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d48cca74 | 1 | #ifndef AliRICHParam_h |
2 | #define AliRICHParam_h | |
3 | ||
db910db9 | 4 | #include <TNamed.h> //base class |
5 | #include <TMath.h> //QdcTot() | |
6 | #include <TVector.h> //old style | |
3582c1f9 | 7 | #include <TVector2.h> |
e42a7b46 | 8 | #include <TVector3.h> |
998b831f | 9 | #include <TRandom.h> |
db910db9 | 10 | #include <TClonesArray.h> //Hit2SDigs() |
998b831f | 11 | #include <AliLog.h> |
db910db9 | 12 | #include <TGeoMatrix.h> //Mars2Lors() Lors2Mars() |
13 | #include <TF1.h> //fields | |
14 | #include <TF2.h> //fields | |
15 | #include "AliRICHDigit.h" //Hit2Sdigs() | |
16 | #include <TGeoManager.h> //Instance() | |
998b831f | 17 | |
e42a7b46 | 18 | static const int kNchambers=7; //number of RICH chambers |
19 | static const int kNpadsX = 160; //number of pads along X in single chamber | |
20 | static const int kNpadsY = 144; //number of pads along Y in single chamber | |
e42a7b46 | 21 | static const int kNsectors=6; //number of sectors per chamber |
ed3ceb24 | 22 | |
ed3ceb24 | 23 | static const int kCerenkov=50000050; //??? go to something more general like TPDGCode |
24 | static const int kFeedback=50000051; //??? go to something more general like TPDGCode | |
25 | ||
ae754cdf | 26 | // Class providing all the needed parametrised information |
27 | // to construct the geometry, to define segmentation and to provide response model | |
28 | // In future will also provide all the staff needed for alignment and calibration | |
29 | ||
30 | ||
db910db9 | 31 | class AliRICHParam :public TNamed |
d48cca74 | 32 | { |
33 | public: | |
a25b3368 | 34 | //ctor&dtor |
db910db9 | 35 | virtual ~AliRICHParam() {delete fIdxC6F14;fgInstance=0;} |
a25b3368 | 36 | //test methodes |
c4a03891 | 37 | void Print(Option_t *opt="") const; //print current parametrization |
d3eb6079 | 38 | static void DrawAxis(); |
39 | static void DrawSectors(); | |
a25b3368 | 40 | //flags staff |
db910db9 | 41 | static inline AliRICHParam* Instance(); //pointer to AliRICHParam singleton |
a25b3368 | 42 | static void SetWireSag(Bool_t a) {fgIsWireSag=a;} |
43 | static Bool_t IsWireSag() {return fgIsWireSag;} | |
44 | static void SetResolveClusters(Bool_t a) {fgIsResolveClusters=a;} | |
45 | static Bool_t IsResolveClusters() {return fgIsResolveClusters;} | |
db910db9 | 46 | static Int_t Stack(Int_t evt=-1,Int_t tid=-1); //Print stack info for event and tid |
47 | static Int_t StackCount(Int_t pid,Int_t evt); //Counts stack particles of given sort in given event | |
48 | static inline Double_t ErrLoc (Double_t thetaC,Double_t phiC,Double_t thetaT,Double_t phiT,Double_t beta); | |
49 | static inline Double_t ErrGeom (Double_t thetaC,Double_t phiC,Double_t thetaT,Double_t phiT,Double_t beta); | |
50 | static inline Double_t ErrCrom (Double_t thetaC,Double_t phiC,Double_t thetaT,Double_t phiT,Double_t beta); | |
51 | static inline TVector3 SigmaSinglePhotonFormula(Double_t thetaC,Double_t phiC,Double_t thetaT,Double_t phiT,Double_t beta); | |
a25b3368 | 52 | //Geometrical properties |
db910db9 | 53 | static Int_t NpadsX () {return kNpadsX;} //number of pads along X in chamber |
54 | static Int_t NpadsY () {return kNpadsY;} //number of pads along Y in chamber | |
55 | static Int_t NpadsXsec () {return NpadsX()/2;} //number of pads along X in sector | |
56 | static Int_t NpadsYsec () {return NpadsY()/3;} //number of pads along Y in sector | |
57 | ||
58 | static Double_t AnodPitch () {return PadSizeY()/2;} //cm between anode wires | |
59 | static Double_t AnodZ () {return 7.806;} //Z positon of anod plane in LORS of the chamber, [cm] | |
60 | static Double_t CathPitch () {return PadSizeY()/4;} //dist between cathode wires [cm] | |
61 | static Double_t CollPitch () {return 0.5;} //dist between collection wires [cm] | |
62 | static Double_t DeadZone () {return 2.6;} //dead zone thickness [cm] | |
63 | static Double_t PadSizeX () {return 0.8;} //pad size x [cm] | |
64 | static Double_t PadSizeY () {return 0.84;} //pad size y [cm] | |
65 | static Double_t PcSizeX () {return NpadsX()*PadSizeX()+DeadZone();} //PC size x [cm] | |
66 | static Double_t PcSizeY () {return NpadsY()*PadSizeY()+2*DeadZone();} //PC size y [cm] | |
67 | static Double_t Pc2Cath () {return 0.445;} //dist between PC entrance plane and cathode wires plane [cm] | |
68 | static Double_t Pc2Win () {return PcZ();} //dist between PC entrance plane and window exit plane [cm] | |
69 | static Double_t PcZ () {return 8.0; } //Z positon of PC entrance plane in LORS of the chamber [cm] | |
70 | static Double_t RadThick () {return 1.5;} //radiator thickness [cm] | |
71 | static Double_t RadZ () {return -2.0; } //Z positon of radiator entrance plane in LORS of the chamber [cm] | |
72 | static Double_t SecSizeX () {return NpadsX()*PadSizeX()/2;} //sector size x [cm] | |
73 | static Double_t SecSizeY () {return NpadsY()*PadSizeY()/3;} //sector size y [cm ] | |
74 | static Double_t WinThick () {return 0.5;} //radiator window thickness [cm] | |
75 | ||
76 | ||
0422a446 | 77 | //trasformation methodes |
db910db9 | 78 | inline TVector3 Lors2Mars (Int_t c,Double_t x,Double_t y,Int_t p=kPc); //LORS->MARS transform of point [cm] for chamber c and plane p |
79 | inline TVector2 Mars2Lors (Int_t c,const TVector3 &x ,Int_t p=kPc); //MARS->LORS transform of point [cm] for chamber c and plane p | |
80 | ||
81 | static inline TVector3 Lors2MarsOld (Int_t c,Double_t x,Double_t y,Int_t p); //LORS->MARS transform of position (cm) for chamber c and plane p | |
82 | static inline TVector2 Mars2LorsOld (Int_t c,const TVector3 &x,Int_t p ); //MARS->LORS transform of position (cm) for chamber c and plane p | |
