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G4INCLNNOmegaToMultiPionsChannel.hh
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//
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// ********************************************************************
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// * License and Disclaimer *
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// * *
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// * The Geant4 software is copyright of the Copyright Holders of *
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// * the Geant4 Collaboration. It is provided under the terms and *
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// * conditions of the Geant4 Software License, included in the file *
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// * LICENSE and available at http://cern.ch/geant4/license . These *
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// * include a list of copyright holders. *
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// * *
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// * Neither the authors of this software system, nor their employing *
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// * institutes,nor the agencies providing financial support for this *
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// * work make any representation or warranty, express or implied, *
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// * regarding this software system or assume any liability for its *
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// * use. Please see the license in the file LICENSE and URL above *
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// * for the full disclaimer and the limitation of liability. *
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// * *
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// * This code implementation is the result of the scientific and *
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// * technical work of the GEANT4 collaboration. *
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// * By using, copying, modifying or distributing the software (or *
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// * any work based on the software) you agree to acknowledge its *
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// * use in resulting scientific publications, and indicate your *
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// * acceptance of all terms of the Geant4 Software license. *
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// ********************************************************************
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//
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// INCL++ intra-nuclear cascade model
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// Alain Boudard, CEA-Saclay, France
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// Joseph Cugnon, University of Liege, Belgium
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// Jean-Christophe David, CEA-Saclay, France
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// Pekka Kaitaniemi, CEA-Saclay, France, and Helsinki Institute of Physics, Finland
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// Sylvie Leray, CEA-Saclay, France
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// Davide Mancusi, CEA-Saclay, France
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//
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#define INCLXX_IN_GEANT4_MODE 1
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#include "
globals.hh
"
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#ifndef G4INCLNNOmegaToMultiPionsChannel_hh
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#define G4INCLNNOmegaToMultiPionsChannel_hh 1
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#include "
G4INCLParticle.hh
"
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#include "
G4INCLIChannel.hh
"
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#include "
G4INCLFinalState.hh
"
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#include "
G4INCLAllocationPool.hh
"
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namespace
G4INCL {
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class
NNOmegaToMultiPionsChannel
:
public
IChannel
{
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public
:
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NNOmegaToMultiPionsChannel
(
const
G4int
,
Particle
*,
Particle
*);
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virtual
~NNOmegaToMultiPionsChannel
();
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void
fillFinalState
(
FinalState
*
fs
);
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private
:
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G4int
npion
;
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G4int
iso1
;
// like isosp, can be changed in isospinRepartition
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G4int
iso2
;
// like isosp, can be changed in isospinRepartition
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G4int
isosp
[4];
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Particle
*
particle1
, *
particle2
;
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static
const
G4double
angularSlope
;
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void
inter2Part
(
const
G4double
p
);
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void
pn_ppPim
();
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void
pn_pnPi0
();
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void
pn_nnPip
();
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void
pp_nnPipPip
();
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void
nn_ppPimPim
();
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void
pn_pnPipPim
();
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void
pn_pnPi0Pi0
();
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void
pp_ppPipPim
();
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void
nn_nnPipPim
();
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void
pp_ppPi0Pi0
();
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void
nn_nnPi0Pi0
();
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void
pp_pnPipPi0
();
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void
pn_ppPimPi0
();
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void
pn_nnPipPi0
();
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void
nn_pnPimPi0
();
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void
pp_pnPipPi0Pi0
();
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void
nn_pnPimPi0Pi0
();
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void
pn_nnPipPi0Pi0
();
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void
pp_ppPipPimPi0
();
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void
nn_nnPipPimPi0
();
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void
pp_ppPi0Pi0Pi0
();
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void
nn_nnPi0Pi0Pi0
();
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void
pp_pnPipPipPim
();
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void
pp_nnPipPipPi0
();
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void
pn_ppPimPi0Pi0
();
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void
pn_ppPimPimPip
();
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void
pn_pnPi0PipPim
();
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void
pn_pnPi0Pi0Pi0
();
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void
pn_nnPipPipPim
();
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void
nn_pnPipPimPim
();
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void
nn_ppPimPimPi0
();
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void
pp_nnPipPipPi0Pi0
();
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void
pp_nnPipPipPipPim
();
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void
nn_ppPi0Pi0PimPim
();
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void
nn_ppPipPimPimPim
();
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void
pp_ppPi0Pi0Pi0Pi0
();
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void
nn_nnPi0Pi0Pi0Pi0
();
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void
pn_pnPi0Pi0Pi0Pi0
();
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void
pp_ppPipPi0Pi0Pim
();
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void
nn_nnPipPi0Pi0Pim
();
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void
pn_pnPipPi0Pi0Pim
();
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void
pp_ppPipPipPimPim
();
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void
nn_nnPipPipPimPim
();
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void
pn_pnPipPipPimPim
();
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void
pp_pnPipPi0Pi0Pi0
();
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void
pn_nnPipPi0Pi0Pi0
();
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void
pp_nnPipPi0Pi0Pi0
();
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void
pp_pnPipPipPi0Pim
();
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void
pn_nnPipPipPi0Pim
();
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void
pp_nnPipPipPi0Pim
();
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void
nn_pnPi0Pi0Pi0Pim
();
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void
pn_ppPi0Pi0Pi0Pim
();
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void
nn_pnPipPi0PimPim
();
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void
pn_ppPipPi0PimPim
();
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void
isospinRepartition
();
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INCL_DECLARE_ALLOCATION_POOL
(
NNOmegaToMultiPionsChannel
);
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};
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}
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#endif
geant4
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geant4-10.6-release
source
processes
hadronic
models
inclxx
incl_physics
include
G4INCLNNOmegaToMultiPionsChannel.hh
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Jin Huang
. updated:
Wed Jun 29 2022 17:25:44
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