[819] | 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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[1196] | 25 | // |
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[1055] | 26 | // !!! Was used in QBBC PL, NOW it is not. Must be absolete !!! |
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| 27 | // ============================================================ |
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[819] | 28 | |
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| 29 | //#define debug |
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| 30 | //#define pdebug |
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| 31 | |
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| 32 | #include "G4StringChipsInterface.hh" |
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| 33 | #include "globals.hh" |
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| 34 | #include <utility> |
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| 35 | #include <list> |
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| 36 | #include "G4KineticTrackVector.hh" |
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| 37 | #include "G4Nucleon.hh" |
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| 38 | #include "G4LorentzRotation.hh" |
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| 39 | |
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| 40 | G4StringChipsInterface::G4StringChipsInterface() |
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| 41 | { |
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| 42 | #ifdef CHIPSdebug |
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| 43 | G4cout << "Please enter the energy loss per fermi in GeV"<<G4endl; |
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| 44 | G4cin >> theEnergyLossPerFermi; |
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| 45 | #endif |
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| 46 | #ifdef debug |
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| 47 | G4cout<<"G4StringChipsInterface::Constructor is called"<<G4endl; |
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| 48 | #endif |
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| 49 | theEnergyLossPerFermi = 0.5*GeV; |
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| 50 | // theEnergyLossPerFermi = 1.*GeV; |
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| 51 | } |
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| 52 | |
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| 53 | G4HadFinalState* G4StringChipsInterface:: |
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| 54 | ApplyYourself(const G4HadProjectile& aTrack, G4Nucleus& theNucleus) |
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| 55 | { |
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| 56 | #ifdef debug |
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| 57 | G4cout<<"G4StringChipsInterface::ApplyYourself is called"<<G4endl; |
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| 58 | #endif |
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| 59 | return theModel.ApplyYourself(aTrack, theNucleus); |
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| 60 | } |
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| 61 | |
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| 62 | G4ReactionProductVector* G4StringChipsInterface:: |
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| 63 | Propagate(G4KineticTrackVector* theSecondaries, G4V3DNucleus* theNucleus) |
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| 64 | { |
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| 65 | #ifdef debug |
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| 66 | G4cout<<"G4StringChipsInterface::Propagate is called"<<G4endl; |
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| 67 | #endif |
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| 68 | // Protection for non physical conditions |
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| 69 | |
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| 70 | if(theSecondaries->size() == 1) |
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| 71 | throw G4HadronicException(__FILE__, __LINE__, "G4StringChipsInterface: Only one particle from String models!"); |
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| 72 | |
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| 73 | // Calculate the mean energy lost |
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| 74 | std::pair<G4double, G4double> theImpact = theNucleus->RefetchImpactXandY(); |
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| 75 | G4double impactX = theImpact.first; |
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| 76 | G4double impactY = theImpact.second; |
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| 77 | G4double inpactPar2 = impactX*impactX + impactY*impactY; |
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| 78 | |
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| 79 | G4double radius2 = theNucleus->GetNuclearRadius(5*perCent); |
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| 80 | radius2 *= radius2; |
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| 81 | G4double pathlength = 0; |
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| 82 | if(radius2 - inpactPar2>0) pathlength = 2.*std::sqrt(radius2 - inpactPar2); |
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| 83 | G4double theEnergyLostInFragmentation = theEnergyLossPerFermi*pathlength/fermi; |
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| 84 | |
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| 85 | // now select all particles in range |
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| 86 | std::list<std::pair<G4double, G4KineticTrack *> > theSorted; |
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| 87 | std::list<std::pair<G4double, G4KineticTrack *> >::iterator current; |
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| 88 | for(unsigned int secondary = 0; secondary<theSecondaries->size(); secondary++) |
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| 89 | { |
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| 90 | G4LorentzVector a4Mom = theSecondaries->operator[](secondary)->Get4Momentum(); |
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| 91 | |
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| 92 | #ifdef CHIPSdebug |
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| 93 | G4cout <<"ALL STRING particles "<<theSecondaries->operator[](secondary)->GetDefinition()->GetPDGCharge()<<" " |
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| 94 | << theSecondaries->operator[](secondary)->GetDefinition()->GetPDGEncoding()<<" " |
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| 95 | << a4Mom <<G4endl; |
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| 96 | #endif |
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| 97 | |
