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cd2a0045 | 1 | /************************************************************************** |
2 | * Copyright(c) 2007-2009, 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 | ||
2ae37d58 | 16 | /* $Id$ */ |
cd2a0045 | 17 | |
18 | /////////////////////////////////////////////////////////////////// | |
19 | // // | |
20 | // Implementation of the class to store the parameters used in // | |
21 | // the simulation of SPD, SDD and SSD detectors // | |
22 | // Origin: F.Prino, Torino, prino@to.infn.it // | |
23 | // // | |
24 | /////////////////////////////////////////////////////////////////// | |
25 | ||
26 | #include "AliITSSimuParam.h" | |
27 | #include <TMath.h> | |
28 | ||
29 | const Float_t AliITSSimuParam::fgkSPDBiasVoltageDefault = 18.182; | |
30 | const Double_t AliITSSimuParam::fgkSPDThreshDefault = 3000.; | |
31 | const Double_t AliITSSimuParam::fgkSPDSigmaDefault = 250.; | |
32 | const TString AliITSSimuParam::fgkSPDCouplingOptDefault = "old"; | |
33 | const Double_t AliITSSimuParam::fgkSPDCouplColDefault = 0.; | |
34 | const Double_t AliITSSimuParam::fgkSPDCouplRowDefault = 0.055; | |
35 | const Float_t AliITSSimuParam::fgkSPDEccDiffDefault = 0.85; | |
a0a6914c | 36 | const Float_t AliITSSimuParam::fgkSPDLorentzHoleWeightDefault = 1.0; |
cd2a0045 | 37 | const Float_t AliITSSimuParam::fgkSDDDiffCoeffDefault = 3.23; |
38 | const Float_t AliITSSimuParam::fgkSDDDiffCoeff1Default = 30.; | |
39 | const Float_t AliITSSimuParam::fgkSDDJitterErrorDefault = 20.; // 20 um from beam test 2001 | |
aebba721 | 40 | const Float_t AliITSSimuParam::fgkSDDDynamicRangeDefault = 1400./2.5; // mV/MOhm = nA |
cd2a0045 | 41 | const Int_t AliITSSimuParam::fgkSDDMaxAdcDefault = 1024; |
42 | const Float_t AliITSSimuParam::fgkSDDChargeLossDefault = 0.; | |
dfd6be22 | 43 | const Float_t AliITSSimuParam::fgkSDDTrigDelayDefault = 54.3; |
cd2a0045 | 44 | const Double_t AliITSSimuParam::fgkSSDCouplingPRDefault = 0.01; |
45 | const Double_t AliITSSimuParam::fgkSSDCouplingPLDefault = 0.01; | |
46 | const Double_t AliITSSimuParam::fgkSSDCouplingNRDefault = 0.01; | |
47 | const Double_t AliITSSimuParam::fgkSSDCouplingNLDefault = 0.01; | |
48 | const Int_t AliITSSimuParam::fgkSSDZSThresholdDefault = 3; | |
49 | ||
50 | const Float_t AliITSSimuParam::fgkNsigmasDefault = 3.; | |
51 | const Int_t AliITSSimuParam::fgkNcompsDefault = 121; | |
52 | ||
53 | ClassImp(AliITSSimuParam) | |
54 | ||
55 | //______________________________________________________________________ | |
56 | AliITSSimuParam::AliITSSimuParam(): | |
57 | TObject(), | |
58 | fGeVcharge(0.), | |
59 | fDOverV(0.), | |
2ae37d58 | 60 | //fSPDBiasVoltage(fgkSPDBiasVoltageDefault), |
61 | //fSPDThresh(fgkSPDThreshDefault), | |
62 | //fSPDSigma(fgkSPDSigmaDefault), | |
cd2a0045 | 63 | fSPDCouplOpt(0), |
64 | fSPDCouplCol(fgkSPDCouplColDefault), | |
65 | fSPDCouplRow(fgkSPDCouplRowDefault), | |
66 | fSPDEccDiff(0.), | |
a0a6914c | 67 | fSPDLorentzDrift(kTRUE), |
68 | fSPDLorentzHoleWeight(fgkSPDLorentzHoleWeightDefault), | |
dba117de | 69 | fSPDAddNoisyFlag(kFALSE), |
70 | fSPDRemoveDeadFlag(kFALSE), | |
cd2a0045 | 71 | fSDDElectronics(0), |
72 | fSDDDiffCoeff(0.), | |
73 | fSDDDiffCoeff1(0.), | |
74 | fSDDJitterError(fgkSDDJitterErrorDefault), | |
75 | fSDDDynamicRange(fgkSDDDynamicRangeDefault), | |
76 | fSDDMaxAdc(0.), | |
77 | fSDDChargeLoss(fgkSDDChargeLossDefault), | |
