Geant4-11
G4LivermoreIonisationModel.cc
Go to the documentation of this file.
1//
2// ********************************************************************
3// * License and Disclaimer *
4// * *
5// * The Geant4 software is copyright of the Copyright Holders of *
6// * the Geant4 Collaboration. It is provided under the terms and *
7// * conditions of the Geant4 Software License, included in the file *
8// * LICENSE and available at http://cern.ch/geant4/license . These *
9// * include a list of copyright holders. *
10// * *
11// * Neither the authors of this software system, nor their employing *
12// * institutes,nor the agencies providing financial support for this *
13// * work make any representation or warranty, express or implied, *
14// * regarding this software system or assume any liability for its *
15// * use. Please see the license in the file LICENSE and URL above *
16// * for the full disclaimer and the limitation of liability. *
17// * *
18// * This code implementation is the result of the scientific and *
19// * technical work of the GEANT4 collaboration. *
20// * By using, copying, modifying or distributing the software (or *
21// * any work based on the software) you agree to acknowledge its *
22// * use in resulting scientific publications, and indicate your *
23// * acceptance of all terms of the Geant4 Software license. *
24// ********************************************************************
25//
26//
27// Author: Luciano Pandola
28// on base of G4LowEnergyIonisation developed by A.Forti and V.Ivanchenko
29//
30// History:
31// --------
32// 12 Jan 2009 L Pandola Migration from process to model
33// 03 Mar 2009 L Pandola Bug fix (release memory in the destructor)
34// 15 Apr 2009 V Ivanchenko Cleanup initialisation and generation of secondaries:
35// - apply internal high-energy limit only in constructor
36// - do not apply low-energy limit (default is 0)
37// - simplify sampling of deexcitation by using cut in energy
38// - set activation of Auger "false"
39// - remove initialisation of element selectors
40// 19 May 2009 L Pandola Explicitely set to zero pointers deleted in
41// Initialise(), since they might be checked later on
42// 23 Oct 2009 L Pandola
43// - atomic deexcitation managed via G4VEmModel::DeexcitationFlag() is
44// set as "true" (default would be false)
45// 12 Oct 2010 L Pandola
46// - add debugging information about energy in
47// SampleDeexcitationAlongStep()
48// - generate fluorescence SampleDeexcitationAlongStep() only above
49// the cuts.
50// 01 Jun 2011 V Ivanchenko general cleanup - all old deexcitation code removed
51//
52
55#include "G4SystemOfUnits.hh"
59#include "G4DynamicParticle.hh"
60#include "G4Element.hh"
62#include "G4Electron.hh"
64#include "G4VEMDataSet.hh"
67#include "G4VEnergySpectrum.hh"
70#include "G4AtomicShell.hh"
71#include "G4DeltaAngle.hh"
72
73//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
74
75
77 const G4String& nam) :
78 G4VEmModel(nam), fParticleChange(nullptr),
79 crossSectionHandler(nullptr), energySpectrum(nullptr),
80 isInitialised(false)
81{
84
85 verboseLevel = 0;
87
89}
90
91//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
92
94{
95 delete energySpectrum;
97}
98
99//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
100
102 const G4DataVector& cuts)
103{
104 //Check that the Livermore Ionisation is NOT attached to e+
105 if (particle != G4Electron::Electron())
106 {
107 G4Exception("G4LivermoreIonisationModel::Initialise",
108 "em0002",FatalException,
109 "Livermore Ionisation Model is applicable only to electrons");
110 }
112
113 //Read energy spectrum
114 if (energySpectrum)
115 {
116 delete energySpectrum;
117 energySpectrum = nullptr;
118 }
120 if (verboseLevel > 3)
121 G4cout << "G4VEnergySpectrum is initialized" << G4endl;
122
123 //Initialize cross section handler
125 {
126 delete crossSectionHandler;
127 crossSectionHandler = nullptr;
128 }
129
130 const size_t nbins = 20;
131 G4double emin = LowEnergyLimit();
133 G4int ndec = G4int(std::log10(emax/emin) + 0.5);
134 if(ndec <= 0) { ndec = 1; }
135
136 G4VDataSetAlgorithm* interpolation = new G4SemiLogInterpolation();
139 emin,emax,nbins*ndec);
141 crossSectionHandler->LoadShellData("ioni/ion-ss-cs-");
142 //This is used to retrieve cross section values later on
143 G4VEMDataSet* emdata =
145 //The method BuildMeanFreePathForMaterials() is required here only to force
146 //the building of an internal table: the output pointer can be deleted
147 delete emdata;
148
149 if (verboseLevel > 0)
150 {
151 G4cout << "Livermore Ionisation model is initialized " << G4endl
