Import Geant4 10.6.0 source tree
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@@ -24,20 +24,19 @@
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// ********************************************************************
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//
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//
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// Maxim Komogorov
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//
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// -----------------------------------------------------------------------------
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// GEANT 4 class implementation file
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//
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// History: first implementation, Maxim Komogorov, 1-Jul-1998
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// -----------------------------------------------------------------------------
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#ifndef G4VLongitudinalStringDecay_h
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#define G4VLongitudinalStringDecay_h 1
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#include "G4VStringFragmentation.hh"
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#include "G4DynamicParticle.hh"
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#include "G4KineticTrack.hh"
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#include "G4KineticTrackVector.hh"
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#include "G4HadronBuilder.hh"
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#include <vector>
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class G4FragmentingString;
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//**************************************************************************************
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@@ -58,14 +57,22 @@ class G4VLongitudinalStringDecay
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public:
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virtual G4KineticTrackVector* FragmentString(const G4ExcitedString& theString)=0;
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protected:
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void AddNewParticles();
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void EraseNewParticles();
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//struct DeleteString { void operator()(G4ExcitedString* aS){delete aS;} };
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// To set minimal mass of a string. The string with mass above the minimal mass can fragment.
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void SetMinMasses();
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void SetMinimalStringMass(const G4FragmentingString * const string);
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void SetMinimalStringMass2(const G4double aValue);
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protected:
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// For changing Mass Cut used for selection of very small mass strings
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virtual void SetMassCut(G4double aValue);
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G4double GetMassCut();
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// For handling a string with very low mass
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G4KineticTrackVector * LightFragmentationTest(const G4ExcitedString * const theString);
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G4KineticTrackVector * ProduceOneHadron(const G4ExcitedString * const theString);
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// To store created quarks or 2 last hadrons
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typedef std::pair<G4ParticleDefinition*, G4ParticleDefinition*> pDefPair;
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@@ -74,52 +81,52 @@ class G4VLongitudinalStringDecay
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typedef G4ParticleDefinition * (G4HadronBuilder::*Pcreate)
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(G4ParticleDefinition*, G4ParticleDefinition*);
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// Used by LightFragmentationTest for estimation of lowest possible mass of
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// given quark system
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G4double FragmentationMass(const G4FragmentingString * const string,
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// Used by ProduceOneHadron method for estimation of lowest possible mass of
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// given quark system -- string.
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G4double PossibleHadronMass(const G4FragmentingString * const string,
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Pcreate build=0, pDefPair * pdefs=0);
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G4ParticleDefinition* FindParticle(G4int Encoding);
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virtual void Sample4Momentum(G4LorentzVector* Mom, G4double Mass,
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G4LorentzVector* AntiMom, G4double AntiMass,
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G4double InitialMass)=0;
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// For decision on continue or stop string fragmentation
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virtual G4bool StopFragmenting(const G4FragmentingString * const string)=0;
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virtual G4bool IsFragmentable(const G4FragmentingString * const string)=0;
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virtual G4bool IsItFragmentable(const G4FragmentingString * const string)=0;
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// If a string can not fragment, make last break into 2 hadrons
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virtual G4bool SplitLast(G4FragmentingString * string,
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G4KineticTrackVector * LeftVector,
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G4KineticTrackVector * RightVector)=0;
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// If a string fragments, do the following
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virtual void Sample4Momentum(G4LorentzVector* Mom, G4double Mass,
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G4LorentzVector* AntiMom, G4double AntiMass,
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G4double InitialMass)=0;
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// To make a copy of a string
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// If a string can fragment, do the following:
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// Make a copy of a string
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G4ExcitedString *CopyExcited(const G4ExcitedString& string);
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G4ParticleDefinition * QuarkSplitup(G4ParticleDefinition* decay,
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G4ParticleDefinition *&created);
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// Produce a hadron at Splitup of the string
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virtual G4KineticTrack * Splitup(G4FragmentingString *string,
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G4FragmentingString *&newString)=0;
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// The hadron can be producet at QuarkSplitup or DiQuarkSplitup
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virtual G4ParticleDefinition * QuarkSplitup(G4ParticleDefinition* decay,
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G4ParticleDefinition *&created);
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virtual G4ParticleDefinition * DiQuarkSplitup(G4ParticleDefinition* decay,
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G4ParticleDefinition *&created)=0;
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// All of them are going through quak-antiquark pair creation
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pDefPair CreatePartonPair(G4int NeedParticle, G4bool AllowDiquarks=true);
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public:
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// used by G4VKinkyStringDecy..
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// For a pair it is needed:
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G4int SampleQuarkFlavor(void);
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G4ThreeVector SampleQuarkPt(G4double ptMax=-1.); // -1. no limit on maxpt.
