1 | // |
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2 | // ******************************************************************** |
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3 | // * License and Disclaimer * |
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9 | // * include a list of copyright holders. * |
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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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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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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 | // $Id: G4QCollision.cc,v 1.32 2009/04/17 15:22:31 mkossov Exp $ |
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27 | // GEANT4 tag $Name: geant4-09-03-beta-cand-01 $ |
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28 | // |
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29 | // ---------------- G4QCollision class ----------------- |
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30 | // by Mikhail Kossov, December 2003. |
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31 | // G4QCollision class of the CHIPS Simulation Branch in GEANT4 |
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32 | // --------------------------------------------------------------- |
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33 | // **************************************************************************************** |
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34 | // ********** This CLASS is temporary moved from the photolepton_hadron directory ********* |
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35 | // **************************************************************************************** |
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36 | // Short description: This is a universal class for the incoherent (inelastic) |
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37 | // nuclear interactions in the CHIPS model. |
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38 | // --------------------------------------------------------------------------- |
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39 | //#define debug |
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40 | //#define pdebug |
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41 | //#define ldebug |
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42 | //#define ppdebug |
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43 | //#define qedebug |
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44 | |
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45 | #include "G4QCollision.hh" |
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46 | |
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47 | // Initialization of static vectors |
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48 | std::vector<G4int> G4QCollision::ElementZ; // Z of the element(i) in theLastCalc |
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49 | std::vector<G4double> G4QCollision::ElProbInMat; // SumProbabilityElements in Material |
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50 | std::vector<std::vector<G4int>*> G4QCollision::ElIsoN; // N of isotope(j) of Element(i) |
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51 | std::vector<std::vector<G4double>*>G4QCollision::IsoProbInEl;//SumProbabIsotopes inElementI |
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52 | |
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53 | G4QCollision::G4QCollision(const G4String& processName): |
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54 | G4VDiscreteProcess(processName, fHadronic) |
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55 | { |
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56 | #ifdef debug |
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57 | G4cout<<"G4QCollision::Constructor is called"<<G4endl; |
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58 | #endif |
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59 | if (verboseLevel>0) G4cout << GetProcessName() << " process is created "<< G4endl; |
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60 | SetProcessSubType(fHadronInelastic); |
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61 | //G4QCHIPSWorld::Get()->GetParticles(nPartCWorld); // Create CHIPSWorld (234 part.max) |
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62 | G4QNucleus::SetParameters(freeNuc,freeDib,clustProb,mediRatio); // Clusterization param's |
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63 | G4Quasmon::SetParameters(Temperature,SSin2Gluons,EtaEtaprime); // Hadronic parameters |
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64 | G4QEnvironment::SetParameters(SolidAngle); // SolAngle of pbar-A secondary mesons capture |
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65 | //@@ Initialize here the G4QuasmonString parameters |
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66 | } |
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67 | |
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68 | G4bool G4QCollision::manualFlag=false; // If false then standard parameters are used |
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69 | G4double G4QCollision::Temperature=180.; // Critical Temperature (sensitive at High En) |
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70 | G4double G4QCollision::SSin2Gluons=0.3; // Supression of s-quarks (in respect to u&d) |
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71 | G4double G4QCollision::EtaEtaprime=0.3; // Supression of eta mesons (gg->qq/3g->qq) |
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72 | G4double G4QCollision::freeNuc=0.5; // Percentage of free nucleons on the surface |
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73 | G4double G4QCollision::freeDib=0.05; // Percentage of free diBaryons on the surface |
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74 | G4double G4QCollision::clustProb=5.; // Nuclear clusterization parameter |
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75 | G4double G4QCollision::mediRatio=10.; // medium/vacuum hadronization ratio |
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76 | G4int G4QCollision::nPartCWorld=152; // The#of particles initialized in CHIPS World |
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77 | G4double G4QCollision::SolidAngle=0.5; // Part of Solid Angle to capture (@@A-dep.) |
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78 | G4bool G4QCollision::EnergyFlux=false; // Flag for Energy Flux use (not MultyQuasmon) |
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79 | G4double G4QCollision::PiPrThresh=141.4; // Pion Production Threshold for gammas |
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80 | G4double G4QCollision::M2ShiftVir=20000.;// Shift for M2=-Q2=m_pi^2 of the virtualGamma |
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81 | G4double G4QCollision::DiNuclMass=1880.; // DoubleNucleon Mass for VirtualNormalization |
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82 | G4double G4QCollision::photNucBias=1.; // BiasingParameter for photo(e,mu,tau)Nuclear |
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83 | G4double G4QCollision::weakNucBias=1.; // BiasingParameter for ChargedCurrents(nu,mu) |
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84 | |
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85 | void G4QCollision::SetManual() {manualFlag=true;} |
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86 | void G4QCollision::SetStandard() {manualFlag=false;} |
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87 | |
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88 | // Fill the private parameters |
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89 | void G4QCollision::SetParameters(G4double temper, G4double ssin2g, G4double etaetap, |
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90 | G4double fN, G4double fD, G4double cP, G4double mR, |
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91 | G4int nParCW, G4double solAn, G4bool efFlag, |
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92 | G4double piThresh, G4double mpisq, G4double dinum) |
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93 | {// ============================================================================= |
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94 | Temperature=temper; |
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95 | SSin2Gluons=ssin2g; |
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96 | EtaEtaprime=etaetap; |
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97 | freeNuc=fN; |
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98 | freeDib=fD; |
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99 | clustProb=cP; |
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100 | mediRatio=mR; |
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101 | nPartCWorld = nParCW; |
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102 | EnergyFlux=efFlag; |
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103 | SolidAngle=solAn; |
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104 | PiPrThresh=piThresh; |
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105 | M2ShiftVir=mpisq; |
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106 | DiNuclMass=dinum; |
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107 | G4QCHIPSWorld::Get()->GetParticles(nPartCWorld); // Create CHIPS World with 234 particles |
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108 | G4QNucleus::SetParameters(freeNuc,freeDib,clustProb,mediRatio); // Clusterization param's |
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109 | G4Quasmon::SetParameters(Temperature,SSin2Gluons,EtaEtaprime); // Hadronic parameters |
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110 | G4QEnvironment::SetParameters(SolidAngle); // SolAngle of pbar-A secondary mesons capture |
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111 | } |
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112 | |
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113 | void G4QCollision::SetPhotNucBias(G4double phnB) {photNucBias=phnB;} |
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114 | void G4QCollision::SetWeakNucBias(G4double ccnB) {weakNucBias=ccnB;} |
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115 | |
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116 | // Destructor |
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117 | |
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118 | G4QCollision::~G4QCollision() {} |
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119 | |
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120 | |
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121 | G4LorentzVector G4QCollision::GetEnegryMomentumConservation() |
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122 | { |
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123 | return EnMomConservation; |
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124 | } |
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125 | |
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126 | G4int G4QCollision::GetNumberOfNeutronsInTarget() |
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127 | { |
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128 | return nOfNeutrons; |
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129 | } |
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130 | |
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131 | // output of the function must be in units of length! L=1/sig_V,sig_V=SUM(n(j,i)*sig(j,i)), |
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132 | // where n(i,j) is a number of nuclei of the isotop j of the element i in V=1(lengtUnit^3) |
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133 | // ********** All CHIPS cross sections are calculated in the surface units ************ |
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134 | G4double G4QCollision::GetMeanFreePath(const G4Track& aTrack,G4double,G4ForceCondition* Fc) |
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135 | { |
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136 | #ifdef debug |
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137 | G4cout<<"G4QCollision::GetMeanFreePath: Called Fc="<<*Fc<<G4endl; |
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138 | #endif |
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139 | *Fc = NotForced; |
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140 | #ifdef debug |
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141 | G4cout<<"G4QCollision::GetMeanFreePath: Before GetDynPart"<<G4endl; |
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142 | #endif |
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143 | const G4DynamicParticle* incidentParticle = aTrack.GetDynamicParticle(); |
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144 | #ifdef debug |
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145 | G4cout<<"G4QCollision::GetMeanFreePath: Before GetDef"<<G4endl; |
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146 | #endif |
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147 | G4ParticleDefinition* incidentParticleDefinition=incidentParticle->GetDefinition(); |
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148 | if( !IsApplicable(*incidentParticleDefinition)) |
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149 | G4cout<<"-W-G4QCollision::GetMeanFreePath called for not implemented particle"<<G4endl; |
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150 | // Calculate the mean Cross Section for the set of Elements(*Isotopes) in the Material |
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151 | G4double Momentum = incidentParticle->GetTotalMomentum(); // 3-momentum of the Particle |
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152 | #ifdef debug |
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153 | G4cout<<"G4QCollis::GetMeanFreePath: BeforeGetMaterial"<<G4endl; |
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154 | #endif |
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155 | const G4Material* material = aTrack.GetMaterial(); // Get the current material |
