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geant4_9_6_p02
source
processes
hadronic
models
chiral_inv_phase_space
processes
include
G4QDiffraction.hh
Go to the documentation of this file.
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//
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// ********************************************************************
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// * License and Disclaimer *
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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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// * 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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// * acceptance of all terms of the Geant4 Software license. *
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// ********************************************************************
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//
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// $Id$
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//
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// ---------------- G4QDiffraction header ----------------
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// by Mikhail Kossov, Aug 2007.
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// Header of G4QDiffraction class (hadron+A) of the CHIPS Simulation Branch in GEANT4
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// -------------------------------------------------------------------------------
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// This is a unique CHIPS class for the Hadron-Nuclear Diffractive Interaction Prosesses
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// -------------------------------------------------------------------------------
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// At present (Aug-07) it is based on the G4QDiffractionRatio class and is not tested.
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// The normalization is based on the temporary G4QProtonNuclearCrossSection class
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// -------------------------------------------------------------------------------
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// Short description: This is a process, which describes the diffraction
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// excitation of the projectile and the nucleus. On nuclei in addition there
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// can be a coherent diffraction process for the projectile, but it is
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// comparably small. The most important part of the diffraction is the
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// progectile diffraction excitation, as in this interaction proton can lose
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// only a small part of its energy and make the shower longer. This is because
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// only 1-2 (n) pions are produce in the diffraction escitation, and the mean
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// kept energy of the nucleon is (1-n/7)=80%. For kaons the kept energy is much
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// smaller (1-n/3.5)=60%, and for pions it is less important (about 40%).
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// ----------------------------------------------------------------------------
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#ifndef G4QDiffraction_hh
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#define G4QDiffraction_hh
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// GEANT4 Headers
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#include "
globals.hh
"
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#include "
G4ios.hh
"
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#include "
Randomize.hh
"
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#include "
G4VDiscreteProcess.hh
"
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#include "
G4Track.hh
"
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#include "
G4Step.hh
"
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#include "
G4ParticleTypes.hh
"
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#include "
G4VParticleChange.hh
"
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#include "
G4ParticleDefinition.hh
"
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#include "
G4DynamicParticle.hh
"
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#include "
G4ThreeVector.hh
"
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#include "
G4LorentzVector.hh
"
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// CHIPS Headers
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#include "
G4QDiffractionRatio.hh
"
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#include "
G4QProtonNuclearCrossSection.hh
"
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#include "
G4QIsotope.hh
"
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#include "
G4QCHIPSWorld.hh
"
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#include "
G4QHadronVector.hh
"
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#include <vector>
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class
G4QDiffraction
:
public
G4VDiscreteProcess
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{
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public
:
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// Constructor
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G4QDiffraction
(
const
G4String
& processName =
"CHIPS_DiffractiveInteraction"
);
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// Destructor
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~G4QDiffraction
();
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G4bool
IsApplicable
(
const
G4ParticleDefinition
& particle);
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G4double
GetMeanFreePath
(
const
G4Track
& aTrack,
G4double
previousStepSize,
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G4ForceCondition
*
condition
);
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// It returns the MeanFreePath of the process for the current track :
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// (energy, material)
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// The previousStepSize and G4ForceCondition* are not used.
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// This function overloads a virtual function of the base class.
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// It is invoked by the ProcessManager of the Particle.
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G4VParticleChange
*
PostStepDoIt
(
const
G4Track
& aTrack,
const
G4Step
& aStep);
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// It computes the final state of the process (at end of step),
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// returned as a ParticleChange object.
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// This function overloads a virtual function of the base class.
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// It is invoked by the ProcessManager of the Particle.
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G4LorentzVector
GetEnegryMomentumConservation
();
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G4int
GetNumberOfNeutronsInTarget
();
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private
:
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// Hide assignment operator as private
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G4QDiffraction
& operator=(
const
G4QDiffraction
&
right
);
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// Copy constructor
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G4QDiffraction
(
const
G4QDiffraction
&);
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// Calculate Cross-Section of the Diffraction Reaction (p is in GeV @@ units)
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G4double
CalculateXS(
G4double
p
,
G4int
Z
,
G4int
N
,
G4int
pPDG);
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// BODY
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// Static Parameters --------------------------------------------------------------------
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static
G4int
nPartCWorld;
// The#of particles for hadronization (limit of A of fragm.)
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//--------------------------------- End of static parameters ---------------------------
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// Working parameters
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G4VQCrossSection
* theCS;
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G4LorentzVector
EnMomConservation;
// Residual of Energy/Momentum Cons.
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G4int
nOfNeutrons;
// #of neutrons in the target nucleus
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// Modifires for the reaction
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G4double
Time;
// Time shift of the capture reaction
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G4double
EnergyDeposition;
// Energy deposited in the reaction
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static
std::vector <G4int> ElementZ;
// Z of the element(i) in theLastCalc
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static
std::vector <G4double> ElProbInMat;
// SumProbabilityElements in Material
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static
std::vector <std::vector<G4int>*> ElIsoN;
// N of isotope(j) of Element(i)
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static
std::vector <std::vector<G4double>*> IsoProbInEl;
// SumProbabIsotopes in Element i
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};
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#endif
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