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| 98 | G4double toSort = a4Mom.rapidity(); |
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| 99 | std::pair<G4double, G4KineticTrack *> it; |
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| 100 | it.first = toSort; |
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| 101 | it.second = theSecondaries->operator[](secondary); |
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| 102 | G4bool inserted = false; |
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| 103 | for(current = theSorted.begin(); current!=theSorted.end(); current++) |
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| 104 | { |
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| 105 | if((*current).first > toSort) |
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| 106 | { |
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| 107 | theSorted.insert(current, it); |
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| 108 | inserted = true; |
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| 109 | break; |
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| 110 | } |
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| 111 | } |
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| 112 | if(!inserted) |
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| 113 | { |
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| 114 | theSorted.push_front(it); |
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| 115 | } |
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| 116 | } |
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| 117 | |
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| 118 | G4LorentzVector proj4Mom(0.,0.,0.,0.); |
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| 119 | // @@ Use the G4QContent class, which is exactly (nD,nU,nS,nAD,nAU,nAS) ! |
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| 120 | // The G4QContent class is a basic clas in CHIPS (not PDG Code as in GEANT4), |
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| 121 | // so in CHIPS on can has a hadronic obgect (Quasmon) with any Quark Content. |
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| 122 | // As a simple extantion for the hadron (which is a special case for Hadron) |
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| 123 | // there is a clas G4QChipolino, which is a Quasmon, which can decay in two |
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| 124 | // hadrons. In future the three-hadron class can be added... |
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| 125 | G4int nD = 0; |
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| 126 | G4int nU = 0; |
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| 127 | G4int nS = 0; |
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| 128 | G4int nAD = 0; |
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| 129 | G4int nAU = 0; |
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| 130 | G4int nAS = 0; |
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| 131 | std::list<std::pair<G4double, G4KineticTrack *> >::iterator firstEscaping = theSorted.begin(); |
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| 132 | G4double runningEnergy = 0; |
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| 133 | G4int particleCount = 0; |
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| 134 | G4LorentzVector theLow = (*(theSorted.begin())).second->Get4Momentum(); |
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| 135 | G4LorentzVector theHigh; |
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| 136 | |
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| 137 | #ifdef CHIPSdebug |
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| 138 | G4cout << "CHIPS ENERGY LOST "<<theEnergyLostInFragmentation<<G4endl; |
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| 139 | G4cout << "sorted rapidities event start"<<G4endl; |
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| 140 | #endif |
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| 141 | |
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| 142 | G4ReactionProductVector * theResult = new G4ReactionProductVector; |
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| 143 | G4ReactionProduct * theSec; |
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| 144 | G4KineticTrackVector * secondaries; |
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| 145 | #ifdef pdebug |
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| 146 | G4cout<<"G4StringChipsInterface::Propagate: Absorption"<<G4endl; |
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| 147 | #endif |
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| 148 | |
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| 149 | // first decay and add all escaping particles. |
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| 150 | for(current = theSorted.begin(); current!=theSorted.end(); current++) |
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| 151 | { |
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| 152 | firstEscaping = current; |
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| 153 | if((*current).second->GetDefinition()->GetQuarkContent(3)!=0 || |
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| 154 | (*current).second->GetDefinition()->GetAntiQuarkContent(3) !=0) |
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| 155 | { |
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| 156 | G4KineticTrack * aResult = (*current).second; |
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| 157 | G4ParticleDefinition * pdef=aResult->GetDefinition(); |
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| 158 | secondaries = NULL; |
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| 159 | if ( pdef->GetPDGWidth() > 0 && pdef->GetPDGLifeTime() < 5E-17*s ) |
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| 160 | { |
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| 161 | secondaries = aResult->Decay(); |
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| 162 | } |
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| 163 | if ( secondaries == NULL ) |
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| 164 | { |
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| 165 | theSec = new G4ReactionProduct(aResult->GetDefinition()); |
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| 166 | G4LorentzVector current4Mom = aResult->Get4Momentum(); |
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| 167 | theSec->SetTotalEnergy(current4Mom.t()); |
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| 168 | theSec->SetMomentum(current4Mom.vect()); |
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| 169 | theResult->push_back(theSec); |
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| 170 | } |
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| 171 | else |
