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geant4/source/processes/hadronic/models/parton_string/diffraction/include/G4FTFModel.hh
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2018-12-07 15:15:39 +01:00

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//
// ********************************************************************
// * 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 *
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// * include a list of copyright holders. *
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// * use. Please see the license in the file LICENSE and URL above *
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// * *
// * 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 *
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// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
//
//
// Class Description
// Final state production code for hadron inelastic scattering above 3 GeV
// based on the modeling ansatz used in FRITIOF.
// To be used in your physics list in case you need this physics.
// In this case you want to register an object of this class with an object
// of G4TheoFSGenerator.
// Class Description - End
#ifndef G4FTFModel_h
#define G4FTFModel_h 1
// ------------------------------------------------------------
// GEANT 4 class header file
//
// ---------------- G4FTFModel ----------------
// by Gunter Folger, May 1998.
// class implementing the excitation in the FTF Parton String Model
// ------------------------------------------------------------
#include "G4VPartonStringModel.hh"
#include "G4FTFParameters.hh"
#include "G4FTFParticipants.hh"
#include "G4ExcitedStringVector.hh"
#include "G4DiffractiveExcitation.hh"
#include "G4ElasticHNScattering.hh"
#include "G4FTFAnnihilation.hh"
#include "G4Proton.hh"
#include "G4Neutron.hh"
class G4VSplitableHadron;
class G4ExcitedString;
class G4FTFModel : public G4VPartonStringModel {
public:
G4FTFModel( const G4String& modelName = "FTF" );
~G4FTFModel();
void Init( const G4Nucleus& aNucleus, const G4DynamicParticle& aProjectile );
G4ExcitedStringVector* GetStrings();
G4V3DNucleus* GetWoundedNucleus() const;
G4V3DNucleus* GetTargetNucleus() const;
G4V3DNucleus* GetProjectileNucleus() const;
virtual void ModelDescription( std::ostream& ) const;
private:
G4FTFModel( const G4FTFModel& right );
const G4FTFModel& operator=( const G4FTFModel& right );
int operator==( const G4FTFModel& right ) const;
int operator!=( const G4FTFModel& right ) const;
void StoreInvolvedNucleon();
void ReggeonCascade();
G4bool PutOnMassShell();
G4bool ExciteParticipants();
G4ExcitedStringVector* BuildStrings();
void GetResiduals();
G4bool AdjustNucleons( G4VSplitableHadron* SelectedAntiBaryon,
G4Nucleon* ProjectileNucleon,
G4VSplitableHadron* SelectedTargetNucleon,
G4Nucleon* TargetNucleon,
G4bool Annihilation );
// The "AdjustNucleons" method uses the following struct and 3 new utility methods:
struct CommonVariables {
G4int TResidualMassNumber = 0, TResidualCharge = 0, PResidualMassNumber = 0,
PResidualCharge = 0;
G4double SqrtS = 0.0, S = 0.0, SumMasses = 0.0,
TResidualExcitationEnergy = 0.0, TResidualMass = 0.0, TNucleonMass = 0.0,
PResidualExcitationEnergy = 0.0, PResidualMass = 0.0, PNucleonMass = 0.0,
Mprojectile = 0.0, M2projectile = 0.0, Pzprojectile = 0.0, Eprojectile = 0.0,
WplusProjectile = 0.0,
Mtarget = 0.0, M2target = 0.0, Pztarget = 0.0, Etarget = 0.0, WminusTarget = 0.0,
Mt2targetNucleon = 0.0, PztargetNucleon = 0.0, EtargetNucleon = 0.0,
Mt2projectileNucleon = 0.0, PzprojectileNucleon = 0.0, EprojectileNucleon = 0.0,
YtargetNucleus = 0.0, YprojectileNucleus = 0.0,
XminusNucleon = 0.0, XplusNucleon = 0.0, XminusResidual = 0.0, XplusResidual = 0.0;
G4ThreeVector PtNucleon, PtResidual, PtNucleonP, PtResidualP, PtNucleonT, PtResidualT;
G4LorentzVector Psum, Pprojectile, Ptmp, Ptarget, TResidual4Momentum, PResidual4Momentum;
G4LorentzRotation toCms, toLab;
};
G4int AdjustNucleonsAlgorithm_beforeSampling( G4int interactionCase,
G4VSplitableHadron* SelectedAntiBaryon,
G4Nucleon* ProjectileNucleon,
G4VSplitableHadron* SelectedTargetNucleon,
G4Nucleon* TargetNucleon,
G4bool Annihilation,
CommonVariables& common );
G4bool AdjustNucleonsAlgorithm_Sampling( G4int interactionCase,
CommonVariables& common );
void AdjustNucleonsAlgorithm_afterSampling( G4int interactionCase,
G4VSplitableHadron* SelectedAntiBaryon,
G4VSplitableHadron* SelectedTargetNucleon,
CommonVariables& common );
G4ThreeVector GaussianPt( G4double AveragePt2, G4double maxPtSquare ) const;
G4bool ComputeNucleusProperties( G4V3DNucleus* nucleus, G4LorentzVector& nucleusMomentum,
G4LorentzVector& residualMomentum, G4double& sumMasses,
G4double& residualExcitationEnergy, G4double& residualMass,
G4int& residualMassNumber, G4int& residualCharge );
// Utility method used by PutOnMassShell.