417ff3f4 | 78 | fSDDTrigDelay(fgkSDDTrigDelayDefault), |
d9ed1779 | 79 | fSDDRawFormat(7), |
cd2a0045 | 80 | fSSDCouplingPR(0), |
81 | fSSDCouplingPL(0), | |
82 | fSSDCouplingNR(0), | |
83 | fSSDCouplingNL(0), | |
84 | fSSDZSThreshold(fgkSSDZSThresholdDefault), | |
85 | fNsigmas(fgkNsigmasDefault), | |
86 | fNcomps(fgkNcompsDefault), | |
2ae37d58 | 87 | fGaus(), |
88 | fN(0.), | |
89 | fT(300.) | |
cd2a0045 | 90 | { |
91 | // default constructor | |
2ae37d58 | 92 | SetSPDBiasVoltageAll(fgkSPDBiasVoltageDefault); |
93 | SetSPDThresholdsAll(fgkSPDThreshDefault,fgkSPDSigmaDefault); | |
94 | SetSPDNoiseAll(0,0); | |
cd2a0045 | 95 | SetGeVToCharge(); |
96 | SetDistanceOverVoltage(); | |
97 | SetSPDCouplingOption(fgkSPDCouplingOptDefault); | |
98 | SetSPDSigmaDiffusionAsymmetry(fgkSPDEccDiffDefault); | |
99 | SetSDDElectronics(); | |
100 | SetSDDDiffCoeff(fgkSDDDiffCoeffDefault,fgkSDDDiffCoeff1Default); | |
101 | SetSDDMaxAdc((Double_t)fgkSDDMaxAdcDefault); | |
cd2a0045 | 102 | SetSSDCouplings(fgkSSDCouplingPRDefault,fgkSSDCouplingPLDefault,fgkSSDCouplingNRDefault,fgkSSDCouplingNLDefault); |
103 | } | |
104 | //______________________________________________________________________ | |
105 | AliITSSimuParam::AliITSSimuParam(const AliITSSimuParam &simpar): | |
106 | TObject(), | |
107 | fGeVcharge(simpar.fGeVcharge), | |
108 | fDOverV(simpar.fDOverV), | |
2ae37d58 | 109 | //fSPDBiasVoltage(simpar.fSPDBiasVoltage), |
110 | //fSPDThresh(simpar.fSPDThresh), | |
111 | //fSPDSigma(simpar.fSPDSigma), | |
cd2a0045 | 112 | fSPDCouplOpt(simpar.fSPDCouplOpt), |
113 | fSPDCouplCol(simpar.fSPDCouplCol), | |
114 | fSPDCouplRow(simpar.fSPDCouplRow), | |
115 | fSPDEccDiff(simpar.fSPDEccDiff), | |
a0a6914c | 116 | fSPDLorentzDrift(simpar.fSPDLorentzDrift), |
117 | fSPDLorentzHoleWeight(simpar.fSPDLorentzHoleWeight), | |
dba117de | 118 | fSPDAddNoisyFlag(simpar.fSPDAddNoisyFlag), |
119 | fSPDRemoveDeadFlag(simpar.fSPDRemoveDeadFlag), | |
cd2a0045 | 120 | fSDDElectronics(simpar.fSDDElectronics), |
121 | fSDDDiffCoeff(simpar.fSDDDiffCoeff), | |
122 | fSDDDiffCoeff1(simpar.fSDDDiffCoeff1), | |
123 | fSDDJitterError(simpar.fSDDJitterError), | |
124 | fSDDDynamicRange(simpar.fSDDDynamicRange), | |
125 | fSDDMaxAdc(simpar.fSDDMaxAdc), | |
126 | fSDDChargeLoss(simpar.fSDDChargeLoss), | |
417ff3f4 | 127 | fSDDTrigDelay(simpar.fSDDTrigDelay), |
d9ed1779 | 128 | fSDDRawFormat(simpar.fSDDRawFormat), |
cd2a0045 | 129 | fSSDCouplingPR(simpar.fSSDCouplingPR), |
130 | fSSDCouplingPL(simpar.fSSDCouplingPL), | |
131 | fSSDCouplingNR(simpar.fSSDCouplingNR), | |
132 | fSSDCouplingNL(simpar.fSSDCouplingNL), | |
133 | fSSDZSThreshold(simpar.fSSDZSThreshold), | |
134 | fNsigmas(simpar.fNsigmas), | |
135 | fNcomps(simpar.fNcomps), | |
2ae37d58 | 136 | fGaus(), |
137 | fN(simpar.fN), | |
138 | fT(simpar.fT){ | |
cd2a0045 | 139 | // copy constructor |
2ae37d58 | 140 | for (Int_t i=0;i<240;i++) { |
141 | fSPDBiasVoltage[i]=simpar.fSPDBiasVoltage[i]; | |
142 | fSPDThresh[i]=simpar.fSPDThresh[i]; | |
143 | fSPDSigma[i]=simpar.fSPDSigma[i]; | |
144 | fSPDNoise[i]=simpar.fSPDNoise[i]; | |
145 | fSPDBaseline[i]=simpar.fSPDBaseline[i]; | |
146 | } | |
cd2a0045 | 147 | } |
148 | ||
149 | //______________________________________________________________________ | |
150 | AliITSSimuParam& AliITSSimuParam::operator=(const AliITSSimuParam& source){ | |
151 | // Assignment operator. | |
152 | this->~AliITSSimuParam(); | |
