| 1 | // |
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| 2 | // ******************************************************************** |
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| 3 | // * License and Disclaimer * |
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| 4 | // * * |
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| 5 | // * The Geant4 software is copyright of the Copyright Holders of * |
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| 6 | // * the Geant4 Collaboration. It is provided under the terms and * |
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| 7 | // * conditions of the Geant4 Software License, included in the file * |
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| 8 | // * LICENSE and available at http://cern.ch/geant4/license . These * |
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| 9 | // * include a list of copyright holders. * |
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| 10 | // * * |
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| 11 | // * Neither the authors of this software system, nor their employing * |
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| 12 | // * institutes,nor the agencies providing financial support for this * |
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| 13 | // * work make any representation or warranty, express or implied, * |
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| 14 | // * regarding this software system or assume any liability for its * |
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| 15 | // * use. Please see the license in the file LICENSE and URL above * |
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| 16 | // * for the full disclaimer and the limitation of liability. * |
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| 17 | // * * |
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| 18 | // * This code implementation is the result of the scientific and * |
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| 19 | // * technical work of the GEANT4 collaboration. * |
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| 20 | // * By using, copying, modifying or distributing the software (or * |
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| 21 | // * any work based on the software) you agree to acknowledge its * |
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| 22 | // * use in resulting scientific publications, and indicate your * |
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| 23 | // * acceptance of all terms of the Geant4 Software license. * |
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| 24 | // ******************************************************************** |
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| 25 | // |
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| 26 | // |
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| 27 | // |
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| 28 | // $Id: G4QString.hh,v 1.2 2006/12/12 11:02:22 mkossov Exp $ |
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| 29 | // GEANT4 tag $Name: $ |
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| 30 | |
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| 31 | #ifndef G4QString_h |
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| 32 | #define G4QString_h 1 |
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| 33 | |
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| 34 | // ------------------------------------------------------------ |
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| 35 | // GEANT 4 class header file |
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| 36 | // |
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| 37 | // ---------------- G4QString ---------------- |
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| 38 | // by Mikhail Kosov, October 2006. |
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| 39 | // class for an excited string used by Parton String Models |
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| 40 | // For comparison mirror member functions are taken from G4 classes: |
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| 41 | // G4FragmentingString |
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| 42 | // G4ExcitedStringDecay |
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| 43 | // |
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| 44 | // ------------------------------------------------------------ |
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| 45 | |
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| 46 | #include "G4ios.hh" |
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| 47 | #include "globals.hh" |
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| 48 | #include "G4ThreeVector.hh" |
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| 49 | #include "G4LorentzVector.hh" |
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| 50 | #include "G4LorentzRotation.hh" |
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| 51 | #include "G4QHadronVector.hh" |
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| 52 | #include "G4QHadronBuilder.hh" |
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| 53 | #include "G4QPartonPair.hh" |
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| 54 | #include "G4QPartonVector.hh" |
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| 55 | #include <algorithm> |
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| 56 | |
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| 57 | class G4QString |
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| 58 | { |
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| 59 | public: |
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| 60 | |
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| 61 | enum {PROJECTILE = 1, TARGET = -1}; // The same as in quark-pair (@@ ? M.K.) |
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| 62 | |
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| 63 | G4QString(); // formal creation of the string with future excitation |
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| 64 | G4QString(G4QParton* Color,G4QParton* Gluon, G4QParton* AntiColor, G4int Dir=PROJECTILE); |
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| 65 | G4QString(G4QParton* Col,G4QParton* AntiCol, G4int Dir=PROJECTILE); |
