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Geant4/processes/hadronic/models/particle_hp/src/G4ParticleHPProduct.cc

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 25 //
 26 // particle_hp -- source file
 27 // J.P. Wellisch, Nov-1996
 28 // A prototype of the low energy neutron transport model.
 29 //
 30 // 080718 As for secondary photons, if its mean value has a value of integer,
 31 //        then a sampling of multiplicity that based on Poisson Distribution
 32 //        is not carried out and the mean is used as a multiplicity.
 33 //        modified by T. Koi.
 34 // 080721 Using ClearHistories() methodl for limiting the sum of secondary energies
 35 //        modified by T. Koi.
 36 // 080901 bug fix of too many secnodaries production in nd reactinos by T. Koi
 37 //
 38 // P. Arce, June-2014 Conversion neutron_hp to particle_hp
 39 // V. Ivanchenko, May-2023 Basic revision of particle HP classes
 40 //
 41 #include "G4ParticleHPProduct.hh"
 42 #include "G4ParticleHPManager.hh"
 43 #include "G4HadronicParameters.hh"
 44 #include "G4HadronicException.hh"
 45 #include "G4ParticleHPContEnergyAngular.hh"
 46 #include "G4ParticleHPDiscreteTwoBody.hh"
 47 #include "G4ParticleHPIsotropic.hh"
 48 #include "G4ParticleHPLabAngularEnergy.hh"
 49 #include "G4ParticleHPNBodyPhaseSpace.hh"
 50 #include "Randomize.hh"
 51 #include "G4Poisson.hh"
 52 #include "G4Proton.hh"
 53 
 54 G4ParticleHPProduct::G4ParticleHPProduct()
 55 {
 56   toBeCached val;
 57   fCache.Put(val);
 58 
 59   if (G4ParticleHPManager::GetInstance()->GetPHCUsePoisson()) {
 60     theMultiplicityMethod = G4HPMultiPoisson;
 61   } else {
 62     theMultiplicityMethod = G4HPMultiBetweenInts;
 63   }
 64 }
 65 
 66 G4ParticleHPProduct::~G4ParticleHPProduct()
 67 {
 68   delete theDist;
 69 }
 70 
 71 void G4ParticleHPProduct::Init(std::istream& aDataFile, const G4ParticleDefinition* projectile)
 72 {
 73   aDataFile >> theMassCode >> theMass >> theIsomerFlag >> theDistLaw >> theGroundStateQValue
 74       >> theActualStateQValue;
 75   theGroundStateQValue *= CLHEP::eV;
 76   theActualStateQValue *= CLHEP::eV;
 77   theYield.Init(aDataFile, CLHEP::eV);
 78   theYield.Hash();
 79   if (theDistLaw == 0) {
 80     // distribution not known, use E-independent, isotropic
 81     // angular distribution
 82     theDist = new G4ParticleHPIsotropic;
 83   }
 84   else if (theDistLaw == 1) {
 85     // Continuum energy-angular distribution
 86     theDist = new G4ParticleHPContEnergyAngular(projectile);
 87   }
 88   else if (theDistLaw == 2) {
 89     // Discrete 2-body scattering
 90     theDist = new G4ParticleHPDiscreteTwoBody;
 91   }
 92   else if (theDistLaw == 3) {
 93     // Isotropic emission
 94     theDist = new G4ParticleHPIsotropic;
 95   }
 96   else if (theDistLaw == 4) {
 97     // Discrete 2-body recoil modification not used for now.
 98     // theDist = new G4ParticleHPDiscreteTwoBody;
 99     // the above is only temporary;
100     // recoils need to be addressed properly
101   }
102   //    else if(theDistLaw == 5)
103   //    {
104   // charged particles only, to be used in a later stage. @@@@
105   //    }
106   else if (theDistLaw == 6) {
107     // N-Body phase space
108     theDist = new G4ParticleHPNBodyPhaseSpace;
109   }
110   else if (theDistLaw == 7) {
111     // Laboratory angular energy paraetrisation
112     theDist = new G4ParticleHPLabAngularEnergy;
113   }
114   else {
115         throw G4HadronicException(__FILE__, __LINE__,
116                                   "distribution law unknown to G4ParticleHPProduct");
117   }
118   if (theDist != nullptr) {
119     theDist->SetQValue(theActualStateQValue);
120     theDist->Init(aDataFile);
121   }
122 }
123 
124 G4int G4ParticleHPProduct::GetMultiplicity(G4double anEnergy)
125 {
126   if (theDist == nullptr) {
127     fCache.Get().theCurrentMultiplicity = 0;
128     return 0;
129   }
130 
131   G4double mean = theYield.GetY(anEnergy);
132   if (mean <= 0.) {
133     fCache.Get().theCurrentMultiplicity = 0;
134     return 0;
135   }
136   G4int multi = (theMultiplicityMethod == G4HPMultiPoisson) ?
137     (G4int)G4Poisson(mean) : G4lrint(mean);
138 
139 #ifdef G4VERBOSE
140   if (G4ParticleHPManager::GetInstance()->GetDEBUG())
141     G4cout << "G4ParticleHPProduct::GetMultiplicity code=" << theMassCode << " M=" << theMass
142      << " multi=" << multi << " mean=" << mean << G4endl;
143 #endif
144   fCache.Get().theCurrentMultiplicity = multi;
145 
146   return multi;
147 }
148 
149 G4ReactionProductVector* G4ParticleHPProduct::Sample(G4double anEnergy, G4int multi)
150 {
151   if (theDist == nullptr) {
152     return nullptr;
153   }
154   auto result = new G4ReactionProductVector;
155 
156   theDist->SetTarget(fCache.Get().theTarget);
157   theDist->SetProjectileRP(fCache.Get().theProjectileRP);
158   G4ReactionProduct* tmp;
159   theDist->ClearHistories();
160 
161   for (G4int i = 0; i < multi; ++i) {
162     tmp = theDist->Sample(anEnergy, theMassCode, theMass);
163     if (tmp != nullptr) {
164       result->push_back(tmp);
165 #ifdef G4VERBOSE
166       if (G4ParticleHPManager::GetInstance()->GetDEBUG())
167   G4cout << "multi=" << multi << " i=" << i << " G4ParticleHPProduct::Sample "
168          << tmp->GetDefinition()->GetParticleName() << " E=" << tmp->GetKineticEnergy()
169          << G4endl;
170 #endif
171     }
172   }
173   if (multi == 0) {
174     tmp = theDist->Sample(anEnergy, theMassCode, theMass);
175     delete tmp;
176   }
177   return result;
178 }
179