153 | new(this) AliITSSimuParam(source); | |
154 | return *this; | |
155 | ||
156 | } | |
157 | ||
158 | ||
159 | //______________________________________________________________________ | |
160 | AliITSSimuParam::~AliITSSimuParam() { | |
161 | // destructor | |
162 | if(fGaus) delete fGaus; | |
163 | } | |
164 | //________________________________________________________________________ | |
165 | void AliITSSimuParam::SetNLookUp(Int_t p1){ | |
166 | // Set number of sigmas over which cluster disintegration is performed | |
167 | fNcomps=p1; | |
168 | if (fGaus) delete fGaus; | |
169 | fGaus = new TArrayF(fNcomps+1); | |
170 | for(Int_t i=0; i<=fNcomps; i++) { | |
171 | Float_t x = -fNsigmas + (2.*i*fNsigmas)/(fNcomps-1); | |
172 | (*fGaus)[i] = exp(-((x*x)/2)); | |
173 | } | |
174 | } | |
175 | //________________________________________________________________________ | |
176 | void AliITSSimuParam::PrintParameters() const{ | |
177 | printf("GeVToCharge = %G\n",fGeVcharge); | |
178 | printf("DistanveOverVoltage = %f \n",fDOverV); | |
179 | printf("\n"); | |
180 | printf("===== SPD parameters =====\n"); | |
2ae37d58 | 181 | printf("Bias Voltage = %f \n",fSPDBiasVoltage[0]); |
182 | printf("Threshold and sigma = %f %f\n",fSPDThresh[0],fSPDSigma[0]); | |
cd2a0045 | 183 | printf("Coupling Option = %s\n",fSPDCouplOpt.Data()); |
184 | printf("Coupling value (column) = %f\n",fSPDCouplCol); | |
185 | printf("Coupling value (row) = %f\n",fSPDCouplRow); | |
186 | printf("Eccentricity in diffusion = %f\n",fSPDEccDiff); | |
a0a6914c | 187 | printf("Flag to add Lorentz Drift = %d\n",fSPDLorentzDrift); |
188 | printf("Weight of Holes in Lor.Drift = %f\n",fSPDLorentzHoleWeight); | |
d600da26 | 189 | printf("Flag to add noisy = %d\n",fSPDAddNoisyFlag); |
190 | printf("Flag to remove dead = %d\n",fSPDRemoveDeadFlag); | |
cd2a0045 | 191 | printf("\n"); |
192 | printf("===== SDD parameters =====\n"); | |
193 | printf("Electronic chips = %d\n",fSDDElectronics); | |
194 | printf("Diffusion Coefficients = %f %f\n",fSDDDiffCoeff,fSDDDiffCoeff1); | |
195 | printf("Jitter Error = %f um\n",fSDDJitterError); | |
196 | printf("Dynamic Range = %f\n",fSDDDynamicRange); | |
197 | printf("Max. ADC = %f\n",fSDDMaxAdc); | |
198 | printf("Charge Loss = %f\n",fSDDChargeLoss); | |
417ff3f4 | 199 | printf("Trigger Delay (ns) = %f\n",fSDDTrigDelay); |
d9ed1779 | 200 | printf("Raw Data Format = %d\n",fSDDRawFormat); |
cd2a0045 | 201 | printf("\n"); |
202 | printf("===== SSD parameters =====\n"); | |
cd2a0045 | 203 | printf("Coupling PR = %f\n",fSSDCouplingPR); |
204 | printf("Coupling PL = %f\n",fSSDCouplingPL); | |
205 | printf("Coupling NR = %f\n",fSSDCouplingNR); | |
206 | printf("Coupling NL = %f\n",fSSDCouplingNL); | |
207 | printf("Zero Supp threshold = %d\n",fSSDZSThreshold); | |
208 | } | |
2ae37d58 | 209 | //______________________________________________________________________ |
210 | Double_t AliITSSimuParam::MobilityElectronSiEmp() const { | |
211 | // Computes the electron mobility in cm^2/volt-sec. Taken from SILVACO | |
212 | // International ATLAS II, 2D Device Simulation Framework, User Manual | |
213 | // Chapter 5 Equation 5-6. An empirical function for low-field mobiliity | |
214 | // in silicon at different tempeatures. | |
215 | // Inputs: | |
216 | // none. | |
217 | // Output: | |
218 | // none. | |
219 | // Return: | |
220 | // The Mobility of electrons in Si at a give temprature and impurity | |
