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cc3e558a | 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 | ||
b4caed64 | 16 | // _________________________________________________________________ |
17 | // | |
18 | // Begin_Html | |
19 | // <h2> AliTPCSpaceCharge3D class </h2> | |
20 | // The class calculates the space point distortions due to an arbitrary space | |
21 | // charge distribution in 3D. | |
22 | // <p> | |
23 | // The method of calculation is based on the analytical solution for the Poisson | |
24 | // problem in 3D (cylindrical coordinates). The solution is used in form of | |
25 | // look up tables, where the pre calculated solutions for different voxel | |
26 | // positions are stored. These voxel solutions can be summed up according | |
27 | // to the weight of the position of the applied space charge distribution. | |
28 | // Further details can be found in \cite[chap.5]{PhD-thesis_S.Rossegger}. | |
29 | // <p> | |
30 | // The class also allows a simple scaling of the resulting distortions | |
31 | // via the function SetCorrectionFactor. This speeds up the calculation | |
32 | // time under the assumption, that the distortions scales linearly with the | |
33 | // magnitude of the space charge distribution $\rho(r,z)$ and the shape stays | |
34 | // the same at higher luminosities. | |
35 | // <p> | |
36 | // In contrast to the implementation in 2D (see the class AliTPCSpaceChargeabove), | |
37 | // the input charge distribution can be of arbitrary character. An example on how | |
38 | // to produce a corresponding charge distribution can be found in the function | |
39 | // WriteChargeDistributionToFile. In there, a $\rho(r,z) = (A-B\,z)/r^2$, | |
40 | // with slightly different magnitude on the A and C side (due to the muon absorber), | |
41 | // is superpositioned with a few leaking wires at arbitrary positions. | |
92a85338 | 42 | // |
43 | // | |
44 | // Marian Ivanov change: 26.06.2013 | |
45 | // Usage of the realy 3D space charge map as an optional input | |
46 | // SetInputSpaceCharge map. | |
47 | // In case given map is used 2 2D maps are ignored and scaling functions $\rho(r,z) = (A-B\,z)/r^2$, | |
48 | // will not work | |
49 | // | |
50 | ||
51 | ||
b4caed64 | 52 | // End_Html |
53 | // | |
6a1caa6b | 54 | // Begin_Macro(source) |
b4caed64 | 55 | // { |
56 | // gROOT->SetStyle("Plain"); gStyle->SetPalette(1); | |
6a1caa6b | 57 | // TCanvas *c2 = new TCanvas("cAliTPCSpaceCharge3D","cAliTPCSpaceCharge3D",500,400); |
b4caed64 | 58 | // AliTPCSpaceCharge3D sc; |
59 | // sc.WriteChargeDistributionToFile("SC_zr2_GGleaks.root"); | |
60 | // sc.SetSCDataFileName("SC_zr2_GGleaks.root"); | |
61 | // sc.SetOmegaTauT1T2(0,1,1); // B=0 | |
62 | // sc.InitSpaceCharge3DDistortion(); | |
63 | // sc.CreateHistoDRinXY(15,300,300)->Draw("colz"); | |
64 | // return c2; | |
65 | // } | |
66 | // End_Macro | |
67 | // | |
68 | // Begin_Html | |
69 | // <p> | |
70 | // Date: 19/06/2010 <br> | |
71 | // Authors: Stefan Rossegger | |
72 | // End_Html | |
73 | // _________________________________________________________________ | |
74 | ||
cc3e558a | 75 | |
76 | #include "AliMagF.h" | |
77 | #include "TGeoGlobalMagField.h" | |
78 | #include "AliTPCcalibDB.h" | |
79 | #include "AliTPCParam.h" | |
80 | #include "AliLog.h" | |
81 | #include "TH2F.h" | |
82 | #include "TH3F.h" | |
83 | #include "TFile.h" | |
84 | #include "TVector.h" | |
85 | #include "TMatrix.h" | |
86 | #include "TMatrixD.h" | |
87 | ||
88 | #include "TMath.h" | |
89 | #include "AliTPCROC.h" | |
90 | #include "AliTPCSpaceCharge3D.h" | |
92a85338 | 91 | #include "AliSysInfo.h" |
cc3e558a | 92 | |
93 | ClassImp(AliTPCSpaceCharge3D) | |
94 | ||
95 | AliTPCSpaceCharge3D::AliTPCSpaceCharge3D() | |
96 | : AliTPCCorrection("SpaceCharge3D","Space Charge - 3D"), | |
97 | fC0(0.),fC1(0.), | |
98 | fCorrectionFactor(1.), | |
99 | fInitLookUp(kFALSE), | |
15687d71 | 100 | fSCDataFileName(""), |
101 | fSCLookUpPOCsFileName3D(""), | |
102 | fSCLookUpPOCsFileNameRZ(""), | |
103 | fSCLookUpPOCsFileNameRPhi(""), | |
104 | fSCdensityInRZ(0), | |
752b0cc7 | 105 | fSCdensityInRPhiA(0), |
92a85338 | 106 | fSCdensityInRPhiC(0), |
107 | fSpaceChargeHistogram3D(0), | |
108 | fSpaceChargeHistogramRPhi(0), | |
109 | fSpaceChargeHistogramRZ(0) | |
cc3e558a | 110 | { |
111 | // | |
112 | // default constructor | |
113 | // | |
114 | ||
115 | // Array which will contain the solution according to the setted charge density distribution | |
116 | // see InitSpaceCharge3DDistortion() function | |
117 | for ( Int_t k = 0 ; k < kNPhi ; k++ ) { | |
2bf29b72 | 118 | fLookUpErOverEz[k] = new TMatrixF(kNR,kNZ); |
119 | fLookUpEphiOverEz[k] = new TMatrixF(kNR,kNZ); | |
120 | fLookUpDeltaEz[k] = new TMatrixF(kNR,kNZ); | |
121 | fSCdensityDistribution[k] = new TMatrixF(kNR,kNZ); | |
cc3e558a | 122 | } |
15687d71 | 123 | fSCdensityInRZ = new TMatrixD(kNR,kNZ); |
124 | fSCdensityInRPhiA = new TMatrixD(kNR,kNPhi); | |
125 | fSCdensityInRPhiC = new TMatrixD(kNR,kNPhi); | |
126 | ||
127 | // location of the precalculated look up tables | |
128 | ||
129 | fSCLookUpPOCsFileName3D="$(ALICE_ROOT)/TPC/Calib/maps/sc_3D_raw_18-18-26_17p-18p-25p-MN30.root"; // rough estimate | |
130 | fSCLookUpPOCsFileNameRZ="$(ALICE_ROOT)/TPC/Calib/maps/sc_radSym_35-01-51_34p-01p-50p_MN60.root"; | |
752b0cc7 | 131 | fSCLookUpPOCsFileNameRPhi="$(ALICE_ROOT)/TPC/Calib/maps/sc_cChInZ_35-144-26_34p-18p-01p-MN30.root"; |
132 | // fSCLookUpPOCsFileNameRPhi="$(ALICE_ROOT)/TPC/Calib/maps/sc_cChInZ_35-36-26_34p-18p-01p-MN40.root"; | |
133 | ||
15687d71 | 134 | |
135 | ||
136 | // standard location of the space charge distibution ... can be changes | |
137 | fSCDataFileName="$(ALICE_ROOT)/TPC/Calib/maps/sc_3D_distribution_Sim.root"; | |
138 | ||
139 | // SetSCDataFileName(fSCDataFileName.Data()); // should be done by the user | |
cc3e558a | 140 | |
cc3e558a | 141 | |
142 | } | |
143 | ||
144 | AliTPCSpaceCharge3D::~AliTPCSpaceCharge3D() { | |
145 | // | |
146 | // default destructor | |
147 | // | |
148 | ||
149 | for ( Int_t k = 0 ; k < kNPhi ; k++ ) { | |
150 | delete fLookUpErOverEz[k]; | |
151 | delete fLookUpEphiOverEz[k]; | |
152 | delete fLookUpDeltaEz[k]; | |
153 | delete fSCdensityDistribution[k]; | |
154 | } | |
15687d71 | 155 | delete fSCdensityInRZ; |
156 | delete fSCdensityInRPhiA; | |
157 | delete fSCdensityInRPhiC; | |
92a85338 | 158 | delete fSpaceChargeHistogram3D; |
159 | delete fSpaceChargeHistogramRPhi; | |
160 | delete fSpaceChargeHistogramRZ; | |
cc3e558a | 161 | } |
162 | ||
163 | ||
cc3e558a | 164 | void AliTPCSpaceCharge3D::Init() { |
165 | // | |
166 | // Initialization funtion | |
167 | // | |
168 | ||
169 | AliMagF* magF= (AliMagF*)TGeoGlobalMagField::Instance()->GetField(); | |
170 | if (!magF) AliError("Magneticd field - not initialized"); | |
171 | Double_t bzField = magF->SolenoidField()/10.; //field in T | |
172 | AliTPCParam *param= AliTPCcalibDB::Instance()->GetParameters(); | |
173 | if (!param) AliError("Parameters - not initialized"); | |
174 | Double_t vdrift = param->GetDriftV()/1000000.; // [cm/us] // From dataBase: to be updated: per second (ideally) | |
175 | Double_t ezField = 400; // [V/cm] // to be updated: never (hopefully) | |
176 | Double_t wt = -10.0 * (bzField*10) * vdrift / ezField ; | |
177 | // Correction Terms for effective omegaTau; obtained by a laser calibration run | |
178 | SetOmegaTauT1T2(wt,fT1,fT2); | |
179 | ||
180 | InitSpaceCharge3DDistortion(); // fill the look up table | |
181 | } | |
182 | ||
183 | void AliTPCSpaceCharge3D::Update(const TTimeStamp &/*timeStamp*/) { | |
184 | // | |
185 | // Update function | |
186 | // | |
187 | AliMagF* magF= (AliMagF*)TGeoGlobalMagField::Instance()->GetField(); | |
188 | if (!magF) AliError("Magneticd field - not initialized"); | |
189 | Double_t bzField = magF->SolenoidField()/10.; //field in T | |
190 | AliTPCParam *param= AliTPCcalibDB::Instance()->GetParameters(); | |
191 | if (!param) AliError("Parameters - not initialized"); | |
192 | Double_t vdrift = param->GetDriftV()/1000000.; // [cm/us] // From dataBase: to be updated: per second (ideally) | |
193 | Double_t ezField = 400; // [V/cm] // to be updated: never (hopefully) | |
194 | Double_t wt = -10.0 * (bzField*10) * vdrift / ezField ; | |
195 | // Correction Terms for effective omegaTau; obtained by a laser calibration run | |
196 | SetOmegaTauT1T2(wt,fT1,fT2); | |
197 | ||
198 | // SetCorrectionFactor(1.); // should come from some database | |
199 | ||
200 | } | |
201 | ||
202 | ||
cc3e558a | 203 | void AliTPCSpaceCharge3D::GetCorrection(const Float_t x[],const Short_t roc,Float_t dx[]) { |
204 | // | |
205 | // Calculates the correction due the Space Charge effect within the TPC drift volume | |
206 | // | |
207 | ||
208 | if (!fInitLookUp) { | |
209 | AliInfo("Lookup table was not initialized! Performing the inizialisation now ..."); | |
210 | InitSpaceCharge3DDistortion(); | |
211 | } | |
212 | ||
213 | Int_t order = 1 ; // FIXME: hardcoded? Linear interpolation = 1, Quadratic = 2 | |
214 | ||
2bf29b72 | 215 | Float_t intEr, intEphi, intdEz ; |
cc3e558a | 216 | Double_t r, phi, z ; |
217 | Int_t sign; | |
218 | ||
219 | r = TMath::Sqrt( x[0]*x[0] + x[1]*x[1] ) ; | |
220 | phi = TMath::ATan2(x[1],x[0]) ; | |
221 | if ( phi < 0 ) phi += TMath::TwoPi() ; // Table uses phi from 0 to 2*Pi | |
222 | z = x[2] ; // Create temporary copy of x[2] | |
223 | ||
224 | if ( (roc%36) < 18 ) { | |
225 | sign = 1; // (TPC A side) | |
226 | } else { | |
227 | sign = -1; // (TPC C side) | |
228 | } | |
229 | ||
230 | if ( sign==1 && z < fgkZOffSet ) z = fgkZOffSet; // Protect against discontinuity at CE | |
231 | if ( sign==-1 && z > -fgkZOffSet ) z = -fgkZOffSet; // Protect against discontinuity at CE | |
232 | ||
233 | ||
234 | if ( (sign==1 && z<0) || (sign==-1 && z>0) ) // just a consistency check | |
235 | AliError("ROC number does not correspond to z coordinate! Calculation of distortions is most likely wrong!"); | |
236 | ||
237 | // Get the Er and Ephi field integrals plus the integral over DeltaEz | |