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| 66 | G4QString(const G4QString &right); |
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| 67 | |
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| 68 | ~G4QString(); |
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| 69 | |
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| 70 | // Selectors |
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| 71 | G4int operator==(const G4QString &right) const {return this == &right;} |
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| 72 | G4int operator!=(const G4QString &right) const {return this != &right;} |
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| 73 | const G4ThreeVector& GetPosition() const {return thePosition;} |
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| 74 | const G4QPartonVector* GetPartonList() const {return &thePartons;} |
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| 75 | G4QParton* GetGluon() const {return thePartons[1];} |
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| 76 | G4QParton* GetGluon(G4int GluonPos) const {return thePartons[1 + GluonPos];} |
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| 77 | G4QParton* GetLeftParton() const {return *thePartons.begin();} |
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| 78 | G4QParton* GetRightParton() const {return *(thePartons.end()-1);} |
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| 79 | G4bool IsItKinkyString() const {return (thePartons.size() > 2);} |
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| 80 | G4int GetDirection() const {return theDirection;} |
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| 81 | G4bool IsExcited() const {return true;} // Can be absolete? @@ M.K. |
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| 82 | G4LorentzVector Get4Momentum() const; |
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| 83 | //G4QHadron* GetAsQHadron(); //@@ Create a QHadron, corresponding to not excited string |
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| 84 | G4QParton* GetColorParton() const; |
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| 85 | G4QParton* GetAntiColorParton() const; |
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| 86 | G4QParton* GetStableParton() const{ return theStableParton;} // stable at the moment |
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| 87 | G4QParton* GetDecayParton() const{return theDecayParton;}// now involved in fragmentation |
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| 88 | G4int GetDecayDirection() const; |
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| 89 | G4bool FourQuarkString() const; // Checks that the string is qq-(qq)bar string |
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| 90 | G4bool DecayIsQuark() const {return theDecayParton->GetParticleSubType()=="quark";} |
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| 91 | G4bool StableIsQuark() const {return theStableParton->GetParticleSubType()=="quark";} |
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| 92 | G4ThreeVector StablePt(); // Get Pt of the stable quark |
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| 93 | G4ThreeVector DecayPt(); // Get Pt of the decaying quark |
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| 94 | G4double LightConePlus(){return Pplus;} |
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| 95 | G4double LightConeMinus() {return Pminus;} |
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| 96 | G4double LightConeDecay(); |
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| 97 | G4LorentzVector GetFragmentation4Mom() const; //!! Instead of Get$Momentum in FragmString |
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| 98 | G4double Mass2() const {return Pplus*Pminus-(Ptleft+Ptright).mag2();} |
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| 99 | G4double Mass() const{return std::sqrt(Mass2());} |
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| 100 | G4bool StopFragmentation() {return FragmentationMass(&G4QHadronBuilder::BuildHighSpin) |
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| 101 | + MassCut > GetFragmentation4Mom().mag();} |
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| 102 | G4bool IsFragmentable() {return FragmentationMass() + MassCut < Mass();} |
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| 103 | G4ThreeVector SampleQuarkPt(); |
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| 104 | G4bool SplitLast(G4QString* string, G4QHadronVector* LeftHV, G4QHadronVector* RightHV); |
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| 105 | |
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| 106 | void Sample4Momentum(G4LorentzVector* Mom, G4double M, G4LorentzVector* aMom, |
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| 107 | G4double aM, G4double InitialMass); |
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| 108 | // Modifiers |
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| 109 | void SetPosition(const G4ThreeVector& aPosition) {thePosition= aPosition;} |
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| 110 | void SetDirection(G4int dir) {theDirection=dir;} |
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| 111 | void LorentzRotate(const G4LorentzRotation& rotation); |
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| 112 | void InsertParton(G4QParton* aParton, const G4QParton* addafter = NULL); |
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| 113 | void Boost(G4ThreeVector& Velocity); |
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| 114 | G4LorentzRotation TransformToCenterOfMass(); |
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| 115 | G4LorentzRotation TransformToAlignedCms(); |
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| 116 | void DiffString(G4QHadron* aHadron, G4bool isProjectile); |
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| 117 | void ExciteString(G4QParton* Col,G4QParton* AntiCol, G4int Dir); |
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| 118 | G4QHadronVector* FragmentString(G4bool QL); // Fragment String using QGSM=true/LUND=false |
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| 119 | G4QString* CPExcited(); // Creates a string, using only CMS end-partons of the string |
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| 120 | G4QHadronVector* LightFragmentationTest(); |
