Geant4 9.6.0
Toolkit for the simulation of the passage of particles through matter
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G4RPGAntiXiMinusInelastic.cc
Go to the documentation of this file.
1//
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25//
26// $Id$
27//
28//
29// NOTE: The FORTRAN version of the cascade, CASAXM, simply called the
30// routine for the XiMinus particle. Hence, the ApplyYourself function
31// below is just a copy of the ApplyYourself from the XiMinus particle.
32
35#include "G4SystemOfUnits.hh"
36#include "Randomize.hh"
37
40 G4Nucleus &targetNucleus )
41{
42 const G4HadProjectile *originalIncident = &aTrack;
43 if (originalIncident->GetKineticEnergy()<= 0.1*MeV)
44 {
48 return &theParticleChange;
49 }
50
51 // create the target particle
52
53 G4DynamicParticle *originalTarget = targetNucleus.ReturnTargetParticle();
54
55 if( verboseLevel > 1 )
56 {
57 const G4Material *targetMaterial = aTrack.GetMaterial();
58 G4cout << "G4RPGAntiXiMinusInelastic::ApplyYourself called" << G4endl;
59 G4cout << "kinetic energy = " << originalIncident->GetKineticEnergy()/MeV << "MeV, ";
60 G4cout << "target material = " << targetMaterial->GetName() << ", ";
61 G4cout << "target particle = " << originalTarget->GetDefinition()->GetParticleName()
62 << G4endl;
63 }
64 //
65 // Fermi motion and evaporation
66 // As of Geant3, the Fermi energy calculation had not been Done
67 //
68 G4double ek = originalIncident->GetKineticEnergy()/MeV;
69 G4double amas = originalIncident->GetDefinition()->GetPDGMass()/MeV;
70 G4ReactionProduct modifiedOriginal;
71 modifiedOriginal = *originalIncident;
72
73 G4double tkin = targetNucleus.Cinema( ek );
74 ek += tkin;
75 modifiedOriginal.SetKineticEnergy( ek*MeV );
76 G4double et = ek + amas;
77 G4double p = std::sqrt( std::abs((et-amas)*(et+amas)) );
78 G4double pp = modifiedOriginal.GetMomentum().mag()/MeV;
79 if( pp > 0.0 )
80 {
81 G4ThreeVector momentum = modifiedOriginal.GetMomentum();
82 modifiedOriginal.SetMomentum( momentum * (p/pp) );
83 }
84 //
85 // calculate black track energies
86 //
87 tkin = targetNucleus.EvaporationEffects( ek );
88 ek -= tkin;
89 modifiedOriginal.SetKineticEnergy( ek*MeV );
90 et = ek + amas;
91 p = std::sqrt( std::abs((et-amas)*(et+amas)) );
92 pp = modifiedOriginal.GetMomentum().mag()/MeV;
93 if( pp > 0.0 )
94 {
95 G4ThreeVector momentum = modifiedOriginal.GetMomentum();
96 modifiedOriginal.SetMomentum( momentum * (p/pp) );
97 }
98 G4ReactionProduct currentParticle = modifiedOriginal;
99 G4ReactionProduct targetParticle;
100 targetParticle = *originalTarget;
101 currentParticle.SetSide( 1 ); // incident always goes in forward hemisphere
102 targetParticle.SetSide( -1 ); // target always goes in backward hemisphere
103 G4bool incidentHasChanged = false;
104 G4bool targetHasChanged = false;
105 G4bool quasiElastic = false;
106 G4FastVector<G4ReactionProduct,GHADLISTSIZE> vec; // vec will contain the secondary particles
107 G4int vecLen = 0;
108 vec.Initialize( 0 );
109
110 const G4double cutOff = 0.1;
111 const G4double anni = std::min( 1.3*currentParticle.GetTotalMomentum()/GeV, 0.4 );
112 if( (currentParticle.GetKineticEnergy()/MeV > cutOff) || (G4UniformRand() > anni) )
113 Cascade( vec, vecLen,
114 originalIncident, currentParticle, targetParticle,
115 incidentHasChanged, targetHasChanged, quasiElastic );
116
117 CalculateMomenta( vec, vecLen,
118 originalIncident, originalTarget, modifiedOriginal,
119 targetNucleus, currentParticle, targetParticle,
120 incidentHasChanged, targetHasChanged, quasiElastic );
121
122 SetUpChange( vec, vecLen,
123 currentParticle, targetParticle,
124 incidentHasChanged );
125
126 delete originalTarget;
127 return &theParticleChange;
128}
129
130
131void G4RPGAntiXiMinusInelastic::Cascade(
133 G4int& vecLen,
134 const G4HadProjectile *originalIncident,
135 G4ReactionProduct &currentParticle,
136 G4ReactionProduct &targetParticle,
137 G4bool &incidentHasChanged,
138 G4bool &targetHasChanged,
139 G4bool &quasiElastic )
140{
141 // Derived from H. Fesefeldt's original FORTRAN code CASAXM
142 // which is just a copy of casxm (cascade for Xi-).
