Geant4 10.7.0
Toolkit for the simulation of the passage of particles through matter
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G4RPGSigmaPlusInelastic.cc
Go to the documentation of this file.
1//
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25//
26//
27
29#include "G4Exp.hh"
31#include "G4SystemOfUnits.hh"
32#include "Randomize.hh"
33
36 G4Nucleus &targetNucleus )
37{
38 const G4HadProjectile *originalIncident = &aTrack;
39 if (originalIncident->GetKineticEnergy()<= 0.1*MeV)
40 {
44 return &theParticleChange;
45 }
46
47 // create the target particle
48
49 G4DynamicParticle *originalTarget = targetNucleus.ReturnTargetParticle();
50
51 if( verboseLevel > 1 )
52 {
53 const G4Material *targetMaterial = aTrack.GetMaterial();
54 G4cout << "G4RPGSigmaPlusInelastic::ApplyYourself called" << G4endl;
55 G4cout << "kinetic energy = " << originalIncident->GetKineticEnergy()/MeV << "MeV, ";
56 G4cout << "target material = " << targetMaterial->GetName() << ", ";
57 G4cout << "target particle = " << originalTarget->GetDefinition()->GetParticleName()
58 << G4endl;
59 }
60
61 // Fermi motion and evaporation
62 // As of Geant3, the Fermi energy calculation had not been Done
63
64 G4double ek = originalIncident->GetKineticEnergy()/MeV;
65 G4double amas = originalIncident->GetDefinition()->GetPDGMass()/MeV;
66 G4ReactionProduct modifiedOriginal;
67 modifiedOriginal = *originalIncident;
68
69 G4double tkin = targetNucleus.Cinema( ek );
70 ek += tkin;
71 modifiedOriginal.SetKineticEnergy( ek*MeV );
72 G4double et = ek + amas;
73 G4double p = std::sqrt( std::abs((et-amas)*(et+amas)) );
74 G4double pp = modifiedOriginal.GetMomentum().mag()/MeV;
75 if( pp > 0.0 )
76 {
77 G4ThreeVector momentum = modifiedOriginal.GetMomentum();
78 modifiedOriginal.SetMomentum( momentum * (p/pp) );
79 }
80 //
81 // calculate black track energies
82 //
83 tkin = targetNucleus.EvaporationEffects( ek );
84 ek -= tkin;
85 modifiedOriginal.SetKineticEnergy( ek*MeV );
86 et = ek + amas;
87 p = std::sqrt( std::abs((et-amas)*(et+amas)) );
88 pp = modifiedOriginal.GetMomentum().mag()/MeV;
89 if( pp > 0.0 )
90 {
91 G4ThreeVector momentum = modifiedOriginal.GetMomentum();
92 modifiedOriginal.SetMomentum( momentum * (p/pp) );
93 }
94 G4ReactionProduct currentParticle = modifiedOriginal;
95 G4ReactionProduct targetParticle;
96 targetParticle = *originalTarget;
97 currentParticle.SetSide( 1 ); // incident always goes in forward hemisphere
98 targetParticle.SetSide( -1 ); // target always goes in backward hemisphere
99 G4bool incidentHasChanged = false;
100 G4bool targetHasChanged = false;
101 G4bool quasiElastic = false;
102 G4FastVector<G4ReactionProduct,GHADLISTSIZE> vec; // vec will contain the secondary particles
103 G4int vecLen = 0;
104 vec.Initialize( 0 );
105
106 const G4double cutOff = 0.1;
107 if( currentParticle.GetKineticEnergy()/MeV > cutOff )
108 Cascade( vec, vecLen,
109 originalIncident, currentParticle, targetParticle,
110 incidentHasChanged, targetHasChanged, quasiElastic );
111
112 CalculateMomenta( vec, vecLen,
113 originalIncident, originalTarget, modifiedOriginal,
114 targetNucleus, currentParticle, targetParticle,
115 incidentHasChanged, targetHasChanged, quasiElastic );
116
117 SetUpChange( vec, vecLen,
118 currentParticle, targetParticle,
119 incidentHasChanged );
120
121 delete originalTarget;
122 return &theParticleChange;
123}
124
125void G4RPGSigmaPlusInelastic::Cascade(
127 G4int& vecLen,
128 const G4HadProjectile *originalIncident,
129 G4ReactionProduct &currentParticle,
130 G4ReactionProduct &targetParticle,
131 G4bool &incidentHasChanged,
132 G4bool &targetHasChanged,
133 G4bool &quasiElastic )
134{
135 // Derived from H. Fesefeldt's original FORTRAN code CASSP
136 //
137 // SigmaPlus undergoes interaction with nucleon within a nucleus. Check if it is
138 // energetically possible to produce pions/kaons. In not, assume nuclear excitation
139 // occurs and input particle is degraded in energy. No other particles are produced.
