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1 | /************************************************************************** | |
2 | * Copyright(c) 1998-1999, 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 | /* $Id$ */ | |
17 | ||
18 | //----------------------------------------------------------------------------- | |
19 | // Class AliMUONTrackExtrap | |
20 | // ------------------------ | |
21 | // Tools for track extrapolation in ALICE dimuon spectrometer | |
22 | // Author: Philippe Pillot | |
23 | //----------------------------------------------------------------------------- | |
24 | ||
25 | #include "AliMUONTrackExtrap.h" | |
26 | #include "AliMUONTrackParam.h" | |
27 | #include "AliMUONConstants.h" | |
28 | #include "AliMUONReconstructor.h" | |
29 | ||
30 | #include "AliMagF.h" | |
31 | #include "AliExternalTrackParam.h" | |
32 | ||
33 | #include <TGeoGlobalMagField.h> | |
34 | #include <TGeoManager.h> | |
35 | #include <TMath.h> | |
36 | #include <TDatabasePDG.h> | |
37 | ||
38 | #include <Riostream.h> | |
39 | ||
40 | /// \cond CLASSIMP | |
41 | ClassImp(AliMUONTrackExtrap) // Class implementation in ROOT context | |
42 | /// \endcond | |
43 | ||
44 | const Double_t AliMUONTrackExtrap::fgkSimpleBPosition = 0.5 * (AliMUONConstants::CoilZ() + AliMUONConstants::YokeZ()); | |
45 | const Double_t AliMUONTrackExtrap::fgkSimpleBLength = 0.5 * (AliMUONConstants::CoilL() + AliMUONConstants::YokeL()); | |
46 | Double_t AliMUONTrackExtrap::fgSimpleBValue = 0.; | |
47 | Bool_t AliMUONTrackExtrap::fgFieldON = kFALSE; | |
48 | const Bool_t AliMUONTrackExtrap::fgkUseHelix = kFALSE; | |
49 | const Int_t AliMUONTrackExtrap::fgkMaxStepNumber = 5000; | |
50 | const Double_t AliMUONTrackExtrap::fgkHelixStepLength = 6.; | |
51 | const Double_t AliMUONTrackExtrap::fgkRungeKuttaMaxResidue = 0.002; | |
52 | ||
53 | //__________________________________________________________________________ | |
54 | void AliMUONTrackExtrap::SetField() | |
55 | { | |
56 | /// set field on/off flag; | |
57 | /// set field at the centre of the dipole | |
58 | const Double_t x[3] = {50.,50.,fgkSimpleBPosition}; | |
59 | Double_t b[3] = {0.,0.,0.}; | |
60 | TGeoGlobalMagField::Instance()->Field(x,b); | |
61 | fgSimpleBValue = b[0]; | |
62 | fgFieldON = fgSimpleBValue ? kTRUE : kFALSE; | |
63 | ||
64 | } | |
65 | ||
66 | //__________________________________________________________________________ | |
67 | Double_t AliMUONTrackExtrap::GetImpactParamFromBendingMomentum(Double_t bendingMomentum) | |
68 | { | |
69 | /// Returns impact parameter at vertex in bending plane (cm), | |
70 | /// from the signed bending momentum "BendingMomentum" in bending plane (GeV/c), | |
71 | /// using simple values for dipole magnetic field. | |
72 | /// The sign of "BendingMomentum" is the sign of the charge. | |
73 | ||
74 | if (bendingMomentum == 0.) return 1.e10; | |
75 | ||
76 | const Double_t kCorrectionFactor = 1.1; // impact parameter is 10% underestimated | |
77 | ||
78 | return kCorrectionFactor * (-0.0003 * fgSimpleBValue * fgkSimpleBLength * fgkSimpleBPosition / bendingMomentum); | |
79 | } | |
80 | ||
81 | //__________________________________________________________________________ | |
82 | Double_t | |
83 | AliMUONTrackExtrap::GetBendingMomentumFromImpactParam(Double_t impactParam) | |
84 | { | |
85 | /// Returns signed bending momentum in bending plane (GeV/c), | |
86 | /// the sign being the sign of the charge for particles moving forward in Z, | |
87 | /// from the impact parameter "ImpactParam" at vertex in bending plane (cm), | |
88 | /// using simple values for dipole magnetic field. | |
89 | ||
90 | if (impactParam == 0.) return 1.e10; | |
91 | ||
92 | const Double_t kCorrectionFactor = 1.1; // bending momentum is 10% underestimated | |
93 | ||
94 | if (fgFieldON) | |
95 | { | |
96 | return kCorrectionFactor * (-0.0003 * fgSimpleBValue * fgkSimpleBLength * fgkSimpleBPosition / impactParam); | |
97 | } | |
98 | else | |
99 | { | |
100 | return AliMUONConstants::GetMostProbBendingMomentum(); | |
101 | } | |
102 | } | |
103 | ||
104 | //__________________________________________________________________________ | |
105 | void AliMUONTrackExtrap::LinearExtrapToZ(AliMUONTrackParam* trackParam, Double_t zEnd) | |
106 | { | |
107 | /// Track parameters linearly extrapolated to the plane at "zEnd". | |
108 | /// On return, results from the extrapolation are updated in trackParam. | |
109 | ||
110 | if (trackParam->GetZ() == zEnd) return; // nothing to be done if same z | |
111 | ||
112 | // Compute track parameters | |
113 | Double_t dZ = zEnd - trackParam->GetZ(); | |
114 | trackParam->SetNonBendingCoor(trackParam->GetNonBendingCoor() + trackParam->GetNonBendingSlope() * dZ); | |
115 | trackParam->SetBendingCoor(trackParam->GetBendingCoor() + trackParam->GetBendingSlope() * dZ); | |
116 | trackParam->SetZ(zEnd); | |
117 | } | |
118 | ||
119 | //__________________________________________________________________________ | |
120 | void AliMUONTrackExtrap::LinearExtrapToZCov(AliMUONTrackParam* trackParam, Double_t zEnd, Bool_t updatePropagator) | |
121 | { | |
122 | /// Track parameters and their covariances linearly extrapolated to the plane at "zEnd". | |
123 | /// On return, results from the extrapolation are updated in trackParam. | |
124 | ||
125 | if (trackParam->GetZ() == zEnd) return; // nothing to be done if same z | |
126 | ||
127 | // No need to propagate the covariance matrix if it does not exist | |
128 | if (!trackParam->CovariancesExist()) { | |
129 | cout<<"W-AliMUONTrackExtrap::LinearExtrapToZCov: Covariance matrix does not exist"<<endl; | |
130 | // Extrapolate linearly track parameters to "zEnd" | |
131 | LinearExtrapToZ(trackParam,zEnd); | |
132 | return; | |
133 | } | |
134 | ||
135 | // Compute track parameters | |
136 | Double_t dZ = zEnd - trackParam->GetZ(); | |
137 | trackParam->SetNonBendingCoor(trackParam->GetNonBendingCoor() + trackParam->GetNonBendingSlope() * dZ); | |
138 | trackParam->SetBendingCoor(trackParam->GetBendingCoor() + trackParam->GetBendingSlope() * dZ); | |
139 | trackParam->SetZ(zEnd); | |
140 | ||
141 | // Calculate the jacobian related to the track parameters linear extrapolation to "zEnd" | |
142 | TMatrixD jacob(5,5); | |
143 | jacob.UnitMatrix(); | |
144 | jacob(0,1) = dZ; | |
145 | jacob(2,3) = dZ; | |
146 | ||
147 | // Extrapolate track parameter covariances to "zEnd" | |
148 | TMatrixD tmp(trackParam->GetCovariances(),TMatrixD::kMultTranspose,jacob); | |
149 | TMatrixD tmp2(jacob,TMatrixD::kMult,tmp); | |
150 | trackParam->SetCovariances(tmp2); | |
151 | ||
152 | // Update the propagator if required | |
153 | if (updatePropagator) trackParam->UpdatePropagator(jacob); | |
154 | } | |
155 | ||
156 | //__________________________________________________________________________ | |
157 | void AliMUONTrackExtrap::ExtrapToZ(AliMUONTrackParam* trackParam, Double_t zEnd) | |
158 | { | |
159 | /// Interface to track parameter extrapolation to the plane at "Z" using Helix or Rungekutta algorithm. | |
160 | /// On return, the track parameters resulting from the extrapolation are updated in trackParam. | |
161 | if (!fgFieldON) AliMUONTrackExtrap::LinearExtrapToZ(trackParam,zEnd); | |
162 | else if (fgkUseHelix) AliMUONTrackExtrap::ExtrapToZHelix(trackParam,zEnd); | |
163 | else AliMUONTrackExtrap::ExtrapToZRungekutta(trackParam,zEnd); | |
164 | } | |
165 | ||
166 | //__________________________________________________________________________ | |
167 | void AliMUONTrackExtrap::ExtrapToZHelix(AliMUONTrackParam* trackParam, Double_t zEnd) | |
168 | { | |
169 | /// Track parameter extrapolation to the plane at "Z" using Helix algorithm. | |
170 | /// On return, the track parameters resulting from the extrapolation are updated in trackParam. | |
171 | if (trackParam->GetZ() == zEnd) return; // nothing to be done if same Z | |
172 | Double_t forwardBackward; // +1 if forward, -1 if backward | |
173 | if (zEnd < trackParam->GetZ()) forwardBackward = 1.0; // spectro. z<0 | |
174 | else forwardBackward = -1.0; | |
175 | Double_t v3[7], v3New[7]; // 7 in parameter ???? | |
176 | Int_t i3, stepNumber; | |
177 | // For safety: return kTRUE or kFALSE ???? | |
178 | // Parameter vector for calling EXTRAP_ONESTEP | |
179 | ConvertTrackParamForExtrap(trackParam, forwardBackward, v3); | |
