StRoot  1
 All Classes Namespaces Files Functions Variables Typedefs Enumerations Enumerator Friends Groups Pages
MiniStringFragmentation.cc
1 // MiniStringFragmentation.cc is a part of the PYTHIA event generator.
2 // Copyright (C) 2012 Torbjorn Sjostrand.
3 // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details.
4 // Please respect the MCnet Guidelines, see GUIDELINES for details.
5 
6 // Function definitions (not found in the header) for the .
7 // MiniStringFragmentation class
8 
9 #include "MiniStringFragmentation.h"
10 
11 namespace Pythia8 {
12 
13 //==========================================================================
14 
15 // The MiniStringFragmentation class.
16 
17 //--------------------------------------------------------------------------
18 
19 // Constants: could be changed here if desired, but normally should not.
20 // These are of technical nature, as described for each.
21 
22 // Since diffractive by definition is > 1 particle, try hard.
23 const int MiniStringFragmentation::NTRYDIFFRACTIVE = 200;
24 
25 // After one-body fragmentation failed, try two-body once more.
26 const int MiniStringFragmentation::NTRYLASTRESORT = 100;
27 
28 // Loop try to combine available endquarks to valid hadron.
29 const int MiniStringFragmentation::NTRYFLAV = 10;
30 
31 //--------------------------------------------------------------------------
32 
33 // Initialize and save pointers.
34 
35 void MiniStringFragmentation::init(Info* infoPtrIn, Settings& settings,
36  ParticleData* particleDataPtrIn, Rndm* rndmPtrIn,
37  StringFlav* flavSelPtrIn, StringPT* pTSelPtrIn, StringZ* zSelPtrIn) {
38 
39  // Save pointers.
40  infoPtr = infoPtrIn;
41  particleDataPtr = particleDataPtrIn;
42  rndmPtr = rndmPtrIn;
43  flavSelPtr = flavSelPtrIn;
44  pTSelPtr = pTSelPtrIn;
45  zSelPtr = zSelPtrIn;
46 
47  // Initialize the MiniStringFragmentation class proper.
48  nTryMass = settings.mode("MiniStringFragmentation:nTry");
49 
50  // Initialize the b parameter of the z spectrum, used when joining jets.
51  bLund = zSelPtr->bAreaLund();
52 
53 }
54 
55 //--------------------------------------------------------------------------
56 
57 // Do the fragmentation: driver routine.
58 
59 bool MiniStringFragmentation::fragment(int iSub, ColConfig& colConfig,
60  Event& event, bool isDiff) {
61 
62  // Read in info on system to be treated.
63  iParton = colConfig[iSub].iParton;
64  flav1 = FlavContainer( event[ iParton.front() ].id() );
65  flav2 = FlavContainer( event[ iParton.back() ].id() );
66  pSum = colConfig[iSub].pSum;
67  mSum = colConfig[iSub].mass;
68  m2Sum = mSum*mSum;
69  isClosed = colConfig[iSub].isClosed;
70 
71  // Do not want diffractive systems to easily collapse to one particle.
72  int nTryFirst = (isDiff) ? NTRYDIFFRACTIVE : nTryMass;
73 
74  // First try to produce two particles from the system.
75  if (ministring2two( nTryFirst, event)) return true;
76 
77  // If this fails, then form one hadron and shuffle momentum.
78  if (ministring2one( iSub, colConfig, event)) return true;
79 
80  // If also this fails, then try harder to produce two particles.
81  if (ministring2two( NTRYLASTRESORT, event)) return true;
82 
83  // Else complete failure.
84  infoPtr->errorMsg("Error in MiniStringFragmentation::fragment: "
85  "no 1- or 2-body state found above mass threshold");
86  return false;
87 
88 }
89 
90 //--------------------------------------------------------------------------
91 
92  // Attempt to produce two particles from the ministring.
93 
94 bool MiniStringFragmentation::ministring2two( int nTry, Event& event) {
95 
96  // Properties of the produced hadrons.
97  int idHad1 = 0;
98  int idHad2 = 0;
99  double mHad1 = 0.;
100  double mHad2 = 0.;
101  double mHadSum = 0.;
102 
103  // Allow a few attempts to find a particle pair with low enough masses.
104  for (int iTry = 0; iTry < nTry; ++iTry) {
105 
106  // For closed gluon loop need to pick an initial flavour.
107  if (isClosed) do {
108  int idStart = flavSelPtr->pickLightQ();
109  FlavContainer flavStart(idStart, 1);
110  flavStart = flavSelPtr->pick( flavStart);
111  flav1 = flavSelPtr->pick( flavStart);
112  flav2.anti(flav1);
113  } while (flav1.id == 0 || flav1.nPop > 0);
114 
115  // Create a new q qbar flavour to form two hadrons.