238 | intEr = Interpolate3DTable(order, r, z, phi, kNR, kNZ, kNPhi, | |
239 | fgkRList, fgkZList, fgkPhiList, fLookUpErOverEz ); | |
240 | intEphi = Interpolate3DTable(order, r, z, phi, kNR, kNZ, kNPhi, | |
241 | fgkRList, fgkZList, fgkPhiList, fLookUpEphiOverEz); | |
242 | intdEz = Interpolate3DTable(order, r, z, phi, kNR, kNZ, kNPhi, | |
243 | fgkRList, fgkZList, fgkPhiList, fLookUpDeltaEz ); | |
244 | ||
245 | // Calculate distorted position | |
246 | if ( r > 0.0 ) { | |
247 | phi = phi + fCorrectionFactor *( fC0*intEphi - fC1*intEr ) / r; | |
248 | r = r + fCorrectionFactor *( fC0*intEr + fC1*intEphi ); | |
249 | } | |
250 | Double_t dz = intdEz * fCorrectionFactor * fgkdvdE; | |
251 | ||
252 | // Calculate correction in cartesian coordinates | |
752b0cc7 | 253 | dx[0] = - (r * TMath::Cos(phi) - x[0]); |
254 | dx[1] = - (r * TMath::Sin(phi) - x[1]); | |
255 | dx[2] = - dz; // z distortion - (scaled with driftvelocity dependency on the Ez field and the overall scaling factor) | |
cc3e558a | 256 | |
257 | } | |
258 | ||
cc3e558a | 259 | void AliTPCSpaceCharge3D::InitSpaceCharge3DDistortion() { |
15687d71 | 260 | // |
261 | // Initialization of the Lookup table which contains the solutions of the | |
262 | // "space charge" (poisson) problem - Faster and more accureate | |
263 | // | |
264 | // Method: Weighted sum-up of the different fields within the look up table | |
265 | // but using two lookup tables with higher granularity in the (r,z) and the (rphi)- plane to emulate | |
266 | // more realistic space charges. (r,z) from primary ionisation. (rphi) for possible Gating leaks | |
267 | ||
268 | if (fInitLookUp) { | |
269 | AliInfo("Lookup table was already initialized! Doing it again anyway ..."); | |
db59c7fb | 270 | return; |
15687d71 | 271 | } |
272 | ||
273 | // ------------------------------------------------------------------------------------------------------ | |
274 | // step 1: lookup table in rz, fine grid, radial symetric, to emulate primary ionization | |
275 | ||
276 | AliInfo("Step 1: Preparation of the weighted look-up tables."); | |
277 | ||
278 | // lookup table in rz, fine grid | |
279 | ||
280 | TFile *fZR = new TFile(fSCLookUpPOCsFileNameRZ.Data(),"READ"); | |
281 | if ( !fZR ) { | |
282 | AliError("Precalculated POC-looup-table in ZR could not be found"); | |
283 | return; | |
284 | } | |
285 | ||
286 | // units are in [m] | |
287 | TVector *gridf1 = (TVector*) fZR->Get("constants"); | |
288 | TVector &grid1 = *gridf1; | |
289 | TMatrix *coordf1 = (TMatrix*) fZR->Get("coordinates"); | |
290 | TMatrix &coord1 = *coordf1; | |
291 | TMatrix *coordPOCf1 = (TMatrix*) fZR->Get("POCcoord"); | |
292 | TMatrix &coordPOC1 = *coordPOCf1; | |
293 | ||
294 | Int_t rows = (Int_t)grid1(0); // number of points in r direction - from RZ or RPhi table | |
295 | Int_t phiSlices = (Int_t)grid1(1); // number of points in phi - from RPhi table | |
296 | Int_t columns = (Int_t)grid1(2); // number of points in z direction - from RZ table | |
297 | ||
298 | Float_t gridSizeR = (fgkOFCRadius-fgkIFCRadius)/(rows-1); // unit in [cm] | |
299 | Float_t gridSizeZ = fgkTPCZ0/(columns-1); // unit in [cm] | |
300 | ||
301 | // temporary matrices needed for the calculation // for rotational symmetric RZ table, phislices is 1 | |
9f3b99e2 | 302 | |
303 | TMatrixD *arrayofErA[kNPhiSlices], *arrayofdEzA[kNPhiSlices]; | |
304 | TMatrixD *arrayofErC[kNPhiSlices], *arrayofdEzC[kNPhiSlices]; | |
15687d71 | 305 | |
9f3b99e2 | 306 | TMatrixD *arrayofEroverEzA[kNPhiSlices], *arrayofDeltaEzA[kNPhiSlices]; |
307 | TMatrixD *arrayofEroverEzC[kNPhiSlices], *arrayofDeltaEzC[kNPhiSlices]; | |
15687d71 | 308 | |
309 | ||
310 | for ( Int_t k = 0 ; k < phiSlices ; k++ ) { | |
311 | ||
312 | arrayofErA[k] = new TMatrixD(rows,columns) ; | |
313 | arrayofdEzA[k] = new TMatrixD(rows,columns) ; | |
314 | arrayofErC[k] = new TMatrixD(rows,columns) ; | |
315 | arrayofdEzC[k] = new TMatrixD(rows,columns) ; | |
316 | ||
317 | arrayofEroverEzA[k] = new TMatrixD(rows,columns) ; | |
318 | arrayofDeltaEzA[k] = new TMatrixD(rows,columns) ; | |
319 | arrayofEroverEzC[k] = new TMatrixD(rows,columns) ; | |
320 | arrayofDeltaEzC[k] = new TMatrixD(rows,columns) ; | |
321 | ||
322 | // zero initialization not necessary, it is done in the constructor of TMatrix | |
323 | ||
324 | } | |
325 | ||
326 | // list of points as used during sum up | |
9f3b99e2 | 327 | Double_t rlist1[kNRows], zedlist1[kNColumns];// , philist1[phiSlices]; |
15687d71 | 328 | for ( Int_t i = 0 ; i < rows ; i++ ) { |
329 | rlist1[i] = fgkIFCRadius + i*gridSizeR ; | |
330 | for ( Int_t j = 0 ; j < columns ; j++ ) { | |
331 | zedlist1[j] = j * gridSizeZ ; | |
332 | } | |
333 | } | |
334 | ||
335 | TTree *treePOC = (TTree*)fZR->Get("POCall"); | |
336 | ||
337 | TVector *bEr = 0; //TVector *bEphi= 0; | |
338 | TVector *bEz = 0; | |
339 | ||
340 | treePOC->SetBranchAddress("Er",&bEr); | |
341 | treePOC->SetBranchAddress("Ez",&bEz); | |
342 | ||
343 | ||
344 | // Read the complete tree and do a weighted sum-up over the POC configurations | |
345 | // +++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ | |
346 | ||
347 | Int_t treeNumPOC = (Int_t)treePOC->GetEntries(); // Number of POC conf. in the look-up table | |
348 | Int_t ipC = 0; // POC Conf. counter (note: different to the POC number in the tree!) | |
349 | ||
350 | for (Int_t itreepC=0; itreepC<treeNumPOC; itreepC++) { // ------------- loop over POC configurations in tree | |
351 | ||
352 | treePOC->GetEntry(itreepC); | |
353 | ||
354 | // center of the POC voxel in [meter] | |
355 | Double_t r0 = coordPOC1(ipC,0); | |
356 | Double_t phi0 = coordPOC1(ipC,1); | |
357 | Double_t z0 = coordPOC1(ipC,2); | |
358 | ||
359 | ipC++; // POC configuration counter | |
360 | ||
361 | // weights (charge density) at POC position on the A and C side (in C/m^3/e0) | |
362 | // note: coordinates are in [cm] | |
363 | Double_t weightA = GetSpaceChargeDensity(r0*100,phi0, z0*100, 1); // partial load in r,z | |
364 | Double_t weightC = GetSpaceChargeDensity(r0*100,phi0,-z0*100, 1); // partial load in r,z | |
365 | ||
366 | // Summing up the vector components according to their weight | |
367 | ||
368 | Int_t ip = 0; | |
369 | for ( Int_t j = 0 ; j < columns ; j++ ) { | |
370 | for ( Int_t i = 0 ; i < rows ; i++ ) { | |
371 | for ( Int_t k = 0 ; k < phiSlices ; k++ ) { | |
372 | ||
373 | // check wether the coordinates were screwed | |
374 | if (TMath::Abs((coord1(0,ip)*100-rlist1[i]))>1 || | |
375 | TMath::Abs((coord1(2,ip)*100-zedlist1[j])>1)) { | |
376 | AliError("internal error: coordinate system was screwed during the sum-up"); | |
9f3b99e2 | 377 | printf("sum-up: (r,z)=(%f,%f)\n",rlist1[i],zedlist1[j]); |
378 | printf("lookup: (r,z)=(%f,%f)\n",coord1(0,ip)*100,coord1(2,ip)*100); | |
15687d71 | 379 | AliError("Don't trust the results of the space charge calculation!"); |
380 | } | |
381 | ||
382 | // unfortunately, the lookup tables were produced to be faster for phi symmetric charges | |
383 | // This will be the most frequent usage (hopefully) | |
384 | // That's why we have to do this here ... | |
385 | ||
386 | TMatrixD &erA = *arrayofErA[k] ; | |
387 | TMatrixD &dEzA = *arrayofdEzA[k] ; | |
388 | ||
389 | TMatrixD &erC = *arrayofErC[k] ; | |
390 | TMatrixD &dEzC = *arrayofdEzC[k] ; | |
391 | ||
392 | // Sum up - Efield values in [V/m] -> transition to [V/cm] | |
393 | erA(i,j) += ((*bEr)(ip)) * weightA /100; | |
394 | erC(i,j) += ((*bEr)(ip)) * weightC /100; | |
395 | dEzA(i,j) += ((*bEz)(ip)) * weightA /100; | |
396 | dEzC(i,j) += ((*bEz)(ip)) * weightC /100; | |
397 | ||
398 | // increase the counter | |
399 | ip++; | |
400 | } | |
401 | } | |
402 | } // end coordinate loop | |
403 | } // end POC loop | |
404 | ||
405 | ||
406 | // ------------------------------------------------------------------------------- | |
407 | // Division by the Ez (drift) field and integration along z | |
408 | ||
409 | // AliInfo("Step 1: Division and integration"); | |
410 | ||
411 | Double_t ezField = (fgkCathodeV-fgkGG)/fgkTPCZ0; // = Electric Field (V/cm) Magnitude ~ -400 V/cm; | |
412 | ||
413 | for ( Int_t k = 0 ; k < phiSlices ; k++ ) { // phi loop | |
414 | ||
415 | // matrices holding the solution - summation of POC charges // see above | |
416 | TMatrixD &erA = *arrayofErA[k] ; | |
417 | TMatrixD &dezA = *arrayofdEzA[k] ; | |
418 | TMatrixD &erC = *arrayofErC[k] ; | |
419 | TMatrixD &dezC = *arrayofdEzC[k] ; | |
420 | ||
421 | // matrices which will contain the integrated fields (divided by the drift field) | |
422 | TMatrixD &erOverEzA = *arrayofEroverEzA[k] ; | |
423 | TMatrixD &deltaEzA = *arrayofDeltaEzA[k]; | |
424 | TMatrixD &erOverEzC = *arrayofEroverEzC[k] ; | |
425 | TMatrixD &deltaEzC = *arrayofDeltaEzC[k]; | |
426 | ||
427 | for ( Int_t i = 0 ; i < rows ; i++ ) { // r loop | |
428 | for ( Int_t j = columns-1 ; j >= 0 ; j-- ) {// z loop | |
429 | // Count backwards to facilitate integration over Z | |
430 | ||
431 | Int_t index = 1 ; // Simpsons rule if N=odd.If N!=odd then add extra point | |
432 | // by trapezoidal rule. | |
433 | ||
434 | erOverEzA(i,j) = 0; //ephiOverEzA(i,j) = 0; | |
435 | deltaEzA(i,j) = 0; | |
436 | erOverEzC(i,j) = 0; //ephiOverEzC(i,j) = 0; | |
437 | deltaEzC(i,j) = 0; | |
438 | ||
439 | for ( Int_t m = j ; m < columns ; m++ ) { // integration | |
440 | ||
441 | erOverEzA(i,j) += index*(gridSizeZ/3.0)*erA(i,m)/(-1*ezField) ; | |
442 | erOverEzC(i,j) += index*(gridSizeZ/3.0)*erC(i,m)/(-1*ezField) ; | |
443 | deltaEzA(i,j) += index*(gridSizeZ/3.0)*dezA(i,m)/(-1) ; | |
444 | deltaEzC(i,j) += index*(gridSizeZ/3.0)*dezC(i,m)/(-1) ; | |
445 | ||
446 | if ( index != 4 ) index = 4; else index = 2 ; | |
447 | ||
448 | } | |
449 | ||
450 | if ( index == 4 ) { | |
451 | erOverEzA(i,j) -= (gridSizeZ/3.0)*erA(i,columns-1)/(-1*ezField) ; | |
452 | erOverEzC(i,j) -= (gridSizeZ/3.0)*erC(i,columns-1)/(-1*ezField) ; | |
453 | deltaEzA(i,j) -= (gridSizeZ/3.0)*dezA(i,columns-1)/(-1) ; | |
454 | deltaEzC(i,j) -= (gridSizeZ/3.0)*dezC(i,columns-1)/(-1) ; | |
455 | } | |
456 | if ( index == 2 ) { | |
