]>
Commit | Line | Data |
---|---|---|
4c039060 | 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 | ||
4c039060 | 16 | |
db83d72f | 17 | #include <TClass.h> |
18 | #include <TFile.h> | |
19 | #include <TSystem.h> | |
33fe5eb1 | 20 | #include <TPRegexp.h> |
fe4da5cc | 21 | |
22 | #include "AliMagF.h" | |
db83d72f | 23 | #include "AliMagWrapCheb.h" |
24 | #include "AliLog.h" | |
972ca52f | 25 | |
fe4da5cc | 26 | ClassImp(AliMagF) |
27 | ||
9251fceb | 28 | const Double_t AliMagF::fgkSol2DipZ = -700.; |
1dd3d90e | 29 | const UShort_t AliMagF::fgkPolarityConvention = kConvLHC; |
db83d72f | 30 | |
1dd3d90e | 31 | /* |
32 | Explanation for polarity conventions: these are the mapping between the | |
33 | current signs and main field components in L3 (Bz) and Dipole (Bx) (in Alice frame) | |
34 | 1) kConvMap2005: used for the field mapping in 2005 | |
35 | positive L3 current -> negative Bz | |
36 | positive Dip current -> positive Bx | |
37 | 2) kConvMapDCS2008: defined by the microswitches/cabling of power converters as of 2008 - 1st half 2009 | |
38 | positive L3 current -> positive Bz | |
39 | positive Dip current -> positive Bx | |
40 | 3) kConvLHC : defined by LHC | |
41 | positive L3 current -> negative Bz | |
42 | positive Dip current -> negative Bx | |
43 | ||
44 | Note: only "negative Bz(L3) with postive Bx(Dipole)" and its inverse was mapped in 2005. Hence | |
45 | the GRP Manager will reject the runs with the current combinations (in the convention defined by the | |
46 | static Int_t AliMagF::GetPolarityConvention()) which do not lead to such field polarities. | |
47 | */ | |
e2afb3b6 | 48 | //_______________________________________________________________________ |
49 | AliMagF::AliMagF(): | |
db83d72f | 50 | TVirtualMagField(), |
51 | fMeasuredMap(0), | |
52 | fMapType(k5kG), | |
53 | fSolenoid(0), | |
54 | fBeamType(kNoBeamField), | |
55 | fBeamEnergy(0), | |
db83d72f | 56 | // |
e2afb3b6 | 57 | fInteg(0), |
db83d72f | 58 | fPrecInteg(0), |
59 | fFactorSol(1.), | |
60 | fFactorDip(1.), | |
61 | fMax(15), | |
62 | fDipoleOFF(kFALSE), | |
e2afb3b6 | 63 | // |
db83d72f | 64 | fQuadGradient(0), |
65 | fDipoleField(0), | |
66 | fCCorrField(0), | |
67 | fACorr1Field(0), | |
68 | fACorr2Field(0), | |
69 | fParNames("","") | |
70 | { | |
e2afb3b6 | 71 | // Default constructor |
72 | // | |
73 | } | |
74 | ||
75 | //_______________________________________________________________________ | |
4642ac4b | 76 | AliMagF::AliMagF(const char *name, const char* title, Double_t factorSol, Double_t factorDip, |
77 | BMap_t maptype, BeamType_t btype, Double_t benergy, Int_t integ, Double_t fmax, | |
78 | const char* path): | |
db83d72f | 79 | TVirtualMagField(name), |
80 | fMeasuredMap(0), | |
81 | fMapType(maptype), | |
82 | fSolenoid(0), | |
4642ac4b | 83 | fBeamType(btype), |
84 | fBeamEnergy(benergy), | |
db83d72f | 85 | // |
86 | fInteg(integ), | |
604e0531 | 87 | fPrecInteg(1), |
db83d72f | 88 | fFactorSol(1.), |
89 | fFactorDip(1.), | |
972ca52f | 90 | fMax(fmax), |
db83d72f | 91 | fDipoleOFF(factorDip==0.), |
92 | // | |
93 | fQuadGradient(0), | |
94 | fDipoleField(0), | |
95 | fCCorrField(0), | |
96 | fACorr1Field(0), | |
97 | fACorr2Field(0), | |