180 | // sign of charge (sign of fInverseBendingMomentum if forward motion) | |
181 | // must be changed if backward extrapolation | |
182 | Double_t chargeExtrap = forwardBackward * TMath::Sign(Double_t(1.0), trackParam->GetInverseBendingMomentum()); | |
183 | // Extrapolation loop | |
184 | stepNumber = 0; | |
185 | while (((-forwardBackward * (v3[2] - zEnd)) <= 0.0) && (stepNumber < fgkMaxStepNumber)) { // spectro. z<0 | |
186 | stepNumber++; | |
187 | ExtrapOneStepHelix(chargeExtrap, fgkHelixStepLength, v3, v3New); | |
188 | if ((-forwardBackward * (v3New[2] - zEnd)) > 0.0) break; // one is beyond Z spectro. z<0 | |
189 | // better use TArray ???? | |
190 | for (i3 = 0; i3 < 7; i3++) {v3[i3] = v3New[i3];} | |
191 | } | |
192 | // check fgkMaxStepNumber ???? | |
193 | // Interpolation back to exact Z (2nd order) | |
194 | // should be in function ???? using TArray ???? | |
195 | Double_t dZ12 = v3New[2] - v3[2]; // 1->2 | |
196 | if (TMath::Abs(dZ12) > 0) { | |
197 | Double_t dZ1i = zEnd - v3[2]; // 1-i | |
198 | Double_t dZi2 = v3New[2] - zEnd; // i->2 | |
199 | Double_t xPrime = (v3New[0] - v3[0]) / dZ12; | |
200 | Double_t xSecond = ((v3New[3] / v3New[5]) - (v3[3] / v3[5])) / dZ12; | |
201 | Double_t yPrime = (v3New[1] - v3[1]) / dZ12; | |
202 | Double_t ySecond = ((v3New[4] / v3New[5]) - (v3[4] / v3[5])) / dZ12; | |
203 | v3[0] = v3[0] + xPrime * dZ1i - 0.5 * xSecond * dZ1i * dZi2; // X | |
204 | v3[1] = v3[1] + yPrime * dZ1i - 0.5 * ySecond * dZ1i * dZi2; // Y | |
205 | v3[2] = zEnd; // Z | |
206 | Double_t xPrimeI = xPrime - 0.5 * xSecond * (dZi2 - dZ1i); | |
207 | Double_t yPrimeI = yPrime - 0.5 * ySecond * (dZi2 - dZ1i); | |
208 | // (PX, PY, PZ)/PTOT assuming forward motion | |
209 | v3[5] = 1.0 / TMath::Sqrt(1.0 + xPrimeI * xPrimeI + yPrimeI * yPrimeI); // PZ/PTOT | |
210 | v3[3] = xPrimeI * v3[5]; // PX/PTOT | |
211 | v3[4] = yPrimeI * v3[5]; // PY/PTOT | |
212 | } else { | |
213 | cout<<"W-AliMUONTrackExtrap::ExtrapToZHelix: Extrap. to Z not reached, Z = "<<zEnd<<endl; | |
214 | } | |
215 | // Recover track parameters (charge back for forward motion) | |
216 | RecoverTrackParam(v3, chargeExtrap * forwardBackward, trackParam); | |
217 | } | |
218 | ||
219 | //__________________________________________________________________________ | |
220 | void AliMUONTrackExtrap::ExtrapToZRungekutta(AliMUONTrackParam* trackParam, Double_t zEnd) | |
221 | { | |
222 | /// Track parameter extrapolation to the plane at "Z" using Rungekutta algorithm. | |
223 | /// On return, the track parameters resulting from the extrapolation are updated in trackParam. | |
224 | if (trackParam->GetZ() == zEnd) return; // nothing to be done if same Z | |
225 | Double_t forwardBackward; // +1 if forward, -1 if backward | |
226 | if (zEnd < trackParam->GetZ()) forwardBackward = 1.0; // spectro. z<0 | |
227 | else forwardBackward = -1.0; | |
228 | // sign of charge (sign of fInverseBendingMomentum if forward motion) | |
229 | // must be changed if backward extrapolation | |
230 | Double_t chargeExtrap = forwardBackward * TMath::Sign(Double_t(1.0), trackParam->GetInverseBendingMomentum()); | |
231 | Double_t v3[7], v3New[7]; | |
232 | Double_t dZ, step; | |
233 | Int_t stepNumber = 0; | |
234 | ||
235 | // Extrapolation loop (until within tolerance) | |
236 | Double_t residue = zEnd - trackParam->GetZ(); | |
237 | while (TMath::Abs(residue) > fgkRungeKuttaMaxResidue && stepNumber <= fgkMaxStepNumber) { | |
238 | dZ = zEnd - trackParam->GetZ(); | |
239 | // step lenght assuming linear trajectory | |
240 | step = dZ * TMath::Sqrt(1.0 + trackParam->GetBendingSlope()*trackParam->GetBendingSlope() + | |
241 | trackParam->GetNonBendingSlope()*trackParam->GetNonBendingSlope()); | |
242 | ConvertTrackParamForExtrap(trackParam, forwardBackward, v3); | |
243 | do { // reduce step lenght while zEnd oversteped | |
244 | if (stepNumber > fgkMaxStepNumber) { | |
245 | cout<<"W-AliMUONTrackExtrap::ExtrapToZRungekutta: Too many trials: "<<stepNumber<<endl; | |
246 | break; | |
247 | } | |
248 | stepNumber ++; | |
249 | step = TMath::Abs(step); | |
250 | AliMUONTrackExtrap::ExtrapOneStepRungekutta(chargeExtrap,step,v3,v3New); | |
251 | residue = zEnd - v3New[2]; | |
252 | step *= dZ/(v3New[2]-trackParam->GetZ()); | |
253 | } while (residue*dZ < 0 && TMath::Abs(residue) > fgkRungeKuttaMaxResidue); | |
254 | RecoverTrackParam(v3New, chargeExtrap * forwardBackward, trackParam); | |
255 | } | |
256 | ||
257 | // terminate the extropolation with a straight line up to the exact "zEnd" value | |
258 | trackParam->SetNonBendingCoor(trackParam->GetNonBendingCoor() + residue * trackParam->GetNonBendingSlope()); | |
259 | trackParam->SetBendingCoor(trackParam->GetBendingCoor() + residue * trackParam->GetBendingSlope()); | |
260 | trackParam->SetZ(zEnd); | |
261 | } | |
262 | ||
263 | //__________________________________________________________________________ | |
264 | void AliMUONTrackExtrap::ConvertTrackParamForExtrap(AliMUONTrackParam* trackParam, Double_t forwardBackward, Double_t *v3) | |
265 | { | |
266 | /// Set vector of Geant3 parameters pointed to by "v3" from track parameters in trackParam. | |
267 | /// Since AliMUONTrackParam is only geometry, one uses "forwardBackward" | |
268 | /// to know whether the particle is going forward (+1) or backward (-1). | |
269 | v3[0] = trackParam->GetNonBendingCoor(); // X | |
270 | v3[1] = trackParam->GetBendingCoor(); // Y | |
271 | v3[2] = trackParam->GetZ(); // Z | |
272 | Double_t pYZ = TMath::Abs(1.0 / trackParam->GetInverseBendingMomentum()); | |
273 | Double_t pZ = pYZ / TMath::Sqrt(1.0 + trackParam->GetBendingSlope() * trackParam->GetBendingSlope()); | |
274 | v3[6] = TMath::Sqrt(pYZ * pYZ + pZ * pZ * trackParam->GetNonBendingSlope() * trackParam->GetNonBendingSlope()); // PTOT | |
275 | v3[5] = -forwardBackward * pZ / v3[6]; // PZ/PTOT spectro. z<0 | |
276 | v3[3] = trackParam->GetNonBendingSlope() * v3[5]; // PX/PTOT | |
277 | v3[4] = trackParam->GetBendingSlope() * v3[5]; // PY/PTOT | |
278 | } | |
279 | ||
280 | //__________________________________________________________________________ | |
281 | void AliMUONTrackExtrap::RecoverTrackParam(Double_t *v3, Double_t charge, AliMUONTrackParam* trackParam) | |
282 | { | |
283 | /// Set track parameters in trackParam from Geant3 parameters pointed to by "v3", | |
284 | /// assumed to be calculated for forward motion in Z. | |
285 | /// "InverseBendingMomentum" is signed with "charge". | |
286 | trackParam->SetNonBendingCoor(v3[0]); // X | |
287 | trackParam->SetBendingCoor(v3[1]); // Y | |
288 | trackParam->SetZ(v3[2]); // Z | |
289 | Double_t pYZ = v3[6] * TMath::Sqrt((1.-v3[3])*(1.+v3[3])); | |
290 | trackParam->SetInverseBendingMomentum(charge/pYZ); | |
291 | trackParam->SetBendingSlope(v3[4]/v3[5]); | |
292 | trackParam->SetNonBendingSlope(v3[3]/v3[5]); | |
293 | } | |
294 | ||
295 | //__________________________________________________________________________ | |
296 | void AliMUONTrackExtrap::ExtrapToZCov(AliMUONTrackParam* trackParam, Double_t zEnd, Bool_t updatePropagator) | |
297 | { | |
298 | /// Track parameters and their covariances extrapolated to the plane at "zEnd". | |
299 | /// On return, results from the extrapolation are updated in trackParam. | |
300 | ||
301 | if (trackParam->GetZ() == zEnd) return; // nothing to be done if same z | |
302 | ||
303 | if (!fgFieldON) { // linear extrapolation if no magnetic field | |
304 | AliMUONTrackExtrap::LinearExtrapToZCov(trackParam,zEnd,updatePropagator); | |
305 | return; | |
306 | } | |
307 | ||
308 | // No need to propagate the covariance matrix if it does not exist | |
309 | if (!trackParam->CovariancesExist()) { | |
310 | cout<<"W-AliMUONTrackExtrap::ExtrapToZCov: Covariance matrix does not exist"<<endl; | |
311 | // Extrapolate track parameters to "zEnd" | |
312 | ExtrapToZ(trackParam,zEnd); | |
313 | return; | |
314 | } | |
315 | ||
316 | // Save the actual track parameters | |
317 | AliMUONTrackParam trackParamSave(*trackParam); | |
318 | TMatrixD paramSave(trackParamSave.GetParameters()); | |
319 | Double_t zBegin = trackParamSave.GetZ(); | |
320 | ||
321 | // Get reference to the parameter covariance matrix | |
322 | const TMatrixD& kParamCov = trackParam->GetCovariances(); | |
323 | ||
324 | // Extrapolate track parameters to "zEnd" | |
325 | ExtrapToZ(trackParam,zEnd); | |
326 | ||
327 | // Get reference to the extrapolated parameters | |
