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b2a297fa | 1 | /************************************************************************* |
2 | * Copyright(c) 1998-2009, ALICE Experiment at CERN, All rights reserved. * | |
3 | * * | |
4 | * Author: The ALICE Off-line Project. * | |
5 | * Contributors are mentioned in the code where appropriate. * | |
6 | * * | |
7 | * Permission to use, copy, modify and distribute this software and its * | |
8 | * documentation strictly for non-commercial purposes is hereby granted * | |
9 | * without fee, provided that the above copyright notice appears in all * | |
10 | * copies and that both the copyright notice and this permission notice * | |
11 | * appear in the supporting documentation. The authors make no claims * | |
12 | * about the suitability of this software for any purpose. It is * | |
13 | * provided "as is" without express or implied warranty. * | |
14 | **************************************************************************/ | |
15 | ||
16 | /////////////////////////////////////////////////////////////////////////// | |
17 | // // | |
18 | // Dielectron Pair class. Internally it makes use of AliKFParticle. // | |
19 | // // | |
20 | /////////////////////////////////////////////////////////////////////////// | |
21 | ||
22 | ||
ba15fdfb | 23 | #include <TDatabasePDG.h> |
24 | #include <AliVTrack.h> | |
25 | #include <AliVVertex.h> | |
26 | #include <AliPID.h> | |
236e1bda | 27 | #include <AliExternalTrackParam.h> |
ba15fdfb | 28 | |
b2a297fa | 29 | #include "AliDielectronPair.h" |
b2a297fa | 30 | |
31 | ClassImp(AliDielectronPair) | |
32 | ||
33 | AliDielectronPair::AliDielectronPair() : | |
b2a297fa | 34 | fType(-1), |
a655b716 | 35 | fLabel(-1), |
e4339752 | 36 | fPdgCode(0), |
b2a297fa | 37 | fPair(), |
572b0139 | 38 | fD1(), |
39 | fD2(), | |
b2a297fa | 40 | fRefD1(), |
41 | fRefD2() | |
42 | { | |
43 | // | |
44 | // Default Constructor | |
45 | // | |
46 | ||
47 | } | |
48 | ||
49 | //______________________________________________ | |
50 | AliDielectronPair::AliDielectronPair(AliVTrack * const particle1, Int_t pid1, | |
51 | AliVTrack * const particle2, Int_t pid2, Char_t type) : | |
b2a297fa | 52 | fType(type), |
a655b716 | 53 | fLabel(-1), |
e4339752 | 54 | fPdgCode(0), |
b2a297fa | 55 | fPair(), |
572b0139 | 56 | fD1(), |
57 | fD2(), | |
b2a297fa | 58 | fRefD1(), |
59 | fRefD2() | |
60 | { | |
61 | // | |
62 | // Constructor with tracks | |
63 | // | |
64 | SetTracks(particle1, pid1, particle2, pid2); | |
65 | } | |
66 | ||
1201a1a9 | 67 | //______________________________________________ |
68 | AliDielectronPair::AliDielectronPair(const AliKFParticle * const particle1, | |
69 | const AliKFParticle * const particle2, | |
70 | AliVTrack * const refParticle1, | |
71 | AliVTrack * const refParticle2, Char_t type) : | |
72 | fType(type), | |
73 | fLabel(-1), | |
e4339752 | 74 | fPdgCode(0), |
1201a1a9 | 75 | fPair(), |
