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Production and Suppression in Heavy Ion Collisions at STAR. February 5, 2013. Anthony Kesich University of California, Davis STAR Collaboration. Outline. Motivation for measuring Upsilons The S olenoidal T racker A t R HIC and its triggers production cross section in p+p - PowerPoint PPT Presentation
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Production and Suppression in Heavy Ion Collisions at STAR
Anthony KesichUniversity of California, Davis
STAR Collaboration
February 5, 2013
2
Outline
• Motivation for measuring Upsilons• The Solenoidal Tracker At RHIC and its
triggers• production cross section in p+p• production in d+Au• Nuclear Modification Factor in Au+Au• Suppression Models• Conclusions
February 5, 2013 WWND 2013 - A. Kesich
WWND 2013 - A. Kesich 3
Goal: Quarkonia states in A+ACharmonia: J/Ψ, Ψ’, χc Bottomonia: (1S), (2S), (3S),χB Key Idea: Quarkonia Melt in the plasma
• Color screening of static potential between heavy quarks• Suppression of states is determined by TC and their binding energy• Lattice QCD: Evaluation of spectral functions Tmelting• Originaly proposed by Matsui & Satz (1986)
When do states melt?
February 5, 2013
H. Satz, HP06
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WWND 2013 - A. Kesich 4
Quarkonia at RHIC
• A cleaner probe compared to J/Ψ • co-mover absorption → negligible• recombination → negligible
• σcc = ~800 µb• σbb= ~ 2µb
• Challenge: low rate, rare probe– Large acceptance detector– Efficient trigger
February 5, 2013
Why do at RHIC instead of J/Ψ?
R. R
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Regeneration of J/ψ!
WWND 2013 - A. Kesich 5
STAR
EM Calorimeter
•|η| < 1•Full φ coverage•Electron ID via E/p•Event Triggering
Time Projection Chamber
•|η| < 1•Full φ coverage•Tracking and EID via Ionization
February 5, 2013
WWND 2013 - A. Kesich 6
Triggering on decays
February 5, 2013
Level 0 Trigger (p+p,d+Au,Au+Au):•Hardware-based•Fires on at least one high tower
Level 2 Trigger (p+p,d+Au):•Software-based•Calculates:• Cluster energies• Opening angle• Mass
High rejection rate allowed us to sample entire luminosity
WWND 2013 - A. Kesich 7
in p+p 200 GeV
February 5, 2013
N(total)= 145±26(stat.)
STAR Preliminary
Phys
. Rev
. D 8
2 (2
010)
120
04
2009, ∫L dt = 19.7 pb-1 2006, ∫L dt = 7.9 pb-1
Statistical error reduced bya factor of 2!
WWND 2013 - A. Kesich 8
in p+p 200 GeV, Comparisons
February 5, 2013
STAR √s=200 GeV p+p ++→e+e- cross section consistent with pQCD and world data trend
STAR Preliminary
CEM
: R. V
ogt,
Phys
. Rep
. 462
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WWND 2013 - A. Kesich 9
in d+Au 200 GeV
February 5, 2013
∫L dt = 32.6 nb-1
N = 79 ± 17 (stat.) ± 13 (syst.)
Signal has ~8σ significancepT reaches ~8 GeV/c
STAR Preliminary
Efficiency/calibrations under study
WWND 2013 - A. Kesich 10
in Au+Au 200 GeV
February 5, 2013
Raw yield of e+e- with |y|<0.5 = 197 ± 36∫L dt ≈ 1400 µb-1
WWND 2013 - A. Kesich 11
in Au+Au 200 GeV, Centrality
February 5, 2013
Peripheral Central
STAR Preliminary
STAR Preliminary
STAR Preliminary
WWND 2013 - A. Kesich 12
in Au+Au 200 GeV, RAA
February 5, 2013M
odel
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. Stri
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. Baz
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•Strickland uses a dynamic model with fireball expansion and feed-down• Results are consistent with complete 2S and 3S suppression in
this model• Model is assumes a T0 in the range of 428-442 MeV and 1/4π<
η/S < 3/4π•Emerick & Rapp band covers two scenarios:• Binding energy of the Upsilon decreases with T (Weak Binding)• Suppression is due to gluo-dissociation of Upsilon (Strong
Binding)
WWND 2013 - A. Kesich 13
Outlook
February 5, 2013
Au+Au @ 200 GeV, 2011• Same setup as in 2010• Double the total luminosity
• Approximately 2.8 nb-1
p+p @ 500 GeV, 2011• High energy doubles Upsilon cross section• Excited-to-ground state ratio• PT spectrum• Approximately 22 pb-1 of data
WWND 2013 - A. Kesich 14
Outlook
February 5, 2013
New muon detectors will open up a second, cleaner channelfor Upsilon detection. About 60% of it is currently installed.Important due to increased material in the detector from new vertexer
Statistical Error Projection for Muon Detectors
WWND 2013 - A. Kesich 15
Conclusions
• Measured production in p+p, d+Au, and Au+Au collisions at 200 GeV
• Au+Au results consistent with 2S and 3S suppression
• Increased Au+Au statistics from run 11 will further decrease RAA uncertainties
• New muon channel will enhance and compliment our electron measurementsFebruary 5, 2013
WWND 2013 - A. Kesich 16February 5, 2013
Thank you