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1b923461 | 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> AliTPCBoundaryVoltError class </h2> | |
20 | // This class calculates the space point distortions due to residual voltage errors on | |
21 | // the main boundaries of the TPC. For example, the inner vessel of the TPC is shifted | |
22 | // by a certain amount, whereas the ROCs on the A side and the C side follow this mechanical | |
23 | // shift (at the inner vessel) in z direction. This example can be named "conical deformation" | |
24 | // of the TPC field cage (see example below). | |
25 | // <p> | |
26 | // The boundary conditions can be set via two arrays (A and C side) which contain the | |
27 | // residual voltage setting modeling a possible shift or an inhomogeneity on the TPC field | |
28 | // cage. In order to avoid that the user splits the Central Electrode (CE), the settings for | |
29 | // the C side is taken from the array on the A side (points: A.6 and A.7). The region betweem | |
30 | // the points is interpolated linearly onto the boundaries. | |
31 | // <p> | |
32 | // The class uses the PoissonRelaxation2D (see AliTPCCorrection) to calculate the resulting | |
33 | // electrical field inhomogeneities in the (r,z)-plane. Then, the Langevin-integral formalism | |
34 | // is used to calculate the space point distortions. <br> | |
35 | // Note: This class assumes a homogeneous magnetic field. | |
36 | // <p> | |
37 | // One has two possibilities when calculating the $dz$ distortions. The resulting distortions | |
38 | // are purely due to the change of the drift velocity (along with the change of the drift field) | |
39 | // when the SetROCDisplacement is FALSE. This emulates for example a Gating-Grid Voltage offset | |
40 | // without moving the ROCs. When the flag is set to TRUE, the ROCs are assumed to be misaligned | |
41 | // and the corresponding offset in z is added. | |
42 | // End_Html | |
43 | // | |
6a1caa6b | 44 | // Begin_Macro(source) |
b4caed64 | 45 | // { |
46 | // gROOT->SetStyle("Plain"); gStyle->SetPalette(1); | |
6a1caa6b | 47 | // TCanvas *c2 = new TCanvas("cAliTPCBoundaryVoltError","cAliTPCBoundaryVoltError",500,300); |
b4caed64 | 48 | // AliTPCBoundaryVoltError bve; |
49 | // Float_t val = 40;// [Volt]; 40V corresponds to 1mm | |
50 | // /* IFC shift, CE follows, ROC follows by factor half */ | |
51 | // Float_t boundA[8] = { val, val, val,0,0,0,0,val}; // voltages A-side | |
52 | // Float_t boundC[6] = {-val,-val,-val,0,0,0}; // voltages C-side | |
53 | // bve.SetBoundariesA(boundA); | |
54 | // bve.SetBoundariesC(boundC); | |
55 | // bve.SetOmegaTauT1T2(-0.32,1,1); | |
56 | // bve.SetROCDisplacement(kTRUE); // include the chamber offset in z when calculating the dz distortions | |
57 | // bve.CreateHistoDRinZR(0)->Draw("surf2"); | |
58 | // return c2; | |
59 | // } | |
60 | // End_Macro | |
61 | // | |
62 | // Begin_Html | |