328 | const TMatrixD& extrapParam = trackParam->GetParameters(); | |
329 | ||
330 | // Calculate the jacobian related to the track parameters extrapolation to "zEnd" | |
331 | TMatrixD jacob(5,5); | |
332 | jacob.Zero(); | |
333 | TMatrixD dParam(5,1); | |
334 | Double_t direction[5] = {-1.,-1.,1.,1.,-1.}; | |
335 | for (Int_t i=0; i<5; i++) { | |
336 | // Skip jacobian calculation for parameters with no associated error | |
337 | if (kParamCov(i,i) <= 0.) continue; | |
338 | ||
339 | // Small variation of parameter i only | |
340 | for (Int_t j=0; j<5; j++) { | |
341 | if (j==i) { | |
342 | dParam(j,0) = TMath::Sqrt(kParamCov(i,i)); | |
343 | dParam(j,0) *= TMath::Sign(1.,direction[j]*paramSave(j,0)); // variation always in the same direction | |
344 | } else dParam(j,0) = 0.; | |
345 | } | |
346 | ||
347 | // Set new parameters | |
348 | trackParamSave.SetParameters(paramSave); | |
349 | trackParamSave.AddParameters(dParam); | |
350 | trackParamSave.SetZ(zBegin); | |
351 | ||
352 | // Extrapolate new track parameters to "zEnd" | |
353 | ExtrapToZ(&trackParamSave,zEnd); | |
354 | ||
355 | // Calculate the jacobian | |
356 | TMatrixD jacobji(trackParamSave.GetParameters(),TMatrixD::kMinus,extrapParam); | |
357 | jacobji *= 1. / dParam(i,0); | |
358 | jacob.SetSub(0,i,jacobji); | |
359 | } | |
360 | ||
361 | // Extrapolate track parameter covariances to "zEnd" | |
362 | TMatrixD tmp(kParamCov,TMatrixD::kMultTranspose,jacob); | |
363 | TMatrixD tmp2(jacob,TMatrixD::kMult,tmp); | |
364 | trackParam->SetCovariances(tmp2); | |
365 | ||
366 | // Update the propagator if required | |
367 | if (updatePropagator) trackParam->UpdatePropagator(jacob); | |
368 | } | |
369 | ||
370 | //__________________________________________________________________________ | |
371 | void AliMUONTrackExtrap::AddMCSEffectInAbsorber(AliMUONTrackParam* param, Double_t pathLength, Double_t f0, Double_t f1, Double_t f2) | |
372 | { | |
373 | /// Add to the track parameter covariances the effects of multiple Coulomb scattering | |
374 | /// The absorber correction parameters are supposed to be calculated at the current track z-position | |
375 | ||
376 | // absorber related covariance parameters | |
377 | Double_t bendingSlope = param->GetBendingSlope(); | |
378 | Double_t nonBendingSlope = param->GetNonBendingSlope(); | |
379 | Double_t inverseBendingMomentum = param->GetInverseBendingMomentum(); | |
380 | Double_t alpha2 = 0.0136 * 0.0136 * inverseBendingMomentum * inverseBendingMomentum * (1.0 + bendingSlope * bendingSlope) / | |
381 | (1.0 + bendingSlope *bendingSlope + nonBendingSlope * nonBendingSlope); // velocity = 1 | |
382 | Double_t varCoor = alpha2 * (pathLength * pathLength * f0 - 2. * pathLength * f1 + f2); | |
383 | Double_t covCorrSlope = alpha2 * (pathLength * f0 - f1); | |
384 | Double_t varSlop = alpha2 * f0; | |
385 | ||
386 | // Set MCS covariance matrix | |
387 | TMatrixD newParamCov(param->GetCovariances()); | |
388 | // Non bending plane | |
389 | newParamCov(0,0) += varCoor; newParamCov(0,1) += covCorrSlope; | |
390 | newParamCov(1,0) += covCorrSlope; newParamCov(1,1) += varSlop; | |
391 | // Bending plane | |
392 | newParamCov(2,2) += varCoor; newParamCov(2,3) += covCorrSlope; | |
393 | newParamCov(3,2) += covCorrSlope; newParamCov(3,3) += varSlop; | |
394 | ||
395 | // Set momentum related covariances if B!=0 | |
396 | if (fgFieldON) { | |
397 | // compute derivative d(q/Pxy) / dSlopeX and d(q/Pxy) / dSlopeY | |
398 | Double_t dqPxydSlopeX = inverseBendingMomentum * nonBendingSlope / (1. + nonBendingSlope*nonBendingSlope + bendingSlope*bendingSlope); | |
399 | Double_t dqPxydSlopeY = - inverseBendingMomentum * nonBendingSlope*nonBendingSlope * bendingSlope / | |
400 | (1. + bendingSlope*bendingSlope) / (1. + nonBendingSlope*nonBendingSlope + bendingSlope*bendingSlope); | |
401 | // Inverse bending momentum (due to dependences with bending and non bending slopes) | |
402 | newParamCov(4,0) += dqPxydSlopeX * covCorrSlope; newParamCov(0,4) += dqPxydSlopeX * covCorrSlope; | |
403 | newParamCov(4,1) += dqPxydSlopeX * varSlop; newParamCov(1,4) += dqPxydSlopeX * varSlop; | |
404 | newParamCov(4,2) += dqPxydSlopeY * covCorrSlope; newParamCov(2,4) += dqPxydSlopeY * covCorrSlope; | |
405 | newParamCov(4,3) += dqPxydSlopeY * varSlop; newParamCov(3,4) += dqPxydSlopeY * varSlop; | |
406 | newParamCov(4,4) += (dqPxydSlopeX*dqPxydSlopeX + dqPxydSlopeY*dqPxydSlopeY) * varSlop; | |
407 | } | |
408 | ||
409 | // Set new covariances | |
410 | param->SetCovariances(newParamCov); | |
411 | } | |
412 | ||
413 | //__________________________________________________________________________ | |
414 | void AliMUONTrackExtrap::CorrectMCSEffectInAbsorber(AliMUONTrackParam* param, | |
415 | Double_t xVtx, Double_t yVtx, Double_t zVtx, | |
416 | Double_t errXVtx, Double_t errYVtx, | |
417 | Double_t absZBeg, Double_t pathLength, Double_t f0, Double_t f1, Double_t f2) | |
418 | { | |
419 | /// Correct parameters and corresponding covariances using Branson correction | |
420 | /// - input param are parameters and covariances at the end of absorber | |
421 | /// - output param are parameters and covariances at vertex | |
422 | /// Absorber correction parameters are supposed to be calculated at the current track z-position | |
423 | ||
424 | // Position of the Branson plane (spectro. (z<0)) | |
425 | Double_t zB = (f1>0.) ? absZBeg - f2/f1 : 0.; | |
426 | ||
427 | // Add MCS effects to current parameter covariances | |
428 | AddMCSEffectInAbsorber(param, pathLength, f0, f1, f2); | |
429 | ||
430 | // Get track parameters and covariances in the Branson plane corrected for magnetic field effect | |
431 | ExtrapToZCov(param,zVtx); | |
432 | LinearExtrapToZCov(param,zB); | |
433 | ||
434 | // compute track parameters at vertex | |
435 | TMatrixD newParam(5,1); | |
436 | newParam(0,0) = xVtx; | |
437 | newParam(1,0) = (param->GetNonBendingCoor() - xVtx) / (zB - zVtx); | |
438 | newParam(2,0) = yVtx; | |
439 | newParam(3,0) = (param->GetBendingCoor() - yVtx) / (zB - zVtx); | |
440 | newParam(4,0) = param->GetCharge() / param->P() * | |
441 | TMath::Sqrt(1.0 + newParam(1,0)*newParam(1,0) + newParam(3,0)*newParam(3,0)) / | |
442 | TMath::Sqrt(1.0 + newParam(3,0)*newParam(3,0)); | |
443 | ||
444 | // Get covariances in (X, SlopeX, Y, SlopeY, q*PTot) coordinate system | |
445 | TMatrixD paramCovP(param->GetCovariances()); | |
446 | Cov2CovP(param->GetParameters(),paramCovP); | |
447 | ||
448 | // Get the covariance matrix in the (XVtx, X, YVtx, Y, q*PTot) coordinate system | |
449 | TMatrixD paramCovVtx(5,5); | |
450 | paramCovVtx.Zero(); | |
451 | paramCovVtx(0,0) = errXVtx * errXVtx; | |
452 | paramCovVtx(1,1) = paramCovP(0,0); | |
453 | paramCovVtx(2,2) = errYVtx * errYVtx; | |
454 | paramCovVtx(3,3) = paramCovP(2,2); | |
455 | paramCovVtx(4,4) = paramCovP(4,4); | |
456 | paramCovVtx(1,3) = paramCovP(0,2); | |
457 | paramCovVtx(3,1) = paramCovP(2,0); | |
458 | paramCovVtx(1,4) = paramCovP(0,4); | |
459 | paramCovVtx(4,1) = paramCovP(4,0); | |
460 | paramCovVtx(3,4) = paramCovP(2,4); | |
461 | paramCovVtx(4,3) = paramCovP(4,2); | |
462 | ||
463 | // Jacobian of the transformation (XVtx, X, YVtx, Y, q*PTot) -> (XVtx, SlopeXVtx, YVtx, SlopeYVtx, q*PTotVtx) | |
464 | TMatrixD jacob(5,5); | |
465 | jacob.UnitMatrix(); | |
466 | jacob(1,0) = - 1. / (zB - zVtx); | |
467 | jacob(1,1) = 1. / (zB - zVtx); | |
468 | jacob(3,2) = - 1. / (zB - zVtx); | |
469 | jacob(3,3) = 1. / (zB - zVtx); | |
470 | ||
471 | // Compute covariances at vertex in the (XVtx, SlopeXVtx, YVtx, SlopeYVtx, q*PTotVtx) coordinate system | |
472 | TMatrixD tmp(paramCovVtx,TMatrixD::kMultTranspose,jacob); | |
473 | TMatrixD newParamCov(jacob,TMatrixD::kMult,tmp); | |
474 | ||
475 | // Compute covariances at vertex in the (XVtx, SlopeXVtx, YVtx, SlopeYVtx, q/PyzVtx) coordinate system | |
476 | CovP2Cov(newParam,newParamCov); | |
477 | ||
478 | // Set parameters and covariances at vertex | |
479 | param->SetParameters(newParam); | |
480 | param->SetZ(zVtx); | |
481 | param->SetCovariances(newParamCov); | |
482 | } | |
483 | ||
484 | //__________________________________________________________________________ | |
485 | void AliMUONTrackExtrap::CorrectELossEffectInAbsorber(AliMUONTrackParam* param, Double_t eLoss, Double_t sigmaELoss2) | |
486 | { | |
