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G4LivermoreNuclearGammaConversionModel Class Reference

#include <G4LivermoreNuclearGammaConversionModel.hh>

Inheritance diagram for G4LivermoreNuclearGammaConversionModel:
G4VEmModel

Public Member Functions

 G4LivermoreNuclearGammaConversionModel (const G4ParticleDefinition *p=0, const G4String &nam="LivermoreNuclearGammaConversion")
 
virtual ~G4LivermoreNuclearGammaConversionModel ()
 
virtual void Initialise (const G4ParticleDefinition *, const G4DataVector &)
 
virtual G4double ComputeCrossSectionPerAtom (const G4ParticleDefinition *, G4double kinEnergy, G4double Z, G4double A=0, G4double cut=0, G4double emax=DBL_MAX)
 
virtual void SampleSecondaries (std::vector< G4DynamicParticle * > *, const G4MaterialCutsCouple *, const G4DynamicParticle *, G4double tmin, G4double maxEnergy)
 
- Public Member Functions inherited from G4VEmModel
 G4VEmModel (const G4String &nam)
 
virtual ~G4VEmModel ()
 
virtual void InitialiseLocal (const G4ParticleDefinition *, G4VEmModel *masterModel)
 
virtual void InitialiseForMaterial (const G4ParticleDefinition *, const G4Material *)
 
virtual void InitialiseForElement (const G4ParticleDefinition *, G4int Z)
 
virtual G4double ComputeDEDXPerVolume (const G4Material *, const G4ParticleDefinition *, G4double kineticEnergy, G4double cutEnergy=DBL_MAX)
 
virtual G4double CrossSectionPerVolume (const G4Material *, const G4ParticleDefinition *, G4double kineticEnergy, G4double cutEnergy=0.0, G4double maxEnergy=DBL_MAX)
 
virtual G4double ChargeSquareRatio (const G4Track &)
 
virtual G4double GetChargeSquareRatio (const G4ParticleDefinition *, const G4Material *, G4double kineticEnergy)
 
virtual G4double GetParticleCharge (const G4ParticleDefinition *, const G4Material *, G4double kineticEnergy)
 
virtual void StartTracking (G4Track *)
 
virtual void CorrectionsAlongStep (const G4MaterialCutsCouple *, const G4DynamicParticle *, G4double &eloss, G4double &niel, G4double length)
 
virtual G4double Value (const G4MaterialCutsCouple *, const G4ParticleDefinition *, G4double kineticEnergy)
 
virtual G4double MinPrimaryEnergy (const G4Material *, const G4ParticleDefinition *, G4double cut=0.0)
 
virtual G4double MinEnergyCut (const G4ParticleDefinition *, const G4MaterialCutsCouple *)
 
virtual void SetupForMaterial (const G4ParticleDefinition *, const G4Material *, G4double kineticEnergy)
 
virtual void DefineForRegion (const G4Region *)
 
void InitialiseElementSelectors (const G4ParticleDefinition *, const G4DataVector &)
 
std::vector
< G4EmElementSelector * > * 		GetElementSelectors ()
 
void SetElementSelectors (std::vector< G4EmElementSelector * > *)
 
G4double ComputeDEDX (const G4MaterialCutsCouple *, const G4ParticleDefinition *, G4double kineticEnergy, G4double cutEnergy=DBL_MAX)
 
G4double CrossSection (const G4MaterialCutsCouple *, const G4ParticleDefinition *, G4double kineticEnergy, G4double cutEnergy=0.0, G4double maxEnergy=DBL_MAX)
 
G4double ComputeMeanFreePath (const G4ParticleDefinition *, G4double kineticEnergy, const G4Material *, G4double cutEnergy=0.0, G4double maxEnergy=DBL_MAX)
 
G4double ComputeCrossSectionPerAtom (const G4ParticleDefinition *, const G4Element *, G4double kinEnergy, G4double cutEnergy=0.0, G4double maxEnergy=DBL_MAX)
 
G4int SelectIsotopeNumber (const G4Element *)
 
const G4Element * SelectRandomAtom (const G4MaterialCutsCouple *, const G4ParticleDefinition *, G4double kineticEnergy, G4double cutEnergy=0.0, G4double maxEnergy=DBL_MAX)
 
const G4Element * SelectRandomAtom (const G4Material *, const G4ParticleDefinition *, G4double kineticEnergy, G4double cutEnergy=0.0, G4double maxEnergy=DBL_MAX)
 