G4bool GenerateDeltaIsobar( const G4double sqrtS, const G4int numberOfInvolvedNucleons,
G4Nucleon* involvedNucleons[], G4double& sumMasses );
// Utility method used by PutOnMassShell.
G4bool SamplingNucleonKinematics( G4double averagePt2, const G4double maxPt2,
G4double dCor, G4V3DNucleus* nucleus,
const G4LorentzVector& pResidual,
const G4double residualMass, const G4int residualMassNumber,
const G4int numberOfInvolvedNucleons,
G4Nucleon* involvedNucleons[], G4double& mass2 );
// Utility method used by PutOnMassShell.
G4bool CheckKinematics( const G4double sValue, const G4double sqrtS,
const G4double projectileMass2, const G4double targetMass2,
const G4double nucleusY, const G4bool isProjectileNucleus,
const G4int numberOfInvolvedNucleons, G4Nucleon* involvedNucleons[],
G4double& targetWminus, G4double& projectileWplus, G4bool& success );
// Utility method used by PutOnMassShell.
G4bool FinalizeKinematics( const G4double w, const G4bool isProjectileNucleus,
const G4LorentzRotation& boostFromCmsToLab,
const G4double residualMass, const G4int residualMassNumber,
const G4int numberOfInvolvedNucleons,
G4Nucleon* involvedNucleons[],
G4LorentzVector& residual4Momentum );
// Utility method used by PutOnMassShell.
G4ReactionProduct theProjectile;
G4FTFParticipants theParticipants;
G4Nucleon* TheInvolvedNucleonsOfTarget[250];
G4int NumberOfInvolvedNucleonsOfTarget;
G4Nucleon* TheInvolvedNucleonsOfProjectile[250];
G4int NumberOfInvolvedNucleonsOfProjectile;
G4FTFParameters* theParameters;
G4DiffractiveExcitation* theExcitation;
G4ElasticHNScattering* theElastic;
G4FTFAnnihilation* theAnnihilation;
std::vector< G4VSplitableHadron* > theAdditionalString;
G4double LowEnergyLimit;
G4bool HighEnergyInter;
G4LorentzVector ProjectileResidual4Momentum;
G4int ProjectileResidualMassNumber;
G4int ProjectileResidualCharge;
G4double ProjectileResidualExcitationEnergy;
G4LorentzVector TargetResidual4Momentum;
G4int TargetResidualMassNumber;
G4int TargetResidualCharge;
G4double TargetResidualExcitationEnergy;
};
inline G4V3DNucleus* G4FTFModel::GetWoundedNucleus() const {
return theParticipants.GetWoundedNucleus();
}
inline G4V3DNucleus* G4FTFModel::GetTargetNucleus() const {
return theParticipants.GetWoundedNucleus();
}
inline G4V3DNucleus* G4FTFModel::GetProjectileNucleus() const {
return theParticipants.GetProjectileNucleus();
}
#endif