98 | fParNames("","") | |
fe4da5cc | 99 | { |
9251fceb | 100 | // Initialize the field with Geant integration option "integ" and max field "fmax, |
101 | // Impose scaling of parameterized L3 field by factorSol and of dipole by factorDip. | |
102 | // The "be" is the energy of the beam in GeV/nucleon | |
aee8290b | 103 | // |
db83d72f | 104 | SetTitle(title); |
105 | if(integ<0 || integ > 2) { | |
106 | AliWarning(Form("Invalid magnetic field flag: %5d; Helix tracking chosen instead",integ)); | |
107 | fInteg = 2; | |
108 | } | |
109 | if (fInteg == 0) fPrecInteg = 0; | |
aee8290b | 110 | // |
4642ac4b | 111 | if (fBeamEnergy<=0 && fBeamType!=kNoBeamField) { |
112 | if (fBeamType == kBeamTypepp) fBeamEnergy = 7000.; // max proton energy | |
113 | else if (fBeamType == kBeamTypeAA) fBeamEnergy = 5500; // max PbPb energy | |
114 | AliInfo("Maximim possible beam energy for requested beam is assumed"); | |
115 | } | |
db83d72f | 116 | const char* parname = 0; |
117 | // | |
f04e7f5f | 118 | if (fMapType == k2kG) parname = fDipoleOFF ? "Sol12_Dip0_Hole":"Sol12_Dip6_Hole"; |
119 | else if (fMapType == k5kG) parname = fDipoleOFF ? "Sol30_Dip0_Hole":"Sol30_Dip6_Hole"; | |
120 | else if (fMapType == k5kGUniform) parname = "Sol30_Dip6_Uniform"; | |
121 | else AliFatal(Form("Unknown field identifier %d is requested\n",fMapType)); | |
db83d72f | 122 | // |
123 | SetDataFileName(path); | |
124 | SetParamName(parname); | |
125 | // | |
db83d72f | 126 | LoadParameterization(); |
127 | InitMachineField(fBeamType,fBeamEnergy); | |
f04e7f5f | 128 | double xyz[3]={0.,0.,0.}; |
129 | fSolenoid = GetBz(xyz); | |
130 | SetFactorSol(factorSol); | |
131 | SetFactorDip(factorDip); | |
e86708b3 | 132 | AliInfo(Form("Alice B fields: Solenoid (%+.2f*)%.0f kG, Dipole %s (%+.2f) %s", |
133 | factorSol,(fMapType==k5kG||fMapType==k5kGUniform)?5.:2., | |
439b5096 | 134 | fDipoleOFF ? "OFF":"ON",factorDip,fMapType==k5kGUniform?" |Constant Field!":"")); |
135 | AliInfo(Form("Machine B fields for %s beam (%.0f GeV): QGrad: %.4f Dipole: %.4f", | |
4642ac4b | 136 | fBeamType==kBeamTypeAA ? "A-A":(fBeamType==kBeamTypepp ? "p-p":"OFF"), |
137 | fBeamEnergy,fQuadGradient,fDipoleField)); | |
fe4da5cc | 138 | } |
139 | ||
eeda4611 | 140 | //_______________________________________________________________________ |
141 | AliMagF::AliMagF(const AliMagF &src): | |
db83d72f | 142 | TVirtualMagField(src), |
143 | fMeasuredMap(0), | |
144 | fMapType(src.fMapType), | |
145 | fSolenoid(src.fSolenoid), | |
146 | fBeamType(src.fBeamType), | |
147 | fBeamEnergy(src.fBeamEnergy), | |
eeda4611 | 148 | fInteg(src.fInteg), |
149 | fPrecInteg(src.fPrecInteg), | |
db83d72f | 150 | fFactorSol(src.fFactorSol), |
151 | fFactorDip(src.fFactorDip), | |
eeda4611 | 152 | fMax(src.fMax), |
db83d72f | 153 | fDipoleOFF(src.fDipoleOFF), |
154 | fQuadGradient(src.fQuadGradient), | |
155 | fDipoleField(src.fDipoleField), | |
156 | fCCorrField(src.fCCorrField), | |
157 | fACorr1Field(src.fACorr1Field), | |
158 | fACorr2Field(src.fACorr2Field), | |
159 | fParNames(src.fParNames) | |
eeda4611 | 160 | { |
db83d72f | 161 | if (src.fMeasuredMap) fMeasuredMap = new AliMagWrapCheb(*src.fMeasuredMap); |
eeda4611 | 162 | } |
163 | ||
