// // ******************************************************************** // * 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 * // * LICENSE and available at http://cern.ch/geant4/license . These * // * include a list of copyright holders. * // * * // * 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. Please see the license in the file LICENSE and URL above * // * for the full disclaimer and the limitation of liability. * // * * // * 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 * // * use in resulting scientific publications, and indicate your * // * acceptance of all terms of the Geant4 Software license. * // ******************************************************************** // // // $Id: G4FTFModel.hh 110870 2018-06-22 12:14:16Z gcosmo $ // GEANT4 tag $Name: $ // // 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