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ddae0931 | 1 | #include "AliRICHSegResV0.h" |
2 | #include "AliRun.h" | |
3 | #include "TParticle.h" | |
4 | #include "TMath.h" | |
5 | #include "TRandom.h" | |
6 | ||
7 | ||
8 | ClassImp(AliRICHsegmentation) | |
9 | ClassImp(AliRICHresponse) | |
10 | //___________________________________________ | |
11 | ClassImp(AliRICHsegmentationV0) | |
12 | ||
13 | void AliRICHsegmentationV0::Init(AliRICHchamber* Chamber) | |
14 | { | |
15 | fNpx=(Int_t) (Chamber->ROuter()/fDpx+1); | |
16 | fNpy=(Int_t) (Chamber->ROuter()/fDpy+1); | |
17 | } | |
18 | ||
19 | ||
20 | Float_t AliRICHsegmentationV0::GetAnod(Float_t xhit) | |
21 | { | |
22 | Float_t wire= (xhit>0)? Int_t(xhit/fWireD)+0.5:Int_t(xhit/fWireD)-0.5; | |
23 | return fWireD*wire; | |
24 | } | |
25 | ||
26 | void AliRICHsegmentationV0::SetPADSIZ(Float_t p1, Float_t p2) | |
27 | { | |
28 | fDpx=p1; | |
29 | fDpy=p2; | |
30 | } | |
31 | void AliRICHsegmentationV0::GetPadIxy(Float_t x, Float_t y, Int_t &ix, Int_t &iy) | |
32 | { | |
33 | // returns pad coordinates (ix,iy) for given real coordinates (x,y) | |
34 | // | |
35 | ix = (x>0)? Int_t(x/fDpx)+1 : Int_t(x/fDpx); | |
36 | iy = (y>0)? Int_t(y/fDpy)+1 : Int_t(y/fDpy); | |
37 | if (iy > fNpy) iy= fNpy; | |
38 | if (iy < -fNpy) iy=-fNpy; | |
39 | if (ix > fNpx) ix= fNpx; | |
40 | if (ix < -fNpx) ix=-fNpx; | |
41 | } | |
42 | void AliRICHsegmentationV0:: | |
43 | GetPadCxy(Int_t ix, Int_t iy, Float_t &x, Float_t &y) | |
44 | { | |
45 | // returns real coordinates (x,y) for given pad coordinates (ix,iy) | |
46 | // | |
47 | x = (ix>0) ? Float_t(ix*fDpx)-fDpx/2. : Float_t(ix*fDpx)-fDpx/2.; | |
48 | y = (iy>0) ? Float_t(iy*fDpy)-fDpy/2. : Float_t(iy*fDpy)-fDpy/2.; | |
49 | } | |
50 | ||
51 | void AliRICHsegmentationV0:: | |
52 | FirstPad(Float_t xhit, Float_t yhit, Float_t dx, Float_t dy) | |
53 | { | |
54 | // | |
55 | // Find the wire position (center of charge distribution) | |
56 | Float_t x0a=GetAnod(xhit); | |
57 | // | |
58 | // and take fNsigma*sigma around this center | |
59 | Float_t x01=x0a - dx; | |
60 | Float_t x02=x0a + dx; | |
61 | Float_t y01=yhit - dy; | |
62 | Float_t y02=yhit + dy; | |
63 | // | |
64 | // find the pads over which the charge distributes | |
65 | GetPadIxy(x01,y01,fixmin,fiymin); | |
66 | GetPadIxy(x02,y02,fixmax,fiymax); | |
67 | // | |
68 | // Set current pad to lower left corner | |
69 | fix=fixmin; | |
70 | fiy=fiymin; | |
71 | GetPadCxy(fix,fiy,fx,fy); | |
72 | } | |
73 | ||
74 | void AliRICHsegmentationV0::NextPad() | |
75 | { | |
76 | // | |
77 | // Step to next pad in integration region | |
78 | if (fix != fixmax) { | |
79 | fix++; | |
80 | } else if (fiy != fiymax) { | |
81 | fix=fixmin; | |
82 | fiy++; | |
83 | } else { | |
84 | printf("\n Error: Stepping outside integration region\n "); | |
85 | } | |
86 | GetPadCxy(fix,fiy,fx,fy); | |
87 | } | |
88 | ||
89 | Int_t AliRICHsegmentationV0::MorePads() | |
90 | ||
91 | // | |
92 | // Are there more pads in the integration region | |
93 | { | |
94 | if (fix == fixmax && fiy == fiymax) { | |
95 | return 0; | |
96 | } else { | |
97 | return 1; | |
98 | ||
99 | } | |
100 | } | |
101 | ||
102 | void AliRICHsegmentationV0::SigGenInit(Float_t x,Float_t y,Float_t) | |
103 | { | |
104 | // | |