63 | // <p> | |
64 | // Date: 01/06/2010 <br> | |
65 | // Authors: Jim Thomas, Stefan Rossegger | |
66 | // End_Html | |
67 | // _________________________________________________________________ | |
68 | ||
1b923461 | 69 | |
70 | #include "AliMagF.h" | |
71 | #include "TGeoGlobalMagField.h" | |
72 | #include "AliTPCcalibDB.h" | |
73 | #include "AliTPCParam.h" | |
74 | #include "AliLog.h" | |
75 | #include "TMatrixD.h" | |
76 | ||
77 | #include "TMath.h" | |
78 | #include "AliTPCROC.h" | |
79 | #include "AliTPCBoundaryVoltError.h" | |
80 | ||
81 | ClassImp(AliTPCBoundaryVoltError) | |
82 | ||
83 | AliTPCBoundaryVoltError::AliTPCBoundaryVoltError() | |
84 | : AliTPCCorrection("BoundaryVoltError","Boundary Voltage Error"), | |
85 | fC0(0.),fC1(0.), | |
c9cbd2f2 | 86 | fROCdisplacement(kTRUE), |
1b923461 | 87 | fInitLookUp(kFALSE) |
88 | { | |
89 | // | |
90 | // default constructor | |
91 | // | |
92 | for (Int_t i=0; i<8; i++){ | |
93 | fBoundariesA[i]= 0; | |
94 | if (i<6) fBoundariesC[i]= 0; | |
95 | } | |
96 | } | |
97 | ||
98 | AliTPCBoundaryVoltError::~AliTPCBoundaryVoltError() { | |
99 | // | |
100 | // default destructor | |
101 | // | |
102 | } | |
103 | ||
104 | ||
105 | ||
954a5d1b | 106 | |
107 | Bool_t AliTPCBoundaryVoltError::AddCorrectionCompact(AliTPCCorrection* corr, Double_t weight){ | |
108 | // | |
109 | // Add correction and make them compact | |
110 | // Assumptions: | |
111 | // - origin of distortion/correction are additive | |
112 | // - only correction ot the same type supported () | |
113 | if (corr==NULL) { | |
114 | AliError("Zerro pointer - correction"); | |
115 | return kFALSE; | |
116 | } | |
117 | AliTPCBoundaryVoltError* corrC = dynamic_cast<AliTPCBoundaryVoltError *>(corr); | |
118 | if (corrC == NULL) { | |
119 | AliError(TString::Format("Inconsistent class types: %s\%s",IsA()->GetName(),corr->IsA()->GetName()).Data()); | |
120 | return kFALSE; | |
121 | } | |
122 | if (fROCdisplacement!=corrC->fROCdisplacement){ | |
123 | AliError(TString::Format("Inconsistent fROCdisplacement : %s\%s",IsA()->GetName(),corr->IsA()->GetName()).Data()); | |
124 | return kFALSE; | |
125 | } | |
126 | for (Int_t i=0;i <8; i++){ | |
127 | fBoundariesA[i]+= corrC->fBoundariesA[i]*weight; | |
128 | fBoundariesC[i]+= corrC->fBoundariesC[i]*weight; | |
129 | } | |
130 | // | |
131 | return kTRUE; | |
132 | } | |
133 | ||
134 | ||
135 | ||
136 | ||
1b923461 | 137 | void AliTPCBoundaryVoltError::Init() { |
138 | // | |
139 | // Initialization funtion | |
140 | // | |
141 | ||
142 | AliMagF* magF= (AliMagF*)TGeoGlobalMagField::Instance()->GetField(); | |
143 | if (!magF) AliError("Magneticd field - not initialized"); | |
144 | Double_t bzField = magF->SolenoidField()/10.; //field in T | |
145 | AliTPCParam *param= AliTPCcalibDB::Instance()->GetParameters(); | |
146 | if (!param) AliError("Parameters - not initialized"); | |
