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9.6.p02
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geant4_9_6_p02
source
processes
electromagnetic
lowenergy
include
G4QAOLowEnergyLoss.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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// * *
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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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//
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// ------------------------------------------------------------
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// GEANT 4 class header file
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//
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// History: New Implementation
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//
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// ---------- G4QAOLowEnergyLoss physics process -------
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// by Stephane Chauvie, 21 May 2000
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//
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// Modified:
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// 16/09/2000 S. Chauvie Oscillator for all materials
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// 23/05/2000 MGP Made compliant to design
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// 01/06/2001 V.Ivanchenko replace names by Z
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//
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// Class description:
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// Quantal Harmonic Oscillator Model for energy loss of low energy antiprotons
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// Further documentation available from http://www.ge.infn.it/geant4/lowE
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// ------------------------------------------------------------
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#ifndef G4QAOLowEnergyLoss_hh
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#define G4QAOLowEnergyLoss_hh 1
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#include "
G4VLowEnergyModel.hh
"
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#include "
globals.hh
"
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class
G4QAOLowEnergyLoss
:
public
G4VLowEnergyModel
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{
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public
:
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G4QAOLowEnergyLoss
(
const
G4String
&
name
);
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~G4QAOLowEnergyLoss
();
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G4double
HighEnergyLimit
(
const
G4ParticleDefinition
* aParticle,
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const
G4Material
*
material
)
const
;
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// returns the higher limit for model validity
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G4double
LowEnergyLimit
(
const
G4ParticleDefinition
* aParticle,
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const
G4Material
* material)
const
;
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// returns the lower limit for model validity
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G4double
HighEnergyLimit
(
const
G4ParticleDefinition
* aParticle)
const
;
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// returns the higher limit for model validity
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G4double
LowEnergyLimit
(
const
G4ParticleDefinition
* aParticle)
const
;
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// returns the lower limit for model validity
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G4bool
IsInCharge
(
const
G4DynamicParticle
* particle,
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const
G4Material
* material)
const
;
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// returns true if the model is applicable at that energy for
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// that particle for that material
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G4bool
IsInCharge
(
const
G4ParticleDefinition
* aParticle,
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const
G4Material
* material)
const
;
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// returns true if the model is applicable at that energy for
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// that particle for that material
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G4double
TheValue
(
const
G4DynamicParticle
* particle,
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const
G4Material
* material);
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// returns the energy loss via the quantal harmonic oscillator model
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G4double
TheValue
(
const
G4ParticleDefinition
* aParticle,
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const
G4Material
* material,
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G4double
kineticEnergy);
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// returns the energy loss via the quantal harmonic oscillator model
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private
:
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G4double
EnergyLoss(
const
G4Material
* material,
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G4double
kineticEnergy,
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G4double
zParticle)
const
;
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// returns the energy loss via the quantal harmonic oscillator model
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// get number of shell, energy and oscillator strenghts for material
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G4int
GetNumberOfShell(
const
G4Material
* material)
const
;
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G4double
GetShellEnergy(
const
G4Material
* material,
G4int
nbOfTheShell)
const
;
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G4double
GetOscillatorEnergy(
const
G4Material
* material,
G4int
nbOfTheShell)
const
;
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G4double
GetShellStrength(
const
G4Material
* material,
G4int
nbOfTheShell)
const
;
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G4double
GetOccupationNumber(
G4int
Z
,
G4int
ShellNb)
const
;
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// calculate stopping number for L's term
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G4double
GetL0(
G4double
normEnergy)
const
;
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// terms in Z^2
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G4double
GetL1(
G4double
normEnergy)
const
;
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// terms in Z^3
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G4double
GetL2(
G4double
normEnergy)
const
;
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// terms in Z^4
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// Z of element at now avaliable for the model
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static
const
G4int
materialAvailable[6];
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// number, energy and oscillator strenghts
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// for an harmonic oscillator model of material
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static
const
G4int
nbofShellForMaterial[6];
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static
G4double
alShellEnergy[3];
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static
G4double
alShellStrength[3];
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static
G4double
siShellEnergy[3];
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static
G4double
siShellStrength[3];
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static
G4double
cuShellEnergy[4];
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static
G4double
cuShellStrength[4];
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static
G4double
taShellEnergy[6];
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static
G4double
taShellStrength[6];
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static
G4double
auShellEnergy[6];
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static
G4double
auShellStrength[6];
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static
G4double
ptShellEnergy[6];
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static
G4double
ptShellStrength[6];
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G4int
numberOfMaterials;
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// variable for calculation of stopping number of L's term
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static
const
G4double
L0[67][2];
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static
const
G4double
L1[22][2];
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static
const
G4double
L2[14][2];
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static
const
G4int
nbOfElectronPerSubShell[1540];
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static
const
G4int
fNumberOfShells[101];
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G4int
sizeL0;
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G4int
sizeL1;
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G4int
sizeL2;
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};
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#endif
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