152 << "Energy range: "
153 << LowEnergyLimit() / keV << " keV - "
154 << HighEnergyLimit() / GeV << " GeV"
155 << G4endl;
156 }
157
158 if (verboseLevel > 3)
159 {
160 G4cout << "Cross section data: " << G4endl;
162 G4cout << "Parameters: " << G4endl;
164 }
165
166 if(isInitialised) { return; }
168 isInitialised = true;
169}
170
171//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
172
178 G4double cutEnergy,
179 G4double)
180{
181 G4int iZ = G4int(Z);
183 {
184 G4Exception("G4LivermoreIonisationModel::ComputeCrossSectionPerAtom",
185 "em1007",FatalException,
186 "The cross section handler is not correctly initialized");
187 return 0;
188 }
189
190 //The cut is already included in the crossSectionHandler
191 G4double cs =
193 cutEnergy,
194 iZ);
195
196 if (verboseLevel > 1)
197 {
198 G4cout << "G4LivermoreIonisationModel " << G4endl;
199 G4cout << "Cross section for delta emission > "
200 << cutEnergy/keV << " keV at "
201 << energy/keV << " keV and Z = " << iZ << " --> "
202 << cs/barn << " barn" << G4endl;
203 }
204 return cs;
205}
206
207
208//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
209
213 G4double kineticEnergy,
214 G4double cutEnergy)
215{
216 G4double sPower = 0.0;
217
218 const G4ElementVector* theElementVector = material->GetElementVector();
219 size_t NumberOfElements = material->GetNumberOfElements() ;
220 const G4double* theAtomicNumDensityVector =
221 material->GetAtomicNumDensityVector();
222
223 // loop for elements in the material
224 for (size_t iel=0; iel<NumberOfElements; iel++ )
225 {
226 G4int iZ = (G4int)((*theElementVector)[iel]->GetZ());
228 for (G4int n=0; n<nShells; n++)
229 {
230 G4double e = energySpectrum->AverageEnergy(iZ, 0.0,cutEnergy,
231 kineticEnergy, n);
232 G4double cs= crossSectionHandler->FindValue(iZ,kineticEnergy, n);
233 sPower += e * cs * theAtomicNumDensityVector[iel];
234 }
235 G4double esp = energySpectrum->Excitation(iZ,kineticEnergy);
236 sPower += esp * theAtomicNumDensityVector[iel];
237 }
238
239 if (verboseLevel > 2)
240 {
241 G4cout << "G4LivermoreIonisationModel " << G4endl;
242 G4cout << "Stopping power < " << cutEnergy/keV
243 << " keV at " << kineticEnergy/keV << " keV = "
244 << sPower/(keV/mm) << " keV/mm" << G4endl;
245 }
246
247 return sPower;
248}
249
250//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
251
253 std::vector<G4DynamicParticle*>* fvect,
254 const G4MaterialCutsCouple* couple,
255 const G4DynamicParticle* aDynamicParticle,
256 G4double cutE,
257 G4double maxE)
258{
259
260 G4double kineticEnergy = aDynamicParticle->GetKineticEnergy();
261
262 if (kineticEnergy <= fIntrinsicLowEnergyLimit)
263 {
266 return;
267 }
268
269 // Select atom and shell
270 G4int Z = crossSectionHandler->SelectRandomAtom(couple, kineticEnergy);
271 G4int shellIndex = crossSectionHandler->SelectRandomShell(Z, kineticEnergy);
272 const G4AtomicShell* shell = transitionManager->Shell(Z,shellIndex);
274
275 // Sample delta energy using energy interval for delta-electrons
276 G4double energyMax =
277 std::min(maxE,energySpectrum->MaxEnergyOfSecondaries(kineticEnergy));
278 G4double energyDelta = energySpectrum->SampleEnergy(Z, cutE, energyMax,
279 kineticEnergy, shellIndex);
280
281 if (energyDelta == 0.) //nothing happens
282 { return; }
283
286 GetAngularDistribution()->SampleDirectionForShell(aDynamicParticle, energyDelta,
287 Z, shellIndex,
288 couple->GetMaterial()),
289 energyDelta);
290
291 fvect->push_back(delta);
292
293 // Change kinematics of primary particle
294 G4ThreeVector direction = aDynamicParticle->GetMomentumDirection();
295 G4double totalMomentum = std::sqrt(kineticEnergy*(kineticEnergy + 2*electron_mass_c2));
296
297 G4ThreeVector finalP = totalMomentum*direction - delta->GetMomentum();
298 finalP = finalP.unit();
299
300 //This is the amount of energy available for fluorescence
301 G4double theEnergyDeposit = bindingEnergy;
302
303 // fill ParticleChange
304 // changed energy and momentum of the actual particle
305 G4double finalKinEnergy = kineticEnergy - energyDelta - theEnergyDeposit;
306 if(finalKinEnergy < 0.0)
307 {
308 theEnergyDeposit += finalKinEnergy;
309 finalKinEnergy = 0.0;
310 }
311 else
312 {
314 }
316
317 if (theEnergyDeposit < 0)
318 {
319 G4cout << "G4LivermoreIonisationModel: Negative energy deposit: "
320 << theEnergyDeposit/eV << " eV" << G4endl;
321 theEnergyDeposit = 0.0;
322 }
323
324 //Assign local energy deposit
326
327 if (verboseLevel > 1)
328 {
329 G4cout << "-----------------------------------------------------------" << G4endl;
