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Self-consistent quasiparticle model for quark-gluon plasma
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Self-consistent quasiparticle model for quark-gluon
plasma
Vishnu M. Bannur
Department of Physics,
University of Calicut, Kerala-673 635, India.
February 2, 2008
Abstract
Here we present a self-consistent quasi-particle model for quark-gluon plasma and apply it to explain
the non-ideal behaviour seen in lattice simulations. The basic idea, borrowed from electrodynamic
plasma, is that the gluons acquire mass as it propagates through plasma due to collective effects and is
approximately equal to the plasma frequency. The statistical mechanics and thermodynamics of such
a system is studied by treating it as an ideal gas of massive gluons. Since mass or plasma frequency
depends on density, which itself is a thermodynamic quantity, the whole problem need to be solved
self-consistently.
PACS Nos : 12.38.Mh, 12.38.Gc, 05.70.Ce, 52.25.Kn
Keywords : Equation of state, quark-gluon plasma, quasiparticle quark-gluon plasma.
1
1 Introduction :
The quasiparticle model of quark-gluon plasma (qQGP) is used to study the thermal properties of quark-
gluon plasma (QGP) [1, 2, 3, 4, 5]. QGP is a plasma of quarks and gluons which exhibits a collective
behaviour because of the interactions, governed by quantum chromodynamics (QCD). At extreamly high
temperature, the interaction may be very weak because of the asymptotic freedom and hence the plasma is
almost ideal gas of quarks and gluons. However, near and above the critical Tc, the coupling constant αs is
not weak and hence QGP may be non-ideal gas of quarks and gluons. Here Tc is the critical temperature of
phase transition or cross over from hadrons to QGP. The lattice simulation of QCD at finite temperature [6]
(LGT) and the elliptical flow observed in relativistic heavy ion collisions (RHICs) signal the existance of non-
ideal QGP. The problem of confinement-deconfinement of QCD and the search for QGP in RHICs depend
on the properties of QGP at temperature close to
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