147 | Double_t vdrift = param->GetDriftV()/1000000.; // [cm/us] // From dataBase: to be updated: per second (ideally) | |
148 | Double_t ezField = 400; // [V/cm] // to be updated: never (hopefully) | |
149 | Double_t wt = -10.0 * (bzField*10) * vdrift / ezField ; | |
150 | // Correction Terms for effective omegaTau; obtained by a laser calibration run | |
151 | SetOmegaTauT1T2(wt,fT1,fT2); | |
152 | ||
153 | InitBoundaryVoltErrorDistortion(); | |
154 | } | |
155 | ||
156 | void AliTPCBoundaryVoltError::Update(const TTimeStamp &/*timeStamp*/) { | |
157 | // | |
158 | // Update function | |
159 | // | |
160 | AliMagF* magF= (AliMagF*)TGeoGlobalMagField::Instance()->GetField(); | |
161 | if (!magF) AliError("Magneticd field - not initialized"); | |
162 | Double_t bzField = magF->SolenoidField()/10.; //field in T | |
163 | AliTPCParam *param= AliTPCcalibDB::Instance()->GetParameters(); | |
164 | if (!param) AliError("Parameters - not initialized"); | |
165 | Double_t vdrift = param->GetDriftV()/1000000.; // [cm/us] // From dataBase: to be updated: per second (ideally) | |
166 | Double_t ezField = 400; // [V/cm] // to be updated: never (hopefully) | |
167 | Double_t wt = -10.0 * (bzField*10) * vdrift / ezField ; | |
168 | // Correction Terms for effective omegaTau; obtained by a laser calibration run | |
169 | SetOmegaTauT1T2(wt,fT1,fT2); | |
170 | ||
1b923461 | 171 | } |
172 | ||
173 | ||
174 | ||
175 | void AliTPCBoundaryVoltError::GetCorrection(const Float_t x[],const Short_t roc,Float_t dx[]) { | |
176 | // | |
177 | // Calculates the correction due e.g. residual voltage errors on the TPC boundaries | |
178 | // | |
179 | ||
c9cbd2f2 | 180 | if (!fInitLookUp) { |
181 | AliInfo("Lookup table was not initialized! Perform the inizialisation now ..."); | |
182 | InitBoundaryVoltErrorDistortion(); | |
183 | } | |
1b923461 | 184 | |
185 | Int_t order = 1 ; // FIXME: hardcoded? Linear interpolation = 1, Quadratic = 2 | |
186 | // note that the poisson solution was linearly mirroed on this grid! | |
c9cbd2f2 | 187 | Double_t intEr, intEphi, intdEz ; |
1b923461 | 188 | Double_t r, phi, z ; |
189 | Int_t sign; | |
190 | ||
191 | r = TMath::Sqrt( x[0]*x[0] + x[1]*x[1] ) ; | |
192 | phi = TMath::ATan2(x[1],x[0]) ; | |
193 | if ( phi < 0 ) phi += TMath::TwoPi() ; // Table uses phi from 0 to 2*Pi | |
194 | z = x[2] ; // Create temporary copy of x[2] | |
195 | ||
196 | if ( (roc%36) < 18 ) { | |
197 | sign = 1; // (TPC A side) | |
198 | } else { | |
199 | sign = -1; // (TPC C side) | |
200 | } | |
201 | ||
202 | if ( sign==1 && z < fgkZOffSet ) z = fgkZOffSet; // Protect against discontinuity at CE | |
203 | if ( sign==-1 && z > -fgkZOffSet ) z = -fgkZOffSet; // Protect against discontinuity at CE | |
204 | ||
205 | ||
206 | intEphi = 0.0; // Efield is symmetric in phi - 2D calculation | |
207 | ||
208 | if ( (sign==1 && z<0) || (sign==-1 && z>0) ) // just a consistency check | |
