[819] | 1 | // |
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| 2 | // ******************************************************************** |
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| 3 | // * License and Disclaimer * |
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| 4 | // * * |
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| 5 | // * The Geant4 software is copyright of the Copyright Holders of * |
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| 6 | // * the Geant4 Collaboration. It is provided under the terms and * |
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| 7 | // * conditions of the Geant4 Software License, included in the file * |
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| 8 | // * LICENSE and available at http://cern.ch/geant4/license . These * |
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| 9 | // * include a list of copyright holders. * |
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| 10 | // * * |
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| 11 | // * Neither the authors of this software system, nor their employing * |
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| 12 | // * institutes,nor the agencies providing financial support for this * |
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| 13 | // * work make any representation or warranty, express or implied, * |
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| 14 | // * regarding this software system or assume any liability for its * |
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| 15 | // * use. Please see the license in the file LICENSE and URL above * |
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| 16 | // * for the full disclaimer and the limitation of liability. * |
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| 17 | // * * |
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| 18 | // * This code implementation is the result of the scientific and * |
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| 19 | // * technical work of the GEANT4 collaboration. * |
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| 20 | // * By using, copying, modifying or distributing the software (or * |
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| 21 | // * any work based on the software) you agree to acknowledge its * |
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| 22 | // * use in resulting scientific publications, and indicate your * |
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| 23 | // * acceptance of all terms of the Geant4 Software license. * |
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| 24 | // ******************************************************************** |
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| 25 | // |
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[962] | 26 | // $Id: G4PreCompoundEmission.icc,v 1.5 2009/02/10 16:01:37 vnivanch Exp $ |
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| 27 | // GEANT4 tag $Name: geant4-09-02-ref-02 $ |
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| 28 | // |
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| 29 | // |
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| 30 | // Author: V.Lara |
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| 31 | // |
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| 32 | // Modified: |
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| 33 | // Modif (03 September 2008) by J. M. Quesada for external choice of inverse |
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| 34 | // cross section option |
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| 35 | // JMQ (06 September 2008) Also external choice has been added for: |
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| 36 | // - superimposed Coulomb barrier (if useSICB=true) |
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| 37 | |
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[819] | 38 | inline void G4PreCompoundEmission::Initialize(const G4Fragment & aFragment) |
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| 39 | { |
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| 40 | theFragmentsVector->Initialize(aFragment); |
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| 41 | return; |
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| 42 | } |
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| 43 | |
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| 44 | inline G4double G4PreCompoundEmission::GetTotalProbability(const G4Fragment & aFragment) |
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| 45 | { |
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| 46 | return theFragmentsVector->CalculateProbabilities(aFragment); |
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| 47 | } |
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| 48 | |
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| 49 | inline void G4PreCompoundEmission::SetUp(const G4Fragment & aFragment) |
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| 50 | { |
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| 51 | // This should be the projectile energy. If I would know which is the projectile (proton, neutron) |
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| 52 | // I could remove the binding energy. But, what happens if INC precedes precompound? This approximation |
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| 53 | // seems to work well enough |
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| 54 | ProjEnergy = aFragment.GetExcitationEnergy(); |
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| 55 | theIncidentDirection = aFragment.GetMomentum().vect().unit(); |
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| 56 | theFragmentsVector->ResetStage(); |
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| 57 | return; |
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| 58 | } |
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[962] | 59 | |
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| 60 | //for inverse cross section choice |
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| 61 | inline void G4PreCompoundEmission::SetOPTxs(G4int opt) |
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| 62 | { |
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| 63 | theFragmentsVector->SetOPTxs(opt); |
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| 64 | return; |
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| 65 | } |
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| 66 | //for superimposed Coumlomb Barrier for inverse cross sections |
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| 67 | inline void G4PreCompoundEmission::UseSICB(G4bool use) |
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| 68 | { |
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| 69 | theFragmentsVector->UseSICB(use); |
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| 70 | return; |
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| 71 | } |
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| 72 | |
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