G4HadronicBuilder Class Reference

#include <G4HadronicBuilder.hh>

Static Public Member Functions
static void	BuildElastic (const std::vector< G4int > &particleList)
static void	BuildHyperonsFTFP_BERT ()
static void	BuildHyperonsFTFQGSP_BERT ()
static void	BuildHyperonsQGSP_FTFP_BERT (G4bool quasiElastic)
static void	BuildKaonsFTFP_BERT ()
static void	BuildKaonsFTFQGSP_BERT ()
static void	BuildKaonsQGSP_FTFP_BERT (G4bool quasiElastic)
static void	BuildAntiLightIonsFTFP ()
static void	BuildBCHadronsFTFP_BERT ()
static void	BuildBCHadronsFTFQGSP_BERT ()
static void	BuildBCHadronsQGSP_FTFP_BERT (G4bool quasiElastic)
static void	BuildDecayTableForBCHadrons ()
static void	BuildHyperNucleiFTFP_BERT ()
static void	BuildHyperAntiNucleiFTFP_BERT ()
static void	BuildHyperNucleiFTFP_INCLXX ()
static void	BuildFTFP_INCLXX (const std::vector< G4int > &partList, const G4String &xsName)

Detailed Description

Definition at line 40 of file G4HadronicBuilder.hh.

Member Function Documentation

BuildAntiLightIonsFTFP()

void G4HadronicBuilder::BuildAntiLightIonsFTFP ( )

static

Definition at line 254 of file G4HadronicBuilder.cc.

                                               {
  BuildFTFP_BERT(G4HadParticles::GetLightAntiIons(), false, "AntiAGlauber");
}

Referenced by G4HadronInelasticQBBC::ConstructProcess(), G4HadronPhysicsFTFQGSP_BERT::ConstructProcess(), G4HadronPhysicsFTFP_BERT::Others(), G4HadronPhysicsQGSP_BERT::Others(), G4HadronPhysicsQGSP_BIC::Others(), and G4HadronPhysicsINCLXX::Others().

BuildBCHadronsFTFP_BERT()

void G4HadronicBuilder::BuildBCHadronsFTFP_BERT ( )

static

Definition at line 263 of file G4HadronicBuilder.cc.

                                                {
  if( G4HadronicParameters::Instance()->EnableBCParticles() ) {
    // Bertini is not applicable for charm and bottom hadrons, therefore FTFP is used
    // down to zero kinetic energy (but at very low energies, a dummy model is used
    // that returns the projectile heavy hadron in the final state).
    BuildFTFP_BERT(G4HadParticles::GetBCHadrons(), false, "Glauber-Gribov");
    BuildDecayTableForBCHadrons();
  }
}

Referenced by G4HadronInelasticQBBC::ConstructProcess(), G4HadronPhysicsFTFP_BERT::Others(), and G4HadronPhysicsINCLXX::Others().

BuildBCHadronsFTFQGSP_BERT()

void G4HadronicBuilder::BuildBCHadronsFTFQGSP_BERT ( )

static

Definition at line 273 of file G4HadronicBuilder.cc.

                                                   {
  if( G4HadronicParameters::Instance()->EnableBCParticles() ) {
    // Bertini is not applicable for charm and bottom hadrons, therefore FTFP is used
    // down to zero kinetic energy (but at very low energies, a dummy model is used
    // that returns the projectile heavy hadron in the final state).
    BuildFTFQGSP_BERT(G4HadParticles::GetBCHadrons(), false, "Glauber-Gribov");
    BuildDecayTableForBCHadrons();
  }
}

Referenced by G4HadronPhysicsFTFQGSP_BERT::ConstructProcess().

BuildBCHadronsQGSP_FTFP_BERT()

void G4HadronicBuilder::BuildBCHadronsQGSP_FTFP_BERT ( G4bool  quasiElastic )

static

Definition at line 283 of file G4HadronicBuilder.cc.