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156 | const G4double* NOfNucPerVolume = material->GetVecNbOfAtomsPerVolume(); |
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157 | const G4ElementVector* theElementVector = material->GetElementVector(); |
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158 | G4int nE=material->GetNumberOfElements(); |
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159 | #ifdef debug |
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160 | G4cout<<"G4QCollision::GetMeanFreePath:"<<nE<<" Elem's in theMaterial"<<G4endl; |
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161 | #endif |
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162 | G4bool leptoNuc=false; // By default the reaction is not lepto-nuclear |
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163 | G4VQCrossSection* CSmanager=0; |
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164 | G4VQCrossSection* CSmanager2=0; |
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165 | G4int pPDG=0; |
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166 | if(incidentParticleDefinition == G4Proton::Proton()) |
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167 | { |
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168 | CSmanager=G4QProtonNuclearCrossSection::GetPointer(); |
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169 | pPDG=2212; |
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170 | } |
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171 | else if(incidentParticleDefinition == G4Gamma::Gamma()) |
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172 | { |
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173 | CSmanager=G4QPhotonNuclearCrossSection::GetPointer(); |
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174 | pPDG=22; |
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175 | } |
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176 | else if(incidentParticleDefinition == G4Electron::Electron() || |
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177 | incidentParticleDefinition == G4Positron::Positron()) |
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178 | { |
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179 | CSmanager=G4QElectronNuclearCrossSection::GetPointer(); |
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180 | leptoNuc=true; |
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181 | pPDG=11; |
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182 | } |
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183 | else if(incidentParticleDefinition == G4MuonPlus::MuonPlus() || |
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184 | incidentParticleDefinition == G4MuonMinus::MuonMinus()) |
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185 | { |
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186 | CSmanager=G4QMuonNuclearCrossSection::GetPointer(); |
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187 | leptoNuc=true; |
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188 | pPDG=13; |
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189 | } |
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190 | else if(incidentParticleDefinition == G4TauPlus::TauPlus() || |
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191 | incidentParticleDefinition == G4TauMinus::TauMinus()) |
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192 | { |
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193 | CSmanager=G4QTauNuclearCrossSection::GetPointer(); |
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194 | leptoNuc=true; |
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195 | pPDG=15; |
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196 | } |
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197 | else if(incidentParticleDefinition == G4NeutrinoMu::NeutrinoMu() ) |
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198 | { |
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199 | CSmanager=G4QNuMuNuclearCrossSection::GetPointer(); |
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200 | CSmanager2=G4QNuNuNuclearCrossSection::GetPointer(); |
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201 | leptoNuc=true; |
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202 | pPDG=14; |
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203 | } |
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204 | else if(incidentParticleDefinition == G4AntiNeutrinoMu::AntiNeutrinoMu() ) |
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205 | { |
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206 | CSmanager=G4QANuMuNuclearCrossSection::GetPointer(); |
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207 | CSmanager2=G4QANuANuNuclearCrossSection::GetPointer(); |
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208 | leptoNuc=true; |
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209 | pPDG=-14; |
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210 | } |
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211 | else if(incidentParticleDefinition == G4NeutrinoE::NeutrinoE() ) |
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212 | { |
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213 | CSmanager=G4QNuENuclearCrossSection::GetPointer(); |
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214 | CSmanager2=G4QNuNuNuclearCrossSection::GetPointer(); |
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215 | leptoNuc=true; |
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216 | pPDG=12; |
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217 | } |
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218 | else if(incidentParticleDefinition == G4AntiNeutrinoE::AntiNeutrinoE() ) |
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219 | { |
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220 | CSmanager=G4QANuENuclearCrossSection::GetPointer(); |
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221 | CSmanager2=G4QANuANuNuclearCrossSection::GetPointer(); |
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222 | leptoNuc=true; |
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223 | pPDG=-12; |
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224 | } |
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225 | else G4cout<<"G4QCollision::GetMeanFreePath:Particle isn't implemented in CHIPS"<<G4endl; |
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226 | |
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227 | G4QIsotope* Isotopes = G4QIsotope::Get(); // Pointer to the G4QIsotopes singleton |
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228 | G4double sigma=0.; // Sums over elements for the material |
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229 | G4int IPIE=IsoProbInEl.size(); // How many old elements? |
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230 | if(IPIE) for(G4int ip=0; ip<IPIE; ++ip) // Clean up the SumProb's of Isotopes (SPI) |
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231 | { |
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232 | std::vector<G4double>* SPI=IsoProbInEl[ip]; // Pointer to the SPI vector |
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233 | SPI->clear(); |
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234 | delete SPI; |
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235 | std::vector<G4int>* IsN=ElIsoN[ip]; // Pointer to the N vector |
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236 | IsN->clear(); |
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237 | delete IsN; |
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238 | } |
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239 | ElProbInMat.clear(); // Clean up the SumProb's of Elements (SPE) |
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240 | ElementZ.clear(); // Clear the body vector for Z of Elements |
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241 | IsoProbInEl.clear(); // Clear the body vector for SPI |
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242 | ElIsoN.clear(); // Clear the body vector for N of Isotopes |
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243 | for(G4int i=0; i<nE; ++i) |
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244 | { |
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245 | G4Element* pElement=(*theElementVector)[i]; // Pointer to the current element |
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246 | G4int Z = static_cast<G4int>(pElement->GetZ()); // Z of the Element |
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247 | ElementZ.push_back(Z); // Remember Z of the Element |
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248 | G4int isoSize=0; // The default for the isoVectorLength is 0 |
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249 | G4int indEl=0; // Index of non-trivial element or 0(default) |
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250 | G4IsotopeVector* isoVector=pElement->GetIsotopeVector(); // Get the predefined IsoVect |
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251 | if(isoVector) isoSize=isoVector->size();// Get size of the existing isotopeVector |
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252 | #ifdef debug |
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253 | G4cout<<"G4QCollision::GetMeanFreePath: isovectorLength="<<isoSize<<G4endl; // Result |
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254 | #endif |
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255 | if(isoSize) // The Element has non-trivial abundance set |
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256 | { |
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257 | indEl=pElement->GetIndex()+1; // Index of the non-trivial element |
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258 | if(!Isotopes->IsDefined(Z,indEl)) // This index is not defined for this Z: define |
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259 | { |
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260 | std::vector<std::pair<G4int,G4double>*>* newAbund = |
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261 | new std::vector<std::pair<G4int,G4double>*>; |
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262 | G4double* abuVector=pElement->GetRelativeAbundanceVector(); |
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263 | for(G4int j=0; j<isoSize; j++) // Calculation of abundance vector for isotopes |
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264 | { |
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265 | G4int N=pElement->GetIsotope(j)->GetN()-Z; // N means A=N+Z ! |
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266 | if(pElement->GetIsotope(j)->GetZ()!=Z)G4cerr<<"G4QCollision::GetMeanFreePath" |
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267 | <<": Z="<<pElement->GetIsotope(j)->GetZ()<<"#"<<Z<<G4endl; |
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268 | G4double abund=abuVector[j]; |
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269 | std::pair<G4int,G4double>* pr= new std::pair<G4int,G4double>(N,abund); |
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270 | #ifdef debug |
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271 | G4cout<<"G4QCollision::GetMeanFreePath: p#="<<j<<",N="<<N<<",ab="<<abund<<G4endl; |
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272 | #endif |
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273 | newAbund->push_back(pr); |
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274 | } |
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275 | #ifdef debug |
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276 | G4cout<<"G4QCollision::GetMeanFreePath: pairVectLength="<<newAbund->size()<<G4endl; |
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277 | #endif |
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278 | indEl=G4QIsotope::Get()->InitElement(Z,indEl,newAbund); // definition of the newInd |
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279 | for(G4int k=0; k<isoSize; k++) delete (*newAbund)[k]; // Cleaning temporary |
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280 | delete newAbund; // Was "new" in the beginning of the name space |
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281 | } |
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282 | } |
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283 | std::vector<std::pair<G4int,G4double>*>* cs= Isotopes->GetCSVector(Z,indEl);//CSPointer |
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284 | std::vector<G4double>* SPI = new std::vector<G4double>; // Pointer to the SPI vector |
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285 | IsoProbInEl.push_back(SPI); |
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286 | std::vector<G4int>* IsN = new std::vector<G4int>; // Pointer to the N vector |
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287 | ElIsoN.push_back(IsN); |
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288 | G4int nIs=cs->size(); // A#Of Isotopes in the Element |
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289 | G4double susi=0.; // sum of CS over isotopes |
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290 | if(nIs) for(G4int j=0; j<nIs; j++) // Calculate CS for eachIsotope of El |
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291 | { |
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292 | std::pair<G4int,G4double>* curIs=(*cs)[j]; // A pointer, which is used twice |
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293 | G4int N=curIs->first; // #of Neuterons in the isotope j of El i |
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294 | IsN->push_back(N); // Remember Min N for the Element |
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295 | G4double CSI=CSmanager->GetCrossSection(true,Momentum,Z,N,pPDG);//CS(j,i) for isotope |
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296 | if(CSmanager2)CSI+=CSmanager2->GetCrossSection(true,Momentum,Z,N,pPDG);//CS(j,i)nu,nu |
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297 | #ifdef debug |
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298 | G4cout<<"GQC::GMF:X="<<CSI<<",M="<<Momentum<<",Z="<<Z<<",N="<<N<<",P="<<pPDG<<G4endl; |
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299 | #endif |