487 | /// Correct parameters for energy loss and add energy loss fluctuation effect to covariances | |
488 | ||
489 | // Get parameter covariances in (X, SlopeX, Y, SlopeY, q*PTot) coordinate system | |
490 | TMatrixD newParamCov(param->GetCovariances()); | |
491 | Cov2CovP(param->GetParameters(),newParamCov); | |
492 | ||
493 | // Compute new parameters corrected for energy loss | |
494 | Double_t muMass = TDatabasePDG::Instance()->GetParticle("mu-")->Mass(); // GeV | |
495 | Double_t p = param->P(); | |
496 | Double_t e = TMath::Sqrt(p*p + muMass*muMass); | |
497 | Double_t eCorr = e + eLoss; | |
498 | Double_t pCorr = TMath::Sqrt(eCorr*eCorr - muMass*muMass); | |
499 | Double_t nonBendingSlope = param->GetNonBendingSlope(); | |
500 | Double_t bendingSlope = param->GetBendingSlope(); | |
501 | param->SetInverseBendingMomentum(param->GetCharge() / pCorr * | |
502 | TMath::Sqrt(1.0 + nonBendingSlope*nonBendingSlope + bendingSlope*bendingSlope) / | |
503 | TMath::Sqrt(1.0 + bendingSlope*bendingSlope)); | |
504 | ||
505 | // Add effects of energy loss fluctuation to covariances | |
506 | newParamCov(4,4) += eCorr * eCorr / pCorr / pCorr * sigmaELoss2; | |
507 | ||
508 | // Get new parameter covariances in (X, SlopeX, Y, SlopeY, q/Pyz) coordinate system | |
509 | CovP2Cov(param->GetParameters(),newParamCov); | |
510 | ||
511 | // Set new parameter covariances | |
512 | param->SetCovariances(newParamCov); | |
513 | } | |
514 | ||
515 | //__________________________________________________________________________ | |
516 | Bool_t AliMUONTrackExtrap::GetAbsorberCorrectionParam(Double_t trackXYZIn[3], Double_t trackXYZOut[3], Double_t pTotal, | |
517 | Double_t &pathLength, Double_t &f0, Double_t &f1, Double_t &f2, | |
518 | Double_t &meanRho, Double_t &totalELoss, Double_t &sigmaELoss2) | |
519 | { | |
520 | /// Parameters used to correct for Multiple Coulomb Scattering and energy loss in absorber | |
521 | /// Calculated assuming a linear propagation from trackXYZIn to trackXYZOut (order is important) | |
522 | // pathLength: path length between trackXYZIn and trackXYZOut (cm) | |
523 | // f0: 0th moment of z calculated with the inverse radiation-length distribution | |
524 | // f1: 1st moment of z calculated with the inverse radiation-length distribution | |
525 | // f2: 2nd moment of z calculated with the inverse radiation-length distribution | |
526 | // meanRho: average density of crossed material (g/cm3) | |
527 | // totalELoss: total energy loss in absorber | |
528 | ||
529 | // Reset absorber's parameters | |
530 | pathLength = 0.; | |
531 | f0 = 0.; | |
532 | f1 = 0.; | |
533 | f2 = 0.; | |
534 | meanRho = 0.; | |
535 | totalELoss = 0.; | |
536 | sigmaELoss2 = 0.; | |
537 | ||
538 | // Check whether the geometry is available | |
539 | if (!gGeoManager) { | |
540 | cout<<"E-AliMUONTrackExtrap::GetAbsorberCorrectionParam: no TGeo"<<endl; | |
541 | return kFALSE; | |
542 | } | |
543 | ||
544 | // Initialize starting point and direction | |
545 | pathLength = TMath::Sqrt((trackXYZOut[0] - trackXYZIn[0])*(trackXYZOut[0] - trackXYZIn[0])+ | |
546 | (trackXYZOut[1] - trackXYZIn[1])*(trackXYZOut[1] - trackXYZIn[1])+ | |
547 | (trackXYZOut[2] - trackXYZIn[2])*(trackXYZOut[2] - trackXYZIn[2])); | |
548 | if (pathLength < TGeoShape::Tolerance()) return kFALSE; | |
549 | Double_t b[3]; | |
550 | b[0] = (trackXYZOut[0] - trackXYZIn[0]) / pathLength; | |
551 | b[1] = (trackXYZOut[1] - trackXYZIn[1]) / pathLength; | |
552 | b[2] = (trackXYZOut[2] - trackXYZIn[2]) / pathLength; | |
553 | TGeoNode *currentnode = gGeoManager->InitTrack(trackXYZIn, b); | |
554 | if (!currentnode) { | |
555 | cout<<"E-AliMUONTrackExtrap::GetAbsorberCorrectionParam: start point out of geometry"<<endl; | |
556 | return kFALSE; | |
557 | } | |
558 | ||
559 | // loop over absorber slices and calculate absorber's parameters | |
560 | Double_t rho = 0.; // material density (g/cm3) | |
561 | Double_t x0 = 0.; // radiation-length (cm-1) | |
562 | Double_t atomicA = 0.; // A of material | |
563 | Double_t atomicZ = 0.; // Z of material | |
564 | Double_t localPathLength = 0; | |
565 | Double_t remainingPathLength = pathLength; | |
566 | Double_t zB = trackXYZIn[2]; | |
567 | Double_t zE, dzB, dzE; | |
568 | do { | |
569 | // Get material properties | |
570 | TGeoMaterial *material = currentnode->GetVolume()->GetMedium()->GetMaterial(); | |
571 | rho = material->GetDensity(); | |
572 | x0 = material->GetRadLen(); | |
573 | if (!material->IsMixture()) x0 /= rho; // different normalization in the modeler for mixture | |
574 | atomicA = material->GetA(); | |
575 | atomicZ = material->GetZ(); | |
576 | ||
577 | // Get path length within this material | |
578 | gGeoManager->FindNextBoundary(remainingPathLength); | |
579 | localPathLength = gGeoManager->GetStep() + 1.e-6; | |
580 | // Check if boundary within remaining path length. If so, make sure to cross the boundary to prepare the next step | |
581 | if (localPathLength >= remainingPathLength) localPathLength = remainingPathLength; | |
582 | else { | |
583 | currentnode = gGeoManager->Step(); | |
584 | if (!currentnode) { | |
585 | cout<<"E-AliMUONTrackExtrap::GetAbsorberCorrectionParam: navigation failed"<<endl; | |
586 | f0 = f1 = f2 = meanRho = totalELoss = sigmaELoss2 = 0.; | |
587 | return kFALSE; | |
588 | } | |
589 | if (!gGeoManager->IsEntering()) { | |
590 | // make another small step to try to enter in new absorber slice | |
591 | gGeoManager->SetStep(0.001); | |
592 | currentnode = gGeoManager->Step(); | |
593 | if (!gGeoManager->IsEntering() || !currentnode) { | |
594 | cout<<"E-AliMUONTrackExtrap::GetAbsorberCorrectionParam: navigation failed"<<endl; | |
595 | f0 = f1 = f2 = meanRho = totalELoss = sigmaELoss2 = 0.; | |
596 | return kFALSE; | |
597 | } | |
598 | localPathLength += 0.001; | |
599 | } | |
600 | } | |
601 | ||
602 | // calculate absorber's parameters | |
603 | zE = b[2] * localPathLength + zB; | |
604 | dzB = zB - trackXYZIn[2]; | |
605 | dzE = zE - trackXYZIn[2]; | |
606 | f0 += localPathLength / x0; | |
607 | f1 += (dzE*dzE - dzB*dzB) / b[2] / b[2] / x0 / 2.; | |
608 | f2 += (dzE*dzE*dzE - dzB*dzB*dzB) / b[2] / b[2] / b[2] / x0 / 3.; | |
609 | meanRho += localPathLength * rho; | |
610 | totalELoss += BetheBloch(pTotal, localPathLength, rho, atomicA, atomicZ); | |
611 | sigmaELoss2 += EnergyLossFluctuation2(pTotal, localPathLength, rho, atomicA, atomicZ); | |
612 | ||
613 | // prepare next step | |
614 | zB = zE; | |
615 | remainingPathLength -= localPathLength; | |
616 | } while (remainingPathLength > TGeoShape::Tolerance()); | |
617 | ||
618 | meanRho /= pathLength; | |
619 | ||
620 | return kTRUE; | |
621 | } | |
622 | ||
623 | //__________________________________________________________________________ | |
624 | Double_t AliMUONTrackExtrap::GetMCSAngle2(const AliMUONTrackParam& param, Double_t dZ, Double_t x0) | |
625 | { | |
626 | /// Return the angular dispersion square due to multiple Coulomb scattering | |
627 | /// through a material of thickness "dZ" and of radiation length "x0" | |
628 | /// assuming linear propagation and using the small angle approximation. | |
629 | ||
630 | Double_t bendingSlope = param.GetBendingSlope(); | |
631 | Double_t nonBendingSlope = param.GetNonBendingSlope(); | |
632 | Double_t inverseTotalMomentum2 = param.GetInverseBendingMomentum() * param.GetInverseBendingMomentum() * | |
633 | (1.0 + bendingSlope * bendingSlope) / | |
634 | (1.0 + bendingSlope *bendingSlope + nonBendingSlope * nonBendingSlope); | |
635 | // Path length in the material | |
636 | Double_t pathLength = TMath::Abs(dZ) * TMath::Sqrt(1.0 + bendingSlope*bendingSlope + nonBendingSlope*nonBendingSlope); | |
637 | // relativistic velocity | |
638 | Double_t velo = 1.; | |
639 | // Angular dispersion square of the track (variance) in a plane perpendicular to the trajectory | |
640 | Double_t theta02 = 0.0136 / velo * (1 + 0.038 * TMath::Log(pathLength/x0)); | |
641 | ||
642 | return theta02 * theta02 * inverseTotalMomentum2 * pathLength / x0; | |
643 | } | |
644 | ||
645 | //__________________________________________________________________________ | |
646 | void AliMUONTrackExtrap::AddMCSEffect(AliMUONTrackParam *param, Double_t dZ, Double_t x0) | |
647 | { | |
648 | /// Add to the track parameter covariances the effects of multiple Coulomb scattering | |
