| 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 | // This is the top level Hadronic Process class
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| 29 | // The inelastic, elastic, capture, and fission processes
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| 30 | // should derive from this class
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| 31 | //
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| 32 | // original by H.P.Wellisch
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| 33 | // J.L. Chuma, TRIUMF, 10-Mar-1997
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| 34 | // Last modified: 04-Apr-1997
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| 35 | // 19-May-2008 V.Ivanchenko cleanup and added comments
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| 36 |
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| 37 | #ifndef G4HadronicProcess_h
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| 38 | #define G4HadronicProcess_h 1
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| 39 |
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| 40 | #include "globals.hh"
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| 41 | #include "G4VDiscreteProcess.hh"
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| 42 | #include "G4EnergyRangeManager.hh"
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| 43 | #include "G4Nucleus.hh"
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| 44 | #include "G4ReactionProduct.hh"
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| 45 | #include <vector>
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| 46 | #include "G4VIsotopeProduction.hh"
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| 47 | #include "G4IsoParticleChange.hh"
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| 48 | #include "G4VCrossSectionDataSet.hh"
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| 49 | #include "G4VLeadingParticleBiasing.hh"
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| 50 | //#include "G4Delete.hh"
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| 51 | #include "G4CrossSectionDataStore.hh"
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| 52 | #include "G4HadronicProcessType.hh"
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| 53 |
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| 54 | class G4Track;
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| 55 | class G4Step;
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| 56 | class G4Element;
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| 57 | class G4ParticleChange;
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| 58 |
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| 59 | class G4HadronicProcess : public G4VDiscreteProcess
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| 60 | {
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| 61 | public:
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| 62 |
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| 63 | G4HadronicProcess( const G4String &processName = "Hadronic",
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| 64 | G4ProcessType aType = fHadronic );
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| 65 |
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| 66 | virtual ~G4HadronicProcess();
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| 67 |
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| 68 | // register generator of secondaries
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| 69 | void RegisterMe( G4HadronicInteraction *a );
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| 70 |
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| 71 | // get cross section per element
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| 72 | virtual
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| 73 | G4double GetMicroscopicCrossSection(const G4DynamicParticle *aParticle,
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| 74 | const G4Element *anElement,
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| 75 | G4double aTemp );
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| 76 |
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| 77 | // generic PostStepDoIt recommended for all derived classes
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| 78 | virtual G4VParticleChange* PostStepDoIt(const G4Track& aTrack,
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| 79 | const G4Step& aStep);
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| 80 |
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| 81 | // initialisation of physics tables and G4HadronicProcessStore
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| 82 | virtual void PreparePhysicsTable(const G4ParticleDefinition&);
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| 83 |
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| 84 | // build physics tables and print out the configuration of the process
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| 85 | virtual void BuildPhysicsTable(const G4ParticleDefinition&);
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| 86 |
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| 87 | // dump physics tables
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| 88 | inline void DumpPhysicsTable(const G4ParticleDefinition& p)
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| 89 | { theCrossSectionDataStore->DumpPhysicsTable(p); }
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| 90 |
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| 91 | // add cross section data set
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| 92 | inline void AddDataSet(G4VCrossSectionDataSet * aDataSet)
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| 93 | { theCrossSectionDataStore->AddDataSet(aDataSet);}
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| 94 |
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| 95 | // access to the manager
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| 96 | inline G4EnergyRangeManager *GetManagerPointer()
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| 97 | { return &theEnergyRangeManager; }
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| 98 |
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| 99 | // get inverse cross section per volume
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| 100 | G4double GetMeanFreePath(const G4Track &aTrack, G4double,
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| 101 | G4ForceCondition *);
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| 102 |
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| 103 | protected:
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| 104 |
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| 105 | // reset number of interaction length and save
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| 106 | virtual void ResetNumberOfInteractionLengthLeft()
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| 107 | { G4VProcess::ResetNumberOfInteractionLengthLeft();
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| 108 | theInitialNumberOfInteractionLength =
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| 109 | G4VProcess::theNumberOfInteractionLengthLeft;
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| 110 | }
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| 111 |
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| 112 | // generic method to choose secondary generator
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| 113 | // recommended for all derived classes
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| 114 | inline G4HadronicInteraction *ChooseHadronicInteraction(
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| 115 | G4double kineticEnergy, G4Material *aMaterial, G4Element *anElement )
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| 116 | { return theEnergyRangeManager.GetHadronicInteraction(kineticEnergy,
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| 117 | aMaterial,anElement);
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| 118 | }
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| 119 |
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| 120 | public:
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| 121 |
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| 122 | // Methods for isotope production