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300 | curIs->second = CSI; |
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301 | susi+=CSI; // Make a sum per isotopes |
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302 | SPI->push_back(susi); // Remember summed cross-section |
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303 | } // End of temporary initialization of the cross sections in the G4QIsotope singeltone |
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304 | sigma+=Isotopes->GetMeanCrossSection(Z,indEl)*NOfNucPerVolume[i];//SUM(MeanCS*NOfNperV) |
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305 | ElProbInMat.push_back(sigma); |
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306 | } // End of LOOP over Elements |
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307 | #ifdef debug |
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308 | G4cout<<"G4QCol::GetMeanFrPa: S="<<sigma<<",e="<<photNucBias<<",w="<<weakNucBias<<G4endl; |
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309 | #endif |
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310 | // Check that cross section is not zero and return the mean free path |
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311 | if(photNucBias!=1.) if(incidentParticleDefinition == G4Gamma::Gamma() || |
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312 | incidentParticleDefinition == G4MuonPlus::MuonPlus() || |
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313 | incidentParticleDefinition == G4MuonMinus::MuonMinus() || |
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314 | incidentParticleDefinition == G4Electron::Electron() || |
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315 | incidentParticleDefinition == G4Positron::Positron() || |
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316 | incidentParticleDefinition == G4TauMinus::TauMinus() || |
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317 | incidentParticleDefinition == G4TauPlus::TauPlus() ) |
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318 | sigma*=photNucBias; |
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319 | if(weakNucBias!=1.) if(incidentParticleDefinition==G4NeutrinoE::NeutrinoE() || |
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320 | incidentParticleDefinition==G4AntiNeutrinoE::AntiNeutrinoE() || |
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321 | incidentParticleDefinition==G4NeutrinoTau::NeutrinoTau() || |
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322 | incidentParticleDefinition==G4AntiNeutrinoTau::AntiNeutrinoTau()|| |
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323 | incidentParticleDefinition==G4NeutrinoMu::NeutrinoMu() || |
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324 | incidentParticleDefinition==G4AntiNeutrinoMu::AntiNeutrinoMu() ) |
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325 | sigma*=weakNucBias; |
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326 | if(sigma > 0.) return 1./sigma; // Mean path [distance] |
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327 | return DBL_MAX; |
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328 | } |
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329 | |
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330 | |
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331 | G4bool G4QCollision::IsApplicable(const G4ParticleDefinition& particle) |
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332 | { |
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333 | if (particle == *( G4MuonPlus::MuonPlus() )) return true; |
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334 | else if (particle == *( G4MuonMinus::MuonMinus() )) return true; |
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335 | else if (particle == *( G4TauPlus::TauPlus() )) return true; |
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336 | else if (particle == *( G4TauMinus::TauMinus() )) return true; |
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337 | else if (particle == *( G4Electron::Electron() )) return true; |
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338 | else if (particle == *( G4Positron::Positron() )) return true; |
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339 | else if (particle == *( G4Gamma::Gamma() )) return true; |
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340 | else if (particle == *( G4Proton::Proton() )) return true; |
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341 | else if (particle == *( G4AntiNeutrinoE::AntiNeutrinoE() )) return true; |
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342 | else if (particle == *( G4NeutrinoE::NeutrinoE() )) return true; |
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343 | else if (particle == *(G4AntiNeutrinoMu::AntiNeutrinoMu())) return true; |
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344 | else if (particle == *( G4NeutrinoMu::NeutrinoMu() )) return true; |
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345 | //else if (particle == *( G4Neutron::Neutron() )) return true; |
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346 | //else if (particle == *( G4PionMinus::PionMinus() )) return true; |
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347 | //else if (particle == *( G4PionPlus::PionPlus() )) return true; |
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348 | //else if (particle == *( G4KaonPlus::KaonPlus() )) return true; |
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349 | //else if (particle == *( G4KaonMinus::KaonMinus() )) return true; |
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350 | //else if (particle == *( G4KaonZeroLong::KaonZeroLong() )) return true; |
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351 | //else if (particle == *( G4KaonZeroShort::KaonZeroShort() )) return true; |
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352 | //else if (particle == *( G4Lambda::Lambda() )) return true; |
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353 | //else if (particle == *( G4SigmaPlus::SigmaPlus() )) return true; |
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354 | //else if (particle == *( G4SigmaMinus::SigmaMinus() )) return true; |
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355 | //else if (particle == *( G4SigmaZero::SigmaZero() )) return true; |
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356 | //else if (particle == *( G4XiMinus::XiMinus() )) return true; |
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357 | //else if (particle == *( G4XiZero::XiZero() )) return true; |
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358 | //else if (particle == *( G4OmegaMinus::OmegaMinus() )) return true; |
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359 | //else if (particle == *( G4AntiNeutron::AntiNeutron() )) return true; |
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360 | //else if (particle == *( G4AntiProton::AntiProton() )) return true; |
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361 | //else if (particle == *(G4AntiNeutrinoTau::AntiNeutrinoTau())) return true; |
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362 | //else if (particle == *( G4NeutrinoTau::NeutrinoTau() )) return true; |
---|
363 | #ifdef debug |
---|
364 | G4cout<<"***G4QCollision::IsApplicable: PDG="<<particle.GetPDGEncoding()<<G4endl; |
---|
365 | #endif |
---|
366 | return false; |
---|
367 | } |
---|
368 | |
---|
369 | G4VParticleChange* G4QCollision::PostStepDoIt(const G4Track& track, const G4Step& step) |
---|
370 | { |
---|
371 | static const G4double third = 1./3.; |
---|
372 | static const G4double me=G4Electron::Electron()->GetPDGMass(); // electron mass |
---|
373 | static const G4double me2=me*me; // squared electron mass |
---|
374 | static const G4double mu=G4MuonMinus::MuonMinus()->GetPDGMass(); // muon mass |
---|
375 | static const G4double mu2=mu*mu; // squared muon mass |
---|
376 | static const G4double mt=G4TauMinus::TauMinus()->GetPDGMass(); // tau mass |
---|
377 | static const G4double mt2=mt*mt; // squared tau mass |
---|
378 | //static const G4double dpi=M_PI+M_PI; // 2*pi (for Phi distr.) ***changed to twopi*** |
---|
379 | static const G4double mNeut= G4QPDGCode(2112).GetMass(); |
---|
380 | static const G4double mNeut2= mNeut*mNeut; |
---|
381 | static const G4double mProt= G4QPDGCode(2212).GetMass(); |
---|
382 | static const G4double mProt2= mProt*mProt; |
---|
383 | static const G4double dM=mProt+mNeut; // doubled nucleon mass |
---|
384 | static const G4double hdM=dM/2.; // M of the "nucleon" |
---|
385 | static const G4double hdM2=hdM*hdM; // M2 of the "nucleon" |
---|
386 | static const G4double mPi0 = G4QPDGCode(111).GetMass(); |
---|
387 | static const G4double mPi0s= mPi0*mPi0; |
---|
388 | static const G4double mDeut= G4QPDGCode(2112).GetNuclMass(1,1,0);// Mass of deuteron |
---|
389 | //static const G4double mDeut2=mDeut*mDeut; // SquaredMassOfDeuteron |
---|
390 | static const G4double mTrit= G4QPDGCode(2112).GetNuclMass(1,2,0);// Mass of tritium |
---|
391 | static const G4double mHel3= G4QPDGCode(2112).GetNuclMass(2,1,0);// Mass of Helium3 |
---|
392 | static const G4double mAlph= G4QPDGCode(2112).GetNuclMass(2,2,0);// Mass of alpha |
---|
393 | static const G4double mPi = G4QPDGCode(211).GetMass(); |
---|
394 | static const G4double tmPi = mPi+mPi; // Doubled mass of the charged pion |
---|
395 | static const G4double stmPi= tmPi*tmPi; // Squared Doubled mass of the charged pion |
---|
396 | static const G4double mPPi = mPi+mProt; // Delta threshold |
---|
397 | static const G4double mPPi2= mPPi*mPPi; // Delta low threshold for W2 |
---|
398 | //static const G4double mDel2= 1400*1400; // Delta up threshold for W2 (in MeV^2) |
---|
399 | // Static definitions for electrons (nu,e) ----------------------------------------- |
---|
400 | static const G4double meN = mNeut+me; |
---|
401 | static const G4double meN2= meN*meN; |
---|
402 | static const G4double fmeN= 4*mNeut2*me2; |
---|
403 | static const G4double mesN= mNeut2+me2; |
---|
404 | static const G4double meP = mProt+me; |
---|
405 | static const G4double meP2= meP*meP; |
---|
406 | static const G4double fmeP= 4*mProt2*me2; |
---|
407 | static const G4double mesP= mProt2+me2; |
---|
408 | static const G4double medM= me2/dM; // for x limit |
---|
409 | static const G4double meD = mPPi+me; // Multiperipheral threshold |
---|
410 | static const G4double meD2= meD*meD; |
---|
411 | // Static definitions for muons (nu,mu) ----------------------------------------- |
---|
412 | static const G4double muN = mNeut+mu; |
---|
413 | static const G4double muN2= muN*muN; |
---|
414 | static const G4double fmuN= 4*mNeut2*mu2; |
---|
415 | static const G4double musN= mNeut2+mu2; |
---|
416 | static const G4double muP = mProt+mu; |
---|
417 | static const G4double muP2= muP*muP; // + |
---|
418 | static const G4double fmuP= 4*mProt2*mu2; // + |
---|
419 | static const G4double musP= mProt2+mu2; |
---|
420 | static const G4double mudM= mu2/dM; // for x limit |
---|
421 | static const G4double muD = mPPi+mu; // Multiperipheral threshold |
---|
422 | static const G4double muD2= muD*muD; |
---|
423 | // Static definitions for muons (nu,nu) ----------------------------------------- |
---|
424 | //static const G4double nuN = mNeut; |
---|
425 | //static const G4double nuN2= mNeut2; |
---|
426 | //static const G4double fnuN= 0.; |
---|
427 | //static const G4double nusN= mNeut2; |
---|
428 | //static const G4double nuP = mProt; |
---|
429 | //static const G4double nuP2= mProt2; |
---|
430 | //static const G4double fnuP= 0.; |
---|
431 | //static const G4double nusP= mProt2; |
---|
432 | //static const G4double nudM= 0.; // for x limit |
---|
433 | //static const G4double nuD = mPPi; // Multiperipheral threshold |
---|
434 | //static const G4double nuD2= mPPi2; |
---|
435 | //------------------------------------------------------------------------------------- |
---|
436 | static G4bool CWinit = true; // CHIPS Warld needs to be initted |
---|
437 | if(CWinit) |
---|
438 | { |
---|
439 | CWinit=false; |
---|
440 | G4QCHIPSWorld::Get()->GetParticles(nPartCWorld); // Create CHIPS World (234 part.max) |
---|
441 | } |
---|
442 | //------------------------------------------------------------------------------------- |
---|
443 | const G4DynamicParticle* projHadron = track.GetDynamicParticle(); |
---|
444 | const G4ParticleDefinition* particle=projHadron->GetDefinition(); |
---|
445 | #ifdef debug |
---|
446 | G4cout<<"G4QCollision::PostStepDoIt: Before the GetMeanFreePath is called"<<G4endl; |
---|
447 | #endif |
---|
448 | G4ForceCondition cond=NotForced; |
---|
449 | GetMeanFreePath(track, 1., &cond); |
---|
450 | #ifdef debug |
---|
451 | G4cout<<"G4QCollision::PostStepDoIt: After the GetMeanFreePath is called"<<G4endl; |
---|
452 | #endif |
---|
453 | G4bool scat=false; // No CHEX in proj scattering |
---|
454 | G4int scatPDG=0; // Must be filled if true (CHEX) |
---|
455 | G4LorentzVector proj4M=projHadron->Get4Momentum(); // 4-momentum of the projectile (IU?) |
---|
456 | G4LorentzVector scat4M=proj4M; // Must be filled if true |
---|
457 | G4double momentum = projHadron->GetTotalMomentum(); // 3-momentum of the Particle |
---|
458 | G4double Momentum=proj4M.rho(); |
---|
459 | if(std::fabs(Momentum-momentum)>.001) |
---|
460 | G4cerr<<"*G4QCollision::PostStepDoIt: P="<<Momentum<<"#"<<momentum<<G4endl; |
---|
461 | #ifdef debug |
---|
462 | G4double mp=proj4M.m(); |
---|
463 | G4cout<<"-->G4QCollis::PostStDoIt:called,P="<<Momentum<<"="<<momentum<<",m="<<mp<<G4endl; |
---|
464 | #endif |
---|
465 | if (!IsApplicable(*particle)) // Check applicability |
---|
466 | { |
---|
467 | G4cerr<<"G4QCollision::PostStepDoIt:Only gam,e+,e-,mu+,mu-,t+,t-,p are implemented." |
---|
468 | <<G4endl; |
---|
469 | return 0; |
---|
470 | } |
---|
471 | const G4Material* material = track.GetMaterial(); // Get the current material |
---|
472 | G4int Z=0; |
---|
473 | const G4ElementVector* theElementVector = material->GetElementVector(); |
---|
474 | G4int nE=material->GetNumberOfElements(); |
---|
475 | #ifdef debug |
---|
476 | G4cout<<"G4QCollision::PostStepDoIt: "<<nE<<" elements in the material."<<G4endl; |
---|
477 | #endif |
---|
478 | G4int projPDG=0; // PDG Code prototype for the captured hadron |
---|