e2afb3b6 | 164 | //_______________________________________________________________________ |
db83d72f | 165 | AliMagF::~AliMagF() |
ff66b122 | 166 | { |
db83d72f | 167 | delete fMeasuredMap; |
168 | } | |
169 | ||
170 | //_______________________________________________________________________ | |
171 | Bool_t AliMagF::LoadParameterization() | |
172 | { | |
173 | if (fMeasuredMap) { | |
174 | AliError(Form("Field data %s are already loaded from %s\n",GetParamName(),GetDataFileName())); | |
175 | return kTRUE; | |
176 | } | |
ff66b122 | 177 | // |
db83d72f | 178 | char* fname = gSystem->ExpandPathName(GetDataFileName()); |
179 | TFile* file = TFile::Open(fname); | |
180 | if (!file) { | |
181 | AliError(Form("Failed to open magnetic field data file %s\n",fname)); | |
182 | return kFALSE; | |
183 | } | |
ff66b122 | 184 | // |
db83d72f | 185 | fMeasuredMap = dynamic_cast<AliMagWrapCheb*>(file->Get(GetParamName())); |
186 | if (!fMeasuredMap) { | |
187 | AliError(Form("Did not find field %s in %s\n",GetParamName(),fname)); | |
188 | return kFALSE; | |
189 | } | |
190 | file->Close(); | |
191 | delete file; | |
192 | return kTRUE; | |
ff66b122 | 193 | } |
194 | ||
db83d72f | 195 | |
ff66b122 | 196 | //_______________________________________________________________________ |
db83d72f | 197 | void AliMagF::Field(const Double_t *xyz, Double_t *b) |
fe4da5cc | 198 | { |
db83d72f | 199 | // Method to calculate the field at point xyz |
aee8290b | 200 | // |
9251fceb | 201 | // b[0]=b[1]=b[2]=0.0; |
202 | if (fMeasuredMap && xyz[2]>fMeasuredMap->GetMinZ() && xyz[2]<fMeasuredMap->GetMaxZ()) { | |
db83d72f | 203 | fMeasuredMap->Field(xyz,b); |
204 | if (xyz[2]>fgkSol2DipZ || fDipoleOFF) for (int i=3;i--;) b[i] *= fFactorSol; | |
9251fceb | 205 | else for (int i=3;i--;) b[i] *= fFactorDip; |
db83d72f | 206 | } |
9251fceb | 207 | else MachineField(xyz, b); |
aee8290b | 208 | // |
fe4da5cc | 209 | } |
eeda4611 | 210 | |
211 | //_______________________________________________________________________ | |
db83d72f | 212 | Double_t AliMagF::GetBz(const Double_t *xyz) const |
eeda4611 | 213 | { |
db83d72f | 214 | // Method to calculate the field at point xyz |
215 | // | |
9251fceb | 216 | if (fMeasuredMap && xyz[2]>fMeasuredMap->GetMinZ() && xyz[2]<fMeasuredMap->GetMaxZ()) { |
217 | double bz = fMeasuredMap->GetBz(xyz); | |
218 | return (xyz[2]>fgkSol2DipZ || fDipoleOFF) ? bz*fFactorSol : bz*fFactorDip; | |
db83d72f | 219 | } |
9251fceb | 220 | else return 0.; |
eeda4611 | 221 | } |
222 | ||
223 | //_______________________________________________________________________ | |
db83d72f | 224 | AliMagF& AliMagF::operator=(const AliMagF& src) |
eeda4611 | 225 | { |
db83d72f | 226 | if (this != &src && src.fMeasuredMap) { |
227 | if (fMeasuredMap) delete fMeasuredMap; | |
228 | fMeasuredMap = new AliMagWrapCheb(*src.fMeasuredMap); | |
229 | SetName(src.GetName()); | |
230 | fSolenoid = src.fSolenoid; | |
231 | fBeamType = src.fBeamType; | |
232 | fBeamEnergy = src.fBeamEnergy; | |
db83d72f | 233 | fInteg = src.fInteg; |
234 | fPrecInteg = src.fPrecInteg; | |
235 | fFactorSol = src.fFactorSol; | |
236 | fFactorDip = src.fFactorDip; | |
237 | fMax = src.fMax; | |