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| 123 | static void EnableIsotopeProductionGlobally();
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| 124 | static void DisableIsotopeProductionGlobally();
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| 125 |
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| 126 | void EnableIsotopeCounting() {isoIsOnAnyway = 1;}
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| 127 | void DisableIsotopeCounting() {isoIsOnAnyway = -1;}
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| 128 |
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| 129 | void RegisterIsotopeProductionModel(G4VIsotopeProduction * aModel)
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| 130 | { theProductionModels.push_back(aModel); }
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| 131 |
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| 132 | static G4IsoParticleChange * GetIsotopeProductionInfo();
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| 133 |
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| 134 | void BiasCrossSectionByFactor(G4double aScale);
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| 135 |
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| 136 | protected:
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| 137 |
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| 138 | // obsolete method will be removed
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| 139 | inline const G4EnergyRangeManager &GetEnergyRangeManager() const
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| 140 | { return theEnergyRangeManager; }
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| 141 |
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| 142 | // obsolete method will be removed
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| 143 | inline void SetEnergyRangeManager( const G4EnergyRangeManager &value )
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| 144 | { theEnergyRangeManager = value; }
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| 145 |
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| 146 | // access to the chosen generator
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| 147 | inline G4HadronicInteraction *GetHadronicInteraction()
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| 148 | { return theInteraction; }
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| 149 |
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| 150 | // access to the cross section data store
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| 151 | inline G4CrossSectionDataStore* GetCrossSectionDataStore()
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| 152 | { return theCrossSectionDataStore; }
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| 153 |
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| 154 | // access to the cross section data set
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| 155 | inline G4double GetLastCrossSection()
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| 156 | { return theLastCrossSection; }
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| 157 |
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| 158 | private:
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| 159 |
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| 160 | void FillTotalResult(G4HadFinalState * aR, const G4Track & aT);
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| 161 |
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| 162 | G4HadFinalState * DoIsotopeCounting(G4HadFinalState * aResult,
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| 163 | const G4Track & aTrack,
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| 164 | const G4Nucleus & aNucleus);
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| 165 |
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| 166 | G4IsoResult * ExtractResidualNucleus(const G4Track & aTrack,
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| 167 | const G4Nucleus & aNucleus,
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| 168 | G4HadFinalState * aResult);
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| 169 |
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| 170 | inline G4double GetTotalNumberOfInteractionLengthTraversed()
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| 171 | { return theInitialNumberOfInteractionLength
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| 172 | -G4VProcess::theNumberOfInteractionLengthLeft;
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| 173 | }
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| 174 |
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| 175 | // inline void SetCrossSectionDataStore(G4CrossSectionDataStore* aDataStore)
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| 176 | // { theCrossSectionDataStore = aDataStore; }
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| 177 |
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| 178 | G4double XBiasSurvivalProbability();
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| 179 | G4double XBiasSecondaryWeight();
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| 180 |
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| 181 | private:
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| 182 |
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| 183 | G4EnergyRangeManager theEnergyRangeManager;
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| 184 |
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| 185 | G4HadronicInteraction *theInteraction;
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| 186 |
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| 187 | G4CrossSectionDataStore* theCrossSectionDataStore;
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| 188 |
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| 189 | G4Nucleus targetNucleus;
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| 190 |
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| 191 | G4HadronicProcess *dispatch;
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| 192 |
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| 193 | bool G4HadronicProcess_debug_flag;
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| 194 |
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| 195 | // swiches for isotope production
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| 196 | static G4bool isoIsEnabled; // true or false; local swich overrides
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| 197 | G4int isoIsOnAnyway; // true(1), false(-1) or default(0)
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| 198 |
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| 199 | G4IsoParticleChange theIsoPC;
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| 200 | std::vector<G4VIsotopeProduction *> theProductionModels;
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| 201 |
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| 202 | std::vector<G4VLeadingParticleBiasing *> theBias;
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| 203 |
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| 204 | static G4IsoParticleChange* theIsoResult;
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| 205 | static G4IsoParticleChange* theOldIsoResult;
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| 206 |
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| 207 | G4ParticleChange* theTotalResult;
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| 208 |
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| 209 | G4double theInitialNumberOfInteractionLength;
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| 210 |
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| 211 | G4double aScaleFactor;
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| 212 | G4bool xBiasOn;
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| 213 | G4double theLastCrossSection;
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| 214 |
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| 215 | G4int ModelingState;
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| 216 | };
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| 217 |
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| 218 | #endif
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| 219 |
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