479 | // Not all these particles are implemented yet (see Is Applicable) |
---|
480 | if (particle == G4MuonPlus::MuonPlus() ) projPDG= -13; |
---|
481 | else if (particle == G4MuonMinus::MuonMinus() ) projPDG= 13; |
---|
482 | else if (particle == G4NeutrinoMu::NeutrinoMu() ) projPDG= 14; |
---|
483 | else if (particle == G4AntiNeutrinoMu::AntiNeutrinoMu() ) projPDG= -14; |
---|
484 | else if (particle == G4Electron::Electron() ) projPDG= 11; |
---|
485 | else if (particle == G4Positron::Positron() ) projPDG= -11; |
---|
486 | else if (particle == G4NeutrinoE::NeutrinoE() ) projPDG= 12; |
---|
487 | else if (particle == G4AntiNeutrinoE::AntiNeutrinoE() ) projPDG= -12; |
---|
488 | else if (particle == G4Gamma::Gamma() ) projPDG= 22; |
---|
489 | else if (particle == G4Proton::Proton() ) projPDG= 2212; |
---|
490 | else if (particle == G4Neutron::Neutron() ) projPDG= 2112; |
---|
491 | else if (particle == G4PionMinus::PionMinus() ) projPDG= -211; |
---|
492 | else if (particle == G4PionPlus::PionPlus() ) projPDG= 211; |
---|
493 | else if (particle == G4KaonPlus::KaonPlus() ) projPDG= 2112; |
---|
494 | else if (particle == G4KaonMinus::KaonMinus() ) projPDG= -321; |
---|
495 | else if (particle == G4KaonZeroLong::KaonZeroLong() ) projPDG= 130; |
---|
496 | else if (particle == G4KaonZeroShort::KaonZeroShort() ) projPDG= 310; |
---|
497 | else if (particle == G4TauPlus::TauPlus() ) projPDG= -15; |
---|
498 | else if (particle == G4TauMinus::TauMinus() ) projPDG= 15; |
---|
499 | else if (particle == G4NeutrinoTau::NeutrinoTau() ) projPDG= 16; |
---|
500 | else if (particle == G4AntiNeutrinoTau::AntiNeutrinoTau()) projPDG= -16; |
---|
501 | else if (particle == G4Lambda::Lambda() ) projPDG= 3122; |
---|
502 | else if (particle == G4SigmaPlus::SigmaPlus() ) projPDG= 3222; |
---|
503 | else if (particle == G4SigmaMinus::SigmaMinus() ) projPDG= 3112; |
---|
504 | else if (particle == G4SigmaZero::SigmaZero() ) projPDG= 3212; |
---|
505 | else if (particle == G4XiMinus::XiMinus() ) projPDG= 3312; |
---|
506 | else if (particle == G4XiZero::XiZero() ) projPDG= 3322; |
---|
507 | else if (particle == G4OmegaMinus::OmegaMinus() ) projPDG= 3334; |
---|
508 | else if (particle == G4AntiNeutron::AntiNeutron() ) projPDG=-2112; |
---|
509 | else if (particle == G4AntiProton::AntiProton() ) projPDG=-2212; |
---|
510 | G4int aProjPDG=std::abs(projPDG); |
---|
511 | #ifdef debug |
---|
512 | G4int prPDG=particle->GetPDGEncoding(); |
---|
513 | G4cout<<"G4QCollision::PostStepDoIt: projPDG="<<projPDG<<", stPDG="<<prPDG<<G4endl; |
---|
514 | #endif |
---|
515 | if(!projPDG) |
---|
516 | { |
---|
517 | G4cerr<<"---Warning---G4QCollision::PostStepDoIt:Undefined interacting hadron"<<G4endl; |
---|
518 | return 0; |
---|
519 | } |
---|
520 | G4int EPIM=ElProbInMat.size(); |
---|
521 | #ifdef debug |
---|
522 | G4cout<<"G4QCollis::PostStDoIt: m="<<EPIM<<",n="<<nE<<",T="<<ElProbInMat[EPIM-1]<<G4endl; |
---|
523 | #endif |
---|
524 | G4int i=0; |
---|
525 | if(EPIM>1) |
---|
526 | { |
---|
527 | G4double rnd = ElProbInMat[EPIM-1]*G4UniformRand(); |
---|
528 | for(i=0; i<nE; ++i) |
---|
529 | { |
---|
530 | #ifdef debug |
---|
531 | G4cout<<"G4QCollision::PostStepDoIt:E["<<i<<"]="<<ElProbInMat[i]<<",r="<<rnd<<G4endl; |
---|
532 | #endif |
---|
533 | if (rnd<ElProbInMat[i]) break; |
---|
534 | } |
---|
535 | if(i>=nE) i=nE-1; // Top limit for the Element |
---|
536 | } |
---|
537 | G4Element* pElement=(*theElementVector)[i]; |
---|
538 | Z=static_cast<G4int>(pElement->GetZ()); |
---|
539 | #ifdef debug |
---|
540 | G4cout<<"G4QCollision::PostStepDoIt: i="<<i<<", Z(element)="<<Z<<G4endl; |
---|
541 | #endif |
---|
542 | if(Z<=0) |
---|
543 | { |
---|
544 | G4cerr<<"---Warning---G4QCollision::PostStepDoIt: Element with Z="<<Z<<G4endl; |
---|
545 | if(Z<0) return 0; |
---|
546 | } |
---|
547 | std::vector<G4double>* SPI = IsoProbInEl[i];// Vector of summedProbabilities for isotopes |
---|
548 | std::vector<G4int>* IsN = ElIsoN[i]; // Vector of "#of neutrons" in the isotope El[i] |
---|
549 | G4int nofIsot=SPI->size(); // #of isotopes in the element i |
---|
550 | #ifdef debug |
---|
551 | G4cout<<"G4QCollis::PosStDoIt:n="<<nofIsot<<",T="<<(*SPI)[nofIsot-1]<<G4endl; |
---|
552 | #endif |
---|
553 | G4int j=0; |
---|
554 | if(nofIsot>1) |
---|
555 | { |
---|
556 | G4double rndI=(*SPI)[nofIsot-1]*G4UniformRand(); // Randomize the isotop of the Element |
---|
557 | for(j=0; j<nofIsot; ++j) |
---|
558 | { |
---|
559 | #ifdef debug |
---|
560 | G4cout<<"G4QCollision::PostStepDoIt: SP["<<j<<"]="<<(*SPI)[j]<<", r="<<rndI<<G4endl; |
---|
561 | #endif |
---|
562 | if(rndI < (*SPI)[j]) break; |
---|
563 | } |
---|
564 | if(j>=nofIsot) j=nofIsot-1; // Top limit for the isotope |
---|
565 | } |
---|
566 | G4int N =(*IsN)[j]; ; // Randomized number of neutrons |
---|
567 | #ifdef debug |
---|
568 | G4cout<<"G4QCollision::PostStepDoIt: Z="<<Z<<", j="<<i<<", N(isotope)="<<N<<G4endl; |
---|
569 | #endif |
---|
570 | if(N<0) |
---|
571 | { |
---|
572 | G4cerr<<"-Warning-G4QCollision::PostStepDoIt: Isotope with Z="<<Z<<", 0>N="<<N<<G4endl; |
---|
573 | return 0; |
---|
574 | } |
---|
575 | nOfNeutrons=N; // Remember it for the energy-momentum check |
---|
576 | G4double dd=0.025; |
---|
577 | G4double am=Z+N; |
---|
578 | G4double sr=std::sqrt(am); |
---|
579 | G4double dsr=0.01*(sr+sr); |
---|
580 | if(dsr<dd)dsr=dd; |
---|
581 | if(manualFlag) G4QNucleus::SetParameters(freeNuc,freeDib,clustProb,mediRatio); // ManualP |
---|
582 | else if(projPDG==-2212) G4QNucleus::SetParameters(1.-dsr-dsr,dd+dd,5.,10.);//aP ClustPars |
---|
583 | else if(projPDG==-211) G4QNucleus::SetParameters(.67-dsr,.32-dsr,5.,9.);//Pi- ClustPars |
---|
584 | #ifdef debug |
---|
585 | G4cout<<"G4QCollision::PostStepDoIt: N="<<N<<" for element with Z="<<Z<<G4endl; |
---|
586 | #endif |
---|
587 | if(N<0) |
---|
588 | { |
---|
589 | G4cerr<<"---Warning---G4QCollision::PostStepDoIt:Element with N="<<N<< G4endl; |
---|
590 | return 0; |
---|
591 | } |
---|
592 | aParticleChange.Initialize(track); |
---|
593 | G4double weight = track.GetWeight(); |
---|
594 | if(photNucBias!=1.) weight/=photNucBias; |
---|
595 | else if(weakNucBias!=1.) weight/=weakNucBias; |
---|
596 | G4double localtime = track.GetGlobalTime(); |
---|
597 | G4ThreeVector position = track.GetPosition(); |
---|
598 | G4TouchableHandle trTouchable = track.GetTouchableHandle(); |
---|
599 | // |
---|
600 | G4int targPDG=90000000+Z*1000+N; // PDG Code of the target nucleus |
---|
601 | G4QPDGCode targQPDG(targPDG); |
---|
602 | G4double tgM=targQPDG.GetMass(); // Target mass |
---|
603 | G4double tM=tgM; // Target mass (copy to be changed) |
---|
604 | G4QHadronVector* output=new G4QHadronVector;// Prototype of EnvironOutput G4QHadronVector |
---|
605 | G4double absMom = 0.; // Prototype of absorbed by nucleus Moment |
---|
606 | G4QHadronVector* leadhs=new G4QHadronVector;// Prototype of QuasmOutput G4QHadronVectorum |
---|
607 | G4LorentzVector lead4M(0.,0.,0.,0.); // Prototype of LeadingQ 4-momentum |
---|
608 | |
---|
609 | // |
---|
610 | // Leptons with photonuclear |
---|
611 | // Lepto-nuclear case with the equivalent photon algorithm. @@InFuture + NC (?) |
---|
612 | // |
---|
613 | if (aProjPDG == 11 || aProjPDG == 13 || aProjPDG == 15) |
---|
614 | { |
---|
615 | #ifdef debug |
---|
616 | G4cout<<"G4QCollision::PostStDoIt:startSt="<<aParticleChange.GetTrackStatus()<<G4endl; |
---|
617 | #endif |
---|
618 | G4double kinEnergy= projHadron->GetKineticEnergy(); |
---|
619 | G4ParticleMomentum dir = projHadron->GetMomentumDirection(); |
---|
620 | G4VQCrossSection* CSmanager=G4QElectronNuclearCrossSection::GetPointer(); |
---|
621 | G4double ml=me; |
---|
622 | G4double ml2=me2; |
---|
623 | if(aProjPDG== 13) |
---|
624 | { |
---|
625 | CSmanager=G4QMuonNuclearCrossSection::GetPointer(); |
---|
626 | ml=mu; |
---|
627 | ml2=mu2; |
---|
628 | } |
---|
629 | if(aProjPDG== 15) |
---|
630 | { |
---|
631 | CSmanager=G4QTauNuclearCrossSection::GetPointer(); |
---|
632 | ml=mt; |
---|
633 | ml2=mt2; |
---|
634 | } |
---|
635 | // @@ Probably this is not necessary any more (?) |
---|
636 | G4double xSec=CSmanager->GetCrossSection(false,Momentum,Z,N,aProjPDG);// Recalculate XS |
---|
637 | // @@ check a possibility to separate p, n, or alpha (!) |
---|
638 | if(xSec <= 0.) // The cross-section is 0 -> Do Nothing |
---|
639 | { |
---|
640 | #ifdef debug |
---|
641 | G4cerr<<"---OUT---G4QCollision::PSDoIt: Called for zero Cross-section"<<G4endl; |
---|
642 | #endif |
---|
643 | //Do Nothing Action insead of the reaction |
---|
644 | aParticleChange.ProposeEnergy(kinEnergy); |
---|
645 | aParticleChange.ProposeLocalEnergyDeposit(0.); |
---|
646 | aParticleChange.ProposeMomentumDirection(dir); |
---|
647 | aParticleChange.ProposeTrackStatus(fAlive); |
---|
648 | return G4VDiscreteProcess::PostStepDoIt(track,step); |
---|
649 | } |
---|
650 | G4double photonEnergy = CSmanager->GetExchangeEnergy(); // Energy of EqivExchangePart |
---|
651 | #ifdef debug |
---|
652 | G4cout<<"G4QCol::PStDoIt: kE="<<kinEnergy<<",dir="<<dir<<",phE="<<photonEnergy<<G4endl; |
---|
653 | #endif |
---|
654 | if( kinEnergy < photonEnergy || photonEnergy < 0.) |
---|
655 | { |
---|
656 | //Do Nothing Action insead of the reaction |
---|
657 | G4cerr<<"--G4QCollision::PSDoIt: photE="<<photonEnergy<<">leptE="<<kinEnergy<<G4endl; |
---|
658 | aParticleChange.ProposeEnergy(kinEnergy); |
---|
659 | aParticleChange.ProposeLocalEnergyDeposit(0.); |
---|
660 | aParticleChange.ProposeMomentumDirection(dir); |
---|
661 | aParticleChange.ProposeTrackStatus(fAlive); |
---|
662 | return G4VDiscreteProcess::PostStepDoIt(track,step); |
---|
663 | } |
---|
664 | G4double photonQ2 = CSmanager->GetExchangeQ2(photonEnergy);// Q2(t) of EqivExchangePart |
---|
665 | G4double W=photonEnergy-photonQ2/dM;// HadronicEnergyFlow (W-energy) for virtual photon |
---|
666 | if(tM<999.) W-=mPi0+mPi0s/dM; // Pion production threshold for a nucleon target |
---|
667 | if(W<0.) |
---|
668 | { |
---|
669 | //Do Nothing Action insead of the reaction |
---|
670 | #ifdef debug |
---|
671 | G4cout<<"--G4QCollision::PostStepDoIt:(lN) negative equivalent energy W="<<W<<G4endl; |
---|
672 | #endif |
---|
673 | aParticleChange.ProposeEnergy(kinEnergy); |
---|
674 | aParticleChange.ProposeLocalEnergyDeposit(0.); |
---|
675 | aParticleChange.ProposeMomentumDirection(dir); |
---|
676 | aParticleChange.ProposeTrackStatus(fAlive); |
---|
677 | return G4VDiscreteProcess::PostStepDoIt(track,step); |
---|
678 | } |
---|
679 | // Update G4VParticleChange for the scattered muon |
---|
680 | G4VQCrossSection* thePhotonData=G4QPhotonNuclearCrossSection::GetPointer(); |
---|
681 | G4double sigNu=thePhotonData->GetCrossSection(true,photonEnergy,Z,N,22);//Integrated XS |
---|
682 | G4double sigK =thePhotonData->GetCrossSection(true, W, Z, N, 22); // Real XS |
---|
683 | G4double rndFraction = CSmanager->GetVirtualFactor(photonEnergy, photonQ2); |
---|
684 | if(sigNu*G4UniformRand()>sigK*rndFraction) |
---|
685 | { |
---|
686 | //Do NothingToDo Action insead of the reaction |
---|
687 | #ifdef debug |
---|
688 | G4cout<<"-DoNoth-G4QCollision::PostStepDoIt: probab. correction - DoNothing"<<G4endl; |
---|
689 | #endif |
---|
690 | aParticleChange.ProposeEnergy(kinEnergy); |
---|
691 | aParticleChange.ProposeLocalEnergyDeposit(0.); |
---|
692 | aParticleChange.ProposeMomentumDirection(dir); |
---|
693 | aParticleChange.ProposeTrackStatus(fAlive); |
---|
694 | return G4VDiscreteProcess::PostStepDoIt(track,step); |
---|
695 | } |
---|
696 | G4double iniE=kinEnergy+ml; // Initial total energy of the lepton |
---|
697 | G4double finE=iniE-photonEnergy; // Final total energy of the lepton |
---|
698 | #ifdef pdebug |
---|
699 | G4cout<<"G4QCollision::PoStDoIt:E="<<iniE<<",lE="<<finE<<"-"<<ml<<"="<<finE-ml<<G4endl; |
---|
700 | #endif |
---|
701 | aParticleChange.ProposeEnergy(finE-ml); |
---|
702 | if(finE<=ml) // Secondary lepton (e/mu/tau) at rest disappears |
---|
703 | { |
---|
704 | aParticleChange.ProposeEnergy(0.); |
---|
705 | if(aProjPDG== 11) aParticleChange.ProposeTrackStatus(fStopAndKill); |
---|
706 | else aParticleChange.ProposeTrackStatus(fStopButAlive); |
---|
707 | aParticleChange.ProposeMomentumDirection(dir); |
---|
708 | } |
---|
709 | else aParticleChange.ProposeTrackStatus(fAlive); |
---|
710 | G4double iniP=std::sqrt(iniE*iniE-ml2); // Initial momentum of the electron |
---|
711 | G4double finP=std::sqrt(finE*finE-ml2); // Final momentum of the electron |
---|
712 | G4double cost=(iniE*finE-ml2-photonQ2/2)/iniP/finP; // cos(scat_ang_of_lepton) |
---|
713 | #ifdef pdebug |
---|
714 | G4cout<<"G4QC::PSDoIt:Q2="<<photonQ2<<",ct="<<cost<<",Pi="<<iniP<<",Pf="<<finP<<G4endl; |
---|
715 | #endif |
---|
716 | if(cost>1.) cost=1.; // To avoid the accuracy of calculation problem |
---|
717 | if(cost<-1.) cost=-1.; // To avoid the accuracy of calculation problem |
---|
718 | // |
---|
719 | // Scatter the lepton ( @@ make the same thing for real photons) |
---|
720 | // At this point we have photonEnergy and photonQ2 (with notDefinedPhi)->SelectProjPart |
---|
721 | G4double absEn = std::pow(am,third)*GeV; // @@(b) Mean Energy Absorbed by a Nucleus |
---|
722 | //if(am>1 && absEn < photonEnergy) // --> the absorption of energy can happen |
---|
723 | if(absEn < photonEnergy) // --> the absorption of energy can happen |
---|
724 | { |
---|
725 | G4double abtEn = absEn+hdM; // @@(b) MeanEnergyAbsorbed by a nucleus (+M_N) |
---|
726 | G4double abEn2 = abtEn*abtEn; // Squared absorbed Energy + MN |
---|
727 | G4double abMo2 = abEn2-hdM2; // Squared absorbed Momentum of compound system |
---|
728 | G4double phEn2 = photonEnergy*photonEnergy; |
---|
729 | G4double phMo2 = phEn2+photonQ2; // Squared momentum of primary virtual photon |
---|
730 | G4double phMo = std::sqrt(phMo2); // Momentum of the primary virtual photon |
---|
731 | absMom = std::sqrt(abMo2); // Absorbed Momentum |
---|
732 | if(absMom < phMo) // --> the absorption of momentum can happen |
---|
733 | { |
---|
734 | G4double dEn = photonEnergy - absEn; // Leading energy |
---|
735 | G4double dMo = phMo - absMom; // Leading momentum |
---|
736 | G4double sF = dEn*dEn - dMo*dMo;// s of leading particle |
---|
737 | #ifdef ppdebug |
---|
738 | G4cout<<"-PhotoAbsorption-G4QCol::PStDoIt:sF="<<sF<<",phEn="<<photonEnergy<<G4endl; |
---|
739 | #endif |
---|
740 | if(sF > stmPi) // --> Leading fragmentation is possible |
---|
741 | { |
---|