83 | static inline TVector3 Mars2LorsVec (Int_t c,const TVector3 &p ); //MARS->LORS transform of vector for chamber c | |
84 | static inline TVector3 Center (Int_t c,Int_t p ); //Center of plane p of chamber c in MARS (cm) | |
85 | static inline TVector3 Norm (Int_t c ); //Norm vector to the chamber c in MARS (cm) | |
86 | static inline TGeoMatrix*Matrix (Int_t iCh, Int_t iPlane ); //TGeoMatrix for the given chamber plain | |
87 | ||
0422a446 | 88 | static Int_t Pad2Cha (Int_t pad ){return pad/100000000; }//abs pad -> chamber |
89 | static Int_t Pad2Sec (Int_t pad ){return pad%100000000/1000000; }//abs pad -> sector | |
90 | static Int_t Pad2PadX (Int_t pad ){return pad%1000000/1000; }//abs pad -> pad x | |
91 | static Int_t Pad2PadY (Int_t pad ){return pad%1000000%100; }//abs pad -> pad y | |
92 | static Int_t PadAbs (Int_t c,Int_t s,Int_t x,Int_t y){return 100000000*c+1000000*s+1000*x+y; }//(c,s,x,y) -> abs pad | |
93 | static inline TVector2 Pad2Loc (Int_t pad ); //abs pad ->LORS | |
94 | static inline TVector2 Pad2Loc (TVector pad ); //pad -> LORS returns center of the pad | |
95 | static TVector2 Pad2Loc (Int_t x,Int_t y ){TVector pad(2);pad[0]=x;pad[1]=y;return Pad2Loc(pad);}//return center of the pad (x,y) | |
96 | static inline TVector Loc2Area (const TVector2 &x2 ); //pads area affected by hit x2. area is LeftDown-RightUp pad numbers | |
97 | static inline Int_t Loc2Sec (const TVector2 &x2 ); //LORS -> sector | |
98 | static Int_t Loc2Sec (Double_t x,Double_t y ){return Loc2Sec(TVector2(x,y));} //LORS -> sector | |
99 | static inline TVector Loc2Pad (const TVector2 &x2 ); //LORS -> pad | |
100 | static TVector Loc2Pad (Double_t x,Double_t y ){return Loc2Pad(TVector2(x,y));} //LORS -> pad | |
101 | static inline Int_t Pad2Sec (const TVector &pad ); //pad -> sector | |
102 | static inline Int_t PadNeighbours (Int_t iPadX,Int_t iPadY,Int_t aListX[4],Int_t aListY[4]); //pad -> list of it neighbours | |
103 | static Bool_t IsAccepted (const TVector2 &x2 ){return ( x2.X()>=0 && x2.X()<=PcSizeX() && x2.Y()>=0 && x2.Y()<=PcSizeY() ) ? kTRUE:kFALSE;} | |
104 | //optical properties methodes | |
db910db9 | 105 | static Float_t EckovMean ( ){return 6.766e-9;} //mean Ckov energy according to the total trasmission curve |
106 | static Float_t EckovMin ( ){return fEckovMin;} //min photon energy [GeV] defined in optical curves | |
107 | static Float_t EckovMax ( ){return fEckovMax;} //min photon energy [GeV] defined in optical curves | |
108 | ||
109 | static Float_t AbsCH4 (Float_t gev ); //AbsLen [cm]=f(Eckov) [GeV] for CH4 used as amp gas | |
db910db9 | 110 | static Float_t AbsAir (Float_t gev ){return fgAbsAir.Eval(gev);} //AbsLen [cm]=f(Eckov) [GeV] for air |
111 | ||
112 | Float_t IdxC6F14 (Float_t gev ){return fIdxC6F14->Eval(gev,fIdxC6F14->GetUniqueID());} //n=f(Eckov) [GeV] for C6H14 used as radiator | |
113 | static Float_t IdxSiO2 (Float_t gev ){return fgIdxSiO2 .Eval(gev);} //n=f(Eckov) [GeV] for SiO2 used as window TDR p.35 | |
114 | static Float_t IdxCH4 (Float_t gev ){return fgIdxCH4 .Eval(gev);} //n=f(Eckov) [GeV] for CF4 | |
db910db9 | 115 | static Float_t IdxAir (Float_t gev ){return fgIdxAir .Eval(gev);} //n=f(Eckov) [GeV] for air |
db910db9 | 116 | |
117 | void CdbRead (Int_t run,Int_t version ); //read all calibration information for requested run | |
e42a7b46 | 118 | |
e42a7b46 | 119 | static Double_t IonisationPotential() {return 26.0e-9;} //for CH4 in GeV taken from ???? |
120 | static TVector2 MathiesonDelta() {return TVector2(5*0.18,5*0.18);} //area of 5 sigmas of Mathieson distribution (cm) | |
121 | static Int_t MaxQdc() {return 4095;} //QDC number of channels | |
fab9e039 | 122 | |
db910db9 | 123 | |
fab9e039 | 124 | static Int_t QthMIP() {return 100;} |
125 | static Double_t DmatchMIP() {return 1.;} | |
126 | static Double_t PmodMax() {return 6.5;} | |
0fe8fa07 | 127 | static Int_t HV(Int_t sector) {if (sector>=1 && sector <=6) return fgHV[sector-1]; else return -1;} //high voltage for this sector |
3582c1f9 | 128 | static void SetHV(Int_t sector,Int_t hv){fgHV[sector-1]=hv;} |
a25b3368 | 129 | //charge response methodes |
130 | inline static Double_t Mathieson(Double_t x1,Double_t x2,Double_t y1,Double_t y2); //Mathienson integral over given limits | |
db910db9 | 131 | |
e42a7b46 | 132 | inline static Double_t GainSag(Double_t x,Int_t sector); //gain variations in % |
a25b3368 | 133 | static Double_t Gain(const TVector2 &x2){//gives chamber gain in terms of QDC channels for given point in local ref system |
134 | if(fgIsWireSag) return QdcSlope(Loc2Sec(x2))*(1+GainSag(x2.X(),Loc2Sec(x2))/100); | |
135 | else return QdcSlope(Loc2Sec(x2));} | |
136 | inline static Double_t FracQdc(const TVector2 &x2,const TVector &pad); //charge fraction to pad from hit | |
db910db9 | 137 | inline static Int_t TotQdc(TVector2 x2,Double_t e ); //total charge for Eloss (GeV) 0 for photons |
138 | static Double_t QdcSlope(Int_t sec){switch(sec){case -1: return 0; default: return 33;}} //weight of electon in QDC channels | |
139 | ||
140 | static inline Int_t Lors2Pad (Double_t x,Double_t y ); //LORS (x,y) [cm] -> abs pad number | |
141 | static Double_t IonPot ( ){return 26.0e-9;} //for CH4 in GeV taken from ???? | |
142 | static inline Int_t QdcTot (Int_t iPad,Double_t e ); //total QDC generated by Eloss or Etot [GeV] | |
143 | static inline Double_t QdcSag (Int_t iPad ); //mean QDC variation due to sagita [0,1] | |
144 | static Double_t QdcEle (Int_t iPad ){return fgIsWireSag?33*(1+QdcSag(iPad)):33;} //mean QDC per electron | |
145 | static inline Int_t Hit2SDigs (Int_t iPad, Double_t e,TClonesArray* pSDigLst); //hit->sdigits, returns Qtot | |