457 | erOverEzA(i,j) += (gridSizeZ/3.0)*(0.5*erA(i,columns-2)-2.5*erA(i,columns-1))/(-1*ezField) ; | |
458 | erOverEzC(i,j) += (gridSizeZ/3.0)*(0.5*erC(i,columns-2)-2.5*erC(i,columns-1))/(-1*ezField) ; | |
459 | deltaEzA(i,j) += (gridSizeZ/3.0)*(0.5*dezA(i,columns-2)-2.5*dezA(i,columns-1))/(-1) ; | |
460 | deltaEzC(i,j) += (gridSizeZ/3.0)*(0.5*dezC(i,columns-2)-2.5*dezC(i,columns-1))/(-1) ; | |
461 | } | |
462 | if ( j == columns-2 ) { | |
463 | erOverEzA(i,j) = (gridSizeZ/3.0)*(1.5*erA(i,columns-2)+1.5*erA(i,columns-1))/(-1*ezField) ; | |
464 | erOverEzC(i,j) = (gridSizeZ/3.0)*(1.5*erC(i,columns-2)+1.5*erC(i,columns-1))/(-1*ezField) ; | |
465 | deltaEzA(i,j) = (gridSizeZ/3.0)*(1.5*dezA(i,columns-2)+1.5*dezA(i,columns-1))/(-1) ; | |
466 | deltaEzC(i,j) = (gridSizeZ/3.0)*(1.5*dezC(i,columns-2)+1.5*dezC(i,columns-1))/(-1) ; | |
467 | } | |
468 | if ( j == columns-1 ) { | |
469 | erOverEzA(i,j) = 0; | |
470 | erOverEzC(i,j) = 0; | |
471 | deltaEzA(i,j) = 0; | |
472 | deltaEzC(i,j) = 0; | |
473 | } | |
474 | } | |
475 | } | |
476 | ||
477 | } | |
478 | ||
479 | // AliInfo("Step 1: Interpolation to Standard grid"); | |
480 | ||
481 | // ------------------------------------------------------------------------------- | |
482 | // Interpolate results onto the standard grid which is used for all AliTPCCorrections classes | |
483 | ||
484 | const Int_t order = 1 ; // Linear interpolation = 1, Quadratic = 2 | |
485 | ||
486 | Double_t r, z;//phi, z ; | |
487 | for ( Int_t k = 0 ; k < kNPhi ; k++ ) { | |
488 | // phi = fgkPhiList[k] ; | |
489 | ||
490 | // final lookup table | |
2bf29b72 | 491 | TMatrixF &erOverEzFinal = *fLookUpErOverEz[k] ; |
492 | TMatrixF &deltaEzFinal = *fLookUpDeltaEz[k] ; | |
15687d71 | 493 | |
494 | // calculated and integrated tables - just one phi slice | |
495 | TMatrixD &erOverEzA = *arrayofEroverEzA[0] ; | |
496 | TMatrixD &deltaEzA = *arrayofDeltaEzA[0]; | |
497 | TMatrixD &erOverEzC = *arrayofEroverEzC[0] ; | |
498 | TMatrixD &deltaEzC = *arrayofDeltaEzC[0]; | |
499 | ||
500 | ||
501 | for ( Int_t j = 0 ; j < kNZ ; j++ ) { | |
502 | ||
503 | z = TMath::Abs(fgkZList[j]) ; // z position is symmetric | |
504 | ||
505 | for ( Int_t i = 0 ; i < kNR ; i++ ) { | |
506 | r = fgkRList[i] ; | |
507 | ||
508 | // Interpolate Lookup tables onto standard grid | |
509 | if (fgkZList[j]>0) { | |
510 | erOverEzFinal(i,j) = Interpolate2DTable(order, r, z, rows, columns, rlist1, zedlist1, erOverEzA ); | |
511 | deltaEzFinal(i,j) = Interpolate2DTable(order, r, z, rows, columns, rlist1, zedlist1, deltaEzA ); | |
512 | } else { | |
513 | erOverEzFinal(i,j) = Interpolate2DTable(order, r, z, rows, columns, rlist1, zedlist1, erOverEzC ); | |
514 | deltaEzFinal(i,j) = - Interpolate2DTable(order, r, z, rows, columns, rlist1, zedlist1, deltaEzC ); | |
515 | // negative coordinate system on C side | |
516 | } | |
517 | ||
518 | } // end r loop | |
519 | } // end z loop | |
520 | } // end phi loop | |
521 | ||
522 | ||
523 | // clear the temporary arrays lists | |
524 | for ( Int_t k = 0 ; k < phiSlices ; k++ ) { | |
525 | ||
526 | delete arrayofErA[k]; | |
527 | delete arrayofdEzA[k]; | |
528 | delete arrayofErC[k]; | |
529 | delete arrayofdEzC[k]; | |
530 | ||
531 | delete arrayofEroverEzA[k]; | |
532 | delete arrayofDeltaEzA[k]; | |
533 | delete arrayofEroverEzC[k]; | |
534 | delete arrayofDeltaEzC[k]; | |
535 | ||
536 | } | |
537 | ||
538 | fZR->Close(); | |
539 | ||
540 | // ------------------------------------------------------------------------------------------------------ | |
541 | // Step 2: Load and sum up lookup table in rphi, fine grid, to emulate for example a GG leak | |
542 | ||
543 | // AliInfo("Step 2: Preparation of the weighted look-up table"); | |
544 | ||
545 | TFile *fRPhi = new TFile(fSCLookUpPOCsFileNameRPhi.Data(),"READ"); | |
546 | if ( !fRPhi ) { | |
547 | AliError("Precalculated POC-looup-table in RPhi could not be found"); | |
548 | return; | |
549 | } | |
550 | ||
551 | // units are in [m] | |
552 | TVector *gridf2 = (TVector*) fRPhi->Get("constants"); | |
553 | TVector &grid2 = *gridf2; | |
554 | TMatrix *coordf2 = (TMatrix*) fRPhi->Get("coordinates"); | |
555 | TMatrix &coord2 = *coordf2; | |
556 | TMatrix *coordPOCf2 = (TMatrix*) fRPhi->Get("POCcoord"); | |
557 | TMatrix &coordPOC2 = *coordPOCf2; | |
558 | ||
559 | rows = (Int_t)grid2(0); // number of points in r direction | |
560 | phiSlices = (Int_t)grid2(1); // number of points in phi | |
561 | columns = (Int_t)grid2(2); // number of points in z direction | |
562 | ||
563 | gridSizeR = (fgkOFCRadius-fgkIFCRadius)/(rows-1); // unit in [cm] | |
564 | Float_t gridSizePhi = TMath::TwoPi()/phiSlices; // unit in [rad] | |
565 | gridSizeZ = fgkTPCZ0/(columns-1); // unit in [cm] | |
566 | ||
567 | // list of points as used during sum up | |
9f3b99e2 | 568 | Double_t rlist2[kNRows], philist2[kNPhiSlices], zedlist2[kNColumns]; |
15687d71 | 569 | for ( Int_t k = 0 ; k < phiSlices ; k++ ) { |
570 | philist2[k] = gridSizePhi * k; | |
571 | for ( Int_t i = 0 ; i < rows ; i++ ) { | |
572 | rlist2[i] = fgkIFCRadius + i*gridSizeR ; | |
573 | for ( Int_t j = 0 ; j < columns ; j++ ) { | |
574 | zedlist2[j] = j * gridSizeZ ; | |
575 | } | |
576 | } | |
577 | } // only done once | |
578 | ||
579 | // temporary matrices needed for the calculation | |
580 | ||
9f3b99e2 | 581 | TMatrixD *arrayofErA2[kNPhiSlices], *arrayofEphiA2[kNPhiSlices], *arrayofdEzA2[kNPhiSlices]; |
582 | TMatrixD *arrayofErC2[kNPhiSlices], *arrayofEphiC2[kNPhiSlices], *arrayofdEzC2[kNPhiSlices]; | |
15687d71 | 583 | |
9f3b99e2 | 584 | TMatrixD *arrayofEroverEzA2[kNPhiSlices], *arrayofEphioverEzA2[kNPhiSlices], *arrayofDeltaEzA2[kNPhiSlices]; |
585 | TMatrixD *arrayofEroverEzC2[kNPhiSlices], *arrayofEphioverEzC2[kNPhiSlices], *arrayofDeltaEzC2[kNPhiSlices]; | |
15687d71 | 586 | |
587 | ||
588 | for ( Int_t k = 0 ; k < phiSlices ; k++ ) { | |
589 | ||
590 | arrayofErA2[k] = new TMatrixD(rows,columns) ; | |
591 | arrayofEphiA2[k] = new TMatrixD(rows,columns) ; | |
592 | arrayofdEzA2[k] = new TMatrixD(rows,columns) ; | |
593 | arrayofErC2[k] = new TMatrixD(rows,columns) ; | |
594 | arrayofEphiC2[k] = new TMatrixD(rows,columns) ; | |
595 | arrayofdEzC2[k] = new TMatrixD(rows,columns) ; | |
596 | ||
597 | arrayofEroverEzA2[k] = new TMatrixD(rows,columns) ; | |
598 | arrayofEphioverEzA2[k] = new TMatrixD(rows,columns) ; | |
599 | arrayofDeltaEzA2[k] = new TMatrixD(rows,columns) ; | |
600 | arrayofEroverEzC2[k] = new TMatrixD(rows,columns) ; | |
601 | arrayofEphioverEzC2[k] = new TMatrixD(rows,columns) ; | |
602 | arrayofDeltaEzC2[k] = new TMatrixD(rows,columns) ; | |
603 | ||
604 | // zero initialization not necessary, it is done in the constructor of TMatrix | |
605 | ||
606 | } | |
607 | ||
608 | ||
609 | treePOC = (TTree*)fRPhi->Get("POCall"); | |
610 | ||
611 | // TVector *bEr = 0; // done above | |
612 | TVector *bEphi= 0; | |
613 | // TVector *bEz = 0; // done above | |
614 | ||
615 | treePOC->SetBranchAddress("Er",&bEr); | |
616 | treePOC->SetBranchAddress("Ephi",&bEphi); | |
617 | treePOC->SetBranchAddress("Ez",&bEz); | |
618 | ||
619 | // Read the complete tree and do a weighted sum-up over the POC configurations | |
620 | // +++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ | |
621 | ||
622 | treeNumPOC = (Int_t)treePOC->GetEntries(); // Number of POC conf. in the look-up table | |
623 | ipC = 0; // POC Conf. counter (note: different to the POC number in the tree!) | |
624 | ||
625 | for (Int_t itreepC=0; itreepC<treeNumPOC; itreepC++) { // ------------- loop over POC configurations in tree | |
626 | ||
627 | treePOC->GetEntry(itreepC); | |
628 | ||
629 | // center of the POC voxel in [meter] | |
630 | Double_t r0 = coordPOC2(ipC,0); | |
631 | Double_t phi0 = coordPOC2(ipC,1); | |
632 | // Double_t z0 = coordPOC2(ipC,2); | |
633 | ||
634 | // weights (charge density) at POC position on the A and C side (in C/m^3/e0) | |
635 | // note: coordinates are in [cm] | |
636 | Double_t weightA = GetSpaceChargeDensity(r0*100,phi0, 0.499, 2); // partial load in r,phi | |
637 | Double_t weightC = GetSpaceChargeDensity(r0*100,phi0,-0.499, 2); // partial load in r,phi | |
638 | ||
9f3b99e2 | 639 | // printf("-----\n%f %f : %e %e\n",r0,phi0,weightA,weightC); |
15687d71 | 640 | |
641 | // Summing up the vector components according to their weight | |
642 | ||
643 | Int_t ip = 0; | |
644 | for ( Int_t j = 0 ; j < columns ; j++ ) { | |
645 | for ( Int_t i = 0 ; i < rows ; i++ ) { | |
646 | for ( Int_t k = 0 ; k < phiSlices ; k++ ) { | |
647 | ||
648 | // check wether the coordinates were screwed | |
649 | if (TMath::Abs((coord2(0,ip)*100-rlist2[i]))>1 || | |
650 | TMath::Abs((coord2(1,ip)-philist2[k]))>1 || | |
651 | TMath::Abs((coord2(2,ip)*100-zedlist2[j]))>1) { | |
652 | AliError("internal error: coordinate system was screwed during the sum-up"); | |
9f3b99e2 | 653 | printf("lookup: (r,phi,z)=(%f,%f,%f)\n",coord2(0,ip)*100,coord2(1,ip),coord2(2,ip)*100); |
654 | printf("sum-up: (r,phi,z)=(%f,%f,%f)\n",rlist2[i],philist2[k],zedlist2[j]); | |
15687d71 | 655 | AliError("Don't trust the results of the space charge calculation!"); |
656 | } | |
657 | ||
658 | // unfortunately, the lookup tables were produced to be faster for phi symmetric charges | |
659 | // This will be the most frequent usage (hopefully) | |
660 | // That's why we have to do this here ... | |
661 | ||
662 | TMatrixD &erA = *arrayofErA2[k] ; | |
663 | TMatrixD &ephiA = *arrayofEphiA2[k]; | |
664 | TMatrixD &dEzA = *arrayofdEzA2[k] ; | |
665 | ||
666 | TMatrixD &erC = *arrayofErC2[k] ; | |
667 | TMatrixD &ephiC = *arrayofEphiC2[k]; | |
668 | TMatrixD &dEzC = *arrayofdEzC2[k] ; | |
669 | ||
670 | // Sum up - Efield values in [V/m] -> transition to [V/cm] | |
671 | erA(i,j) += ((*bEr)(ip)) * weightA /100; | |
672 | erC(i,j) += ((*bEr)(ip)) * weightC /100; | |
673 | ephiA(i,j) += ((*bEphi)(ip)) * weightA/100; // [V/rad] | |
674 | ephiC(i,j) += ((*bEphi)(ip)) * weightC/100; // [V/rad] | |
675 | dEzA(i,j) += ((*bEz)(ip)) * weightA /100; | |
676 | dEzC(i,j) += ((*bEz)(ip)) * weightC /100; | |
677 | ||
678 | // increase the counter | |
679 | ip++; | |