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| 172 | { |
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| 173 | for (unsigned int aSecondary=0; aSecondary<secondaries->size(); aSecondary++) |
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| 174 | { |
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| 175 | theSec = new G4ReactionProduct(secondaries->operator[](aSecondary)->GetDefinition()); |
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| 176 | G4LorentzVector current4Mom = secondaries->operator[](aSecondary)->Get4Momentum(); |
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| 177 | theSec->SetTotalEnergy(current4Mom.t()); |
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| 178 | theSec->SetMomentum(current4Mom.vect()); |
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| 179 | theResult->push_back(theSec); |
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| 180 | } |
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| 181 | std::for_each(secondaries->begin(), secondaries->end(), DeleteKineticTrack()); |
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| 182 | delete secondaries; |
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| 183 | } |
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| 184 | continue; |
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| 185 | } |
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| 186 | runningEnergy += (*current).second->Get4Momentum().t(); |
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| 187 | if(runningEnergy > theEnergyLostInFragmentation) break; |
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| 188 | |
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| 189 | #ifdef CHIPSdebug |
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| 190 | G4cout <<"ABSORBED STRING particles "<<current->second->GetDefinition()->GetPDGCharge()<<" " |
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| 191 | << current->second->GetDefinition()->GetPDGEncoding()<<" " |
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| 192 | << current->second->Get4Momentum() <<G4endl; |
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| 193 | #endif |
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| 194 | #ifdef pdebug |
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| 195 | G4cout<<"G4StringChipsInterface::Propagate:C=" |
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| 196 | <<current->second->GetDefinition()->GetPDGCharge()<<", PDG=" |
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| 197 | << current->second->GetDefinition()->GetPDGEncoding()<<", 4M=" |
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| 198 | << current->second->Get4Momentum() <<G4endl; |
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| 199 | #endif |
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| 200 | |
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| 201 | // projectile 4-momentum needed in constructor of quasmon |
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| 202 | particleCount++; |
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| 203 | theHigh = (*current).second->Get4Momentum(); |
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| 204 | proj4Mom += (*current).second->Get4Momentum(); |
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| 205 | |
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| 206 | #ifdef CHIPSdebug |
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| 207 | G4cout << "sorted rapidities "<<current->second->Get4Momentum().rapidity()<<G4endl; |
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| 208 | #endif |
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| 209 | |
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| 210 | // projectile quark contents needed for G4QContent construction (@@ ? -> G4QContent class) |
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| 211 | nD += (*current).second->GetDefinition()->GetQuarkContent(1); |
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| 212 | nU += (*current).second->GetDefinition()->GetQuarkContent(2); |
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| 213 | nS += (*current).second->GetDefinition()->GetQuarkContent(3); |
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| 214 | nAD += (*current).second->GetDefinition()->GetAntiQuarkContent(1); |
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| 215 | nAU += (*current).second->GetDefinition()->GetAntiQuarkContent(2); |
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| 216 | nAS += (*current).second->GetDefinition()->GetAntiQuarkContent(3); |
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| 217 | } |
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| 218 | // construct G4QContent |
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| 219 | |
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| 220 | #ifdef CHIPSdebug |
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| 221 | G4cout << "Quark content: d="<<nD<<", u="<<nU<< ", s="<< nS << G4endl; |
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| 222 | G4cout << "Anti-quark content: anit-d="<<nAD<<", anti-u="<<nAU<< ", anti-s="<< nAS << G4endl; |
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| 223 | #endif |
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| 224 | |
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| 225 | G4QContent theProjectiles(nD, nU, nS, nAD, nAU, nAS); |
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| 226 | |
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| 227 | #ifdef CHIPSdebug |
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| 228 | G4cout << "G4QContent is constructed"<<endl; |
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| 229 | #endif |
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| 230 | |
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| 231 | // target properties needed in constructor of quasmon |
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| 232 | // remove all hit nucleons to get Target code |
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| 233 | theNucleus->StartLoop(); |
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| 234 | G4Nucleon * aNucleon; |
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| 235 | G4int resA = 0; |
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| 236 | G4int resZ = 0; |
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| 237 | G4ThreeVector hitMomentum(0,0,0); |
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| 238 | G4double hitMass = 0; |
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| 239 | G4int hitCount = 0; |
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| 240 | while((aNucleon = theNucleus->GetNextNucleon())) |
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| 241 | { |
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| 242 | if(!aNucleon->AreYouHit()) |
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| 243 | { |