146 | static inline Int_t Hit2SDigs (TVector2 hit,Double_t e,TClonesArray* pSDigLst); //hit->sdigits, returns Qtot, old style | |
147 | static void TestHit2SDigs (Double_t x,Double_t y,Double_t e,Bool_t isNew=kFALSE); //test hit->sdigits | |
148 | ||
0fe8fa07 | 149 | inline static Bool_t IsOverTh(Int_t c,TVector pad,Double_t q); //is QDC of the pad registered by FEE |
db910db9 | 150 | static Int_t NsigmaTh() {return fgNsigmaTh;} // |
e42a7b46 | 151 | static Float_t SigmaThMean() {return fgSigmaThMean;} //QDC electronic noise mean |
152 | static Float_t SigmaThSpread() {return fgSigmaThSpread;} //QDC electronic noise width | |
e42a7b46 | 153 | |
ae754cdf | 154 | static Double_t CogCorr(Double_t x) {return 3.31267e-2*TMath::Sin(2*TMath::Pi()/PadSizeX()*x) //correction of cluster CoG due to sinoidal |
ed83829e | 155 | -2.66575e-3*TMath::Sin(4*TMath::Pi()/PadSizeX()*x) |
f770edb5 | 156 | +2.80553e-3*TMath::Sin(6*TMath::Pi()/PadSizeX()*x)+0.0070;} |
d0831219 | 157 | static void ReadErrFiles(); //Read Err file parameters |
db910db9 | 158 | TVector3 SigmaSinglePhoton(Int_t Npart, Double_t mom, Double_t theta, Double_t phi); //Find Sigma for single photon from momentum and particle id |
159 | TVector3 SigmaSinglePhoton(Double_t thetaCer, Double_t theta, Double_t phi); //Fing sigma for single photon from thetacer | |
160 | static Double_t Interpolate(Double_t par[4][330],Double_t x, Double_t y, Double_t phi); //Find the error value from interpolation | |
161 | ||
162 | TVector3 ForwardTracing(TVector3 entranceTrackPoint,TVector3 vectorTrack, Double_t thetaC, Double_t phiC); //it traces foward a photon from Emission Point to PC | |
163 | static TVector3 PlaneIntersect(const TVector3 &lineDir,const TVector3 &linePoint,const TVector3 &planeNorm,const TVector3 &planePoint); //intersection between line and plane | |
164 | static Double_t SnellAngle(Float_t n1, Float_t n2, Float_t theta1); // Snell law | |
165 | static void AnglesInDRS(Double_t trackTheta,Double_t trackPhi,Double_t thetaCerenkov,Double_t phiCerenkov,Double_t &tout,Double_t &pout);//It finds photon angles in | |
166 | static Double_t AlphaFeedback(Int_t c,Int_t s) {c++;s++; return 0.02;} //for sector s of chamber c | |
167 | //test part | |
168 | static void Test() {TestSeg();TestTrans();TestResp();} //test all groups of methodes | |
169 | static void TestResp(); //test the response group of methodes | |
170 | static void TestSeg(); //test the segmentation group of methodes | |
171 | static void TestTrans(); //test the transform group of methodes | |
172 | ||
068217e3 | 173 | static Double_t fgMass[5]; // mass array |
a25b3368 | 174 | static Bool_t fgIsTestBeam; //test beam geometry instead of normal RICH flag |
db910db9 | 175 | enum EPlaneId {kCenter,kPc,kRad,kAnod,kNch=7}; //4 planes in chamber and total number of chambers |
176 | protected: | |
177 | AliRICHParam(); //default ctor is protected to enforce it to be singleton | |
178 | static AliRICHParam *fgInstance; //static pointer to instance of AliRICHParam singleton | |
179 | //optical curves | |
180 | static Double_t fEckovMin; //min Eckov | |
181 | static Double_t fEckovMax; //max Eckov | |
182 | ||
183 | TF2* fIdxC6F14; //n=f(Ephot,T) [GeV] for radiator freon C6F14 | |
184 | static TF1 fgIdxSiO2; //n=f(Ephot) [GeV] for window quartz SiO2 | |
185 | static TF1 fgIdxCH4; //n=f(Ephot) [GeV] for MWPC amp gas CF4 | |
186 | static TF1 fgIdxAir; //n=f(Ephot) [GeV] for air | |
101624cd | 187 | |
db910db9 | 188 | static TF1 fgAbsC6F14; //abs len curve for radiator freon C6F14, cm versus GeV |
189 | static TF1 fgAbsSiO2; //abs len curve for window quartz SiO2 , cm versus GeV | |
190 | static TF1 fgAbsCH4; //abs len curve for MWPC methane CF4 , cm versus GeV | |
191 | static TF1 fgAbsAir; //abs len curve for air, cm versus GeV | |
db910db9 | 192 | |
193 | static Bool_t fgIsWireSag; //wire sagitta ON/OFF flag | |
194 | static Bool_t fgIsResolveClusters; //declustering ON/OFF flag | |
195 | static Bool_t fgIsFeedback; //generate feedback photon? | |
196 | ||
197 | static Int_t fgHV[6]; //HV applied to anod wires | |
198 | static Int_t fgNsigmaTh; //n. of sigmas to cut for zero suppression | |
199 | static Float_t fgSigmaThMean; //sigma threshold value | |
200 | static Float_t fgSigmaThSpread; //spread of sigma | |
201 | ||
202 | static Double_t fgErrChrom[4][330]; // | |
203 | static Double_t fgErrGeom[4][330]; // | |
204 | static Double_t fgErrLoc[4][330]; //Chromatic, Geometric and Localization array to parametrize SigmaCerenkov | |
205 | TGeoHMatrix *fMatrix[kNchambers]; //poiners to matrices defining RICH chambers rotations-translations | |
206 | ClassDef(AliRICHParam,0) //RICH main parameters class | |
d48cca74 | 207 | }; |
db910db9 | 208 | |
209 | AliRICHParam* AliRICHParam::Instance() | |
210 | { | |
211 | // Return pointer to the AliRICHParam singleton. | |
212 | // Arguments: none | |
213 | // Returns: pointer to the instance of AliRICHParam or 0 if no geometry | |
214 | if(!fgInstance&&gGeoManager) new AliRICHParam; | |
215 | else if(!gGeoManager) Printf("No geometry imported"); | |
216 | return fgInstance; | |
217 | }//Instance() | |
c2c6679b | 218 | //__________________________________________________________________________________________________ |
c712cb2f | 219 | Int_t AliRICHParam::PadNeighbours(Int_t iPadX,Int_t iPadY,Int_t listX[4],Int_t listY[4]) |
220 | { | |
a25b3368 | 221 | //Determines all the neighbouring pads for the given one (iPadX,iPadY). Returns total number of these pads. |
222 | //Dead zones are taken into account, meaning pads from different sector are not taken. | |
e42a7b46 | 223 | // 1 |
224 | // 2 3 | |
225 | // 4 | |
c712cb2f | 226 | Int_t nPads=0; |