G4int SelectRandomAtomNumber (const G4Material *)
 
void SetParticleChange (G4VParticleChange *, G4VEmFluctuationModel *f=0)
 
void SetCrossSectionTable (G4PhysicsTable *, G4bool isLocal)
 
G4ElementData * GetElementData ()
 
G4PhysicsTable * GetCrossSectionTable ()
 
G4VEmFluctuationModel * GetModelOfFluctuations ()
 
G4VEmAngularDistribution * GetAngularDistribution ()
 
void SetAngularDistribution (G4VEmAngularDistribution *)
 
G4double HighEnergyLimit () const
 
G4double LowEnergyLimit () const
 
G4double HighEnergyActivationLimit () const
 
G4double LowEnergyActivationLimit () const
 
G4double PolarAngleLimit () const
 
G4double SecondaryThreshold () const
 
G4bool LPMFlag () const
 
G4bool DeexcitationFlag () const
 
G4bool ForceBuildTableFlag () const
 
G4bool UseAngularGeneratorFlag () const
 
void SetAngularGeneratorFlag (G4bool)
 
void SetHighEnergyLimit (G4double)
 
void SetLowEnergyLimit (G4double)
 
void SetActivationHighEnergyLimit (G4double)
 
void SetActivationLowEnergyLimit (G4double)
 
G4bool IsActive (G4double kinEnergy)
 
void SetPolarAngleLimit (G4double)
 
void SetSecondaryThreshold (G4double)
 
void SetLPMFlag (G4bool val)
 
void SetDeexcitationFlag (G4bool val)
 
void SetForceBuildTable (G4bool val)
 
void SetMasterThread (G4bool val)
 
G4bool IsMaster () const
 
G4double MaxSecondaryKinEnergy (const G4DynamicParticle *dynParticle)
 
const G4String & GetName () const
 
void SetCurrentCouple (const G4MaterialCutsCouple *)
 
const G4Element * GetCurrentElement () const
 

Protected Member Functions

G4double GetMeanFreePath (const G4Track &aTrack, G4double previousStepSize, G4ForceCondition *condition)
 
- Protected Member Functions inherited from G4VEmModel
G4ParticleChangeForLoss * GetParticleChangeForLoss ()
 
G4ParticleChangeForGamma * GetParticleChangeForGamma ()
 
virtual G4double MaxSecondaryEnergy (const G4ParticleDefinition *, G4double kineticEnergy)
 
const G4MaterialCutsCouple * CurrentCouple () const
 
void SetCurrentElement (const G4Element *)
 

Protected Attributes

G4ParticleChangeForGamma * fParticleChange
 
- Protected Attributes inherited from G4VEmModel
G4ElementData * fElementData
 
G4VParticleChange * pParticleChange
 
G4PhysicsTable * xSectionTable
 
const std::vector< G4double > * theDensityFactor
 
const std::vector< G4int > * theDensityIdx
 
size_t idxTable
 

Detailed Description

Definition at line 43 of file G4LivermoreNuclearGammaConversionModel.hh.

Constructor & Destructor Documentation

G4LivermoreNuclearGammaConversionModel::G4LivermoreNuclearGammaConversionModel ( const G4ParticleDefinition *  p = 0,
const G4String &  nam = "LivermoreNuclearGammaConversion" 
)

Definition at line 41 of file G4LivermoreNuclearGammaConversionModel.cc.

References python.hepunit::electron_mass_c2, G4cout, G4endl, python.hepunit::GeV, python.hepunit::MeV, and G4VEmModel::SetHighEnergyLimit().