76 | fD1(), | |
77 | fD2(), | |
78 | fRefD1(), | |
79 | fRefD2() | |
80 | { | |
81 | // | |
82 | // Constructor with tracks | |
83 | // | |
84 | SetTracks(particle1, particle2,refParticle1,refParticle2); | |
85 | } | |
86 | ||
b2a297fa | 87 | //______________________________________________ |
88 | AliDielectronPair::~AliDielectronPair() | |
89 | { | |
90 | // | |
91 | // Default Destructor | |
92 | // | |
93 | ||
94 | } | |
95 | ||
96 | //______________________________________________ | |
97 | void AliDielectronPair::SetTracks(AliVTrack * const particle1, Int_t pid1, | |
98 | AliVTrack * const particle2, Int_t pid2) | |
99 | { | |
100 | // | |
572b0139 | 101 | // Sort particles by pt, first particle larget Pt |
102 | // set AliKF daughters and pair | |
1201a1a9 | 103 | // refParticle1 and 2 are the original tracks. In the case of track rotation |
104 | // they are needed in the framework | |
b2a297fa | 105 | // |
106 | fPair.Initialize(); | |
572b0139 | 107 | fD1.Initialize(); |
108 | fD2.Initialize(); | |
8df8e382 | 109 | |
b2a297fa | 110 | AliKFParticle kf1(*particle1,pid1); |
111 | AliKFParticle kf2(*particle2,pid2); | |
572b0139 | 112 | |
b2a297fa | 113 | fPair.AddDaughter(kf1); |
114 | fPair.AddDaughter(kf2); | |
8df8e382 | 115 | |
a655b716 | 116 | if (particle1->Pt()>particle2->Pt()){ |
117 | fRefD1 = particle1; | |
118 | fRefD2 = particle2; | |
572b0139 | 119 | fD1+=kf1; |
120 | fD2+=kf2; | |
a655b716 | 121 | } else { |
122 | fRefD1 = particle2; | |
123 | fRefD2 = particle1; | |
572b0139 | 124 | fD1+=kf2; |
125 | fD2+=kf1; | |
a655b716 | 126 | } |
b2a297fa | 127 | } |
128 | ||
1201a1a9 | 129 | //______________________________________________ |
130 | void AliDielectronPair::SetTracks(const AliKFParticle * const particle1, | |
131 | const AliKFParticle * const particle2, | |
132 | AliVTrack * const refParticle1, | |
133 | AliVTrack * const refParticle2) | |
134 | { | |
135 | // | |
136 | // Sort particles by pt, first particle larget Pt | |
137 | // set AliKF daughters and pair | |
138 | // refParticle1 and 2 are the original tracks. In the case of track rotation | |
139 | // they are needed in the framework | |
140 | // | |
141 | fPair.Initialize(); | |
142 | fD1.Initialize(); | |
143 | fD2.Initialize(); | |
144 | ||
145 | AliKFParticle kf1(*particle1); | |
146 | AliKFParticle kf2(*particle2); | |
147 | ||
148 | fPair.AddDaughter(kf1); | |
149 | fPair.AddDaughter(kf2); | |
150 | ||
151 | if (kf1.GetPt()>kf2.GetPt()){ | |
152 | fRefD1 = refParticle1; | |
153 | fRefD2 = refParticle2; | |
154 | fD1+=kf1; | |
155 | fD2+=kf2; | |
156 | } else { | |
157 | fRefD1 = refParticle2; | |
158 | fRefD2 = refParticle1; | |
159 | fD1+=kf2; | |
160 | fD2+=kf1; | |
161 | } | |
162 | } | |
163 | ||
61d106d3 | 164 | //______________________________________________ |
165 | void AliDielectronPair::GetThetaPhiCM(Double_t &thetaHE, Double_t &phiHE, Double_t &thetaCS, Double_t &phiCS) const | |