e42a7b46 | 227 | if(iPadY!=NpadsY()&&iPadY!=2*NpadsYsec()&&iPadY!=NpadsYsec()){listX[nPads]=iPadX; listY[nPads]=iPadY+1; nPads++;} //1 |
228 | if(iPadX!=1&&iPadX!=NpadsXsec()+1) {listX[nPads]=iPadX-1; listY[nPads]=iPadY; nPads++;} //2 | |
229 | if(iPadX!=NpadsXsec()&&iPadX!=NpadsX()) {listX[nPads]=iPadX+1; listY[nPads]=iPadY; nPads++;} //3 | |
230 | if(iPadY!=1&&iPadY!=NpadsYsec()+1&&2*NpadsYsec()+1) {listX[nPads]=iPadX; listY[nPads]=iPadY-1; nPads++;} //4 | |
ed3ceb24 | 231 | |
c712cb2f | 232 | return nPads; |
233 | }//Pad2ClosePads() | |
234 | //__________________________________________________________________________________________________ | |
a25b3368 | 235 | Int_t AliRICHParam::Loc2Sec(const TVector2 &v2) |
3582c1f9 | 236 | { |
db910db9 | 237 | // Determines sector containing the given point. y ^ 5 6 |
238 | // | 3 4 | |
239 | // | 1 2 | |
240 | // -------> x | |
241 | // Arguments: v2- LORS position [cm] | |
242 | // Returns: sector code | |
243 | Double_t x0=0; Double_t x1=SecSizeX(); Double_t x2=SecSizeX()+DeadZone(); Double_t x3=PcSizeX(); | |
244 | Double_t y0=0; Double_t y1=SecSizeY(); Double_t y2=SecSizeY()+DeadZone(); Double_t y3=2*SecSizeY()+DeadZone(); | |
245 | Double_t y4=PcSizeY()-SecSizeY(); Double_t y5=PcSizeY(); | |
e42a7b46 | 246 | |
0fe8fa07 | 247 | Int_t sector=-1; |
a25b3368 | 248 | if (v2.X() >= x0 && v2.X() <= x1 ) sector=1; |
249 | else if(v2.X() >= x2 && v2.X() <= x3 ) sector=2; | |
0fe8fa07 | 250 | else return -1; |
3582c1f9 | 251 | |
a25b3368 | 252 | if (v2.Y() >= y0 && v2.Y() <= y1 ) ; //sectors 1 or 2 |
253 | else if(v2.Y() >= y2 && v2.Y() <= y3 ) sector+=2; //sectors 3 or 4 | |
254 | else if(v2.Y() >= y4 && v2.Y() <= y5 ) sector+=4; //sectors 5 or 6 | |
0fe8fa07 | 255 | else return -1; |
3582c1f9 | 256 | return sector; |
c712cb2f | 257 | }//Loc2Sec(Double_t x, Double_t y) |
c2c6679b | 258 | //__________________________________________________________________________________________________ |
a25b3368 | 259 | TVector AliRICHParam::Loc2Pad(const TVector2 &loc) |
3582c1f9 | 260 | { |
a25b3368 | 261 | //Determines pad number TVector(padx,pady) containing the given point x2 defined in the chamber RS. |
262 | //Pad count starts in lower left corner from 1,1 to 144,160 in upper right corner of a chamber. | |
e42a7b46 | 263 | //y ^ 5 6 |
264 | // | 3 4 | |
265 | // | 1 2 | |
266 | // -------> x | |
267 | TVector pad(2); | |
a25b3368 | 268 | Int_t sec=Loc2Sec(loc);//trasforms x2 to sector reference system |
0fe8fa07 | 269 | if(sec==-1) {pad[0]=pad[1]=-1; return pad;} |
a25b3368 | 270 | //first we deal with x |
271 | if(sec==1||sec==3||sec==5) pad[0]= Int_t( loc.X() / PadSizeX() )+1; //sector 1 or 3 or 5 | |
272 | else pad[0]=NpadsX() - Int_t( (PcSizeX()-loc.X()) / PadSizeX() ) ; //sector 2 or 4 or 6 | |
273 | //second deal with y | |
d3eb6079 | 274 | if(sec==1||sec==2) pad[1]=Int_t( loc.Y() / PadSizeY())+1; //sector 1 or 2 |
db910db9 | 275 | else if(sec==3||sec==4) pad[1]=Int_t( (loc.Y()-SecSizeY()-DeadZone()) / PadSizeY())+NpadsYsec()+1; //sector 3 or 4 |
d3eb6079 | 276 | else pad[1]=NpadsY() - Int_t( (PcSizeY()-loc.Y()) / PadSizeY()); //sector 5 or 6 |
e42a7b46 | 277 | return pad; |
3582c1f9 | 278 | } |
db910db9 | 279 | //++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
280 | Int_t AliRICHParam::Lors2Pad(Double_t x,Double_t y) | |
281 | { | |
282 | // Determines abs pad number containing the given point (x,y) defined in the chamber RS. | |
283 | // Pad count starts in lower left corner from 1,1 to 144,160 in upper right corner of a chamber. | |
284 | // y ^ 5 6 | |
285 | // | 3 4 | |
286 | // | 1 2 | |
287 | // -------> x | |
288 | Int_t padx,pady; | |
289 | if (x>= 0 && x<= SecSizeX() ) padx= 1 + Int_t( x /PadSizeX() ); //sector 1 or 3 or 5 | |
290 | else if(x>=SecSizeX()+DeadZone() && x<= PcSizeX() ) padx= NpadsX() - Int_t( (PcSizeX()-x)/PadSizeX() ); //sector 2 or 4 or 6 | |
291 | else return -1; //dead zone or out of chamber | |
292 | ||
293 | ||
294 | if (y>= 0 && y<= SecSizeY() ) pady= 1 + Int_t( y /PadSizeY() ); //sector 1 or 2 | |
295 | else if(y>=SecSizeY()+DeadZone() && y<=2*SecSizeY()+DeadZone() ) pady= 1 + NpadsYsec() + Int_t( (y-SecSizeY()-DeadZone()) / PadSizeY()); //sector 3 or 4 | |
296 | else if(y>= PcSizeY()-SecSizeY() && y<= PcSizeY() ) pady= NpadsY() - Int_t( (PcSizeY()-y)/PadSizeY() ); //sector 5 or 6 | |
297 | else return -1; //dead zone or out of chamber | |
298 | ||
299 | return AliRICHDigit::P2A(0,padx,pady); | |
300 | }//Lors2Pad() | |
301 | //++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ | |
998b831f | 302 | Int_t AliRICHParam::Pad2Sec(const TVector &pad) |
3582c1f9 | 303 | { |
a25b3368 | 304 | //Determines sector containing the given pad. |
0fe8fa07 | 305 | Int_t sector=-1; |
e42a7b46 | 306 | if (pad[0] >= 1 && pad[0] <= NpadsXsec() ) {sector=1;} |
307 | else if(pad[0] > NpadsXsec() && pad[0] <= NpadsX() ) {sector=2;} | |
998b831f | 308 | else AliDebugClass(1,Form("Wrong pad (%3.0f,%3.0f)",pad[0],pad[1])); |
e42a7b46 | 309 | |
310 | if (pad[1] >= 1 && pad[1] <= NpadsYsec() ) {} | |
311 | else if(pad[1] > NpadsYsec() && pad[1] <= 2*NpadsYsec() ) {sector+=2;} | |
312 | else if(pad[1] > 2*NpadsYsec() && pad[1] <= NpadsY() ) {sector+=4;} | |
998b831f | 313 | else AliDebugClass(1,Form("Wrong pad (%3.0f,%3.0f)",pad[0],pad[1])); |
c712cb2f | 314 | |
e42a7b46 | 315 | return sector; |
c712cb2f | 316 | }//Pad2Sec() |
db910db9 | 317 | //++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
e42a7b46 | 318 | TVector2 AliRICHParam::Pad2Loc(TVector pad) |
c712cb2f | 319 | { |
a25b3368 | 320 | //Returns position of the center of the given pad in local system of the chamber (cm) |
e42a7b46 | 321 | // y ^ 5 6 |
998b831f | 322 | // | 3 4 sector numbers |
e42a7b46 | 323 | // | 1 2 |
324 | // -------> x | |
