector *	PropagateNuclNucl (G4KineticTrackVector *theSecondaries, G4V3DNucleus *theNucleus, G4V3DNucleus *theProjectileNucleus)
void	SetDeExcitation (G4VPreCompoundModel *ptr)
void	Set3DNucleus (G4V3DNucleus *const value)
void	SetPrimaryProjectile (const G4HadProjectile &aPrimary)
const G4String &	GetModelName () const
virtual void	PropagateModelDescription (std::ostream &outFile) const
Public Member Functions inherited from G4HadronicInteraction
	G4HadronicInteraction (const G4String &modelName="HadronicModel")
virtual	~G4HadronicInteraction ()
virtual G4double	SampleInvariantT (const G4ParticleDefinition *p, G4double plab, G4int Z, G4int A)
virtual G4bool	IsApplicable (const G4HadProjectile &aTrack, G4Nucleus &targetNucleus)
G4double	GetMinEnergy () const
G4double	GetMinEnergy (const G4Material *aMaterial, const G4Element *anElement) const
void	SetMinEnergy (G4double anEnergy)
void	SetMinEnergy (G4double anEnergy, const G4Element *anElement)
void	SetMinEnergy (G4double anEnergy, const G4Material *aMaterial)
G4double	GetMaxEnergy () const
G4double	GetMaxEnergy (const G4Material *aMaterial, const G4Element *anElement) const
void	SetMaxEnergy (const G4double anEnergy)
void	SetMaxEnergy (G4double anEnergy, const G4Element *anElement)
void	SetMaxEnergy (G4double anEnergy, const G4Material *aMaterial)
G4int	GetVerboseLevel () const
void	SetVerboseLevel (G4int value)
const G4String &	GetModelName () const
void	DeActivateFor (const G4Material *aMaterial)
void	ActivateFor (const G4Material *aMaterial)
void	DeActivateFor (const G4Element *anElement)
void	ActivateFor (const G4Element *anElement)
G4bool	IsBlocked (const G4Material *aMaterial) const
G4bool	IsBlocked (const G4Element *anElement) const
void	SetRecoilEnergyThreshold (G4double val)
G4double	GetRecoilEnergyThreshold () const
virtual const std::pair < G4double, G4double >	GetFatalEnergyCheckLevels () const
virtual std::pair< G4double, G4double >	GetEnergyMomentumCheckLevels () const
void	SetEnergyMomentumCheckLevels (G4double relativeLevel, G4double absoluteLevel)
virtual void	BuildPhysicsTable (const G4ParticleDefinition &)
virtual void	InitialiseModel ()

Additional Inherited Members
Protected Member Functions inherited from G4VIntraNuclearTransportModel
G4V3DNucleus *	Get3DNucleus () const
G4VPreCompoundModel *	GetDeExcitation () const
const G4HadProjectile *	GetPrimaryProjectile () const
Protected Member Functions inherited from G4HadronicInteraction
void	SetModelName (const G4String &nam)
G4bool	IsBlocked () const
void	Block ()
Protected Attributes inherited from G4VIntraNuclearTransportModel
G4String	theTransportModelName
G4V3DNucleus *	the3DNucleus
G4VPreCompoundModel *	theDeExcitation
const G4HadProjectile *	thePrimaryProjectile
Protected Attributes inherited from G4HadronicInteraction
G4HadFinalState	theParticleChange
G4int	verboseLevel
G4double	theMinEnergy
G4double	theMaxEnergy
G4bool	isBlocked

Detailed Description

INCL++ intra-nuclear cascade.

Interface for INCL++. This interface handles basic hadron bullet particles (protons, neutrons, pions), as well as light ions.