43  :G4VEmModel(nam),fParticleChange(0),smallEnergy(2.*MeV),
44  isInitialised(false),
45  crossSectionHandler(0),meanFreePathTable(0)
46 {
47  lowEnergyLimit = 2.0*electron_mass_c2;
48  highEnergyLimit = 100 * GeV;
49  SetHighEnergyLimit(highEnergyLimit);
50 
51  verboseLevel= 0;
52  // Verbosity scale:
53  // 0 = nothing
54  // 1 = warning for energy non-conservation
55  // 2 = details of energy budget
56  // 3 = calculation of cross sections, file openings, sampling of atoms
57  // 4 = entering in methods
58 
59  if(verboseLevel > 0) {
60  G4cout << "Livermore Nuclear Gamma conversion is constructed " << G4endl
61  << "Energy range: "
62  << lowEnergyLimit / MeV << " MeV - "
63  << highEnergyLimit / GeV << " GeV"
64  << G4endl;
65  }
66 }
G4VEmModel::G4VEmModel
G4VEmModel(const G4String &nam)
Definition: G4VEmModel.cc:65
G4VEmModel::SetHighEnergyLimit
void SetHighEnergyLimit(G4double)
Definition: G4VEmModel.hh:683
G4cout
G4GLOB_DLL std::ostream G4cout
python.hepunit.electron_mass_c2
float electron_mass_c2
Definition: hepunit.py:274
G4endl
#define G4endl
Definition: G4ios.hh:61
G4LivermoreNuclearGammaConversionModel::~G4LivermoreNuclearGammaConversionModel ( )
virtual

Definition at line 70 of file G4LivermoreNuclearGammaConversionModel.cc.

71 {
72  if (crossSectionHandler) delete crossSectionHandler;
73 }

Member Function Documentation

G4double G4LivermoreNuclearGammaConversionModel::ComputeCrossSectionPerAtom ( const G4ParticleDefinition *  ,
G4double  kinEnergy,
G4double  Z,
G4double  A = 0,
G4double  cut = 0,
G4double  emax = DBL_MAX 
)
virtual

Reimplemented from G4VEmModel.

Definition at line 121 of file G4LivermoreNuclearGammaConversionModel.cc.

References G4VCrossSectionHandler::FindValue(), G4cout, and G4endl.

125 {
126  if (verboseLevel > 3) {
127  G4cout << "Calling ComputeCrossSectionPerAtom() of G4LivermoreNuclearGammaConversionModel"
128  << G4endl;
129  }
130  if (GammaEnergy < lowEnergyLimit || GammaEnergy > highEnergyLimit) return 0;
131 
132  G4double cs = crossSectionHandler->FindValue(G4int(Z), GammaEnergy);
133  return cs;
134 }
G4int
int G4int
Definition: G4Types.hh:78
G4VCrossSectionHandler::FindValue
G4double FindValue(G4int Z, G4double e) const
Definition: G4VCrossSectionHandler.cc:379
G4cout
G4GLOB_DLL std::ostream G4cout
G4endl
#define G4endl
Definition: G4ios.hh:61
G4double
double G4double
Definition: G4Types.hh:76
G4double G4LivermoreNuclearGammaConversionModel::GetMeanFreePath ( const G4Track &  aTrack,
G4double  previousStepSize,
G4ForceCondition *  condition 
)
protected
void G4LivermoreNuclearGammaConversionModel::Initialise ( const G4ParticleDefinition *  ,
const G4DataVector &   
)
virtual

Implements G4VEmModel.

Definition at line 78 of file G4LivermoreNuclearGammaConversionModel.cc.

References G4VCrossSectionHandler::Clear(), fParticleChange, G4cout, G4endl, G4VEmModel::GetParticleChangeForGamma(), python.hepunit::GeV, G4VEmModel::HighEnergyLimit(), G4VCrossSectionHandler::Initialise(), G4VCrossSectionHandler::LoadData(), G4VEmModel::LowEnergyLimit(), and python.hepunit::MeV.

