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G4QString.hh
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28 // $Id$
29 
30 #ifndef G4QString_h
31 #define G4QString_h 1
32 
33 // ------------------------------------------------------------
34 // GEANT 4 class header file
35 //
36 // ---------------- G4QString ----------------
37 // by Mikhail Kosov, October 2006.
38 // class for an excited string used by Parton String Models
39 // For comparison mirror member functions are taken from G4 classes:
40 // G4FragmentingString
41 // G4ExcitedStringDecay
42 //
43 // ------------------------------------------------------------
44 // Short description: If partons from the G4QPartonPair are close in
45 // rapidity, they create Quasmons, but if they are far in the rapidity
46 // space, they can not interact directly. Say the bottom parton (quark)
47 // has rapidity 0, and the top parton (antiquark) has rapidity 8, then
48 // the top quark splits in two by radiating gluon, and each part has
49 // rapidity 4, then the gluon splits in quark-antiquark pair (rapidity
50 // 2 each), and then the quark gadiates anothe gluon and reachs rapidity
51 // 1. Now it can interact with the bottom antiquark, creating a Quasmon
52 // or a hadron. The intermediate partons is the string ladder.
53 // ---------------------------------------------------------------------
54 
55 #include "G4ios.hh"
56 #include "globals.hh"
57 #include "G4ThreeVector.hh"
58 #include "G4LorentzVector.hh"
59 #include "G4LorentzRotation.hh"
60 #include "G4QHadronVector.hh"
61 #include "G4QPartonPair.hh"
62 #include "G4QPartonVector.hh"
63 #include <algorithm>
64 
65 class G4QString
66 {
67  public:
68 
69  enum {PROJECTILE = 1, TARGET = -1}; // The same as in quark-pair (@@ ? M.K.)
70 
71  G4QString(); // formal creation of the string with future excitation
72  G4QString(G4QParton* Color,G4QParton* Gluon, G4QParton* AntiColor, G4int Dir=PROJECTILE);
73  G4QString(G4QParton* Col, G4QParton* AntiCol, G4int Dir=PROJECTILE);
74  G4QString(G4QPartonPair* ColAntiCol);
75  G4QString(const G4QString &right);
76  G4QString(const G4QString &old, G4QParton* newdecay, const G4LorentzVector *momentum);
77  G4QString(const G4QString &old, G4QParton* newdecay);
78  G4QString(G4QParton* newdecay, const G4LorentzVector* momentum);
79 
80  ~G4QString();
81 
82  // Selectors
83  G4int operator==(const G4QString &right) const {return this == &right;}
84  G4int operator!=(const G4QString &right) const {return this != &right;}
85  const G4ThreeVector& GetPosition() const {return thePosition;}
86  const G4QPartonVector* GetPartonList() const {return &thePartons;}
87  G4QParton* GetLeftParton() const {return *thePartons.begin();}
88  G4QParton* GetRightParton() const {return *(thePartons.end()-1);}
89  G4int GetDirection() const {return theDirection;}
92  G4int GetCharge() const {return GetQC().GetCharge();}
94  G4int GetStrangeness() const {return GetQC().GetStrangeness();}
95  G4int GetDecayDirection() const;
96  G4bool DecayIsQuark() const {return theDecayParton->GetType()==1;}
97  G4bool StableIsQuark() const {return theStableParton->GetType()==1;}
98  G4ThreeVector DecayPt(); // Get Pt of the decaying quark @@ Called once
99  G4double Mass2() const { return Pplus*Pminus-(Ptleft+Ptright).mag2();}
100  G4double Mass() const // @@ Very dangerous! USE ONLY FORE THE LIGHT CONE ALGORITHM !!
101  {
102  G4double mass2=Mass2();
103  if(mass2>0) return std::sqrt(Mass2());
104  else return 0.; // @@ Make Warning
105  }
107  {
108  G4LorentzVector mom(Ptleft+Ptright, 0.5*(Pplus+Pminus));
109  mom.setPz(0.5*(Pplus-Pminus));
110  return FragmentationMass(1) + MassCut > mom.mag();
