// // ******************************************************************** // * 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. * // ******************************************************************** // // // $Id: G4HEAntiSigmaZeroInelastic.cc,v 1.10 2006/06/29 20:30:08 gunter Exp $ // GEANT4 tag $Name: geant4-09-03-ref-09 $ // // #include "globals.hh" #include "G4ios.hh" // // G4 Process: Gheisha High Energy Collision model. // This includes the high energy cascading model, the two-body-resonance model // and the low energy two-body model. Not included are the low energy stuff like // nuclear reactions, nuclear fission without any cascading and all processes for // particles at rest. // First work done by J.L.Chuma and F.W.Jones, TRIUMF, June 96. // H. Fesefeldt, RWTH-Aachen, 23-October-1996 // Last modified: 29-July-1998 #include "G4HEAntiSigmaZeroInelastic.hh" #include "G4Gamma.hh" G4HadFinalState * G4HEAntiSigmaZeroInelastic:: ApplyYourself( const G4HadProjectile &aTrack, G4Nucleus &targetNucleus ) { G4HEVector * pv = new G4HEVector[MAXPART]; const G4HadProjectile *aParticle = &aTrack; G4HEVector incidentParticle(aParticle); G4HEAntiLambdaInelastic theAntiLambdaInelastic; theAntiLambdaInelastic.SetMaxNumberOfSecondaries(MAXPART); theAntiLambdaInelastic.SetVerboseLevel(verboseLevel); G4double incidentTotalMomentum = incidentParticle.getTotalMomentum(); G4double pgam = G4UniformRand()*incidentTotalMomentum*0.75; G4HEVector incidentAntiLambda; incidentAntiLambda.SmulAndUpdate( incidentParticle, (incidentTotalMomentum - pgam)/incidentTotalMomentum); G4DynamicParticle * aLambda = new G4DynamicParticle(); aLambda->SetDefinition(G4AntiLambda::AntiLambda()); aLambda->SetMomentum(incidentAntiLambda.getMomentum()); G4HadProjectile aLambdaTrack(*aLambda); G4HadFinalState * result = theAntiLambdaInelastic.ApplyYourself(aLambdaTrack, targetNucleus); vecLength = theAntiLambdaInelastic.GetNumberOfSecondaries(); pv[vecLength] = Gamma; pv[vecLength].setMomentum(incidentParticle.getMomentum()); pv[vecLength].SmulAndUpdate( pv[vecLength],pgam/incidentTotalMomentum); G4DynamicParticle * aPhoton = new G4DynamicParticle(); aPhoton->SetDefinition(G4Gamma::Gamma()); aPhoton->SetMomentum(pv[vecLength].getMomentum()); result->AddSecondary(aPhoton); delete [] pv; return result; }