G4QInelastic.hh

Go to the documentation of this file.

//
// ********************************************************************
// * 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.          *
// ********************************************************************
//
// $Id$
//
//      ---------------- G4QInelastic header ----------------
//                 by Mikhail Kossov, December 2003.
//  Header of G4QInelastic class (all particles) of the CHIPS Physics Pachage in GEANT4
// ------------------------------------------------------------------------------------
// This is a unique CHIPS class for the Hadron-Nuclear Inelastic Interaction Prosesses.
// ------------------------------------------------------------------------------------
// At present (Dec.04) only pi+/-, K+/- proton, neutron, antiproton and antineutron
// collisions with protons are implemented, which are fundamental for the in matter
// simulation of hadronic reactions. The interactions of the same particles with
// nuclei are implemented only for the low energy (below 1 GeV) nucleon-nuclear
// reactions only. The collisions of nuclei with nuclei are planned for the near future.
// The simulation is based on the G4QuasmonString class, which extends the CHIPS model
// to the highest energyes, implementing the Quasmon string with the
// String->Quasmons->Hadrons scenario of the quark-gluon string fragmentation
// --> CHIPS is a SU(3) event generator, so it does not include reactions with the
// heavy c,b,t-quarks, which can be simulated only by the SU(6) QUIPS (QUark Invariant
// Phase Space) model which is an expantion of the CHIPS.- May 2009, M.Kossov.-
// --------------------------------------------------------------------------------------
// Algorithms: the vacuum interactions in CHIPS are described by the quark exchange (QE)
// process. The first step is the low energy quark exchange. If as a result of the QE one
// or both secondary hadrons are below the pi0 threshold (roughly) they are pushed to the
// Ground State (GS) value(s). The excited (above the pi0 production threshold) hadronic
// state is considered as a Quasmon, which is filled in the G4QuasmonVector of the
// G4QuasmonString class. On the second step all G4Quasmons are decayed by the
// G4Quasmon class and fill the G4QHadronVector output. If the exchange quark is too far
// in the rapidity space (a parameter of the G4QuasmonString class) from any of the quarks
// of the other hadron it creates a string with the nearest in the rapidity space quark.
// This string is converted into a Quasmon. This forces the coalescence of the residuals
// to create another Quasmon, while the possibility exists to create more residual
// Quasmons instead of one - one per each target-quark+projectile-antiquark(diquark) pair.
// This possibility is tuned by the Drell-Yan pair production process. If the target (or
// pojectile) is a nucleus, then the Quasmons are created not only in vacuum, where they
// can be fragmented by the G4Quasmon class, but in nuclear matter of the residual target
// (or projectile). If the Quasmons are created in nuclear matter, they are fragmented by
// the G4QEnvironment class with the subsequent Quark Exchange nuclear fragmentation.
// This is the present general scenario.- May 2009, Mikhail Kossov.-
// --------------------------------------------------------------------------------
// ****************************************************************************************
// This Header is a part of the CHIPS Physics Package (author: M. Kosov)
// ****************************************************************************************
// Short description: This is a universal class for the incoherent (inelastic)
// nuclear interactions within the framework of the CHIPS model.
// ---------------------------------------------------------------------------
 
#ifndef G4QInelastic_hh
#define G4QInelastic_hh
 
// GEANT4 Headers
#include "globals.hh"
#include "G4ios.hh"
#include "Randomize.hh" 
#include "G4QThd.hh"
#include "G4VDiscreteProcess.hh"
#include "G4Track.hh"
#include "G4Step.hh"
#include "G4ParticleTypes.hh"
#include "G4VParticleChange.hh"
#include "G4ParticleDefinition.hh"
#include "G4DynamicParticle.hh"
#include "G4ThreeVector.hh"
#include "G4LorentzVector.hh"
#include "G4RandomDirection.hh"
 
// CHIPS Headers
#include "G4QEnvironment.hh"
#include "G4VQCrossSection.hh"
#include "G4QIsotope.hh"
#include "G4QProtonNuclearCrossSection.hh"
#include "G4QPionMinusNuclearCrossSection.hh"
#include "G4QPionPlusNuclearCrossSection.hh"
#include "G4QKaonPlusNuclearCrossSection.hh"
#include "G4QKaonMinusNuclearCrossSection.hh"
#include "G4QKaonZeroNuclearCrossSection.hh"
#include "G4QHyperonNuclearCrossSection.hh"
#include "G4QHyperonPlusNuclearCrossSection.hh"
#include "G4QAntiBaryonPlusNuclearCrossSection.hh"
#include "G4QAntiBaryonNuclearCrossSection.hh"
#include "G4QPhotonNuclearCrossSection.hh"
#include "G4QElectronNuclearCrossSection.hh"
#include "G4QMuonNuclearCrossSection.hh"
#include "G4QTauNuclearCrossSection.hh"
#include "G4QNuMuNuclearCrossSection.hh"
#include "G4QANuMuNuclearCrossSection.hh"
#include "G4QNuENuclearCrossSection.hh"
#include "G4QANuENuclearCrossSection.hh"
#include "G4QNuNuNuclearCrossSection.hh"
#include "G4QANuANuNuclearCrossSection.hh"
#include "G4QNeutronNuclearCrossSection.hh"
#include "G4QNeutronCaptureRatio.hh"
#include "G4QIonIonCollision.hh"
#include "G4QFragmentation.hh"
#include "G4QuasiFreeRatios.hh"
#include "G4QPDGToG4Particle.hh"
 
class G4QInelastic : public G4VDiscreteProcess
{
public:
 