166 | { | |
167 | // | |
168 | // Calculate theta and phi in helicity and Collins-Soper coordinate frame | |
169 | // | |
170 | const Double_t kBeamEnergy = 3500.; | |
1201a1a9 | 171 | Double_t pxyz1[3]={fD1.GetPx(),fD1.GetPy(),fD1.GetPz()}; |
172 | Double_t pxyz2[3]={fD2.GetPx(),fD2.GetPy(),fD2.GetPz()}; | |
61d106d3 | 173 | Double_t eleMass=AliPID::ParticleMass(AliPID::kElectron); |
174 | Double_t proMass=AliPID::ParticleMass(AliPID::kProton); | |
175 | ||
1201a1a9 | 176 | // AliVParticle *d1 = static_cast<AliVParticle*>(fRefD1.GetObject()); |
177 | // AliVParticle *d2 = static_cast<AliVParticle*>(fRefD2.GetObject()); | |
61d106d3 | 178 | |
1201a1a9 | 179 | // d1->PxPyPz(pxyz1); |
180 | // d2->PxPyPz(pxyz2); | |
61d106d3 | 181 | |
182 | TLorentzVector projMom(0.,0.,-kBeamEnergy,TMath::Sqrt(kBeamEnergy*kBeamEnergy+proMass*proMass)); | |
183 | TLorentzVector targMom(0.,0., kBeamEnergy,TMath::Sqrt(kBeamEnergy*kBeamEnergy+proMass*proMass)); | |
184 | ||
185 | // first & second daughter 4-mom | |
186 | TLorentzVector p1Mom(pxyz1[0],pxyz1[1],pxyz1[2], | |
187 | TMath::Sqrt(pxyz1[0]*pxyz1[0]+pxyz1[1]*pxyz1[1]+pxyz1[2]*pxyz1[2]+eleMass*eleMass)); | |
188 | TLorentzVector p2Mom(pxyz2[0],pxyz2[1],pxyz2[2], | |
189 | TMath::Sqrt(pxyz2[0]*pxyz2[0]+pxyz2[1]*pxyz2[1]+pxyz2[2]*pxyz2[2]+eleMass*eleMass)); | |
190 | // J/Psi 4-momentum vector | |
191 | TLorentzVector motherMom=p1Mom+p2Mom; | |
192 | ||
193 | // boost all the 4-mom vectors to the mother rest frame | |
194 | TVector3 beta = (-1.0/motherMom.E())*motherMom.Vect(); | |
195 | p1Mom.Boost(beta); | |
196 | p2Mom.Boost(beta); | |
197 | projMom.Boost(beta); | |
198 | targMom.Boost(beta); | |
199 | ||
200 | // x,y,z axes | |
201 | TVector3 zAxisHE = (motherMom.Vect()).Unit(); | |
202 | TVector3 zAxisCS = ((projMom.Vect()).Unit()-(targMom.Vect()).Unit()).Unit(); | |
203 | TVector3 yAxis = ((projMom.Vect()).Cross(targMom.Vect())).Unit(); | |
204 | TVector3 xAxisHE = (yAxis.Cross(zAxisHE)).Unit(); | |
205 | TVector3 xAxisCS = (yAxis.Cross(zAxisCS)).Unit(); | |
206 | ||
207 | // fill theta and phi | |
1201a1a9 | 208 | if(fD1.GetQ()>0){ |
61d106d3 | 209 | thetaHE = zAxisHE.Dot((p1Mom.Vect()).Unit()); |
210 | thetaCS = zAxisCS.Dot((p1Mom.Vect()).Unit()); | |
211 | phiHE = TMath::ATan2((p1Mom.Vect()).Dot(yAxis), (p1Mom.Vect()).Dot(xAxisHE)); | |
212 | phiCS = TMath::ATan2((p1Mom.Vect()).Dot(yAxis), (p1Mom.Vect()).Dot(xAxisCS)); | |
213 | } else { | |
214 | thetaHE = zAxisHE.Dot((p2Mom.Vect()).Unit()); | |
215 | thetaCS = zAxisCS.Dot((p2Mom.Vect()).Unit()); | |
216 | phiHE = TMath::ATan2((p2Mom.Vect()).Dot(yAxis), (p2Mom.Vect()).Dot(xAxisHE)); | |
217 | phiCS = TMath::ATan2((p2Mom.Vect()).Dot(yAxis), (p2Mom.Vect()).Dot(xAxisCS)); | |
218 | } | |
219 | } | |
220 | ||
236e1bda | 221 | //______________________________________________ |
222 | Double_t AliDielectronPair::PsiPair(Double_t MagField) const | |
223 | { | |
