| 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 | // 05-11-21 NeutronHP or Low Energy Parameterization Models
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| 28 | // Implemented by T. Koi (SLAC/SCCS)
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| 29 | // If NeutronHP data do not available for an element, then Low Energy
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| 30 | // Parameterization models handle the interactions of the element.
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| 31 | // 080319 Compilation warnings - gcc-4.3.0 fix by T. Koi
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| 32 | //
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| 33 |
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| 34 | // neutron_hp -- source file
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| 35 | // J.P. Wellisch, Nov-1996
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| 36 | // A prototype of the low energy neutron transport model.
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| 37 | //
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| 38 | #include "G4NeutronHPorLFission.hh"
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| 39 | #include "G4NeutronHPFissionFS.hh"
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| 40 |
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| 41 | G4NeutronHPorLFission::G4NeutronHPorLFission()
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| 42 | :G4HadronicInteraction("NeutronHPorLFission")
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| 43 | {
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| 44 | SetMinEnergy(0.*eV);
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| 45 | SetMaxEnergy(20.*MeV);
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| 46 |
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| 47 | if( !getenv("G4NEUTRONHPDATA") )
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| 48 | throw G4HadronicException(__FILE__, __LINE__, "Please setenv G4NEUTRONHPDATA to point to the neutron cross-section files.");
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| 49 |
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| 50 | dirName = getenv("G4NEUTRONHPDATA");
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| 51 | G4String tString = "/Fission/";
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| 52 | dirName = dirName + tString;
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| 53 | // G4cout <<"G4NeutronHPorLFission::G4NeutronHPorLFission testit "<<dirName<<G4endl;
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| 54 | unavailable_elements.clear();
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| 55 |
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| 56 | numEle = G4Element::GetNumberOfElements();
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| 57 | theFission = new G4NeutronHPChannel[numEle];
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| 58 |
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| 59 | for ( G4int i = 0; i < numEle ; i++)
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| 60 | {
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| 61 | if ( (*(G4Element::GetElementTable()))[i]-> GetZ() > 89 )
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| 62 | {
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| 63 | theFission[i].Init((*(G4Element::GetElementTable()))[i], dirName);
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| 64 | try { while(!theFission[i].Register(&theFS)) ; }
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| 65 | catch ( G4HadronicException )
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| 66 | {
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| 67 | unavailable_elements.insert ( (*(G4Element::GetElementTable()))[i]->GetName() );
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| 68 | }
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| 69 | }
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| 70 | }
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| 71 |
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| 72 | if ( unavailable_elements.size() > 0 )
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| 73 | {
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| 74 | std::set< G4String>::iterator it;
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| 75 | G4cout << "HP Fission data are not available for thess elements "<< G4endl;
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| 76 | for ( it = unavailable_elements.begin() ; it != unavailable_elements.end() ; it++ )
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| 77 | {
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| 78 | G4cout << *it << G4endl;
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| 79 | }
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| 80 | G4cout << "Low Energy Parameterization Models will be used."<< G4endl;
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| 81 | }
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| 82 |
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| 83 | createXSectionDataSet();
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| 84 | }
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| 85 |
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| 86 | G4NeutronHPorLFission::~G4NeutronHPorLFission()
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| 87 | {
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| 88 | delete [] theFission;
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| 89 | delete theDataSet;
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| 90 | }
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| 91 |
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| 92 | #include "G4NeutronHPThermalBoost.hh"
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| 93 |
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| 94 | G4HadFinalState * G4NeutronHPorLFission::ApplyYourself(const G4HadProjectile& aTrack, G4Nucleus& )
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| 95 | {
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| 96 | const G4Material * theMaterial = aTrack.GetMaterial();
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| 97 | G4int n = theMaterial->GetNumberOfElements();
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| 98 | G4int index = theMaterial->GetElement(0)->GetIndex();
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| 99 | if(n!=1)
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| 100 | {
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| 101 | G4int i;
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| 102 | xSec = new G4double[n];
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| 103 | G4double sum=0;
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| 104 | const G4double * NumAtomsPerVolume = theMaterial->GetVecNbOfAtomsPerVolume();
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| 105 | G4double rWeight;
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| 106 | G4NeutronHPThermalBoost aThermalE;
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| 107 | for (i=0; i<n; i++)
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| 108 | {
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| 109 | index = theMaterial->GetElement(i)->GetIndex();
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| 110 | rWeight = NumAtomsPerVolume[i];
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| 111 | G4double x = aThermalE.GetThermalEnergy(aTrack, theMaterial->GetElement(i), theMaterial->GetTemperature());
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| 112 |
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| 113 | //xSec[i] = theFission[index].GetXsec(aThermalE.GetThermalEnergy(aTrack,
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| 114 | // theMaterial->GetElement(i),
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| 115 | // theMaterial->GetTemperature()));
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| 116 | xSec[i] = theFission[index].GetXsec(x);
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| 117 |
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| 118 | xSec[i] *= rWeight;
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| 119 | sum+=xSec[i];
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| 120 | }
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| 121 | G4double random = G4UniformRand();
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| 122 | G4double running = 0;
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| 123 | for (i=0; i<n; i++)
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| 124 | {
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| 125 | running += xSec[i];
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| 126 | index = theMaterial->GetElement(i)->GetIndex();
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| 127 | if(random<=running/sum) break;
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| 128 | }
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| 129 | delete [] xSec;
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| 130 | // it is element-wise initialised.
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| 131 | }
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| 132 | return theFission[index].ApplyYourself(aTrack);
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| 133 | }
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| 134 |
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| 135 |
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| 136 |
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| 137 | G4bool G4NeutronHPorLFission::IsThisElementOK( G4String name )
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| 138 | {
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| 139 | if ( unavailable_elements.find( name ) == unavailable_elements.end() )
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| 140 | return TRUE;
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| 141 | else
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| 142 | return FALSE;
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| 143 | }
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| 144 |
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| 145 |
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| 146 |
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| 147 | void G4NeutronHPorLFission::createXSectionDataSet()
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| 148 | {
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| 149 | theDataSet = new G4NeutronHPorLFissionData ( theFission , &unavailable_elements );
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| 150 | }
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