330 G4cout << "Energy balance from G4LivermoreIonisation" << G4endl;
331 G4cout << "Incoming primary energy: " << kineticEnergy/keV << " keV" << G4endl;
332 G4cout << "-----------------------------------------------------------" << G4endl;
333 G4cout << "Outgoing primary energy: " << finalKinEnergy/keV << " keV" << G4endl;
334 G4cout << "Delta ray " << energyDelta/keV << " keV" << G4endl;
335 G4cout << "Fluorescence: " << (bindingEnergy-theEnergyDeposit)/keV << " keV" << G4endl;
336 G4cout << "Local energy deposit " << theEnergyDeposit/keV << " keV" << G4endl;
337 G4cout << "Total final state: " << (finalKinEnergy+energyDelta+bindingEnergy)
338 << " keV" << G4endl;
339 G4cout << "-----------------------------------------------------------" << G4endl;
340 }
341 return;
342}
343
344//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
345
static const G4double emax
std::vector< const G4Element * > G4ElementVector
@ FatalException
void G4Exception(const char *originOfException, const char *exceptionCode, G4ExceptionSeverity severity, const char *description)
Definition: G4Exception.cc:35
static constexpr double barn
Definition: G4SIunits.hh:85
static constexpr double mm
Definition: G4SIunits.hh:95
static constexpr double keV
Definition: G4SIunits.hh:202
static constexpr double eV
Definition: G4SIunits.hh:201
static constexpr double GeV
Definition: G4SIunits.hh:203
double G4double
Definition: G4Types.hh:83
int G4int
Definition: G4Types.hh:85
const G4int Z[17]
#define G4endl
Definition: G4ios.hh:57
G4GLOB_DLL std::ostream G4cout
Hep3Vector unit() const
G4double BindingEnergy() const
G4AtomicShell * Shell(G4int Z, size_t shellIndex) const
void Initialise()
needs to be called once from other code before start of run
static G4AtomicTransitionManager * Instance()
const G4ThreeVector & GetMomentumDirection() const
G4double GetKineticEnergy() const
G4ThreeVector GetMomentum() const
static G4Electron * Electron()
Definition: G4Electron.cc:93
G4AtomicTransitionManager * transitionManager
void SampleSecondaries(std::vector< G4DynamicParticle * > *, const G4MaterialCutsCouple *, const G4DynamicParticle *, G4double tmin, G4double maxEnergy) override
G4eIonisationCrossSectionHandler * crossSectionHandler
G4ParticleChangeForLoss * fParticleChange
G4double ComputeDEDXPerVolume(const G4Material *, const G4ParticleDefinition *, G4double kineticEnergy, G4double cutEnergy) override
void Initialise(const G4ParticleDefinition *, const G4DataVector &) override
G4LivermoreIonisationModel(const G4ParticleDefinition *p=nullptr, const G4String &processName="LowEnergyIoni")
G4double ComputeCrossSectionPerAtom(const G4ParticleDefinition *, G4double kinEnergy, G4double Z, G4double A=0, G4double cut=0, G4double emax=DBL_MAX) override
const G4Material * GetMaterial() const
void SetProposedKineticEnergy(G4double proposedKinEnergy)
void ProposeMomentumDirection(G4double Px, G4double Py, G4double Pz)
void LoadShellData(const G4String &dataFile)
G4VEMDataSet * BuildMeanFreePathForMaterials(const G4DataVector *energyCuts=nullptr)
G4double FindValue(G4int Z, G4double e) const
G4int SelectRandomAtom(const G4MaterialCutsCouple *couple, G4double e) const
G4int SelectRandomShell(G4int Z, G4double e) const
G4VEmAngularDistribution * GetAngularDistribution()
Definition: G4VEmModel.hh:621
G4double LowEnergyLimit() const
Definition: G4VEmModel.hh:662
G4double HighEnergyLimit() const
Definition: G4VEmModel.hh:655
void SetAngularDistribution(G4VEmAngularDistribution *)
Definition: G4VEmModel.hh:628
G4ParticleChangeForLoss * GetParticleChangeForLoss()
Definition: G4VEmModel.cc:108
virtual void PrintData() const =0
virtual G4double MaxEnergyOfSecondaries(G4double kineticEnergy, G4int Z=0, const G4ParticleDefinition *pd=nullptr) const =0
virtual G4double AverageEnergy(G4int Z, G4double minKineticEnergy, G4double maxKineticEnergy, G4double kineticEnergy, G4int shell=0, const G4ParticleDefinition *pd=nullptr) const =0
virtual G4double SampleEnergy(G4int Z, G4double minKineticEnergy, G4double maxKineticEnergy, G4double kineticEnergy, G4int shell=0, const G4ParticleDefinition *pd=nullptr) const =0
virtual G4double Excitation(G4int Z, G4double kineticEnergy) const =0
void ProposeLocalEnergyDeposit(G4double anEnergyPart)
G4double GetCrossSectionAboveThresholdForElement(G4double energy, G4double cutEnergy, G4int Z)
G4double energy(const ThreeVector &p, const G4double m)
T min(const T t1, const T t2)
brief Return the smallest of the two arguments
G4double bindingEnergy(G4int A, G4int Z)
string material
Definition: eplot.py:19
float electron_mass_c2
Definition: hepunit.py:273