// // ******************************************************************** // * 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. * // ******************************************************************** // // $Id$ // //--------------------------------------------------------------------------- // // ClassName: HadronPhysicsQGSC_CHIPS // // Author: 2009 M. Kosov // // Modified: // //---------------------------------------------------------------------------- // Short description: In fact this is the definition of the Hadronic Inelastic // physics. The definition of the Hadronic Elastic physics one can find in the // G4HadronQElasticPhysics, which is stable (the same for all physics lists). // The only "unstable" part of the physics is the Hadronic Inelastic physics, // which is usually composed of the wixing of the High Energy Inelastic Model // (HEIM) and the Low Energy Inelastic Model (LEIM), which are applied only for // some hadrons (mostly nucleons and pi-mesons), above the LHEP model, which // usually covers all particles (but for Sigma_0 ?) and sometimes covers the // "hole" between the LEIM and HIME at intermediate energies. The name of the // Physics list is usually have a form HEIM_LEIM and the inelastic interactions // are defined in the HadronicPhysicsHEIM_LEIM class. So in this particular // physics list the low energy model is CHIPS (G4QCollision process) and the // high energy model is QGSC (QGS with the Energy Flow interface to CHIPS), // which are in terms of the energy boundary are mixed not on the model level, // but on the process level (G4DiscProcessMixer class). The LHEP is completely // excluded from this physics list, because the MiscLHEP is substituted by the // MiscQGSC class (QGS with the Energy Flow interface to CHIPS), covering all // particles, which are not N, pi, or K, defined by the separate builders. //--------------------------------------------------------------------------- #ifndef HadronPhysicsQGSC_CHIPS_h #define HadronPhysicsQGSC_CHIPS_h 1 #include "globals.hh" #include "G4ios.hh" #include "G4VPhysicsConstructor.hh" #include "G4MiscQGSCBuilder.hh" #include "G4PiKBuilder.hh" #include "G4QGSC_CHIPSPiKBuilder.hh" #include "G4QProtonBuilder.hh" #include "G4QGSC_CHIPSProtonBuilder.hh" #include "G4QNeutronBuilder.hh" #include "G4QGSC_CHIPSNeutronBuilder.hh" class HadronPhysicsQGSC_CHIPS : public G4VPhysicsConstructor { public: HadronPhysicsQGSC_CHIPS(G4int verbose =1); HadronPhysicsQGSC_CHIPS(const G4String& name, G4bool quasiElastic=true); virtual ~HadronPhysicsQGSC_CHIPS(); public: virtual void ConstructParticle(); virtual void ConstructProcess(); private: void CreateModels(); G4QNeutronBuilder* theNeut; G4QGSC_CHIPSNeutronBuilder* theQGSCNeut; G4PiKBuilder* thePiK; G4QGSC_CHIPSPiKBuilder* theQGSCPiK; G4QProtonBuilder* theProt; G4QGSC_CHIPSProtonBuilder * theQGSCProt; G4MiscQGSCBuilder* theMiscQGSC; G4bool QuasiElastic; }; #endif