224 | //Following idea to use opening of colinear pairs in magnetic field from e.g. PHENIX | |
225 | //to ID conversions. Adapted from AliTRDv0Info class | |
226 | Double_t x, y, z; | |
227 | x = fPair.GetX(); | |
228 | y = fPair.GetY(); | |
229 | z = fPair.GetZ(); | |
230 | ||
231 | Double_t m1[3] = {0,0,0}; | |
232 | Double_t m2[3] = {0,0,0}; | |
233 | ||
234 | m1[0] = fD1.GetPx(); | |
235 | m1[1] = fD1.GetPy(); | |
236 | m1[2] = fD1.GetPz(); | |
237 | ||
238 | m2[0] = fD2.GetPx(); | |
239 | m2[1] = fD2.GetPy(); | |
240 | m2[2] = fD2.GetPz(); | |
241 | ||
242 | Double_t deltat = 1.; | |
243 | deltat = TMath::ATan(m2[2]/(TMath::Sqrt(m2[0]*m2[0] + m2[1]*m2[1])+1.e-13))- | |
244 | TMath::ATan(m1[2]/(TMath::Sqrt(m1[0]*m1[0] + m1[1]*m1[1])+1.e-13));//difference of angles of the two daughter tracks with z-axis | |
245 | ||
246 | Double_t radiussum = TMath::Sqrt(x*x + y*y) + 50;//radius to which tracks shall be propagated | |
247 | ||
248 | Double_t mom1Prop[3]; | |
249 | Double_t mom2Prop[3]; | |
250 | ||
251 | AliExternalTrackParam *d1 = static_cast<AliExternalTrackParam*>(fRefD1.GetObject()); | |
252 | AliExternalTrackParam *d2 = static_cast<AliExternalTrackParam*>(fRefD2.GetObject()); | |
253 | ||
254 | AliExternalTrackParam nt(*d1), pt(*d2); | |
236e1bda | 255 | |
256 | Double_t fPsiPair = 4.; | |
257 | if(nt.PropagateTo(radiussum,MagField) == 0)//propagate tracks to the outside | |
258 | fPsiPair = -5.; | |
259 | if(pt.PropagateTo(radiussum,MagField) == 0) | |
260 | fPsiPair = -5.; | |
261 | pt.GetPxPyPz(mom1Prop);//Get momentum vectors of tracks after propagation | |
262 | nt.GetPxPyPz(mom2Prop); | |
263 | ||
264 | ||
265 | ||
266 | Double_t pEle = | |
267 | TMath::Sqrt(mom2Prop[0]*mom2Prop[0]+mom2Prop[1]*mom2Prop[1]+mom2Prop[2]*mom2Prop[2]);//absolute momentum val | |
268 | Double_t pPos = | |
269 | TMath::Sqrt(mom1Prop[0]*mom1Prop[0]+mom1Prop[1]*mom1Prop[1]+mom1Prop[2]*mom1Prop[2]);//absolute momentum val | |
270 | ||
271 | Double_t scalarproduct = | |
272 | mom1Prop[0]*mom2Prop[0]+mom1Prop[1]*mom2Prop[1]+mom1Prop[2]*mom2Prop[2];//scalar product of propagated posit | |
273 | ||
274 | Double_t chipair = TMath::ACos(scalarproduct/(pEle*pPos));//Angle between propagated daughter tracks | |
275 | ||
276 | fPsiPair = TMath::Abs(TMath::ASin(deltat/chipair)); | |
277 | ||
278 | return fPsiPair; | |
279 | ||
280 | } | |
281 | ||
8df8e382 | 282 | //______________________________________________ |
283 | Double_t AliDielectronPair::ThetaPhiCM(const AliVParticle* d1, const AliVParticle* d2, | |
61d106d3 | 284 | const Bool_t isHE, const Bool_t isTheta) |
285 | { | |
286 | // The function calculates theta and phi in the mother rest frame with | |
8df8e382 | 287 | // respect to the helicity coordinate system and Collins-Soper coordinate system |
288 | // TO DO: generalize for different decays (only J/Psi->e+e- now) | |
289 | ||
290 | // Laboratory frame 4-vectors: | |