649 | /// through a material of thickness "dZ" and of radiation length "x0" | |
650 | /// assuming linear propagation and using the small angle approximation. | |
651 | ||
652 | Double_t bendingSlope = param->GetBendingSlope(); | |
653 | Double_t nonBendingSlope = param->GetNonBendingSlope(); | |
654 | Double_t inverseBendingMomentum = param->GetInverseBendingMomentum(); | |
655 | Double_t inverseTotalMomentum2 = inverseBendingMomentum * inverseBendingMomentum * | |
656 | (1.0 + bendingSlope * bendingSlope) / | |
657 | (1.0 + bendingSlope *bendingSlope + nonBendingSlope * nonBendingSlope); | |
658 | // Path length in the material | |
659 | Double_t pathLength = TMath::Abs(dZ) * TMath::Sqrt(1.0 + bendingSlope*bendingSlope + nonBendingSlope*nonBendingSlope); | |
660 | Double_t pathLength2 = pathLength * pathLength; | |
661 | // relativistic velocity | |
662 | Double_t velo = 1.; | |
663 | // Angular dispersion square of the track (variance) in a plane perpendicular to the trajectory | |
664 | Double_t theta02 = 0.0136 / velo * (1 + 0.038 * TMath::Log(pathLength/x0)); | |
665 | theta02 *= theta02 * inverseTotalMomentum2 * pathLength / x0; | |
666 | ||
667 | Double_t varCoor = pathLength2 * theta02 / 3.; | |
668 | Double_t varSlop = theta02; | |
669 | Double_t covCorrSlope = pathLength * theta02 / 2.; | |
670 | ||
671 | // Set MCS covariance matrix | |
672 | TMatrixD newParamCov(param->GetCovariances()); | |
673 | // Non bending plane | |
674 | newParamCov(0,0) += varCoor; newParamCov(0,1) += covCorrSlope; | |
675 | newParamCov(1,0) += covCorrSlope; newParamCov(1,1) += varSlop; | |
676 | // Bending plane | |
677 | newParamCov(2,2) += varCoor; newParamCov(2,3) += covCorrSlope; | |
678 | newParamCov(3,2) += covCorrSlope; newParamCov(3,3) += varSlop; | |
679 | ||
680 | // Set momentum related covariances if B!=0 | |
681 | if (fgFieldON) { | |
682 | // compute derivative d(q/Pxy) / dSlopeX and d(q/Pxy) / dSlopeY | |
683 | Double_t dqPxydSlopeX = inverseBendingMomentum * nonBendingSlope / (1. + nonBendingSlope*nonBendingSlope + bendingSlope*bendingSlope); | |
684 | Double_t dqPxydSlopeY = - inverseBendingMomentum * nonBendingSlope*nonBendingSlope * bendingSlope / | |
685 | (1. + bendingSlope*bendingSlope) / (1. + nonBendingSlope*nonBendingSlope + bendingSlope*bendingSlope); | |
686 | // Inverse bending momentum (due to dependences with bending and non bending slopes) | |
687 | newParamCov(4,0) += dqPxydSlopeX * covCorrSlope; newParamCov(0,4) += dqPxydSlopeX * covCorrSlope; | |
688 | newParamCov(4,1) += dqPxydSlopeX * varSlop; newParamCov(1,4) += dqPxydSlopeX * varSlop; | |
689 | newParamCov(4,2) += dqPxydSlopeY * covCorrSlope; newParamCov(2,4) += dqPxydSlopeY * covCorrSlope; | |
690 | newParamCov(4,3) += dqPxydSlopeY * varSlop; newParamCov(3,4) += dqPxydSlopeY * varSlop; | |
691 | newParamCov(4,4) += (dqPxydSlopeX*dqPxydSlopeX + dqPxydSlopeY*dqPxydSlopeY) * varSlop; | |
692 | } | |
693 | ||
694 | // Set new covariances | |
695 | param->SetCovariances(newParamCov); | |
696 | } | |
697 | ||
698 | //__________________________________________________________________________ | |
699 | void AliMUONTrackExtrap::ExtrapToVertex(AliMUONTrackParam* trackParam, | |
700 | Double_t xVtx, Double_t yVtx, Double_t zVtx, | |
701 | Double_t errXVtx, Double_t errYVtx, | |
702 | Bool_t correctForMCS, Bool_t correctForEnergyLoss) | |
703 | { | |
704 | /// Main method for extrapolation to the vertex: | |
705 | /// Returns the track parameters and covariances resulting from the extrapolation of the current trackParam | |
706 | /// Changes parameters and covariances according to multiple scattering and energy loss corrections: | |
707 | /// if correctForMCS=kTRUE: compute parameters using Branson correction and add correction resolution to covariances | |
708 | /// if correctForMCS=kFALSE: add parameter dispersion due to MCS in parameter covariances | |
709 | /// if correctForEnergyLoss=kTRUE: correct parameters for energy loss and add energy loss fluctuation to covariances | |
710 | /// if correctForEnergyLoss=kFALSE: do nothing about energy loss | |
711 | ||
712 | if (trackParam->GetZ() == zVtx) return; // nothing to be done if already at vertex | |
713 | ||
714 | if (trackParam->GetZ() > zVtx) { // spectro. (z<0) | |
715 | cout<<"E-AliMUONTrackExtrap::ExtrapToVertex: Starting Z ("<<trackParam->GetZ() | |
716 | <<") upstream the vertex (zVtx = "<<zVtx<<")"<<endl; | |
717 | return; | |
718 | } | |
719 | ||
720 | // Check the vertex position relatively to the absorber | |
721 | if (zVtx < AliMUONConstants::AbsZBeg() && zVtx > AliMUONConstants::AbsZEnd()) { // spectro. (z<0) | |
722 | cout<<"W-AliMUONTrackExtrap::ExtrapToVertex: Ending Z ("<<zVtx | |
723 | <<") inside the front absorber ("<<AliMUONConstants::AbsZBeg()<<","<<AliMUONConstants::AbsZEnd()<<")"<<endl; | |
724 | } else if (zVtx < AliMUONConstants::AbsZEnd() ) { // spectro. (z<0) | |
725 | cout<<"W-AliMUONTrackExtrap::ExtrapToVertex: Ending Z ("<<zVtx | |
726 | <<") downstream the front absorber (zAbsorberEnd = "<<AliMUONConstants::AbsZEnd()<<")"<<endl; | |
727 | if (trackParam->CovariancesExist()) ExtrapToZCov(trackParam,zVtx); | |
728 | else ExtrapToZ(trackParam,zVtx); | |
729 | return; | |
730 | } | |
731 | ||
732 | // Check the track position relatively to the absorber and extrapolate track parameters to the end of the absorber if needed | |
733 | if (trackParam->GetZ() > AliMUONConstants::AbsZBeg()) { // spectro. (z<0) | |
734 | cout<<"W-AliMUONTrackExtrap::ExtrapToVertex: Starting Z ("<<trackParam->GetZ() | |
735 | <<") upstream the front absorber (zAbsorberBegin = "<<AliMUONConstants::AbsZBeg()<<")"<<endl; | |
736 | if (trackParam->CovariancesExist()) ExtrapToZCov(trackParam,zVtx); | |
737 | else ExtrapToZ(trackParam,zVtx); | |
738 | return; | |
739 | } else if (trackParam->GetZ() > AliMUONConstants::AbsZEnd()) { // spectro. (z<0) | |
740 | cout<<"W-AliMUONTrackExtrap::ExtrapToVertex: Starting Z ("<<trackParam->GetZ() | |
741 | <<") inside the front absorber ("<<AliMUONConstants::AbsZBeg()<<","<<AliMUONConstants::AbsZEnd()<<")"<<endl; | |
742 | } else { | |
743 | if (trackParam->CovariancesExist()) ExtrapToZCov(trackParam,AliMUONConstants::AbsZEnd()); | |
744 | else ExtrapToZ(trackParam,AliMUONConstants::AbsZEnd()); | |
745 | } | |
746 | ||
747 | // Get absorber correction parameters assuming linear propagation in absorber | |
748 | Double_t trackXYZOut[3]; | |
749 | trackXYZOut[0] = trackParam->GetNonBendingCoor(); | |
750 | trackXYZOut[1] = trackParam->GetBendingCoor(); | |
751 | trackXYZOut[2] = trackParam->GetZ(); | |
752 | Double_t trackXYZIn[3]; | |
753 | if (correctForMCS) { // assume linear propagation until the vertex | |
754 | trackXYZIn[2] = TMath::Min(zVtx, AliMUONConstants::AbsZBeg()); // spectro. (z<0) | |
755 | trackXYZIn[0] = trackXYZOut[0] + (xVtx - trackXYZOut[0]) / (zVtx - trackXYZOut[2]) * (trackXYZIn[2] - trackXYZOut[2]); | |
756 | trackXYZIn[1] = trackXYZOut[1] + (yVtx - trackXYZOut[1]) / (zVtx - trackXYZOut[2]) * (trackXYZIn[2] - trackXYZOut[2]); | |
757 | } else { | |
758 | AliMUONTrackParam trackParamIn(*trackParam); | |
759 | ExtrapToZ(&trackParamIn, TMath::Min(zVtx, AliMUONConstants::AbsZBeg())); | |
760 | trackXYZIn[0] = trackParamIn.GetNonBendingCoor(); | |
761 | trackXYZIn[1] = trackParamIn.GetBendingCoor(); | |
762 | trackXYZIn[2] = trackParamIn.GetZ(); | |
763 | } | |
764 | Double_t pTot = trackParam->P(); | |
765 | Double_t pathLength, f0, f1, f2, meanRho, totalELoss, sigmaELoss2; | |
766 | if (!GetAbsorberCorrectionParam(trackXYZIn,trackXYZOut,pTot,pathLength,f0,f1,f2,meanRho,totalELoss,sigmaELoss2)) { | |
767 | cout<<"E-AliMUONTrackExtrap::ExtrapToVertex: Unable to take into account the absorber effects"<<endl; | |
768 | if (trackParam->CovariancesExist()) ExtrapToZCov(trackParam,zVtx); | |
769 | else ExtrapToZ(trackParam,zVtx); | |
770 | return; | |
771 | } | |
772 | ||
773 | // Compute track parameters and covariances at vertex according to correctForMCS and correctForEnergyLoss flags | |
774 | if (correctForMCS) { | |
775 | ||
776 | if (correctForEnergyLoss) { | |
777 | ||
778 | // Correct for multiple scattering and energy loss | |
779 | CorrectELossEffectInAbsorber(trackParam, 0.5*totalELoss, 0.5*sigmaELoss2); | |
780 | CorrectMCSEffectInAbsorber(trackParam, xVtx, yVtx, zVtx, errXVtx, errYVtx, | |
781 | trackXYZIn[2], pathLength, f0, f1, f2); | |