105 | // Initialises pad and wire position during stepping | |
106 | fxt =x; | |
107 | fyt =y; | |
108 | GetPadIxy(x,y,fixt,fiyt); | |
109 | fiwt=Int_t(x/fWireD)+1; | |
110 | ||
111 | } | |
112 | ||
113 | Int_t AliRICHsegmentationV0::SigGenCond(Float_t x,Float_t y,Float_t) | |
114 | { | |
115 | // | |
116 | // Signal will be generated if particle crosses pad boundary or | |
117 | // boundary between two wires. | |
118 | Int_t ixt, iyt; | |
119 | GetPadIxy(x,y,ixt,iyt); | |
120 | Int_t iwt=Int_t(x/fWireD)+1; | |
121 | ||
122 | if ((ixt != fixt) || (iyt !=fiyt) || (iwt != fiwt)) { | |
123 | return 1; | |
124 | } else { | |
125 | return 0; | |
126 | } | |
127 | } | |
128 | void AliRICHsegmentationV0:: | |
129 | IntegrationLimits(Float_t& x1,Float_t& x2,Float_t& y1, Float_t& y2) | |
130 | { | |
131 | x1=fxt-fx-fDpx/2.; | |
132 | x2=x1+fDpx; | |
133 | y1=fyt-fy-fDpy/2.; | |
134 | y2=y1+fDpy; | |
135 | ||
136 | } | |
137 | ||
138 | void AliRICHsegmentationV0:: | |
139 | Neighbours(Int_t iX, Int_t iY, Int_t* Nlist, Int_t Xlist[7], Int_t Ylist[7]) | |
140 | { | |
141 | //Is used for the cluster finder, include diagonal elements | |
142 | ||
143 | *Nlist=4;Xlist[0]=Xlist[1]=iX;Xlist[2]=iX-1;Xlist[3]=iX+1; | |
144 | Ylist[0]=iY-1;Ylist[1]=iY+1;Ylist[2]=Ylist[3]=iY; | |
145 | } | |
146 | ||
147 | void AliRICHsegmentationV0:: | |
148 | FitXY(AliRICHRecCluster* ,TClonesArray* ) | |
149 | // Default : Centre of gravity method | |
150 | { | |
151 | ; | |
152 | } | |
153 | ||
154 | ||
155 | //___________________________________________ | |
156 | ClassImp(AliRICHresponseV0) | |
157 | Float_t AliRICHresponseV0::IntPH(Float_t eloss) | |
158 | { | |
159 | // Get number of electrons and return charge | |
160 | ||
161 | Int_t nel; | |
162 | //E9/26=magic number should parameter | |
163 | nel= Int_t(eloss*1.e9/26.); | |
164 | Float_t charge=0; | |
165 | if (nel == 0) nel=1; | |
166 | for (Int_t i=1;i<=nel;i++) { | |
167 | charge -= fChslope*TMath::Log(gRandom->Rndm()); | |
168 | } | |
169 | return charge; | |
170 | } | |
171 | // ------------------------------------------- | |
172 | Float_t AliRICHresponseV0::IntXY(AliRICHsegmentation * segmentation) | |
173 | { | |
174 | ||
175 | const Float_t invpitch = 1/fPitch; | |
176 | Float_t response; | |
177 | // | |
178 | // Integration limits defined by segmentation model | |
179 | // | |
180 | ||
181 | Float_t xi1, xi2, yi1, yi2; | |
182 | segmentation->IntegrationLimits(xi1,xi2,yi1,yi2); | |
183 | xi1=xi1*invpitch; | |
184 | xi2=xi2*invpitch; | |
185 | yi1=yi1*invpitch; | |
186 | yi2=yi2*invpitch; | |
187 | ||
188 | // | |
189 | // The Mathieson function | |
190 | Double_t ux1=fSqrtKx3*TMath::TanH(fKx2*xi1); | |
191 | Double_t ux2=fSqrtKx3*TMath::TanH(fKx2*xi2); | |
192 | ||
193 | Double_t uy1=fSqrtKy3*TMath::TanH(fKy2*yi1); | |
194 | Double_t uy2=fSqrtKy3*TMath::TanH(fKy2*yi2); | |
195 | ||
196 | response=4.*fKx4*(TMath::ATan(ux2)-TMath::ATan(ux1))*fKy4*(TMath::ATan(uy2)-TMath::ATan(uy1)); | |
197 | ||
198 | return response; | |
199 | ||
200 | } | |
201 | //___________________________________________ | |
202 | Int_t AliRICHresponseV0::FeedBackPhotons(Float_t source[3], Float_t qtot) | |
203 | { | |
204 | // | |
205 | // Generate FeedBack photons | |
206 | // | |
207 | Int_t j, ipart, nt; | |
208 | ||