221 | // concentration. [cm^2/Volt-sec] | |
222 | const Double_t km0 = 55.24; // cm^2/Volt-sec | |
223 | const Double_t km1 = 7.12E+08; // cm^2 (degree K)^2.3 / Volt-sec | |
224 | const Double_t kN0 = 1.072E17; // #/cm^3 | |
225 | const Double_t kT0 = 300.; // degree K. | |
226 | const Double_t keT0 = -2.3; // Power of Temp. | |
227 | const Double_t keT1 = -3.8; // Power of Temp. | |
228 | const Double_t keN = 0.73; // Power of Dopent Consentrations | |
229 | Double_t m; | |
230 | Double_t tT = fT,nN = fN; | |
231 | ||
232 | if(nN<=0.0){ // Simple case. | |
233 | if(tT==300.) return 1350.0; // From Table 5-1 at consentration 1.0E14. | |
234 | m = km1*TMath::Power(tT,keT0); | |
235 | return m; | |
236 | } // if nN<=0.0 | |
237 | m = km1*TMath::Power(tT,keT0) - km0; | |
238 | m /= 1.0 + TMath::Power(tT/kT0,keT1)*TMath::Power(nN/kN0,keN); | |
239 | m += km0; | |
240 | return m; | |
241 | } | |
242 | //______________________________________________________________________ | |
243 | Double_t AliITSSimuParam::MobilityHoleSiEmp() const { | |
244 | // Computes the Hole mobility in cm^2/volt-sec. Taken from SILVACO | |
245 | // International ATLAS II, 2D Device Simulation Framework, User Manual | |
246 | // Chapter 5 Equation 5-7 An empirical function for low-field mobiliity | |
247 | // in silicon at different tempeatures. | |
248 | // Inputs: | |
249 | // none. | |
250 | // Output: | |
251 | // none. | |
252 | // Return: | |
253 | // The Mobility of Hole in Si at a give temprature and impurity | |
254 | // concentration. [cm^2/Volt-sec] | |
255 | const Double_t km0a = 49.74; // cm^2/Volt-sec | |
256 | const Double_t km0b = 49.70; // cm^2/Volt-sec | |
257 | const Double_t km1 = 1.35E+08; // cm^2 (degree K)^2.3 / Volt-sec | |
258 | const Double_t kN0 = 1.606E17; // #/cm^3 | |
259 | const Double_t kT0 = 300.; // degree K. | |
260 | const Double_t keT0 = -2.2; // Power of Temp. | |
261 | const Double_t keT1 = -3.7; // Power of Temp. | |
262 | const Double_t keN = 0.70; // Power of Dopent Consentrations | |
263 | Double_t m; | |
264 | Double_t tT = fT,nN = fN; | |
265 | ||
266 | if(nN<=0.0){ // Simple case. | |
267 | if(tT==300.) return 495.0; // From Table 5-1 at consentration 1.0E14. | |
268 | m = km1*TMath::Power(tT,keT0) + km0a-km0b; | |
269 | return m; | |
270 | } // if nN<=0.0 | |
271 | m = km1*TMath::Power(tT,keT0) - km0b; | |
272 | m /= 1.0 + TMath::Power(tT/kT0,keT1)*TMath::Power(nN/kN0,keN); | |
273 | m += km0a; | |
274 | return m; | |
275 | } | |
276 | //______________________________________________________________________ | |
277 | Double_t AliITSSimuParam::DiffusionCoefficientElectron() const { | |
278 | // Computes the Diffusion coefficient for electrons in cm^2/sec. Taken | |
279 | // from SILVACO International ATLAS II, 2D Device Simulation Framework, | |
280 | // User Manual Chapter 5 Equation 5-53. Einstein relations for diffusion | |
281 | // coefficient. Note: 1 cm^2/sec = 10 microns^2/nanosec. | |
282 | // Inputs: | |
283 | // none. | |
284 | // Output: | |
285 | // none. | |
286 | // Return: | |
287 | // The Diffusion Coefficient of electrons in Si at a give temprature | |
288 | // and impurity concentration. [cm^2/sec] | |
289 | // const Double_t kb = 1.3806503E-23; // Joules/degree K | |
290 | // const Double_t qe = 1.60217646E-19; // Coulumbs. | |
291 | const Double_t kbqe = 8.617342312E-5; // Volt/degree K | |