680 | } | |
681 | } | |
682 | } // end coordinate loop | |
683 | ||
684 | ||
685 | // Rotation and summation in the rest of the dPhiSteps | |
686 | // which were not stored in the this tree due to storage & symmetry reasons | |
687 | ||
688 | ||
689 | Int_t phiPoints = (Int_t) grid2(1); | |
690 | Int_t phiPOC = (Int_t) grid2(4); | |
691 | ||
692 | // printf("%d %d\n",phiPOC,flagRadSym); | |
693 | ||
694 | for (Int_t phiiC = 1; phiiC<phiPOC; phiiC++) { // just used for non-radial symetric table | |
695 | ||
696 | Double_t phi0R = phiiC*phi0*2 + phi0; // rotate further | |
697 | ||
698 | // weights (charge density) at POC position on the A and C side (in C/m^3/e0) | |
699 | // note: coordinates are in [cm] // ecxept z | |
700 | weightA = GetSpaceChargeDensity(r0*100,phi0R, 0.499, 2); // partial load in r,phi | |
701 | weightC = GetSpaceChargeDensity(r0*100,phi0R,-0.499, 2); // partial load in r,phi | |
702 | ||
9f3b99e2 | 703 | // printf("%f %f : %e %e\n",r0,phi0R,weightA,weightC); |
15687d71 | 704 | |
705 | // Summing up the vector components according to their weight | |
706 | ip = 0; | |
707 | for ( Int_t j = 0 ; j < columns ; j++ ) { | |
708 | for ( Int_t i = 0 ; i < rows ; i++ ) { | |
709 | for ( Int_t k = 0 ; k < phiSlices ; k++ ) { | |
710 | ||
711 | // Note: rotating the coordinated during the sum up | |
712 | ||
713 | Int_t rotVal = (phiPoints/phiPOC)*phiiC; | |
714 | Int_t ipR = -1; | |
715 | ||
716 | if ((ip%phiPoints)>=rotVal) { | |
717 | ipR = ip-rotVal; | |
718 | } else { | |
719 | ipR = ip+(phiPoints-rotVal); | |
720 | } | |
721 | ||
722 | // unfortunately, the lookup tables were produced to be faster for phi symmetric charges | |
723 | // This will be the most frequent usage | |
724 | // That's why we have to do this here and not outside the loop ... | |
725 | ||
726 | TMatrixD &erA = *arrayofErA2[k] ; | |
727 | TMatrixD &ephiA = *arrayofEphiA2[k]; | |
728 | TMatrixD &dEzA = *arrayofdEzA2[k] ; | |
729 | ||
730 | TMatrixD &erC = *arrayofErC2[k] ; | |
731 | TMatrixD &ephiC = *arrayofEphiC2[k]; | |
732 | TMatrixD &dEzC = *arrayofdEzC2[k] ; | |
733 | ||
734 | // Sum up - Efield values in [V/m] -> transition to [V/cm] | |
735 | erA(i,j) += ((*bEr)(ipR)) * weightA /100; | |
736 | erC(i,j) += ((*bEr)(ipR)) * weightC /100; | |
737 | ephiA(i,j) += ((*bEphi)(ipR)) * weightA/100; // [V/rad] | |
738 | ephiC(i,j) += ((*bEphi)(ipR)) * weightC/100; // [V/rad] | |
739 | dEzA(i,j) += ((*bEz)(ipR)) * weightA /100; | |
740 | dEzC(i,j) += ((*bEz)(ipR)) * weightC /100; | |
741 | ||
742 | // increase the counter | |
743 | ip++; | |
744 | } | |
745 | } | |
746 | } // end coordinate loop | |
747 | ||
748 | } // end phi-POC summation (phiiC) | |
749 | ||
750 | ipC++; // POC configuration counter | |
751 | ||
9f3b99e2 | 752 | // printf("POC: (r,phi,z) = (%f %f %f) | weight(A,C): %03.1lf %03.1lf\n",r0,phi0,z0, weightA, weightC); |
15687d71 | 753 | |
754 | } | |
755 | ||
756 | ||
757 | ||
758 | ||
759 | // ------------------------------------------------------------------------------- | |
760 | // Division by the Ez (drift) field and integration along z | |
761 | ||
762 | // AliInfo("Step 2: Division and integration"); | |
763 | ||
764 | ||
765 | for ( Int_t k = 0 ; k < phiSlices ; k++ ) { // phi loop | |
766 | ||
767 | // matrices holding the solution - summation of POC charges // see above | |
768 | TMatrixD &erA = *arrayofErA2[k] ; | |
769 | TMatrixD &ephiA = *arrayofEphiA2[k]; | |
770 | TMatrixD &dezA = *arrayofdEzA2[k] ; | |
771 | TMatrixD &erC = *arrayofErC2[k] ; | |
772 | TMatrixD &ephiC = *arrayofEphiC2[k]; | |
773 | TMatrixD &dezC = *arrayofdEzC2[k] ; | |
774 | ||
775 | // matrices which will contain the integrated fields (divided by the drift field) | |
776 | TMatrixD &erOverEzA = *arrayofEroverEzA2[k] ; | |
777 | TMatrixD &ephiOverEzA = *arrayofEphioverEzA2[k]; | |
778 | TMatrixD &deltaEzA = *arrayofDeltaEzA2[k]; | |
779 | TMatrixD &erOverEzC = *arrayofEroverEzC2[k] ; | |
780 | TMatrixD &ephiOverEzC = *arrayofEphioverEzC2[k]; | |
781 | TMatrixD &deltaEzC = *arrayofDeltaEzC2[k]; | |
782 | ||
783 | for ( Int_t i = 0 ; i < rows ; i++ ) { // r loop | |
784 | for ( Int_t j = columns-1 ; j >= 0 ; j-- ) {// z loop | |
785 | // Count backwards to facilitate integration over Z | |
786 | ||
787 | Int_t index = 1 ; // Simpsons rule if N=odd.If N!=odd then add extra point by trapezoidal rule. | |
788 | ||
789 | erOverEzA(i,j) = 0; | |
790 | ephiOverEzA(i,j) = 0; | |
791 | deltaEzA(i,j) = 0; | |
792 | erOverEzC(i,j) = 0; | |
793 | ephiOverEzC(i,j) = 0; | |
794 | deltaEzC(i,j) = 0; | |
795 | ||
796 | for ( Int_t m = j ; m < columns ; m++ ) { // integration | |
797 | ||
798 | erOverEzA(i,j) += index*(gridSizeZ/3.0)*erA(i,m)/(-1*ezField) ; | |
799 | erOverEzC(i,j) += index*(gridSizeZ/3.0)*erC(i,m)/(-1*ezField) ; | |
800 | ephiOverEzA(i,j) += index*(gridSizeZ/3.0)*ephiA(i,m)/(-1*ezField) ; | |
801 | ephiOverEzC(i,j) += index*(gridSizeZ/3.0)*ephiC(i,m)/(-1*ezField) ; | |
802 | deltaEzA(i,j) += index*(gridSizeZ/3.0)*dezA(i,m)/(-1) ; | |
803 | deltaEzC(i,j) += index*(gridSizeZ/3.0)*dezC(i,m)/(-1) ; | |
804 | ||
805 | if ( index != 4 ) index = 4; else index = 2 ; | |
806 | ||
807 | } | |
808 | ||
809 | if ( index == 4 ) { | |
810 | erOverEzA(i,j) -= (gridSizeZ/3.0)*erA(i,columns-1)/(-1*ezField) ; | |
811 | erOverEzC(i,j) -= (gridSizeZ/3.0)*erC(i,columns-1)/(-1*ezField) ; | |
812 | ephiOverEzA(i,j) -= (gridSizeZ/3.0)*ephiA(i,columns-1)/(-1*ezField) ; | |
813 | ephiOverEzC(i,j) -= (gridSizeZ/3.0)*ephiC(i,columns-1)/(-1*ezField) ; | |
814 | deltaEzA(i,j) -= (gridSizeZ/3.0)*dezA(i,columns-1)/(-1) ; | |
815 | deltaEzC(i,j) -= (gridSizeZ/3.0)*dezC(i,columns-1)/(-1) ; | |
816 | } | |
817 | if ( index == 2 ) { | |
818 | erOverEzA(i,j) += (gridSizeZ/3.0)*(0.5*erA(i,columns-2)-2.5*erA(i,columns-1))/(-1*ezField) ; | |
819 | erOverEzC(i,j) += (gridSizeZ/3.0)*(0.5*erC(i,columns-2)-2.5*erC(i,columns-1))/(-1*ezField) ; | |
820 | ephiOverEzA(i,j) += (gridSizeZ/3.0)*(0.5*ephiA(i,columns-2)-2.5*ephiA(i,columns-1))/(-1*ezField) ; | |
821 | ephiOverEzC(i,j) += (gridSizeZ/3.0)*(0.5*ephiC(i,columns-2)-2.5*ephiC(i,columns-1))/(-1*ezField) ; | |
822 | deltaEzA(i,j) += (gridSizeZ/3.0)*(0.5*dezA(i,columns-2)-2.5*dezA(i,columns-1))/(-1) ; | |
823 | deltaEzC(i,j) += (gridSizeZ/3.0)*(0.5*dezC(i,columns-2)-2.5*dezC(i,columns-1))/(-1) ; | |
824 | } | |
825 | if ( j == columns-2 ) { | |
826 | erOverEzA(i,j) = (gridSizeZ/3.0)*(1.5*erA(i,columns-2)+1.5*erA(i,columns-1))/(-1*ezField) ; | |
827 | erOverEzC(i,j) = (gridSizeZ/3.0)*(1.5*erC(i,columns-2)+1.5*erC(i,columns-1))/(-1*ezField) ; | |
828 | ephiOverEzA(i,j) = (gridSizeZ/3.0)*(1.5*ephiA(i,columns-2)+1.5*ephiA(i,columns-1))/(-1*ezField) ; | |
829 | ephiOverEzC(i,j) = (gridSizeZ/3.0)*(1.5*ephiC(i,columns-2)+1.5*ephiC(i,columns-1))/(-1*ezField) ; | |
830 | deltaEzA(i,j) = (gridSizeZ/3.0)*(1.5*dezA(i,columns-2)+1.5*dezA(i,columns-1))/(-1) ; | |
831 | deltaEzC(i,j) = (gridSizeZ/3.0)*(1.5*dezC(i,columns-2)+1.5*dezC(i,columns-1))/(-1) ; | |
832 | } | |
833 | if ( j == columns-1 ) { | |
834 | erOverEzA(i,j) = 0; | |
835 | erOverEzC(i,j) = 0; | |
836 | ephiOverEzA(i,j) = 0; | |
837 | ephiOverEzC(i,j) = 0; | |
838 | deltaEzA(i,j) = 0; | |
839 | deltaEzC(i,j) = 0; | |
840 | } | |
841 | } | |
842 | } | |
843 | ||
844 | } | |
845 | ||
846 | AliInfo("Step 2: Interpolation to Standard grid"); | |
847 | ||
848 | // ------------------------------------------------------------------------------- | |
849 | // Interpolate results onto the standard grid which is used for all AliTPCCorrections classes | |
850 | ||
851 | ||
852 | for ( Int_t k = 0 ; k < kNPhi ; k++ ) { | |
853 | Double_t phi = fgkPhiList[k] ; | |
854 | ||
855 | // final lookup table | |
2bf29b72 | 856 | TMatrixF &erOverEzFinal = *fLookUpErOverEz[k] ; |
857 | TMatrixF &ephiOverEzFinal = *fLookUpEphiOverEz[k]; | |
858 | TMatrixF &deltaEzFinal = *fLookUpDeltaEz[k] ; | |
15687d71 | 859 | |
860 | for ( Int_t j = 0 ; j < kNZ ; j++ ) { | |
861 | ||
862 | z = TMath::Abs(fgkZList[j]) ; // z position is symmetric | |
863 | ||
864 | for ( Int_t i = 0 ; i < kNR ; i++ ) { | |
865 | r = fgkRList[i] ; | |
866 | ||
867 | // Interpolate Lookup tables onto standard grid | |
868 | if (fgkZList[j]>0) { | |
869 | erOverEzFinal(i,j) += Interpolate3DTable(order, r, z, phi, rows, columns, phiSlices, | |
870 | rlist2, zedlist2, philist2, arrayofEroverEzA2 ); | |
871 | ephiOverEzFinal(i,j) += Interpolate3DTable(order, r, z, phi, rows, columns, phiSlices, | |
872 | rlist2, zedlist2, philist2, arrayofEphioverEzA2); | |
873 | deltaEzFinal(i,j) += Interpolate3DTable(order, r, z, phi, rows, columns, phiSlices, | |
874 | rlist2, zedlist2, philist2, arrayofDeltaEzA2 ); | |
875 | } else { | |
876 | erOverEzFinal(i,j) += Interpolate3DTable(order, r, z, phi, rows, columns, phiSlices, | |
877 | rlist2, zedlist2, philist2, arrayofEroverEzC2 ); | |
878 | ephiOverEzFinal(i,j) += Interpolate3DTable(order, r, z, phi, rows, columns, phiSlices, | |
879 | rlist2, zedlist2, philist2, arrayofEphioverEzC2); | |
880 | deltaEzFinal(i,j) -= Interpolate3DTable(order, r, z, phi, rows, columns, phiSlices, | |
881 | rlist2, zedlist2, philist2, arrayofDeltaEzC2 ); | |
882 | } | |
883 | ||
884 | } // end r loop | |
885 | } // end z loop | |
886 | } // end phi loop | |
887 | ||
888 | ||
889 | // clear the temporary arrays lists | |
890 | for ( Int_t k = 0 ; k < phiSlices ; k++ ) { | |
891 | ||
892 | delete arrayofErA2[k]; | |
893 | delete arrayofEphiA2[k]; | |
894 | delete arrayofdEzA2[k]; | |
895 | delete arrayofErC2[k]; | |
896 | delete arrayofEphiC2[k]; | |
897 | delete arrayofdEzC2[k]; | |
898 | ||
899 | delete arrayofEroverEzA2[k]; | |
900 | delete arrayofEphioverEzA2[k]; | |
901 | delete arrayofDeltaEzA2[k]; | |
902 | delete arrayofEroverEzC2[k]; | |
903 | delete arrayofEphioverEzC2[k]; | |
904 | delete arrayofDeltaEzC2[k]; | |
905 | ||
906 | } | |
907 | ||
908 | fRPhi->Close(); | |
909 | ||
910 | // FINISHED | |
911 | ||
912 | fInitLookUp = kTRUE; | |
913 | ||
914 | } | |
915 | ||
916 | void AliTPCSpaceCharge3D::InitSpaceCharge3DDistortionCourse() { | |
cc3e558a | 917 | // |