238 | fDipoleOFF = src.fDipoleOFF; | |
239 | fParNames = src.fParNames; | |
240 | } | |
241 | return *this; | |
eeda4611 | 242 | } |
243 | ||
244 | //_______________________________________________________________________ | |
db83d72f | 245 | void AliMagF::InitMachineField(BeamType_t btype, Double_t benergy) |
eeda4611 | 246 | { |
4642ac4b | 247 | if (btype==kNoBeamField) { |
db83d72f | 248 | fQuadGradient = fDipoleField = fCCorrField = fACorr1Field = fACorr2Field = 0.; |
9251fceb | 249 | return; |
db83d72f | 250 | } |
251 | // | |
9251fceb | 252 | double rigScale = benergy/7000.; // scale according to ratio of E/Enominal |
253 | // for ions assume PbPb (with energy provided per nucleon) and account for A/Z | |
254 | if (btype == kBeamTypeAA) rigScale *= 208./82.; | |
255 | // | |
256 | fQuadGradient = 22.0002*rigScale; | |
257 | fDipoleField = 37.8781*rigScale; | |
258 | // | |
259 | // SIDE C | |
260 | fCCorrField = -9.6980; | |
261 | // SIDE A | |
262 | fACorr1Field = -13.2247; | |
263 | fACorr2Field = 11.7905; | |
db83d72f | 264 | // |
eeda4611 | 265 | } |
eed8a1a2 | 266 | |
db83d72f | 267 | //_______________________________________________________________________ |
268 | void AliMagF::MachineField(const Double_t *x, Double_t *b) const | |
eed8a1a2 | 269 | { |
db83d72f | 270 | // ---- This is the ZDC part |
9251fceb | 271 | // Compansators for Alice Muon Arm Dipole |
272 | const Double_t kBComp1CZ = 1075., kBComp1hDZ = 260./2., kBComp1SqR = 4.0*4.0; | |
273 | const Double_t kBComp2CZ = 2049., kBComp2hDZ = 153./2., kBComp2SqR = 4.5*4.5; | |
274 | // | |
275 | const Double_t kTripQ1CZ = 2615., kTripQ1hDZ = 637./2., kTripQ1SqR = 3.5*3.5; | |
90ae20c9 | 276 | const Double_t kTripQ2CZ = 3480., kTripQ2hDZ = 550./2., kTripQ2SqR = 3.5*3.5; |
9251fceb | 277 | const Double_t kTripQ3CZ = 4130., kTripQ3hDZ = 550./2., kTripQ3SqR = 3.5*3.5; |
278 | const Double_t kTripQ4CZ = 5015., kTripQ4hDZ = 637./2., kTripQ4SqR = 3.5*3.5; | |
db83d72f | 279 | // |
9251fceb | 280 | const Double_t kDip1CZ = 6310.8, kDip1hDZ = 945./2., kDip1SqRC = 4.5*4.5, kDip1SqRA = 3.375*3.375; |
281 | const Double_t kDip2CZ = 12640.3, kDip2hDZ = 945./2., kDip2SqRC = 4.5*4.5, kDip2SqRA = 3.75*3.75; | |
282 | const Double_t kDip2DXC = 9.7, kDip2DXA = 9.4; | |
db83d72f | 283 | // |
284 | double rad2 = x[0] * x[0] + x[1] * x[1]; | |
285 | // | |
9251fceb | 286 | b[0] = b[1] = b[2] = 0; |
287 | // | |
db83d72f | 288 | // SIDE C ************************************************** |
289 | if(x[2]<0.){ | |
9251fceb | 290 | if(TMath::Abs(x[2]+kBComp2CZ)<kBComp2hDZ && rad2 < kBComp2SqR){ |
291 | b[0] = fCCorrField*fFactorDip; | |
db83d72f | 292 | } |
9251fceb | 293 | else if(TMath::Abs(x[2]+kTripQ1CZ)<kTripQ1hDZ && rad2 < kTripQ1SqR){ |
db83d72f | 294 | b[0] = fQuadGradient*x[1]; |
295 | b[1] = fQuadGradient*x[0]; | |
db83d72f | 296 | } |
9251fceb | 297 | else if(TMath::Abs(x[2]+kTripQ2CZ)<kTripQ2hDZ && rad2 < kTripQ2SqR){ |
db83d72f | 298 | b[0] = -fQuadGradient*x[1]; |
299 | b[1] = -fQuadGradient*x[0]; | |
db83d72f | 300 | } |
9251fceb | 301 | else if(TMath::Abs(x[2]+kTripQ3CZ)<kTripQ3hDZ && rad2 < kTripQ3SqR){ |
db83d72f | 302 | b[0] = -fQuadGradient*x[1]; |
303 | b[1] = -fQuadGradient*x[0]; | |