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| 244 | resA++; |
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| 245 | resZ+=G4int (aNucleon->GetDefinition()->GetPDGCharge()); |
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| 246 | } |
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| 247 | else |
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| 248 | { |
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| 249 | hitMomentum += aNucleon->GetMomentum().vect(); |
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| 250 | hitMass += aNucleon->GetMomentum().m(); |
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| 251 | hitCount ++; |
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| 252 | } |
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| 253 | } |
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| 254 | G4int targetPDGCode = 90000000 + 1000*resZ + (resA-resZ); |
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| 255 | G4double targetMass = theNucleus->GetMass(); |
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| 256 | targetMass -= hitMass; |
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| 257 | G4double targetEnergy = std::sqrt(hitMomentum.mag2()+targetMass*targetMass); |
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| 258 | // !! @@ Target should be at rest: hitMomentum=(0,0,0) @@ !! M.K. |
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| 259 | G4LorentzVector targ4Mom(-1.*hitMomentum, targetEnergy); |
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| 260 | |
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| 261 | // construct the quasmon |
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| 262 | // G4int nop = 122; // clusters up to Alpha cluster |
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| 263 | G4int nop = 152; // V.Ivanchenko set the same parameter as for all CHIPS models |
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| 264 | G4double fractionOfSingleQuasiFreeNucleons = 0.5; // It is A-dependent (C=.85, U=.40) |
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| 265 | G4double fractionOfPairedQuasiFreeNucleons = 0.05; |
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| 266 | G4double clusteringCoefficient = 5.; |
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| 267 | G4double temperature = 180.; |
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| 268 | G4double halfTheStrangenessOfSee = 0.3; // = s/d = s/u |
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| 269 | G4double etaToEtaPrime = 0.3; |
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| 270 | |
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| 271 | G4QNucleus::SetParameters(fractionOfSingleQuasiFreeNucleons, |
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| 272 | fractionOfPairedQuasiFreeNucleons, |
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| 273 | clusteringCoefficient); |
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| 274 | G4Quasmon::SetParameters(temperature, |
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| 275 | halfTheStrangenessOfSee, |
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| 276 | etaToEtaPrime); |
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| 277 | |
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| 278 | #ifdef CHIPSdebug |
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| 279 | G4cout << "G4QNucleus parameters "<< fractionOfSingleQuasiFreeNucleons << " " |
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| 280 | << fractionOfPairedQuasiFreeNucleons << " "<< clusteringCoefficient << G4endl; |
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| 281 | G4cout << "G4Quasmon parameters "<< temperature << " "<< halfTheStrangenessOfSee << " " |
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| 282 | <<etaToEtaPrime << G4endl; |
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| 283 | G4cout << "The Target PDG code = "<<targetPDGCode<<G4endl; |
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| 284 | G4cout << "The projectile momentum = "<<1./MeV*proj4Mom<<G4endl; |
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| 285 | G4cout << "The target momentum = "<<1./MeV*targ4Mom<<G4endl; |
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| 286 | #endif |
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| 287 | |
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| 288 | |
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| 289 | // Chips expects all in target rest frame, along z. |
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| 290 | // G4QCHIPSWorld aWorld(nop); // Create CHIPS World of nop particles |
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| 291 | G4QCHIPSWorld::Get()->GetParticles(nop); |
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| 292 | G4QHadronVector projHV; |
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| 293 | // target rest frame |
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| 294 | proj4Mom.boost(-1.*targ4Mom.boostVector()); |
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| 295 | // now go along z |
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| 296 | G4LorentzRotation toZ; |
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| 297 | toZ.rotateZ(-1*proj4Mom.phi()); |
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| 298 | toZ.rotateY(-1*proj4Mom.theta()); |
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| 299 | proj4Mom = toZ*proj4Mom; |
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| 300 | G4LorentzRotation toLab(toZ.inverse()); |
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| 301 | |
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| 302 | #ifdef CHIPSdebug |
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| 303 | G4cout << "a Boosted projectile vector along z"<<proj4Mom<<" "<<proj4Mom.mag()<<G4endl; |
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| 304 | #endif |
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| 305 | |
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| 306 | G4QHadron* iH = new G4QHadron(theProjectiles, 1./MeV*proj4Mom); |
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| 307 | projHV.push_back(iH); |
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| 308 | |
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| 309 | // now call chips with this info in place |
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| 310 | G4QHadronVector * output = 0; |
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| 311 | if (particleCount!=0) |
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| 312 | { |
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| 313 | G4QEnvironment* pan= new G4QEnvironment(projHV, targetPDGCode); |
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| 314 | try |
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| 315 | { |