918 | // Initialization of the Lookup table which contains the solutions of the | |
919 | // "space charge" (poisson) problem | |
920 | // | |
921 | // The sum-up uses a look-up table which contains different discretized Space charge fields | |
922 | // in order to calculate the corresponding field deviations due to a given (discretized) | |
923 | // space charge distribution .... | |
924 | // | |
15687d71 | 925 | // Method of calculation: Weighted sum-up of the different fields within the look up table |
926 | // Note: Full 3d version: Course and slow ... | |
cc3e558a | 927 | |
928 | if (fInitLookUp) { | |
929 | AliInfo("Lookup table was already initialized!"); | |
930 | // return; | |
931 | } | |
932 | ||
933 | AliInfo("Preparation of the weighted look-up table"); | |
934 | ||
15687d71 | 935 | TFile *f = new TFile(fSCLookUpPOCsFileName3D.Data(),"READ"); |
936 | if ( !f ) { | |
cc3e558a | 937 | AliError("Precalculated POC-looup-table could not be found"); |
938 | return; | |
939 | } | |
940 | ||
941 | // units are in [m] | |
942 | TVector *gridf = (TVector*) f->Get("constants"); | |
943 | TVector &grid = *gridf; | |
944 | TMatrix *coordf = (TMatrix*) f->Get("coordinates"); | |
945 | TMatrix &coord = *coordf; | |
946 | TMatrix *coordPOCf = (TMatrix*) f->Get("POCcoord"); | |
947 | TMatrix &coordPOC = *coordPOCf; | |
948 | ||
949 | Bool_t flagRadSym = 0; | |
950 | if (grid(1)==1 && grid(4)==1) { | |
15687d71 | 951 | // AliInfo("LOOK UP TABLE IS RADIAL SYMETTRIC - Field in Phi is ZERO"); |
cc3e558a | 952 | flagRadSym=1; |
953 | } | |
954 | ||
955 | Int_t rows = (Int_t)grid(0); // number of points in r direction | |
956 | Int_t phiSlices = (Int_t)grid(1); // number of points in phi | |
957 | Int_t columns = (Int_t)grid(2); // number of points in z direction | |
958 | ||
15687d71 | 959 | const Float_t gridSizeR = (fgkOFCRadius-fgkIFCRadius)/(rows-1); // unit in [cm] |
960 | const Float_t gridSizePhi = TMath::TwoPi()/phiSlices; // unit in [rad] | |
961 | const Float_t gridSizeZ = fgkTPCZ0/(columns-1); // unit in [cm] | |
cc3e558a | 962 | |
963 | // temporary matrices needed for the calculation | |
9f3b99e2 | 964 | TMatrixD *arrayofErA[kNPhiSlices], *arrayofEphiA[kNPhiSlices], *arrayofdEzA[kNPhiSlices]; |
965 | TMatrixD *arrayofErC[kNPhiSlices], *arrayofEphiC[kNPhiSlices], *arrayofdEzC[kNPhiSlices]; | |
cc3e558a | 966 | |
9f3b99e2 | 967 | TMatrixD *arrayofEroverEzA[kNPhiSlices], *arrayofEphioverEzA[kNPhiSlices], *arrayofDeltaEzA[kNPhiSlices]; |
968 | TMatrixD *arrayofEroverEzC[kNPhiSlices], *arrayofEphioverEzC[kNPhiSlices], *arrayofDeltaEzC[kNPhiSlices]; | |
cc3e558a | 969 | |
970 | ||
971 | for ( Int_t k = 0 ; k < phiSlices ; k++ ) { | |
972 | ||
973 | arrayofErA[k] = new TMatrixD(rows,columns) ; | |
974 | arrayofEphiA[k] = new TMatrixD(rows,columns) ; // zero if radial symmetric | |
975 | arrayofdEzA[k] = new TMatrixD(rows,columns) ; | |
976 | arrayofErC[k] = new TMatrixD(rows,columns) ; | |
977 | arrayofEphiC[k] = new TMatrixD(rows,columns) ; // zero if radial symmetric | |
978 | arrayofdEzC[k] = new TMatrixD(rows,columns) ; | |
979 | ||
980 | arrayofEroverEzA[k] = new TMatrixD(rows,columns) ; | |
981 | arrayofEphioverEzA[k] = new TMatrixD(rows,columns) ; // zero if radial symmetric | |
982 | arrayofDeltaEzA[k] = new TMatrixD(rows,columns) ; | |
983 | arrayofEroverEzC[k] = new TMatrixD(rows,columns) ; | |
984 | arrayofEphioverEzC[k] = new TMatrixD(rows,columns) ; // zero if radial symmetric | |
985 | arrayofDeltaEzC[k] = new TMatrixD(rows,columns) ; | |
986 | ||
987 | // Set the values to zero the lookup tables | |
988 | // not necessary, it is done in the constructor of TMatrix - code deleted | |
989 | ||
990 | } | |
991 | ||
992 | // list of points as used in the interpolation (during sum up) | |
9f3b99e2 | 993 | Double_t rlist[kNRows], zedlist[kNColumns] , philist[kNPhiSlices]; |
cc3e558a | 994 | for ( Int_t k = 0 ; k < phiSlices ; k++ ) { |
995 | philist[k] = gridSizePhi * k; | |
996 | for ( Int_t i = 0 ; i < rows ; i++ ) { | |
997 | rlist[i] = fgkIFCRadius + i*gridSizeR ; | |
998 | for ( Int_t j = 0 ; j < columns ; j++ ) { | |
999 | zedlist[j] = j * gridSizeZ ; | |
1000 | } | |
1001 | } | |
1002 | } // only done once | |
1003 | ||
1004 | ||
cc3e558a | 1005 | TTree *treePOC = (TTree*)f->Get("POCall"); |
1006 | ||
1007 | TVector *bEr = 0; TVector *bEphi= 0; TVector *bEz = 0; | |
1008 | ||
1009 | treePOC->SetBranchAddress("Er",&bEr); | |
1010 | if (!flagRadSym) treePOC->SetBranchAddress("Ephi",&bEphi); | |
1011 | treePOC->SetBranchAddress("Ez",&bEz); | |
1012 | ||
cc3e558a | 1013 | |
1014 | // Read the complete tree and do a weighted sum-up over the POC configurations | |
1015 | // +++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ | |
1016 | ||
1017 | Int_t treeNumPOC = (Int_t)treePOC->GetEntries(); // Number of POC conf. in the look-up table | |
1018 | Int_t ipC = 0; // POC Conf. counter (note: different to the POC number in the tree!) | |
1019 | ||
15687d71 | 1020 | for (Int_t itreepC=0; itreepC<treeNumPOC; itreepC++) { // ------------- loop over POC configurations in tree |
cc3e558a | 1021 | |
cc3e558a | 1022 | treePOC->GetEntry(itreepC); |
1023 | ||
cc3e558a | 1024 | // center of the POC voxel in [meter] |
1025 | Double_t r0 = coordPOC(ipC,0); | |
1026 | Double_t phi0 = coordPOC(ipC,1); | |
1027 | Double_t z0 = coordPOC(ipC,2); | |
1028 | ||
15687d71 | 1029 | ipC++; // POC configuration counter |
cc3e558a | 1030 | |
1031 | // weights (charge density) at POC position on the A and C side (in C/m^3/e0) | |
1032 | // note: coordinates are in [cm] | |
92a85338 | 1033 | Double_t weightA = GetSpaceChargeDensity(r0*100,phi0, z0*100,0); |
1034 | Double_t weightC = GetSpaceChargeDensity(r0*100,phi0,-z0*100,0); | |
cc3e558a | 1035 | |
1036 | // Summing up the vector components according to their weight | |
1037 | ||
1038 | Int_t ip = 0; | |
1039 | for ( Int_t j = 0 ; j < columns ; j++ ) { | |
1040 | for ( Int_t i = 0 ; i < rows ; i++ ) { | |
1041 | for ( Int_t k = 0 ; k < phiSlices ; k++ ) { | |
1042 | ||
1043 | // check wether the coordinates were screwed | |
15687d71 | 1044 | if (TMath::Abs((coord(0,ip)*100-rlist[i]))>1 || |
1045 | TMath::Abs((coord(1,ip)-philist[k]))>1 || | |
1046 | TMath::Abs((coord(2,ip)*100-zedlist[j]))>1) { | |
cc3e558a | 1047 | AliError("internal error: coordinate system was screwed during the sum-up"); |
9f3b99e2 | 1048 | printf("lookup: (r,phi,z)=(%f,%f,%f)\n",coord(0,ip)*100,coord(1,ip),coord(2,ip)*100); |
1049 | printf("sum-up: (r,phi,z)=(%f,%f,%f)\n",rlist[i],philist[k],zedlist[j]); | |
15687d71 | 1050 | AliError("Don't trust the results of the space charge calculation!"); |
cc3e558a | 1051 | } |
1052 | ||
1053 | // unfortunately, the lookup tables were produced to be faster for phi symmetric charges | |
1054 | // This will be the most frequent usage (hopefully) | |
1055 | // That's why we have to do this here ... | |
1056 | ||
1057 | TMatrixD &erA = *arrayofErA[k] ; | |
1058 | TMatrixD &ephiA = *arrayofEphiA[k]; | |
15687d71 | 1059 | TMatrixD &dEzA = *arrayofdEzA[k] ; |
cc3e558a | 1060 | |
1061 | TMatrixD &erC = *arrayofErC[k] ; | |
1062 | TMatrixD &ephiC = *arrayofEphiC[k]; | |
15687d71 | 1063 | TMatrixD &dEzC = *arrayofdEzC[k] ; |
cc3e558a | 1064 | |
1065 | // Sum up - Efield values in [V/m] -> transition to [V/cm] | |
1066 | erA(i,j) += ((*bEr)(ip)) * weightA /100; | |
1067 | erC(i,j) += ((*bEr)(ip)) * weightC /100; | |
1068 | if (!flagRadSym) { | |
15687d71 | 1069 | ephiA(i,j) += ((*bEphi)(ip)) * weightA/100; // [V/rad] |
1070 | ephiC(i,j) += ((*bEphi)(ip)) * weightC/100; // [V/rad] | |
cc3e558a | 1071 | } |
1072 | dEzA(i,j) += ((*bEz)(ip)) * weightA /100; | |
1073 | dEzC(i,j) += ((*bEz)(ip)) * weightC /100; | |
1074 | ||
1075 | // increase the counter | |
1076 | ip++; | |
1077 | } | |
1078 | } | |
15687d71 | 1079 | } // end coordinate loop |
1080 | ||
cc3e558a | 1081 | |
1082 | // Rotation and summation in the rest of the dPhiSteps | |
15687d71 | 1083 | // which were not stored in the this tree due to storage & symmetry reasons |
cc3e558a | 1084 | |
1085 | Int_t phiPoints = (Int_t) grid(1); | |
1086 | Int_t phiPOC = (Int_t) grid(4); | |
1087 | ||
15687d71 | 1088 | // printf("%d %d\n",phiPOC,flagRadSym); |
cc3e558a | 1089 | |
15687d71 | 1090 | for (Int_t phiiC = 1; phiiC<phiPOC; phiiC++) { // just used for non-radial symetric table |
cc3e558a | 1091 | |
1092 | r0 = coordPOC(ipC,0); | |
1093 | phi0 = coordPOC(ipC,1); | |
1094 | z0 = coordPOC(ipC,2); | |
1095 | ||
1096 | ipC++; // POC conf. counter | |
1097 | ||
1098 | // weights (charge density) at POC position on the A and C side (in C/m^3/e0) | |
1099 | // note: coordinates are in [cm] | |
92a85338 | 1100 | weightA = GetSpaceChargeDensity(r0*100,phi0, z0*100,0); |
1101 | weightC = GetSpaceChargeDensity(r0*100,phi0,-z0*100,0); | |
cc3e558a | 1102 | |
9f3b99e2 | 1103 | // printf("%f %f %f: %e %e\n",r0,phi0,z0,weightA,weightC); |
15687d71 | 1104 | |
cc3e558a | 1105 | // Summing up the vector components according to their weight |
1106 | ip = 0; | |
1107 | for ( Int_t j = 0 ; j < columns ; j++ ) { | |
1108 | for ( Int_t i = 0 ; i < rows ; i++ ) { | |
1109 | for ( Int_t k = 0 ; k < phiSlices ; k++ ) { | |
1110 | ||
1111 | // Note: rotating the coordinated during the sum up | |
1112 | ||
1113 | Int_t rotVal = (phiPoints/phiPOC)*phiiC; | |
1114 | Int_t ipR = -1; | |
1115 | ||
1116 | if ((ip%phiPoints)>=rotVal) { | |
1117 | ipR = ip-rotVal; | |
1118 | } else { | |
1119 | ipR = ip+(phiPoints-rotVal); | |
1120 | } | |
1121 | ||
1122 | // unfortunately, the lookup tables were produced to be faster for phi symmetric charges | |
15687d71 | 1123 | // This will be the most frequent usage |
cc3e558a | 1124 | // That's why we have to do this here and not outside the loop ... |
1125 | ||
1126 | TMatrixD &erA = *arrayofErA[k] ; | |
1127 | TMatrixD &ephiA = *arrayofEphiA[k]; | |
1128 | TMatrixD &dEzA = *arrayofdEzA[k] ; | |
1129 | ||
1130 | TMatrixD &erC = *arrayofErC[k] ; | |
1131 | TMatrixD &ephiC = *arrayofEphiC[k]; | |
1132 | TMatrixD &dEzC = *arrayofdEzC[k] ; | |
1133 | ||
1134 | // Sum up - Efield values in [V/m] -> transition to [V/cm] | |