db83d72f | 304 | } |
9251fceb | 305 | else if(TMath::Abs(x[2]+kTripQ4CZ)<kTripQ4hDZ && rad2 < kTripQ4SqR){ |
db83d72f | 306 | b[0] = fQuadGradient*x[1]; |
307 | b[1] = fQuadGradient*x[0]; | |
db83d72f | 308 | } |
9251fceb | 309 | else if(TMath::Abs(x[2]+kDip1CZ)<kDip1hDZ && rad2 < kDip1SqRC){ |
db83d72f | 310 | b[1] = fDipoleField; |
db83d72f | 311 | } |
9251fceb | 312 | else if(TMath::Abs(x[2]+kDip2CZ)<kDip2hDZ && rad2 < kDip2SqRC) { |
313 | double dxabs = TMath::Abs(x[0])-kDip2DXC; | |
314 | if ( (dxabs*dxabs + x[1]*x[1])<kDip2SqRC) { | |
db83d72f | 315 | b[1] = -fDipoleField; |
db83d72f | 316 | } |
317 | } | |
318 | } | |
319 | // | |
320 | // SIDE A ************************************************** | |
321 | else{ | |
9251fceb | 322 | if(TMath::Abs(x[2]-kBComp1CZ)<kBComp1hDZ && rad2 < kBComp1SqR) { |
db83d72f | 323 | // Compensator magnet at z = 1075 m |
9251fceb | 324 | b[0] = fACorr1Field*fFactorDip; |
db83d72f | 325 | } |
326 | // | |
9251fceb | 327 | if(TMath::Abs(x[2]-kBComp2CZ)<kBComp2hDZ && rad2 < kBComp2SqR){ |
328 | b[0] = fACorr2Field*fFactorDip; | |
329 | } | |
330 | else if(TMath::Abs(x[2]-kTripQ1CZ)<kTripQ1hDZ && rad2 < kTripQ1SqR){ | |
db83d72f | 331 | b[0] = -fQuadGradient*x[1]; |
332 | b[1] = -fQuadGradient*x[0]; | |
eed8a1a2 | 333 | } |
9251fceb | 334 | else if(TMath::Abs(x[2]-kTripQ2CZ)<kTripQ2hDZ && rad2 < kTripQ2SqR){ |
335 | b[0] = fQuadGradient*x[1]; | |
336 | b[1] = fQuadGradient*x[0]; | |
eed8a1a2 | 337 | } |
9251fceb | 338 | else if(TMath::Abs(x[2]-kTripQ3CZ)<kTripQ3hDZ && rad2 < kTripQ3SqR){ |
339 | b[0] = fQuadGradient*x[1]; | |
340 | b[1] = fQuadGradient*x[0]; | |
db83d72f | 341 | } |
9251fceb | 342 | else if(TMath::Abs(x[2]-kTripQ4CZ)<kTripQ4hDZ && rad2 < kTripQ4SqR){ |
db83d72f | 343 | b[0] = -fQuadGradient*x[1]; |
344 | b[1] = -fQuadGradient*x[0]; | |
db83d72f | 345 | } |
9251fceb | 346 | else if(TMath::Abs(x[2]-kDip1CZ)<kDip1hDZ && rad2 < kDip1SqRA){ |
db83d72f | 347 | b[1] = -fDipoleField; |
db83d72f | 348 | } |
9251fceb | 349 | else if(TMath::Abs(x[2]-kDip2CZ)<kDip2hDZ && rad2 < kDip2SqRA) { |
350 | double dxabs = TMath::Abs(x[0])-kDip2DXA; | |
351 | if ( (dxabs*dxabs + x[1]*x[1])<kDip2SqRA) { | |
db83d72f | 352 | b[1] = fDipoleField; |
353 | } | |
354 | } | |
355 | } | |
9251fceb | 356 | // |
db83d72f | 357 | } |
358 | ||
359 | //_______________________________________________________________________ | |
360 | void AliMagF::GetTPCInt(const Double_t *xyz, Double_t *b) const | |
361 | { | |
362 | // Method to calculate the integral of magnetic integral from xyz to nearest cathode plane | |
363 | b[0]=b[1]=b[2]=0.0; | |
364 | if (fMeasuredMap) { | |
365 | fMeasuredMap->GetTPCInt(xyz,b); | |
366 | for (int i=3;i--;) b[i] *= fFactorSol; | |
367 | } | |
368 | } | |
369 | ||
370 | //_______________________________________________________________________ | |
371 | void AliMagF::GetTPCIntCyl(const Double_t *rphiz, Double_t *b) const | |
372 | { | |
373 | // Method to calculate the integral of magnetic integral from point to nearest cathode plane | |
374 | // in cylindrical coordiates ( -pi<phi<pi convention ) | |
375 | b[0]=b[1]=b[2]=0.0; | |
376 | if (fMeasuredMap) { | |
377 | fMeasuredMap->GetTPCIntCyl(rphiz,b); | |
