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Measurements of identified hadron production at high p T in p+p and Au+Au collisions at RHIC-STAR. 许依春 (Yichun Xu) Center for Particle Physics and Technology University of Science and Technology of China. Outline. Motivation - PowerPoint PPT Presentation
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2010/04/18 Yichun Xu@HEP8th-Nanchang 1
Measurements of identified hadron production at high pT in p+p and Au+Au collisions at RHIC-STAR许依春 (Yichun Xu)Center for Particle Physics and Technolo
gyUniversity of Science and Technology of
China
2010/04/18 Yichun Xu@HEP8th-Nanchang 2
Outline Motivation
In p+p, extend identified hadron spectra study up to pT~15 GeV/c Good constraints to pQCD calculation. Baseline for study of nuclear modification factor in HIC.
In Au+Au, study of nuclear modification factor (RAA) Color charge effect, Jet conversion, Jet hadrochemistry
Data analysis Identify charged , K, p and pbar by dE/dx Reconstruct K0
S with one triggered daughter
Results & Summary
2010/04/18 Yichun Xu@HEP8th-Nanchang 3
Extend Charged hadron spectra in p+p
Proton spectra was limited to 7GeV/c with current statistics from minbias p+p @ STAR.[1]
In Au+Au, it has been extended to 12GeV/c. [2][1] Phys. Lett. B 637 (2006) 161 [2] Phys. Rev. Lett. 97 (2006) 152301
2010/04/18 Yichun Xu@HEP8th-Nanchang 4
Energy loss and QCD
Color charge effect of parton energy loss
ddpdddpNd
NR
Tpp
TAB
binAB /
/12
2
Eg
Eq
~ 9/4In pQCD:
hardparton
path length L
Quark
Quark
RAA(p)<RAA()STAR: PRL97,152301(2006)
2010/04/18 Yichun Xu@HEP8th-Nanchang 5
Jet Conversion
hardparton
path length L
Quark
gluon
W. Liu, R.J. Fries, Phys. Rev. C77 (2008) 054902
q + qbar g + g
q(qbar) + g g + q(qbar)
W. Liu, C.M. Ko, B.W. Zhang, Phys. Rev. C 75, 051901 (2007).
2010/04/18 Yichun Xu@HEP8th-Nanchang 6
Jet hadrochemistry
Enhanced parton splitting in medium calculation for LHC. Mechanism may lead to higher p/ and K/ ratios in A+A jets.
S.Sapeta and U.A. Wiedemann, arXiv:0707.3494
2010/04/18 Yichun Xu@HEP8th-Nanchang 7
±/K±/p(p) with dE/dx
Where Bπ is the expected mean dE/dx of from Bichsel function of ionization energy loss in TPC.
pT>3GeV
)/)/log(( BdxdEn XX
STAR preliminary
- +
Nucl. Instru. & Meth. A 614 (2010) 28–33Nucl. Instr. & Meth. A 558 (2006) 419
2010/04/18 Yichun Xu@HEP8th-Nanchang 8
K0S with triggered
K0S→(trg)
Barrel Electro-Magnetic Calorimeter
K0S
Triggered by tower
STAR preliminary
STAR preliminary
2010/04/18 Yichun Xu@HEP8th-Nanchang 9
Kaon in p+p collisions
Charged and neutral kaons are extended up to 15 GeV/c in p+p collisions.
Charged and neutral kaons are consistent.
Phys. Rev. C 75 (2007) 64901
STAR preliminary STAR preliminary
AKK: S. Albino, B. A. Kniehl, and G. Kramer, arXiv: 0803.2768v2DSS: Daniel de Florian, Werner Vogelsang, and Federico Wagner, arXiv: 0708.3060v3
2010/04/18 Yichun Xu@HEP8th-Nanchang 10
Constraint for pQCD calculation
[1] arXiv:0803.2768 , [2] Phys. Rev. Lett. 98, 252001 (2007)
Simon, private communication
Our data will provide a better constraint on Fragmentation Function!
2010/04/18 Yichun Xu@HEP8th-Nanchang 11
Particles Ratios in p+p collisions
Experimental data:(Consistent with published data)1. +, p/p: decrease with p
T indicates a significant quark jet contribution not only to meson but also to baryon.
2. p/ and p/: p/~0.2, and p/~0.1
Compare to models:1. PYTHIA(v6.205) describe
ratios reasonably.2. DSS over-predicts anti-pr
otons relative to pions and protons.
PLB 637 (2006) 161
STAR preliminary
2010/04/18 Yichun Xu@HEP8th-Nanchang 12
RAA for , K and p1. RAA(proton)>RAA(pion)@ high pT
Which is in contrast to the prediction of color charge dependence of Energy Loss.
How the gluon jet/quark jet interact with the medium created in Au+Au collisions?
2. RAA(K) ~ 0.4 at high pT > 5.0 GeV/c
Consistent with the prediction of jet conversion by interaction with the medium in Au+Au.
3. RAA() ~ RAA() at high pT
Light quark mesons have no mass effect
pT (GeV/c)
STAR preliminary
2010/04/18 Yichun Xu@HEP8th-Nanchang 13
RAA vs Npart
Integral RAA at pT>5.5 GeV/c, <pT
>~6.2 GeV/c
RAA for kaon and pion are suppressed more in central collisions.
RAA for kaon > RAA for pion, even in peripheral collisions.
=> Does jet chemistry change in small system?
2010/04/18 Yichun Xu@HEP8th-Nanchang 14
Summary
p+p collisions: Extend identified hadron spectra up to 15 GeV/c in p+p. Provide constraints for Fragmentation Function. Indicates a significant quark jet contribution to baryon from
decrease of pbar/p with pT .
Au+Au collisions: No mass effect from RAA() ~ RAA()
Color charge effect cannot explain RAA(p) > RAA().
RAA(K)~0.4 in central Au+Au collisions is consistent with the prediction of Jet Conversion in the medium.
Thanks for your attention!
2010/04/18 Yichun Xu@HEP8th-Nanchang 15
2010/04/18 Yichun Xu@HEP8th-Nanchang 16
with triggered p
can be extended up to 10 GeV/c in p+p collisions with the triggered data sample, which will provide additional probe for the jet conversion.
_
7<pT<8 GeV/c
STAR preliminary
2010/04/18 Yichun Xu@HEP8th-Nanchang 17
Experiment and Data set
Time Projection Chamber (TPC) Electro-Magnetic Calorimeter (EMC)
Data set:EMC Triggers in run5 pp @ 200GeV Jet Patch trigger: ETtot>6.4 GeV High Tower trigger: ET>2.5 GeV ET>3.6 GeV Central trigger in run4 AuAu@200GeV
2010/04/18 Yichun Xu@HEP8th-Nanchang 18
Triggered and enhancement factor
STAR preliminary
Given pT=5 GeV/c, ~5.6M HT1 triggered events are equivalent to
L(0.64 pb-1)*(30mb)*effTrg(3%)/effTrk(90%) ~600M minibias evts.
A factor of 100 enhancement