Download presentation
Presentation is loading. Please wait.
Published byKenneth Warner Modified over 9 years ago
1
Cynthia HadjidakisTerzo Convegno sulla Fisica di ALICE Detection of photons and electrons in EMCAL Photons, Electrons and 0 at large p T Identification of photons and 0 with EMCAL Detection of electrons in EMCAL Cynthia Hadjidakis Terzo Convegno sulla Fisica di ALICE Wednesday, November 14, 2007
2
Cynthia HadjidakisTerzo Convegno sulla Fisica di ALICE Photons, 0 and electrons at large p T Direct photons prompt photons hard processes: compton (g q q) and annihilation (q q test QCD production unperturbed by the medium -jet events Neutral mesons via decay photons detection medium effect observation of hadron suppression in Heavy Ion collisions Electrons from semi-leptonic decays of b and c quarks medium effect different suppression for light and heavy quarks in Heavy Ion collisions _
3
Cynthia HadjidakisTerzo Convegno sulla Fisica di ALICE Calorimetry in ALICE PHOS: = 0.24, =100º Distance to I.P 4.40 m high granularity: 17.920 crystals E > 10 GeV E/E < 1.5% 11 Super Modules 2 SM per 20 o sector EMCAL = 1.4, = 110 o Distance to I.P 4.28 m granularity: 12.672 towers × ~ 0.014×0.014 E>10 GeV E/E < 4% Y X
4
Cynthia HadjidakisTerzo Convegno sulla Fisica di ALICE EMCal and high p T physics EMCAL capabilities: inclusive jets : E T ~ 200 GeV dijets: E T ~ 170 GeV inclusive : p T ~ 90 GeV/c inclusive : p T ~ 70 GeV/c + jet p T ~ 40 GeV/c e (semi-leptonic decay of heavy quarks ): p T ~ 25 GeV/c 10k/year Annual yields in ALICE with EMCAL
5
Cynthia HadjidakisTerzo Convegno sulla Fisica di ALICE Identification of photons and 0 in EMCAL p T < ~ 10 GeV/c10 ~ < p T < ~ 40 GeV/c merged cluster → shower shape analysis resolved clusters → invariant mass analysis small aperture angle isolation cut → talk by Gustavo R TPC candidate IP three regions of analysis
6
Cynthia HadjidakisTerzo Convegno sulla Fisica di ALICE 0 reconstruction via invariant mass → effect of the HI environment: efficiency decreases (<10%) → measured 0 yield as input of simulation to obtain the decay distribution → measurement of direct efficiency only EMCAL ● single particles ○ + HI events 1 2 invariant mass (GeV) simulation for pp and PbPb conditions high occupancy in PbPb: increase cluster energy threshold 100 MeV (pp) → 500 MeV (PbPb) m GeV simulation: single particles+HI only EMCAL - single particles + HI
7
Cynthia HadjidakisTerzo Convegno sulla Fisica di ALICE Shower shape analysis 0, longest axis of cluster ellipsoid Bayesian method developed for the PID based on a parametrization of 0 , e- ° charged hadrons 0 27 GeV fit: Landau+Gaussian 0 2 dn/d 0 2 Guénole Bourdaud
8
Cynthia HadjidakisTerzo Convegno sulla Fisica di ALICE rejection ( ) about 5 N direct /N from NLO calculations: → isolation cut needed to improve rejection Shower shape analysis → HI environment: lower efficiency (10 to 20%) → Identification of and 0 from ~10 GeV to ~40 GeV with this method (preliminary results: studies with realistic background needed) ppPbPb 0.002-0.020.01-0.1 PID for 0 PID for efficiency/purity simulation: single particles full ALICE flat and 0 distributions
9
Cynthia HadjidakisTerzo Convegno sulla Fisica di ALICE Detection of electrons in EMCaL track matching: each charged track is associated with a EMCAL cluster (if any) → add ALICE PID information from EMCAL to high p T charged tracks (TRD rejection for high p T ) simulation: single particles full ALICE Alberto Pulvirenti Mark Heinz, Jennifer Klay, Alex Donoghue p TPC / E EMCAL
10
Cynthia HadjidakisTerzo Convegno sulla Fisica di ALICE Electron identification → rejection of 100-500
11
Cynthia HadjidakisTerzo Convegno sulla Fisica di ALICE Photon Conversion Center of Collision Time Projection Chamber EMCAL Inner Tracking System TRD and TOF 50% of photons convert into e + e - → 45% of photons convert into TRD and TOF → removed by p/E cut Other sources of background: photon conversion and Dalitz decay X (cm) Y (cm)
12
Cynthia HadjidakisTerzo Convegno sulla Fisica di ALICE Conclusion EMCAL improves ALICE capabilities to measure high p T photons, electrons and 0 Direct photons and 0 measurements Identification with invariant mass technique up to p T ~ 10 GeV/c Identification with shower shape analysis up to p T ~ 40 GeV/c Isolation cut to improve rejection and for higher p T region Detection of electrons Electron identification and good rejection with track matching
Similar presentations
© 2024 SlidePlayer.com. Inc.
All rights reserved.