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