143 // AntiXiMinus undergoes interaction with nucleon within a nucleus. Check if it is
144 // energetically possible to produce pions/kaons. In not, assume nuclear excitation
145 // occurs and input particle is degraded in energy. No other particles are produced.
146 // If reaction is possible, find the correct number of pions/protons/neutrons
147 // produced using an interpolation to multiplicity data. Replace some pions or
148 // protons/neutrons by kaons or strange baryons according to the average
149 // multiplicity per Inelastic reaction.
150
151 const G4double mOriginal = originalIncident->GetDefinition()->GetPDGMass()/MeV;
152 const G4double etOriginal = originalIncident->GetTotalEnergy()/MeV;
153 const G4double targetMass = targetParticle.GetMass()/MeV;
154 G4double centerofmassEnergy = std::sqrt( mOriginal*mOriginal +
155 targetMass*targetMass +
156 2.0*targetMass*etOriginal );
157 G4double availableEnergy = centerofmassEnergy-(targetMass+mOriginal);
158 if (availableEnergy <= G4PionPlus::PionPlus()->GetPDGMass()/MeV) {
159 quasiElastic = true;
160 return;
161 }
162 static G4bool first = true;
163 const G4int numMul = 1200;
164 const G4int numSec = 60;
165 static G4double protmul[numMul], protnorm[numSec]; // proton constants
166 static G4double neutmul[numMul], neutnorm[numSec]; // neutron constants
167
168 // np = number of pi+, nneg = number of pi-, nz = number of pi0
169 G4int counter, nt=0, np=0, nneg=0, nz=0;
170 G4double test;
171 const G4double c = 1.25;
172 const G4double b[] = { 0.7, 0.7 };
173 if (first) { // Computation of normalization constants will only be done once
174 first = false;
175 G4int i;
176 for( i=0; i<numMul; ++i )protmul[i] = 0.0;
177 for( i=0; i<numSec; ++i )protnorm[i] = 0.0;
178 counter = -1;
179 for( np=0; np<(numSec/3); ++np )
180 {
181 for( nneg=std::max(0,np-1); nneg<=(np+1); ++nneg )
182 {
183 for( nz=0; nz<numSec/3; ++nz )
184 {
185 if( ++counter < numMul )
186 {
187 nt = np+nneg+nz;
188 if( nt>0 && nt<=numSec )
189 {
190 protmul[counter] = Pmltpc(np,nneg,nz,nt,b[0],c);
191 protnorm[nt-1] += protmul[counter];
192 }
193 }
194 }
195 }
196 }
197 for( i=0; i<numMul; ++i )neutmul[i] = 0.0;
198 for( i=0; i<numSec; ++i )neutnorm[i] = 0.0;
199 counter = -1;
200 for( np=0; np<numSec/3; ++np )
201 {
202 for( nneg=np; nneg<=(np+2); ++nneg )
203 {
204 for( nz=0; nz<numSec/3; ++nz )
205 {
206 if( ++counter < numMul )
207 {
208 nt = np+nneg+nz;
209 if( nt>0 && nt<=numSec )
210 {
211 neutmul[counter] = Pmltpc(np,nneg,nz,nt,b[1],c);
212 neutnorm[nt-1] += neutmul[counter];
213 }
214 }
215 }
216 }
217 }
218 for( i=0; i<numSec; ++i )
219 {
220 if( protnorm[i] > 0.0 )protnorm[i] = 1.0/protnorm[i];
221 if( neutnorm[i] > 0.0 )neutnorm[i] = 1.0/neutnorm[i];
222 }
223 } // end of initialization
224
225 const G4double expxu = 82.; // upper bound for arg. of exp
226 const G4double expxl = -expxu; // lower bound for arg. of exp
232 //