140 // If reaction is possible, find the correct number of pions/protons/neutrons
141 // produced using an interpolation to multiplicity data. Replace some pions or
142 // protons/neutrons by kaons or strange baryons according to the average
143 // multiplicity per inelastic reaction.
144
145 const G4double mOriginal = originalIncident->GetDefinition()->GetPDGMass()/MeV;
146 const G4double etOriginal = originalIncident->GetTotalEnergy()/MeV;
147 const G4double targetMass = targetParticle.GetMass()/MeV;
148 G4double centerofmassEnergy = std::sqrt( mOriginal*mOriginal +
149 targetMass*targetMass +
150 2.0*targetMass*etOriginal );
151 G4double availableEnergy = centerofmassEnergy-(targetMass+mOriginal);
152 if( availableEnergy <= G4PionPlus::PionPlus()->GetPDGMass()/MeV )
153 {
154 quasiElastic = true;
155 return;
156 }
157 static G4ThreadLocal G4bool first = true;
158 const G4int numMul = 1200;
159 const G4int numSec = 60;
160 static G4ThreadLocal G4double protmul[numMul], protnorm[numSec]; // proton constants
161 static G4ThreadLocal G4double neutmul[numMul], neutnorm[numSec]; // neutron constants
162 // np = number of pi+, nneg = number of pi-, nz = number of pi0
163 G4int counter, nt=0, np=0, nneg=0, nz=0;
164 G4double test;
165 const G4double c = 1.25;
166 const G4double b[] = { 0.7, 0.7 };
167 if( first ) // compute normalization constants, this will only be Done once
168 {
169 first = false;
170 G4int i;
171 for( i=0; i<numMul; ++i )protmul[i] = 0.0;
172 for( i=0; i<numSec; ++i )protnorm[i] = 0.0;
173 counter = -1;
174 for( np=0; np<(numSec/3); ++np )
175 {
176 for( nneg=np; nneg<=(np+2); ++nneg )
177 {
178 for( nz=0; nz<numSec/3; ++nz )
179 {
180 if( ++counter < numMul )
181 {
182 nt = np+nneg+nz;
183 if( nt>0 && nt<=numSec )
184 {
185 protmul[counter] = Pmltpc(np,nneg,nz,nt,b[0],c);
186 protnorm[nt-1] += protmul[counter];
187 }
188 }
189 }
190 }
191 }
192 for( i=0; i<numMul; ++i )neutmul[i] = 0.0;
193 for( i=0; i<numSec; ++i )neutnorm[i] = 0.0;
194 counter = -1;
195 for( np=0; np<numSec/3; ++np )
196 {
197 for( nneg=std::max(0,np-1); nneg<=(np+1); ++nneg )
198 {
199 for( nz=0; nz<numSec/3; ++nz )
200 {
201 if( ++counter < numMul )
202 {
203 nt = np+nneg+nz;
204 if( nt>0 && nt<=numSec )
205 {
206 neutmul[counter] = Pmltpc(np,nneg,nz,nt,b[1],c);
207 neutnorm[nt-1] += neutmul[counter];
208 }
209 }
210 }
211 }
212 }
213 for( i=0; i<numSec; ++i )
214 {
215 if( protnorm[i] > 0.0 )protnorm[i] = 1.0/protnorm[i];
216 if( neutnorm[i] > 0.0 )neutnorm[i] = 1.0/neutnorm[i];
217 }
218 } // end of initialization
219
220 const G4double expxu = 82.; // upper bound for arg. of exp
221 const G4double expxl = -expxu; // lower bound for arg. of exp
226 //
227 // energetically possible to produce pion(s) --> inelastic scattering
228 //
229 G4double n, anpn;
230 GetNormalizationConstant( availableEnergy, n, anpn );
231 G4double ran = G4UniformRand();
232 G4double dum, excs = 0.0;
233 if( targetParticle.GetDefinition() == aProton )
234 {
235 counter = -1;
236 for( np=0; np<numSec/3 && ran>=excs; ++np )
237 {
238 for( nneg=np; nneg<=(np+2) && ran>=excs; ++nneg )
239 {
240 for( nz=0; nz<numSec/3 && ran>=excs; ++nz )
241 {
242 if( ++counter < numMul )
