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This commit is contained in:
Gabriele Cosmo
2016-06-08 16:10:37 +02:00
parent 137e303ecc
commit 36c080dca6
3464 changed files with 119310 additions and 52696 deletions
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source/processes/electromagnetic/lowenergy/include/G4hLowEnergyIonisation.hh
+35 -19
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@@ -1,15 +1,29 @@
// This code implementation is the intellectual property of
// the GEANT4 collaboration.
//
// By copying, distributing or modifying the Program (or any work
// based on the Program) you indicate your acceptance of this statement,
// and all its terms.
// ********************************************************************
// * DISCLAIMER *
// * *
// * The following disclaimer summarizes all the specific disclaimers *
// * of contributors to this software. The specific disclaimers,which *
// * govern, are listed with their locations in: *
// * http://cern.ch/geant4/license *
// * *
// * 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. *
// * *
// * This code implementation is the intellectual property of the *
// * GEANT4 collaboration. *
// * By copying, distributing or modifying the Program (or any work *
// * based on the Program) you indicate your acceptance of this *
// * statement, and all its terms. *
// ********************************************************************
//
//
// ------------------------------------------------------------
// GEANT 4 class header file
//
// For information related to this code contact:
// CERN, IT Division, ASD group
// History: based on object model of
// 2nd December 1995, G.Cosmo
// ---------- G4hLowEnergyIonisation physics process -----
@@ -43,6 +57,7 @@
// Nuclear stopping powers: "ICRU_49" (default), "Ziegler1977",
// "Ziegler1985"
// Further documentation available from http://www.ge.infn.it/geant4/lowE
// and in the Physics Reference Manual
// ------------------------------------------------------------
@@ -79,7 +94,7 @@ public: // With description
// True for all charged hadrons/ions
void BuildPhysicsTable(const G4ParticleDefinition& aParticleType) ;
// Build physics table during inicialisation
// Build physics table during initialisation
G4double GetMeanFreePath(const G4Track& track,
G4double previousStepSize,
@@ -92,25 +107,26 @@ public: // With description
void SetHighEnergyForProtonParametrisation(G4double energy)
{protonHighEnergy = energy;} ;
// Definition of the boundary proton energy. For higher energies
// Bethe-Bloch formula is used, for lower energies parametrisation
// of the energy losses is performed.
// Bethe-Bloch formula is used, for lower energies a parametrisation
// of the energy losses is performed. Default is 2 MeV.
void SetLowEnergyForProtonParametrisation(G4double energy)
{protonLowEnergy = energy;} ;
// Definition of the boundary proton energy. For lower energies
// Free Electron Gas model is used for the energy losses
// Set of the boundary proton energy. For lower energies
// the Free Electron Gas model is used for the energy losses.
// Default is 1 keV.
void SetHighEnergyForAntiProtonParametrisation(G4double energy)
{antiProtonHighEnergy = energy;} ;
// Definition of the boundary antiproton energy. For higher energies
// Set of the boundary antiproton energy. For higher energies
// Bethe-Bloch formula is used, for lower energies parametrisation
// of the energy losses is performed. Default is 2 MeV.
void SetLowEnergyForAntiProtonParametrisation(G4double energy)
{antiProtonLowEnergy = energy;} ;
// Definition of the boundary antiproton energy. For lower energies
// Free Electron Gas model is used for the energy losses. Default
// is 1 keV.
// Set of the boundary antiproton energy. For lower energies
// the Free Electron Gas model is used for the energy losses.
// Default is 1 keV.
G4double GetContinuousStepLimit(const G4Track& track,
G4double previousStepSize,
@@ -135,10 +151,10 @@ public: // With description
// This method switch off calculation of the nuclear stopping power.
void SetBarkasOn() {theBarkas = true;};
// This method switch on calculation of the Barkas and Bloch effects
// This method switch on calculation of the Barkas and Bloch effects.
void SetBarkasOff() {theBarkas = false;};
// This method switch off calculation of the Barkas and Bloch effects
// This method switch off calculation of the Barkas and Bloch effects.
G4VParticleChange* AlongStepDoIt(const G4Track& trackData ,
const G4Step& stepData ) ;
@@ -146,7 +162,7 @@ public: // With description
G4VParticleChange* PostStepDoIt(const G4Track& track,
const G4Step& Step ) ;
// Simulation of delta rays production
// Simulation of delta rays production.
G4double ComputeDEDX(const G4ParticleDefinition* aParticle,
const G4Material* material,