| 1 | //
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| 2 | // ********************************************************************
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| 3 | // * DISCLAIMER *
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| 4 | // * *
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| 5 | // * The following disclaimer summarizes all the specific disclaimers *
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| 6 | // * of contributors to this software. The specific disclaimers,which *
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| 7 | // * govern, are listed with their locations in: *
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| 8 | // * http://cern.ch/geant4/license *
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| 9 | // * *
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| 10 | // * Neither the authors of this software system, nor their employing *
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| 11 | // * institutes,nor the agencies providing financial support for this *
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| 12 | // * work make any representation or warranty, express or implied, *
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| 13 | // * regarding this software system or assume any liability for its *
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| 14 | // * use. *
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| 15 | // * *
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| 16 | // * This code implementation is the intellectual property of the *
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| 17 | // * GEANT4 collaboration. *
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| 18 | // * By copying, distributing or modifying the Program (or any work *
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| 19 | // * based on the Program) you indicate your acceptance of this *
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| 20 | // * statement, and all its terms. *
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| 21 | // ********************************************************************
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| 22 | //
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| 23 | #include "G4NuclearShellModelDensity.hh"
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| 24 | #include "G4NuclearFermiDensity.hh"
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| 25 | #include "G4FermiMomentum.hh"
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| 26 |
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| 27 | #include "G4NucleiProperties.hh"
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| 28 | #include "G4ParticleTable.hh"
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| 29 | #include "G4IonTable.hh"
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| 30 | #include "globals.hh"
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| 31 | #include "G4Fancy3DNucleus.hh"
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| 32 | #include "G4KineticTrackVectorSTL.hh"
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| 33 | #include "G4ThreeVector.hh"
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| 34 | #include "G4LorentzVector.hh"
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| 35 |
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| 36 | G4V3DNucleus * the3DNucleus;
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| 37 | G4KineticTrackVectorSTL theTargetList;
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| 38 |
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| 39 | void BuildTargetList();
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| 40 | G4ThreeVector GetSpherePoint(G4double r);
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| 41 |
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| 42 | int main(int argc, char ** argv)
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| 43 | {
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| 44 | G4int A, Z, nEvents;
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| 45 |
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| 46 | if(argc != 4)
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| 47 | {
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| 48 | cout << "Input A and Z: ";
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| 49 | cin >> A >> Z;
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| 50 | cout << "Input number of events: ";
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| 51 | cin >> nEvents;
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| 52 | }
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| 53 | else
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| 54 | {
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| 55 | A = atoi(argv[1]);
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| 56 | Z = atoi(argv[2]);
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| 57 | nEvents = atoi(argv[3]);
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| 58 | }
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| 59 |
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| 60 | G4KineticTrackVectorSTL::iterator iter;
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| 61 | for(G4int i = 0; i < nEvents; ++i)
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| 62 | {
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| 63 | // create the nucleus
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| 64 | the3DNucleus = new G4Fancy3DNucleus;
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| 65 | the3DNucleus->Init(A, Z);
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| 66 | // create theTargetList
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| 67 | BuildTargetList();
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| 68 | G4LorentzVector totalMom(0, 0, 0, 0);
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| 69 | for(iter = theTargetList.begin(); iter != theTargetList.end(); ++iter)
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| 70 | {
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| 71 | G4ThreeVector pos = (1/fermi)*(*iter)->GetPosition();
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| 72 | G4LorentzVector mom = (1/MeV)*(*iter)->Get4Momentum();
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| 73 | totalMom+=mom;
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| 74 | cout << pos.x() << " " << pos.y() << " " << pos.z() << " "
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| 75 | << pos.mag() << " " << mom.x() << " " << mom.y() << " "
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| 76 | << mom.z() << " " << mom.t() << " " << mom.vect().mag()
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| 77 | << " " << mom.mag() << endl;
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| 78 | }
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| 79 | cerr << totalMom.x() << " " << totalMom.y() << " "
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| 80 | << totalMom.z() << " " << totalMom.t() << " "
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| 81 | << totalMom.vect().mag() << " " << totalMom.mag() << " "
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| 82 | << (1/MeV) * G4ParticleTable::GetParticleTable()->GetIonTable()->GetIonMass(Z, A)
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| 83 | << endl;
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| 84 | }
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| 85 | return 0;
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| 86 | }
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| 87 |
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| 88 | void BuildTargetList()
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| 89 | {
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| 90 | G4KineticTrackVectorSTL::iterator iter;
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| 91 | for(iter = theTargetList.begin(); iter != theTargetList.end(); ++iter)
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| 92 | delete (*iter);
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| 93 |
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| 94 | theTargetList.clear();
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| 95 |
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| 96 | if(!the3DNucleus->StartLoop())
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| 97 | {
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| 98 | G4cerr << "G4HadronKineticModel::BuildTargetList(): StartLoop() error!"
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| 99 | << G4endl;
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| 100 | return;
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| 101 | }
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| 102 | G4Nucleon * nucleon;
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| 103 | G4ParticleDefinition * definition;
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| 104 | G4ThreeVector pos;
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| 105 | G4LorentzVector mom;
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| 106 | while((nucleon = the3DNucleus->GetNextNucleon()) != NULL)
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| 107 | {
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| 108 | definition = nucleon->GetDefinition();
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| 109 | pos = nucleon->GetPosition();
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| 110 | mom = nucleon->GetMomentum();
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| 111 | G4KineticTrack * kt = new G4KineticTrack(definition, 0., pos, mom);
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| 112 | theTargetList.push_back(kt);
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| 113 | }
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| 114 | }
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| 115 |
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| 116 |
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| 117 |
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| 118 |
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| 119 |
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| 120 |
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