742 | photonEnergy = absEn; // New value of the photon energy |
---|
743 | photonQ2=abMo2-absEn*absEn; // New value of the photon Q2 |
---|
744 | absEn = dEn; // Put energy of leading particle to absEn (!) |
---|
745 | } |
---|
746 | else absMom=0.; // Flag that nothing has happened |
---|
747 | } |
---|
748 | else absMom=0.; // Flag that nothing has happened |
---|
749 | } |
---|
750 | // ------------- End of ProjPart selection |
---|
751 | // |
---|
752 | // Scattering in respect to the derection of the incident muon is made impicitly: |
---|
753 | G4ThreeVector ort=dir.orthogonal(); // Not normed orthogonal vector (!) (to dir) |
---|
754 | G4ThreeVector ortx = ort.unit(); // First unit vector orthogonal to the direction |
---|
755 | G4ThreeVector orty = dir.cross(ortx);// Second unit vector orthoganal to the direction |
---|
756 | G4double sint=std::sqrt(1.-cost*cost); // Perpendicular component |
---|
757 | G4double phi=twopi*G4UniformRand(); // phi of scattered electron |
---|
758 | G4double sinx=sint*std::sin(phi); // x perpendicular component |
---|
759 | G4double siny=sint*std::cos(phi); // y perpendicular component |
---|
760 | G4ThreeVector findir=cost*dir+sinx*ortx+siny*orty; |
---|
761 | aParticleChange.ProposeMomentumDirection(findir); // new direction for the lepton |
---|
762 | #ifdef pdebug |
---|
763 | G4cout<<"G4QCollision::PostStepDoIt: E="<<aParticleChange.GetEnergy()<<"="<<finE<<"-" |
---|
764 | <<ml<<", d="<<*aParticleChange.GetMomentumDirection()<<","<<findir<<G4endl; |
---|
765 | #endif |
---|
766 | G4ThreeVector photon3M=iniP*dir-finP*findir;// 3D total momentum of photon |
---|
767 | if(absMom) // Photon must be reduced & LeadingSyst fragmented |
---|
768 | { |
---|
769 | G4double ptm=photon3M.mag(); // 3M of the virtual photon |
---|
770 | #ifdef ppdebug |
---|
771 | G4cout<<"-Absorption-G4QCollision::PostStepDoIt: ph3M="<<photon3M<<", eIn3M=" |
---|
772 | <<iniP*dir<<", eFin3M="<<finP*findir<<", abs3M="<<absMom<<"<ptm="<<ptm<<G4endl; |
---|
773 | #endif |
---|
774 | G4ThreeVector lead3M=photon3M*(ptm-absMom)/ptm; // Keep the direction for leading Q |
---|
775 | photon3M-=lead3M; // Reduced photon Momentum (photEn already = absEn) |
---|
776 | proj4M=G4LorentzVector(lead3M,absEn); // 4-momentum of leading System |
---|
777 | #ifdef ppdebug |
---|
778 | G4cout<<"-->G4QC::PoStDoIt: new sF="<<proj4M.m2()<<", lead4M="<<proj4M<<G4endl; |
---|
779 | #endif |
---|
780 | lead4M=proj4M; // Remember 4-mom for the total 4-momentum |
---|
781 | G4Quasmon* pan= new G4Quasmon(G4QContent(1,1,0,1,1,0),proj4M);// ---> DELETED -->---+ |
---|
782 | try // | |
---|
783 | { // | |
---|
784 | delete leadhs; // | |
---|
785 | G4QNucleus vac(90000000); // | |
---|
786 | leadhs=pan->Fragment(vac,1); // DELETED after it is copied to output vector | |
---|
787 | } // | |
---|
788 | catch (G4QException& error) // | |
---|
789 | { // | |
---|
790 | G4cerr<<"***G4QCollision::PostStepDoIt: G4Quasmon Exception is catched"<<G4endl;//| |
---|
791 | G4Exception("G4QCollision::PostStepDoIt:","72",FatalException,"QuasmonCrash"); //| |
---|
792 | } // | |
---|
793 | delete pan; // Delete the Nuclear Environment <----<---+ |
---|
794 | #ifdef ppdebug |
---|
795 | G4cout<<"G4QCol::PStDoIt: l4M="<<proj4M<<proj4M.m2()<<", N="<<leadhs->size()<<",pt=" |
---|
796 | <<ptm<<",pa="<<absMom<<",El="<<absEn<<",Pl="<<ptm-absMom<<G4endl; |
---|
797 | #endif |
---|
798 | } |
---|
799 | projPDG=22; |
---|
800 | proj4M=G4LorentzVector(photon3M,photonEnergy); |
---|
801 | #ifdef debug |
---|
802 | G4cout<<"G4QCollision::PostStDoIt: St="<<aParticleChange.GetTrackStatus()<<", g4m=" |
---|
803 | <<proj4M<<", lE="<<finE<<", lP="<<finP*findir<<", d="<<findir.mag2()<<G4endl; |
---|
804 | #endif |
---|
805 | |
---|
806 | // |
---|
807 | // neutrinoNuclear interactions (nu_e, nu_mu only) |
---|
808 | // |
---|
809 | } |
---|
810 | else if (aProjPDG == 12 || aProjPDG == 14) |
---|
811 | { |
---|
812 | G4double kinEnergy= projHadron->GetKineticEnergy()/MeV; // Total energy of the neutrino |
---|
813 | G4double dKinE=kinEnergy+kinEnergy; // doubled energy for s calculation |
---|
814 | #ifdef debug |
---|
815 | G4cout<<"G4QCollision::PostStDoIt: 2*nuEnergy="<<dKinE<<"(MeV), PDG="<<projPDG<<G4endl; |
---|
816 | #endif |
---|
817 | G4ParticleMomentum dir = projHadron->GetMomentumDirection(); // unit vector |
---|
818 | G4double ml = mu; |
---|
819 | G4double ml2 = mu2; |
---|
820 | //G4double mlN = muN; |
---|
821 | G4double mlN2= muN2; |
---|
822 | G4double fmlN= fmuN; |
---|
823 | G4double mlsN= musN; |
---|
824 | //G4double mlP = muP; |
---|
825 | G4double mlP2= muP2; |
---|
826 | G4double fmlP= fmuP; |
---|
827 | G4double mlsP= musP; |
---|
828 | G4double mldM= mudM; |
---|
829 | //G4double mlD = muD; |
---|
830 | G4double mlD2= muD2; |
---|
831 | if(aProjPDG==12) |
---|
832 | { |
---|
833 | ml = me; |
---|
834 | ml2 = me2; |
---|
835 | //mlN = meN; |
---|
836 | mlN2= meN2; |
---|
837 | fmlN= fmeN; |
---|
838 | mlsN= mesN; |
---|
839 | //mlP = meP; |
---|
840 | mlP2= meP2; |
---|
841 | fmlP= fmeP; |
---|
842 | mlsP= mesP; |
---|
843 | mldM= medM; |
---|
844 | //mlD = meD; |
---|
845 | mlD2= meD2; |
---|
846 | } |
---|
847 | G4VQCrossSection* CSmanager =G4QNuMuNuclearCrossSection::GetPointer(); // (nu,l) |
---|
848 | G4VQCrossSection* CSmanager2=G4QNuNuNuclearCrossSection::GetPointer(); // (nu,nu) |
---|
849 | proj4M=G4LorentzVector(dir*kinEnergy,kinEnergy); // temporary |
---|
850 | G4bool nuanu=true; |
---|
851 | scatPDG=13; // Prototype = secondary scattered mu- |
---|
852 | if(projPDG==-14) |
---|
853 | { |
---|
854 | nuanu=false; // Anti-neutrino |
---|
855 | CSmanager=G4QANuMuNuclearCrossSection::GetPointer(); // (anu,mu+) CC @@ open |
---|
856 | CSmanager=G4QANuANuNuclearCrossSection::GetPointer(); // (anu,anu) NC @@ open |
---|
857 | scatPDG=-13; // secondary scattered mu+ |
---|
858 | } |
---|
859 | else if(projPDG==12) |
---|
860 | { |
---|
861 | CSmanager=G4QNuENuclearCrossSection::GetPointer(); // @@ open (only CC is changed) |
---|
862 | scatPDG=11; // secondary scattered e- |
---|
863 | } |
---|
864 | else if(projPDG==-12) |
---|
865 | { |
---|
866 | nuanu=false; // anti-neutrino |
---|
867 | CSmanager=G4QANuENuclearCrossSection::GetPointer(); // (anu,e+) CC @@ open |
---|
868 | CSmanager=G4QANuANuNuclearCrossSection::GetPointer(); // (anu,anu) NC @@ open |
---|
869 | scatPDG=-11; // secondary scattered e+ |
---|
870 | } |
---|
871 | // @@ Probably this is not necessary any more |
---|
872 | G4double xSec1=CSmanager->GetCrossSection(false,Momentum,Z,N,projPDG); //Recalculate XS |
---|
873 | G4double xSec2=CSmanager2->GetCrossSection(false,Momentum,Z,N,projPDG);//Recalculate XS |
---|
874 | G4double xSec=xSec1+xSec2; |
---|
875 | // @@ check a possibility to separate p, n, or alpha (!) |
---|
876 | if(xSec <= 0.) // The cross-section = 0 -> Do Nothing |
---|
877 | { |
---|
878 | G4cerr<<"G4QCollision::PSDoIt:nuE="<<kinEnergy<<",X1="<<xSec1<<",X2="<<xSec2<<G4endl; |
---|
879 | //Do Nothing Action insead of the reaction |
---|
880 | aParticleChange.ProposeEnergy(kinEnergy); |
---|
881 | aParticleChange.ProposeLocalEnergyDeposit(0.); |
---|
882 | aParticleChange.ProposeMomentumDirection(dir); |
---|
883 | aParticleChange.ProposeTrackStatus(fAlive); |
---|
884 | return G4VDiscreteProcess::PostStepDoIt(track,step); |
---|
885 | } |
---|
886 | G4bool secnu=false; |
---|
887 | if(xSec*G4UniformRand()>xSec1) // recover neutrino/antineutrino |
---|
888 | { |
---|
889 | if(scatPDG>0) scatPDG++; |
---|
890 | else scatPDG--; |
---|
891 | secnu=true; |
---|
892 | } |
---|
893 | scat=true; // event with changed scattered projectile |
---|
894 | G4double totCS1 = CSmanager->GetLastTOTCS(); // the last total cross section1(isotope?) |
---|
895 | G4double totCS2 = CSmanager2->GetLastTOTCS();// the last total cross section2(isotope?) |
---|
896 | G4double totCS = totCS1+totCS2; // the last total cross section (isotope?) |
---|
897 | if(std::fabs(xSec-totCS*millibarn)/xSec>.0001) |
---|
898 | G4cout<<"-Warning-G4QCollision::PostStepDoIt: xS="<<xSec<<"# CS="<<totCS<<G4endl; |
---|
899 | G4double qelCS1 = CSmanager->GetLastQELCS(); // the last quasi-elastic cross section1 |
---|
900 | G4double qelCS2 = CSmanager2->GetLastQELCS();// the last quasi-elastic cross section2 |
---|
901 | G4double qelCS = qelCS1+qelCS2; // the last quasi-elastic cross section |
---|
902 | if(totCS - qelCS < 0.) // only at low energies |
---|
903 | { |
---|
904 | totCS = qelCS; |
---|
905 | totCS1 = qelCS1; |
---|
906 | totCS2 = qelCS2; |
---|
907 | } |
---|
908 | // make different definitions for neutrino and antineutrino |
---|
909 | G4double mIN=mProt; // Just a prototype (for anu, Z=1, N=0) |
---|
910 | G4double mOT=mNeut; |
---|
911 | G4double OT=mlN2; |
---|
912 | G4double mOT2=mNeut2; |
---|
913 | G4double mlOT=fmlN; |
---|
914 | G4double mlsOT=mlsN; |
---|
915 | if(secnu) |
---|
916 | { |
---|
917 | if(am*G4UniformRand()>Z) // Neutron target |
---|
918 | { |
---|
919 | targPDG-=1; // subtract neutron |
---|
920 | projPDG=2112; // neutron is going out |
---|
921 | mIN =mNeut; |
---|
922 | OT =mNeut2; |
---|
923 | mOT2=mNeut2; |
---|
924 | mlOT=0.; |
---|
925 | mlsOT=mNeut2; |
---|
926 | } |
---|
927 | else |
---|
928 | { |
---|
929 | targPDG-=1000; // subtract neutron |
---|
930 | projPDG=2212; // neutron is going out |
---|
931 | mOT =mProt; |
---|
932 | OT =mProt2; |
---|
933 | mOT2 =mProt2; |
---|
934 | mlOT =0.; |
---|
935 | mlsOT=mProt2; |
---|
936 | } |
---|
937 | ml=0.; |
---|
938 | ml2=0.; |
---|
939 | mldM=0.; |
---|
940 | mlD2=mPPi2; |
---|
941 | G4QPDGCode targQPDG(targPDG); |
---|
942 | G4double rM=targQPDG.GetMass(); |
---|
943 | mIN=tM-rM; // bounded in-mass of the neutron |
---|
944 | tM=rM; |
---|
945 | } |
---|
946 | else if(nuanu) |
---|
947 | { |
---|
948 | targPDG-=1; // Neutrino -> subtract neutron |
---|
949 | G4QPDGCode targQPDG(targPDG); |
---|
950 | G4double rM=targQPDG.GetMass(); |
---|
951 | mIN=tM-rM; // bounded in-mass of the neutron |
---|
952 | tM=rM; |
---|
953 | mOT=mProt; |
---|
954 | OT=mlP2; |
---|
955 | mOT2=mProt2; |
---|
956 | mlOT=fmlP; |
---|
957 | mlsOT=mlsP; |
---|
958 | projPDG=2212; // proton is going out |
---|
959 | } |
---|
960 | else |
---|
961 | { |
---|
962 | if(Z>1||N>0) // Calculate the splitted mass |
---|
963 | { |
---|
964 | targPDG-=1000; // Anti-Neutrino -> subtract proton |
---|
965 | G4QPDGCode targQPDG(targPDG); |
---|
966 | G4double rM=targQPDG.GetMass(); |
---|
967 | mIN=tM-rM; // bounded in-mass of the proton |
---|
968 | tM=rM; |
---|
969 | } |
---|
970 | else |
---|
971 | { |
---|
972 | targPDG=0; |
---|
973 | mIN=tM; |
---|
974 | tM=0.; |
---|
975 | } |
---|
976 | projPDG=2112; // neutron is going out |
---|
977 | } |
---|
978 | G4double s=mIN*(mIN+dKinE); // s=(M_cm)^2=m2+2mE (m=targetMass,E=E_nu) |
---|
979 | #ifdef debug |
---|
980 | G4cout<<"G4QCollision::PostStDoIt: s="<<s<<" >? OT="<<OT<<", mlD2="<<mlD2<<G4endl; |
---|
981 | #endif |
---|
982 | if(s<=OT) // *** Do nothing solution *** |
---|
983 | { |
---|
984 | //Do NothingToDo Action insead of the reaction (@@ Can we make it common?) |
---|
985 | G4cout<<"G4QCollision::PostStepDoIt: tooSmallFinalMassOfCompound: DoNothing"<<G4endl; |
---|
986 | aParticleChange.ProposeEnergy(kinEnergy); |
---|
987 | aParticleChange.ProposeLocalEnergyDeposit(0.); |
---|
988 | aParticleChange.ProposeMomentumDirection(dir); |
---|
989 | aParticleChange.ProposeTrackStatus(fAlive); |
---|
990 | return G4VDiscreteProcess::PostStepDoIt(track,step); |
---|
991 | } |
---|
992 | #ifdef debug |
---|
993 | G4cout<<"G4QCollision::PostStDoIt: Stop and kill the projectile neutrino"<<G4endl; |
---|
994 | #endif |
---|
995 | aParticleChange.ProposeEnergy(0.); |
---|
996 | aParticleChange.ProposeTrackStatus(fStopAndKill); // the initial neutrino is killed |
---|
997 | // There is no way back from here |
---|
998 | |
---|
999 | if ( ((secnu || !nuanu || N) && totCS*G4UniformRand() < qelCS) || s < mlD2 ) |
---|
1000 | { // Quasi-Elastic interaction |
---|
1001 | G4double Q2=0.; // Simulate transferred momentum, in MeV^2 |
---|
1002 | if(secnu) Q2=CSmanager2->GetQEL_ExchangeQ2(); |
---|
1003 | else Q2=CSmanager->GetQEL_ExchangeQ2(); |
---|
1004 | #ifdef debug |
---|
1005 | G4cout<<"G4QCollision::PostStDoIt:QuasiEl(nu="<<secnu<<"),s="<<s<<",Q2="<<Q2<<G4endl; |
---|
1006 | #endif |
---|
1007 | //G4double ds=s+s; // doubled s |
---|
1008 | G4double sqs=std::sqrt(s); // M_cm |
---|
1009 | G4double dsqs=sqs+sqs; // 2*M_cm |
---|
1010 | G4double pi=(s-mIN*mIN)/dsqs; // initial momentum in CMS (checked MK) |
---|
1011 | G4double dpi=pi+pi; // doubled initial momentum in CMS |
---|
1012 | G4double sd=s-mlsOT; // s-ml2-mOT2 (mlsOT=m^2_neut+m^2_lept) |
---|
1013 | G4double qo2=(sd*sd-mlOT)/dsqs; // squared momentum of secondaries in CMS |
---|
1014 | G4double qo=std::sqrt(qo2); // momentum of secondaries in CMS |
---|
1015 | G4double cost=(dpi*std::sqrt(qo2+ml2)-Q2-ml2)/dpi/qo; // cos(theta) in CMS (chck MK) |
---|
1016 | G4LorentzVector t4M(0.,0.,0.,mIN); // 4mom of the effective target |
---|
1017 | G4LorentzVector c4M=t4M+proj4M; // 4mom of the compound system |
---|
1018 | t4M.setT(mOT); // now it is 4mom of the outgoing nucleon |
---|
1019 | scat4M=G4LorentzVector(0.,0.,0.,ml); // 4mom of the scattered muon |
---|
1020 | if(!G4QHadron(c4M).RelDecayIn2(scat4M, t4M, proj4M, cost, cost)) |
---|
1021 | { |
---|
1022 | G4cerr<<"G4QCol::PSD:c4M="<<c4M<<sqs<<",mM="<<ml<<",tM="<<mOT<<",c="<<cost<<G4endl; |
---|
1023 | throw G4QException("G4QCollision::HadronizeQuasm: Can't dec QE nu,lept Compound"); |
---|
1024 | } |
---|
1025 | proj4M=t4M; // 4mom of the new projectile nucleon |
---|
1026 | } |
---|
1027 | else // ***** Non Quasi Elastic interaction |
---|
1028 | { |
---|
1029 | |
---|
1030 | if ( (secnu && projPDG == 2212) || (!secnu && projPDG == 2112) ) { |
---|
1031 | targPDG+=1; // Recover target PDG, |
---|
1032 | } else if ( (secnu && projPDG == 2112) || (!secnu && projPDG == 2212) ) { |
---|
1033 | targPDG+=1000; // if not quasiEl |
---|
1034 | } |
---|
1035 | G4double Q2=0; // Simulate transferred momentum, in MeV^2 |
---|
1036 | if(secnu) Q2=CSmanager->GetNQE_ExchangeQ2(); |
---|
1037 | else Q2=CSmanager2->GetNQE_ExchangeQ2(); |
---|
1038 | #ifdef debug |
---|
1039 | G4cout<<"G4QColl::PStDoIt: MultiPeriferal s="<<s<<",Q2="<<Q2<<",T="<<targPDG<<G4endl; |
---|
1040 | #endif |
---|
1041 | if(secnu) projPDG=CSmanager2->GetExchangePDGCode();// PDG Code of the effective gamma |
---|