1135 | erA(i,j) += ((*bEr)(ipR)) * weightA /100; | |
1136 | erC(i,j) += ((*bEr)(ipR)) * weightC /100; | |
1137 | if (!flagRadSym) { | |
15687d71 | 1138 | ephiA(i,j) += ((*bEphi)(ipR)) * weightA/100; // [V/rad] |
1139 | ephiC(i,j) += ((*bEphi)(ipR)) * weightC/100; // [V/rad] | |
cc3e558a | 1140 | } |
1141 | dEzA(i,j) += ((*bEz)(ipR)) * weightA /100; | |
1142 | dEzC(i,j) += ((*bEz)(ipR)) * weightC /100; | |
1143 | ||
1144 | // increase the counter | |
1145 | ip++; | |
1146 | } | |
1147 | } | |
1148 | } // end coordinate loop | |
1149 | ||
1150 | } // end phi-POC summation (phiiC) | |
1151 | ||
1152 | ||
9f3b99e2 | 1153 | // printf("POC: (r,phi,z) = (%f %f %f) | weight(A,C): %03.1lf %03.1lf\n",r0,phi0,z0, weightA, weightC); |
15687d71 | 1154 | |
1155 | } | |
1156 | ||
cc3e558a | 1157 | |
cc3e558a | 1158 | |
1159 | // ------------------------------------------------------------------------------- | |
1160 | // Division by the Ez (drift) field and integration along z | |
1161 | ||
15687d71 | 1162 | AliInfo("Division and integration"); |
1163 | ||
cc3e558a | 1164 | Double_t ezField = (fgkCathodeV-fgkGG)/fgkTPCZ0; // = Electric Field (V/cm) Magnitude ~ -400 V/cm; |
1165 | ||
1166 | for ( Int_t k = 0 ; k < phiSlices ; k++ ) { // phi loop | |
1167 | ||
15687d71 | 1168 | // matrices holding the solution - summation of POC charges // see above |
cc3e558a | 1169 | TMatrixD &erA = *arrayofErA[k] ; |
1170 | TMatrixD &ephiA = *arrayofEphiA[k]; | |
1171 | TMatrixD &dezA = *arrayofdEzA[k] ; | |
1172 | TMatrixD &erC = *arrayofErC[k] ; | |
1173 | TMatrixD &ephiC = *arrayofEphiC[k]; | |
1174 | TMatrixD &dezC = *arrayofdEzC[k] ; | |
1175 | ||
15687d71 | 1176 | // matrices which will contain the integrated fields (divided by the drift field) |
cc3e558a | 1177 | TMatrixD &erOverEzA = *arrayofEroverEzA[k] ; |
1178 | TMatrixD &ephiOverEzA = *arrayofEphioverEzA[k]; | |
1179 | TMatrixD &deltaEzA = *arrayofDeltaEzA[k]; | |
1180 | TMatrixD &erOverEzC = *arrayofEroverEzC[k] ; | |
1181 | TMatrixD &ephiOverEzC = *arrayofEphioverEzC[k]; | |
1182 | TMatrixD &deltaEzC = *arrayofDeltaEzC[k]; | |
1183 | ||
1184 | for ( Int_t i = 0 ; i < rows ; i++ ) { // r loop | |
1185 | for ( Int_t j = columns-1 ; j >= 0 ; j-- ) {// z loop | |
1186 | // Count backwards to facilitate integration over Z | |
1187 | ||
1188 | Int_t index = 1 ; // Simpsons rule if N=odd.If N!=odd then add extra point by trapezoidal rule. | |
1189 | ||
1190 | erOverEzA(i,j) = 0; ephiOverEzA(i,j) = 0; deltaEzA(i,j) = 0; | |
1191 | erOverEzC(i,j) = 0; ephiOverEzC(i,j) = 0; deltaEzC(i,j) = 0; | |
1192 | ||
1193 | for ( Int_t m = j ; m < columns ; m++ ) { // integration | |
1194 | ||
1195 | erOverEzA(i,j) += index*(gridSizeZ/3.0)*erA(i,m)/(-1*ezField) ; | |
1196 | erOverEzC(i,j) += index*(gridSizeZ/3.0)*erC(i,m)/(-1*ezField) ; | |
1197 | if (!flagRadSym) { | |
1198 | ephiOverEzA(i,j) += index*(gridSizeZ/3.0)*ephiA(i,m)/(-1*ezField) ; | |
1199 | ephiOverEzC(i,j) += index*(gridSizeZ/3.0)*ephiC(i,m)/(-1*ezField) ; | |
1200 | } | |
15687d71 | 1201 | deltaEzA(i,j) += index*(gridSizeZ/3.0)*dezA(i,m)/(-1) ; |
1202 | deltaEzC(i,j) += index*(gridSizeZ/3.0)*dezC(i,m)/(-1) ; | |
cc3e558a | 1203 | |
1204 | if ( index != 4 ) index = 4; else index = 2 ; | |
1205 | ||
1206 | } | |
1207 | ||
1208 | if ( index == 4 ) { | |
1209 | erOverEzA(i,j) -= (gridSizeZ/3.0)*erA(i,columns-1)/(-1*ezField) ; | |
1210 | erOverEzC(i,j) -= (gridSizeZ/3.0)*erC(i,columns-1)/(-1*ezField) ; | |
1211 | if (!flagRadSym) { | |
1212 | ephiOverEzA(i,j) -= (gridSizeZ/3.0)*ephiA(i,columns-1)/(-1*ezField) ; | |
1213 | ephiOverEzC(i,j) -= (gridSizeZ/3.0)*ephiC(i,columns-1)/(-1*ezField) ; | |
1214 | } | |
15687d71 | 1215 | deltaEzA(i,j) -= (gridSizeZ/3.0)*dezA(i,columns-1)/(-1) ; |
1216 | deltaEzC(i,j) -= (gridSizeZ/3.0)*dezC(i,columns-1)/(-1) ; | |
cc3e558a | 1217 | } |
1218 | if ( index == 2 ) { | |
1219 | erOverEzA(i,j) += (gridSizeZ/3.0)*(0.5*erA(i,columns-2)-2.5*erA(i,columns-1))/(-1*ezField) ; | |
1220 | erOverEzC(i,j) += (gridSizeZ/3.0)*(0.5*erC(i,columns-2)-2.5*erC(i,columns-1))/(-1*ezField) ; | |
1221 | if (!flagRadSym) { | |
1222 | ephiOverEzA(i,j) += (gridSizeZ/3.0)*(0.5*ephiA(i,columns-2)-2.5*ephiA(i,columns-1))/(-1*ezField) ; | |
1223 | ephiOverEzC(i,j) += (gridSizeZ/3.0)*(0.5*ephiC(i,columns-2)-2.5*ephiC(i,columns-1))/(-1*ezField) ; | |
1224 | } | |
15687d71 | 1225 | deltaEzA(i,j) += (gridSizeZ/3.0)*(0.5*dezA(i,columns-2)-2.5*dezA(i,columns-1))/(-1) ; |
1226 | deltaEzC(i,j) += (gridSizeZ/3.0)*(0.5*dezC(i,columns-2)-2.5*dezC(i,columns-1))/(-1) ; | |
cc3e558a | 1227 | } |
1228 | if ( j == columns-2 ) { | |
1229 | erOverEzA(i,j) = (gridSizeZ/3.0)*(1.5*erA(i,columns-2)+1.5*erA(i,columns-1))/(-1*ezField) ; | |
1230 | erOverEzC(i,j) = (gridSizeZ/3.0)*(1.5*erC(i,columns-2)+1.5*erC(i,columns-1))/(-1*ezField) ; | |
1231 | if (!flagRadSym) { | |
1232 | ephiOverEzA(i,j) = (gridSizeZ/3.0)*(1.5*ephiA(i,columns-2)+1.5*ephiA(i,columns-1))/(-1*ezField) ; | |
1233 | ephiOverEzC(i,j) = (gridSizeZ/3.0)*(1.5*ephiC(i,columns-2)+1.5*ephiC(i,columns-1))/(-1*ezField) ; | |
1234 | } | |
15687d71 | 1235 | deltaEzA(i,j) = (gridSizeZ/3.0)*(1.5*dezA(i,columns-2)+1.5*dezA(i,columns-1))/(-1) ; |
1236 | deltaEzC(i,j) = (gridSizeZ/3.0)*(1.5*dezC(i,columns-2)+1.5*dezC(i,columns-1))/(-1) ; | |
cc3e558a | 1237 | } |
1238 | if ( j == columns-1 ) { | |
15687d71 | 1239 | erOverEzA(i,j) = 0; |
1240 | erOverEzC(i,j) = 0; | |
cc3e558a | 1241 | if (!flagRadSym) { |
15687d71 | 1242 | ephiOverEzA(i,j) = 0; |
1243 | ephiOverEzC(i,j) = 0; | |
cc3e558a | 1244 | } |
15687d71 | 1245 | deltaEzA(i,j) = 0; |
1246 | deltaEzC(i,j) = 0; | |
cc3e558a | 1247 | } |
1248 | } | |
1249 | } | |
1250 | ||
1251 | } | |
1252 | ||
15687d71 | 1253 | |
1254 | ||
cc3e558a | 1255 | AliInfo("Interpolation to Standard grid"); |
1256 | ||
1257 | // ------------------------------------------------------------------------------- | |
15687d71 | 1258 | // Interpolate results onto the standard grid which is used for all AliTPCCorrections classes |
cc3e558a | 1259 | |
1260 | const Int_t order = 1 ; // Linear interpolation = 1, Quadratic = 2 | |
1261 | ||
1262 | Double_t r, phi, z ; | |
1263 | for ( Int_t k = 0 ; k < kNPhi ; k++ ) { | |
1264 | phi = fgkPhiList[k] ; | |
1265 | ||
2bf29b72 | 1266 | TMatrixF &erOverEz = *fLookUpErOverEz[k] ; |
1267 | TMatrixF &ephiOverEz = *fLookUpEphiOverEz[k]; | |
1268 | TMatrixF &deltaEz = *fLookUpDeltaEz[k] ; | |
cc3e558a | 1269 | |
1270 | for ( Int_t j = 0 ; j < kNZ ; j++ ) { | |
1271 | ||
1272 | z = TMath::Abs(fgkZList[j]) ; // z position is symmetric | |
1273 | ||
1274 | for ( Int_t i = 0 ; i < kNR ; i++ ) { | |
1275 | r = fgkRList[i] ; | |
1276 | ||
1277 | // Interpolate Lookup tables onto standard grid | |
1278 | if (fgkZList[j]>0) { | |
1279 | erOverEz(i,j) = Interpolate3DTable(order, r, z, phi, rows, columns, phiSlices, | |
1280 | rlist, zedlist, philist, arrayofEroverEzA ); | |
1281 | ephiOverEz(i,j) = Interpolate3DTable(order, r, z, phi, rows, columns, phiSlices, | |
1282 | rlist, zedlist, philist, arrayofEphioverEzA); | |
1283 | deltaEz(i,j) = Interpolate3DTable(order, r, z, phi, rows, columns, phiSlices, | |
1284 | rlist, zedlist, philist, arrayofDeltaEzA ); | |
1285 | } else { | |
1286 | erOverEz(i,j) = Interpolate3DTable(order, r, z, phi, rows, columns, phiSlices, | |
1287 | rlist, zedlist, philist, arrayofEroverEzC ); | |
1288 | ephiOverEz(i,j) = Interpolate3DTable(order, r, z, phi, rows, columns, phiSlices, | |
1289 | rlist, zedlist, philist, arrayofEphioverEzC); | |
1290 | deltaEz(i,j) = - Interpolate3DTable(order, r, z, phi, rows, columns, phiSlices, | |
1291 | rlist, zedlist, philist, arrayofDeltaEzC ); | |
1292 | // negative coordinate system on C side | |
1293 | } | |
1294 | ||
1295 | } // end r loop | |
1296 | } // end z loop | |
1297 | } // end phi loop | |
1298 | ||
15687d71 | 1299 | |
cc3e558a | 1300 | // clear the temporary arrays lists |
1301 | for ( Int_t k = 0 ; k < phiSlices ; k++ ) { | |
1302 | ||
1303 | delete arrayofErA[k]; | |
1304 | delete arrayofEphiA[k]; | |
1305 | delete arrayofdEzA[k]; | |
1306 | delete arrayofErC[k]; | |
1307 | delete arrayofEphiC[k]; | |
1308 | delete arrayofdEzC[k]; | |
1309 | ||
1310 | delete arrayofEroverEzA[k]; | |
1311 | delete arrayofEphioverEzA[k]; | |
1312 | delete arrayofDeltaEzA[k]; | |
1313 | delete arrayofEroverEzC[k]; | |
1314 | delete arrayofEphioverEzC[k]; | |
1315 | delete arrayofDeltaEzC[k]; | |
1316 | ||
1317 | } | |
1318 | ||
cc3e558a | 1319 | fInitLookUp = kTRUE; |
1320 | ||
1321 | } | |
1322 | ||
1323 | ||
15687d71 | 1324 | void AliTPCSpaceCharge3D::SetSCDataFileName(TString fname) { |
cc3e558a | 1325 | // |
1326 | // Set & load the Space charge density distribution from a file | |
1327 | // (linear interpolation onto a standard grid) | |
1328 | // | |
1329 | ||
15687d71 | 1330 | |
cc3e558a | 1331 | fSCDataFileName = fname; |
1332 | ||
15687d71 | 1333 | TFile *f = new TFile(fSCDataFileName.Data(),"READ"); |
cc3e558a | 1334 | if (!f) { |
1335 | AliError(Form("File %s, which should contain the space charge distribution, could not be found", | |
15687d71 | 1336 | fSCDataFileName.Data())); |
cc3e558a | 1337 | return; |
1338 | } | |
1339 | ||
15687d71 | 1340 | TH2F *densityRZ = (TH2F*) f->Get("SpaceChargeInRZ"); |
1341 | if (!densityRZ) { | |
cc3e558a | 1342 | AliError(Form("The indicated file (%s) does not contain a histogram called %s", |
15687d71 | 1343 | fSCDataFileName.Data(),"SpaceChargeInRZ")); |
1344 | return; | |
1345 | } | |
1346 | ||
1347 | TH3F *densityRPhi = (TH3F*) f->Get("SpaceChargeInRPhi"); | |
1348 | if (!densityRPhi) { | |
1349 | AliError(Form("The indicated file (%s) does not contain a histogram called %s", | |
1350 | fSCDataFileName.Data(),"SpaceChargeInRPhi")); | |
cc3e558a | 1351 | return; |
1352 | } | |
1353 | ||
1354 | ||
1355 | Double_t r, phi, z ; | |
15687d71 | 1356 | |
1357 | TMatrixD &scDensityInRZ = *fSCdensityInRZ; | |
1358 | TMatrixD &scDensityInRPhiA = *fSCdensityInRPhiA; | |
1359 | TMatrixD &scDensityInRPhiC = *fSCdensityInRPhiC; | |
cc3e558a | 1360 | for ( Int_t k = 0 ; k < kNPhi ; k++ ) { |
1361 | phi = fgkPhiList[k] ; | |