292 | Double_t m = MobilityElectronSiEmp(); | |
293 | Double_t tT = fT; | |
294 | ||
295 | return m*kbqe*tT; // [cm^2/sec] | |
296 | } | |
297 | //______________________________________________________________________ | |
298 | Double_t AliITSSimuParam::DiffusionCoefficientHole() const { | |
299 | // Computes the Diffusion coefficient for Holes in cm^2/sec. Taken | |
300 | // from SILVACO International ATLAS II, 2D Device Simulation Framework, | |
301 | // User Manual Chapter 5 Equation 5-53. Einstein relations for diffusion | |
302 | // coefficient. Note: 1 cm^2/sec = 10 microns^2/nanosec. | |
303 | // Inputs: | |
304 | // none. | |
305 | // Output: | |
306 | // none. | |
307 | // Return: | |
308 | // The Defusion Coefficient of Hole in Si at a give temprature and | |
309 | // impurity concentration. [cm^2/sec] | |
310 | // and impurity concentration. [cm^2/sec] | |
311 | // const Double_t kb = 1.3806503E-23; // Joules/degree K | |
312 | // const Double_t qe = 1.60217646E-19; // Coulumbs. | |
313 | const Double_t kbqe = 8.617342312E-5; // Volt/degree K | |
314 | Double_t m = MobilityHoleSiEmp(); | |
315 | Double_t tT = fT; | |
316 | ||
317 | return m*kbqe*tT; // [cm^2/sec] | |
318 | } | |
319 | //______________________________________________________________________ | |
320 | Double_t AliITSSimuParam::LorentzAngleHole(Double_t B) const { | |
321 | // Computes the Lorentz angle for electrons in Si | |
322 | // Input: magnetic Field in KGauss | |
323 | // Output: Lorentz angle in radians (positive if Bz is positive) | |
324 | // Main Reference: NIM A 497 (2003) 389–396. | |
325 | // "An algorithm for calculating the Lorentz angle in silicon detectors", V. Bartsch et al. | |
326 | // | |
327 | const Double_t krH=0.70; // Hall scattering factor for Hole | |
328 | const Double_t kT0 = 300.; // reference Temperature (degree K). | |
329 | const Double_t kmulow0 = 470.5; // cm^2/Volt-sec | |
330 | const Double_t keT0 = -2.5; // Power of Temp. | |
331 | const Double_t beta0 = 1.213; // beta coeff. at T0=300K | |
332 | const Double_t keT1 = 0.17; // Power of Temp. for beta | |
333 | const Double_t kvsat0 = 8.37E+06; // saturated velocity at T0=300K (cm/sec) | |
334 | const Double_t keT2 = 0.52; // Power of Temp. for vsat | |
335 | Double_t tT = fT; | |
336 | Double_t eE= 1./fDOverV; | |
337 | Double_t muLow=kmulow0*TMath::Power(tT/kT0,keT0); | |
338 | Double_t beta=beta0*TMath::Power(tT/kT0,keT1); | |
339 | Double_t vsat=kvsat0*TMath::Power(tT/kT0,keT2); | |
340 | Double_t mu=muLow/TMath::Power(1+TMath::Power(muLow*eE/vsat,beta),1/beta); | |
341 | Double_t angle=TMath::ATan(krH*mu*B*1.E-05); // Conversion Factor | |
342 | return angle; | |
343 | } | |
344 | //______________________________________________________________________ | |
345 | Double_t AliITSSimuParam::LorentzAngleElectron(Double_t B) const { | |
346 | // Computes the Lorentz angle for electrons in Si | |
347 | // Input: magnetic Field in KGauss | |
348 | // Output: Lorentz angle in radians (positive if Bz is positive) | |
349 | // Main Reference: NIM A 497 (2003) 389–396. | |
350 | // "An algorithm for calculating the Lorentz angle in silicon detectors", V. Bartsch et al. | |
351 | // | |
352 | const Double_t krH=1.15; // Hall scattering factor for Electron | |
353 | const Double_t kT0 = 300.; // reference Temperature (degree K). | |
354 | const Double_t kmulow0 = 1417.0; // cm^2/Volt-sec | |
355 | const Double_t keT0 = -2.2; // Power of Temp. | |