243 {
244 nt = np+nneg+nz;
245 if( nt>0 && nt<=numSec )
246 {
247 test = G4Exp( std::min( expxu, std::max( expxl, -(pi/4.0)*(nt*nt)/(n*n) ) ) );
248 dum = (pi/anpn)*nt*protmul[counter]*protnorm[nt-1]/(2.0*n*n);
249 if( std::fabs(dum) < 1.0 )
250 {
251 if( test >= 1.0e-10 )excs += dum*test;
252 }
253 else
254 excs += dum*test;
255 }
256 }
257 }
258 }
259 }
260 if( ran >= excs ) // 3 previous loops continued to the end
261 {
262 quasiElastic = true;
263 return;
264 }
265 np--; nneg--; nz--;
266 switch( std::min( 3, std::max( 1, np-nneg+3 ) ) )
267 {
268 case 1:
269 if( G4UniformRand() < 0.5 )
270 currentParticle.SetDefinitionAndUpdateE( aLambda );
271 else
272 currentParticle.SetDefinitionAndUpdateE( aSigmaZero );
273 incidentHasChanged = true;
274 targetParticle.SetDefinitionAndUpdateE( aNeutron );
275 targetHasChanged = true;
276 break;
277 case 2:
278 if( G4UniformRand() < 0.5 )
279 {
280 targetParticle.SetDefinitionAndUpdateE( aNeutron );
281 targetHasChanged = true;
282 }
283 else
284 {
285 if( G4UniformRand() < 0.5 )
286 currentParticle.SetDefinitionAndUpdateE( aLambda );
287 else
288 currentParticle.SetDefinitionAndUpdateE( aSigmaZero );
289 incidentHasChanged = true;
290 }
291 break;
292 case 3:
293 break;
294 }
295 }
296 else // target must be a neutron
297 {
298 counter = -1;
299 for( np=0; np<numSec/3 && ran>=excs; ++np )
300 {
301 for( nneg=std::max(0,np-1); nneg<=(np+1) && ran>=excs; ++nneg )
302 {
303 for( nz=0; nz<numSec/3 && ran>=excs; ++nz )
304 {
305 if( ++counter < numMul )
306 {
307 nt = np+nneg+nz;
308 if( nt>0 && nt<=numSec )
309 {
310 test = G4Exp( std::min( expxu, std::max( expxl, -(pi/4.0)*(nt*nt)/(n*n) ) ) );
311 dum = (pi/anpn)*nt*neutmul[counter]*neutnorm[nt-1]/(2.0*n*n);
312 if( std::fabs(dum) < 1.0 )
313 {
314 if( test >= 1.0e-10 )excs += dum*test;
315 }
316 else
317 excs += dum*test;
318 }
319 }
320 }
321 }
322 }
323 if( ran >= excs ) // 3 previous loops continued to the end
324 {
325 quasiElastic = true;
326 return;
327 }
328 np--; nneg--; nz--;
329 switch( std::min( 3, std::max( 1, np-nneg+2 ) ) )
330 {
331 case 1:
332 targetParticle.SetDefinitionAndUpdateE( aProton );
333 targetHasChanged = true;
334 break;
335 case 2:
336 if( G4UniformRand() < 0.5 )
337 {
338 if( G4UniformRand() < 0.5 )
339 {
340 currentParticle.SetDefinitionAndUpdateE( aLambda );
341 incidentHasChanged = true;
342 targetParticle.SetDefinitionAndUpdateE( aProton );
343 targetHasChanged = true;
344 }
345 else
346 {
347 targetParticle.SetDefinitionAndUpdateE( aNeutron );
348 targetHasChanged = true;
349 }
350 }
351 else
352 {
353 if( G4UniformRand() < 0.5 )
354 {
355 currentParticle.SetDefinitionAndUpdateE( aSigmaZero );
356 incidentHasChanged = true;
357 targetParticle.SetDefinitionAndUpdateE( aProton );
358 targetHasChanged = true;
359 }
360 }
361 break;
362 case 3:
363 if( G4UniformRand() < 0.5 )
364 currentParticle.SetDefinitionAndUpdateE( aLambda );
365 else
366 currentParticle.SetDefinitionAndUpdateE( aSigmaZero );
367 incidentHasChanged = true;
368 break;
369 }
370 }
371
372 SetUpPions(np, nneg, nz, vec, vecLen);
373 return;
374}
375
376 /* end of file */
377
G4double G4Exp(G4double initial_x)
Exponential Function double precision.