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| 121 | G4double FragmentationMass(G4QHcreate build=0, G4QHadronPair* pdefs=0); |
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| 122 | void CalculateHadronTimePosition(G4double theInitialStringMass, G4QHadronVector*); |
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| 123 | void SetLeftPartonStable(); |
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| 124 | void SetRightPartonStable(); |
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| 125 | void UpdateString(G4QParton* decay, const G4LorentzVector* mom); |
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| 126 | G4QString(G4QParton* newdecay, const G4LorentzVector* momentum); |
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| 127 | G4QHadron* Splitup(G4bool QL); // Split Hadron & update the string, QGSM:true,Lund:false |
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| 128 | G4LorentzVector* SplitEandP(G4QHadron* pHadron, G4bool QL); // QGSM:QL=true,Lund:QL=false |
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| 129 | G4QParton* CreateParton(G4int PDGcode) {return new G4QParton(PDGcode);} |
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| 130 | G4QPartonPair CreatePartonPair(G4int NeedParticle, G4bool AllowDiquarks=true); |
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| 131 | G4QHadron* QuarkSplitup(G4QParton* decay, G4QParton* &created); |
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| 132 | G4QHadron* DiQuarkSplitup(G4QParton* decay, G4QParton* &created); |
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| 133 | G4int SampleQuarkFlavor() {return (1+G4int(G4UniformRand()/StrangeSuppress));} // ? M.K. |
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| 134 | |
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| 135 | // Static functions |
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| 136 | static void SetParameters(G4double mCut, G4double clustM, G4double sigQT, G4double DQSup, |
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| 137 | G4double DQBU, G4double smPar, G4double SSup, G4double SigPt, G4int SLmax, G4int CLmax); |
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| 138 | |
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| 139 | private: |
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| 140 | // Private functions |
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| 141 | G4ThreeVector GaussianPt(G4double widthSquare, G4double maxPtSquare) const; |
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| 142 | G4double GetLundLightConeZ(G4double zmin, G4double zmax, G4int PartonEncoding, |
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| 143 | G4QHadron* pHadron, G4double Px, G4double Py); |
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| 144 | G4double GetQGSMLightConeZ(G4double zmin, G4double zmax, G4int PartonEncoding, |
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| 145 | G4QHadron* pHadron, G4double Px, G4double Py); |
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| 146 | |
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| 147 | // Static parameters |
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| 148 | // Parameters of Longitudinal String Fragmentation |
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| 149 | static G4double MassCut; // minimum mass cut for the string |
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| 150 | static G4double ClusterMass; // minimum cluster mass for the fragmentation |
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| 151 | static G4double SigmaQT; // quark transverse momentum distribution parameter |
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| 152 | static G4double DiquarkSuppress; // is Diquark suppression parameter |
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| 153 | static G4double DiquarkBreakProb; // is Diquark breaking probability |
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| 154 | static G4double SmoothParam; // QGS model parameter |
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| 155 | static G4double StrangeSuppress; // Strangeness suppression parameter |
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| 156 | static G4double widthOfPtSquare; // width^2 of pt for string excitation |
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| 157 | static G4int StringLoopInterrupt; // String fragmentation LOOP limit |
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| 158 | static G4int ClusterLoopInterrupt; // Cluster fragmentation LOOP limit |
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| 159 | |
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| 160 | // Body |
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| 161 | G4int theDirection; // must be 1 or -1 (PROJECTILE or TARGET) |
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| 162 | G4ThreeVector thePosition; // Defined by the first quark position |
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| 163 | G4QPartonVector thePartons; // would like initial capacity for 3 Partons (? M.K.) |
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| 164 | G4QHadronBuilder* hadronizer;// Hadronizer of hodrons out of partons |
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| 165 | G4ThreeVector Ptleft,Ptright;// Pt (px,py) for partons (pz ignored!) |
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| 166 | G4double Pplus, Pminus; // p-, p+ of string, Plus is assigned to Left! |
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| 167 | G4QParton* theStableParton; // Parton on the stable side of the string |
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| 168 | G4QParton* theDecayParton; // Parton on the decaying part of the string |
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| 169 | enum DecaySide {None, Left, Right}; // @@ To have two @@ Leav : 1=Left |
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| 170 | DecaySide decaying; // @@ it's too much @@ only : 0=Unknown |
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| 171 | G4int SideOfDecay; // @@ of a good thing @@ one! : -1=Right |
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| 172 | }; |
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| 173 | |
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| 174 | #endif |
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