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| 316 | output = pan->Fragment(); |
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| 317 | } |
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| 318 | catch(G4HadronicException & aR) |
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| 319 | { |
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| 320 | G4cerr << "Exception thrown passing through G4ChiralInvariantPhaseSpace "<<G4endl; |
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| 321 | G4cerr << " targetPDGCode = "<< targetPDGCode <<G4endl; |
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| 322 | G4cerr << " Dumping the information in the pojectile list"<<G4endl; |
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| 323 | for(size_t i=0; i< projHV.size(); i++) |
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| 324 | { |
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| 325 | G4cerr <<" Incoming 4-momentum and PDG code of "<<i<<"'th hadron: " |
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| 326 | <<" "<< projHV[i]->Get4Momentum()<<" "<<projHV[i]->GetPDGCode()<<G4endl; |
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| 327 | } |
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| 328 | throw; |
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| 329 | } |
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| 330 | std::for_each(projHV.begin(), projHV.end(), DeleteQHadron()); |
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| 331 | projHV.clear(); |
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| 332 | delete pan; |
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| 333 | } |
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| 334 | else output = new G4QHadronVector; |
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| 335 | |
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| 336 | // Fill the result. |
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| 337 | #ifdef CHIPSdebug |
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| 338 | G4cout << "NEXT EVENT"<<endl; |
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| 339 | #endif |
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| 340 | |
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| 341 | // first decay and add all escaping particles. |
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| 342 | for(current = firstEscaping; current!=theSorted.end(); current++) |
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| 343 | { |
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| 344 | G4KineticTrack * aResult = (*current).second; |
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| 345 | G4ParticleDefinition * pdef=aResult->GetDefinition(); |
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| 346 | secondaries = NULL; |
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| 347 | if ( pdef->GetPDGWidth() > 0 && pdef->GetPDGLifeTime() < 5E-17*s ) |
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| 348 | { |
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| 349 | secondaries = aResult->Decay(); |
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| 350 | } |
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| 351 | if ( secondaries == NULL ) |
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| 352 | { |
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| 353 | theSec = new G4ReactionProduct(aResult->GetDefinition()); |
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| 354 | G4LorentzVector current4Mom = aResult->Get4Momentum(); |
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| 355 | current4Mom = toLab*current4Mom; |
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| 356 | current4Mom.boost(targ4Mom.boostVector()); |
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| 357 | theSec->SetTotalEnergy(current4Mom.t()); |
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| 358 | theSec->SetMomentum(current4Mom.vect()); |
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| 359 | theResult->push_back(theSec); |
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| 360 | } |
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| 361 | else |
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| 362 | { |
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| 363 | for (unsigned int aSecondary=0; aSecondary<secondaries->size(); aSecondary++) |
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| 364 | { |
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| 365 | theSec = new G4ReactionProduct(secondaries->operator[](aSecondary)->GetDefinition()); |
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| 366 | G4LorentzVector current4Mom = secondaries->operator[](aSecondary)->Get4Momentum(); |
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| 367 | current4Mom = toLab*current4Mom; |
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| 368 | current4Mom.boost(targ4Mom.boostVector()); |
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| 369 | theSec->SetTotalEnergy(current4Mom.t()); |
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| 370 | theSec->SetMomentum(current4Mom.vect()); |
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| 371 | theResult->push_back(theSec); |
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| 372 | } |
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| 373 | std::for_each(secondaries->begin(), secondaries->end(), DeleteKineticTrack()); |
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| 374 | delete secondaries; |
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| 375 | } |
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| 376 | } |
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| 377 | std::for_each(theSecondaries->begin(), theSecondaries->end(), DeleteKineticTrack()); |
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| 378 | delete theSecondaries; |
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| 379 | |
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| 380 | // now add the quasmon output |
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| 381 | #ifdef CHIPSdebug |
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| 382 | G4cout << "Number of particles from string"<<theResult->size()<<G4endl; |
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| 383 | G4cout << "Number of particles from chips"<<output->size()<<G4endl; |
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| 384 | #endif |
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| 385 | |
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| 386 | for(unsigned int particle = 0; particle < output->size(); particle++) |
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| 387 | { |
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| 388 | if(output->operator[](particle)->GetNFragments() != 0) |
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| 389 | { |