209 | AliError("ROC number does not correspond to z coordinate! Calculation of distortions is most likely wrong!"); | |
210 | ||
211 | // Get the E field integral | |
212 | Interpolate2DEdistortion( order, r, z, fLookUpErOverEz, intEr ); | |
c9cbd2f2 | 213 | // Get DeltaEz field integral |
214 | Interpolate2DEdistortion( order, r, z, fLookUpDeltaEz, intdEz ); | |
1b923461 | 215 | |
216 | // Calculate distorted position | |
217 | if ( r > 0.0 ) { | |
218 | phi = phi + ( fC0*intEphi - fC1*intEr ) / r; | |
219 | r = r + ( fC0*intEr + fC1*intEphi ); | |
220 | } | |
221 | ||
222 | // Calculate correction in cartesian coordinates | |
223 | dx[0] = r * TMath::Cos(phi) - x[0]; | |
224 | dx[1] = r * TMath::Sin(phi) - x[1]; | |
c9cbd2f2 | 225 | dx[2] = intdEz; // z distortion - (internally scaled with driftvelocity dependency |
226 | // on the Ez field plus the actual ROC misalignment (if set TRUE) | |
227 | ||
1b923461 | 228 | |
229 | } | |
230 | ||
231 | void AliTPCBoundaryVoltError::InitBoundaryVoltErrorDistortion() { | |
232 | // | |
233 | // Initialization of the Lookup table which contains the solutions of the | |
234 | // Dirichlet boundary problem | |
235 | // | |
236 | ||
237 | const Float_t gridSizeR = (fgkOFCRadius-fgkIFCRadius) / (kRows-1) ; | |
238 | const Float_t gridSizeZ = fgkTPCZ0 / (kColumns-1) ; | |
239 | ||
240 | TMatrixD voltArrayA(kRows,kColumns), voltArrayC(kRows,kColumns); // boundary vectors | |
241 | TMatrixD chargeDensity(kRows,kColumns); // dummy charge | |
242 | TMatrixD arrayErOverEzA(kRows,kColumns), arrayErOverEzC(kRows,kColumns); // solution | |
c9cbd2f2 | 243 | TMatrixD arrayDeltaEzA(kRows,kColumns), arrayDeltaEzC(kRows,kColumns); // solution |
1b923461 | 244 | |
245 | Double_t rList[kRows], zedList[kColumns] ; | |
246 | ||
247 | // Fill arrays with initial conditions. V on the boundary and ChargeDensity in the volume. | |
248 | for ( Int_t j = 0 ; j < kColumns ; j++ ) { | |
249 | Double_t zed = j*gridSizeZ ; | |
250 | zedList[j] = zed ; | |
251 | for ( Int_t i = 0 ; i < kRows ; i++ ) { | |
252 | Double_t radius = fgkIFCRadius + i*gridSizeR ; | |
253 | rList[i] = radius ; | |
254 | voltArrayA(i,j) = 0; // Initialize voltArrayA to zero | |
255 | voltArrayC(i,j) = 0; // Initialize voltArrayC to zero | |
256 | chargeDensity(i,j) = 0; // Initialize ChargeDensity to zero - not used in this class | |
257 | } | |
258 | } | |
259 | ||
260 | ||
261 | // check if boundary values are the same for the C side (for later, saving some calculation time) | |
262 | ||
263 | Int_t symmetry = -1; // assume that A and C side are identical (but anti-symmetric!) // e.g conical deformation | |
264 | Int_t sVec[8]; | |
265 | ||
266 | // check if boundaries are different (regardless the sign) | |
267 | for (Int_t i=0; i<8; i++) { | |
35108d57 | 268 | if (TMath::Abs(TMath::Abs(fBoundariesA[i]) - TMath::Abs(fBoundariesC[i])) > 1e-5) |
269 | symmetry = 0; | |
270 | sVec[i] = (Int_t)( TMath::Sign((Float_t)1.,fBoundariesA[i]) * TMath::Sign((Float_t)1.,fBoundariesC[i])); | |