378 | for (int i=3;i--;) b[i] *= fFactorSol; | |
379 | } | |
eed8a1a2 | 380 | } |
1dd3d90e | 381 | |
382 | //_______________________________________________________________________ | |
383 | void AliMagF::SetFactorSol(Float_t fc) | |
384 | { | |
385 | // set the sign/scale of the current in the L3 according to fgkPolarityConvention | |
386 | switch (fgkPolarityConvention) { | |
387 | case kConvDCS2008: fFactorSol = -fc; break; | |
388 | case kConvLHC : fFactorSol = -fc; break; | |
389 | default : fFactorSol = fc; break; // case kConvMap2005: fFactorSol = fc; break; | |
390 | } | |
391 | } | |
392 | ||
393 | //_______________________________________________________________________ | |
394 | void AliMagF::SetFactorDip(Float_t fc) | |
395 | { | |
396 | // set the sign*scale of the current in the Dipole according to fgkPolarityConvention | |
397 | switch (fgkPolarityConvention) { | |
398 | case kConvDCS2008: fFactorDip = fc; break; | |
399 | case kConvLHC : fFactorDip = -fc; break; | |
400 | default : fFactorDip = fc; break; // case kConvMap2005: fFactorDip = fc; break; | |
401 | } | |
402 | } | |
403 | ||
404 | //_______________________________________________________________________ | |
405 | Double_t AliMagF::GetFactorSol() const | |
406 | { | |
407 | // return the sign*scale of the current in the Dipole according to fgkPolarityConventionthe | |
408 | switch (fgkPolarityConvention) { | |
409 | case kConvDCS2008: return -fFactorSol; | |
410 | case kConvLHC : return -fFactorSol; | |
411 | default : return fFactorSol; // case kConvMap2005: return fFactorSol; | |
412 | } | |
413 | } | |
414 | ||
415 | //_______________________________________________________________________ | |
416 | Double_t AliMagF::GetFactorDip() const | |
417 | { | |
418 | // return the sign*scale of the current in the Dipole according to fgkPolarityConventionthe | |
419 | switch (fgkPolarityConvention) { | |
420 | case kConvDCS2008: return fFactorDip; | |
421 | case kConvLHC : return -fFactorDip; | |
422 | default : return fFactorDip; // case kConvMap2005: return fFactorDip; | |
423 | } | |
424 | } | |
33fe5eb1 | 425 | |
426 | //_____________________________________________________________________________ | |
427 | AliMagF* AliMagF::CreateFieldMap(Float_t l3Cur, Float_t diCur, Int_t convention, Bool_t uniform, | |
428 | Float_t beamenergy, const Char_t *beamtype, const Char_t *path) | |
429 | { | |
430 | //------------------------------------------------ | |
431 | // The magnetic field map, defined externally... | |
432 | // L3 current 30000 A -> 0.5 T | |
433 | // L3 current 12000 A -> 0.2 T | |
434 | // dipole current 6000 A | |
435 | // The polarities must match the convention (LHC or DCS2008) | |
436 | // unless the special uniform map was used for MC | |
437 | //------------------------------------------------ | |
438 | const Float_t l3NominalCurrent1=30000.; // (A) | |
439 | const Float_t l3NominalCurrent2=12000.; // (A) | |
440 | const Float_t diNominalCurrent =6000. ; // (A) | |
441 | ||
442 | const Float_t tolerance=0.03; // relative current tolerance | |
443 | const Float_t zero=77.; // "zero" current (A) | |
444 | // | |
445 | BMap_t map; | |
446 | double sclL3,sclDip; | |