209 | //Probability of feedback | |
210 | Float_t fAlphaFeed=0.05; | |
211 | ||
212 | Int_t sNfeed=0; | |
213 | ||
214 | // Local variables | |
215 | Float_t cthf, ranf[2], phif, enfp = 0, sthf, weight; | |
216 | Int_t i, ifeed; | |
217 | Float_t e1[3], e2[3], e3[3]; | |
218 | Float_t vmod, uswop; | |
219 | Float_t fp, random; | |
220 | Float_t dir[3], phi; | |
221 | Int_t nfp; | |
222 | Float_t pol[3], mom[3]; | |
223 | TLorentzVector position; | |
224 | // | |
225 | // Determine number of feedback photons | |
226 | ||
227 | // Get weight of current particle | |
228 | TParticle *current = (TParticle*) | |
229 | (*gAlice->Particles())[gAlice->CurrentTrack()]; | |
230 | ||
231 | ifeed = Int_t(current->GetWeight()/100+0.5); | |
232 | ipart = gMC->TrackPid(); | |
233 | fp = fAlphaFeed * qtot; | |
234 | nfp = gRandom->Poisson(fp); | |
235 | ||
236 | // This call to fill the time of flight | |
237 | gMC->TrackPosition(position); | |
238 | // | |
239 | // Generate photons | |
240 | for (i = 0; i <nfp; ++i) { | |
241 | ||
242 | // Direction | |
243 | gMC->Rndm(ranf, 2); | |
244 | cthf = ranf[0] * 2 - 1.; | |
245 | if (cthf < 0) continue; | |
246 | sthf = TMath::Sqrt((1 - cthf) * (1 + cthf)); | |
247 | phif = ranf[1] * 2 * TMath::Pi(); | |
248 | // | |
249 | gMC->Rndm(&random, 1); | |
250 | if (random <= .57) { | |
251 | enfp = 7.5e-9; | |
252 | } else if (random <= .7) { | |
253 | enfp = 6.4e-9; | |
254 | } else { | |
255 | enfp = 7.9e-9; | |
256 | } | |
257 | ||
258 | dir[0] = sthf * TMath::Sin(phif); | |
259 | dir[1] = cthf; | |
260 | dir[2] = sthf * TMath::Cos(phif); | |
261 | gMC->Gdtom(dir, mom, 2); | |
262 | mom[0]*=enfp; | |
263 | mom[1]*=enfp; | |
264 | mom[2]*=enfp; | |
265 | ||
266 | // Polarisation | |
267 | e1[0] = 0; | |
268 | e1[1] = -dir[2]; | |
269 | e1[2] = dir[1]; | |
270 | ||
271 | e2[0] = -dir[1]; | |
272 | e2[1] = dir[0]; | |
273 | e2[2] = 0; | |
274 | ||
275 | e3[0] = dir[1]; | |
276 | e3[1] = 0; | |
277 | e3[2] = -dir[0]; | |
278 | ||
279 | vmod=0; | |
280 | for(j=0;j<3;j++) vmod+=e1[j]*e1[j]; | |
281 | if (!vmod) for(j=0;j<3;j++) { | |
282 | uswop=e1[j]; | |
283 | e1[j]=e3[j]; | |
284 | e3[j]=uswop; | |
285 | } | |
286 | vmod=0; | |
287 | for(j=0;j<3;j++) vmod+=e2[j]*e2[j]; | |
288 | if (!vmod) for(j=0;j<3;j++) { | |
289 | uswop=e2[j]; | |
290 | e2[j]=e3[j]; | |
291 | e3[j]=uswop; | |
292 | } | |
293 | ||
294 | vmod=0; | |
295 | for(j=0;j<3;j++) vmod+=e1[j]*e1[j]; | |
296 | vmod=TMath::Sqrt(1/vmod); | |
297 | for(j=0;j<3;j++) e1[j]*=vmod; | |
298 | ||
299 | vmod=0; | |
300 | for(j=0;j<3;j++) vmod+=e2[j]*e2[j]; | |
301 | vmod=TMath::Sqrt(1/vmod); | |
302 | for(j=0;j<3;j++) e2[j]*=vmod; | |
303 | ||
304 | gMC->Rndm(ranf, 1); | |
305 | phi = ranf[0] * 2 * TMath::Pi(); | |
306 | for(j=0;j<3;j++) pol[j]=e1[j]*TMath::Sin(phi)+e2[j]*TMath::Cos(phi); | |
307 | gMC->Gdtom(pol, pol, 2); | |
308 | ||
309 | // Put photon on the stack and label it as feedback (51, 52) | |
310 | ++sNfeed; | |
311 | if (ipart == 50000050 && ifeed != 50000052) { | |
312 | weight = 5000; | |
313 | } else { | |
314 | weight = 5000; | |
315 | } | |
316 | gAlice->SetTrack(1, gAlice->CurrentTrack(), gMC->PDGFromId(50), | |
317 | mom,source,pol,position[3], | |
318 | "Cherenkov", nt, weight); | |
319 | } | |
f91473f6 | 320 | return(sNfeed); |
ddae0931 | 321 | } |