Example usage in case of protons:

* G4INCLXXInterface* inclModel = new G4INCLXXInterface;
* inclModel -> SetMinEnergy(0.0 * MeV); // Set the energy limits
* inclModel -> SetMaxEnergy(3.0 * GeV);
*
* G4ProtonInelasticProcess* protonInelasticProcess = new G4ProtonInelasticProcess();
* G4ProtonInelasticCrossSection* protonInelasticCrossSection =  new G4ProtonInelasticCrossSection();
*
* protonInelasticProcess -> RegisterMe(inclModel);
* protonInelasticProcess -> AddDataSet(protonInelasticCrossSection);
*
* particle = G4Proton::Proton();
* processManager = particle -> GetProcessManager();
* processManager -> AddDiscreteProcess(protonInelasticProcess);
* 

The same setup procedure is needed for neutron, pion and generic-ion inelastic processes as well.

Definition at line 103 of file G4INCLXXInterface.hh.

Constructor & Destructor Documentation

G4INCLXXInterface::G4INCLXXInterface

(

G4VPreCompoundModel *const

aPreCompound = 0

)

Definition at line 59 of file G4INCLXXInterface.cc.

                                                                             :
  G4VIntraNuclearTransportModel(G4INCLXXInterfaceStore::GetInstance()->getINCLXXVersionName()),
  theINCLModel(NULL),
  thePreCompoundModel(aPreCompound),
  theInterfaceStore(G4INCLXXInterfaceStore::GetInstance()),
  theTally(NULL),
  complainedAboutBackupModel(false),
  complainedAboutPreCompound(false),
  theIonTable(G4IonTable::GetIonTable()),
  theINCLXXLevelDensity(NULL),
  theINCLXXFissionProbability(NULL)
{
  if(!thePreCompoundModel) {
    G4HadronicInteraction* p =
      G4HadronicInteractionRegistry::Instance()->FindModel("PRECO");
    thePreCompoundModel = static_cast<G4VPreCompoundModel*>(p);
    if(!thePreCompoundModel) { thePreCompoundModel = new G4PreCompoundModel; }
  }

  // Use the environment variable G4INCLXX_NO_DE_EXCITATION to disable de-excitation
  if(getenv("G4INCLXX_NO_DE_EXCITATION")) {
    G4String message = "de-excitation is completely disabled!";
    theInterfaceStore->EmitWarning(message);
    theDeExcitation = 0;
  } else {
    G4HadronicInteraction* p =
      G4HadronicInteractionRegistry::Instance()->FindModel("PRECO");
    theDeExcitation = static_cast<G4VPreCompoundModel*>(p);
    if(!theDeExcitation) { theDeExcitation = new G4PreCompoundModel; }

    // set the fission parameters for G4ExcitationHandler
    G4VEvaporationChannel * const theFissionChannel =
      theDeExcitation->GetExcitationHandler()->GetEvaporation()->GetFissionChannel();
    G4CompetitiveFission * const theFissionChannelCast = dynamic_cast<G4CompetitiveFission *>(theFissionChannel);
    if(theFissionChannelCast) {
      theINCLXXLevelDensity = new G4FissionLevelDensityParameterINCLXX;
      theFissionChannelCast->SetLevelDensityParameter(theINCLXXLevelDensity);
      theINCLXXFissionProbability = new G4FissionProbability;
      theINCLXXFissionProbability->SetFissionLevelDensityParameter(theINCLXXLevelDensity);
      theFissionChannelCast->SetEmissionStrategy(theINCLXXFissionProbability);
      theInterfaceStore->EmitBigWarning("INCL++/G4ExcitationHandler uses its own level-density parameter for fission");
    } else {
      theInterfaceStore->EmitBigWarning("INCL++/G4ExcitationHandler could not use its own level-density parameter for fission");
    }
  }

  // use the envvar G4INCLXX_DUMP_REMNANT to dump information about the
  // remnants on stdout
  if(getenv("G4INCLXX_DUMP_REMNANT"))
    dumpRemnantInfo = true;
  else
    dumpRemnantInfo = false;

  theBackupModel = new G4BinaryLightIonReaction;
  theBackupModelNucleon = new G4BinaryCascade;
}

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G4INCLXXInterface::~G4INCLXXInterface

(

)

Definition at line 116 of file G4INCLXXInterface.cc.

