Heavy Ion Tea
Tuesday, April 14, 2009 | 3:30 pm, Pers Hall |
Search for the QCD Critical Point Through Kurtosis of
For better sensitivity, it has been proposed to study higher
moments (Kurtosis of net-baryons, for example) of event-by-event
proton multiplicities [3] compared to the lower moments. The
kurtosis (fourth moment) of these multiplicity distribution is
expected to be proportional to seventh power of correlation length
whereas the second moment is proportional to square of correlation
length [3]. Further in Lattice calculations, which assumes the system
to be in thermal equilibrium, the kurtosis of event-by-event net-proton
is related to baryon susceptibilities. These susceptibilities shows
large values or diverge at critical temperature in presence of QCD
critical point [1, 4]. The measuring higher moments of event-by-event
identified particle multiplicity distributions will provide the
first direct connection between experimental observables and Lattice
Gauge Theory calculations [4].
In this talk, we present the first results on energy and centrality
dependence of fourth moments of event-by-event multiplicity
distributions of protons and net-protons as measured in the STAR
experiments Time Projection Chamber at RHIC. Results based on a
systematic study of various moments of cleanly identified
proton ($\bar{p}) multiplicity distribution measured at mid-rapidity
(|y| < 0.5, pT<=0.8 GeV/c) from Au+Au and Cu+Cu collisions
at $\sqrt{s_{NN}}$ = 62.4 and 200 GeV will be discussed.
The benefits from the completion of STAR Time-Of-Flight
in 2010, towards particle identification (pions and kaons) for
analysis related to isospin susceptibilities and strangeness
susceptibilities will be also briefly discussed.
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Event-by-Event
Proton Multiplicity Distributions in STAR Experiment at RHIC
Bedanga Mohanty (VECC)
Abstract:
Several experiments at RHIC, SPS and FAIR have planned to look
for the existence of QCD phase boundary and the possible critical
point by colliding heavy ions at varying incident beam energies.
The characteristic signature of existence of a critical point is
increase and divergence of fluctuations [1, 2].
References :
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[1] V. Koch, arXiv:0810.2520 [nucl-th]
[2] M. A. Stephanov, arXiv:0809.3450 [hep-ph]
[3] M. Cheng et al., arXiv:0811.1006