80 {
81  if (verboseLevel > 3)
82  G4cout << "Calling G4LivermoreNuclearGammaConversionModel::Initialise()" << G4endl;
83 
84  if (crossSectionHandler)
85  {
86  crossSectionHandler->Clear();
87  delete crossSectionHandler;
88  }
89 
90  // Read data tables for all materials
91 
92  crossSectionHandler = new G4CrossSectionHandler();
93  crossSectionHandler->Initialise(0,lowEnergyLimit,100.*GeV,400);
94  G4String crossSectionFile = "pairdata/pp-pair-cs-"; // here only pair in nuclear field cs should be used
95  crossSectionHandler->LoadData(crossSectionFile);
96 
97  //
98 
99  if (verboseLevel > 0) {
100  G4cout << "Loaded cross section files for Livermore GammaConversion" << G4endl;
101  G4cout << "To obtain the total cross section this should be used only " << G4endl
102  << "in connection with G4ElectronGammaConversion " << G4endl;
103  }
104 
105  if (verboseLevel > 0) {
106  G4cout << "Livermore Nuclear Gamma Conversion model is initialized " << G4endl
107  << "Energy range: "
108  << LowEnergyLimit() / MeV << " MeV - "
109  << HighEnergyLimit() / GeV << " GeV"
110  << G4endl;
111  }
112 
113  if(isInitialised) return;
114  fParticleChange = GetParticleChangeForGamma();
115  isInitialised = true;
116 }
G4VEmModel::LowEnergyLimit
G4double LowEnergyLimit() const
Definition: G4VEmModel.hh:599
G4VEmModel::HighEnergyLimit
G4double HighEnergyLimit() const
Definition: G4VEmModel.hh:592
G4cout
G4GLOB_DLL std::ostream G4cout
G4VCrossSectionHandler::Initialise
void Initialise(G4VDataSetAlgorithm *interpolation=0, G4double minE=250 *CLHEP::eV, G4double maxE=100 *CLHEP::GeV, G4int numberOfBins=200, G4double unitE=CLHEP::MeV, G4double unitData=CLHEP::barn, G4int minZ=1, G4int maxZ=99)
Definition: G4VCrossSectionHandler.cc:140
G4VCrossSectionHandler::LoadData
void LoadData(const G4String &dataFile)
Definition: G4VCrossSectionHandler.cc:187
G4endl
#define G4endl
Definition: G4ios.hh:61
G4VEmModel::GetParticleChangeForGamma
G4ParticleChangeForGamma * GetParticleChangeForGamma()
Definition: G4VEmModel.cc:121
void G4LivermoreNuclearGammaConversionModel::SampleSecondaries ( std::vector< G4DynamicParticle * > *  fvect,
const G4MaterialCutsCouple *  couple,
const G4DynamicParticle *  aDynamicGamma,
G4double  tmin,
G4double  maxEnergy 
)
virtual

Implements G4VEmModel.

Definition at line 138 of file G4LivermoreNuclearGammaConversionModel.cc.

References G4Electron::Electron(), python.hepunit::electron_mass_c2, fParticleChange, fStopAndKill, G4cout, G4endl, G4UniformRand, G4DynamicParticle::GetDefinition(), G4Element::GetfCoulomb(), G4Element::GetIonisation(), G4DynamicParticle::GetKineticEnergy(), G4IonisParamElm::GetlogZ3(), G4DynamicParticle::GetMomentumDirection(), G4IonisParamElm::GetZ3(), G4INCL::Math::max(), python.hepunit::MeV, G4INCL::Math::min(), G4Positron::Positron(), G4VParticleChange::ProposeTrackStatus(), CLHEP::Hep3Vector::rotateUz(), G4VEmModel::SelectRandomAtom(), G4ParticleChangeForGamma::SetProposedKineticEnergy(), and python.hepunit::twopi.