2bf29b72 | 1362 | TMatrixF &scDensity = *fSCdensityDistribution[k] ; |
cc3e558a | 1363 | for ( Int_t j = 0 ; j < kNZ ; j++ ) { |
15687d71 | 1364 | z = fgkZList[j] ; |
cc3e558a | 1365 | for ( Int_t i = 0 ; i < kNR ; i++ ) { |
1366 | r = fgkRList[i] ; | |
15687d71 | 1367 | |
1368 | // partial load in (r,z) | |
1369 | if (k==0) // do just once | |
1370 | scDensityInRZ(i,j) = densityRZ->Interpolate(r,z); | |
1371 | ||
1372 | // partial load in (r,phi) | |
1373 | if ( j==0 || j == kNZ/2 ) { | |
1374 | if (z>0) | |
1375 | scDensityInRPhiA(i,k) = densityRPhi->Interpolate(r,phi,0.499); // A side | |
1376 | else | |
1377 | scDensityInRPhiC(i,k) = densityRPhi->Interpolate(r,phi,-0.499); // C side | |
1378 | } | |
1379 | ||
1380 | // Full 3D configuration ... | |
1381 | if (z>0) | |
1382 | scDensity(i,j) = scDensityInRZ(i,j) + scDensityInRPhiA(i,k); | |
1383 | else | |
1384 | scDensity(i,j) = scDensityInRZ(i,j) + scDensityInRPhiC(i,k); | |
cc3e558a | 1385 | } |
1386 | } | |
1387 | } | |
1388 | ||
cc3e558a | 1389 | f->Close(); |
1390 | ||
1391 | fInitLookUp = kFALSE; | |
1392 | ||
1393 | ||
1394 | } | |
1395 | ||
92a85338 | 1396 | void AliTPCSpaceCharge3D::SetInputSpaceCharge(TH3 * hisSpaceCharge3D, TH2 * hisRPhi, TH2* hisRZ, Double_t norm){ |
1397 | // | |
1398 | // Use 3D space charge map as an optional input | |
1399 | // The layout of the input histogram is assumed to be: (phi,r,z) | |
1400 | // Density histogram is expreseed is expected to bin in C/m^3 | |
1401 | // | |
1402 | // Standard histogram interpolation is used in order to use the density at center of voxel | |
1403 | // | |
1404 | // | |
1405 | fSpaceChargeHistogram3D = hisSpaceCharge3D; | |
1406 | fSpaceChargeHistogramRPhi = hisRPhi; | |
1407 | fSpaceChargeHistogramRZ = hisRZ; | |
1408 | ||
1409 | Double_t r, phi, z ; | |
1410 | TMatrixD &scDensityInRZ = *fSCdensityInRZ; | |
1411 | TMatrixD &scDensityInRPhiA = *fSCdensityInRPhiA; | |
1412 | TMatrixD &scDensityInRPhiC = *fSCdensityInRPhiC; | |
1413 | // | |
1414 | Double_t rmin=hisSpaceCharge3D->GetYaxis()->GetBinCenter(0); | |
1415 | Double_t rmax=hisSpaceCharge3D->GetYaxis()->GetBinUpEdge(hisSpaceCharge3D->GetYaxis()->GetNbins()); | |
1416 | Double_t zmin=hisSpaceCharge3D->GetZaxis()->GetBinCenter(0); | |
1417 | Double_t zmax=hisSpaceCharge3D->GetZaxis()->GetBinCenter(hisSpaceCharge3D->GetZaxis()->GetNbins()); | |
1418 | ||
1419 | for ( Int_t k = 0 ; k < kNPhi ; k++ ) { | |
1420 | phi = fgkPhiList[k] ; | |
1421 | TMatrixF &scDensity = *fSCdensityDistribution[k] ; | |
1422 | for ( Int_t j = 0 ; j < kNZ ; j++ ) { | |
1423 | z = fgkZList[j] ; | |
1424 | for ( Int_t i = 0 ; i < kNR ; i++ ) { | |
1425 | // Full 3D configuration ... | |
1426 | r = fgkRList[i] ; | |
1427 | if (r>rmin && r<rmax && z>zmin && z< zmax){ | |
1428 | // partial load in (r,z) | |
1429 | if (k==0) { | |
1430 | if (fSpaceChargeHistogramRZ) scDensityInRZ(i,j) = norm*fSpaceChargeHistogramRZ->Interpolate(r,z) ; | |
1431 | } | |
1432 | // partial load in (r,phi) | |
1433 | if ( (j==0 || j == kNZ/2) && fSpaceChargeHistogramRPhi) { | |
1434 | if (z>0) | |
1435 | scDensityInRPhiA(i,k) = norm*fSpaceChargeHistogramRPhi->Interpolate(phi,r); // A side | |
1436 | else | |
1437 | scDensityInRPhiC(i,k) = norm*fSpaceChargeHistogramRPhi->Interpolate(phi+TMath::TwoPi(),r); // C side | |
1438 | } | |
1439 | ||
1440 | if (z>0) | |
1441 | scDensity(i,j) = norm*fSpaceChargeHistogram3D->Interpolate(phi,r,z); | |
1442 | else | |
1443 | scDensity(i,j) = norm*fSpaceChargeHistogram3D->Interpolate(phi,r,z); | |
1444 | } | |
1445 | } | |
1446 | } | |
1447 | } | |
1448 | ||
1449 | fInitLookUp = kFALSE; | |
1450 | ||
1451 | } | |
1452 | ||
cc3e558a | 1453 | |
15687d71 | 1454 | Float_t AliTPCSpaceCharge3D::GetSpaceChargeDensity(Float_t r, Float_t phi, Float_t z, Int_t mode) { |
cc3e558a | 1455 | // |
1456 | // returns the (input) space charge density at a given point according | |
1457 | // Note: input in [cm], output in [C/m^3/e0] !! | |
1458 | // | |
1459 | ||
cc3e558a | 1460 | while (phi<0) phi += TMath::TwoPi(); |
1461 | while (phi>TMath::TwoPi()) phi -= TMath::TwoPi(); | |
1462 | ||
1463 | ||
1464 | // Float_t sc =fSCdensityDistribution->Interpolate(r0,phi0,z0); | |
1465 | Int_t order = 1; // | |
15687d71 | 1466 | Float_t sc = 0; |
cc3e558a | 1467 | |
15687d71 | 1468 | if (mode == 0) { // return full load |
1469 | sc = Interpolate3DTable(order, r, z, phi, kNR, kNZ, kNPhi, | |
1470 | fgkRList, fgkZList, fgkPhiList, fSCdensityDistribution ); | |
1471 | ||
1472 | } else if (mode == 1) { // return partial load in (r,z) | |
1473 | TMatrixD &scDensityInRZ = *fSCdensityInRZ; | |
1474 | sc = Interpolate2DTable(order, r, z, kNR, kNZ, fgkRList, fgkZList, scDensityInRZ ); | |
1475 | ||
1476 | } else if (mode == 2) { // return partial load in (r,phi) | |
1477 | ||
1478 | if (z>0) { | |
1479 | TMatrixD &scDensityInRPhi = *fSCdensityInRPhiA; | |
1480 | sc = Interpolate2DTable(order, r, phi, kNR, kNPhi, fgkRList, fgkPhiList, scDensityInRPhi ); | |
1481 | } else { | |
1482 | TMatrixD &scDensityInRPhi = *fSCdensityInRPhiC; | |
1483 | sc = Interpolate2DTable(order, r, phi, kNR, kNPhi, fgkRList, fgkPhiList, scDensityInRPhi ); | |
1484 | } | |
1485 | ||
1486 | } else { | |
1487 | // should i give a warning? | |
1488 | sc = 0; | |
1489 | } | |
1490 | ||
9f3b99e2 | 1491 | // printf("%f %f %f: %f\n",r,phi,z,sc); |
cc3e558a | 1492 | |
1493 | return sc; | |
1494 | } | |
1495 | ||
1496 | ||
15687d71 | 1497 | TH2F * AliTPCSpaceCharge3D::CreateHistoSCinXY(Float_t z, Int_t nx, Int_t ny, Int_t mode) { |
cc3e558a | 1498 | // |
1499 | // return a simple histogramm containing the space charge distribution (input for the calculation) | |
1500 | // | |
1501 | ||
1502 | TH2F *h=CreateTH2F("spaceCharge",GetTitle(),"x [cm]","y [cm]","#rho_{sc} [C/m^{3}/e_{0}]", | |
1503 | nx,-250.,250.,ny,-250.,250.); | |
1504 | ||
1505 | for (Int_t iy=1;iy<=ny;++iy) { | |
1506 | Double_t yp = h->GetYaxis()->GetBinCenter(iy); | |
1507 | for (Int_t ix=1;ix<=nx;++ix) { | |
1508 | Double_t xp = h->GetXaxis()->GetBinCenter(ix); | |
1509 | ||
1510 | Float_t r = TMath::Sqrt(xp*xp+yp*yp); | |
1511 | Float_t phi = TMath::ATan2(yp,xp); | |
1512 | ||
1513 | if (85.<=r && r<=250.) { | |
15687d71 | 1514 | Float_t sc = GetSpaceChargeDensity(r,phi,z,mode)/fgke0; // in [C/m^3/e0] |
cc3e558a | 1515 | h->SetBinContent(ix,iy,sc); |
1516 | } else { | |
1517 | h->SetBinContent(ix,iy,0.); | |
1518 | } | |
1519 | } | |
1520 | } | |
1521 | ||
1522 | return h; | |
1523 | } | |
1524 | ||
15687d71 | 1525 | TH2F * AliTPCSpaceCharge3D::CreateHistoSCinZR(Float_t phi, Int_t nz, Int_t nr,Int_t mode ) { |
cc3e558a | 1526 | // |
1527 | // return a simple histogramm containing the space charge distribution (input for the calculation) | |
1528 | // | |
1529 | ||
1530 | TH2F *h=CreateTH2F("spaceCharge",GetTitle(),"z [cm]","r [cm]","#rho_{sc} [C/m^{3}/e_{0}]", | |
1531 | nz,-250.,250.,nr,85.,250.); | |
1532 | ||
1533 | for (Int_t ir=1;ir<=nr;++ir) { | |
1534 | Float_t r = h->GetYaxis()->GetBinCenter(ir); | |
1535 | for (Int_t iz=1;iz<=nz;++iz) { | |
1536 | Float_t z = h->GetXaxis()->GetBinCenter(iz); | |
15687d71 | 1537 | Float_t sc = GetSpaceChargeDensity(r,phi,z,mode)/fgke0; // in [C/m^3/e0] |
cc3e558a | 1538 | h->SetBinContent(iz,ir,sc); |
1539 | } | |
1540 | } | |
1541 | ||
1542 | return h; | |
1543 | } | |
1544 | ||
1545 | void AliTPCSpaceCharge3D::WriteChargeDistributionToFile(const char* fname) { | |
1546 | // | |
1547 | // Example on how to write a Space charge distribution into a File | |
1548 | // (see below: estimate from scaling STAR measurements to Alice) | |
15687d71 | 1549 | // Charge distribution is splitted into two (RZ and RPHI) in order to speed up |
1550 | // the needed calculation time | |
cc3e558a | 1551 | // |
1552 | ||
1553 | TFile *f = new TFile(fname,"RECREATE"); | |
15687d71 | 1554 | |
cc3e558a | 1555 | // some grid, not too course |
15687d71 | 1556 | Int_t nr = 350; |
cc3e558a | 1557 | Int_t nphi = 180; |
15687d71 | 1558 | Int_t nz = 500; |
cc3e558a | 1559 | |
1560 | Double_t dr = (fgkOFCRadius-fgkIFCRadius)/(nr+1); | |
1561 | Double_t dphi = TMath::TwoPi()/(nphi+1); | |
1562 | Double_t dz = 500./(nz+1); | |
1563 | Double_t safty = 0.; // due to a root bug which does not interpolate the boundary (first and last bin) correctly | |
1564 | ||
15687d71 | 1565 | |
1566 | // Charge distribution in ZR (rotational symmetric) ------------------ | |
1567 | ||
1568 | TH2F *histoZR = new TH2F("chargeZR","chargeZR", | |
1569 | nr,fgkIFCRadius-dr-safty,fgkOFCRadius+dr+safty, | |
1570 | nz,-250-dz-safty,250+dz+safty); | |
cc3e558a | 1571 | |
1572 | for (Int_t ir=1;ir<=nr;++ir) { | |
15687d71 | 1573 | Double_t rp = histoZR->GetXaxis()->GetBinCenter(ir); |
1574 | for (Int_t iz=1;iz<=nz;++iz) { | |
1575 | Double_t zp = histoZR->GetYaxis()->GetBinCenter(iz); | |
1576 | ||
1577 | // recalculation to meter | |
1578 | Double_t lZ = 2.5; // approx. TPC drift length | |
1579 | Double_t rpM = rp/100.; // in [m] | |
1580 | Double_t zpM = TMath::Abs(zp/100.); // in [m] | |
1581 | ||
1582 | // setting of mb multiplicity and Interaction rate | |
1583 | Double_t multiplicity = 950; | |
1584 | Double_t intRate = 7800; | |
cc3e558a | 1585 | |
15687d71 | 1586 | // calculation of "scaled" parameters |
1587 | Double_t a = multiplicity*intRate/79175; | |
1588 | Double_t b = a/lZ; | |
1589 | ||
1590 | Double_t charge = (a - b*zpM)/(rpM*rpM); // charge in [C/m^3/e0] | |
cc3e558a | 1591 | |
15687d71 | 1592 | charge = charge*fgke0; // [C/m^3] |
cc3e558a | 1593 | |
15687d71 | 1594 | if (zp<0) charge *= 0.9; // e.g. slightly less on C side due to front absorber |
cc3e558a | 1595 | |
15687d71 | 1596 | // charge = 0; // for tests |
1597 | histoZR->SetBinContent(ir,iz,charge); | |
1598 | } | |
1599 | } | |
1600 | ||
1601 | histoZR->Write("SpaceChargeInRZ"); | |
1602 | ||
1603 | ||
1604 | // Charge distribution in RPhi (e.g. Floating GG wire) ------------ | |
1605 | ||
1606 | TH3F *histoRPhi = new TH3F("chargeRPhi","chargeRPhi", | |
1607 | nr,fgkIFCRadius-dr-safty,fgkOFCRadius+dr+safty, | |
1608 | nphi,0-dphi-safty,TMath::TwoPi()+dphi+safty, | |
