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f3c4a6df 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
155f1576 16
17/*
18$Log$
88cb7938 19Revision 1.3.4.1 2003/07/07 14:13:31 schutz
20NewIO
21
22Revision 1.4 2002/12/18 08:25:31 morsch
23Correction in efficiency for p < 0.5.
24
b03ac336 25Revision 1.3 2002/02/05 11:32:15 morsch
26Smearing parameters with TRD included added.
27
33e0ecee 28Revision 1.2 2002/01/18 03:27:12 morsch
29Acceptance and random rejection added.
30
155f1576 31*/
32
f3c4a6df 33
34//*-- Author: Andreas Morsch (CERN)
35
36#include "AliEMCALFast.h"
37#include <TRandom.h>
38
39
40ClassImp(AliEMCALFast)
41
42//____________________________________________________________________________
43
44
45Float_t AliEMCALFast::SmearMomentum(Int_t ind, Float_t p)
46{
47//
155f1576 48// The relative momentum error, i.e.
49// (delta p)/p = sqrt (a**2 + (b*p)**2) * 10**-2,
f3c4a6df 50// where typically a = 0.75 and b = 0.16 - 0.24 depending on multiplicity
51// (the lower value is for dn/d(eta) about 2000, and the higher one for 8000)
52//
33e0ecee 53// If we include information from TRD b will be by a factor 2/3 smaller.
54//
55// ind = 1: high multiplicity
56// ind = 2: low multiplicity
57// ind = 3: high multiplicity + TRD
58// ind = 4: low multiplicity + TRD
59
f3c4a6df 60 Float_t pSmeared;
61 Float_t a = 0.75;
62 Float_t b = 0.24;
33e0ecee 63
64 if (ind == 1) b = 0.24;
f3c4a6df 65 if (ind == 2) b = 0.16;
33e0ecee 66 if (ind == 3) b = 0.16;
67 if (ind == 4) b = 0.11;
f3c4a6df 68
69 Float_t sigma = p*TMath::Sqrt(a*a+b*b*p*p)*0.01;
70 pSmeared = p + gRandom->Gaus(0., sigma);
71 return pSmeared;
72}
73
74
75Float_t AliEMCALFast::Efficiency(Int_t ind, Float_t p)
76{
77// Tracking efficiency:
155f1576 78// above pt 0.5 GeV practically constant, between 90 and 95 % (again,
f3c4a6df 79// depending on multplicity)
80// below 0.5 GeV goes down to about 70% at 0.2 GeV.
81// On top of that there is 90% geometrical acceptance for tracking due
82// to TPC (dead zones between readout chambers).
f3c4a6df 83// Tracking
b03ac336 84//
85 Float_t eff = 0.9;
86 if (ind == 2) eff = 0.95;
87 if (p < 0.5) eff -= (0.5-p)*0.2/0.3;
88// Geometry
155f1576 89 eff *= 0.9;
f3c4a6df 90// Acceptance
91 return eff;
92}
93
155f1576 94Bool_t AliEMCALFast::EmcalAcceptance(Float_t eta, Float_t phi)
95{
96//
97// EMCAL eta-phi acceptance
98 Bool_t acc = kFALSE;
99 if (TMath::Abs(eta) < 0.7 &&
100 phi > 0. &&
101 phi < 120.*TMath::Pi()/180.)
102 acc = kTRUE;
103 return acc;
104}
105
106
107Bool_t AliEMCALFast::RandomReject(Float_t eff)
108{
109//
110// Random rejection
111 Bool_t rej = kFALSE;
112 Float_t ran = gRandom->Rndm();
113 if (ran > eff) rej = kTRUE;
114 return rej;
115}
f3c4a6df 116
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