  // Constructor
  G4QInelastic(const G4String& processName ="CHIPS_Inelastic");
 
  // Destructor
  ~G4QInelastic();
 
  G4bool IsApplicable(const G4ParticleDefinition& particle);
 
  G4double GetMeanFreePath(const G4Track& aTrack, G4double previousStepSize,
                           G4ForceCondition* condition);
  // It returns the MeanFreePath of the process for the current track :
  // (energy, material)
  // The previousStepSize and G4ForceCondition* are not used.
  // This function overloads a virtual function of the base class.        
  // It is invoked by the ProcessManager of the Particle.
 
 
  G4VParticleChange* PostStepDoIt(const G4Track& aTrack, const G4Step& aStep); 
  // It computes the final state of the process (at end of step),
  // returned as a ParticleChange object.       
  // This function overloads a virtual function of the base class.
  // It is invoked by the ProcessManager of the Particle.
 
  // Fake void functions
  void SetPhysicsTableBining(G4double, G4double, G4int) {;}
  void BuildPhysicsTable(const G4ParticleDefinition&) {;}
  void PrintInfoDefinition() {;}
 
  // Internal Energy-Momentum Residual
  G4LorentzVector GetEnegryMomentumConservation();
 
  // Number of neutrons in the target nucleus (primary)
  G4int GetNumberOfNeutronsInTarget();
 
  // Static functions ---------------------------------------------------------------------
  static void SetManual();
  static void SetStandard();
  static void SetParameters(G4double temper=180., G4double ssin2g=.1, G4double etaetap=.3,
                            G4double fN=0., G4double fD=0., G4double cP=1., G4double mR=1.,
                            G4int npCHIPSWorld=234, G4double solAn=.5, G4bool efFlag=false,
                            G4double piTh=141.4,G4double mpi2=20000.,G4double dinum=1880.);
  static void SetPhotNucBias(G4double phnB=1.);
  static void SetWeakNucBias(G4double ccnB=1.);
  //--- End of static member functions ----------------------------------------------------
 
  G4double GetPhotNucBias(){return photNucBias;}
  G4double GetWeakNucBias(){return weakNucBias;}
 
private:
 
  // Hide assignment operator as private 
  G4QInelastic& operator=(const G4QInelastic &right);
 
  // Copy constructor
  G4QInelastic(const G4QInelastic&);
 
  // Random direction in two dimentions pair(first=sin(phi), second=cos(phi))
  std::pair<G4double,G4double> Random2DDirection();
 
  // BODY
  // Static Parameters --------------------------------------------------------------------
  static G4bool   manualFlag;  // If false then standard parameters are used
  static G4int    nPartCWorld; // The#of particles for hadronization (limit of A of fragm.)
  // -> Parameters of the G4Quasmon class:
  static G4double Temperature; // Quasmon Temperature
  static G4double SSin2Gluons; // Percent of ssbar sea in a constituen gluon
  static G4double EtaEtaprime; // Part of eta-prime in all etas
  // -> Parameters of the G4QNucleus class:
  static G4double freeNuc;     // probability of the quasi-free baryon on surface
  static G4double freeDib;     // probability of the quasi-free dibaryon on surface
  static G4double clustProb;   // clusterization probability in dense region
  static G4double mediRatio;   // relative vacuum hadronization probability
  // -> Parameters of the G4QEnvironment class:
  static G4bool   EnergyFlux;  // Flag for Energy Flux use instead of Multy Quasmon
  static G4double SolidAngle;  // Part of Solid Angle to capture secondaries(@@A-dep)
  static G4double PiPrThresh;  // Pion Production Threshold for gammas
  static G4double M2ShiftVir;  // Shift for M2=-Q2=m_pi^2 of the virtual gamma
  static G4double DiNuclMass;  // Double Nucleon Mass for virtual normalization
  // -> Biasing parameters:
  static G4double photNucBias; // Biasing parameter for photo-($e,mu,tau)Nuclear reactions
  static G4double weakNucBias; // Biasing parameter for Charged Currents (nu,mu) reactions
  //--------------------------------- End of static parameters ---------------------------
  // Working parameters
  G4VQCrossSection* theCS;
  G4LorentzVector EnMomConservation;                  // Residual of Energy/Momentum Cons.
  G4int nOfNeutrons;                                  // #of neutrons in the target nucleus
 
  // Modifires for the reaction
  G4double Time;                                      // Time shift of the capture reaction
  G4double EnergyDeposition;                          // Energy deposited in the reaction
  static std::vector <G4int> ElementZ;                // Z of the element(i) in theLastCalc
  static std::vector <G4double> ElProbInMat;          // SumProbabilityElements in Material
  static std::vector <std::vector<G4int>*> ElIsoN;    // N of isotope(j) of Element(i)
  static std::vector <std::vector<G4double>*> IsoProbInEl;// SumProbabIsotopes in Element i
};
#endif