                                                                    {
  if( G4HadronicParameters::Instance()->EnableBCParticles() ) {
    // Bertini is not applicable for charm and bottom hadrons, therefore FTFP is used
    // down to zero kinetic energy (but at very low energies, a dummy model is used
    // that returns the projectile heavy hadron in the final state).
    // QGSP is used at high energies in all cases.
    BuildQGSP_FTFP_BERT(G4HadParticles::GetBCHadrons(), false, qElastic, "Glauber-Gribov");
    BuildDecayTableForBCHadrons();
  }
}

Referenced by G4HadronPhysicsQGSP_BERT::Others(), G4HadronPhysicsQGSP_BIC::Others(), and G4HadronPhysicsINCLXX::Others().

BuildDecayTableForBCHadrons()

void G4HadronicBuilder::BuildDecayTableForBCHadrons ( )

static

Definition at line 294 of file G4HadronicBuilder.cc.

                                                    {
  // Geant4 does not define the decay of most of charmed and bottom hadrons.
  // The reason is that most of these heavy hadrons have many different
  // decay channels, with a complex dynamics, quite different from the flat
  // phase space kinematical treatment used in Geant4 for most of hadronic decays.
  // High-energy experiments usually use dedicated Monte Carlo Event Generators
  // for the decays of charmed and bottom hadrons; therefore, these heavy
  // hadrons, which are passed to Geant4 as primary tracks, have pre-assigned
  // decays. Moreover, no charmed or bottom secondary hadrons were created
  // in Geant4 hadronic interactions before Geant4 10.7.
  // With the extension of Geant4 hadronic interactions to charmed and bottom
  // hadrons, in version Geant4 10.7, we do need to define decays in Geant4
  // for these heavy hadrons, for two reasons:
  // 1. For testing purposes, unless we pre-assign decays of heavy hadrons
  //    (as the HEP experiments normally do by using MC Event Generators);
  // 2. To avoid crashes (due to missing decay channels) whenever charmed or
  //    bottom secondary hadrons are produced by Geant4 hadronic interactions,
  //    even with ordinary (i.e. not heavy) hadron projectiles, because in
  //    this case we cannot (easily!) pre-assign decays to them.
  // Given that 1. is just a convenience for testing, and 2. happens rather
  // rarely in practice - because very few primary energetic (i.e. boosted)
  // heavy hadrons fly enough to reach the beam pipe or the tracker and
  // having an inelastic interaction there, and the very low probability
  // to create a heavy hadrons from the string fragmentation in ordinary
  // (i.e. not heavy) hadronic interactions - there is no need in practice
  // to define accurately the decays of heavy hadrons in Geant4.
  // So, for our practical purposes, it is enough to define very simple,
  // "dummy" decays of charmed and bottom hadrons.
  // Here we use a single, fully hadronic channel, with 2 or 3 or 4
  // daughters, for each of these heavy hadrons, assigning to this single
  // decay channel a 100% branching ratio, although in reality such a
  // channel is one between hundreds of possible ones (and therefore its
  // real branching ratio is typical of a few per-cent); moreover, we treat
  // the decay without any dynamics, i.e. with a flat phase space kinematical
  // treatment.
  // Note that some of the charmed and bottom hadrons such as SigmaC++,
  // SigmaC+, SigmaC0, SigmaB+, SigmaB0 and SigmaB- have one dominant
  // decay channel (to LambdaC/B + Pion) which is already defined in Geant4.
  // This is not the case for EtaC, JPsi and Upsilon, whose decays need to
  // be defined here (although they decay so quickly that their hadronic
  // interactions can be neglected, as we do for Pi0 and Sigma0).
  // Note that our definition of the decay tables for these heavy hadrons
  // do not interfere with the pre-assign decays of primary charmed and
  // bottom tracks made by the HEP experiments. In fact, pre-assign decays
  // have priority over (i.e. override) decay tables.
  static G4bool isFirstCall = true;
  if ( ! isFirstCall ) return;
  isFirstCall = false;
  G4ParticleTable* particleTable = G4ParticleTable::GetParticleTable();
  for ( auto & pdg : G4HadParticles::GetBCHadrons() ) {
    auto part = particleTable->FindParticle( pdg );
    if ( part == nullptr ) {
      G4cout << "G4HadronicBuilder::BuildDecayTableForBCHadrons : ERROR ! particlePDG="
             << pdg << " is not defined !" << G4endl;
      continue;
    }
    if ( part->GetDecayTable() ) {
      G4cout << "G4HadronicBuilder::BuildDecayTableForBCHadrons : WARNING ! particlePDG="
             << pdg << " has already a decay table defined !" << G4endl;
      continue;
    }
    G4DecayTable* decayTable = new G4DecayTable;