116  // Start from a diquark, if any.
117  do {
118  FlavContainer flav3 =
119  (flav1.isDiquark() || (!flav2.isDiquark() && rndmPtr->flat() < 0.5) )
120  ? flavSelPtr->pick( flav1) : flavSelPtr->pick( flav2).anti();
121  idHad1 = flavSelPtr->combine( flav1, flav3);
122  idHad2 = flavSelPtr->combine( flav2, flav3.anti());
123  } while (idHad1 == 0 || idHad2 == 0);
124 
125  // Check whether the mass sum fits inside the available phase space.
126  mHad1 = particleDataPtr->mass(idHad1);
127  mHad2 = particleDataPtr->mass(idHad2);
128  mHadSum = mHad1 + mHad2;
129  if (mHadSum < mSum) break;
130  }
131  if (mHadSum >= mSum) return false;
132 
133  // Define an effective two-parton string, by splitting intermediate
134  // gluon momenta in proportion to their closeness to either endpoint.
135  Vec4 pSum1 = event[ iParton.front() ].p();
136  Vec4 pSum2 = event[ iParton.back() ].p();
137  if (iParton.size() > 2) {
138  Vec4 pEnd1 = pSum1;
139  Vec4 pEnd2 = pSum2;
140  Vec4 pEndSum = pEnd1 + pEnd2;
141  for (int i = 1; i < int(iParton.size()) - 1 ; ++i) {
142  Vec4 pNow = event[ iParton[i] ].p();
143  double ratio = (pEnd2 * pNow) / (pEndSum * pNow);
144  pSum1 += ratio * pNow;
145  pSum2 += (1. - ratio) * pNow;
146  }
147  }
148 
149  // Set up a string region based on the two effective endpoints.
150  StringRegion region;
151  region.setUp( pSum1, pSum2);
152 
153  // Generate an isotropic decay in the ministring rest frame,
154  // suppressed at large pT by a fragmentation pT Gaussian.
155  double pAbs2 = 0.25 * ( pow2(m2Sum - mHad1*mHad1 - mHad2*mHad2)
156  - pow2(2. * mHad1 * mHad2) ) / m2Sum;
157  double pT2 = 0.;
158  do {
159  double cosTheta = rndmPtr->flat();
160  pT2 = (1. - pow2(cosTheta)) * pAbs2;
161  } while (pTSelPtr->suppressPT2(pT2) < rndmPtr->flat() );
162 
163  // Construct the forward-backward asymmetry of the two particles.
164  double mT21 = mHad1*mHad1 + pT2;
165  double mT22 = mHad2*mHad2 + pT2;
166  double lambda = sqrtpos( pow2(m2Sum - mT21 - mT22) - 4. * mT21 * mT22 );
167  double probReverse = 1. / (1. + exp( min( 50., bLund * lambda) ) );
168 
169  // Construct kinematics, as viewed in the transverse rest frame.
170  double xpz1 = 0.5 * lambda/ m2Sum;
171  if (probReverse > rndmPtr->flat()) xpz1 = -xpz1;
172  double xmDiff = (mT21 - mT22) / m2Sum;
173  double xe1 = 0.5 * (1. + xmDiff);
174  double xe2 = 0.5 * (1. - xmDiff );
175 
176  // Distribute pT isotropically in angle.
177  double phi = 2. * M_PI * rndmPtr->flat();
178  double pT = sqrt(pT2);
179  double px = pT * cos(phi);
180  double py = pT * sin(phi);
181 
182  // Translate this into kinematics in the string frame.
183  Vec4 pHad1 = region.pHad( xe1 + xpz1, xe1 - xpz1, px, py);
184  Vec4 pHad2 = region.pHad( xe2 - xpz1, xe2 + xpz1, -px, -py);
185 
186  // Add produced particles to the event record.
187  int iFirst = event.append( idHad1, 82, iParton.front(), iParton.back(),
188  0, 0, 0, 0, pHad1, mHad1);
189  int iLast = event.append( idHad2, 82, iParton.front(), iParton.back(),
190  0, 0, 0, 0, pHad2, mHad2);
191 
192  // Set decay vertex when this is displaced.
193  if (event[iParton.front()].hasVertex()) {
194  Vec4 vDec = event[iParton.front()].vDec();
195  event[iFirst].vProd( vDec );
196  event[iLast].vProd( vDec );
197  }
198 
199  // Set lifetime of hadrons.
200  event[iFirst].tau( event[iFirst].tau0() * rndmPtr->exp() );
201  event[iLast].tau( event[iLast].tau0() * rndmPtr->exp() );
202 
203  // Mark original partons as hadronized and set their daughter range.
204  for (int i = 0; i < int(iParton.size()); ++i) {
205  event[ iParton[i] ].statusNeg();
206  event[ iParton[i] ].daughters(iFirst, iLast);
207  }
208 
209  // Successfully done.
