// // ******************************************************************** // * 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. * // ******************************************************************** // // $Id$ // // ---------------- G4QDiffraction header ---------------- // by Mikhail Kossov, Aug 2007. // Header of G4QDiffraction class (hadron+A) of the CHIPS Simulation Branch in GEANT4 // ------------------------------------------------------------------------------- // This is a unique CHIPS class for the Hadron-Nuclear Diffractive Interaction Prosesses // ------------------------------------------------------------------------------- // At present (Aug-07) it is based on the G4QDiffractionRatio class and is not tested. // The normalization is based on the temporary G4QProtonNuclearCrossSection class // ------------------------------------------------------------------------------- // Short description: This is a process, which describes the diffraction // excitation of the projectile and the nucleus. On nuclei in addition there // can be a coherent diffraction process for the projectile, but it is // comparably small. The most important part of the diffraction is the // progectile diffraction excitation, as in this interaction proton can lose // only a small part of its energy and make the shower longer. This is because // only 1-2 (n) pions are produce in the diffraction escitation, and the mean // kept energy of the nucleon is (1-n/7)=80%. For kaons the kept energy is much // smaller (1-n/3.5)=60%, and for pions it is less important (about 40%). // ---------------------------------------------------------------------------- #ifndef G4QDiffraction_hh #define G4QDiffraction_hh // GEANT4 Headers #include "globals.hh" #include "G4ios.hh" #include "Randomize.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" // CHIPS Headers #include "G4QDiffractionRatio.hh" #include "G4QProtonNuclearCrossSection.hh" #include "G4QIsotope.hh" #include "G4QCHIPSWorld.hh" #include "G4QHadronVector.hh" #include class G4QDiffraction : public G4VDiscreteProcess { public: // Constructor G4QDiffraction(const G4String& processName ="CHIPS_DiffractiveInteraction"); // Destructor ~G4QDiffraction(); 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. G4LorentzVector GetEnegryMomentumConservation(); G4int GetNumberOfNeutronsInTarget(); private: // Hide assignment operator as private G4QDiffraction& operator=(const G4QDiffraction &right); // Copy constructor G4QDiffraction(const G4QDiffraction&); // Calculate Cross-Section of the Diffraction Reaction (p is in GeV @@ units) G4double CalculateXS(G4double p, G4int Z, G4int N, G4int pPDG); // BODY // Static Parameters -------------------------------------------------------------------- static G4int nPartCWorld; // The#of particles for hadronization (limit of A of fragm.) //--------------------------------- 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 ElementZ; // Z of the element(i) in theLastCalc static std::vector ElProbInMat; // SumProbabilityElements in Material static std::vector *> ElIsoN; // N of isotope(j) of Element(i) static std::vector *> IsoProbInEl;// SumProbabIsotopes in Element i }; #endif