    const G4int numberDecayChannels = 1;
    G4VDecayChannel** mode = new G4VDecayChannel*[ numberDecayChannels ];
    for ( G4int i = 0; i < numberDecayChannels; ++i ) mode[i] = nullptr;
    switch ( pdg ) {
      // Charmed mesons
      case  411 :  // D+ 
        mode[0] = new G4PhaseSpaceDecayChannel( "D+", 1.0, 3, "kaon-", "pi+", "pi+" );
        break;
      case -411 :  // D- 
        mode[0] = new G4PhaseSpaceDecayChannel( "D-", 1.0, 3, "kaon+", "pi-", "pi-" );
        break;
      case  421 :  // D0
        mode[0] = new G4PhaseSpaceDecayChannel( "D0", 1.0, 3, "kaon-", "pi+", "pi0" );
        break;
      case -421 :  // anti_D0
        mode[0] = new G4PhaseSpaceDecayChannel( "anti_D0", 1.0, 3, "kaon+", "pi-", "pi0" );
        break;
      case  431 :  // Ds+ 
        mode[0] = new G4PhaseSpaceDecayChannel( "Ds+", 1.0, 3, "kaon+", "kaon-", "pi+" );
        break;
      case -431 :  // Ds- 
        mode[0] = new G4PhaseSpaceDecayChannel( "Ds-", 1.0, 3, "kaon-", "kaon+", "pi-" );
        break;
      // Bottom mesons  
      case  521 :  // B+ 
        mode[0] = new G4PhaseSpaceDecayChannel( "B+", 1.0, 3, "anti_D0", "pi+", "pi0" );
        break;
      case -521 :  // B- 
        mode[0] = new G4PhaseSpaceDecayChannel( "B-", 1.0, 3, "D0", "pi-", "pi0" );
        break;
      case  511 :  // B0
        mode[0] = new G4PhaseSpaceDecayChannel( "B0", 1.0, 3, "D-", "pi+", "pi0" );
        break;
      case -511 :  // anti_B0
        mode[0] = new G4PhaseSpaceDecayChannel( "anti_B0", 1.0, 3, "D+", "pi-", "pi0" );
        break;
      case  531 :  // Bs0
        mode[0] = new G4PhaseSpaceDecayChannel( "Bs0", 1.0, 3, "Ds-", "pi+", "pi0" );
        break;
      case -531 :  // anti_Bs0
        mode[0] = new G4PhaseSpaceDecayChannel( "anti_Bs0", 1.0, 3, "Ds+", "pi-", "pi0" );
        break;
      case  541 :  // Bc+ 
        mode[0] = new G4PhaseSpaceDecayChannel( "Bc+", 1.0, 2, "J/psi", "pi+" );
        break;
      case -541 :  // Bc- 
        mode[0] = new G4PhaseSpaceDecayChannel( "Bc-", 1.0, 2, "J/psi", "pi-" );
        break;
      // Charmed baryons (and anti-baryons)
      case  4122 :  // lambda_c+ 
        mode[0] = new G4PhaseSpaceDecayChannel( "lambda_c+", 1.0, 3, "proton", "kaon-", "pi+" );
        break;
      case -4122 :  // anti_lambda_c+ 
        mode[0] = new G4PhaseSpaceDecayChannel( "anti_lambda_c+", 1.0, 3, "anti_proton", "kaon+", "pi-" );
        break;
      case  4232 :  // xi_c+ 
        mode[0] = new G4PhaseSpaceDecayChannel( "xi_c+", 1.0, 3, "sigma+", "kaon-", "pi+" );
        break;
      case -4232 :  // anti_xi_c+ 
        mode[0] = new G4PhaseSpaceDecayChannel( "anti_xi_c+", 1.0, 3, "anti_sigma+", "kaon+", "pi-" );
        break;
      case  4132 :  // xi_c0 
        mode[0] = new G4PhaseSpaceDecayChannel( "xi_c0", 1.0, 3, "lambda", "kaon-", "pi+" );
        break;
      case -4132 :  // anti_xi_c0 
        mode[0] = new G4PhaseSpaceDecayChannel( "anti_xi_c0", 1.0, 3, "anti_lambda", "kaon+", "pi-" );
        break;
      case  4332 :  // omega_c0
        mode[0] = new G4PhaseSpaceDecayChannel( "omega_c0", 1.0, 3, "xi0", "kaon-", "pi+" );
        break;
      case -4332 :  // anti_omega_c0
        mode[0] = new G4PhaseSpaceDecayChannel( "anti_omega_c0", 1.0, 3, "anti_xi0", "kaon+", "pi-" );
        break;
      // Bottom baryons (and anti-baryons)
      case  5122 :  // lambda_b
        mode[0] = new G4PhaseSpaceDecayChannel( "lambda_b", 1.0, 4, "lambda_c+", "pi+", "pi-", "pi-" );
        break;
      case -5122 :  // anti_lambda_b
        mode[0] = new G4PhaseSpaceDecayChannel( "anti_lambda_b", 1.0, 4, "anti_lambda_c+", "pi-", "pi+", "pi+" );
        break;
      case  5232 :  // xi_b0
        mode[0] = new G4PhaseSpaceDecayChannel( "xi_b0", 1.0, 3, "lambda_c+", "kaon-", "pi0" );
        break;
      case -5232 :  // anti_xi_b0
        mode[0] = new G4PhaseSpaceDecayChannel( "anti_xi_b0", 1.0, 3, "anti_lambda_c+", "kaon+", "pi0" );
        break;
      case  5132 :  // xi_b-
        mode[0] = new G4PhaseSpaceDecayChannel( "xi_b-", 1.0, 3, "lambda_c+", "kaon-", "pi-" );
        break;
      case -5132 :  // anti_xi_b-
        mode[0] = new G4PhaseSpaceDecayChannel( "anti_xi_b-", 1.0, 3, "anti_lambda_c+", "kaon+", "pi+" );
        break;
      case  5332 :  // omega_b-
        mode[0] = new G4PhaseSpaceDecayChannel( "omega_b-", 1.0, 3, "xi_c+", "kaon-", "pi-" );
        break;
      case -5332 :  // anti_omega_b-
        mode[0] = new G4PhaseSpaceDecayChannel( "anti_omega_b-", 1.0, 3, "anti_xi_c+", "kaon+", "pi+" );
        break;
      default :
        G4cout << "G4HadronicBuilder::BuildDecayTableForBCHadrons : UNKNOWN particlePDG=" << pdg << G4endl;
    }  // End of the switch
 