1042 | else projPDG=CSmanager->GetExchangePDGCode(); // PDG Code of the effective pion |
---|
1043 | //@@ Temporary made only for direct interaction and for N=3 (good for small Q2) |
---|
1044 | //@@ inFuture use N=GetNPartons and directFraction=GetDirectPart, @@ W2... |
---|
1045 | G4double r=G4UniformRand(); |
---|
1046 | G4double r1=0.5; // (1-x) |
---|
1047 | if(r<0.5) r1=std::sqrt(r+r)*(.5+.1579*(r-.5)); |
---|
1048 | else if(r>0.5) r1=1.-std::sqrt(2.-r-r)*(.5+.1579*(.5-r)); |
---|
1049 | G4double xn=1.-mldM/Momentum; // Normalization of (1-x) [x>mldM/Mom] |
---|
1050 | G4double x1=xn*r1; // (1-x) |
---|
1051 | G4double x=1.-x1; // x=2k/M |
---|
1052 | //G4double W2=(hdM2+Q2/x)*x1; // W2 candidate |
---|
1053 | G4double mx=hdM*x; // Part of the target to interact with |
---|
1054 | G4double we=Q2/(mx+mx); // transfered energy |
---|
1055 | if(we>=kinEnergy-ml-.001) we=kinEnergy-ml-.0001; // safety to avoid nan=sqrt(neg) |
---|
1056 | G4double pot=kinEnergy-we; // energy of the secondary lepton |
---|
1057 | G4double mlQ2=ml2+Q2; |
---|
1058 | G4double cost=(pot-mlQ2/dKinE)/std::sqrt(pot*pot-ml2); // LS cos(theta) |
---|
1059 | if(std::fabs(cost)>1) |
---|
1060 | { |
---|
1061 | #ifdef debug |
---|
1062 | G4cout<<"*G4QCollision::PostStDoIt: cost="<<cost<<", Q2="<<Q2<<", nu="<<we<<", mx=" |
---|
1063 | <<mx<<", pot="<<pot<<", 2KE="<<dKinE<<G4endl; |
---|
1064 | #endif |
---|
1065 | if(cost>1.) cost=1.; |
---|
1066 | else cost=-1.; |
---|
1067 | pot=mlQ2/dKinE+dKinE*ml2/mlQ2; // extreme output momentum |
---|
1068 | } |
---|
1069 | G4double lEn=std::sqrt(pot*pot+ml2); // Lepton energy |
---|
1070 | G4double lPl=pot*cost; // Lepton longitudinal momentum |
---|
1071 | G4double lPt=pot*std::sqrt(1.-cost*cost); // Lepton transverse momentum |
---|
1072 | std::pair<G4double,G4double> d2d=Random2DDirection(); // Randomize phi |
---|
1073 | G4double lPx=lPt*d2d.first; |
---|
1074 | G4double lPy=lPt*d2d.second; |
---|
1075 | G4ThreeVector vdir=proj4M.vect(); // 3D momentum of the projectile |
---|
1076 | G4ThreeVector vz= vdir.unit(); // Ort in the direction of the projectile |
---|
1077 | G4ThreeVector vv= vz.orthogonal(); // Not normed orthogonal vector (!) |
---|
1078 | G4ThreeVector vx= vv.unit(); // First ort orthogonal to the direction |
---|
1079 | G4ThreeVector vy= vz.cross(vx); // Second ort orthoganal to the direction |
---|
1080 | G4ThreeVector lP= lPl*vz+lPx*vx+lPy*vy; // 3D momentum of the scattered lepton |
---|
1081 | scat4M=G4LorentzVector(lP,lEn); // 4mom of the scattered lepton |
---|
1082 | proj4M-=scat4M; // 4mom of the W/Z (effective pion/gamma) |
---|
1083 | #ifdef debug |
---|
1084 | G4cout<<"G4QCollision::PostStDoIt: proj4M="<<proj4M<<", ml="<<ml<<G4endl; |
---|
1085 | #endif |
---|
1086 | // Check that the en/mom transfer is possible, if not -> elastic |
---|
1087 | G4int fintPDG=targPDG; // Prototype for the compound nucleus |
---|
1088 | if(!secnu) |
---|
1089 | { |
---|
1090 | if(projPDG<0) fintPDG-= 999; |
---|
1091 | else fintPDG+= 999; |
---|
1092 | } |
---|
1093 | G4double fM=G4QPDGCode(fintPDG).GetMass();// compound nucleus Mass (MeV) |
---|
1094 | G4double fM2=fM*fM; |
---|
1095 | G4LorentzVector tg4M=G4LorentzVector(0.,0.,0.,tgM); |
---|
1096 | G4LorentzVector c4M=tg4M+proj4M; |
---|
1097 | #ifdef debug |
---|
1098 | G4cout<<"G4QCol::PSDI:fM2="<<fM2<<" <? mc4M="<<c4M.m2()<<",dM="<<fM-tgM<<G4endl; |
---|
1099 | #endif |
---|
1100 | if(fM2>=c4M.m2()) // Elastic scattering should be done |
---|
1101 | { |
---|
1102 | G4LorentzVector tot4M=tg4M+proj4M+scat4M; // recover the total 4-momentum |
---|
1103 | s=tot4M.m2(); |
---|
1104 | G4double fs=s-fM2-ml2; |
---|
1105 | G4double fMl=fM2*ml2; |
---|
1106 | G4double hQ2max=(fs*fs/2-fMl-fMl)/s; // Maximum possible Q2/2 |
---|
1107 | G4double cost=1.-Q2/hQ2max; // cos(theta) in CMS (use MultProd Q2) |
---|
1108 | #ifdef debug |
---|
1109 | G4cout<<"G4QC::PSDI:ct="<<cost<<",Q2="<<Q2<<",hQ2="<<hQ2max<<",4M="<<tot4M<<G4endl; |
---|
1110 | #endif |
---|
1111 | G4double acost=std::fabs(cost); |
---|
1112 | if(acost>1.) |
---|
1113 | { |
---|
1114 | if(acost>1.001) G4cout<<"-Warning-G4QCollision::PostStDoIt: cost="<<cost<<G4endl; |
---|
1115 | if (cost> 1.) cost= 1.; |
---|
1116 | else if(cost<-1.) cost=-1.; |
---|
1117 | } |
---|
1118 | G4LorentzVector reco4M=G4LorentzVector(0.,0.,0.,fM); // 4mom of the recoilNucleus |
---|
1119 | scat4M=G4LorentzVector(0.,0.,0.,ml); // 4mom of the scatteredLepton |
---|
1120 | G4LorentzVector dir4M=tot4M-G4LorentzVector(0.,0.,0.,(tot4M.e()-ml)*.01); |
---|
1121 | if(!G4QHadron(tot4M).RelDecayIn2(scat4M, reco4M, dir4M, cost, cost)) |
---|
1122 | { |
---|
1123 | G4cerr<<"G4QC::PSDI:t4M="<<tot4M<<",lM="<<ml<<",rM="<<fM<<",cost="<<cost<<G4endl; |
---|
1124 | //G4Exception("G4QCollision::PostStepDoIt:","027",FatalException,"ElasticDecay"); |
---|
1125 | } |
---|
1126 | #ifdef debug |
---|
1127 | G4cout<<"G4QCol::PStDoI:l4M="<<scat4M<<"+r4M="<<reco4M<<"="<<scat4M+reco4M<<G4endl; |
---|
1128 | #endif |
---|
1129 | // ---------------------------------------------------- |
---|
1130 | G4ParticleDefinition* theDefinition=0; // Prototype of a particle for E-Secondaries |
---|
1131 | // Fill scattered lepton |
---|
1132 | if (scatPDG==-11) theDefinition = G4Positron::Positron(); |
---|
1133 | else if(scatPDG== 11) theDefinition = G4Electron::Electron(); |
---|
1134 | else if(scatPDG== 13) theDefinition = G4MuonMinus::MuonMinus(); |
---|
1135 | else if(scatPDG==-13) theDefinition = G4MuonPlus::MuonPlus(); |
---|
1136 | //else if(scatPDG== 15) theDefinition = G4TauMinus::TauMinus(); |
---|
1137 | //else if(scatPDG==-15) theDefinition = G4TauPlus::TauPlus(); |
---|
1138 | if (scatPDG==-12) theDefinition = G4AntiNeutrinoE::AntiNeutrinoE(); |
---|
1139 | else if(scatPDG== 12) theDefinition = G4NeutrinoE::NeutrinoE(); |
---|
1140 | else if(scatPDG== 14) theDefinition = G4NeutrinoMu::NeutrinoMu(); |
---|
1141 | else if(scatPDG==-14) theDefinition = G4AntiNeutrinoMu::AntiNeutrinoMu(); |
---|
1142 | //else if(scatPDG== 16) theDefinition = G4NeutrinoTau::NeutrinoTau(); |
---|
1143 | //else if(scatPDG==-16) theDefinition = G4AntiNeutrinoTau::AntiNeutrinoTau(); |
---|
1144 | else G4cout<<"-Warning-G4QCollision::PostStDoIt: UnknownLepton="<<scatPDG<<G4endl; |
---|
1145 | G4DynamicParticle* theScL = new G4DynamicParticle(theDefinition,scat4M); |
---|
1146 | G4Track* scatLep = new G4Track(theScL, localtime, position ); // scattered |
---|
1147 | scatLep->SetWeight(weight); // weighted |
---|
1148 | scatLep->SetTouchableHandle(trTouchable); // residual |
---|
1149 | aParticleChange.AddSecondary(scatLep); // lepton |
---|
1150 | // Fill residual nucleus |
---|
1151 | if (fintPDG==90000001) theDefinition = G4Neutron::Neutron(); // neutron |
---|
1152 | else if(fintPDG==90001000) theDefinition = G4Proton::Proton(); // proton |
---|
1153 | else // ion |
---|
1154 | { |
---|
1155 | G4int fm=static_cast<G4int>(fintPDG/1000000); // Strange part |
---|
1156 | G4int ZN=fintPDG-1000000*fm; |
---|
1157 | G4int rZ=static_cast<G4int>(ZN/1000); |
---|
1158 | G4int rA=ZN-999*rZ; |
---|
1159 | theDefinition = G4ParticleTable::GetParticleTable()->FindIon(rZ,rA,0,rZ); |
---|
1160 | } |
---|
1161 | G4DynamicParticle* theReN = new G4DynamicParticle(theDefinition,reco4M); |
---|
1162 | G4Track* scatReN = new G4Track(theReN, localtime, position ); // scattered |
---|
1163 | scatReN->SetWeight(weight); // weighted |
---|
1164 | scatReN->SetTouchableHandle(trTouchable); // residual |
---|
1165 | aParticleChange.AddSecondary(scatReN); // nucleus |
---|
1166 | return G4VDiscreteProcess::PostStepDoIt(track, step); |
---|
1167 | } |
---|
1168 | } |
---|
1169 | // |
---|
1170 | // quasi-elastic (& pickup process) for p+A(Z,N) |
---|
1171 | // |
---|
1172 | } |
---|
1173 | else if (aProjPDG == 2212 && Z > 0 && N > 0) |
---|
1174 | //else if(2>3) |
---|
1175 | { |
---|
1176 | G4QuasiFreeRatios* qfMan=G4QuasiFreeRatios::GetPointer(); |
---|
1177 | std::pair<G4double,G4double> fief=qfMan->GetRatios(momentum, aProjPDG, Z, N); |
---|
1178 | G4double qepart=fief.first*fief.second; |
---|
1179 | // Keep QE part for the quasi-free nucleons |
---|
1180 | const G4int lCl=3; // The last clProb[lCl]==1. by definition, MUST be increasing |
---|
1181 | G4double clProb[lCl]={.65,.85,.95};// N/P,D,t/He3,He4, integratedProb for .65,.2,.1,.05 |
---|
1182 | if(qepart>0.45) qepart=.45; // Quasielastic part is too large - shrink |
---|
1183 | else qepart/=clProb[0]; // Add corresponding number of 2N, 3N, & 4N clusters |
---|
1184 | G4double pickup=1.-qepart; // Estimate the rest of the cross-section |
---|
1185 | G4double thresh=100.; |
---|
1186 | if(momentum > thresh) pickup*=50./momentum/std::pow((double)Z+N,(double)third); // 50. is a par(!) |
---|
1187 | // pickup = 0.; // To exclude the pickup process |
---|
1188 | if (N) pickup+=qepart; |
---|
1189 | else pickup =qepart; |
---|
1190 | G4double rnd=G4UniformRand(); |
---|
1191 | #ifdef ldebug |
---|
1192 | G4cout<<"-->G4QCol::PSD:QE[p("<<proj4M<<")+(Z="<<Z<<",N="<<N<<")]="<<qepart |
---|
1193 | <<", pickup="<<pickup<<G4endl; |
---|
1194 | #endif |
---|
1195 | if(rnd<pickup) // Make a quasi free scattering (out:A-1,h,N) @@ KinLim,CoulBar,PauliBl |
---|
1196 | { |
---|
1197 | G4double dmom=91.; // Fermi momentum (proto default for a deuteron) |
---|
1198 | G4double fmm=287.; // @@ Can be A-dependent |
---|
1199 | if(Z>1||N>1) dmom=fmm*std::pow(-std::log(G4UniformRand()),third); |
---|
1200 | // Values to be redefined for quasi-elastic |
---|
1201 | G4LorentzVector r4M(0.,0.,0.,0.); // Prototype of 4mom of the residual nucleus |
---|
1202 | G4LorentzVector n4M(0.,0.,0.,0.); // Prototype of 4mom of the quasi-cluster |
---|
1203 | G4int nPDG=90000001; // Prototype for quasi-cluster mass calculation |
---|
1204 | G4int restPDG=targPDG; // Prototype should be reduced by quasi-cluster |
---|
1205 | G4int rA=Z+N-1; // Prototype for the residualNucl definition |
---|
1206 | G4int rZ=Z; // residZ: OK for the quasi-free neutron |
---|
1207 | G4int nA=1; // Prototype for the quasi-cluster definition |
---|
1208 | G4int nZ=0; // nA=1,nZ=0: OK for the quasi-free neutron |
---|
1209 | G4double qM=mNeut; // Free mass of the quasi-free cluster |
---|
1210 | G4int A = Z + N; // Baryon number of the nucleus |
---|
1211 | if(rnd<qepart) |
---|
1212 | { |
---|
1213 | // ===> First decay a nucleus in a nucleon and a residual (A-1) nucleus |
---|
1214 | // Calculate cluster probabilities (n,p,d,t,he3,he4 now only, can use UpdateClusters) |
---|
1215 | G4double base=1.; // Base for randomization (can be reduced by totZ & totN) |
---|
1216 | G4int max=lCl; // Number of boundaries (can be reduced by totZ & totN) |
---|
1217 | // Take into account that at least one nucleon must be left ! |
---|
1218 | if (Z<2 || N<2 || A<5) base = clProb[--max]; // Alpha cluster is impossible |
---|
1219 | if ( (Z > 1 && N < 2) || (Z < 2 && N > 1) ) |
---|
1220 | base=(clProb[max]+clProb[max-1])/2; // t or He3 is impossible |
---|
1221 | if ( (Z < 2 && N < 2) || A < 4) base=clProb[--max];// He3 & t clusters are impossible |
---|
1222 | if(A<3) base=clProb[--max]; // Deuteron cluster is impossible |
---|
1223 | G4int cln=0; // Cluster#0 (Default for the selected nucleon) |
---|
1224 | if(max) // Not only nucleons are possible |
---|
1225 | //if(2>3) |
---|
1226 | { |
---|
1227 | G4double ran=base*G4UniformRand(); // Base can be reduced |
---|
1228 | G4int ic=0; // Start from the smallest cluster boundary |
---|
1229 | while(ic<max) if(ran>clProb[ic++]) cln=ic; |
---|
1230 | } |
---|
1231 | G4ParticleDefinition* theDefinition; // Prototype for qfNucleon |
---|
1232 | G4bool cp1 = cln+2==A; // A=ClusterBN+1 condition |
---|
1233 | if(!cln || cp1) // Split in nucleon + (A-1) with Fermi momentum |
---|
1234 | { |
---|
1235 | G4int nln=0; |
---|
1236 | if(cln==2) nln=1; // @@ only for cp1: t/He3 choice from A=4 |
---|
1237 | // mass(A)=tM. Calculate masses of A-1 (rM) and mN (mNeut or mProt bounded mass) |
---|
1238 | if ( ((!cln || cln == 2) && G4UniformRand()*(A-cln) > (N-nln)) || |
---|
1239 | ((cln == 3 || cln == 1) && Z > N) ) |
---|
1240 | { |
---|
1241 | nPDG=90001000; // Update quasi-free nucleon PDGCode to P |
---|
1242 | nZ=1; // Change charge of the quasiFree nucleon |
---|
1243 | qM=mProt; // Update quasi-free nucleon mass |
---|
1244 | rZ--; // Reduce the residual Z |
---|
1245 | restPDG-=1000; // Reduce the residual PDGCode |
---|
1246 | } |
---|
1247 | else restPDG--; |
---|
1248 | G4LorentzVector t4M(0.,0.,0.,tM); // 4m of the target nucleus to be decayed |
---|
1249 | G4double rM=G4QPDGCode(restPDG).GetMass();// Mass of the residual nucleus |
---|
1250 | r4M=G4LorentzVector(0.,0.,0.,rM); // 4mom of the residual nucleus |
---|
1251 | G4double rM2=rM*rM; |
---|
1252 | G4double nM=std::sqrt(rM2+tM*tM-(tM+tM)*std::sqrt(rM2+dmom*dmom));// M of q-nucleon |
---|
1253 | n4M=G4LorentzVector(0.,0.,0.,nM); // 4mom of the quasi-nucleon |
---|
1254 | #ifdef qedebug |
---|
1255 | G4cout<<"G4QCollis::PStDoIt:QE,p="<<dmom<<",tM="<<tM<<",R="<<rM<<",N="<<nM<<G4endl; |
---|
1256 | #endif |
---|
1257 | if(!G4QHadron(t4M).DecayIn2(r4M, n4M)) |
---|
1258 | { |
---|
1259 | G4cerr<<"G4QCol::PostStDoIt: M="<<tM<<"<rM="<<rM<<"+nM="<<nM<<"="<<rM+nM<<G4endl; |
---|
1260 | throw G4QException("G4QCollision::HadronizeQuasm:Can'tDec totNuc->QENuc+ResNuc"); |
---|
1261 | } |
---|
1262 | #ifdef qedebug |
---|
1263 | G4cout<<"G4QCol::PStDoIt:QE-N,RA="<<r4M.rho()<<r4M<<",QN="<<n4M.rho()<<n4M<<G4endl; |
---|
1264 | #endif |
---|
1265 | if(cp1 && cln) // Quasi-cluster case: swap the output |
---|
1266 | { |
---|
1267 | qM=rM; // Scattering will be made on a cluster |
---|
1268 | nln=nPDG; |
---|
1269 | nPDG=restPDG; |
---|
1270 | restPDG=nln; |
---|
1271 | t4M=n4M; |
---|
1272 | n4M=r4M; |
---|
1273 | r4M=t4M; |
---|
1274 | nln=nZ; |
---|
1275 | nZ=rZ; |
---|
1276 | rZ=nln; |
---|
1277 | nln=nA; |
---|
1278 | nA=rA; |
---|
1279 | rA=nln; |
---|
1280 | } |
---|
1281 | } |
---|
1282 | else // Split the cluster (with or w/o "Fermi motion" and "Fermi decay") |
---|
1283 | { |
---|
1284 | if(cln==1) |
---|
1285 | { |
---|
1286 | nPDG=90001001; // Deuteron |
---|
1287 | qM=mDeut; |
---|
1288 | nA=2; |
---|
1289 | nZ=1; |
---|
1290 | restPDG-=1001; |
---|
1291 | // Recalculate dmom |
---|
1292 | G4ThreeVector sumv=G4ThreeVector(0.,0.,dmom) + |
---|
1293 | fmm*std::pow(-std::log(G4UniformRand()),third)*G4RandomDirection(); |
---|
1294 | dmom=sumv.mag(); |
---|
1295 | } |
---|
1296 | else if(cln==2) |
---|