447 | // | |
448 | Float_t l3Pol = l3Cur > 0 ? 1:-1; | |
449 | Float_t diPol = diCur > 0 ? 1:-1; | |
450 | ||
451 | l3Cur = TMath::Abs(l3Cur); | |
452 | diCur = TMath::Abs(diCur); | |
453 | // | |
454 | if (TMath::Abs((sclDip=diCur/diNominalCurrent)-1.) > tolerance && !uniform) { | |
455 | if (diCur <= zero) sclDip = 0.; // some small current.. -> Dipole OFF | |
456 | else { | |
457 | AliErrorGeneral("AliMagF",Form("Wrong dipole current (%f A)!",diCur)); | |
458 | return 0; | |
459 | } | |
460 | } | |
461 | // | |
462 | if (uniform) { | |
463 | // special treatment of special MC with uniform mag field (normalized to 0.5 T) | |
464 | // no check for scaling/polarities are done | |
465 | map = k5kGUniform; | |
466 | sclL3 = l3Cur/l3NominalCurrent1; | |
467 | } | |
468 | else { | |
469 | if (TMath::Abs((sclL3=l3Cur/l3NominalCurrent1)-1.) < tolerance) map = k5kG; | |
470 | else if (TMath::Abs((sclL3=l3Cur/l3NominalCurrent2)-1.) < tolerance) map = k2kG; | |
471 | else if (l3Cur <= zero) { sclL3 = 0; map = k5kGUniform;} | |
472 | else { | |
473 | AliErrorGeneral("AliMagF",Form("Wrong L3 current (%f A)!",l3Cur)); | |
474 | return 0; | |
475 | } | |
476 | } | |
477 | // | |
478 | if (sclDip!=0 && (map==k5kG || map==k2kG) && | |
479 | ((convention==kConvLHC && l3Pol!=diPol) || | |
480 | (convention==kConvDCS2008 && l3Pol==diPol)) ) { | |
481 | AliErrorGeneral("AliMagF",Form("Wrong combination for L3/Dipole polarities (%c/%c) for convention %d", | |
482 | l3Pol>0?'+':'-',diPol>0?'+':'-',GetPolarityConvention())); | |
483 | return 0; | |
484 | } | |
485 | // | |
486 | if (l3Pol<0) sclL3 = -sclL3; | |
487 | if (diPol<0) sclDip = -sclDip; | |
488 | // | |
489 | BeamType_t btype = kNoBeamField; | |
490 | TString btypestr = beamtype; | |
491 | btypestr.ToLower(); | |
492 | TPRegexp protonBeam("(proton|p)\\s*-?\\s*\\1"); | |
493 | TPRegexp ionBeam("(lead|pb|ion|a)\\s*-?\\s*\\1"); | |
494 | if (btypestr.Contains(ionBeam)) btype = kBeamTypeAA; | |
495 | else if (btypestr.Contains(protonBeam)) btype = kBeamTypepp; | |
496 | else AliInfoGeneral("AliMagF",Form("Assume no LHC magnet field for the beam type %s, ",beamtype)); | |
497 | char ttl[80]; | |
498 | sprintf(ttl,"L3: %+5d Dip: %+4d kA; %s | Polarities in %s convention",(int)TMath::Sign(l3Cur,float(sclL3)), | |
499 | (int)TMath::Sign(diCur,float(sclDip)),uniform ? " Constant":"", | |
500 | convention==kConvLHC ? "LHC":"DCS2008"); | |
501 | // LHC and DCS08 conventions have opposite dipole polarities | |
502 | if ( GetPolarityConvention() != convention) sclDip = -sclDip; | |
503 | // | |
4642ac4b | 504 | return new AliMagF("MagneticFieldMap", ttl,sclL3,sclDip,map,btype,beamenergy,2,10.,path); |
33fe5eb1 | 505 | // |
506 | } | |
507 | ||
508 | //_____________________________________________________________________________ | |
509 | const char* AliMagF::GetBeamTypeText() const | |
510 | { | |
511 | const char *beamNA = "No Beam"; | |
512 | const char *beamPP = "p-p"; | |
513 | const char *beamPbPb= "Pb-Pb"; | |
514 | switch ( fBeamType ) { | |
515 | case kBeamTypepp : return beamPP; | |
516 | case kBeamTypeAA : return beamPbPb; | |
517 | case kNoBeamField: | |
518 | default: return beamNA; | |
519 | } | |
520 | } | |
521 |