    for ( G4int index = 0; index < numberDecayChannels; ++index ) decayTable->Insert( mode[index] );
    delete [] mode;
    part->SetDecayTable( decayTable );
  }  // End of the for loop over heavy hadrons
  // Add now the decay for etac, JPsi and Upsilon because these can be produced as
  // secondaries in hadronic interactions, while they are not part of the heavy
  // hadrons included in G4HadParticles::GetBCHadrons() because they live too shortly
  // and therefore their hadronic interactions can be neglected (as we do for pi0 and sigma0).
  if ( ! G4Etac::Definition()->GetDecayTable() ) {
    G4DecayTable* decayTable = new G4DecayTable;
    const G4int numberDecayChannels = 1;
    G4VDecayChannel** mode = new G4VDecayChannel*[ numberDecayChannels ];
    for ( G4int i = 0; i < numberDecayChannels; ++i ) mode[i] = nullptr;
    mode[0] = new G4PhaseSpaceDecayChannel( "etac", 1.0, 3, "eta", "pi+", "pi-" );
    for ( G4int index = 0; index < numberDecayChannels; ++index ) decayTable->Insert( mode[index] );
    delete [] mode;
    G4Etac::Definition()->SetDecayTable( decayTable );
  }
  if ( ! G4JPsi::Definition()->GetDecayTable() ) {
    G4DecayTable* decayTable = new G4DecayTable;
    const G4int numberDecayChannels = 1;
    G4VDecayChannel** mode = new G4VDecayChannel*[ numberDecayChannels ];
    for ( G4int i = 0; i < numberDecayChannels; ++i ) mode[i] = nullptr;
    mode[0] = new G4PhaseSpaceDecayChannel( "J/psi", 1.0, 3, "pi0", "pi+", "pi-" );
    for ( G4int index = 0; index < numberDecayChannels; ++index ) decayTable->Insert( mode[index] );
    delete [] mode;
    G4JPsi::Definition()->SetDecayTable( decayTable );
  }
  if ( ! G4Upsilon::Definition()->GetDecayTable() ) {
    G4DecayTable* decayTable = new G4DecayTable;
    const G4int numberDecayChannels = 1;
    G4VDecayChannel** mode = new G4VDecayChannel*[ numberDecayChannels ];
    for ( G4int i = 0; i < numberDecayChannels; ++i ) mode[i] = nullptr;
    mode[0] = new G4PhaseSpaceDecayChannel( "Upsilon", 1.0, 3, "eta_prime", "pi+", "pi-" );
    for ( G4int index = 0; index < numberDecayChannels; ++index ) decayTable->Insert( mode[index] );
    delete [] mode;
    G4Upsilon::Definition()->SetDecayTable( decayTable );
  }  
}