{
  delete theINCLXXLevelDensity;
  delete theINCLXXFissionProbability;
}

Member Function Documentation

G4HadFinalState * G4INCLXXInterface::ApplyYourself ( const G4HadProjectile &  aTrack, G4Nucleus &  theNucleus  )

virtual

Main method to apply the INCL physics model.

Parameters

aTrack	the projectile particle
theNucleus	target nucleus

Returns

the output of the INCL physics model

Implements G4HadronicInteraction.

Definition at line 167 of file G4INCLXXInterface.cc.

{
  G4ParticleDefinition const * const trackDefinition = aTrack.GetDefinition();
  const G4bool isIonTrack = trackDefinition->GetParticleType()==G4GenericIon::GenericIon()->GetParticleType();
  const G4int trackA = trackDefinition->GetAtomicMass();
  const G4int trackZ = (G4int) trackDefinition->GetPDGCharge();
  const G4int nucleusA = theNucleus.GetA_asInt();
  const G4int nucleusZ = theNucleus.GetZ_asInt();

  // For reactions induced by weird projectiles (e.g. He2), bail out
  if((isIonTrack && (trackZ<=0 || trackA<=trackZ)) || (nucleusA>1 && (nucleusZ<=0 || nucleusA<=nucleusZ))) {
    theResult.Clear();
    theResult.SetStatusChange(isAlive);
    theResult.SetEnergyChange(aTrack.GetKineticEnergy());
    theResult.SetMomentumChange(aTrack.Get4Momentum().vect().unit());
    return &theResult;
  }

  // For reactions on nucleons, use the backup model (without complaining)
  if(trackA<=1 && nucleusA<=1) {
    return theBackupModelNucleon->ApplyYourself(aTrack, theNucleus);
  }

  // For systems heavier than theMaxProjMassINCL, use another model (typically
  // BIC)
  const G4int theMaxProjMassINCL = theInterfaceStore->GetMaxProjMassINCL();
  if(trackA > theMaxProjMassINCL && nucleusA > theMaxProjMassINCL) {
    if(!complainedAboutBackupModel) {
      complainedAboutBackupModel = true;
      std::stringstream ss;
      ss << "INCL++ refuses to handle reactions between nuclei with A>"
        << theMaxProjMassINCL
        << ". A backup model ("
        << theBackupModel->GetModelName()
        << ") will be used instead.";
      theInterfaceStore->EmitBigWarning(ss.str());
    }
    return theBackupModel->ApplyYourself(aTrack, theNucleus);
  }

  // For energies lower than cascadeMinEnergyPerNucleon, use PreCompound
  const G4double cascadeMinEnergyPerNucleon = theInterfaceStore->GetCascadeMinEnergyPerNucleon();
  const G4double trackKinE = aTrack.GetKineticEnergy();
  if((trackDefinition==G4Neutron::NeutronDefinition() || trackDefinition==G4Proton::ProtonDefinition())
      && trackKinE < cascadeMinEnergyPerNucleon) {
    if(!complainedAboutPreCompound) {
      complainedAboutPreCompound = true;
      std::stringstream ss;
      ss << "INCL++ refuses to handle nucleon-induced reactions below "
        << cascadeMinEnergyPerNucleon / MeV
        << " MeV. A PreCoumpound model ("
        << thePreCompoundModel->GetModelName()
        << ") will be used instead.";
      theInterfaceStore->EmitBigWarning(ss.str());
    }
    return thePreCompoundModel->ApplyYourself(aTrack, theNucleus);
  }

  // Calculate the total four-momentum in the entrance channel
  const G4double theNucleusMass = theIonTable->GetIonMass(nucleusZ, nucleusA);
  const G4double theTrackMass = trackDefinition->GetPDGMass();
  const G4double theTrackEnergy = trackKinE + theTrackMass;
  const G4double theTrackMomentumAbs2 = theTrackEnergy*theTrackEnergy - theTrackMass*theTrackMass;
  const G4double theTrackMomentumAbs = ((theTrackMomentumAbs2>0.0) ? std::sqrt(theTrackMomentumAbs2) : 0.0);
  const G4ThreeVector theTrackMomentum = aTrack.Get4Momentum().getV().unit() * theTrackMomentumAbs;