233 // energetically possible to produce pion(s) --> inelastic scattering
234 //
235 G4double n, anpn;
236 GetNormalizationConstant( availableEnergy, n, anpn );
237 G4double ran = G4UniformRand();
238 G4double dum, excs = 0.0;
239 if( targetParticle.GetDefinition() == aProton )
240 {
241 counter = -1;
242 for( np=0; np<numSec/3 && ran>=excs; ++np )
243 {
244 for( nneg=std::max(0,np-1); nneg<=(np+1) && ran>=excs; ++nneg )
245 {
246 for( nz=0; nz<numSec/3 && ran>=excs; ++nz )
247 {
248 if( ++counter < numMul )
249 {
250 nt = np+nneg+nz;
251 if( nt>0 && nt<=numSec )
252 {
253 test = std::exp( std::min( expxu, std::max( expxl, -(pi/4.0)*(nt*nt)/(n*n) ) ) );
254 dum = (pi/anpn)*nt*protmul[counter]*protnorm[nt-1]/(2.0*n*n);
255 if( std::fabs(dum) < 1.0 )
256 {
257 if( test >= 1.0e-10 )excs += dum*test;
258 }
259 else
260 excs += dum*test;
261 }
262 }
263 }
264 }
265 }
266 if( ran >= excs ) // 3 previous loops continued to the end
267 {
268 quasiElastic = true;
269 return;
270 }
271 np--; nneg--; nz--;
272 //
273 // number of secondary mesons determined by kno distribution
274 // check for total charge of final state mesons to determine
275 // the kind of baryons to be produced, taking into account
276 // charge and strangeness conservation
277 //
278 if( np < nneg )
279 {
280 if( np+1 == nneg )
281 {
282 currentParticle.SetDefinitionAndUpdateE( aXiZero );
283 incidentHasChanged = true;
284 }
285 else // charge mismatch
286 {
287 currentParticle.SetDefinitionAndUpdateE( aSigmaPlus );
288 incidentHasChanged = true;
289 //
290 // correct the strangeness by replacing a pi- by a kaon-
291 //
292 vec.Initialize( 1 );
294 p->SetDefinition( aKaonMinus );
295 (G4UniformRand() < 0.5) ? p->SetSide( -1 ) : p->SetSide( 1 );
296 vec.SetElement( vecLen++, p );
297 --nneg;
298 }
299 }
300 else if( np == nneg )
301 {
302 if( G4UniformRand() >= 0.5 )
303 {
304 currentParticle.SetDefinitionAndUpdateE( aXiZero );
305 incidentHasChanged = true;
306 targetParticle.SetDefinitionAndUpdateE( aNeutron );
307 targetHasChanged = true;
308 }
309 }
310 else
311 {
312 targetParticle.SetDefinitionAndUpdateE( aNeutron );
313 targetHasChanged = true;
314 }
315 }
316 else // target must be a neutron
317 {
318 counter = -1;
319 for( np=0; np<numSec/3 && ran>=excs; ++np )
320 {
321 for( nneg=np; nneg<=(np+2) && ran>=excs; ++nneg )
322 {
323 for( nz=0; nz<numSec/3 && ran>=excs; ++nz )
324 {
325 if( ++counter < numMul )
326 {
327 nt = np+nneg+nz;
328 if( nt>0 && nt<=numSec )
329 {
330 test = std::exp( std::min( expxu, std::max( expxl, -(pi/4.0)*(nt*nt)/(n*n) ) ) );
331 dum = (pi/anpn)*nt*neutmul[counter]*neutnorm[nt-1]/(2.0*n*n);
332 if( std::fabs(dum) < 1.0 )
333 {
334 if( test >= 1.0e-10 )excs += dum*test;
335 }
336 else
337 excs += dum*test;
338 }
339 }
340 }
341 }
342 }
343 if( ran >= excs ) // 3 previous loops continued to the end
344 {
345 quasiElastic = true;
346 return;
347 }
348 np--; nneg--; nz--;