143 {
144 
145 // The energies of the e+ e- secondaries are sampled using the Bethe - Heitler
146 // cross sections with Coulomb correction. A modified version of the random
147 // number techniques of Butcher & Messel is used (Nuc Phys 20(1960),15).
148 
149 // Note 1 : Effects due to the breakdown of the Born approximation at low
150 // energy are ignored.
151 // Note 2 : The differential cross section implicitly takes account of
152 // pair creation in both nuclear and atomic electron fields. However triplet
153 // prodution is not generated.
154 
155  if (verboseLevel > 3)
156  G4cout << "Calling SampleSecondaries() of G4LivermoreNuclearGammaConversionModel" << G4endl;
157 
158  G4double photonEnergy = aDynamicGamma->GetKineticEnergy();
159  G4ParticleMomentum photonDirection = aDynamicGamma->GetMomentumDirection();
160 
161  G4double epsilon ;
162  G4double epsilon0Local = electron_mass_c2 / photonEnergy ;
163 
164  // Do it fast if photon energy < 2. MeV
165  if (photonEnergy < smallEnergy )
166  {
167  epsilon = epsilon0Local + (0.5 - epsilon0Local) * G4UniformRand();
168  }
169  else
170  {
171  // Select randomly one element in the current material
172  //const G4Element* element = crossSectionHandler->SelectRandomElement(couple,photonEnergy);
173  const G4ParticleDefinition* particle = aDynamicGamma->GetDefinition();
174  const G4Element* element = SelectRandomAtom(couple,particle,photonEnergy);
175 
176  if (element == 0)
177  {
178  G4cout << "G4LivermoreNuclearGammaConversionModel::SampleSecondaries - element = 0"
179  << G4endl;
180  return;
181  }
182  G4IonisParamElm* ionisation = element->GetIonisation();
183  if (ionisation == 0)
184  {
185  G4cout << "G4LivermoreNuclearGammaConversionModel::SampleSecondaries - ionisation = 0"
186  << G4endl;
187  return;
188  }
189 
190  // Extract Coulomb factor for this Element
191  G4double fZ = 8. * (ionisation->GetlogZ3());
192  if (photonEnergy > 50. * MeV) fZ += 8. * (element->GetfCoulomb());
193 
194  // Limits of the screening variable
195  G4double screenFactor = 136. * epsilon0Local / (element->GetIonisation()->GetZ3()) ;
196  G4double screenMax = std::exp ((42.24 - fZ)/8.368) - 0.952 ;
197  G4double screenMin = std::min(4.*screenFactor,screenMax) ;
198 
199  // Limits of the energy sampling
200  G4double epsilon1 = 0.5 - 0.5 * std::sqrt(1. - screenMin / screenMax) ;
201  G4double epsilonMin = std::max(epsilon0Local,epsilon1);
202  G4double epsilonRange = 0.5 - epsilonMin ;
203 
204  // Sample the energy rate of the created electron (or positron)
205  G4double screen;
206  G4double gReject ;
207 
208  G4double f10 = ScreenFunction1(screenMin) - fZ;
209  G4double f20 = ScreenFunction2(screenMin) - fZ;
210  G4double normF1 = std::max(f10 * epsilonRange * epsilonRange,0.);
211  G4double normF2 = std::max(1.5 * f20,0.);
212 
213  do {
214  if (normF1 / (normF1 + normF2) > G4UniformRand() )
215  {
216  epsilon = 0.5 - epsilonRange * std::pow(G4UniformRand(), 0.3333) ;
217  screen = screenFactor / (epsilon * (1. - epsilon));
218  gReject = (ScreenFunction1(screen) - fZ) / f10 ;
219  }
220  else
221  {
222  epsilon = epsilonMin + epsilonRange * G4UniformRand();
223  screen = screenFactor / (epsilon * (1 - epsilon));
224  gReject = (ScreenFunction2(screen) - fZ) / f20 ;
225  }
226  } while ( gReject < G4UniformRand() );
227 
228  } // End of epsilon sampling
229 
230  // Fix charges randomly
231 
232  G4double electronTotEnergy;
233  G4double positronTotEnergy;
234 
235  if (G4int(2*G4UniformRand()))
236  {
237  electronTotEnergy = (1. - epsilon) * photonEnergy;
238  positronTotEnergy = epsilon * photonEnergy;
239  }
240  else
241  {
242  positronTotEnergy = (1. - epsilon) * photonEnergy;
243  electronTotEnergy = epsilon * photonEnergy;
244  }
245 
246  // Scattered electron (positron) angles. ( Z - axis along the parent photon)
247  // Universal distribution suggested by L. Urban (Geant3 manual (1993) Phys211),
248  // derived from Tsai distribution (Rev. Mod. Phys. 49, 421 (1977)
249 
250  G4double u;
251  const G4double a1 = 0.625;
252  G4double a2 = 3. * a1;
253  // G4double d = 27. ;
254 
255  // if (9. / (9. + d) > G4UniformRand())
256  if (0.25 > G4UniformRand())
257  {