  G4LorentzVector goodTrack4Momentum(theTrackMomentum, theTrackEnergy);
  G4LorentzVector fourMomentumIn;
  fourMomentumIn.setE(theTrackEnergy + theNucleusMass);
  fourMomentumIn.setVect(theTrackMomentum);

  // Check if inverse kinematics should be used
  const G4bool inverseKinematics = AccurateProjectile(aTrack, theNucleus);

  // If we are running in inverse kinematics, redefine aTrack and theNucleus
  G4LorentzRotation *toInverseKinematics = NULL;
  G4LorentzRotation *toDirectKinematics = NULL;
  G4HadProjectile const *aProjectileTrack = &aTrack;
  G4Nucleus *theTargetNucleus = &theNucleus;
  if(inverseKinematics) {
    G4ParticleDefinition *oldTargetDef = theIonTable->GetIon(nucleusZ, nucleusA, 0);
    const G4ParticleDefinition *oldProjectileDef = trackDefinition;

    if(oldProjectileDef != 0 && oldTargetDef != 0) {
      const G4int newTargetA = oldProjectileDef->GetAtomicMass();
      const G4int newTargetZ = oldProjectileDef->GetAtomicNumber();

      if(newTargetA > 0 && newTargetZ > 0) {
        // This should give us the same energy per nucleon
        theTargetNucleus = new G4Nucleus(newTargetA, newTargetZ);
        toInverseKinematics = new G4LorentzRotation(goodTrack4Momentum.boostVector());
        G4LorentzVector theProjectile4Momentum(0.0, 0.0, 0.0, theNucleusMass);
        G4DynamicParticle swappedProjectileParticle(oldTargetDef, (*toInverseKinematics) * theProjectile4Momentum);
        aProjectileTrack = new G4HadProjectile(swappedProjectileParticle);
      } else {
        G4String message = "badly defined target after swapping. Falling back to normal (non-swapped) mode.";
        theInterfaceStore->EmitWarning(message);
        toInverseKinematics = new G4LorentzRotation;
      }
    } else {
      G4String message = "oldProjectileDef or oldTargetDef was null";
      theInterfaceStore->EmitWarning(message);
      toInverseKinematics = new G4LorentzRotation;
    }
  }

  // INCL assumes the projectile particle is going in the direction of
  // the Z-axis. Here we construct proper rotation to convert the
  // momentum vectors of the outcoming particles to the original
  // coordinate system.
  G4LorentzVector projectileMomentum = aProjectileTrack->Get4Momentum();

  // INCL++ assumes that the projectile is going in the direction of
  // the z-axis. In principle, if the coordinate system used by G4
  // hadronic framework is defined differently we need a rotation to
  // transform the INCL++ reaction products to the appropriate
  // frame. Please note that it isn't necessary to apply this
  // transform to the projectile because when creating the INCL++
  // projectile particle; \see{toINCLKineticEnergy} needs to use only the
  // projectile energy (direction is simply assumed to be along z-axis).
  G4RotationMatrix toZ;
  toZ.rotateZ(-projectileMomentum.phi());
  toZ.rotateY(-projectileMomentum.theta());
  G4RotationMatrix toLabFrame3 = toZ.inverse();
  G4LorentzRotation toLabFrame(toLabFrame3);
  // However, it turns out that the projectile given to us by G4
  // hadronic framework is already going in the direction of the
  // z-axis so this rotation is actually unnecessary. Both toZ and
  // toLabFrame turn out to be unit matrices as can be seen by
  // uncommenting the folowing two lines:
  // G4cout <<"toZ = " << toZ << G4endl;
  // G4cout <<"toLabFrame = " << toLabFrame << G4endl;

  theResult.Clear(); // Make sure the output data structure is clean.
  theResult.SetStatusChange(stopAndKill);

  std::list<G4Fragment> remnants;

  const G4int maxTries = 200;
  G4int nTries = 0;
  // INCL can generate transparent events. However, this is meaningful
  // only in the standalone code. In Geant4 we must "force" INCL to
  // produce a valid cascade.
  G4bool eventIsOK = false;
  do {
    const G4INCL::ParticleSpecies theSpecies = toINCLParticleSpecies(*aProjectileTrack);
    const G4double kineticEnergy = toINCLKineticEnergy(*aProjectileTrack);