782 | CorrectELossEffectInAbsorber(trackParam, 0.5*totalELoss, 0.5*sigmaELoss2); | |
783 | ||
784 | } else { | |
785 | ||
786 | // Correct for multiple scattering | |
787 | CorrectMCSEffectInAbsorber(trackParam, xVtx, yVtx, zVtx, errXVtx, errYVtx, | |
788 | trackXYZIn[2], pathLength, f0, f1, f2); | |
789 | } | |
790 | ||
791 | } else { | |
792 | ||
793 | if (correctForEnergyLoss) { | |
794 | ||
795 | // Correct for energy loss add multiple scattering dispersion in covariance matrix | |
796 | CorrectELossEffectInAbsorber(trackParam, 0.5*totalELoss, 0.5*sigmaELoss2); | |
797 | AddMCSEffectInAbsorber(trackParam, pathLength, f0, f1, f2); | |
798 | ExtrapToZCov(trackParam, trackXYZIn[2]); | |
799 | CorrectELossEffectInAbsorber(trackParam, 0.5*totalELoss, 0.5*sigmaELoss2); | |
800 | ExtrapToZCov(trackParam, zVtx); | |
801 | ||
802 | } else { | |
803 | ||
804 | // add multiple scattering dispersion in covariance matrix | |
805 | AddMCSEffectInAbsorber(trackParam, pathLength, f0, f1, f2); | |
806 | ExtrapToZCov(trackParam, zVtx); | |
807 | ||
808 | } | |
809 | ||
810 | } | |
811 | ||
812 | } | |
813 | ||
814 | //__________________________________________________________________________ | |
815 | void AliMUONTrackExtrap::ExtrapToVertex(AliMUONTrackParam* trackParam, | |
816 | Double_t xVtx, Double_t yVtx, Double_t zVtx, | |
817 | Double_t errXVtx, Double_t errYVtx) | |
818 | { | |
819 | /// Extrapolate track parameters to vertex, corrected for multiple scattering and energy loss effects | |
820 | /// Add branson correction resolution and energy loss fluctuation to parameter covariances | |
821 | ExtrapToVertex(trackParam, xVtx, yVtx, zVtx, errXVtx, errYVtx, kTRUE, kTRUE); | |
822 | } | |
823 | ||
824 | //__________________________________________________________________________ | |
825 | void AliMUONTrackExtrap::ExtrapToVertexWithoutELoss(AliMUONTrackParam* trackParam, | |
826 | Double_t xVtx, Double_t yVtx, Double_t zVtx, | |
827 | Double_t errXVtx, Double_t errYVtx) | |
828 | { | |
829 | /// Extrapolate track parameters to vertex, corrected for multiple scattering effects only | |
830 | /// Add branson correction resolution to parameter covariances | |
831 | ExtrapToVertex(trackParam, xVtx, yVtx, zVtx, errXVtx, errYVtx, kTRUE, kFALSE); | |
832 | } | |
833 | ||
834 | //__________________________________________________________________________ | |
835 | void AliMUONTrackExtrap::ExtrapToVertexWithoutBranson(AliMUONTrackParam* trackParam, Double_t zVtx) | |
836 | { | |
837 | /// Extrapolate track parameters to vertex, corrected for energy loss effects only | |
838 | /// Add dispersion due to multiple scattering and energy loss fluctuation to parameter covariances | |
839 | ExtrapToVertex(trackParam, 0., 0., zVtx, 0., 0., kFALSE, kTRUE); | |
840 | } | |
841 | ||
842 | //__________________________________________________________________________ | |
843 | void AliMUONTrackExtrap::ExtrapToVertexUncorrected(AliMUONTrackParam* trackParam, Double_t zVtx) | |
844 | { | |
845 | /// Extrapolate track parameters to vertex without multiple scattering and energy loss corrections | |
846 | /// Add dispersion due to multiple scattering to parameter covariances | |
847 | ExtrapToVertex(trackParam, 0., 0., zVtx, 0., 0., kFALSE, kFALSE); | |
848 | } | |
849 | ||
850 | //__________________________________________________________________________ | |
851 | Double_t AliMUONTrackExtrap::TotalMomentumEnergyLoss(AliMUONTrackParam* trackParam, Double_t xVtx, Double_t yVtx, Double_t zVtx) | |
852 | { | |
853 | /// Calculate the total momentum energy loss in-between the track position and the vertex assuming a linear propagation | |
854 | ||
855 | if (trackParam->GetZ() == zVtx) return 0.; // nothing to be done if already at vertex | |
856 | ||
857 | // Check whether the geometry is available | |
858 | if (!gGeoManager) { | |
859 | cout<<"E-AliMUONTrackExtrap::TotalMomentumEnergyLoss: no TGeo"<<endl; | |
860 | return 0.; | |
861 | } | |
862 | ||
863 | // Get encountered material correction parameters assuming linear propagation from vertex to the track position | |
864 | Double_t trackXYZOut[3]; | |
865 | trackXYZOut[0] = trackParam->GetNonBendingCoor(); | |
866 | trackXYZOut[1] = trackParam->GetBendingCoor(); | |
867 | trackXYZOut[2] = trackParam->GetZ(); | |
868 | Double_t trackXYZIn[3]; | |
869 | trackXYZIn[0] = xVtx; | |
870 | trackXYZIn[1] = yVtx; | |
871 | trackXYZIn[2] = zVtx; | |
872 | Double_t pTot = trackParam->P(); | |
873 | Double_t pathLength, f0, f1, f2, meanRho, totalELoss, sigmaELoss2; | |
874 | GetAbsorberCorrectionParam(trackXYZIn,trackXYZOut,pTot,pathLength,f0,f1,f2,meanRho,totalELoss,sigmaELoss2); | |
875 | ||
876 | // total momentum corrected for energy loss | |
877 | Double_t muMass = TDatabasePDG::Instance()->GetParticle("mu-")->Mass(); // GeV | |
878 | Double_t e = TMath::Sqrt(pTot*pTot + muMass*muMass); | |
879 | Double_t eCorr = e + totalELoss; | |
880 | Double_t pTotCorr = TMath::Sqrt(eCorr*eCorr - muMass*muMass); | |
881 | ||
882 | return pTotCorr - pTot; | |
883 | } | |
884 | ||
885 | //__________________________________________________________________________ | |
886 | Double_t AliMUONTrackExtrap::BetheBloch(Double_t pTotal, Double_t pathLength, Double_t rho, Double_t atomicA, Double_t atomicZ) | |
887 | { | |
888 | /// Returns the mean total momentum energy loss of muon with total momentum='pTotal' | |
889 | /// in the absorber layer of lenght='pathLength', density='rho', A='atomicA' and Z='atomicZ' | |
890 | Double_t muMass = TDatabasePDG::Instance()->GetParticle("mu-")->Mass(); // GeV | |
891 | ||
892 | // mean exitation energy (GeV) | |
893 | Double_t i; | |
894 | if (atomicZ < 13) i = (12. * atomicZ + 7.) * 1.e-9; | |
895 | else i = (9.76 * atomicZ + 58.8 * TMath::Power(atomicZ,-0.19)) * 1.e-9; | |
896 | ||
897 | return pathLength * rho * AliExternalTrackParam::BetheBlochGeant(pTotal/muMass, rho, 0.20, 3.00, i, atomicZ/atomicA); | |
898 | } | |
899 | ||
900 | //__________________________________________________________________________ | |
901 | Double_t AliMUONTrackExtrap::EnergyLossFluctuation2(Double_t pTotal, Double_t pathLength, Double_t rho, Double_t atomicA, Double_t atomicZ) | |
902 | { | |
903 | /// Returns the total momentum energy loss fluctuation of muon with total momentum='pTotal' | |
904 | /// in the absorber layer of lenght='pathLength', density='rho', A='atomicA' and Z='atomicZ' | |
905 | Double_t muMass = TDatabasePDG::Instance()->GetParticle("mu-")->Mass(); // GeV | |
906 | //Double_t eMass = 0.510998918e-3; // GeV | |
907 | Double_t k = 0.307075e-3; // GeV.g^-1.cm^2 | |
908 | Double_t p2=pTotal*pTotal; | |
909 | Double_t beta2=p2/(p2 + muMass*muMass); | |
910 | ||
911 | Double_t fwhm = 2. * k * rho * pathLength * atomicZ / atomicA / beta2; // FWHM of the energy loss Landau distribution | |
912 | Double_t sigma2 = fwhm * fwhm / (8.*log(2.)); // gaussian: fwmh = 2 * srqt(2*ln(2)) * sigma (i.e. fwmh = 2.35 * sigma) | |
913 | ||
914 | //sigma2 = k * rho * pathLength * atomicZ / atomicA * eMass; // sigma2 of the energy loss gaussian distribution | |
915 | ||
916 | return sigma2; | |
917 | } | |
918 | ||
919 | //__________________________________________________________________________ | |
920 | void AliMUONTrackExtrap::Cov2CovP(const TMatrixD ¶m, TMatrixD &cov) | |
921 | { | |
922 | /// change coordinate system: (X, SlopeX, Y, SlopeY, q/Pyz) -> (X, SlopeX, Y, SlopeY, q*PTot) | |
923 | /// parameters (param) are given in the (X, SlopeX, Y, SlopeY, q/Pyz) coordinate system | |
924 | ||
925 | // charge * total momentum | |
926 | Double_t qPTot = TMath::Sqrt(1. + param(1,0)*param(1,0) + param(3,0)*param(3,0)) / | |
927 | TMath::Sqrt(1. + param(3,0)*param(3,0)) / param(4,0); | |
928 | ||
929 | // Jacobian of the opposite transformation | |
930 | TMatrixD jacob(5,5); | |
931 | jacob.UnitMatrix(); | |
932 | jacob(4,1) = qPTot * param(1,0) / (1. + param(1,0)*param(1,0) + param(3,0)*param(3,0)); | |
933 | jacob(4,3) = - qPTot * param(1,0) * param(1,0) * param(3,0) / | |
934 | (1. + param(3,0)*param(3,0)) / (1. + param(1,0)*param(1,0) + param(3,0)*param(3,0)); | |
935 | jacob(4,4) = - qPTot / param(4,0); | |
936 | ||
937 | // compute covariances in new coordinate system | |
938 | TMatrixD tmp(cov,TMatrixD::kMultTranspose,jacob); | |
939 | cov.Mult(jacob,tmp); | |
940 | } | |
941 | ||