258  u = - std::log(G4UniformRand() * G4UniformRand()) / a1 ;
259  }
260  else
261  {
262  u = - std::log(G4UniformRand() * G4UniformRand()) / a2 ;
263  }
264 
265  G4double thetaEle = u*electron_mass_c2/electronTotEnergy;
266  G4double thetaPos = u*electron_mass_c2/positronTotEnergy;
267  G4double phi = twopi * G4UniformRand();
268 
269  G4double dxEle= std::sin(thetaEle)*std::cos(phi),dyEle= std::sin(thetaEle)*std::sin(phi),dzEle=std::cos(thetaEle);
270  G4double dxPos=-std::sin(thetaPos)*std::cos(phi),dyPos=-std::sin(thetaPos)*std::sin(phi),dzPos=std::cos(thetaPos);
271 
272 
273  // Kinematics of the created pair:
274  // the electron and positron are assumed to have a symetric angular
275  // distribution with respect to the Z axis along the parent photon
276 
277  G4double electronKineEnergy = std::max(0.,electronTotEnergy - electron_mass_c2) ;
278 
279  // SI - The range test has been removed wrt original G4LowEnergyGammaconversion class
280 
281  G4ThreeVector electronDirection (dxEle, dyEle, dzEle);
282  electronDirection.rotateUz(photonDirection);
283 
284  G4DynamicParticle* particle1 = new G4DynamicParticle (G4Electron::Electron(),
285  electronDirection,
286  electronKineEnergy);
287 
288  // The e+ is always created (even with kinetic energy = 0) for further annihilation
289  G4double positronKineEnergy = std::max(0.,positronTotEnergy - electron_mass_c2) ;
290 
291  // SI - The range test has been removed wrt original G4LowEnergyGammaconversion class
292 
293  G4ThreeVector positronDirection (dxPos, dyPos, dzPos);
294  positronDirection.rotateUz(photonDirection);
295 
296  // Create G4DynamicParticle object for the particle2
297  G4DynamicParticle* particle2 = new G4DynamicParticle(G4Positron::Positron(),
298  positronDirection, positronKineEnergy);
299  // Fill output vector
300 
301  fvect->push_back(particle1);
302  fvect->push_back(particle2);
303 
304  // kill incident photon
305  fParticleChange->SetProposedKineticEnergy(0.);
306  fParticleChange->ProposeTrackStatus(fStopAndKill);
307 
308 }
G4DynamicParticle::GetKineticEnergy
G4double GetKineticEnergy() const
G4Element::GetfCoulomb
G4double GetfCoulomb() const
Definition: G4Element.hh:190
G4DynamicParticle::GetDefinition
G4ParticleDefinition * GetDefinition() const
G4int
int G4int
Definition: G4Types.hh:78
G4UniformRand
#define G4UniformRand()
Definition: Randomize.hh:87
G4cout
G4GLOB_DLL std::ostream G4cout
G4DynamicParticle::GetMomentumDirection
const G4ThreeVector & GetMomentumDirection() const
python.hepunit.electron_mass_c2
float electron_mass_c2
Definition: hepunit.py:274
G4IonisParamElm::GetlogZ3
G4double GetlogZ3() const
Definition: G4IonisParamElm.hh:63
G4Positron::Positron
static G4Positron * Positron()
Definition: G4Positron.cc:94
G4INCL::Math::max
T max(const T t1, const T t2)
brief Return the largest of the two arguments
Definition: G4INCLGlobals.hh:116
G4Element::GetIonisation
G4IonisParamElm * GetIonisation() const
Definition: G4Element.hh:198
G4INCL::Math::min
T min(const T t1, const T t2)
brief Return the smallest of the two arguments
Definition: G4INCLGlobals.hh:121
fStopAndKill
Definition: G4TrackStatus.hh:56
G4Electron::Electron
static G4Electron * Electron()
Definition: G4Electron.cc:94
G4ParticleChangeForGamma::SetProposedKineticEnergy
void SetProposedKineticEnergy(G4double proposedKinEnergy)
Definition: G4ParticleChangeForGamma.hh:129
G4endl
#define G4endl
Definition: G4ios.hh:61
G4double
double G4double
Definition: G4Types.hh:76
G4VParticleChange::ProposeTrackStatus
void ProposeTrackStatus(G4TrackStatus status)
G4IonisParamElm::GetZ3
G4double GetZ3() const
Definition: G4IonisParamElm.hh:61
G4VEmModel::SelectRandomAtom
const G4Element * SelectRandomAtom(const G4MaterialCutsCouple *, const G4ParticleDefinition *, G4double kineticEnergy, G4double cutEnergy=0.0, G4double maxEnergy=DBL_MAX)
Definition: G4VEmModel.hh:510

Field Documentation

G4ParticleChangeForGamma* G4LivermoreNuclearGammaConversionModel::fParticleChange
protected

Definition at line 71 of file G4LivermoreNuclearGammaConversionModel.hh.

Referenced by Initialise(), and SampleSecondaries().

The documentation for this class was generated from the following files:
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