1b923461 | 271 | } |
272 | if (symmetry==-1) { // still the same values? | |
273 | // check the kind of symmetry , if even ... | |
274 | if (sVec[0]==1 && sVec[1]==1 && sVec[2]==1 && sVec[3]==1 && sVec[4]==1 && sVec[5]==1 && sVec[6]==1 && sVec[7]==1 ) | |
275 | symmetry = 1; | |
276 | else if (sVec[0]==-1 && sVec[1]==-1 && sVec[2]==-1 && sVec[3]==-1 && sVec[4]==-1 && sVec[5]==-1 && sVec[6]==-1 && sVec[7]==-1 ) | |
277 | symmetry = -1; | |
278 | else | |
279 | symmetry = 0; // some of the values differ in the sign -> neither symmetric nor antisymmetric | |
280 | } | |
281 | ||
282 | ||
283 | ||
284 | // Solve the electrosatic problem in 2D | |
285 | ||
286 | // Fill the complete Boundary vectors | |
287 | // Start at IFC at CE and work anti-clockwise through IFC, ROC, OFC, and CE (clockwise for C side) | |
288 | for ( Int_t j = 0 ; j < kColumns ; j++ ) { | |
289 | Double_t zed = j*gridSizeZ ; | |
290 | for ( Int_t i = 0 ; i < kRows ; i++ ) { | |
291 | Double_t radius = fgkIFCRadius + i*gridSizeR ; | |
292 | ||
293 | // A side boundary vectors | |
294 | if ( i == 0 ) voltArrayA(i,j) += zed *((fBoundariesA[1]-fBoundariesA[0])/((kColumns-1)*gridSizeZ)) | |
295 | + fBoundariesA[0] ; // IFC | |
c9cbd2f2 | 296 | if ( j == kColumns-1 ) voltArrayA(i,j) += (radius-fgkIFCRadius)*((fBoundariesA[3]-fBoundariesA[2])/((kRows-1)*gridSizeR)) |
1b923461 | 297 | + fBoundariesA[2] ; // ROC |
298 | if ( i == kRows-1 ) voltArrayA(i,j) += zed *((fBoundariesA[4]-fBoundariesA[5])/((kColumns-1)*gridSizeZ)) | |
299 | + fBoundariesA[5] ; // OFC | |
c9cbd2f2 | 300 | if ( j == 0 ) voltArrayA(i,j) += (radius-fgkIFCRadius)*((fBoundariesA[6]-fBoundariesA[7])/((kRows-1)*gridSizeR)) |
1b923461 | 301 | + fBoundariesA[7] ; // CE |
c9cbd2f2 | 302 | |
1b923461 | 303 | if (symmetry==0) { |
304 | // C side boundary vectors | |
305 | if ( i == 0 ) voltArrayC(i,j) += zed *((fBoundariesC[1]-fBoundariesC[0])/((kColumns-1)*gridSizeZ)) | |
306 | + fBoundariesC[0] ; // IFC | |
c9cbd2f2 | 307 | if ( j == kColumns-1 ) voltArrayC(i,j) += (radius-fgkIFCRadius)*((fBoundariesC[3]-fBoundariesC[2])/((kRows-1)*gridSizeR)) |
1b923461 | 308 | + fBoundariesC[2] ; // ROC |
309 | if ( i == kRows-1 ) voltArrayC(i,j) += zed *((fBoundariesC[4]-fBoundariesC[5])/((kColumns-1)*gridSizeZ)) | |
310 | + fBoundariesC[5] ; // OFC | |
c9cbd2f2 | 311 | if ( j == 0 ) voltArrayC(i,j) += (radius-fgkIFCRadius)*((fBoundariesC[6]-fBoundariesC[7])/((kRows-1)*gridSizeR)) |
1b923461 | 312 | + fBoundariesC[7] ; // CE |
1b923461 | 313 | } |
c9cbd2f2 | 314 | |
1b923461 | 315 | } |
316 | } | |
317 | ||
318 | voltArrayA(0,0) *= 0.5 ; // Use average boundary condition at corner | |
319 | voltArrayA(kRows-1,0) *= 0.5 ; // Use average boundary condition at corner | |
320 | voltArrayA(0,kColumns-1) *= 0.5 ; // Use average boundary condition at corner | |
321 | voltArrayA(kRows-1,kColumns-1)*= 0.5 ; // Use average boundary condition at corner | |