942 | //__________________________________________________________________________ | |
943 | void AliMUONTrackExtrap::CovP2Cov(const TMatrixD ¶m, TMatrixD &covP) | |
944 | { | |
945 | /// change coordinate system: (X, SlopeX, Y, SlopeY, q*PTot) -> (X, SlopeX, Y, SlopeY, q/Pyz) | |
946 | /// parameters (param) are given in the (X, SlopeX, Y, SlopeY, q/Pyz) coordinate system | |
947 | ||
948 | // charge * total momentum | |
949 | Double_t qPTot = TMath::Sqrt(1. + param(1,0)*param(1,0) + param(3,0)*param(3,0)) / | |
950 | TMath::Sqrt(1. + param(3,0)*param(3,0)) / param(4,0); | |
951 | ||
952 | // Jacobian of the transformation | |
953 | TMatrixD jacob(5,5); | |
954 | jacob.UnitMatrix(); | |
955 | jacob(4,1) = param(4,0) * param(1,0) / (1. + param(1,0)*param(1,0) + param(3,0)*param(3,0)); | |
956 | jacob(4,3) = - param(4,0) * param(1,0) * param(1,0) * param(3,0) / | |
957 | (1. + param(3,0)*param(3,0)) / (1. + param(1,0)*param(1,0) + param(3,0)*param(3,0)); | |
958 | jacob(4,4) = - param(4,0) / qPTot; | |
959 | ||
960 | // compute covariances in new coordinate system | |
961 | TMatrixD tmp(covP,TMatrixD::kMultTranspose,jacob); | |
962 | covP.Mult(jacob,tmp); | |
963 | } | |
964 | ||
965 | //__________________________________________________________________________ | |
966 | void AliMUONTrackExtrap::ExtrapOneStepHelix(Double_t charge, Double_t step, Double_t *vect, Double_t *vout) | |
967 | { | |
968 | /// <pre> | |
969 | /// ****************************************************************** | |
970 | /// * * | |
971 | /// * Performs the tracking of one step in a magnetic field * | |
972 | /// * The trajectory is assumed to be a helix in a constant field * | |
973 | /// * taken at the mid point of the step. * | |
974 | /// * Parameters: * | |
975 | /// * input * | |
976 | /// * STEP =arc length of the step asked * | |
977 | /// * VECT =input vector (position,direction cos and momentum) * | |
978 | /// * CHARGE= electric charge of the particle * | |
979 | /// * output * | |
980 | /// * VOUT = same as VECT after completion of the step * | |
981 | /// * * | |
982 | /// * ==>Called by : USER, GUSWIM * | |
983 | /// * Author m.hansroul ********* * | |
984 | /// * modified s.egli, s.v.levonian * | |
985 | /// * modified v.perevoztchikov | |
986 | /// * * | |
987 | /// ****************************************************************** | |
988 | /// </pre> | |
989 | ||
990 | // modif: everything in double precision | |
991 | ||
992 | Double_t xyz[3], h[4], hxp[3]; | |
993 | Double_t h2xy, hp, rho, tet; | |
994 | Double_t sint, sintt, tsint, cos1t; | |
995 | Double_t f1, f2, f3, f4, f5, f6; | |
996 | ||
997 | const Int_t kix = 0; | |
998 | const Int_t kiy = 1; | |
999 | const Int_t kiz = 2; | |
1000 | const Int_t kipx = 3; | |
1001 | const Int_t kipy = 4; | |
1002 | const Int_t kipz = 5; | |
1003 | const Int_t kipp = 6; | |
1004 | ||
1005 | const Double_t kec = 2.9979251e-4; | |
1006 | // | |
1007 | // ------------------------------------------------------------------ | |
1008 | // | |
1009 | // units are kgauss,centimeters,gev/c | |
1010 | // | |
1011 | vout[kipp] = vect[kipp]; | |
1012 | if (TMath::Abs(charge) < 0.00001) { | |
1013 | for (Int_t i = 0; i < 3; i++) { | |
1014 | vout[i] = vect[i] + step * vect[i+3]; | |
1015 | vout[i+3] = vect[i+3]; | |
1016 | } | |
1017 | return; | |
1018 | } | |
1019 | xyz[0] = vect[kix] + 0.5 * step * vect[kipx]; | |
1020 | xyz[1] = vect[kiy] + 0.5 * step * vect[kipy]; | |
1021 | xyz[2] = vect[kiz] + 0.5 * step * vect[kipz]; | |
1022 | ||
1023 | //cmodif: call gufld (xyz, h) changed into: | |
1024 | TGeoGlobalMagField::Instance()->Field(xyz,h); | |
1025 | ||
1026 | h2xy = h[0]*h[0] + h[1]*h[1]; | |
1027 | h[3] = h[2]*h[2]+ h2xy; | |
1028 | if (h[3] < 1.e-12) { | |
1029 | for (Int_t i = 0; i < 3; i++) { | |
1030 | vout[i] = vect[i] + step * vect[i+3]; | |
1031 | vout[i+3] = vect[i+3]; | |
1032 | } | |
1033 | return; | |
1034 | } | |
1035 | if (h2xy < 1.e-12*h[3]) { | |
1036 | ExtrapOneStepHelix3(charge*h[2], step, vect, vout); | |
1037 | return; | |
1038 | } | |
1039 | h[3] = TMath::Sqrt(h[3]); | |
1040 | h[0] /= h[3]; | |
1041 | h[1] /= h[3]; | |
1042 | h[2] /= h[3]; | |
1043 | h[3] *= kec; | |
1044 | ||
1045 | hxp[0] = h[1]*vect[kipz] - h[2]*vect[kipy]; | |
1046 | hxp[1] = h[2]*vect[kipx] - h[0]*vect[kipz]; | |
1047 | hxp[2] = h[0]*vect[kipy] - h[1]*vect[kipx]; | |
1048 | ||
1049 | hp = h[0]*vect[kipx] + h[1]*vect[kipy] + h[2]*vect[kipz]; | |
1050 | ||
1051 | rho = -charge*h[3]/vect[kipp]; | |
1052 | tet = rho * step; | |
1053 | ||
1054 | if (TMath::Abs(tet) > 0.15) { | |
1055 | sint = TMath::Sin(tet); | |
1056 | sintt = (sint/tet); | |
1057 | tsint = (tet-sint)/tet; | |
1058 | cos1t = 2.*(TMath::Sin(0.5*tet))*(TMath::Sin(0.5*tet))/tet; | |
1059 | } else { | |
1060 | tsint = tet*tet/36.; | |
1061 | sintt = (1. - tsint); | |
1062 | sint = tet*sintt; | |
1063 | cos1t = 0.5*tet; | |
1064 | } | |
1065 | ||
1066 | f1 = step * sintt; | |
1067 | f2 = step * cos1t; | |
1068 | f3 = step * tsint * hp; | |
1069 | f4 = -tet*cos1t; | |
1070 | f5 = sint; | |
1071 | f6 = tet * cos1t * hp; | |
1072 | ||
1073 | vout[kix] = vect[kix] + f1*vect[kipx] + f2*hxp[0] + f3*h[0]; | |
1074 | vout[kiy] = vect[kiy] + f1*vect[kipy] + f2*hxp[1] + f3*h[1]; | |
1075 | vout[kiz] = vect[kiz] + f1*vect[kipz] + f2*hxp[2] + f3*h[2]; | |
1076 | ||
1077 | vout[kipx] = vect[kipx] + f4*vect[kipx] + f5*hxp[0] + f6*h[0]; | |
1078 | vout[kipy] = vect[kipy] + f4*vect[kipy] + f5*hxp[1] + f6*h[1]; | |
1079 | vout[kipz] = vect[kipz] + f4*vect[kipz] + f5*hxp[2] + f6*h[2]; | |
1080 | ||
1081 | return; | |
1082 | } | |
1083 | ||
1084 | //__________________________________________________________________________ | |
1085 | void AliMUONTrackExtrap::ExtrapOneStepHelix3(Double_t field, Double_t step, Double_t *vect, Double_t *vout) | |
1086 | { | |
1087 | /// <pre> | |
1088 | /// ****************************************************************** | |
1089 | /// * * | |
1090 | /// * Tracking routine in a constant field oriented * | |
1091 | /// * along axis 3 * | |
1092 | /// * Tracking is performed with a conventional * | |
1093 | /// * helix step method * | |
1094 | /// * * | |
1095 | /// * ==>Called by : USER, GUSWIM * | |
1096 | /// * Authors R.Brun, M.Hansroul ********* * | |
1097 | /// * Rewritten V.Perevoztchikov | |
1098 | /// * * | |
1099 | /// ****************************************************************** | |
1100 | /// </pre> | |
1101 | ||
1102 | Double_t hxp[3]; | |
1103 | Double_t h4, hp, rho, tet; | |
1104 | Double_t sint, sintt, tsint, cos1t; | |
1105 | Double_t f1, f2, f3, f4, f5, f6; | |
1106 | ||
1107 | const Int_t kix = 0; | |
1108 | const Int_t kiy = 1; | |
1109 | const Int_t kiz = 2; | |
1110 | const Int_t kipx = 3; | |
1111 | const Int_t kipy = 4; | |
1112 | const Int_t kipz = 5; | |
1113 | const Int_t kipp = 6; | |
1114 | ||
1115 | const Double_t kec = 2.9979251e-4; | |
1116 | ||
1117 | // | |
1118 | // ------------------------------------------------------------------ | |
1119 | // | |
1120 | // units are kgauss,centimeters,gev/c | |
1121 | // | |
1122 | vout[kipp] = vect[kipp]; | |
1123 | h4 = field * kec; | |
1124 | ||
1125 | hxp[0] = - vect[kipy]; | |
1126 | hxp[1] = + vect[kipx]; | |
1127 | ||
1128 | hp = vect[kipz]; | |
1129 | ||
1130 | rho = -h4/vect[kipp]; | |
1131 | tet = rho * step; | |
1132 | if (TMath::Abs(tet) > 0.15) { | |
1133 | sint = TMath::Sin(tet); | |
1134 | sintt = (sint/tet); | |
1135 | tsint = (tet-sint)/tet; | |
1136 | cos1t = 2.* TMath::Sin(0.5*tet) * TMath::Sin(0.5*tet)/tet; | |
1137 | } else { | |
1138 | tsint = tet*tet/36.; | |
1139 | sintt = (1. - tsint); | |
1140 | sint = tet*sintt; | |
1141 | cos1t = 0.5*tet; | |
1142 | } | |
1143 | ||
1144 | f1 = step * sintt; | |
1145 | f2 = step * cos1t; | |
1146 | f3 = step * tsint * hp; | |
1147 | f4 = -tet*cos1t; | |
1148 | f5 = sint; | |
1149 | f6 = tet * cos1t * hp; | |
1150 | ||
1151 | vout[kix] = vect[kix] + f1*vect[kipx] + f2*hxp[0]; | |
1152 | vout[kiy] = vect[kiy] + f1*vect[kipy] + f2*hxp[1]; | |
1153 | vout[kiz] = vect[kiz] + f1*vect[kipz] + f3; | |
1154 | ||
1155 | vout[kipx] = vect[kipx] + f4*vect[kipx] + f5*hxp[0]; | |
1156 | vout[kipy] = vect[kipy] + f4*vect[kipy] + f5*hxp[1]; | |
1157 | vout[kipz] = vect[kipz] + f4*vect[kipz] + f6; | |
1158 | ||
1159 | return; | |
1160 | } | |
1161 | ||
1162 | //__________________________________________________________________________ | |