0fe8fa07 | 325 | Double_t x=-1,y=-1; |
e42a7b46 | 326 | if(pad[0] > 0 && pad[0] <= NpadsXsec())//it's 1 or 3 or 5 |
327 | x=(pad[0]-0.5)*PadSizeX(); | |
328 | else if(pad[0] > NpadsXsec() && pad[0] <= NpadsX())//it's 2 or 4 or 6 | |
329 | x=(pad[0]-0.5)*PadSizeX()+DeadZone(); | |
c2c6679b | 330 | else |
998b831f | 331 | AliDebugClass(1,Form("Wrong pad (%3.0f,%3.0f)",pad[0],pad[1])); |
e42a7b46 | 332 | |
333 | if(pad[1] > 0 && pad[1] <= NpadsYsec())//it's 1 or 2 | |
334 | y=(pad[1]-0.5)*PadSizeY(); | |
335 | else if(pad[1] > NpadsYsec() && pad[1] <= 2*NpadsYsec())//it's 3 or 4 | |
336 | y=(pad[1]-0.5)*PadSizeY()+DeadZone(); | |
337 | else if(pad[1] > 2*NpadsYsec() && pad[1]<= NpadsY())//it's 5 or 6 | |
338 | y=(pad[1]-0.5)*PadSizeY()+2*DeadZone(); | |
339 | else | |
998b831f | 340 | AliDebugClass(1,Form("Wrong pad (%3.0f,%3.0f)",pad[0],pad[1])); |
e42a7b46 | 341 | |
3582c1f9 | 342 | return TVector2(x,y); |
343 | } | |
db910db9 | 344 | //++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
0422a446 | 345 | TVector2 AliRICHParam::Pad2Loc(Int_t pad) |
346 | { | |
db910db9 | 347 | // Converts absolute pad number to local position in LORS |
348 | // LORS is a chamber reference system with origin in left-down coner looking from IP | |
349 | // Arguments: pad- absolute pad number | |
350 | // Returns: pad center position as TVector2 in PCRS | |
0422a446 | 351 | TVector2 pos; |
352 | pos.Set((Pad2PadX(pad)-0.5)*PadSizeX() , (Pad2PadY(pad)-0.5)*PadSizeY());//set to sector LORS | |
353 | return pos; | |
354 | } | |
db910db9 | 355 | //++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
e42a7b46 | 356 | Double_t AliRICHParam::GainSag(Double_t x,Int_t sector) |
c60862bf | 357 | { |
a25b3368 | 358 | //Returns % of gain variation due to wire sagita. |
359 | //All curves are parametrized as per sector basis, so x must be apriory transformed to the Sector RS. | |
360 | //Here x is a distance along wires. | |
db910db9 | 361 | x-=SecSizeX()/2; |
362 | if(x>SecSizeX()) x-=SecSizeX(); | |
3582c1f9 | 363 | switch(HV(sector)){ |
e42a7b46 | 364 | case 2150: return 9e-6*TMath::Power(x,4)+2e-7*TMath::Power(x,3)-0.0316*TMath::Power(x,2)-3e-4*x+25.367;//% |
365 | case 2100: return 8e-6*TMath::Power(x,4)+2e-7*TMath::Power(x,3)-0.0283*TMath::Power(x,2)-2e-4*x+23.015; | |
366 | case 2050: return 7e-6*TMath::Power(x,4)+1e-7*TMath::Power(x,3)-0.0254*TMath::Power(x,2)-2e-4*x+20.888; | |
367 | case 2000: return 6e-6*TMath::Power(x,4)+8e-8*TMath::Power(x,3)-0.0227*TMath::Power(x,2)-1e-4*x+18.961; | |
3582c1f9 | 368 | default: return 0; |
369 | } | |
c712cb2f | 370 | } |
db910db9 | 371 | //++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
372 | Double_t AliRICHParam::QdcSag(Int_t iPad) | |
373 | { | |
374 | // It was observed at BNL that wires are affected by gravitation field providing a significant sagita leading to the local electric field variation | |
375 | // which means that different pads produce different signals. | |
376 | // Arguments: iPad- absolute pad number | |
377 | // Returns: gain variation due to wire sagita 0 < QdcSag < 1. | |
378 | // Curves are parametrised in terms of distance x (cm) along wires having 0 on the left edge of the photocathode | |
379 | Double_t x=AliRICHDigit::P2X(iPad)*PadSizeX()-0.5*PadSizeX(); //center of the padx (count from 1) | |
380 | switch(HV(iPad)){ | |
381 | case 2150: return 0.01*(9e-6*TMath::Power(x,4)+2e-7*TMath::Power(x,3)-0.0316*TMath::Power(x,2)-3e-4*x+25.367);//function is a fit in % so multiply by 0.01 | |
382 | case 2100: return 0.01*(8e-6*TMath::Power(x,4)+2e-7*TMath::Power(x,3)-0.0283*TMath::Power(x,2)-2e-4*x+23.015); | |
383 | case 2050: return 0.01*(7e-6*TMath::Power(x,4)+1e-7*TMath::Power(x,3)-0.0254*TMath::Power(x,2)-2e-4*x+20.888); | |
384 | case 2000: return 0.01*(6e-6*TMath::Power(x,4)+8e-8*TMath::Power(x,3)-0.0227*TMath::Power(x,2)-1e-4*x+18.961); | |
385 | default: return 0; | |
386 | } | |
387 | }//QdcSag() | |
388 | //++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ | |
389 | Int_t AliRICHParam::QdcTot(Int_t iPad,Double_t e) | |
390 | { | |
391 | // Calculates the total charge produced by the hit. Method: | |
392 | // 1. number of electrons is calculated as energy lost in amp gas divided by ionisation potential (for photon only one electron as Etot is always less then ionization potential) | |
393 | // 2. each electron imposes a charge distributed as Poisson with QdcEle() mean. Different pads produce different means. See QdcEle(). | |
394 | // Arguments: iPad- absolute pad number contaning the hit; | |
395 | // e- Eloss for mip in amplification gas or Etot for photon | |
396 | // Returns: charge parametrised in QDC channels. | |
397 | Int_t iNele=Int_t(e/IonPot()); if(iNele==0) iNele=1;//e < ion. pot. means it's photoelectron | |
398 | Double_t dQdc=0; | |
399 | for(Int_t i=1;i<=iNele;i++) dQdc+=-QdcEle(iPad)*TMath::Log(gRandom->Rndm()); | |
400 | return Int_t(dQdc); | |
401 | }//QdcTot() | |
402 | //++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ | |
3582c1f9 | 403 | Int_t AliRICHParam::TotQdc(TVector2 x2,Double_t eloss) |
404 | { | |
a25b3368 | 405 | //Calculates the total charge produced by the eloss in point x2 (Chamber RS). |
406 | //Returns this change parametrised in QDC channels, or 0 if the hit in the dead zone. | |
407 | //eloss=0 means photon which produces 1 electron only eloss > 0 for Mip | |
0fe8fa07 | 408 | if(Loc2Sec(x2)==-1) return 0; //hit in the dead zone |
3582c1f9 | 409 | Int_t iNelectrons=Int_t(eloss/IonisationPotential()); if(iNelectrons==0) iNelectrons=1; |
410 | Double_t qdc=0; | |
411 | for(Int_t i=1;i<=iNelectrons;i++) qdc+=-Gain(x2)*TMath::Log(gRandom->Rndm()); | |
412 | return Int_t(qdc); | |