1609 | 2,-1,1); // z part - to allow A and C side differences | |
1610 | ||
1611 | // some 'arbitrary' GG leaks | |
1612 | Int_t nGGleaks = 5; | |
1613 | Double_t secPosA[5] = {3,6,6,11,13}; // sector | |
752b0cc7 | 1614 | Double_t radialPosA[5] = {125,100,160,200,230}; // radius in cm |
1615 | Double_t secPosC[5] = {1,8,12,15,15}; // sector | |
1616 | Double_t radialPosC[5] = {245,120,140,120,190}; // radius in cm | |
15687d71 | 1617 | |
1618 | for (Int_t ir=1;ir<=nr;++ir) { | |
1619 | Double_t rp = histoRPhi->GetXaxis()->GetBinCenter(ir); | |
1620 | for (Int_t iphi=1;iphi<=nphi;++iphi) { | |
1621 | Double_t phip = histoRPhi->GetYaxis()->GetBinCenter(iphi); | |
1622 | for (Int_t iz=1;iz<=2;++iz) { | |
1623 | Double_t zp = histoRPhi->GetZaxis()->GetBinCenter(iz); | |
cc3e558a | 1624 | |
15687d71 | 1625 | Double_t charge = 0; |
1626 | ||
1627 | for (Int_t igg = 0; igg<nGGleaks; igg++) { // loop over GG leaks | |
1628 | ||
1629 | // A side | |
1630 | Double_t secPos = secPosA[igg]; | |
1631 | Double_t radialPos = radialPosA[igg]; | |
1632 | ||
1633 | if (zp<0) { // C side | |
1634 | secPos = secPosC[igg]; | |
1635 | radialPos = radialPosC[igg]; | |
1636 | } | |
1637 | ||
1638 | // some 'arbitrary' GG leaks | |
1639 | if ( (phip<(TMath::Pi()/9*(secPos+1)) && phip>(TMath::Pi()/9*secPos) ) ) { // sector slice | |
1640 | if ( rp>(radialPos-2.5) && rp<(radialPos+2.5)) // 5 cm slice | |
1641 | charge = 300; | |
1642 | } | |
1643 | ||
1644 | } | |
cc3e558a | 1645 | |
cc3e558a | 1646 | charge = charge*fgke0; // [C/m^3] |
1647 | ||
15687d71 | 1648 | histoRPhi->SetBinContent(ir,iphi,iz,charge); |
cc3e558a | 1649 | } |
1650 | } | |
1651 | } | |
1652 | ||
15687d71 | 1653 | histoRPhi->Write("SpaceChargeInRPhi"); |
cc3e558a | 1654 | |
cc3e558a | 1655 | f->Close(); |
1656 | ||
1657 | } | |
1658 | ||
1659 | ||
1660 | void AliTPCSpaceCharge3D::Print(const Option_t* option) const { | |
1661 | // | |
1662 | // Print function to check the settings of the boundary vectors | |
1663 | // option=="a" prints the C0 and C1 coefficents for calibration purposes | |
1664 | // | |
1665 | ||
1666 | TString opt = option; opt.ToLower(); | |
1667 | printf("%s\n",GetTitle()); | |
1668 | printf(" - Space Charge effect with arbitrary 3D charge density (as input).\n"); | |
1669 | printf(" SC correction factor: %f \n",fCorrectionFactor); | |
1670 | ||
1671 | if (opt.Contains("a")) { // Print all details | |
1672 | printf(" - T1: %1.4f, T2: %1.4f \n",fT1,fT2); | |
1673 | printf(" - C1: %1.4f, C0: %1.4f \n",fC1,fC0); | |
1674 | } | |
1675 | ||
1676 | if (!fInitLookUp) AliError("Lookup table was not initialized! You should do InitSpaceCharge3DDistortion() ..."); | |
1677 | ||
92a85338 | 1678 | } |
1679 | ||
1680 | ||
1681 | ||
1682 | void AliTPCSpaceCharge3D::InitSpaceCharge3DPoisson(Int_t kRows, Int_t kColumns, Int_t kPhiSlices, Int_t kIterations){ | |
1683 | // | |
1684 | // MI extension - calculate E field | |
1685 | // - inspired by AliTPCROCVoltError3D::InitROCVoltError3D() | |
1686 | // Initialization of the Lookup table which contains the solutions of the | |
1687 | // Dirichlet boundary problem | |
1688 | // Calculation of the single 3D-Poisson solver is done just if needed | |
1689 | // (see basic lookup tables in header file) | |
1690 | // | |
1691 | Int_t kPhiSlicesPerSector = kPhiSlices/18; | |
1692 | // | |
1693 | const Int_t order = 1 ; // Linear interpolation = 1, Quadratic = 2 | |
1694 | const Float_t gridSizeR = (fgkOFCRadius-fgkIFCRadius) / (kRows-1) ; | |
1695 | const Float_t gridSizeZ = fgkTPCZ0 / (kColumns-1) ; | |
1696 | const Float_t gridSizePhi = TMath::TwoPi() / ( 18.0 * kPhiSlicesPerSector); | |
1697 | ||
1698 | // temporary arrays to create the boundary conditions | |
1699 | TMatrixD *arrayofArrayV[kPhiSlices], *arrayofCharge[kPhiSlices] ; | |
1700 | TMatrixD *arrayofEroverEz[kPhiSlices], *arrayofEphioverEz[kPhiSlices], *arrayofDeltaEz[kPhiSlices] ; | |
1701 | ||
1702 | for ( Int_t k = 0 ; k < kPhiSlices ; k++ ) { | |
1703 | arrayofArrayV[k] = new TMatrixD(kRows,kColumns) ; | |
1704 | arrayofCharge[k] = new TMatrixD(kRows,kColumns) ; | |
1705 | arrayofEroverEz[k] = new TMatrixD(kRows,kColumns) ; | |
1706 | arrayofEphioverEz[k] = new TMatrixD(kRows,kColumns) ; | |
1707 | arrayofDeltaEz[k] = new TMatrixD(kRows,kColumns) ; | |
1708 | } | |
1709 | ||
1710 | // list of point as used in the poisson relation and the interpolation (during sum up) | |
1711 | Double_t rlist[kRows], zedlist[kColumns] , philist[kPhiSlices]; | |
1712 | for ( Int_t k = 0 ; k < kPhiSlices ; k++ ) { | |
1713 | philist[k] = gridSizePhi * k; | |
1714 | for ( Int_t i = 0 ; i < kRows ; i++ ) { | |
1715 | rlist[i] = fgkIFCRadius + i*gridSizeR ; | |
1716 | for ( Int_t j = 0 ; j < kColumns ; j++ ) { // Fill Vmatrix with Boundary Conditions | |
1717 | zedlist[j] = j * gridSizeZ ; | |
1718 | } | |
1719 | } | |
1720 | } | |
1721 | ||
1722 | // ========================================================================== | |
1723 | // Solve Poisson's equation in 3D cylindrical coordinates by relaxation technique | |
1724 | // Allow for different size grid spacing in R and Z directions | |
1725 | ||
1726 | const Int_t symmetry = 0; | |
1727 | ||
1728 | // Set bondaries and solve Poisson's equation -------------------------- | |
1729 | ||
1730 | if ( !fInitLookUp ) { | |
1731 | ||
1732 | AliInfo(Form("Solving the poisson equation (~ %d sec)",2*10*(int)(kPhiSlices/10))); | |
1733 | ||
1734 | for ( Int_t side = 0 ; side < 2 ; side++ ) { // Solve Poisson3D twice; once for +Z and once for -Z | |
1735 | AliSysInfo::AddStamp("RunSide", 1,side,0); | |
1736 | for ( Int_t k = 0 ; k < kPhiSlices ; k++ ) { | |
1737 | TMatrixD &arrayV = *arrayofArrayV[k] ; | |
1738 | TMatrixD &charge = *arrayofCharge[k] ; | |
1739 | ||
1740 | //Fill arrays with initial conditions. V on the boundary and Charge in the volume. | |
1741 | // for ( Int_t i = 0 ; i < kRows ; i++ ) { | |
1742 | // for ( Int_t j = 0 ; j < kColumns ; j++ ) { // Fill Vmatrix with Boundary Conditions | |
1743 | // arrayV(i,j) = 0.0 ; | |
1744 | // charge(i,j) = 0.0 ; | |
1745 | ||
1746 | // // Float_t radius0 = rlist[i] ; | |
1747 | // // Float_t phi0 = gridSizePhi * k ; | |
1748 | ||
1749 | // // To avoid problems at sector boundaries, use an average of +- 1 degree from actual phi location | |
1750 | // // if ( j == (kColumns-1) ) { | |
1751 | // // arrayV(i,j) = 0.5* ( GetROCVoltOffset( side, radius0, phi0+0.02 ) + GetROCVoltOffset( side, radius0, phi0-0.02 ) ) ; | |
1752 | ||
1753 | // // if (side==1) // C side | |
1754 | // // arrayV(i,j) = -arrayV(i,j); // minus sign on the C side to allow a consistent usage of global z when setting the boundaries | |
1755 | // // } | |
1756 | // } | |
1757 | // } | |
1758 | ||
1759 | for ( Int_t i = 1 ; i < kRows-1 ; i++ ) { | |
1760 | for ( Int_t j = 1 ; j < kColumns-1 ; j++ ) { | |
1761 | Float_t radius0 = rlist[i] ; | |
1762 | Float_t phi0 = gridSizePhi * k ; | |
1763 | Double_t z0 = zedlist[j]; | |
1764 | if (side==1) z0= -TMath::Abs(zedlist[j]); | |
1765 | arrayV(i,j) = 0.0 ; | |
1766 | charge(i,j) = fSpaceChargeHistogram3D->Interpolate(phi0,radius0,z0); | |
1767 | } | |
1768 | } | |
1769 | } | |
1770 | AliSysInfo::AddStamp("RunPoisson", 2,side,0); | |
1771 | ||
1772 | // Solve Poisson's equation in 3D cylindrical coordinates by relaxation technique | |
1773 | // Allow for different size grid spacing in R and Z directions | |
1774 | ||
1775 | // PoissonRelaxation3D( arrayofArrayV, arrayofCharge, | |
1776 | // arrayofEroverEz, arrayofEphioverEz, arrayofDeltaEz, | |
1777 | // kRows, kColumns, kPhiSlices, gridSizePhi, kIterations, | |
1778 | // symmetry , fROCdisplacement) ; | |
1779 | PoissonRelaxation3D( arrayofArrayV, arrayofCharge, | |
1780 | arrayofEroverEz, arrayofEphioverEz, arrayofDeltaEz, | |
1781 | kRows, kColumns, kPhiSlices, gridSizePhi, kIterations, | |
1782 | symmetry ) ; | |
1783 | ||
1784 | //Interpolate results onto a custom grid which is used just for these calculations. | |
1785 | Double_t r, phi, z ; | |
1786 | for ( Int_t k = 0 ; k < kNPhi ; k++ ) { | |
1787 | phi = fgkPhiList[k] ; | |
1788 | ||
1789 | TMatrixF &erOverEz = *fLookUpErOverEz[k] ; | |
1790 | TMatrixF &ephiOverEz = *fLookUpEphiOverEz[k]; | |
1791 | TMatrixF &deltaEz = *fLookUpDeltaEz[k] ; | |
1792 | ||
1793 | for ( Int_t j = 0 ; j < kNZ ; j++ ) { | |
1794 | ||
1795 | z = TMath::Abs(fgkZList[j]) ; // Symmetric solution in Z that depends only on ABS(Z) | |
1796 | ||
1797 | if ( side == 0 && fgkZList[j] < 0 ) continue; // Skip rest of this loop if on the wrong side | |
1798 | if ( side == 1 && fgkZList[j] > 0 ) continue; // Skip rest of this loop if on the wrong side | |
1799 | ||
1800 | for ( Int_t i = 0 ; i < kNR ; i++ ) { | |
1801 | r = fgkRList[i] ; | |
1802 | ||
1803 | // Interpolate basicLookup tables; once for each rod, then sum the results | |
1804 | erOverEz(i,j) = Interpolate3DTable(order, r, z, phi, kRows, kColumns, kPhiSlices, | |
1805 | rlist, zedlist, philist, arrayofEroverEz ); | |
1806 | ephiOverEz(i,j) = Interpolate3DTable(order, r, z, phi, kRows, kColumns, kPhiSlices, | |
1807 | rlist, zedlist, philist, arrayofEphioverEz); | |
1808 | deltaEz(i,j) = Interpolate3DTable(order, r, z, phi, kRows, kColumns, kPhiSlices, | |
1809 | rlist, zedlist, philist, arrayofDeltaEz ); | |
1810 | ||
1811 | if (side == 1) deltaEz(i,j) = - deltaEz(i,j); // negative coordinate system on C side | |
1812 | ||
1813 | } // end r loop | |
1814 | }// end z loop | |
1815 | }// end phi loop | |
1816 | AliSysInfo::AddStamp("Interpolate Poisson", 3,side,0); | |
1817 | if ( side == 0 ) AliInfo(" A side done"); | |
1818 | if ( side == 1 ) AliInfo(" C side done"); | |
1819 | } // end side loop | |
1820 | } | |
1821 | ||
1822 | // clear the temporary arrays lists | |
1823 | for ( Int_t k = 0 ; k < kPhiSlices ; k++ ) { | |
1824 | delete arrayofArrayV[k]; | |
1825 | delete arrayofCharge[k]; | |
1826 | delete arrayofEroverEz[k]; | |
1827 | delete arrayofEphioverEz[k]; | |
1828 | delete arrayofDeltaEz[k]; | |
1829 | } | |
1830 | ||
1831 | ||
1832 | fInitLookUp = kTRUE; | |
1833 | ||
cc3e558a | 1834 | } |
92a85338 | 1835 |