356 | const Double_t beta0 = 1.109; // beta coeff. at T0=300K | |
357 | const Double_t keT1 = 0.66; // Power of Temp. for beta | |
358 | const Double_t kvsat0 = 1.07E+07; // saturated velocity at T0=300K (cm/sec) | |
359 | const Double_t keT2 = 0.87; // Power of Temp. for vsat | |
360 | Double_t tT = fT; | |
361 | Double_t eE= 1./fDOverV; | |
362 | Double_t muLow=kmulow0*TMath::Power(tT/kT0,keT0); | |
363 | Double_t beta=beta0*TMath::Power(tT/kT0,keT1); | |
364 | Double_t vsat=kvsat0*TMath::Power(tT/kT0,keT2); | |
365 | Double_t mu=muLow/TMath::Power(1+TMath::Power(muLow*eE/vsat,beta),1/beta); | |
366 | Double_t angle=TMath::ATan(krH*mu*B*1.E-05); | |
367 | return angle; | |
368 | } | |
369 | //______________________________________________________________________ | |
370 | Double_t AliITSSimuParam::SpeedElectron() const { | |
371 | // Computes the average speed for electrons in Si under the low-field | |
372 | // approximation. [cm/sec]. | |
373 | // Inputs: | |
374 | // none. | |
375 | // Output: | |
376 | // none. | |
377 | // Return: | |
378 | // The speed the holes are traveling at due to the low field applied. | |
379 | // [cm/sec] | |
380 | Double_t m = MobilityElectronSiEmp(); | |
381 | ||
382 | return m/fDOverV; // [cm/sec] | |
383 | } | |
384 | //______________________________________________________________________ | |
385 | Double_t AliITSSimuParam::SpeedHole() const { | |
386 | // Computes the average speed for Holes in Si under the low-field | |
387 | // approximation.[cm/sec]. | |
388 | // Inputs: | |
389 | // none. | |
390 | // Output: | |
391 | // none. | |
392 | // Return: | |
393 | // The speed the holes are traveling at due to the low field applied. | |
394 | // [cm/sec] | |
395 | Double_t m = MobilityHoleSiEmp(); | |
396 | ||
397 | return m/fDOverV; // [cm/sec] | |
398 | } | |
399 | //______________________________________________________________________ | |
400 | Double_t AliITSSimuParam::SigmaDiffusion3D(Double_t l) const { | |
401 | // Returns the Gaussian sigma^2 == <x^2+y^2+z^2> [cm^2] due to the | |
402 | // defusion of electrons or holes through a distance l [cm] caused | |
403 | // by an applied voltage v [volt] through a distance d [cm] in any | |
404 | // material at a temperature T [degree K]. The sigma diffusion when | |
405 | // expressed in terms of the distance over which the diffusion | |
406 | // occures, l=time/speed, is independent of the mobility and therefore | |
407 | // the properties of the material. The charge distributions is given by | |
408 | // n = exp(-r^2/4Dt)/(4piDt)^1.5. From this <r^2> = 6Dt where D=mkT/e | |
409 | // (m==mobility, k==Boltzman's constant, T==temparature, e==electric | |
410 | // charge. and vel=m*v/d. consiquently sigma^2=6kTdl/ev. | |
411 | // Inputs: | |
412 | // Double_t l Distance the charge has to travel. | |
413 | // Output: | |
414 | // none. | |
415 | // Return: | |
416 | // The Sigma due to the diffution of electrons. [cm] | |
417 | const Double_t kcon = 5.17040258E-04; // == 6k/e [J/col or volts] | |
418 | ||
419 | return TMath::Sqrt(kcon*fT*fDOverV*l); // [cm] | |
420 | } | |
421 | //______________________________________________________________________ | |
422 | Double_t AliITSSimuParam::SigmaDiffusion2D(Double_t l) const { | |
423 | // Returns the Gaussian sigma^2 == <x^2+z^2> [cm^2] due to the defusion | |
424 | // of electrons or holes through a distance l [cm] caused by an applied | |
