1986
DOI: 10.1103/revmodphys.58.1021
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The physics of the quark-gluon plasma

Abstract: This paper is based on a series of eleven lectures that were presented at a workshop on The Physics of the Quark-Gluon Plasma held at Hua-Zhong Normal University in Wuhan, People's Republic of China, inSeptember 1983. The lectures were updated for publication in November 1985. They cover perturbation theory of the plasma at high temperature, as well as the nonperturbative methods and results of lattice gauge theory computations. Physical models of the conflnement-deconfinement phase transition and the modes of… Show more

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Cited by 217 publications
(130 citation statements)
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References 156 publications
(97 reference statements)
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“…Due to the confinement free quarks and gluons cannot be detected. The search for QGP has to be carried out by analyzing certain proposed hadronic and electromagnetic signatures [1,2,3,4,5,6,7,8]. However, the possible signatures of the QGP may also come in part from the late time dynamics of a hadron gas formed after the phase transition [9,10,11,12,13,14,15].…”
Section: Introductionmentioning
confidence: 99%
“…Due to the confinement free quarks and gluons cannot be detected. The search for QGP has to be carried out by analyzing certain proposed hadronic and electromagnetic signatures [1,2,3,4,5,6,7,8]. However, the possible signatures of the QGP may also come in part from the late time dynamics of a hadron gas formed after the phase transition [9,10,11,12,13,14,15].…”
Section: Introductionmentioning
confidence: 99%
“…Ultrarelativistic heavy ion collisions (HIC) provide a unique controllable experimental tool to investigate properties of nuclear matter at high temperature and small baryon density. It is believed that at the Relativistic Heavy Ion collider (RHIC) and the Large Hadron Collider (LHC), the quarks and gluons can become deconfined and form hot quark-gluon plasma (QGP) [1,2]. The main target of HIC is to study the equation of state (EoS) and transport properties of hot/dense QCD matter.…”
Section: Introductionmentioning
confidence: 99%
“…Here we assume that the known hadronic interactions can be extrapolated to 1 There is a factor 1/ √ 2 because V µ = τ a √ 2 ρ a µ , where a is the isospin index finite temperature and describe the interactions among particles in hot hadronic matter.…”
Section: Isospin Mixing At Finite Temperaturementioning
confidence: 99%