413 | } | |
db910db9 | 414 | //++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
a25b3368 | 415 | Double_t AliRICHParam::FracQdc(const TVector2 &x2,const TVector &pad) |
3582c1f9 | 416 | { |
a25b3368 | 417 | //Calculates the charge fraction induced to given pad by the hit from the given point. |
418 | //Integrated Mathieson distribution is used. | |
e42a7b46 | 419 | TVector2 center2=Pad2Loc(pad);//gives center of requested pad |
998b831f | 420 | Double_t normXmin=(x2.X()-center2.X()-PadSizeX()/2) /Pc2Cath();//parametrise for Mathienson |
421 | Double_t normXmax=(x2.X()-center2.X()+PadSizeX()/2) /Pc2Cath(); | |
422 | Double_t normYmin=(x2.Y()-center2.Y()-PadSizeY()/2) /Pc2Cath(); | |
423 | Double_t normYmax=(x2.Y()-center2.Y()+PadSizeY()/2) /Pc2Cath(); | |
424 | ||
425 | //requested pad might not belong to the sector of the given hit position, hence the check: | |
426 | return (Loc2Sec(x2)!=Pad2Sec(pad)) ? 0:Mathieson(normXmin, normYmin, normXmax, normYmax); | |
3582c1f9 | 427 | } |
db910db9 | 428 | //++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
0422a446 | 429 | Double_t AliRICHParam::Mathieson(Double_t x1,Double_t y1,Double_t x2,Double_t y2) |
3582c1f9 | 430 | { |
db910db9 | 431 | // This is the answer to electrostatic problem of charge distrubution in MWPC described elsewhere. (NIM A370(1988)602-603) |
432 | // Arguments: x1- diff between center of distribution which is a hit position and left edge of interested pad divided by anod-cathode distance | |
433 | // x2- right edge of the pad | |
434 | // y1- up edge of the pad | |
435 | // y2- bottom edge of the pad | |
436 | // Returns: a charge fraction [0-1] imposed into the pad | |
53fd478b | 437 | const Double_t kSqrtKx3=0.77459667;const Double_t kX2=0.962;const Double_t kX4=0.379; |
438 | const Double_t kSqrtKy3=0.77459667;const Double_t kY2=0.962;const Double_t kY4=0.379; | |
c712cb2f | 439 | |
0422a446 | 440 | Double_t ux1=kSqrtKx3*TMath::TanH(kX2*x1); |
441 | Double_t ux2=kSqrtKx3*TMath::TanH(kX2*x2); | |
442 | Double_t uy1=kSqrtKy3*TMath::TanH(kY2*y1); | |
443 | Double_t uy2=kSqrtKy3*TMath::TanH(kY2*y2); | |
53fd478b | 444 | return 4*kX4*(TMath::ATan(ux2)-TMath::ATan(ux1))*kY4*(TMath::ATan(uy2)-TMath::ATan(uy1)); |
0422a446 | 445 | } |
db910db9 | 446 | //++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
a25b3368 | 447 | TVector AliRICHParam::Loc2Area(const TVector2 &x2) |
3582c1f9 | 448 | { |
db910db9 | 449 | // Calculates the area of disintegration for a given point. It's assumed here that this points lays on anode wire. |
450 | // Area is a rectangulare set of pads defined by its left-down and right-up coners. | |
e42a7b46 | 451 | TVector area(4); |
452 | TVector pad=Loc2Pad(x2); | |
453 | area[0]=area[2]=pad[0]; area[1]=area[3]=pad[1];//area is just a pad fired | |
454 | if(pad[0]!=1 && pad[0]!= NpadsXsec()+1 ) area[0]--; //left down coner X | |
455 | if(pad[1]!=1 && pad[1]!= NpadsYsec()+1 && pad[1]!= 2*NpadsYsec()+1) area[1]--; //left down coner Y | |
456 | if(pad[0]!=NpadsXsec() && pad[0]!= NpadsX() ) area[2]++; //right up coner X | |
457 | if(pad[1]!=NpadsYsec() && pad[1]!= 2*NpadsYsec() && pad[1]!= NpadsY() ) area[3]++; //right up coner Y | |
458 | return area; | |
3582c1f9 | 459 | } |
db910db9 | 460 | //++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
461 | Bool_t AliRICHParam::IsOverTh(Int_t ,TVector ,Double_t qdc) | |
3582c1f9 | 462 | { |
db910db9 | 463 | // Checks if the current QDC is over threshold and FEE will save this value to data concentrator. |
464 | // This is done on pad by pad level, so the pad pedestal map is to be used. ?????????????? | |
465 | // Arguments: | |
466 | // Returns: true if QDC over treshold | |
467 | return (qdc>NsigmaTh()*(SigmaThMean()+(1.-2*gRandom->Rndm())*SigmaThSpread())); //??????????? to be change to real values | |
3582c1f9 | 468 | } |
db910db9 | 469 | //++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
470 | TGeoMatrix* AliRICHParam::Matrix(Int_t iChamN,Int_t iPlane) | |
471 | { | |
472 | TGeoHMatrix *pMatrix=new TGeoHMatrix; | |
473 | ||
474 | const Double_t kAngHor=19.5; // horizontal angle between chambers 19.5 grad | |
475 | const Double_t kAngVer=20; // vertical angle between chambers 20 grad | |
476 | const Double_t kAngCom=30; // common RICH rotation with respect to x axis 30 grad | |
477 | ||
478 | pMatrix->RotateY(90); //rotate around y since initial position is in XY plane -> now in YZ plane | |
479 | Double_t trans[3]={490,0,0}; //center of the chamber is on window-gap surface | |
480 | ||
481 | switch(iPlane){ | |
482 | case kCenter: break; | |
483 | case kPc : trans[0]+=PcZ(); break; | |
484 | case kRad : trans[0]+=RadZ(); break; | |
485 | case kAnod : trans[0]+=AnodZ(); break; | |
486 | default: return 0; break; | |
487 | } | |
488 | pMatrix->SetTranslation(trans); //now plane in YZ is shifted along x | |
489 | ||
490 | switch(iChamN){ | |
491 | case 1: pMatrix->RotateY(kAngHor); pMatrix->RotateZ(-kAngVer); break; //right and down | |
492 | case 2: pMatrix->RotateZ(-kAngVer); break; //down | |
493 | case 3: pMatrix->RotateY(kAngHor); break; //right | |
494 | case 4: break; //no rotation | |
495 | case 5: pMatrix->RotateY(-kAngHor); break; //left | |
496 | case 6: pMatrix->RotateZ(kAngVer); break; //up | |
497 | case 7: pMatrix->RotateY(-kAngHor); pMatrix->RotateZ(kAngVer); break; //left and up | |
498 | default: return 0; break; | |
499 | }//switch(iChamber) | |
500 | pMatrix->RotateZ(kAngCom); //apply common rotation in XY plane | |
501 | return pMatrix; | |
502 | }//Matrix() | |
503 | //++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ | |
504 | TVector3 AliRICHParam::Lors2Mars(Int_t iChId,Double_t x,Double_t y,Int_t iPlnId) | |
505 | { | |