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| 390 | delete output->operator[](particle); |
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| 391 | continue; |
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| 392 | } |
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| 393 | theSec = new G4ReactionProduct; |
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| 394 | G4int pdgCode = output->operator[](particle)->GetPDGCode(); |
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| 395 | G4ParticleDefinition * theDefinition; |
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| 396 | // Note that I still have to take care of strange nuclei |
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| 397 | // For this I need the mass calculation, and a changed interface |
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| 398 | // for ion-table ==> work for Hisaya @@@@@@@ |
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| 399 | // Then I can sort out the pdgCode. I also need a decau process |
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| 400 | // for strange nuclei; may be another chips interface |
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| 401 | if(pdgCode>90000000) |
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| 402 | { |
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| 403 | G4int aZ = (pdgCode-90000000)/1000; |
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| 404 | if (aZ>1000) aZ=aZ%1000; // patch for strange nuclei, to be repaired @@@@ |
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| 405 | G4int anN = pdgCode-90000000-1000*aZ; |
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| 406 | if(anN>1000) anN=anN%1000; // patch for strange nuclei, to be repaired @@@@ |
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| 407 | if(pdgCode==91000000) theDefinition = G4Lambda::LambdaDefinition(); |
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| 408 | else if(pdgCode==92000000) theDefinition = G4Lambda::LambdaDefinition(); |
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| 409 | else if(pdgCode==93000000) theDefinition = G4Lambda::LambdaDefinition(); |
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| 410 | else if(pdgCode==94000000) theDefinition = G4Lambda::LambdaDefinition(); |
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| 411 | else if(pdgCode==95000000) theDefinition = G4Lambda::LambdaDefinition(); |
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| 412 | else if(pdgCode==96000000) theDefinition = G4Lambda::LambdaDefinition(); |
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| 413 | else if(pdgCode==97000000) theDefinition = G4Lambda::LambdaDefinition(); |
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| 414 | else if(pdgCode==98000000) theDefinition = G4Lambda::LambdaDefinition(); |
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| 415 | else if(aZ == 0 && anN == 1) theDefinition = G4Neutron::Neutron(); |
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| 416 | else theDefinition = G4ParticleTable::GetParticleTable()->FindIon(aZ,anN+aZ,0,aZ); |
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| 417 | } |
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| 418 | else |
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| 419 | { |
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| 420 | theDefinition = G4ParticleTable::GetParticleTable()->FindParticle(output->operator[](particle)->GetPDGCode()); |
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| 421 | } |
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| 422 | #ifdef CHIPSdebug |
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| 423 | G4cout << "Particle code produced = "<< pdgCode <<G4endl; |
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| 424 | #endif |
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| 425 | |
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| 426 | theSec = new G4ReactionProduct(theDefinition); |
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| 427 | G4LorentzVector current4Mom = output->operator[](particle)->Get4Momentum(); |
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| 428 | current4Mom = toLab*current4Mom; |
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| 429 | current4Mom.boost(targ4Mom.boostVector()); |
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| 430 | theSec->SetTotalEnergy(current4Mom.t()); |
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| 431 | theSec->SetMomentum(current4Mom.vect()); |
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| 432 | theResult->push_back(theSec); |
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| 433 | |
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| 434 | #ifdef CHIPSdebug |
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| 435 | G4cout <<"CHIPS particles "<<theDefinition->GetPDGCharge()<<" " |
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| 436 | << theDefinition->GetPDGEncoding()<<" " |
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| 437 | << current4Mom <<G4endl; |
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| 438 | #endif |
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| 439 | |
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| 440 | delete output->operator[](particle); |
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| 441 | } |
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| 442 | delete output; |
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| 443 | #ifdef CHIPSdebug |
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| 444 | G4cout << "Number of particles"<<theResult->size()<<G4endl; |
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| 445 | G4cout << G4endl; |
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| 446 | // @@ G4QContent has even the out option! |
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| 447 | G4cout << "QUASMON preparation info " |
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| 448 | << 1./MeV*proj4Mom<<" " |
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| 449 | << 1./MeV*targ4Mom<<" " |
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| 450 | << nD<<" "<<nU<<" "<<nS<<" "<<nAD<<" "<<nAU<<" "<<nAS<<" " |
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| 451 | << hitCount<<" " |
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| 452 | << particleCount<<" " |
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| 453 | << theLow<<" " |
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| 454 | << theHigh<<" " |
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| 455 | << G4endl; |
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| 456 | #endif |
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| 457 | |
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| 458 | return theResult; |
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| 459 | } |
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