    // The INCL model will be created at the first use
    theINCLModel = G4INCLXXInterfaceStore::GetInstance()->GetINCLModel();

    const G4INCL::EventInfo eventInfo = theINCLModel->processEvent(theSpecies, kineticEnergy, theTargetNucleus->GetA_asInt(), theTargetNucleus->GetZ_asInt());
    //    eventIsOK = !eventInfo.transparent && nTries < maxTries;
    eventIsOK = !eventInfo.transparent;
    if(eventIsOK) {

      // If the collision was run in inverse kinematics, prepare to boost back
      // all the reaction products
      if(inverseKinematics) {
        toDirectKinematics = new G4LorentzRotation(toInverseKinematics->inverse());
      }

      G4LorentzVector fourMomentumOut;

      for(G4int i = 0; i < eventInfo.nParticles; ++i) {
    G4int A = eventInfo.A[i];
 G4int Z = eventInfo.Z[i];
 G4int PDGCode = eventInfo.PDGCode[i];
    //  G4cout <<"INCL particle A = " << A << " Z = " << Z << G4endl;
    G4double kinE = eventInfo.EKin[i];
    G4double px = eventInfo.px[i];
    G4double py = eventInfo.py[i];
    G4double pz = eventInfo.pz[i];
    G4DynamicParticle *p = toG4Particle(A, Z, PDGCode, kinE, px, py, pz);
    if(p != 0) {
      G4LorentzVector momentum = p->Get4Momentum();

          // Apply the toLabFrame rotation
          momentum *= toLabFrame;
          // Apply the inverse-kinematics boost
          if(inverseKinematics) {
            momentum *= *toDirectKinematics;
            momentum.setVect(-momentum.vect());
          }

      // Set the four-momentum of the reaction products
      p->Set4Momentum(momentum);
          fourMomentumOut += momentum;
      theResult.AddSecondary(p);

    } else {
      G4String message = "the model produced a particle that couldn't be converted to Geant4 particle.";
          theInterfaceStore->EmitWarning(message);
    }
      }

      for(G4int i = 0; i < eventInfo.nRemnants; ++i) {
    const G4int A = eventInfo.ARem[i];
    const G4int Z = eventInfo.ZRem[i];
    //  G4cout <<"INCL particle A = " << A << " Z = " << Z << G4endl;
    const G4double kinE = eventInfo.EKinRem[i];
    const G4double px = eventInfo.pxRem[i];
    const G4double py = eventInfo.pyRem[i];
    const G4double pz = eventInfo.pzRem[i];
        G4ThreeVector spin(
            eventInfo.jxRem[i]*hbar_Planck,
            eventInfo.jyRem[i]*hbar_Planck,
            eventInfo.jzRem[i]*hbar_Planck
            );
    const G4double excitationE = eventInfo.EStarRem[i];
    const G4double nuclearMass = G4NucleiProperties::GetNuclearMass(A, Z) + excitationE;
        const G4double scaling = remnant4MomentumScaling(nuclearMass,
            kinE,
            px, py, pz);
    G4LorentzVector fourMomentum(scaling * px, scaling * py, scaling * pz,
                     nuclearMass + kinE);
    if(std::abs(scaling - 1.0) > 0.01) {
          std::stringstream ss;
          ss << "momentum scaling = " << scaling
            << "\n                Lorentz vector = " << fourMomentum
            << ")\n                A = " << A << ", Z = " << Z
            << "\n                E* = " << excitationE << ", nuclearMass = " << nuclearMass
            << "\n                remnant i=" << i << ", nRemnants=" << eventInfo.nRemnants
            << "\n                Reaction was: " << aTrack.GetKineticEnergy()/MeV
            << "-MeV " << trackDefinition->GetParticleName() << " + "
            << theIonTable->GetIonName(theNucleus.GetZ_asInt(), theNucleus.GetA_asInt(), 0)
            << ", in " << (inverseKinematics ? "inverse" : "direct") << " kinematics.";
          theInterfaceStore->EmitWarning(ss.str());
    }