506 | // Trasform from LORS to MARS | |
507 | // Arguments: iChId - chamber code 1..7 | |
508 | // x,y - point in LORS | |
509 | // iPlnN - chamber plane code might be kPc kRad kCenter kAnod | |
510 | Double_t z=0; | |
511 | switch(iPlnId){ | |
512 | case kPc : z=PcZ() ; break; | |
513 | case kAnod : z=AnodZ(); break; | |
514 | case kCenter: z=0 ; break; | |
515 | case kRad : z=RadZ() ; break; | |
516 | } | |
517 | Double_t lors[3]={x-0.5*PcSizeX(),y-0.5*PcSizeY(),z}, mars[3]; | |
518 | fMatrix[iChId-1]->LocalToMaster(lors,mars); | |
519 | return TVector3(mars); | |
520 | } | |
521 | //++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ | |
522 | TVector2 AliRICHParam::Mars2Lors(Int_t iChId,const TVector3 &x,Int_t iPlnId) | |
523 | { | |
524 | // Trasform from MARS to LORS | |
525 | // Arguments: iChId - chamber code 1..7 | |
526 | // mars - point in MARS | |
527 | // iPlnN - chamber plane code might be kPc kRad kCenter kAnod | |
528 | Double_t z=0; | |
529 | switch(iPlnId){ | |
530 | case kPc : z=PcZ() ; break; | |
531 | case kAnod : z=AnodZ(); break; | |
532 | case kCenter: z=0 ; break; | |
533 | case kRad : z=RadZ() ; break; | |
534 | } | |
535 | Double_t lors[3],mars[3]; | |
536 | x.GetXYZ(mars); | |
537 | fMatrix[iChId-1]->MasterToLocal(mars,lors); | |
538 | return TVector2(lors[0]+0.5*PcSizeX(),lors[1]+0.5*PcSizeY()); | |
539 | } | |
540 | //++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ | |
541 | TVector3 AliRICHParam::Lors2MarsOld(Int_t iChId,Double_t x,Double_t y,Int_t iPlnId) | |
542 | { | |
543 | // Trasform from LORS to MARS | |
544 | // Arguments: iChId - chamber code 0..6 | |
545 | // x,y - point in LORS | |
546 | // iPlnN - chamber plane code might be kPc kRad kCenter kAnod | |
547 | TGeoMatrix *pMatrix=Matrix(iChId,iPlnId); | |
548 | Double_t lors[3]={x-0.5*PcSizeX(),y-0.5*PcSizeY(),0}, mars[3]; pMatrix->LocalToMaster(lors,mars); delete pMatrix; | |
549 | return TVector3(mars); | |
550 | } | |
551 | //++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ | |
552 | TVector2 AliRICHParam::Mars2LorsOld(Int_t iChamN,const TVector3 &x,Int_t iPlaneN) | |
553 | { | |
554 | TGeoMatrix *pMatrix=Matrix(iChamN,iPlaneN); | |
555 | Double_t mars[3]={x.X(),x.Y(),x.Z()} , lors[3]; pMatrix->MasterToLocal(mars,lors); delete pMatrix; | |
556 | return TVector2(lors[0]+0.5*PcSizeX(),lors[1]+0.5*PcSizeY()); | |
557 | } | |
558 | //++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ | |
559 | TVector3 AliRICHParam::Mars2LorsVec(Int_t iChamN,const TVector3 &x) | |
560 | { | |
561 | TGeoMatrix *pMatrix=Matrix(iChamN,kPc); | |
562 | Double_t mars[3]={x.X(),x.Y(),x.Z()} , lors[3]; pMatrix->MasterToLocalVect(mars,lors); delete pMatrix; | |
563 | return TVector3(lors); | |
564 | } | |
565 | //++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ | |
566 | TVector3 AliRICHParam::Center(Int_t iChamN,Int_t iPlaneN) | |
567 | { | |
568 | TGeoMatrix *pMatrix=Matrix(iChamN,iPlaneN); | |
569 | Double_t mars[3] , lors[3]={0,0,0}; pMatrix->LocalToMaster(lors,mars); delete pMatrix; | |
570 | return TVector3(mars); | |
571 | } | |
572 | //++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ | |
573 | TVector3 AliRICHParam::Norm(Int_t iChamN) | |
574 | { | |
575 | TGeoMatrix *pMatrix=Matrix(iChamN,kPc); | |
576 | Double_t mars[3] , lors[3]={0,0,1}; pMatrix->LocalToMasterVect(lors,mars); delete pMatrix; | |
577 | return TVector3(mars); | |
578 | } | |
579 | //++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ | |
580 | Int_t AliRICHParam::Hit2SDigs(Int_t iHitPad,Double_t e,TClonesArray *pSDigLst) | |
581 | { | |
582 | // Determines a number of pads affected by the hit and calculates the charge induced to each pad. | |
583 | // Integrated Mathieson distribution is used. Invoked from AliRICHvX::Hits2SDigits() | |
584 | // Arguments: iHitPad - hit pad absolute number | |
585 | // e - energy (GeV) of this hit (Eloss for mip or Etot for photon) | |
586 | // pSDigLst - pointer to clones array to store in calculated sdigits | |
587 | // Returns: total QDC for this hit | |
588 | Int_t iQtot=QdcTot(iHitPad,e); //total QDC value collected for this hit | |
589 | Int_t a=1; //analise current pad +- a pads in both directions | |
590 | Int_t iLeftX=0,iBotY=0,iRightX=0,iTopY=0; //area of disintegration for cluster formation, shifts to hit pad, not pad numbers | |
591 | if(AliRICHDigit::P2X(iHitPad) > a) iLeftX =-a;//determine area of disintegration as hit pad +- parametrised number | |
592 | if(AliRICHDigit::P2X(iHitPad) < AliRICHDigit::kPadsSecX-a) iRightX= a;//of pads. this number is determined by5 sigmas of Mathieson shape | |
593 | if(AliRICHDigit::P2Y(iHitPad) > a) iBotY =-a;//see RICH TDR page 29 | |
594 | if(AliRICHDigit::P2Y(iHitPad) < AliRICHDigit::kPadsSecY-a) iTopY = a;//also boundary conditions are checked (edge of sector aka PC) | |
595 | Int_t iPadsCnt=0; | |
596 | for(Int_t iShiftX=iLeftX;iShiftX<=iRightX;iShiftX++){//affected pads loop iShiftX is a distance (in pads) between hit pad and pad under analisys | |
597 | for(Int_t iShiftY=iBotY;iShiftY<=iTopY;iShiftY++){//affected pads loop | |
598 | iHitPad+=AliRICHDigit::kPadAbsX*iShiftX+iShiftY; | |
599 | Double_t x1=PadSizeX()/Pc2Cath()*(iShiftX-0.5);//parametrise for Mathienson | |
600 | Double_t x2=PadSizeX()/Pc2Cath()*(iShiftX+0.5);//parametrise for Mathienson | |
601 | Double_t y1=PadSizeY()/Pc2Cath()*(iShiftY-0.5);//parametrise for Mathienson | |
602 | Double_t y2=PadSizeY()/Pc2Cath()*(iShiftY+0.5);//parametrise for Mathienson | |
603 | (*pSDigLst)[iPadsCnt++]= new AliRICHDigit(iHitPad,iQtot*Mathieson(x1,y1,x2,y2)); | |
604 | }//Y loop | |
605 | }//X loop | |
606 | return iQtot; | |
607 | }//Hit2SDigs() for abs pad | |