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protected:
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// For determination of kinematical properties of created hadron
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// virtual G4LorentzVector * SplitEandP(G4ParticleDefinition * pHadron,
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// G4FragmentingString * string )=0;
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virtual G4KineticTrack * Splitup(G4FragmentingString *string,
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G4FragmentingString *&newString)=0;
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// For determination of kinematical properties of the created hadron
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virtual G4LorentzVector * SplitEandP(G4ParticleDefinition * pHadron,
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G4FragmentingString * string,
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G4FragmentingString * newString )=0;
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@@ -139,9 +146,6 @@ class G4VLongitudinalStringDecay
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G4bool theGivenSpin, G4int theSpin);
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public:
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G4KineticTrackVector* DecayResonans (G4KineticTrackVector* aHadrons);
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void SetSigmaTransverseMomentum(G4double aQT);
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void SetStrangenessSuppression(G4double aValue);
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void SetDiquarkSuppression(G4double aValue);
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@@ -155,29 +159,33 @@ class G4VLongitudinalStringDecay
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void SetStringTensionParameter(G4double aValue);
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// G4LorentzVector RestMomentum;
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void SetProbCCbar(G4double aValue);
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void SetProbEta_c(G4double aValue);
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void SetProbBBbar(G4double aValue);
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void SetProbEta_b(G4double aValue);
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//private:
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protected:
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G4double GetDiquarkSuppress() {return DiquarkSuppress;};
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G4double GetDiquarkBreakProb() {return DiquarkBreakProb;};
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G4double GetStrangeSuppress() {return StrangeSuppress;};
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G4double GetClusterMass() {return ClusterMass;};
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G4int GetClusterLoopInterrupt() {return ClusterLoopInterrupt;};
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G4double GetProbCCbar(){return ProbCCbar;};
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G4double GetProbEta_c(){return ProbEta_c;};
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G4double GetProbBBbar(){return ProbBBbar;};
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G4double GetProbEta_b(){return ProbEta_b;};
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G4double GetStringTensionParameter() {return Kappa;};
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//private:
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protected:
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G4double MassCut;
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G4double ClusterMass;
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G4double SigmaQT; // sigma_q_t is quark transverse momentum distribution parameter
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G4double DiquarkSuppress; // is Diquark suppression parameter
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G4double DiquarkBreakProb; // is Diquark breaking probability
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G4double SmoothParam; // model parameter
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G4double SigmaQT; // sigma_q_t of quark/hadron transverse momentum distribution parameter
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G4double DiquarkSuppress; // Diquark suppression parameter
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G4double DiquarkBreakProb; // Diquark breaking probability, qq->h+qq'
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G4double StrangeSuppress ;
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G4int StringLoopInterrupt;
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G4int ClusterLoopInterrupt;
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G4HadronBuilder *hadronizer;
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G4double pspin_meson;
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@@ -185,16 +193,63 @@ class G4VLongitudinalStringDecay
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std::vector<G4double> vectorMesonMix;
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std::vector<G4double> scalarMesonMix;
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G4bool PastInitPhase;
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G4double ProbCCbar; // Probability of C-Cbar pair creation
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G4double ProbEta_c; // Mixing of Eta_c and J/Psi
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G4double Kappa; // String tension parameter
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G4double ProbBBbar; // Probability of B-Bbar pair creation
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G4double ProbEta_b; // Mixing of Eta_b and Ipsilon_b
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// G4double MinFragmentationMass(G4ExcitedString * theString,
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// G4ParticleDefinition*& Hadron1,
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// G4ParticleDefinition*& Hadron2);
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G4double ProbCB; // = ProbCCbar + ProbBBbar
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G4double MaxMass;
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G4bool PastInitPhase;
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G4double Kappa; // String tension parameter
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std::vector<G4ParticleDefinition *> NewParticles;
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public:
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// ------ For estimation of a minimal string mass ---------------
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G4double Mass_of_light_quark;
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G4double Mass_of_s_quark;
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G4double Mass_of_c_quark;
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G4double Mass_of_b_quark;
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G4double Mass_of_string_junction;
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G4double minMassQQbarStr[5][5];
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G4double minMassQDiQStr[5][5][5];
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// ------ An estimated minimal string mass ----------------------
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G4double MinimalStringMass;
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G4double MinimalStringMass2;
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G4int Qcharge[5]; // quark charges
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G4int Meson[5][5][7];
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G4double MesonWeight[5][5][7];
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G4int Baryon[5][5][5][4];
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G4double BaryonWeight[5][5][5][4];
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G4double Prob_QQbar[5];
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G4int DecayQuark;
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G4int NewQuark;
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/*
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G4double FFq2q[5][5][2];
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G4double FFq2qq[5][15][2];
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G4double FFqq2q[15][5][2];
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G4double FFqq2qq[15][5][2];
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*/
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// ------ To improve the code structure
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G4ParticleDefinition * FS_LeftHadron[350], * FS_RightHadron[350];
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G4double FS_Weight[350];
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G4int NumberOf_FS;
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};
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//*************************************************************************************
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// Class G4VLongitudinalStringDecay
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#endif
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