425 | // voltage v [volt] through a distance d [cm] in any material at a | |
426 | // temperature T [degree K]. The sigma diffusion when expressed in terms | |
427 | // of the distance over which the diffusion occures, l=time/speed, is | |
428 | // independent of the mobility and therefore the properties of the | |
429 | // material. The charge distributions is given by | |
430 | // n = exp(-r^2/4Dt)/(4piDt)^1.5. From this <x^2+z^2> = 4Dt where D=mkT/e | |
431 | // (m==mobility, k==Boltzman's constant, T==temparature, e==electric | |
432 | // charge. and vel=m*v/d. consiquently sigma^2=4kTdl/ev. | |
433 | // Inputs: | |
434 | // Double_t l Distance the charge has to travel. | |
435 | // Output: | |
436 | // none. | |
437 | // Return: | |
438 | // The Sigma due to the diffution of electrons. [cm] | |
439 | const Double_t kcon = 3.446935053E-04; // == 4k/e [J/col or volts] | |
440 | ||
441 | return TMath::Sqrt(kcon*fT*fDOverV*l); // [cm] | |
442 | } | |
443 | //______________________________________________________________________ | |
444 | Double_t AliITSSimuParam::SigmaDiffusion1D(Double_t l) const { | |
445 | // Returns the Gaussian sigma^2 == <x^2> [cm^2] due to the defusion | |
446 | // of electrons or holes through a distance l [cm] caused by an applied | |
447 | // voltage v [volt] through a distance d [cm] in any material at a | |
448 | // temperature T [degree K]. The sigma diffusion when expressed in terms | |
449 | // of the distance over which the diffusion occures, l=time/speed, is | |
450 | // independent of the mobility and therefore the properties of the | |
451 | // material. The charge distributions is given by | |
452 | // n = exp(-r^2/4Dt)/(4piDt)^1.5. From this <r^2> = 2Dt where D=mkT/e | |
453 | // (m==mobility, k==Boltzman's constant, T==temparature, e==electric | |
454 | // charge. and vel=m*v/d. consiquently sigma^2=2kTdl/ev. | |
455 | // Inputs: | |
456 | // Double_t l Distance the charge has to travel. | |
457 | // Output: | |
458 | // none. | |
459 | // Return: | |
460 | // The Sigma due to the diffution of electrons. [cm] | |
461 | const Double_t kcon = 1.723467527E-04; // == 2k/e [J/col or volts] | |
462 | ||
463 | return TMath::Sqrt(kcon*fT*fDOverV*l); // [cm] | |
464 | } | |
465 | //---------------------------------------------------------------------- | |
466 | Double_t AliITSSimuParam::DepletedRegionThicknessA(Double_t dopCons, | |
467 | Double_t voltage, | |
468 | Double_t elecCharge, | |
469 | Double_t voltBuiltIn)const{ | |
470 | // Computes the thickness of the depleted region in Si due to the | |
471 | // application of an external bias voltage. From the Particle Data | |
472 | // Book, 28.8 Silicon semiconductor detectors equation 28.19 (2004) | |
473 | // Physics Letters B "Review of Particle Physics" Volume 592, Issue 1-4 | |
474 | // July 15 2004, ISSN 0370-2693 page 263. First equation. | |
475 | // Inputs: | |
476 | // Double_t dopCons "N" doping concentration | |
477 | // Double_t voltage "V" external bias voltage | |
478 | // Double_t elecCharge "e" electronic charge | |
479 | // Double_t voltBuiltIn=0.5 "V_bi" "built-in" Voltage (~0.5V for | |
480 | // resistivities typically used in detectors) | |
481 | // Output: | |
482 | // none. | |
483 | // Return: | |
484 | // The thickness of the depleted region | |
485 | ||
486 | return TMath::Sqrt(2.0*(voltage+voltBuiltIn)/(dopCons*elecCharge)); | |