608 | //++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ | |
609 | Int_t AliRICHParam::Hit2SDigs(TVector2 hitX2,Double_t e,TClonesArray *pSDigLst) | |
610 | { | |
611 | // Determines a number of pads affected by the hit and calculates the charge induced to each pad. | |
612 | // Integrated Mathieson distribution is used. Invoked from AliRICHvX::Hits2SDigits() | |
613 | // Arguments: hitX2 - hit position in LORS, cm | |
614 | // e - energy (GeV) of this hit (Eloss for mip or Etot for photon) | |
615 | // pSDigLst - pointer to clones array to store in calculated sdigits | |
616 | // Returns: total QDC for this hit | |
617 | Int_t iQtot=TotQdc(hitX2,e);//total charge produced by hit, 0 if hit in dead zone | |
618 | if(iQtot==0) return 0; | |
619 | ||
620 | TVector hitPad=Loc2Pad(hitX2); TVector2 padCenterX2=Pad2Loc(hitPad); //shift the hit position to the nearest anod wire | |
621 | TVector2 anod; | |
622 | if((hitX2.Y()-padCenterX2.Y())>0) anod.Set(hitX2.X(),padCenterX2.Y()+AnodPitch()/2); //upper part of the pad: shift to upper anod wire | |
623 | else anod.Set(hitX2.X(),padCenterX2.Y()-AnodPitch()/2); //lower part of the pad: shift to lower anod wire | |
624 | ||
625 | TVector area=Loc2Area(anod);//determine affected pads, dead zones analysed inside | |
626 | TVector pad(2); //current pad | |
627 | Int_t iPadsCnt=0; | |
628 | for(pad[1]=area[1];pad[1]<=area[3];pad[1]++){//affected pads loop | |
629 | for(pad[0]=area[0];pad[0]<=area[2];pad[0]++){ | |
630 | Double_t dQpad=iQtot*FracQdc(anod,pad); | |
631 | if(dQpad>0.1) (*pSDigLst)[iPadsCnt++]= new AliRICHDigit(pad,dQpad);//make sdigit if Qpad is large enough, meaning after merging there is a chance to go above threshold | |
632 | }//X loop | |
633 | }//Y loop | |
634 | return iQtot; | |
635 | }//Hit2SDigs() for TVector2 | |
636 | //++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ | |
637 | TVector3 AliRICHParam::SigmaSinglePhotonFormula(Double_t thetaCer, Double_t phiCer, Double_t theta, Double_t phi, Double_t beta) | |
638 | { | |
639 | TVector3 v(-999,-999,-999); | |
640 | ||
641 | v.SetX(AliRICHParam::ErrLoc(thetaCer,phiCer,theta,phi,beta)); | |
642 | v.SetY(AliRICHParam::ErrGeom(thetaCer,phiCer,theta,phi,beta)); | |
643 | v.SetZ(AliRICHParam::ErrCrom(thetaCer,phiCer,theta,phi,beta)); | |
644 | ||
645 | return v; | |
646 | } | |
647 | //++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ | |
648 | Double_t AliRICHParam::ErrLoc(Double_t thetaC, Double_t phiC, Double_t Ptheta, Double_t Pphi, Double_t beta) | |
649 | { | |
650 | //par->RefIdxC6F14(par->MeanCkovEnergy()) | |
651 | //(Float_t)1.29337525367736816e+00 | |
652 | Double_t RefC6F14m = 1.29337; | |
653 | Double_t Hgap = Pc2Win(); | |
654 | Double_t dphi = phiC - Pphi; | |
655 | ||
656 | Double_t alpha =TMath::Cos(Ptheta)-TMath::Tan(thetaC)*TMath::Cos(dphi)*TMath::Sin(Ptheta); | |
657 | Double_t k = 1.-RefC6F14m*RefC6F14m+alpha*alpha/(beta*beta); | |
658 | ||
659 | Double_t mu = TMath::Sin(Ptheta)*TMath::Sin(Pphi) + TMath::Tan(thetaC)*(TMath::Cos(Ptheta)*TMath::Cos(dphi)*TMath::Sin(Pphi) | |
660 | + TMath::Sin(dphi)*TMath::Cos(Pphi)); | |
661 | ||
662 | Double_t e = TMath::Sin(Ptheta)*TMath::Cos(Pphi)+TMath::Tan(thetaC)*(TMath::Cos(Ptheta)*TMath::Cos(dphi)*TMath::Cos(Pphi) -TMath::Sin(dphi)*TMath::Sin(Pphi)); | |
663 | ||
664 | Double_t kk = beta*TMath::Sqrt(k)/(Hgap*alpha); | |
665 | Double_t dtdxc = kk*(k*(TMath::Cos(dphi)*TMath::Cos(Pphi) - TMath::Cos(Ptheta)*TMath::Sin(dphi)*TMath::Sin(Pphi)) - ( alpha* | |
666 | mu/(beta*beta) )*TMath::Sin(Ptheta)*TMath::Sin(dphi)); | |
667 | ||
668 | Double_t dtdyc = kk*(k*(TMath::Cos(dphi)*TMath::Sin(Pphi) + TMath::Cos(Ptheta)*TMath::Sin(dphi)*TMath::Cos(Pphi)) + ( alpha* | |
669 | e/(beta*beta) )* TMath::Sin(Ptheta)*TMath::Sin(dphi)); | |
670 | ||
671 | return TMath::Sqrt(0.2*0.2*dtdxc*dtdxc + 0.25*0.25*dtdyc*dtdyc); | |
672 | } | |
673 | ||
674 | Double_t AliRICHParam::ErrCrom(Double_t thetaC, Double_t phiC, Double_t Ptheta, Double_t Pphi, Double_t beta) | |
675 | { | |
676 | Double_t dphi = phiC - Pphi; | |
677 | Double_t RefC6F14m = 1.29337; | |
678 | Double_t alpha =TMath::Cos(Ptheta)-TMath::Tan(thetaC)*TMath::Cos(dphi)*TMath::Sin(Ptheta); | |
679 | ||
680 | Double_t dtdn = TMath::Cos(Ptheta)*RefC6F14m*beta*beta/(alpha*TMath::Tan(thetaC)); | |
681 | ||
682 | Double_t f = 0.00928*(7.75-5.635)/TMath::Sqrt(12.); | |
683 | ||
684 | return f*dtdn; | |
685 | } | |
686 | //++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ | |
687 | Double_t AliRICHParam::ErrGeom(Double_t thetaC, Double_t phiC, Double_t Ptheta, Double_t Pphi, Double_t beta ) | |
688 | { | |
689 | ||
690 | Double_t Tr = RadThick(); | |
691 | Double_t Xep = 0.5*Tr; | |
692 | ||
693 | Double_t dphi = phiC - Pphi; | |
694 | Double_t RefC6F14m = 1.29337; | |
695 | Double_t alpha =TMath::Cos(Ptheta)-TMath::Tan(thetaC)*TMath::Cos(dphi)*TMath::Sin(Ptheta); | |
696 | ||
697 | Double_t k = 1.-RefC6F14m*RefC6F14m+alpha*alpha/(beta*beta); | |
698 | ||
699 | Double_t Hgap = Pc2Win(); | |
700 | ||
701 | ||
702 | Double_t eTr = (Tr - Xep)*beta*TMath::Sqrt(k)/(Hgap*alpha); | |
703 | Double_t lambda = 1.-TMath::Sin(Ptheta)*TMath::Sin(Ptheta)*TMath::Sin(phiC)*TMath::Sin(phiC); | |
704 | ||
705 | Double_t c = 1./(1.+ eTr*k/(alpha*alpha*TMath::Cos(thetaC)*TMath::Cos(thetaC))); | |
706 | Double_t I = beta*TMath::Tan(thetaC)*lambda*TMath::Power(k,1.5); | |
707 | Double_t II = 1.+eTr*beta*I; | |
708 | ||
709 | Double_t err = c * (I/(alpha*alpha*Hgap) + II* (1.-lambda) / ( alpha*alpha*Hgap*beta*(1.+eTr)) ); | |
710 | Double_t TrErr = Tr/(TMath::Sqrt(12.)*TMath::Cos(Ptheta)); | |
711 | ||
712 | return TrErr*err; | |
713 | }//ErrGeom() | |
714 | ||
d48cca74 | 715 | #endif //AliRICHParam_h |