Definition: G4Exp.hh:179
@ isAlive
double G4double
Definition: G4Types.hh:83
bool G4bool
Definition: G4Types.hh:86
int G4int
Definition: G4Types.hh:85
#define G4endl
Definition: G4ios.hh:57
G4GLOB_DLL std::ostream G4cout
#define G4UniformRand()
Definition: Randomize.hh:52
Hep3Vector unit() const
double mag() const
Hep3Vector vect() const
G4ParticleDefinition * GetDefinition() const
void Initialize(G4int items)
Definition: G4FastVector.hh:59
void SetStatusChange(G4HadFinalStateStatus aS)
void SetEnergyChange(G4double anEnergy)
void SetMomentumChange(const G4ThreeVector &aV)
const G4Material * GetMaterial() const
const G4ParticleDefinition * GetDefinition() const
G4double GetKineticEnergy() const
const G4LorentzVector & Get4Momentum() const
G4double GetTotalEnergy() const
static G4Lambda * Lambda()
Definition: G4Lambda.cc:107
const G4String & GetName() const
Definition: G4Material.hh:175
static G4Neutron * Neutron()
Definition: G4Neutron.cc:103
G4double EvaporationEffects(G4double kineticEnergy)
Definition: G4Nucleus.cc:278
G4double Cinema(G4double kineticEnergy)
Definition: G4Nucleus.cc:382
G4DynamicParticle * ReturnTargetParticle() const
Definition: G4Nucleus.cc:241
const G4String & GetParticleName() const
static G4PionPlus * PionPlus()
Definition: G4PionPlus.cc:97
static G4Proton * Proton()
Definition: G4Proton.cc:92
void SetUpPions(const G4int np, const G4int nm, const G4int nz, G4FastVector< G4ReactionProduct, 256 > &vec, G4int &vecLen)
void GetNormalizationConstant(const G4double availableEnergy, G4double &n, G4double &anpn)
void CalculateMomenta(G4FastVector< G4ReactionProduct, 256 > &vec, G4int &vecLen, const G4HadProjectile *originalIncident, const G4DynamicParticle *originalTarget, G4ReactionProduct &modifiedOriginal, G4Nucleus &targetNucleus, G4ReactionProduct &currentParticle, G4ReactionProduct &targetParticle, G4bool &incidentHasChanged, G4bool &targetHasChanged, G4bool quasiElastic)
void SetUpChange(G4FastVector< G4ReactionProduct, 256 > &vec, G4int &vecLen, G4ReactionProduct &currentParticle, G4ReactionProduct &targetParticle, G4bool &incidentHasChanged)
G4double Pmltpc(G4int np, G4int nm, G4int nz, G4int n, G4double b, G4double c)
G4HadFinalState * ApplyYourself(const G4HadProjectile &aTrack, G4Nucleus &targetNucleus)
void SetMomentum(const G4double x, const G4double y, const G4double z)
G4double GetKineticEnergy() const
const G4ParticleDefinition * GetDefinition() const
G4ThreeVector GetMomentum() const
void SetSide(const G4int sid)
void SetDefinitionAndUpdateE(const G4ParticleDefinition *aParticleDefinition)
void SetKineticEnergy(const G4double en)
G4double GetMass() const
static G4SigmaZero * SigmaZero()
Definition: G4SigmaZero.cc:101
const G4double pi
#define G4ThreadLocal
Definition: tls.hh:77