Referenced by BuildBCHadronsFTFP_BERT(), BuildBCHadronsFTFQGSP_BERT(), and BuildBCHadronsQGSP_FTFP_BERT().

BuildElastic()

void G4HadronicBuilder::BuildElastic ( const std::vector< G4int > &  particleList )

static

Definition at line 196 of file G4HadronicBuilder.cc.

                                                                     {
 
  G4HadronicParameters* param = G4HadronicParameters::Instance();
  G4PhysicsListHelper* ph = G4PhysicsListHelper::GetPhysicsListHelper();
 
  auto xsel = G4HadProcesses::ElasticXS("Glauber-Gribov");
 
  auto elModel = new G4HadronElastic();
  elModel->SetMaxEnergy( param->GetMaxEnergy() );
 
  G4ParticleTable* table = G4ParticleTable::GetParticleTable();
  for( auto & pdg : partList ) {
 
    auto part = table->FindParticle( pdg );
    if ( part == nullptr ) { continue; }
 
    auto hade = new G4HadronElasticProcess();
    hade->AddDataSet( xsel );
    hade->RegisterMe( elModel );
    if( param->ApplyFactorXS() ) hade->MultiplyCrossSectionBy( param->XSFactorHadronElastic() );
    ph->RegisterProcess(hade, part);
  }
}

Referenced by G4HadronDElasticPhysics::ConstructProcess(), G4HadronElasticPhysics::ConstructProcess(), and G4HadronHElasticPhysics::ConstructProcess().