487 | } | |
488 | //---------------------------------------------------------------------- | |
489 | Double_t AliITSSimuParam::DepletedRegionThicknessB(Double_t resist, | |
490 | Double_t voltage, | |
491 | Double_t mobility, | |
492 | Double_t voltBuiltIn, | |
493 | Double_t dielConst)const{ | |
494 | // Computes the thickness of the depleted region in Si due to the | |
495 | // application of an external bias voltage. From the Particle Data | |
496 | // Book, 28.8 Silicon semiconductor detectors equation 28.19 (2004) | |
497 | // Physics Letters B "Review of Particle Physics" Volume 592, Issue 1-4 | |
498 | // July 15 2004, ISSN 0370-2693 page 263. Second Equation. | |
499 | // Inputs: | |
500 | // Double_t resist "rho" resistivity (typically 1-10 kOhm cm) | |
501 | // Double_t voltage "V" external bias voltage | |
502 | // Double_t mobility "mu" charge carrier mobility | |
503 | // (electons 1350, holes 450 cm^2/V/s) | |
504 | // Double_t voltBuiltIn=0.5 "V_bi" "built-in" Voltage (~0.5V for | |
505 | // resistivities typically used in detectors) | |
506 | // Double_t dielConst=1.E-12 "epsilon" dielectric constant = 11.9 * | |
507 | // (permittivity of free space) or ~ 1 pF/cm | |
508 | // Output: | |
509 | // none. | |
510 | // Return: | |
511 | // The thickness of the depleted region | |
512 | ||
513 | return TMath::Sqrt(2.8*resist*mobility*dielConst*(voltage+voltBuiltIn)); | |
514 | } | |
515 | //---------------------------------------------------------------------- | |
516 | Double_t AliITSSimuParam::ReverseBiasCurrent(Double_t temp, | |
517 | Double_t revBiasCurT1, | |
518 | Double_t tempT1, | |
519 | Double_t energy)const{ | |
520 | // Computes the temperature dependance of the reverse bias current | |
521 | // of Si detectors. From the Particle Data | |
522 | // Book, 28.8 Silicon semiconductor detectors equation 28.21 (2004) | |
523 | // Physics Letters B "Review of Particle Physics" Volume 592, Issue 1-4 | |
524 | // July 15 2004, ISSN 0370-2693 page 263. | |
525 | // Inputs: | |
526 | // Double_t temp The temperature at which the current is wanted | |
527 | // Double_t revBiasCurT1 The reference bias current at temp T1 | |
528 | // Double_t tempT1 The temperature correstponding to revBiasCurT1 | |
529 | // Double_t energy=1.2 Some energy [eV] | |
530 | // Output: | |
531 | // none. | |
532 | // Return: | |
533 | // The reverse bias current at the tempeature temp. | |
534 | const Double_t kBoltz = 8.617343E-5; //[eV/K] | |
535 | ||
536 | return revBiasCurT1*(temp*temp/(tempT1*tempT1))* | |
537 | TMath::Exp(-0.5*energy*(tempT1-temp)/(kBoltz*tempT1*temp)); | |
538 | } | |
539 | //______________________________________________________________________ | |
540 | void AliITSSimuParam::SPDThresholds(const Int_t mod, Double_t& thresh, Double_t& sigma) const { | |
541 | if(mod<0 || mod>239) { | |
542 | thresh=0; | |
543 | sigma=0; | |
544 | return; | |
545 | } | |
546 | thresh=fSPDThresh[mod]; | |
547 | sigma=fSPDSigma[mod]; | |
548 | return; | |
549 | } | |
550 | //_______________________________________________________________________ | |
551 | void AliITSSimuParam::SPDNoise(const Int_t mod,Double_t &noise, Double_t &baseline) const { | |
552 | if(mod<0 || mod>239) { | |
553 | noise=0; | |
554 | baseline=0; | |
555 | return; | |
556 | } | |
557 | noise=fSPDNoise[mod]; | |
558 | baseline=fSPDBaseline[mod]; | |
559 | return; | |
560 | } | |
561 |