291 | // projectile beam & target beam 4-mom | |
61d106d3 | 292 | // TODO: need to retrieve the beam energy from somewhere |
293 | const Double_t kBeamEnergy = 3500.; | |
294 | Double_t px1=d1->Px(); | |
295 | Double_t py1=d1->Py(); | |
296 | Double_t pz1=d1->Pz(); | |
297 | Double_t px2=d2->Px(); | |
298 | Double_t py2=d2->Py(); | |
299 | Double_t pz2=d2->Pz(); | |
300 | Double_t eleMass=AliPID::ParticleMass(AliPID::kElectron); | |
301 | Double_t proMass=AliPID::ParticleMass(AliPID::kProton); | |
302 | ||
303 | TLorentzVector projMom(0.,0.,-kBeamEnergy,TMath::Sqrt(kBeamEnergy*kBeamEnergy+proMass*proMass)); | |
304 | TLorentzVector targMom(0.,0., kBeamEnergy,TMath::Sqrt(kBeamEnergy*kBeamEnergy+proMass*proMass)); | |
8df8e382 | 305 | |
306 | // first & second daughter 4-mom | |
61d106d3 | 307 | TLorentzVector p1Mom(px1,py1,pz1,TMath::Sqrt(px1*px1+py1*py1+pz1*pz1+eleMass*eleMass)); |
308 | TLorentzVector p2Mom(px2,py2,pz2,TMath::Sqrt(px2*px2+py2*py2+pz2*pz2+eleMass*eleMass)); | |
8df8e382 | 309 | // J/Psi 4-momentum vector |
310 | TLorentzVector motherMom=p1Mom+p2Mom; | |
311 | ||
312 | // boost all the 4-mom vectors to the mother rest frame | |
313 | TVector3 beta = (-1.0/motherMom.E())*motherMom.Vect(); | |
314 | p1Mom.Boost(beta); | |
315 | p2Mom.Boost(beta); | |
316 | projMom.Boost(beta); | |
317 | targMom.Boost(beta); | |
318 | ||
319 | // x,y,z axes | |
320 | TVector3 zAxis; | |
321 | if(isHE) zAxis = (motherMom.Vect()).Unit(); | |
322 | else zAxis = ((projMom.Vect()).Unit()-(targMom.Vect()).Unit()).Unit(); | |
323 | TVector3 yAxis = ((projMom.Vect()).Cross(targMom.Vect())).Unit(); | |
324 | TVector3 xAxis = (yAxis.Cross(zAxis)).Unit(); | |
325 | ||
326 | // return either theta or phi | |
327 | if(isTheta) { | |
328 | if(d1->Charge()>0) | |
329 | return zAxis.Dot((p1Mom.Vect()).Unit()); | |
330 | else | |
331 | return zAxis.Dot((p2Mom.Vect()).Unit()); | |
332 | ||
333 | } | |
334 | else { | |
335 | if(d1->Charge()>0) | |
336 | return TMath::ATan2((p1Mom.Vect()).Dot(yAxis), (p1Mom.Vect()).Dot(xAxis)); | |
337 | else | |
338 | return TMath::ATan2((p2Mom.Vect()).Dot(yAxis), (p2Mom.Vect()).Dot(xAxis)); | |
339 | } | |
340 | } | |
341 | ||
342 | //______________________________________________ | |
343 | Double_t AliDielectronPair::ThetaPhiCM(const Bool_t isHE, const Bool_t isTheta) const { | |
344 | // The function calculates theta and phi in the mother rest frame with | |
345 | // respect to the helicity coordinate system and Collins-Soper coordinate system | |
346 | // TO DO: generalize for different decays (only J/Psi->e+e- now) | |
347 | ||
348 | // Laboratory frame 4-vectors: | |
349 | // projectile beam & target beam 4-mom | |
45b2b1b8 | 350 | AliVParticle *d1 = static_cast<AliVParticle*>(fRefD1.GetObject()); |
351 | AliVParticle *d2 = static_cast<AliVParticle*>(fRefD2.GetObject()); | |
61d106d3 | 352 | |
353 | const Double_t kBeamEnergy = 3500.; | |
354 | Double_t px1=d1->Px(); | |
