// // ******************************************************************** // * License and Disclaimer * // * * // * The Geant4 software is copyright of the Copyright Holders of * // * the Geant4 Collaboration. It is provided under the terms and * // * conditions of the Geant4 Software License, included in the file * // * LICENSE and available at http://cern.ch/geant4/license . These * // * include a list of copyright holders. * // * * // * Neither the authors of this software system, nor their employing * // * institutes,nor the agencies providing financial support for this * // * work make any representation or warranty, express or implied, * // * regarding this software system or assume any liability for its * // * use. Please see the license in the file LICENSE and URL above * // * for the full disclaimer and the limitation of liability. * // * * // * This code implementation is the result of the scientific and * // * technical work of the GEANT4 collaboration. * // * By using, copying, modifying or distributing the software (or * // * any work based on the software) you agree to acknowledge its * // * use in resulting scientific publications, and indicate your * // * acceptance of all terms of the Geant4 Software license. * // ******************************************************************** // // neutron_hp -- source file // J.P. Wellisch, Nov-1996 // A prototype of the low energy neutron transport model. // // 080718 As for secondary photons, if its mean value has a value of integer, // then a sampling of multiplicity that based on Poisson Distribution // is not carried out and the mean is used as a multiplicity. // modified by T. Koi. // 080721 Using ClearHistories() methodl for limiting the sum of secondary energies // modified by T. Koi. // 080901 bug fix of too many secnodaries production in nd reactinos by T. Koi // #include "G4NeutronHPProduct.hh" #include "G4Poisson.hh" #include "G4Proton.hh" G4ReactionProductVector * G4NeutronHPProduct::Sample(G4double anEnergy) { if(theDist == 0) { return 0; } G4ReactionProductVector * result = new G4ReactionProductVector; G4double mean = theYield.GetY(anEnergy); G4int multi; multi = G4int(mean+0.0001); //if(theMassCode==0) multi = G4Poisson(mean); // @@@@gammas. please X-check this //080718 if ( theMassCode == 0 ) { if ( G4int ( mean ) == mean ) { multi = (G4int) mean; } else { multi = G4Poisson ( mean ); } } theDist->SetTarget(theTarget); theDist->SetNeutron(theNeutron); G4int i; // G4double eMax = GetTarget()->GetMass()+GetNeutron()->GetMass() // - theActualStateQValue; theCurrentMultiplicity = static_cast(mean); G4ReactionProduct * tmp; theDist->ClearHistories(); for(i=0;iSample(anEnergy, theMassCode, theMass); if(tmp != 0) { result->push_back(tmp); } } if(multi == 0) { tmp = theDist->Sample(anEnergy, theMassCode, theMass); delete tmp; } /* //080901 TK Comment out, too many secondaries are produced in deuteron reactions if(theTarget->GetMass()<2*GeV) // @@@ take care of residuals in all cases { tmp = theDist->Sample(anEnergy, theMassCode, theMass); tmp->SetDefinition(G4Proton::Proton()); if(tmp != 0) { result->push_back(tmp); } } */ return result; }