210  return true;
211 
212 }
213 
214 //--------------------------------------------------------------------------
215 
216 // Attempt to produce one particle from a ministring.
217 // Current algorithm: find the system with largest invariant mass
218 // relative to the existing one, and boost that system appropriately.
219 // Try more sophisticated alternatives later?? (Z0 mass shifted??)
220 // Also, if problems, attempt several times to obtain closer mass match??
221 
222 bool MiniStringFragmentation::ministring2one( int iSub,
223  ColConfig& colConfig, Event& event) {
224 
225  // Cannot handle qq + qbarqbar system.
226  if (abs(flav1.id) > 100 && abs(flav2.id) > 100) return false;
227 
228  // For closed gluon loop need to pick an initial flavour.
229  if (isClosed) do {
230  int idStart = flavSelPtr->pickLightQ();
231  FlavContainer flavStart(idStart, 1);
232  flav1 = flavSelPtr->pick( flavStart);
233  flav2 = flav1.anti();
234  } while (abs(flav1.id) > 100);
235 
236  // Select hadron flavour from available quark flavours.
237  int idHad = 0;
238  for (int iTryFlav = 0; iTryFlav < NTRYFLAV; ++iTryFlav) {
239  idHad = flavSelPtr->combine( flav1, flav2);
240  if (idHad != 0) break;
241  }
242  if (idHad == 0) return false;
243 
244  // Find mass.
245  double mHad = particleDataPtr->mass(idHad);
246 
247  // Find the untreated parton system which combines to the largest
248  // squared mass above mimimum required.
249  int iMax = -1;
250  double deltaM2 = mHad*mHad - mSum*mSum;
251  double delta2Max = 0.;
252  for (int iRec = iSub + 1; iRec < colConfig.size(); ++iRec) {
253  double delta2Rec = 2. * (pSum * colConfig[iRec].pSum) - deltaM2
254  - 2. * mHad * colConfig[iRec].mass;
255  if (delta2Rec > delta2Max) { iMax = iRec; delta2Max = delta2Rec;}
256  }
257  if (iMax == -1) return false;
258 
259  // Construct kinematics of the hadron and recoiling system.
260  Vec4& pRec = colConfig[iMax].pSum;
261  double mRec = colConfig[iMax].mass;
262  double vecProd = pSum * pRec;
263  double coefOld = mSum*mSum + vecProd;
264  double coefNew = mHad*mHad + vecProd;
265  double coefRec = mRec*mRec + vecProd;
266  double coefSum = coefOld + coefNew;
267  double sHat = coefOld + coefRec;
268  double root = sqrtpos( (pow2(coefSum) - 4. * sHat * mHad*mHad)
269  / (pow2(vecProd) - pow2(mSum * mRec)) );
270  double k2 = 0.5 * (coefOld * root - coefSum) / sHat;
271  double k1 = (coefRec * k2 + 0.5 * deltaM2) / coefOld;
272  Vec4 pHad = (1. + k1) * pSum - k2 * pRec;
273  Vec4 pRecNew = (1. + k2) * pRec - k1 * pSum;
274 
275  // Add the produced particle to the event record.
276  int iHad = event.append( idHad, 81, iParton.front(), iParton.back(),
277  0, 0, 0, 0, pHad, mHad);
278 
279  // Set decay vertex when this is displaced.
280  if (event[iParton.front()].hasVertex()) {
281  Vec4 vDec = event[iParton.front()].vDec();
282  event[iHad].vProd( vDec );
283  }
284 
285  // Set lifetime of hadron.
286  event[iHad].tau( event[iHad].tau0() * rndmPtr->exp() );
287 
288  // Mark original partons as hadronized and set their daughter range.
289  for (int i = 0; i < int(iParton.size()); ++i) {
290  event[ iParton[i] ].statusNeg();
291  event[ iParton[i] ].daughters(iHad, iHad);
292  }
293 
294  // Copy down recoiling system, with boosted momentum. Update current partons.
295  RotBstMatrix M;
296  M.bst(pRec, pRecNew);
297  for (int i = 0; i < colConfig[iMax].size(); ++i) {
298  int iOld = colConfig[iMax].iParton[i];
299  // Do not touch negative iOld = beginning of new junction leg.
300  if (iOld >= 0) {
301  int iNew = event.copy(iOld, 72);
302  event[iNew].rotbst(M);
303  colConfig[iMax].iParton[i] = iNew;
304  }
305  }
306  colConfig[iMax].pSum = pRecNew;
307  colConfig[iMax].isCollected = true;
308 
309  // Successfully done.
310  return true;
311 
312 }
313 
314 //==========================================================================
315 
316 } // end namespace Pythia8
Definition: AgUStep.h:26