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G4RPGAntiXiMinusInelastic.cc
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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 
34 #include "G4PhysicalConstants.hh"
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 
131 void 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 G4ThreadLocal G4bool first = true;
163  const G4int numMul = 1200;
164  const G4int numSec = 60;
165  static G4ThreadLocal G4double protmul[numMul], protnorm[numSec]; // proton constants
166  static G4ThreadLocal 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 
void SetElement(G4int anIndex, Type *anElement)
Definition: G4FastVector.hh:76
G4double EvaporationEffects(G4double kineticEnergy)
Definition: G4Nucleus.cc:264
G4double GetTotalMomentum() const
void SetUpChange(G4FastVector< G4ReactionProduct, 256 > &vec, G4int &vecLen, G4ReactionProduct &currentParticle, G4ReactionProduct &targetParticle, G4bool &incidentHasChanged)
void SetKineticEnergy(const G4double en)
void SetMomentum(const G4double x, const G4double y, const G4double z)
const char * p
Definition: xmltok.h:285
const G4String & GetName() const
Definition: G4Material.hh:176
void SetSide(const G4int sid)
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)
G4ParticleDefinition * GetDefinition() const
#define G4ThreadLocal
Definition: tls.hh:52
void Initialize(G4int items)
Definition: G4FastVector.hh:63
int G4int
Definition: G4Types.hh:78
G4DynamicParticle * ReturnTargetParticle() const
Definition: G4Nucleus.cc:227
void SetDefinitionAndUpdateE(G4ParticleDefinition *aParticleDefinition)
const G4String & GetParticleName() const
static G4KaonMinus * KaonMinus()
Definition: G4KaonMinus.cc:113
G4ParticleDefinition * GetDefinition() const
void SetStatusChange(G4HadFinalStateStatus aS)
G4double Pmltpc(G4int np, G4int nm, G4int nz, G4int n, G4double b, G4double c)
static G4XiZero * XiZero()
Definition: G4XiZero.cc:106
Hep3Vector vect() const
#define G4UniformRand()
Definition: Randomize.hh:87
G4GLOB_DLL std::ostream G4cout
const G4ParticleDefinition * GetDefinition() const
bool G4bool
Definition: G4Types.hh:79
G4double GetKineticEnergy() const
static G4Proton * Proton()
Definition: G4Proton.cc:93
static G4PionPlus * PionPlus()
Definition: G4PionPlus.cc:98
static G4Neutron * Neutron()
Definition: G4Neutron.cc:104
const G4int n
const G4LorentzVector & Get4Momentum() const
G4double GetKineticEnergy() const
void SetEnergyChange(G4double anEnergy)
G4HadFinalState * ApplyYourself(const G4HadProjectile &aTrack, G4Nucleus &targetNucleus)
G4double GetPDGMass() const
T max(const T t1, const T t2)
brief Return the largest of the two arguments
Hep3Vector unit() const
G4double Cinema(G4double kineticEnergy)
Definition: G4Nucleus.cc:368
T min(const T t1, const T t2)
brief Return the smallest of the two arguments
void SetDefinition(G4ParticleDefinition *aParticleDefinition)
G4ThreeVector GetMomentum() const
#define G4endl
Definition: G4ios.hh:61
const G4Material * GetMaterial() const
def test
Definition: mcscore.py:117
static G4SigmaPlus * SigmaPlus()
Definition: G4SigmaPlus.cc:108
void GetNormalizationConstant(const G4double availableEnergy, G4double &n, G4double &anpn)
double G4double
Definition: G4Types.hh:76
void SetUpPions(const G4int np, const G4int nm, const G4int nz, G4FastVector< G4ReactionProduct, 256 > &vec, G4int &vecLen)
double mag() const
void SetMomentumChange(const G4ThreeVector &aV)
G4double GetMass() const
G4double GetTotalEnergy() const