349 if( np+1 < nneg )
350 {
351 if( np+2 == nneg )
352 {
353 currentParticle.SetDefinitionAndUpdateE( aXiZero );
354 incidentHasChanged = true;
355 targetParticle.SetDefinitionAndUpdateE( aProton );
356 targetHasChanged = true;
357 }
358 else // charge mismatch
359 {
360 currentParticle.SetDefinitionAndUpdateE( aSigmaPlus );
361 incidentHasChanged = true;
362 targetParticle.SetDefinitionAndUpdateE( aProton );
363 targetHasChanged = true;
364 //
365 // correct the strangeness by replacing a pi- by a kaon-
366 //
367 vec.Initialize( 1 );
369 p->SetDefinition( aKaonMinus );
370 (G4UniformRand() < 0.5) ? p->SetSide( -1 ) : p->SetSide( 1 );
371 vec.SetElement( vecLen++, p );
372 --nneg;
373 }
374 }
375 else if( np+1 == nneg )
376 {
377 if( G4UniformRand() < 0.5 )
378 {
379 currentParticle.SetDefinitionAndUpdateE( aXiZero );
380 incidentHasChanged = true;
381 }
382 else
383 {
384 targetParticle.SetDefinitionAndUpdateE( aProton );
385 targetHasChanged = true;
386 }
387 }
388 }
389
390 SetUpPions(np, nneg, nz, vec, vecLen);
391 return;
392}
393
394 /* end of file */
395
@ isAlive
double G4double
Definition: G4Types.hh:64
int G4int
Definition: G4Types.hh:66
bool G4bool
Definition: G4Types.hh:67
#define G4endl
Definition: G4ios.hh:52
G4DLLIMPORT std::ostream G4cout
#define G4UniformRand()
Definition: Randomize.hh:53
Hep3Vector unit() const
double mag() const
Hep3Vector vect() const
G4ParticleDefinition * GetDefinition() const
void SetElement(G4int anIndex, Type *anElement)
Definition: G4FastVector.hh:76
void Initialize(G4int items)
Definition: G4FastVector.hh:63
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 G4KaonMinus * KaonMinus()
Definition: G4KaonMinus.cc:113
const G4String & GetName() const
Definition: G4Material.hh:177
static G4Neutron * Neutron()
Definition: G4Neutron.cc:104
G4double EvaporationEffects(G4double kineticEnergy)
Definition: G4Nucleus.cc:264
G4double Cinema(G4double kineticEnergy)
Definition: G4Nucleus.cc:368
G4DynamicParticle * ReturnTargetParticle() const
Definition: G4Nucleus.cc:227
const G4String & GetParticleName() const
static G4PionPlus * PionPlus()
Definition: G4PionPlus.cc:98
static G4Proton * Proton()
Definition: G4Proton.cc:93
G4HadFinalState * ApplyYourself(const G4HadProjectile &aTrack, G4Nucleus &targetNucleus)
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)
void SetMomentum(const G4double x, const G4double y, const G4double z)
G4double GetTotalMomentum() const
G4double GetKineticEnergy() const
G4ThreeVector GetMomentum() const
void SetSide(const G4int sid)
void SetDefinitionAndUpdateE(G4ParticleDefinition *aParticleDefinition)
void SetKineticEnergy(const G4double en)
G4ParticleDefinition * GetDefinition() const
void SetDefinition(G4ParticleDefinition *aParticleDefinition)
G4double GetMass() const
static G4SigmaPlus * SigmaPlus()
Definition: G4SigmaPlus.cc:108
static G4XiZero * XiZero()
Definition: G4XiZero.cc:106
const G4double pi