322 | ||
323 | if (symmetry==0) { | |
324 | voltArrayC(0,0) *= 0.5 ; // Use average boundary condition at corner | |
325 | voltArrayC(kRows-1,0) *= 0.5 ; // Use average boundary condition at corner | |
326 | voltArrayC(0,kColumns-1) *= 0.5 ; // Use average boundary condition at corner | |
327 | voltArrayC(kRows-1,kColumns-1)*= 0.5 ; // Use average boundary condition at corner | |
328 | } | |
329 | ||
330 | ||
331 | // always solve the problem on the A side | |
c9cbd2f2 | 332 | PoissonRelaxation2D( voltArrayA, chargeDensity, arrayErOverEzA, arrayDeltaEzA, |
333 | kRows, kColumns, kIterations, fROCdisplacement ) ; | |
1b923461 | 334 | |
335 | if (symmetry!=0) { // A and C side are the same ("anti-symmetric" or "symmetric") | |
336 | for ( Int_t j = 0 ; j < kColumns ; j++ ) { | |
337 | for ( Int_t i = 0 ; i < kRows ; i++ ) { | |
338 | arrayErOverEzC(i,j) = symmetry*arrayErOverEzA(i,j); | |
c9cbd2f2 | 339 | arrayDeltaEzC(i,j) = -symmetry*arrayDeltaEzA(i,j); |
1b923461 | 340 | } |
341 | } | |
342 | } else if (symmetry==0) { // A and C side are different - Solve the problem on the C side too | |
c9cbd2f2 | 343 | PoissonRelaxation2D( voltArrayC, chargeDensity, arrayErOverEzC, arrayDeltaEzC, |
344 | kRows, kColumns, kIterations, fROCdisplacement ) ; | |
345 | for ( Int_t j = 0 ; j < kColumns ; j++ ) { | |
346 | for ( Int_t i = 0 ; i < kRows ; i++ ) { | |
347 | arrayDeltaEzC(i,j) = -arrayDeltaEzC(i,j); // negative z coordinate! | |
348 | } | |
349 | } | |
1b923461 | 350 | } |
351 | ||
35108d57 | 352 | // Interpolate results onto standard grid for Electric Fields |
1b923461 | 353 | Int_t ilow=0, jlow=0 ; |
354 | Double_t z,r; | |
355 | Float_t saveEr[2] ; | |
c9cbd2f2 | 356 | Float_t saveEz[2] ; |
1b923461 | 357 | for ( Int_t i = 0 ; i < kNZ ; ++i ) { |
358 | z = TMath::Abs( fgkZList[i] ) ; | |
359 | for ( Int_t j = 0 ; j < kNR ; ++j ) { | |
360 | // Linear interpolation !! | |
361 | r = fgkRList[j] ; | |
c9cbd2f2 | 362 | Search( kRows, rList, r, ilow ) ; // Note switch - R in rows and Z in columns |
363 | Search( kColumns, zedList, z, jlow ) ; | |
364 | if ( ilow < 0 ) ilow = 0 ; // check if out of range | |
365 | if ( jlow < 0 ) jlow = 0 ; | |
366 | if ( ilow + 1 >= kRows - 1 ) ilow = kRows - 2 ; | |
367 | if ( jlow + 1 >= kColumns - 1 ) jlow = kColumns - 2 ; | |
368 | ||
369 | if (fgkZList[i]>0) { // A side solution | |
370 | saveEr[0] = arrayErOverEzA(ilow,jlow) + | |
371 | (arrayErOverEzA(ilow,jlow+1)-arrayErOverEzA(ilow,jlow))*(z-zedList[jlow])/gridSizeZ ; | |
372 | saveEr[1] = arrayErOverEzA(ilow+1,jlow) + | |
373 | (arrayErOverEzA(ilow+1,jlow+1)-arrayErOverEzA(ilow+1,jlow))*(z-zedList[jlow])/gridSizeZ ; | |
374 | saveEz[0] = arrayDeltaEzA(ilow,jlow) + | |
375 | (arrayDeltaEzA(ilow,jlow+1)-arrayDeltaEzA(ilow,jlow))*(z-zedList[jlow])/gridSizeZ ; | |
376 | saveEz[1] = arrayDeltaEzA(ilow+1,jlow) + | |