BuildFTFP_INCLXX()

void G4HadronicBuilder::BuildFTFP_INCLXX ( const std::vector< G4int > &  partList, const G4String &  xsName  )

static

Definition at line 525 of file G4HadronicBuilder.cc.

                                                                                                     {
  G4HadronicParameters* param = G4HadronicParameters::Instance();
  G4PhysicsListHelper* ph = G4PhysicsListHelper::GetPhysicsListHelper();
  auto theTheoFSModel = new G4TheoFSGenerator( "FTFP" );
  auto theStringModel = new G4FTFModel;
  theStringModel->SetFragmentationModel( new G4ExcitedStringDecay );
  theTheoFSModel->SetHighEnergyGenerator( theStringModel );
  theTheoFSModel->SetTransport( new G4GeneratorPrecompoundInterface );
  theTheoFSModel->SetMaxEnergy( param->GetMaxEnergy() );
  theTheoFSModel->SetMinEnergy( 15.0*CLHEP::GeV );
  G4VPreCompoundModel* thePrecoModel = new G4PreCompoundModel;
  thePrecoModel->SetMinEnergy( 0.0 );
  thePrecoModel->SetMaxEnergy( 2.0*CLHEP::MeV );
  G4INCLXXInterface* theINCLXXModel = new G4INCLXXInterface( thePrecoModel );
  theINCLXXModel->SetMinEnergy( 1.0*CLHEP::MeV );
  theINCLXXModel->SetMaxEnergy( 20.0*CLHEP::GeV );
  auto xsinel = G4HadProcesses::InelasticXS( xsName );
  G4ParticleTable* table = G4ParticleTable::GetParticleTable();
  for ( auto & pdg : partList ) {
    auto part = table->FindParticle( pdg );
    if ( part == nullptr ) continue;
    auto hadi = new G4HadronInelasticProcess( part->GetParticleName()+"Inelastic", part );
    hadi->AddDataSet( xsinel );
    hadi->RegisterMe( theTheoFSModel );
    hadi->RegisterMe( theINCLXXModel );
    if ( param->ApplyFactorXS() ) hadi->MultiplyCrossSectionBy( param->XSFactorHadronInelastic() );
    ph->RegisterProcess( hadi, part );
  }
}

Referenced by BuildHyperNucleiFTFP_INCLXX().

BuildHyperAntiNucleiFTFP_BERT()

void G4HadronicBuilder::BuildHyperAntiNucleiFTFP_BERT ( )

static

Definition at line 510 of file G4HadronicBuilder.cc.

                                                      {
  if ( G4HadronicParameters::Instance()->EnableHyperNuclei() ) {
    // FTFP can be used down to zero kinetic energy.
    BuildFTFP_BERT( G4HadParticles::GetHyperAntiNuclei(), false, "AntiAGlauber" );
  }
}

Referenced by G4HadronPhysicsFTFP_BERT::Others(), and G4HadronPhysicsINCLXX::Others().

BuildHyperNucleiFTFP_BERT()

void G4HadronicBuilder::BuildHyperNucleiFTFP_BERT ( )

static

Definition at line 499 of file G4HadronicBuilder.cc.

                                                  {
  if ( G4HadronicParameters::Instance()->EnableHyperNuclei() ) {
    // Bertini intra-nuclear cascade model is currently not applicable for light
    // hypernuclei, therefore FTFP is used down to zero kinetic energy (but at
    // very low energies, a dummy model is used that simply returns the projectile
    // hypernucleus in the final state).
    BuildFTFP_BERT( G4HadParticles::GetHyperNuclei(), false, "Glauber-Gribov" );
  }
}

Referenced by G4HadronPhysicsFTFP_BERT::Others().

BuildHyperNucleiFTFP_INCLXX()

void G4HadronicBuilder::BuildHyperNucleiFTFP_INCLXX ( )

static

Definition at line 518 of file G4HadronicBuilder.cc.