1297 | { |
---|
1298 | nA=3; |
---|
1299 | if(G4UniformRand()*(A-2)>(N-1)) // He3 |
---|
1300 | { |
---|
1301 | nPDG=90002001; |
---|
1302 | qM=mHel3; |
---|
1303 | nZ=2; |
---|
1304 | restPDG-=2001; |
---|
1305 | } |
---|
1306 | else // tritium |
---|
1307 | { |
---|
1308 | nPDG=90001002; |
---|
1309 | qM=mTrit; |
---|
1310 | nZ=1; |
---|
1311 | restPDG-=1002; |
---|
1312 | } |
---|
1313 | // Recalculate dmom |
---|
1314 | G4ThreeVector sumv=G4ThreeVector(0.,0.,dmom) + |
---|
1315 | fmm*std::pow(-std::log(G4UniformRand()),third)*G4RandomDirection()+ |
---|
1316 | fmm*std::pow(-std::log(G4UniformRand()),third)*G4RandomDirection(); |
---|
1317 | dmom=sumv.mag(); |
---|
1318 | } |
---|
1319 | else |
---|
1320 | { |
---|
1321 | nPDG=90002002; // Alpha |
---|
1322 | qM=mAlph; |
---|
1323 | nA=4; |
---|
1324 | nZ=2; |
---|
1325 | restPDG-=2002; |
---|
1326 | G4ThreeVector sumv=G4ThreeVector(0.,0.,dmom) + |
---|
1327 | fmm*std::pow(-std::log(G4UniformRand()),third)*G4RandomDirection()+ |
---|
1328 | fmm*std::pow(-std::log(G4UniformRand()),third)*G4RandomDirection()+ |
---|
1329 | fmm*std::pow(-std::log(G4UniformRand()),third)*G4RandomDirection(); |
---|
1330 | dmom=sumv.mag(); |
---|
1331 | } |
---|
1332 | rA=A-nA; |
---|
1333 | rZ=Z-nZ; |
---|
1334 | // This is a simple case of cluster at rest |
---|
1335 | //G4double rM=G4QPDGCode(restPDG).GetMass();// Mass of the residual nucleus |
---|
1336 | //r4M=G4LorentzVector(0.,0.,0.,rM); // 4mom of the residual nucleus |
---|
1337 | //n4M=G4LorentzVector(0.,0.,0.,tM-rM); // 4mom of the quasi-free cluster |
---|
1338 | // --- End of the "simple case of cluster at rest" |
---|
1339 | // Make a fake quasi-Fermi distribution for clusters (clusters are not at rest) |
---|
1340 | G4LorentzVector t4M(0.,0.,0.,tM); // 4m of the target nucleus to be decayed |
---|
1341 | G4double rM=G4QPDGCode(restPDG).GetMass();// Mass of the residual nucleus |
---|
1342 | r4M=G4LorentzVector(0.,0.,0.,rM); // 4mom of the residual nucleus |
---|
1343 | G4double rM2=rM*rM; |
---|
1344 | G4double nM=std::sqrt(rM2+tM*tM-(tM+tM)*std::sqrt(rM2+dmom*dmom));// M of q-cluster |
---|
1345 | n4M=G4LorentzVector(0.,0.,0.,nM); // 4mom of the quasi-nucleon |
---|
1346 | #ifdef qedebug |
---|
1347 | G4cout<<"G4QCollis::PStDoIt:QEC,p="<<dmom<<",T="<<tM<<",R="<<rM<<",N="<<nM<<G4endl; |
---|
1348 | #endif |
---|
1349 | if(!G4QHadron(t4M).DecayIn2(r4M, n4M)) |
---|
1350 | { |
---|
1351 | G4cerr<<"G4QCol::PostStDoIt: M="<<tM<<"<rM="<<rM<<"+cM="<<nM<<"="<<rM+nM<<G4endl; |
---|
1352 | throw G4QException("G4QCollision::HadronizeQuasm:Can'tDec totNuc->QEClu+ResNuc"); |
---|
1353 | } |
---|
1354 | // --- End of the moving cluster implementation --- |
---|
1355 | #ifdef qedebug |
---|
1356 | G4cout<<"G4QCol::PStDoIt:QEC,RN="<<r4M.rho()<<r4M<<",QCl="<<n4M.rho()<<n4M<<G4endl; |
---|
1357 | #endif |
---|
1358 | } |
---|
1359 | G4LorentzVector s4M=n4M+proj4M; // Tot 4-momentum for scattering |
---|
1360 | G4double prjM2 = proj4M.m2(); // Squared mass of the projectile |
---|
1361 | G4double prjM = std::sqrt(prjM2); // @@ Get from pPDG (?) |
---|
1362 | G4double minM = prjM+qM; // Min mass sum for the final products |
---|
1363 | G4double cmM2 =s4M.m2(); |
---|
1364 | if(cmM2>minM*minM) |
---|
1365 | { |
---|
1366 | #ifdef qedebug |
---|
1367 | G4cout<<"G4QCol::PStDoIt:***Enter***,cmM2="<<cmM2<<" > minM2="<<minM*minM<<G4endl; |
---|
1368 | #endif |
---|
1369 | // Estimate and randomize charge-exchange with quasi-free cluster |
---|
1370 | G4bool chex=false; // Flag of the charge exchange scattering |
---|
1371 | G4ParticleDefinition* projpt=G4Proton::Proton(); // Prototype, only for chex=true |
---|
1372 | // This is reserved for the charge-exchange scattering (to help neutron spectras) |
---|
1373 | //if(cln&&!cp1 &&(projPDG==2212&&rA>rZ || projPDG==2112&&rZ>1))// @@ Use proj chex |
---|
1374 | if(2>3) |
---|
1375 | { |
---|
1376 | #ifdef qedebug |
---|
1377 | G4cout<<"G4QCol::PStDoIt:-Enter,P="<<projPDG<<",cln="<<cln<<",cp1="<<cp1<<G4endl; |
---|
1378 | #endif |
---|
1379 | G4double tprM=mProt; |
---|
1380 | G4double tprM2=mProt2; |
---|
1381 | G4int tprPDG=2212; |
---|
1382 | G4int tresPDG=restPDG+999; |
---|
1383 | if(projPDG==2212) |
---|
1384 | { |
---|
1385 | projpt=G4Neutron::Neutron(); |
---|
1386 | tprM=mNeut; |
---|
1387 | tprM2=mNeut2; |
---|
1388 | tprPDG=2112; |
---|
1389 | tresPDG=restPDG-999; |
---|
1390 | } |
---|
1391 | minM=tprM+qM; |
---|
1392 | G4double efE=(cmM2-tprM2-qM*qM)/(qM+qM); |
---|
1393 | G4double efP=std::sqrt(efE*efE-tprM2); |
---|
1394 | G4double chl=qfMan->ChExElCoef(efP*MeV, nZ, nA-nZ, projPDG); // ChEx/Elast(pPDG!) |
---|
1395 | #ifdef qedebug |
---|
1396 | G4cout<<"G4QCol::PStDoIt:chl="<<chl<<",P="<<efP<<",nZ="<<nZ<<",nA="<<nA<<G4endl; |
---|
1397 | #endif |
---|
1398 | if(chl>0.&&cmM2>minM*minM&&G4UniformRand()<chl/(1.+chl)) // minM is redefined |
---|
1399 | { |
---|
1400 | projPDG=tprPDG; |
---|
1401 | prjM=tprM; |
---|
1402 | G4double rM=G4QPDGCode(tresPDG).GetMass();// Mass of the residual nucleus |
---|
1403 | r4M=G4LorentzVector(0.,0.,0.,rM); // 4mom of the residual nucleus |
---|
1404 | n4M=G4LorentzVector(0.,0.,0.,tM-rM); // 4mom of the quasi-free cluster |
---|
1405 | chex=true; // Confirm charge exchange scattering |
---|
1406 | } |
---|
1407 | } |
---|
1408 | // |
---|
1409 | std::pair<G4LorentzVector,G4LorentzVector> sctout=qfMan->Scatter(nPDG, n4M, |
---|
1410 | projPDG, proj4M); |
---|
1411 | #ifdef qedebug |
---|
1412 | G4cout<<"G4QCollis::PStDoIt:QElS,proj="<<prjM<<sctout.second<<",qfCl="<<qM |
---|
1413 | <<sctout.first<<",chex="<<chex<<",nA="<<nA<<",nZ="<<nZ<<G4endl; |
---|
1414 | #endif |
---|
1415 | aParticleChange.ProposeLocalEnergyDeposit(0.); // Everything is in particles |
---|
1416 | // @@ @@ @@ Coulomb barriers must be checked !! @@ @@ @@ Skip if not |
---|
1417 | if(chex) // ==> Projectile is changed: fill everything to secondaries |
---|
1418 | { |
---|
1419 | aParticleChange.ProposeEnergy(0.); // @@ ?? |
---|
1420 | aParticleChange.ProposeTrackStatus(fStopAndKill); // projectile nucleon is killed |
---|
1421 | aParticleChange.SetNumberOfSecondaries(3); |
---|
1422 | G4DynamicParticle* thePrH = new G4DynamicParticle(projpt,sctout.second); |
---|
1423 | G4Track* scatPrH = new G4Track(thePrH, localtime, position ); // scattered & chex |
---|
1424 | scatPrH->SetWeight(weight); // weighted |
---|
1425 | scatPrH->SetTouchableHandle(trTouchable); // projectile |
---|
1426 | aParticleChange.AddSecondary(scatPrH); // hadron |
---|
1427 | } |
---|
1428 | else // ==> The leading particle is filled to the updated projectilee |
---|
1429 | { |
---|
1430 | aParticleChange.SetNumberOfSecondaries(2); // @@ if proj=leading |
---|
1431 | G4double ldT=(sctout.second).e()-prjM; // kin Energy of scat project. |
---|
1432 | aParticleChange.ProposeEnergy(ldT); // Change the kin Energy |
---|
1433 | G4ThreeVector ldV=(sctout.second).vect(); // Change momentum direction |
---|
1434 | aParticleChange.ProposeMomentumDirection(ldV/ldV.mag()); |
---|
1435 | aParticleChange.ProposeTrackStatus(fAlive); |
---|
1436 | } |
---|
1437 | // --------------------------------------------------------- |
---|
1438 | // Fill scattered quasi-free nucleon |
---|
1439 | if (nPDG==90000001) theDefinition = G4Neutron::Neutron(); |
---|
1440 | else if(nPDG==90001000) theDefinition = G4Proton::Proton(); |
---|
1441 | else theDefinition = G4ParticleTable::GetParticleTable()->FindIon(nZ,nA,0,nZ);//ion |
---|
1442 | G4DynamicParticle* theQFN = new G4DynamicParticle(theDefinition,sctout.first); |
---|
1443 | G4Track* scatQFN = new G4Track(theQFN, localtime, position ); // scattered |
---|
1444 | scatQFN->SetWeight(weight); // weighted |
---|
1445 | scatQFN->SetTouchableHandle(trTouchable); // quasi-free |
---|
1446 | aParticleChange.AddSecondary(scatQFN); // nucleon/cluster |
---|
1447 | // ---------------------------------------------------- |
---|
1448 | // Fill residual nucleus |
---|
1449 | if (restPDG==90000001) theDefinition = G4Neutron::Neutron(); |
---|
1450 | else if(restPDG==90001000) theDefinition = G4Proton::Proton(); |
---|
1451 | else theDefinition = G4ParticleTable::GetParticleTable()->FindIon(rZ,rA,0,rZ);//ion |
---|
1452 | G4DynamicParticle* theReN = new G4DynamicParticle(theDefinition,r4M); |
---|
1453 | G4Track* scatReN = new G4Track(theReN, localtime, position ); // scattered |
---|
1454 | scatReN->SetWeight(weight); // weighted |
---|
1455 | scatReN->SetTouchableHandle(trTouchable); // residual |
---|
1456 | aParticleChange.AddSecondary(scatReN); // nucleus |
---|
1457 | return G4VDiscreteProcess::PostStepDoIt(track, step); |
---|
1458 | } |
---|
1459 | #ifdef qedebug |
---|
1460 | else G4cout<<"G4QCol::PSD: OUT, M2="<<s4M.m2()<<"<"<<minM*minM<<", N="<<nPDG<<G4endl; |
---|
1461 | #endif |
---|
1462 | } // end of proton quasi-elastic (including QE on NF) |
---|
1463 | else // @@ make cost-condition @@ Pickup process (pickup 1 or 2 n and make d or t) |
---|
1464 | { |
---|
1465 | restPDG--; // Res. nucleus PDG is one neutron less than targ. PDG |
---|
1466 | G4double mPUF=mDeut; // Prototype of the mass of the created pickup fragment |
---|
1467 | G4ParticleDefinition* theDefinition = G4Deuteron::Deuteron(); |
---|
1468 | //theDefinition = G4ParticleTable::GetParticleTable()->FindIon(nZ,nA,0,nZ);//ion |
---|
1469 | G4bool din=false; // Flag of picking up 2 neutrons to create t (tritium) |
---|
1470 | //G4bool hin=false; // Flag of picking up 1 n + 1 p to create He3 (NOT IMPL) |
---|
1471 | G4bool tin=false; // Flag of picking up 2 n + 1 p to create alpha (He4) |
---|
1472 | G4double frn=G4UniformRand(); |
---|
1473 | if(N>2 && frn > 0.95) // .95 is a parameter to pickup 2n (cteate t or +1p=alph) |
---|
1474 | { |
---|
1475 | theDefinition = G4Triton::Triton(); |
---|
1476 | restPDG--; // Res. nucleus PDG is two neutrons less than target PDG |
---|
1477 | rA--; // Reduce the baryon number of the residual nucleus |
---|
1478 | mPUF=mTrit; // The mass of the created pickup fragment (triton) |
---|
1479 | // Recalculate dmom |
---|
1480 | G4ThreeVector sumv=G4ThreeVector(0.,0.,dmom) + |
---|
1481 | fmm*std::pow(-std::log(G4UniformRand()),third)*G4RandomDirection(); |
---|
1482 | dmom=sumv.mag(); |
---|
1483 | din=true; |
---|
1484 | if(Z>1 && frn > 0.99) // 0.99 is a parameter to pickup 2n + 1p and create alpha |
---|
1485 | { |
---|
1486 | theDefinition = G4Alpha::Alpha(); |
---|
1487 | restPDG-=1000; // Res. nucleus PDG is (2 n + 1 p) less than target PDG |
---|
1488 | rA--; // Reduce the baryon number of the residual nucleus |
---|
1489 | rZ--; // Reduce the charge of the residual nucleus |
---|
1490 | mPUF=mAlph; // The mass of the created pickup fragment (triton) |
---|
1491 | // Recalculate dmom |
---|
1492 | sumv += fmm*std::pow(-std::log(G4UniformRand()),third)*G4RandomDirection(); |
---|
1493 | dmom=sumv.mag(); |
---|
1494 | tin=true; |
---|
1495 | } |
---|
1496 | } |
---|
1497 | G4double mPUF2=mPUF*mPUF; |
---|
1498 | G4LorentzVector t4M(0.,0.,0.,tM); // 4m of the target nucleus to be decayed |
---|
1499 | G4double rM=G4QPDGCode(restPDG).GetMass();// Mass of the residual nucleus |
---|
1500 | G4double rM2=rM*rM; // Squared mass of the residual nucleus |
---|
1501 | G4double nM2=rM2+tM*tM-(tM+tM)*std::sqrt(rM2+dmom*dmom);// M2 of boundQF-nucleon(2N) |
---|
1502 | if(nM2 < 0) nM2=0.; |
---|
1503 | G4double nM=std::sqrt(nM2); // M of bQF-nucleon |
---|
1504 | G4double den2=(dmom*dmom+nM2); // squared energy of bQF-nucleon |
---|
1505 | G4double den=std::sqrt(den2); // energy of bQF-nucleon |
---|
1506 | #ifdef qedebug |
---|
1507 | G4cout<<"G4QCollis::PStDoIt:PiU,p="<<dmom<<",tM="<<tM<<",R="<<rM<<",N="<<nM<<G4endl; |
---|
1508 | #endif |
---|
1509 | G4double qp=momentum*dmom; |
---|
1510 | G4double srm=proj4M.e()*den; |
---|
1511 | G4double cost=(nM2+mProt2+srm+srm-mPUF2)/(qp+qp); |
---|
1512 | G4int ict=0; |
---|
1513 | while(std::fabs(cost)>1. && ict<3) |
---|
1514 | { |
---|
1515 | dmom=91.; // Fermi momentum (proto default for a deuteron) |
---|
1516 | if(Z>1||N>1) dmom=fmm*std::pow(-std::log(G4UniformRand()),third); |
---|
1517 | if(din) // Recalculate dmom for the final triton |
---|
1518 | { |
---|
1519 | G4ThreeVector sumv=G4ThreeVector(0.,0.,dmom) + |
---|
1520 | fmm*std::pow(-std::log(G4UniformRand()),third)*G4RandomDirection(); |
---|
1521 | if(tin) sumv+=fmm*std::pow(-std::log(G4UniformRand()),third)*G4RandomDirection(); |
---|
1522 | dmom=sumv.mag(); |
---|
1523 | } |
---|
1524 | nM2=rM2+tM*tM-(tM+tM)*std::sqrt(rM2+dmom*dmom); // M2 of bQF-nucleon |
---|
1525 | if(nM2 < 0) nM2=0.; |
---|
1526 | nM=std::sqrt(nM2); // M of bQF-nucleon |
---|
1527 | den2=(dmom*dmom+nM2); // squared energy of bQF-nucleon |
---|
1528 | den=std::sqrt(den2); // energy of bQF-nucleon |
---|
1529 | qp=momentum*dmom; |
---|
1530 | srm=proj4M.e()*den; |
---|
1531 | cost=(nM2+mProt2+srm+srm-mPUF2)/(qp+qp); |
---|
1532 | ict++; |
---|
1533 | #ifdef ldebug |
---|
1534 | if(ict>2)G4cout<<"G4QCollis::PStDoIt:i="<<ict<<",d="<<dmom<<",ct="<<cost<<G4endl; |
---|
1535 | #endif |
---|
1536 | } |
---|
1537 | if(std::fabs(cost)<=1.) |
---|
1538 | {// ---- @@ From here can be a MF for QF nucleon extraction (if used by others) |
---|
1539 | G4ThreeVector vdir = proj4M.vect(); // 3-Vector in the projectile direction |
---|
1540 | G4ThreeVector vx(0.,0.,1.); // ProtoOrt in theDirection of the projectile |
---|
1541 | G4ThreeVector vy(0.,1.,0.); // First ProtoOrt orthogonal to the direction |
---|
1542 | G4ThreeVector vz(1.,0.,0.); // SecondProtoOrt orthoganal to the direction |
---|
1543 | if(vdir.mag2() > 0.) // the projectile isn't at rest |
---|
1544 | { |
---|
1545 | vx = vdir.unit(); // Ort in the direction of the projectile |
---|
1546 | G4ThreeVector vv= vx.orthogonal(); // Not normed orthogonal vector (!) |
---|
1547 | vy = vv.unit(); // First ort orthogonal to the proj direction |
---|
1548 | vz = vx.cross(vy); // Second ort orthoganal to the projDirection |
---|
1549 | } |
---|
1550 | // ---- @@ End of possible MF (Similar is in G4QEnvironment) |
---|
1551 | G4double tdom=dmom*std::sqrt(1-cost*cost);// Transversal component of the Fermi-Mom |
---|
1552 | G4double phi=twopi*G4UniformRand(); // Phi of the Fermi-Mom |
---|
1553 | G4ThreeVector vedm=vx*dmom*cost+vy*tdom*std::sin(phi)+vz*tdom*std::cos(phi);// bQFN |
---|
1554 | G4LorentzVector bqf(vedm,den); // 4-mom of the bQF nucleon |
---|
1555 | r4M=t4M-bqf; // 4mom of the residual nucleus |
---|