377 | (arrayDeltaEzA(ilow+1,jlow+1)-arrayDeltaEzA(ilow+1,jlow))*(z-zedList[jlow])/gridSizeZ ; | |
378 | ||
379 | } else if (fgkZList[i]<0) { // C side solution | |
380 | saveEr[0] = arrayErOverEzC(ilow,jlow) + | |
381 | (arrayErOverEzC(ilow,jlow+1)-arrayErOverEzC(ilow,jlow))*(z-zedList[jlow])/gridSizeZ ; | |
382 | saveEr[1] = arrayErOverEzC(ilow+1,jlow) + | |
383 | (arrayErOverEzC(ilow+1,jlow+1)-arrayErOverEzC(ilow+1,jlow))*(z-zedList[jlow])/gridSizeZ ; | |
384 | saveEz[0] = arrayDeltaEzC(ilow,jlow) + | |
385 | (arrayDeltaEzC(ilow,jlow+1)-arrayDeltaEzC(ilow,jlow))*(z-zedList[jlow])/gridSizeZ ; | |
386 | saveEz[1] = arrayDeltaEzC(ilow+1,jlow) + | |
387 | (arrayDeltaEzC(ilow+1,jlow+1)-arrayDeltaEzC(ilow+1,jlow))*(z-zedList[jlow])/gridSizeZ ; | |
388 | ||
389 | } else { | |
390 | AliWarning("Field calculation at z=0 (CE) is not allowed!"); | |
391 | saveEr[0]=0; saveEr[1]=0; | |
392 | saveEz[0]=0; saveEz[1]=0; | |
1b923461 | 393 | } |
c9cbd2f2 | 394 | fLookUpErOverEz[i][j] = saveEr[0] + (saveEr[1]-saveEr[0])*(r-rList[ilow])/gridSizeR ; |
395 | fLookUpDeltaEz[i][j] = saveEz[0] + (saveEz[1]-saveEz[0])*(r-rList[ilow])/gridSizeR ; | |
396 | } | |
1b923461 | 397 | } |
398 | ||
c9cbd2f2 | 399 | voltArrayA.Clear(); |
400 | voltArrayC.Clear(); | |
401 | chargeDensity.Clear(); | |
402 | arrayErOverEzA.Clear(); | |
403 | arrayErOverEzC.Clear(); | |
404 | arrayDeltaEzA.Clear(); | |
405 | arrayDeltaEzC.Clear(); | |
406 | ||
1b923461 | 407 | fInitLookUp = kTRUE; |
408 | ||
409 | } | |
410 | ||
411 | void AliTPCBoundaryVoltError::Print(const Option_t* option) const { | |
412 | // | |
413 | // Print function to check the settings of the boundary vectors | |
414 | // option=="a" prints the C0 and C1 coefficents for calibration purposes | |
415 | // | |
416 | ||
417 | TString opt = option; opt.ToLower(); | |
418 | printf("%s\n",GetTitle()); | |
419 | printf(" - Voltage settings (on the TPC boundaries) - linearly interpolated\n"); | |
420 | printf(" : A-side (anti-clockwise)\n"); | |
421 | printf(" (0,1):\t IFC (CE) : %3.1f V \t IFC (ROC): %3.1f V \n",fBoundariesA[0],fBoundariesA[1]); | |
422 | printf(" (2,3):\t ROC (IFC): %3.1f V \t ROC (OFC): %3.1f V \n",fBoundariesA[2],fBoundariesA[3]); | |
423 | printf(" (4,5):\t OFC (ROC): %3.1f V \t OFC (CE) : %3.1f V \n",fBoundariesA[4],fBoundariesA[5]); | |
424 | printf(" (6,7):\t CE (OFC): %3.1f V \t CE (IFC): %3.1f V \n",fBoundariesA[6],fBoundariesA[7]); | |
425 | printf(" : C-side (clockwise)\n"); | |
426 | printf(" (0,1):\t IFC (CE) : %3.1f V \t IFC (ROC): %3.1f V \n",fBoundariesC[0],fBoundariesC[1]); | |
427 | printf(" (2,3):\t ROC (IFC): %3.1f V \t ROC (OFC): %3.1f V \n",fBoundariesC[2],fBoundariesC[3]); | |
428 | printf(" (4,5):\t OFC (ROC): %3.1f V \t OFC (CE) : %3.1f V \n",fBoundariesC[4],fBoundariesC[5]); | |
429 | printf(" (6,7):\t CE (OFC): %3.1f V \t CE (IFC): %3.1f V \n",fBoundariesC[6],fBoundariesC[7]); | |
430 | ||
431 | // Check wether the settings of the Central Electrode agree (on the A and C side) | |