                                                    {
  if ( G4HadronicParameters::Instance()->EnableHyperNuclei() ) {
    BuildFTFP_INCLXX( G4HadParticles::GetHyperNuclei(), "Glauber-Gribov" );
  }
}

Referenced by G4HadronPhysicsINCLXX::Others().

BuildHyperonsFTFP_BERT()

void G4HadronicBuilder::BuildHyperonsFTFP_BERT ( )

static

Definition at line 220 of file G4HadronicBuilder.cc.

                                               {
  // For hyperons, Bertini is used at low energies;
  // for anti-hyperons, FTFP can be used down to zero kinetic energy.
  BuildFTFP_BERT(G4HadParticles::GetHyperons(), true, "Glauber-Gribov");
  BuildFTFP_BERT(G4HadParticles::GetAntiHyperons(), false, "Glauber-Gribov");
}

Referenced by G4HadronInelasticQBBC::ConstructProcess(), G4HadronPhysicsFTFP_BERT::Others(), and G4HadronPhysicsINCLXX::Others().

BuildHyperonsFTFQGSP_BERT()

void G4HadronicBuilder::BuildHyperonsFTFQGSP_BERT ( )

static

Definition at line 227 of file G4HadronicBuilder.cc.

                                                  {
  // For hyperons, Bertini is used at low energies;
  // for anti-hyperons, FTFP can be used down to zero kinetic energy.
  BuildFTFQGSP_BERT(G4HadParticles::GetHyperons(), true, "Glauber-Gribov");
  BuildFTFQGSP_BERT(G4HadParticles::GetAntiHyperons(), false, "Glauber-Gribov");
}

Referenced by G4HadronPhysicsFTFQGSP_BERT::ConstructProcess().

BuildHyperonsQGSP_FTFP_BERT()

void G4HadronicBuilder::BuildHyperonsQGSP_FTFP_BERT ( G4bool  quasiElastic )

static

Definition at line 234 of file G4HadronicBuilder.cc.

                                                                   {
  // For hyperons, Bertini is used at low energies;
  // for anti-hyperons, FTFP can be used down to zero kinetic energy.
  // QGSP is used at high energies in all cases.
  BuildQGSP_FTFP_BERT(G4HadParticles::GetHyperons(), true, qElastic, "Glauber-Gribov");
  BuildQGSP_FTFP_BERT(G4HadParticles::GetAntiHyperons(), false, qElastic, "Glauber-Gribov");
}

Referenced by G4HadronPhysicsQGSP_BERT::Others(), G4HadronPhysicsQGSP_BIC::Others(), and G4HadronPhysicsINCLXX::Others().

BuildKaonsFTFP_BERT()

void G4HadronicBuilder::BuildKaonsFTFP_BERT ( )

static

Definition at line 242 of file G4HadronicBuilder.cc.

                                            {
  BuildFTFP_BERT(G4HadParticles::GetKaons(), true, "Glauber-Gribov");
}

Referenced by G4HadronInelasticQBBC::ConstructProcess().

BuildKaonsFTFQGSP_BERT()

void G4HadronicBuilder::BuildKaonsFTFQGSP_BERT ( )

static

Definition at line 246 of file G4HadronicBuilder.cc.

                                               {
  BuildFTFP_BERT(G4HadParticles::GetKaons(), true, "Glauber-Gribov");
}

Referenced by G4HadronPhysicsFTFQGSP_BERT::ConstructProcess().

BuildKaonsQGSP_FTFP_BERT()

void G4HadronicBuilder::BuildKaonsQGSP_FTFP_BERT ( G4bool  quasiElastic )

static

Definition at line 250 of file G4HadronicBuilder.cc.

                                                                {
  BuildQGSP_FTFP_BERT(G4HadParticles::GetKaons(), true, qElastic, "Glauber-Gribov");
}

---

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

• G4HadronicBuilder.hh
• G4HadronicBuilder.cc