111  }
112  G4bool IsFragmentable() {return FragmentationMass() + MassCut < Mass();} // @@ Mass() ?
113  G4ThreeVector SampleQuarkPt(); // @@ Called once
114  G4QHadron* CreateHadron(G4QParton* black, G4QParton* white);
117 
118  // Modifiers
119  void SetPosition(const G4ThreeVector& aPosition){thePosition= aPosition;}
120  void SetDirection(G4int dir) {if(dir==1 || dir==-1) theDirection=dir;}
121  void SetLeftParton(G4QParton* LP) {thePartons[0]=LP;} // !! Not deleting the substituty
122  void SetRightParton(G4QParton* RP) {thePartons.pop_back(); thePartons.push_back(RP);}
123  void KillString() {theDirection=0;} // @@ Can be absolete
124  void LorentzRotate(const G4LorentzRotation& rotation);
125  //void InsertParton(G4QParton* aParton, const G4QParton* addafter = NULL);
126  void Boost(G4ThreeVector& Velocity);
127  G4LorentzRotation TransformToAlignedCms(); // @@ caled once
128  //void DiffString(G4QHadron* aHadron, G4bool isProjectile); @@ Mast be used!!
129  void ExciteString(G4QParton* Col,G4QParton* AntiCol, G4int Dir);
130  G4QHadronVector* FragmentString(G4bool QL); // Fragment String using QGSM=true/LUND=false
132  G4double FragmentationMass(G4int HighSpin = 0, G4QHadronPair* pdefs = 0);
133  void SetLeftPartonStable();
134  void SetRightPartonStable();
135  G4QHadron* Splitup(G4bool QL);
136  G4LorentzVector* SplitEandP(G4QHadron* pHadron, G4bool QL); // QGSM:QL=true,Lund:QL=false
137  G4QPartonPair CreatePartonPair(G4int NeedParticle, G4bool AllowDiquarks=true);
138  G4QHadron* QuarkSplitup(G4QParton* decay, G4QParton* &created);
139  G4QHadron* DiQuarkSplitup(G4QParton* decay, G4QParton* &created);
140  G4int SampleQuarkFlavor() {return (1+G4int(G4UniformRand()/StrangeSuppress));} // ? M.K.
141 
142  // Static functions
143  static void SetParameters(G4double mCut, G4double sigQT, G4double DQSup, G4double DQBU,
144  G4double smPar, G4double SSup, G4double SigPt);
145 
146  private:
147  enum Spin {SpinZero=1, SpinHalf=2, SpinOne=3, SpinThreeHalf=4};
148  // Private functions
149  G4QHadron* CreateMeson(G4QParton* black, G4QParton* white, Spin spin);
150  G4QHadron* CreateBaryon(G4QParton* black,G4QParton* white, Spin spin);
151  G4ThreeVector GaussianPt(G4double widthSquare, G4double maxPtSquare) const;
152  G4double GetLundLightConeZ(G4double zmin, G4double zmax, G4int PartonEncoding,
153  G4QHadron* pHadron, G4double Px, G4double Py);
154  G4double GetQGSMLightConeZ(G4double zmin, G4double zmax, G4int PartonEncoding,
155  G4QHadron* pHadron, G4double Px, G4double Py);
156 
157  // Static parameters
158  // Parameters of Longitudinal String Fragmentation
159  static G4double MassCut; // minimum mass cut for the string
160  static G4double SigmaQT; // quark transverse momentum distribution parameter
161  static G4double DiquarkSuppress; // is Diquark suppression parameter
162  static G4double DiquarkBreakProb; // is Diquark breaking probability
163  static G4double SmoothParam; // QGS model parameter
164  static G4double StrangeSuppress; // Strangeness suppression parameter
165  static G4double widthOfPtSquare; // width^2 of pt for string excitation
166 
167  // Body
168  G4int theDirection; // must be 1 (PROJECTILE) or -1 (TARGET), 0 - DEAD
169  G4ThreeVector thePosition; // Defined by the first quark position
170  G4QPartonVector thePartons; // Partons on the ends of the string @@ Use PartonPair
171  G4ThreeVector Ptleft,Ptright; // Pt (px,py) for partons (pz ignored!)
172  G4double Pplus, Pminus; // p-, p+ of string, Plus is assigned to Left!
173  G4QParton* theStableParton; // Parton on the stable side of the string
174  G4QParton* theDecayParton; // Parton on the decaying part of the string
175  enum DecaySide {None, Left, Right};// @@ To have two @@ Leav : 1=Left
176  DecaySide decaying; // @@ it's too much @@ only : 0=Unknown
177  G4int SideOfDecay; // @@ of a good thing @@ one! : -1=Right
178 };
179 
180 #endif