        // Apply the toLabFrame rotation
        fourMomentum *= toLabFrame;
        spin *= toLabFrame3;
        // Apply the inverse-kinematics boost
        if(inverseKinematics) {
          fourMomentum *= *toDirectKinematics;
          fourMomentum.setVect(-fourMomentum.vect());
        }

        fourMomentumOut += fourMomentum;
    G4Fragment remnant(A, Z, fourMomentum);
        remnant.SetAngularMomentum(spin);
        if(dumpRemnantInfo) {
          G4cerr << "G4INCLXX_DUMP_REMNANT: " << remnant << "  spin: " << spin << G4endl;
        }
    remnants.push_back(remnant);
      }

      // Check four-momentum conservation
      const G4LorentzVector violation4Momentum = fourMomentumOut - fourMomentumIn;
      const G4double energyViolation = std::abs(violation4Momentum.e());
      const G4double momentumViolation = violation4Momentum.rho();
      if(energyViolation > G4INCLXXInterfaceStore::GetInstance()->GetConservationTolerance()) {
        std::stringstream ss;
        ss << "energy conservation violated by " << energyViolation/MeV << " MeV in "
          << aTrack.GetKineticEnergy()/MeV << "-MeV " << trackDefinition->GetParticleName()
          << " + " << theIonTable->GetIonName(theNucleus.GetZ_asInt(), theNucleus.GetA_asInt(), 0)
          << " inelastic reaction, in " << (inverseKinematics ? "inverse" : "direct") << " kinematics. Will resample.";
        theInterfaceStore->EmitWarning(ss.str());
        eventIsOK = false;
        const G4int nSecondaries = theResult.GetNumberOfSecondaries();
        for(G4int j=0; j<nSecondaries; ++j)
          delete theResult.GetSecondary(j)->GetParticle();
        theResult.Clear();
        theResult.SetStatusChange(stopAndKill);
        remnants.clear();
      } else if(momentumViolation > G4INCLXXInterfaceStore::GetInstance()->GetConservationTolerance()) {
        std::stringstream ss;
        ss << "momentum conservation violated by " << momentumViolation/MeV << " MeV in "
          << aTrack.GetKineticEnergy()/MeV << "-MeV " << trackDefinition->GetParticleName()
          << " + " << theIonTable->GetIonName(theNucleus.GetZ_asInt(), theNucleus.GetA_asInt(), 0)
          << " inelastic reaction, in " << (inverseKinematics ? "inverse" : "direct") << " kinematics. Will resample.";
        theInterfaceStore->EmitWarning(ss.str());
        eventIsOK = false;
        const G4int nSecondaries = theResult.GetNumberOfSecondaries();
        for(G4int j=0; j<nSecondaries; ++j)
          delete theResult.GetSecondary(j)->GetParticle();
        theResult.Clear();
        theResult.SetStatusChange(stopAndKill);
        remnants.clear();
      }
    }
    nTries++;
  } while(!eventIsOK && nTries < maxTries); /* Loop checking, 10.07.2015, D.Mancusi */

  // Clean up the objects that we created for the inverse kinematics
  if(inverseKinematics) {
    delete aProjectileTrack;
    delete theTargetNucleus;
    delete toInverseKinematics;
    delete toDirectKinematics;
  }

  if(!eventIsOK) {
    std::stringstream ss;
    ss << "maximum number of tries exceeded for the proposed "
    << aTrack.GetKineticEnergy()/MeV << "-MeV " << trackDefinition->GetParticleName()
    << " + " << theIonTable->GetIonName(nucleusZ, nucleusA, 0)
    << " inelastic reaction, in " << (inverseKinematics ? "inverse" : "direct") << " kinematics.";
    theInterfaceStore->EmitWarning(ss.str());
    theResult.SetStatusChange(isAlive);
    theResult.SetEnergyChange(aTrack.GetKineticEnergy());
    theResult.SetMomentumChange(aTrack.Get4Momentum().vect().unit());
    return &theResult;
  }