1556 | if(std::fabs(r4M.m()-rM)>.001) G4cout<<"G4QCol::PSD:rM="<<rM<<"#"<<r4M.m()<<G4endl; |
---|
1557 | G4LorentzVector f4M=proj4M+bqf; // Prototype of 4-mom of Deuteron |
---|
1558 | if(std::fabs(f4M.m()-mPUF)>.001) |
---|
1559 | G4cout<<"G4QCol::PSD:mDeut="<<mPUF<<" # "<<f4M.m()<<G4endl; |
---|
1560 | aParticleChange.ProposeEnergy(0.); // @@ ?? |
---|
1561 | aParticleChange.ProposeTrackStatus(fStopAndKill);// projectile nucleon is killed |
---|
1562 | aParticleChange.SetNumberOfSecondaries(2); |
---|
1563 | // Fill pickup hadron |
---|
1564 | G4DynamicParticle* theQFN = new G4DynamicParticle(theDefinition,f4M); |
---|
1565 | G4Track* scatQFN = new G4Track(theQFN, localtime, position ); // pickup |
---|
1566 | scatQFN->SetWeight(weight); // weighted |
---|
1567 | scatQFN->SetTouchableHandle(trTouchable); // nuclear |
---|
1568 | aParticleChange.AddSecondary(scatQFN); // cluster |
---|
1569 | // ---------------------------------------------------- |
---|
1570 | // Fill residual nucleus |
---|
1571 | if (restPDG==90000001) theDefinition = G4Neutron::Neutron(); |
---|
1572 | else if(restPDG==90001000) theDefinition = G4Proton::Proton(); |
---|
1573 | else theDefinition = G4ParticleTable::GetParticleTable()->FindIon(rZ,rA,0,rZ);//ion |
---|
1574 | G4DynamicParticle* theReN = new G4DynamicParticle(theDefinition,r4M); |
---|
1575 | G4Track* scatReN = new G4Track(theReN, localtime, position ); // scattered |
---|
1576 | scatReN->SetWeight(weight); // weighted |
---|
1577 | scatReN->SetTouchableHandle(trTouchable); // residual |
---|
1578 | aParticleChange.AddSecondary(scatReN); // nucleus |
---|
1579 | return G4VDiscreteProcess::PostStepDoIt(track, step); |
---|
1580 | } |
---|
1581 | } |
---|
1582 | } // end of decoupled processes for the proton projectile |
---|
1583 | } // end lepto-nuclear, neutrino-nuclear, proton quasi-elastic |
---|
1584 | EnMomConservation=proj4M+G4LorentzVector(0.,0.,0.,tM); // Total 4-mom of the reaction |
---|
1585 | if(absMom) EnMomConservation+=lead4M; // Add E/M of leading System |
---|
1586 | #ifdef debug |
---|
1587 | G4cout<<"G4QCollision::PostStDoIt:before St="<<aParticleChange.GetTrackStatus()<<G4endl; |
---|
1588 | #endif |
---|
1589 | |
---|
1590 | // @@@@@@@@@@@@@@ Temporary for the testing purposes --- Begin |
---|
1591 | //G4bool elF=false; // Flag of the ellastic scattering is "false" by default |
---|
1592 | //G4double eWei=1.; |
---|
1593 | // @@@@@@@@@@@@@@ Temporary for the testing purposes --- End |
---|
1594 | #ifdef ldebug |
---|
1595 | G4cout<<"^^G4QCollision::PostStepDoIt: projPDG="<<projPDG<<", targPDG="<<targPDG<<G4endl; |
---|
1596 | #endif |
---|
1597 | G4QHadron* pH = new G4QHadron(projPDG,proj4M); // ---> DELETED -->----+* |
---|
1598 | //if(momentum<1000.) // Condition for using G4QEnvironment (not G4QuasmonString) | |
---|
1599 | { // | |
---|
1600 | G4QHadronVector projHV; // | |
---|
1601 | projHV.push_back(pH); // DESTROYED over 2 lines-+ | |
---|
1602 | G4QEnvironment* pan= new G4QEnvironment(projHV,targPDG);// ---> DELETED --->----+ | | |
---|
1603 | std::for_each(projHV.begin(), projHV.end(), DeleteQHadron()); // <---<------<---+-+-+ |
---|
1604 | projHV.clear(); // <------------<---------------<-------------------<-----------+-+ . |
---|
1605 | #ifdef debug |
---|
1606 | G4cout<<"G4QCol::PStDoIt:Proj="<<projPDG<<proj4M<<",Targ="<<targPDG<<G4endl; // | . |
---|
1607 | #endif |
---|
1608 | try // | . |
---|
1609 | { // | . |
---|
1610 | delete output; // | . |
---|
1611 | output = pan->Fragment();// DESTROYED in the end of the LOOP work space | . |
---|
1612 | } // | . |
---|
1613 | catch (G4QException& error)// | . |
---|
1614 | { // | . |
---|
1615 | //#ifdef pdebug |
---|
1616 | G4cerr<<"***G4QCollision::PostStepDoIt: G4QE Exception is catched"<<G4endl;// | . |
---|
1617 | //#endif |
---|
1618 | G4Exception("G4QCollision::PostStepDoIt:","27",FatalException,"CHIPSCrash");//| . |
---|
1619 | } // | . |
---|
1620 | delete pan; // Delete the Nuclear Environment <-<--+ . |
---|
1621 | } // . |
---|
1622 | //else // Use G4QuasmonString . |
---|
1623 | //{ // ^ |
---|
1624 | // G4QuasmonString* pan= new G4QuasmonString(pH,false,targPDG,false);//-> DELETED --+ | |
---|
1625 | // delete pH; // --------<-------+--+ |
---|
1626 | #ifdef debug |
---|
1627 | // G4double mp=G4QPDGCode(projPDG).GetMass(); // Mass of the projectile particle | |
---|
1628 | // G4cout<<"G4QCollision::PostStepDoIt: pPDG="<<projPDG<<", pM="<<mp<<G4endl; // | |
---|
1629 | #endif |
---|
1630 | // //G4int tNH=0; // Prototype of the number of secondaries inOut| |
---|
1631 | // try // | |
---|
1632 | // { // | |
---|
1633 | // delete output; // | |
---|
1634 | // output = pan->Fragment();// DESTROYED in the end of the LOOP work space | |
---|
1635 | // // @@@@@@@@@@@@@@ Temporary for the testing purposes --- Begin | |
---|
1636 | // //tNH=pan->GetNOfHadrons(); // For the test purposes of the String | |
---|
1637 | // //if(tNH==2) // At least 2 hadrons are in the Constr.Output | |
---|
1638 | // //{// | |
---|
1639 | // // elF=true; // Just put a flag for the ellastic Scattering | |
---|
1640 | // // delete output; // Delete a prototype of dummy G4QHadronVector | |
---|
1641 | // // output = pan->GetHadrons(); // DESTROYED in the end of the LOOP work space | |
---|
1642 | // //}// | |
---|
1643 | // //eWei=pan->GetWeight(); // Just an example for the weight of the event | |
---|
1644 | #ifdef debug |
---|
1645 | // //G4cout<<"=====>>G4QCollision::PostStepDoIt: elF="<<elF<<",n="<<tNH<<G4endl;//| |
---|
1646 | #endif |
---|
1647 | // // @@@@@@@@@@@@@@ Temporary for the testing purposes --- End | |
---|
1648 | // } // | |
---|
1649 | // catch (G4QException& error)// | |
---|
1650 | // { // | |
---|
1651 | // //#ifdef pdebug |
---|
1652 | // G4cerr<<"***G4QCollision::PostStepDoIt: GEN Exception is catched"<<G4endl; // | |
---|
1653 | // //#endif |
---|
1654 | // G4Exception("G4QCollision::PostStDoIt:","27",FatalException,"QString Excep");//| |
---|
1655 | // } // | |
---|
1656 | // delete pan; // Delete the Nuclear Environment ---<--+ |
---|
1657 | //} |
---|
1658 | // --- the scattered hadron with changed nature can be added here --- |
---|
1659 | if(scat) |
---|
1660 | { |
---|
1661 | G4QHadron* scatHadron = new G4QHadron(scatPDG,scat4M); |
---|
1662 | output->push_back(scatHadron); |
---|
1663 | } |
---|
1664 | G4int qNH=leadhs->size(); |
---|
1665 | if(absMom) |
---|
1666 | { |
---|
1667 | if(qNH) for(G4int iq=0; iq<qNH; iq++) |
---|
1668 | { |
---|
1669 | G4QHadron* loh=(*leadhs)[iq]; // Pointer to the output hadron |
---|
1670 | output->push_back(loh); |
---|
1671 | } |
---|
1672 | delete leadhs; |
---|
1673 | } |
---|
1674 | // ------------- From here the secondaries are filled ------------------------- |
---|
1675 | G4int tNH = output->size(); // A#of hadrons in the output |
---|
1676 | aParticleChange.SetNumberOfSecondaries(tNH); |
---|
1677 | // Now add nuclear fragments |
---|
1678 | #ifdef debug |
---|
1679 | G4cout<<"G4QCollision::PostStepDoIt: "<<tNH<<" particles are generated"<<G4endl; |
---|
1680 | #endif |
---|
1681 | #ifdef ppdebug |
---|
1682 | if(absMom)G4cout<<"G4QCollision::PostStepDoIt: t="<<tNH<<", q="<<qNH<<G4endl; |
---|
1683 | #endif |
---|
1684 | G4int nOut=output->size(); // Real length of the output @@ Temporary |
---|
1685 | if(tNH==1 && !scat) // @@ Temporary. Find out why it happened! |
---|
1686 | { |
---|
1687 | G4cout<<"-Warning-G4QCollision::PostStepDoIt: 1 secondary! absMom="<<absMom; |
---|
1688 | if(absMom) G4cout<<", qNH="<<qNH; |
---|
1689 | G4cout<<", PDG0="<<(*output)[0]->GetPDGCode(); |
---|
1690 | G4cout<<G4endl; |
---|
1691 | tNH=0; |
---|
1692 | delete output->operator[](0); // delete the creazy hadron |
---|
1693 | output->pop_back(); // clean up the output vector |
---|
1694 | } |
---|
1695 | if(tNH==2&&2!=nOut) G4cout<<"--Warning--G4QCollision::PostStepDoIt: 2 # "<<nOut<<G4endl; |
---|
1696 | // Deal with ParticleChange final state interface to GEANT4 output of the process |
---|
1697 | //if(tNH==2) for(i=0; i<tNH; i++) // @@ Temporary tNH==2 instead of just tNH |
---|
1698 | if(tNH) for(i=0; i<tNH; i++) // @@ Temporary tNH==2 instead of just tNH |
---|
1699 | { |
---|
1700 | // Note that one still has to take care of Hypernuclei (with Lambda or Sigma inside) |
---|
1701 | // Hypernucleus mass calculation and ion-table interface upgrade => work for Hisaya @@ |
---|
1702 | // The decau process for hypernuclei must be developed in GEANT4 (change CHIPS body) |
---|
1703 | G4QHadron* hadr=(*output)[i]; // Pointer to the output hadron |
---|
1704 | G4int PDGCode = hadr->GetPDGCode(); |
---|
1705 | G4int nFrag = hadr->GetNFragments(); |
---|
1706 | #ifdef pdebug |
---|
1707 | G4cout<<"G4QCollision::PostStepDoIt: H#"<<i<<",PDG="<<PDGCode<<",nF="<<nFrag |
---|
1708 | <<", 4Mom="<<hadr->Get4Momentum()<<G4endl; |
---|
1709 | #endif |
---|
1710 | if(nFrag) // Skip intermediate (decayed) hadrons |
---|
1711 | { |
---|
1712 | #ifdef debug |
---|
1713 | G4cout<<"G4QCollision::PostStepDoIt: Intermediate particle is found i="<<i<<G4endl; |
---|
1714 | #endif |
---|
1715 | delete hadr; |
---|
1716 | continue; |
---|
1717 | } |
---|
1718 | G4DynamicParticle* theSec = new G4DynamicParticle; |
---|
1719 | G4ParticleDefinition* theDefinition; |
---|
1720 | if (PDGCode==90000001) theDefinition = G4Neutron::Neutron(); |
---|
1721 | else if(PDGCode==90001000) theDefinition = G4Proton::Proton();//While it can be in ions |
---|
1722 | else if(PDGCode==91000000) theDefinition = G4Lambda::Lambda(); |
---|
1723 | else if(PDGCode==311 || PDGCode==-311) |
---|
1724 | { |
---|
1725 | if(G4UniformRand()>.5) theDefinition = G4KaonZeroLong::KaonZeroLong(); // K_L |
---|
1726 | else theDefinition = G4KaonZeroShort::KaonZeroShort(); // K_S |
---|
1727 | } |
---|
1728 | else if(PDGCode==91000999) theDefinition = G4SigmaPlus::SigmaPlus(); |
---|
1729 | else if(PDGCode==90999001) theDefinition = G4SigmaMinus::SigmaMinus(); |
---|
1730 | else if(PDGCode==91999000) theDefinition = G4XiMinus::XiMinus(); |
---|
1731 | else if(PDGCode==91999999) theDefinition = G4XiZero::XiZero(); |
---|
1732 | else if(PDGCode==92998999) theDefinition = G4OmegaMinus::OmegaMinus(); |
---|
1733 | else if(PDGCode >80000000) // Defines hypernuclei as normal nuclei (N=N+S Correction!) |
---|
1734 | { |
---|
1735 | G4int aZ = hadr->GetCharge(); |
---|
1736 | G4int aA = hadr->GetBaryonNumber(); |
---|
1737 | #ifdef pdebug |
---|
1738 | G4cout<<"G4QCollision::PostStepDoIt:Ion Z="<<aZ<<", A="<<aA<<G4endl; |
---|
1739 | #endif |
---|
1740 | theDefinition = G4ParticleTable::GetParticleTable()->FindIon(aZ,aA,0,aZ); |
---|
1741 | } |
---|
1742 | //else theDefinition = G4ParticleTable::GetParticleTable()->FindParticle(PDGCode); |
---|
1743 | else |
---|
1744 | { |
---|
1745 | #ifdef pdebug |
---|
1746 | G4cout<<"G4QCollision::PostStepDoIt:Define particle with PDG="<<PDGCode<<G4endl; |
---|
1747 | #endif |
---|
1748 | theDefinition = G4QPDGToG4Particle::Get()->GetParticleDefinition(PDGCode); |
---|
1749 | #ifdef pdebug |
---|
1750 | G4cout<<"G4QCollision::PostStepDoIt:AfterParticleDefinition PDG="<<PDGCode<<G4endl; |
---|
1751 | #endif |
---|
1752 | } |
---|
1753 | if(!theDefinition) |
---|
1754 | { |
---|
1755 | #ifdef debug |
---|
1756 | G4cout<<"---Warning---G4QCollision::PostStepDoIt: drop PDG="<<PDGCode<<G4endl; |
---|
1757 | #endif |
---|
1758 | delete hadr; |
---|
1759 | continue; |
---|
1760 | } |
---|
1761 | #ifdef pdebug |
---|
1762 | G4cout<<"G4QCollision::PostStepDoIt:Name="<<theDefinition->GetParticleName()<<G4endl; |
---|
1763 | #endif |
---|
1764 | theSec->SetDefinition(theDefinition); |
---|
1765 | G4LorentzVector h4M=hadr->Get4Momentum(); |
---|
1766 | EnMomConservation-=h4M; |
---|
1767 | #ifdef tdebug |
---|
1768 | G4cout<<"G4QCollis::PSDI:"<<i<<","<<PDGCode<<h4M<<h4M.m()<<EnMomConservation<<G4endl; |
---|
1769 | #endif |
---|
1770 | #ifdef debug |
---|
1771 | G4cout<<"G4QCollision::PostStepDoIt:#"<<i<<",PDG="<<PDGCode<<",4M="<<h4M<<G4endl; |
---|
1772 | #endif |
---|
1773 | theSec->Set4Momentum(h4M); // ^ |
---|
1774 | delete hadr; // <-----<-----------<-------------<---------------------<---------<-----+ |
---|
1775 | #ifdef debug |
---|
1776 | G4ThreeVector curD=theSec->GetMomentumDirection(); // ^ |
---|
1777 | G4double curM=theSec->GetMass(); // | |
---|
1778 | G4double curE=theSec->GetKineticEnergy()+curM; // ^ |
---|
1779 | G4cout<<"G4QCollis::PSDoIt:p="<<curD<<curD.mag()<<",e="<<curE<<",m="<<curM<<G4endl;// | |
---|
1780 | #endif |
---|
1781 | G4Track* aNewTrack = new G4Track(theSec, localtime, position ); // ^ |
---|
1782 | aNewTrack->SetWeight(weight); // weighted | |
---|
1783 | aNewTrack->SetTouchableHandle(trTouchable); // | |
---|
1784 | aParticleChange.AddSecondary( aNewTrack ); // | |
---|
1785 | #ifdef debug |
---|
1786 | G4cout<<"G4QCollision::PostStepDoIt:#"<<i<<" is done."<<G4endl; // | |
---|
1787 | #endif |
---|
1788 | } // | |
---|
1789 | delete output; // instances of the G4QHadrons from the output are already deleted above + |
---|
1790 | #ifdef debug |
---|
1791 | G4cout<<"G4QCollision::PostStDoIt: after St="<<aParticleChange.GetTrackStatus()<<G4endl; |
---|
1792 | #endif |
---|
1793 | if(aProjPDG!=11 && aProjPDG!=13 && aProjPDG!=15) |
---|
1794 | aParticleChange.ProposeTrackStatus(fStopAndKill); // Kill the absorbed particle |
---|
1795 | //return &aParticleChange; // This is not enough (ClearILL) |
---|
1796 | #ifdef pdebug |
---|
1797 | G4cout<<"G4QCollision::PostStepDoIt: E="<<aParticleChange.GetEnergy() |
---|
1798 | <<", d="<<*aParticleChange.GetMomentumDirection()<<G4endl; |
---|
1799 | #endif |
---|
1800 | #ifdef ldebug |
---|
1801 | G4cout<<"G4QCollision::PostStepDoIt:*** PostStepDoIt is done ***, P="<<aProjPDG<<", St=" |
---|
1802 | <<aParticleChange.GetTrackStatus()<<G4endl; |
---|
1803 | #endif |
---|
1804 | return G4VDiscreteProcess::PostStepDoIt(track, step); |
---|
1805 | } |
---|
1806 | |
---|
1807 | std::pair<G4double,G4double> G4QCollision::Random2DDirection() |
---|
1808 | { |
---|
1809 | G4double sp=0; // sin(phi) |
---|
1810 | G4double cp=1.; // cos(phi) |
---|
1811 | G4double r2=2.; // to enter the loop |
---|
1812 | while(r2>1. || r2<.0001) // pi/4 efficiency |
---|
1813 | { |
---|
1814 | G4double s=G4UniformRand(); |
---|
1815 | G4double c=G4UniformRand(); |
---|
1816 | sp=1.-s-s; |
---|
1817 | cp=1.-c-c; |
---|
1818 | r2=sp*sp+cp*cp; |
---|
1819 | } |
---|
1820 | G4double norm=std::sqrt(r2); |
---|
1821 | return std::make_pair(sp/norm,cp/norm); |
---|
1822 | } |
---|