* provided "as is" without express or implied warranty. *
**************************************************************************/
-/* $Id$ */
+
+/*
+$Log$
+Revision 1.2 2002/01/18 03:27:12 morsch
+Acceptance and random rejection added.
+
+*/
+
//*-- Author: Andreas Morsch (CERN)
Float_t AliEMCALFast::SmearMomentum(Int_t ind, Float_t p)
{
//
-// The relative momentum error, i.e. (delta p)/p = sqrt (a**2 + (b*p)**2) *
-// 10**-2,
+// The relative momentum error, i.e.
+// (delta p)/p = sqrt (a**2 + (b*p)**2) * 10**-2,
// where typically a = 0.75 and b = 0.16 - 0.24 depending on multiplicity
// (the lower value is for dn/d(eta) about 2000, and the higher one for 8000)
//
+// If we include information from TRD b will be by a factor 2/3 smaller.
+//
+// ind = 1: high multiplicity
+// ind = 2: low multiplicity
+// ind = 3: high multiplicity + TRD
+// ind = 4: low multiplicity + TRD
+
Float_t pSmeared;
Float_t a = 0.75;
Float_t b = 0.24;
+
+ if (ind == 1) b = 0.24;
if (ind == 2) b = 0.16;
+ if (ind == 3) b = 0.16;
+ if (ind == 4) b = 0.11;
Float_t sigma = p*TMath::Sqrt(a*a+b*b*p*p)*0.01;
pSmeared = p + gRandom->Gaus(0., sigma);
Float_t AliEMCALFast::Efficiency(Int_t ind, Float_t p)
{
// Tracking efficiency:
-// above pt 0.5 GeV practically constant, between 90 and 95 % (agian,
+// above pt 0.5 GeV practically constant, between 90 and 95 % (again,
// depending on multplicity)
// below 0.5 GeV goes down to about 70% at 0.2 GeV.
// On top of that there is 90% geometrical acceptance for tracking due
} else {
eff = eff-(0.5-p)*0.2/0.3;
}
- eff*= 0.9;
+ eff *= 0.9;
// Acceptance
return eff;
}
+Bool_t AliEMCALFast::EmcalAcceptance(Float_t eta, Float_t phi)
+{
+//
+// EMCAL eta-phi acceptance
+ Bool_t acc = kFALSE;
+ if (TMath::Abs(eta) < 0.7 &&
+ phi > 0. &&
+ phi < 120.*TMath::Pi()/180.)
+ acc = kTRUE;
+ return acc;
+}
+
+
+Bool_t AliEMCALFast::RandomReject(Float_t eff)
+{
+//
+// Random rejection
+ Bool_t rej = kFALSE;
+ Float_t ran = gRandom->Rndm();
+ if (ran > eff) rej = kTRUE;
+ return rej;
+}