  // De-excitation:

  if(theDeExcitation != 0) {
    for(std::list<G4Fragment>::iterator i = remnants.begin();
    i != remnants.end(); ++i) {
      G4ReactionProductVector *deExcitationResult = theDeExcitation->DeExcite((*i));

      for(G4ReactionProductVector::iterator fragment = deExcitationResult->begin();
      fragment != deExcitationResult->end(); ++fragment) {
    const G4ParticleDefinition *def = (*fragment)->GetDefinition();
    if(def != 0) {
      G4DynamicParticle *theFragment = new G4DynamicParticle(def, (*fragment)->GetMomentum());
      theResult.AddSecondary(theFragment);
    }
      }

      for(G4ReactionProductVector::iterator fragment = deExcitationResult->begin();
      fragment != deExcitationResult->end(); ++fragment) {
    delete (*fragment);
      }
      deExcitationResult->clear();
      delete deExcitationResult;
    }
  }

  remnants.clear();

  if((theTally = theInterfaceStore->GetTally()))
    theTally->Tally(aTrack, theNucleus, theResult);

  return &theResult;
}

void G4INCLXXInterface::DeleteModel ( )

inline

Definition at line 128 of file G4INCLXXInterface.hh.

                     {
    delete theINCLModel;
    theINCLModel = NULL;
  }

G4String const & G4INCLXXInterface::GetDeExcitationModelName

(

)

const

Definition at line 606 of file G4INCLXXInterface.cc.

                                                                  {
  return theDeExcitation->GetModelName();
}

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void G4INCLXXInterface::ModelDescription ( std::ostream &  outFile ) const

virtual

Reimplemented from G4VIntraNuclearTransportModel.

Definition at line 591 of file G4INCLXXInterface.cc.

                                                                  {
   outFile
     << "The Liège Intranuclear Cascade (INCL++) is a model for reactions induced\n"
     << "by nucleons, pions and light ion on any nucleus. The reaction is\n"
     << "described as an avalanche of binary nucleon-nucleon collisions, which can\n"
     << "lead to the emission of energetic particles and to the formation of an\n"
     << "excited thermalised nucleus (remnant). The de-excitation of the remnant is\n"
     << "outside the scope of INCL++ and is typically described by another model.\n\n"
     << "INCL++ has been reasonably well tested for nucleon (~50 MeV to ~15 GeV),\n"
     << "pion (idem) and light-ion projectiles (up to A=18, ~10A MeV to 1A GeV).\n"
     << "Most tests involved target nuclei close to the stability valley, with\n"
     << "numbers between 4 and 250.\n\n"
     << "Reference: D. Mancusi et al., Phys. Rev. C90 (2014) 054602\n\n";
}

G4int G4INCLXXInterface::operator!= ( G4INCLXXInterface &  right )

inline

Definition at line 112 of file G4INCLXXInterface.hh.

                                             {
    return (this != &right);
  }

G4int G4INCLXXInterface::operator== ( G4INCLXXInterface &  right )

inline

Definition at line 108 of file G4INCLXXInterface.hh.

                                             {
    return (this == &right);
  }

G4ReactionProductVector * G4INCLXXInterface::Propagate ( G4KineticTrackVector *  theSecondaries, G4V3DNucleus *  theNucleus  )

virtual

Implements G4VIntraNuclearTransportModel.

Definition at line 506 of file G4INCLXXInterface.cc.

                                                                                            {
  return 0;
}

---

The documentation for this class was generated from the following files:

• source/geant4.10.03.p02/source/processes/hadronic/models/inclxx/interface/include/G4INCLXXInterface.hh
• source/geant4.10.03.p02/source/processes/hadronic/models/inclxx/interface/src/G4INCLXXInterface.cc