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Jaroslav Bielcik

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Jaroslav Bielcik, Yale/BNL. 1. Rencontres de Moriond 2006 ... Me e- 0.14 GeV/c2 flagged photonic. Correct for primary electrons. misidentified as background ... – PowerPoint PPT presentation

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Title: Jaroslav Bielcik


1
Heavy flavor physics in STAR
  • Jaroslav Bielcik
  • Yale University/BNL
  • Motivation
  • Charm via hadronic decays
  • STAR and electron ID
  • Analysis of nonphotonic electrons
  • Results pp, dAu, and AuAu at ?sNN 200 GeV
  • Summary

2
Light quarks sector
  • Inclusive yields and back-to-back di-hadron
    correlations are very similar in
  • pp and dAu collisions
  • Both are strongly suppressed in central AuAu
    collisions at 200 GeV
  • Large energy loss of light quarks in the formed
    nuclear matter

Energy loss depends on properties of medium
(gluon densities, size)
depends on properties of probe (color charge,
mass)
3
Heavy quarks sector
D, B
  • D,B spectra are affected by energy loss
  • Effect of elastic energy loss for heavy quarks
  • M.G.Mustafa Phys. Rev C 72 (2005)

4
Measuring charm and beauty
  • Hadronic decay channels D0?Kp, D?D0p,
    D/-?Kpp
  • Non-photonic electrons
  • Semileptonic channels
  • c ? e anything (B.R. 9.6)
  • D0 ? e anything (B.R. 6.87)
  • D? ? e? anything (B.R. 17.2)
  • b ? e anything (B.R. 10.9)
  • B? ? e? anything (B.R. 10.2)
  • Drell-Yan (small contribution for pT lt 10 GeV/c)
  • Photonic electron background
  • g conversions (p0 ? gg g ? ee- )
  • p0, h, h Dalitz decays
  • r, f decays (small)
  • Ke3 decays (small)

5
Charm reconstruction via hadronic decays
Total charm cross section per NN interaction
dAu 1.4 ? 0.2(stat.) ? 0.4(sys.) mb
AuAu 1.11? 0.08(stat.) ? 0.42(sys.) mb
Binary scaling dAu to AuAu ? Charm produced in
initial phase of the


collision
6
Expected electron nuclear modification factor
RAA
Two different theories
Single e- from FONLL
scaled to
M. Cacciari et al., Phys.Rev.Lett 95 (2005)
Theory I Djordjevic et al.(DVGL)
  • Beauty predicted to dominate above 4-5 GeV/c

dNg/dy1000 small suppression RAA 0.7
for cb
dNg/dy3500 medium suppression RAA 0.5 for
cb
Theory II Armesto et al.
7
STAR Detector and Data Sample
  • Electrons in STAR
  • TPC tracking, PID hlt1.3 f2p
  • BEMC (tower, SMD) PID 0lthlt1 f2p
  • TOF patch

Preliminary results from
Run2003/2004 min. bias. 6.7M events
with half field high tower
trigger 2.6M events with full field (45
of all) 10 central
4.2M events (15 of all )
8
Electron ID in STAR EMC
  • TPC dE/dx for p gt 1.5 GeV/c
  • Only primary tracks
  • (reduces effective radiation length)
  • Electrons can be discriminated well from hadrons
    up to 8 GeV/c
  • Allows to determine the remaining hadron
    contamination after EMC
  • EMC
  • Tower E ? p/E
  • Shower Max Detector (SMD)
  • Hadrons/Electron shower develop different shape
  • Use hits cuts
  • 85-90 purity of electrons
  • (pT dependent)
  • h discrimination power 103-104

8
9
Photonic electrons background
  • Background Mainly from g conv and p0,h Dalitz
  • Rejection strategy
  • For every electron candidate
  • Combinations with all TPC
  • electron candidates
  • Mee-lt0.14 GeV/c2 flagged photonic
  • Correct for primary electrons
  • misidentified as background
  • Correct for background rejection efficiency
  • 50-60 for central AuAu

Inclusive/Photonic
  • Excess over photonic electrons observed
  • for all system and centralities
  • gt non-photonic signal

10
STAR non-photonic electron spectra pp, dAu, AuAu
?sNN 200 GeV
  • pp, dAu up to 10 GeV/c
  • AuAu 0-5, 10-40, 40-80
  • up to 8 GeV/c
  • Photonic electrons subtracted
  • Corrected for 10-15 hadron contamination

11
RAA nuclear modification factor
Armesto et al. hep-th/0511257 van
Hess et al. hep-th/0508055 Wicks et
al. (DVGL) hep-th/0512076
  • Suppression up to 0.5-0.6 observed in 40-80
    centrality
  • 0.5 -0.6 in centrality 10-40
  • Strong suppression up to 0.2 observed at high
    pT in 0-5
  • Maximum of suppression at pT 5-6 GeV/c

Theories currently do not describe the data well
Only c contribution would be consistent with
the RAA but not the pp spectra
12
Large electrons suppression is a PUZZLE
  • Large suppression gt large dE/dx of heavy
    quarks (NOT EXPECTED)

Not enough, RAA saturates!
  • Where b starts to play a role?

Maybe higher at pT?
  • Elastic energy loss?

Important, helps, but not enough!
  • Recent study on 3 body cqq
  • elastic scattering in QGP

No beauty included!
13
Summary
  • Direct charm reconstruction in dAu and AuAu
    from hadronic decays


  • (binary scalling)
  • Charm is produced in initial phase
    of the collision
  • Non-photonic electrons from heavy flavor decays
    were measured in ?s 200 GeV pp, dAu and AuAu
    collisions by STAR up to pT10 GeV/c
  • Expected to have contribution from
    both charm and beauty
  • Strong suppression of non-photonic electrons has
    been observed in AuAu, increasing with
    centrality
  • Suggests large energy loss for heavy
    quarks

  • (similar to light quarks )
  • Theoretical attempts to explain it seem to fail
    if both bc are included
  • What is the contribution of b? Are
    there other/different

  • contributions to energy loss?
  • It is desirable to separate contribution bc
    experimentally
  • detector upgrades (displaced vertex)
  • e-h correlations
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