432 | // Note: they have to be antisymmetric! | |
433 | if (( TMath::Abs(fBoundariesA[6]+fBoundariesC[6])>1e-5) || ( TMath::Abs(fBoundariesA[7]+fBoundariesC[7])>1e-5 ) ){ | |
434 | AliWarning("Boundary parameters for the Central Electrode (CE) are not anti-symmetric! HOW DID YOU MANAGE THAT?"); | |
435 | AliWarning("Congratulations, you just splitted the Central Electrode of the TPC!"); | |
436 | AliWarning("Non-physical settings of the boundary parameter at the Central Electrode"); | |
437 | } | |
438 | ||
439 | if (opt.Contains("a")) { // Print all details | |
440 | printf(" - T1: %1.4f, T2: %1.4f \n",fT1,fT2); | |
441 | printf(" - C1: %1.4f, C0: %1.4f \n",fC1,fC0); | |
442 | } | |
443 | ||
c9cbd2f2 | 444 | if (!fInitLookUp) |
445 | AliError("Lookup table was not initialized! You should do InitBoundaryVoltErrorDistortion() ..."); | |
1b923461 | 446 | |
447 | } | |
448 | ||
449 | ||
450 | void AliTPCBoundaryVoltError::SetBoundariesA(Float_t boundariesA[8]){ | |
451 | // | |
452 | // set voltage errors on the TPC boundaries - A side | |
453 | // | |
454 | // Start at IFC at the Central electrode and work anti-clockwise (clockwise for C side) through | |
455 | // IFC, ROC, OFC, and CE. The boundary conditions are currently defined to be a linear | |
456 | // interpolation between pairs of numbers in the Boundary (e.g. fBoundariesA) vector. | |
457 | // The first pair of numbers represent the beginning and end of the Inner Field cage, etc. | |
458 | // The unit of the error potential vector is [Volt], whereas 1mm shift of the IFC would | |
459 | // correspond to ~ 40 V | |
460 | // | |
461 | // Note: The setting for the CE will be passed to the C side! | |
462 | ||
463 | for (Int_t i=0; i<8; i++) { | |
464 | fBoundariesA[i]= boundariesA[i]; | |
465 | if (i>5) fBoundariesC[i]= -boundariesA[i]; // setting for the CE is passed to C side | |
466 | } | |
c9cbd2f2 | 467 | fInitLookUp=kFALSE; |
1b923461 | 468 | } |
469 | void AliTPCBoundaryVoltError::SetBoundariesC(Float_t boundariesC[6]){ | |
470 | // | |
c9cbd2f2 | 471 | // set voltage errors on the TPC boundaries - C side |
1b923461 | 472 | // |
473 | // Start at IFC at the Central electrode and work clockwise (for C side) through | |
474 | // IFC, ROC and OFC. The boundary conditions are currently defined to be a linear | |
475 | // interpolation between pairs of numbers in the Boundary (e.g. fBoundariesC) vector. | |
476 | // The first pair of numbers represent the beginning and end of the Inner Field cage, etc. | |
477 | // The unit of the error potential vector is [Volt], whereas 1mm shift of the IFC would | |
478 | // correspond to ~ 40 V | |
479 | // | |
480 | // Note: The setting for the CE will be taken from the A side (pos 6 and 7)! | |
481 | ||
482 | for (Int_t i=0; i<6; i++) { | |
483 | fBoundariesC[i]= boundariesC[i]; | |
484 | } | |
c9cbd2f2 | 485 | fInitLookUp=kFALSE; |
1b923461 | 486 | } |