355 | Double_t py1=d1->Py(); | |
356 | Double_t pz1=d1->Pz(); | |
357 | Double_t px2=d2->Px(); | |
358 | Double_t py2=d2->Py(); | |
359 | Double_t pz2=d2->Pz(); | |
360 | Double_t eleMass=AliPID::ParticleMass(AliPID::kElectron); | |
361 | Double_t proMass=AliPID::ParticleMass(AliPID::kProton); | |
362 | ||
363 | TLorentzVector projMom(0.,0.,-kBeamEnergy,TMath::Sqrt(kBeamEnergy*kBeamEnergy+proMass*proMass)); | |
364 | TLorentzVector targMom(0.,0., kBeamEnergy,TMath::Sqrt(kBeamEnergy*kBeamEnergy+proMass*proMass)); | |
365 | ||
366 | // first & second daughter 4-mom | |
367 | // first & second daughter 4-mom | |
368 | TLorentzVector p1Mom(px1,py1,pz1,TMath::Sqrt(px1*px1+py1*py1+pz1*pz1+eleMass*eleMass)); | |
369 | TLorentzVector p2Mom(px2,py2,pz2,TMath::Sqrt(px2*px2+py2*py2+pz2*pz2+eleMass*eleMass)); | |
8df8e382 | 370 | // J/Psi 4-momentum vector |
371 | TLorentzVector motherMom=p1Mom+p2Mom; | |
372 | ||
373 | // boost all the 4-mom vectors to the mother rest frame | |
374 | TVector3 beta = (-1.0/motherMom.E())*motherMom.Vect(); | |
375 | p1Mom.Boost(beta); | |
376 | p2Mom.Boost(beta); | |
377 | projMom.Boost(beta); | |
378 | targMom.Boost(beta); | |
379 | ||
380 | // x,y,z axes | |
381 | TVector3 zAxis; | |
382 | if(isHE) zAxis = (motherMom.Vect()).Unit(); | |
383 | else zAxis = ((projMom.Vect()).Unit()-(targMom.Vect()).Unit()).Unit(); | |
384 | TVector3 yAxis = ((projMom.Vect()).Cross(targMom.Vect())).Unit(); | |
385 | TVector3 xAxis = (yAxis.Cross(zAxis)).Unit(); | |
386 | ||
387 | // return either theta or phi | |
388 | if(isTheta) { | |
389 | if(fD1.GetQ()>0) | |
390 | return zAxis.Dot((p1Mom.Vect()).Unit()); | |
391 | else | |
392 | return zAxis.Dot((p2Mom.Vect()).Unit()); | |
393 | } | |
394 | else { | |
395 | if(fD1.GetQ()>0) | |
396 | return TMath::ATan2((p1Mom.Vect()).Dot(yAxis), (p1Mom.Vect()).Dot(xAxis)); | |
397 | else | |
398 | return TMath::ATan2((p2Mom.Vect()).Dot(yAxis), (p2Mom.Vect()).Dot(xAxis)); | |
399 | } | |
400 | } | |
ba15fdfb | 401 | |
5720c765 | 402 | // //______________________________________________ |
403 | // Double_t AliDielectronPair::GetLXY(const AliVVertex * const vtx) const | |
404 | // { | |
405 | // // | |
406 | // // Calculate the decay length in XY taking into account the primary vertex position | |
407 | // // | |
408 | // if(!vtx) return 0; | |
409 | // return ( (Xv()-vtx->GetX()) * Px() + (Yv()-vtx->GetY()) * Py() )/Pt() ; | |
410 | // } | |
ba15fdfb | 411 | |
5720c765 | 412 | // //______________________________________________ |
413 | // Double_t AliDielectronPair::GetPseudoProperTime(const AliVVertex * const vtx) const | |
414 | // { | |
415 | // // | |
416 | // // Calculate the pseudo proper time | |
417 | // // | |
418 | // Double_t lxy=GetLXY(vtx); | |
419 | // Double_t psProperDecayLength = lxy*(TDatabasePDG::Instance()->GetParticle(443)->Mass())/Pt(); | |
420 | // return psProperDecayLength; | |
421 | // } |