1163 | void AliMUONTrackExtrap::ExtrapOneStepRungekutta(Double_t charge, Double_t step, Double_t* vect, Double_t* vout) | |
1164 | { | |
1165 | /// <pre> | |
1166 | /// ****************************************************************** | |
1167 | /// * * | |
1168 | /// * Runge-Kutta method for tracking a particle through a magnetic * | |
1169 | /// * field. Uses Nystroem algorithm (See Handbook Nat. Bur. of * | |
1170 | /// * Standards, procedure 25.5.20) * | |
1171 | /// * * | |
1172 | /// * Input parameters * | |
1173 | /// * CHARGE Particle charge * | |
1174 | /// * STEP Step size * | |
1175 | /// * VECT Initial co-ords,direction cosines,momentum * | |
1176 | /// * Output parameters * | |
1177 | /// * VOUT Output co-ords,direction cosines,momentum * | |
1178 | /// * User routine called * | |
1179 | /// * CALL GUFLD(X,F) * | |
1180 | /// * * | |
1181 | /// * ==>Called by : USER, GUSWIM * | |
1182 | /// * Authors R.Brun, M.Hansroul ********* * | |
1183 | /// * V.Perevoztchikov (CUT STEP implementation) * | |
1184 | /// * * | |
1185 | /// * * | |
1186 | /// ****************************************************************** | |
1187 | /// </pre> | |
1188 | ||
1189 | Double_t h2, h4, f[4]; | |
1190 | Double_t xyzt[3], a, b, c, ph,ph2; | |
1191 | Double_t secxs[4],secys[4],seczs[4],hxp[3]; | |
1192 | Double_t g1, g2, g3, g4, g5, g6, ang2, dxt, dyt, dzt; | |
1193 | Double_t est, at, bt, ct, cba; | |
1194 | Double_t f1, f2, f3, f4, rho, tet, hnorm, hp, rho1, sint, cost; | |
1195 | ||
1196 | Double_t x; | |
1197 | Double_t y; | |
1198 | Double_t z; | |
1199 | ||
1200 | Double_t xt; | |
1201 | Double_t yt; | |
1202 | Double_t zt; | |
1203 | ||
1204 | Double_t maxit = 1992; | |
1205 | Double_t maxcut = 11; | |
1206 | ||
1207 | const Double_t kdlt = 1e-4; | |
1208 | const Double_t kdlt32 = kdlt/32.; | |
1209 | const Double_t kthird = 1./3.; | |
1210 | const Double_t khalf = 0.5; | |
1211 | const Double_t kec = 2.9979251e-4; | |
1212 | ||
1213 | const Double_t kpisqua = 9.86960440109; | |
1214 | const Int_t kix = 0; | |
1215 | const Int_t kiy = 1; | |
1216 | const Int_t kiz = 2; | |
1217 | const Int_t kipx = 3; | |
1218 | const Int_t kipy = 4; | |
1219 | const Int_t kipz = 5; | |
1220 | ||
1221 | // *. | |
1222 | // *. ------------------------------------------------------------------ | |
1223 | // *. | |
1224 | // * this constant is for units cm,gev/c and kgauss | |
1225 | // * | |
1226 | Int_t iter = 0; | |
1227 | Int_t ncut = 0; | |
1228 | for(Int_t j = 0; j < 7; j++) | |
1229 | vout[j] = vect[j]; | |
1230 | ||
1231 | Double_t pinv = kec * charge / vect[6]; | |
1232 | Double_t tl = 0.; | |
1233 | Double_t h = step; | |
1234 | Double_t rest; | |
1235 | ||
1236 | ||
1237 | do { | |
1238 | rest = step - tl; | |
1239 | if (TMath::Abs(h) > TMath::Abs(rest)) h = rest; | |
1240 | //cmodif: call gufld(vout,f) changed into: | |
1241 | TGeoGlobalMagField::Instance()->Field(vout,f); | |
1242 | ||
1243 | // * | |
1244 | // * start of integration | |
1245 | // * | |
1246 | x = vout[0]; | |
1247 | y = vout[1]; | |
1248 | z = vout[2]; | |
1249 | a = vout[3]; | |
1250 | b = vout[4]; | |
1251 | c = vout[5]; | |
1252 | ||
1253 | h2 = khalf * h; | |
1254 | h4 = khalf * h2; | |
1255 | ph = pinv * h; | |
1256 | ph2 = khalf * ph; | |
1257 | secxs[0] = (b * f[2] - c * f[1]) * ph2; | |
1258 | secys[0] = (c * f[0] - a * f[2]) * ph2; | |
1259 | seczs[0] = (a * f[1] - b * f[0]) * ph2; | |
1260 | ang2 = (secxs[0]*secxs[0] + secys[0]*secys[0] + seczs[0]*seczs[0]); | |
1261 | if (ang2 > kpisqua) break; | |
1262 | ||
1263 | dxt = h2 * a + h4 * secxs[0]; | |
1264 | dyt = h2 * b + h4 * secys[0]; | |
1265 | dzt = h2 * c + h4 * seczs[0]; | |
1266 | xt = x + dxt; | |
1267 | yt = y + dyt; | |
1268 | zt = z + dzt; | |
1269 | // * | |
1270 | // * second intermediate point | |
1271 | // * | |
1272 | ||
1273 | est = TMath::Abs(dxt) + TMath::Abs(dyt) + TMath::Abs(dzt); | |
1274 | if (est > h) { | |
1275 | if (ncut++ > maxcut) break; | |
1276 | h *= khalf; | |
1277 | continue; | |
1278 | } | |
1279 | ||
1280 | xyzt[0] = xt; | |
1281 | xyzt[1] = yt; | |
1282 | xyzt[2] = zt; | |
1283 | ||
1284 | //cmodif: call gufld(xyzt,f) changed into: | |
1285 | TGeoGlobalMagField::Instance()->Field(xyzt,f); | |
1286 | ||
1287 | at = a + secxs[0]; | |
1288 | bt = b + secys[0]; | |
1289 | ct = c + seczs[0]; | |
1290 | ||
1291 | secxs[1] = (bt * f[2] - ct * f[1]) * ph2; | |
1292 | secys[1] = (ct * f[0] - at * f[2]) * ph2; | |
1293 | seczs[1] = (at * f[1] - bt * f[0]) * ph2; | |
1294 | at = a + secxs[1]; | |
1295 | bt = b + secys[1]; | |
1296 | ct = c + seczs[1]; | |
1297 | secxs[2] = (bt * f[2] - ct * f[1]) * ph2; | |
1298 | secys[2] = (ct * f[0] - at * f[2]) * ph2; | |
1299 | seczs[2] = (at * f[1] - bt * f[0]) * ph2; | |
1300 | dxt = h * (a + secxs[2]); | |
1301 | dyt = h * (b + secys[2]); | |
1302 | dzt = h * (c + seczs[2]); | |
1303 | xt = x + dxt; | |
1304 | yt = y + dyt; | |
1305 | zt = z + dzt; | |
1306 | at = a + 2.*secxs[2]; | |
1307 | bt = b + 2.*secys[2]; | |
1308 | ct = c + 2.*seczs[2]; | |
1309 | ||
1310 | est = TMath::Abs(dxt)+TMath::Abs(dyt)+TMath::Abs(dzt); | |
1311 | if (est > 2.*TMath::Abs(h)) { | |
1312 | if (ncut++ > maxcut) break; | |
1313 | h *= khalf; | |
1314 | continue; | |
1315 | } | |
1316 | ||
1317 | xyzt[0] = xt; | |
1318 | xyzt[1] = yt; | |
1319 | xyzt[2] = zt; | |
1320 | ||
1321 | //cmodif: call gufld(xyzt,f) changed into: | |
1322 | TGeoGlobalMagField::Instance()->Field(xyzt,f); | |
1323 | ||
1324 | z = z + (c + (seczs[0] + seczs[1] + seczs[2]) * kthird) * h; | |
1325 | y = y + (b + (secys[0] + secys[1] + secys[2]) * kthird) * h; | |
1326 | x = x + (a + (secxs[0] + secxs[1] + secxs[2]) * kthird) * h; | |
1327 | ||
1328 | secxs[3] = (bt*f[2] - ct*f[1])* ph2; | |
1329 | secys[3] = (ct*f[0] - at*f[2])* ph2; | |
1330 | seczs[3] = (at*f[1] - bt*f[0])* ph2; | |
1331 | a = a+(secxs[0]+secxs[3]+2. * (secxs[1]+secxs[2])) * kthird; | |
1332 | b = b+(secys[0]+secys[3]+2. * (secys[1]+secys[2])) * kthird; | |
1333 | c = c+(seczs[0]+seczs[3]+2. * (seczs[1]+seczs[2])) * kthird; | |
1334 | ||
1335 | est = TMath::Abs(secxs[0]+secxs[3] - (secxs[1]+secxs[2])) | |
1336 | + TMath::Abs(secys[0]+secys[3] - (secys[1]+secys[2])) | |
1337 | + TMath::Abs(seczs[0]+seczs[3] - (seczs[1]+seczs[2])); | |
1338 | ||
1339 | if (est > kdlt && TMath::Abs(h) > 1.e-4) { | |
1340 | if (ncut++ > maxcut) break; | |
1341 | h *= khalf; | |
1342 | continue; | |
1343 | } | |
1344 | ||
1345 | ncut = 0; | |
1346 | // * if too many iterations, go to helix | |
1347 | if (iter++ > maxit) break; | |
1348 | ||
1349 | tl += h; | |
1350 | if (est < kdlt32) | |
1351 | h *= 2.; | |
1352 | cba = 1./ TMath::Sqrt(a*a + b*b + c*c); | |
1353 | vout[0] = x; | |
1354 | vout[1] = y; | |
1355 | vout[2] = z; | |
1356 | vout[3] = cba*a; | |
1357 | vout[4] = cba*b; | |
1358 | vout[5] = cba*c; | |
1359 | rest = step - tl; | |
1360 | if (step < 0.) rest = -rest; | |
1361 | if (rest < 1.e-5*TMath::Abs(step)) return; | |
1362 | ||
1363 | } while(1); | |
1364 | ||
1365 | // angle too big, use helix | |
1366 | ||
1367 | f1 = f[0]; | |
1368 | f2 = f[1]; | |
1369 | f3 = f[2]; | |
1370 | f4 = TMath::Sqrt(f1*f1+f2*f2+f3*f3); | |
1371 | rho = -f4*pinv; | |
1372 | tet = rho * step; | |
1373 | ||
1374 | hnorm = 1./f4; | |
1375 | f1 = f1*hnorm; | |
1376 | f2 = f2*hnorm; | |
1377 | f3 = f3*hnorm; | |
1378 | ||
1379 | hxp[0] = f2*vect[kipz] - f3*vect[kipy]; | |
1380 | hxp[1] = f3*vect[kipx] - f1*vect[kipz]; | |
1381 | hxp[2] = f1*vect[kipy] - f2*vect[kipx]; | |
1382 | ||
1383 | hp = f1*vect[kipx] + f2*vect[kipy] + f3*vect[kipz]; | |
1384 | ||
1385 | rho1 = 1./rho; | |
1386 | sint = TMath::Sin(tet); | |
1387 | cost = 2.*TMath::Sin(khalf*tet)*TMath::Sin(khalf*tet); | |
1388 | ||
1389 | g1 = sint*rho1; | |
1390 | g2 = cost*rho1; | |
1391 | g3 = (tet-sint) * hp*rho1; | |
1392 | g4 = -cost; | |
1393 | g5 = sint; | |
1394 | g6 = cost * hp; | |
1395 | ||
1396 | vout[kix] = vect[kix] + g1*vect[kipx] + g2*hxp[0] + g3*f1; | |
1397 | vout[kiy] = vect[kiy] + g1*vect[kipy] + g2*hxp[1] + g3*f2; | |
1398 | vout[kiz] = vect[kiz] + g1*vect[kipz] + g2*hxp[2] + g3*f3; | |
1399 | ||
1400 | vout[kipx] = vect[kipx] + g4*vect[kipx] + g5*hxp[0] + g6*f1; | |
1401 | vout[kipy] = vect[kipy] + g4*vect[kipy] + g5*hxp[1] + g6*f2; | |
1402 | vout[kipz] = vect[kipz] + g4*vect[kipz] + g5*hxp[2] + g6*f3; | |
1403 | ||
1404 | return; | |
1405 | } | |
1406 |