The Quark gluon plasma in equilibrium
By Dirk H. Rischke. 2003
365 citations recorded by the source corpus.
Abstract Our current knowledge of the quark–gluon plasma in thermodynamical equilibrium is reviewed. The phase diagram of strongly interacting matter is discussed, with emphasis on the quark–hadron phase transition and the colour-superconducting phases of quark matter. Lattice quantum chromodynamics results on the order of the phase transition, the thermodynamical functions, the heavy quark free energy, mesonic spectral functions, and recent results for nonzero quark chemical potential are presented. Analytic attempts to compute the thermodynamical properties of strongly interacting matter, such as perturbation theory, quasiparticle models, “hard-thermal-loop”-resummed perturbation theory, the Polyakov-loop model, as well as linear sigma models are discussed. Finally, colour-superconducting quark matter is considered in the limit of weak coupling. The gap equation and the excitation spectrum are derived. The solution of the gap equation, gap parameters in various colour-superconducting phases, and critical temperatures for the transition to normal-conducting quark matter are presented. A summary of gluon and photon properties in colour superconductors is given.
Subfields: Astronomy and Astrophysics, Condensed Matter Physics, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/5fea319c660eb4a4132fe998ca13ff23b1dbd25e
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Citations in the corpus
- QCD at finite temperature and chemical potential from Dyson–Schwinger equations (2018, neutral): “[25, 45–52].”
- Polyakov loop modeling for hot QCD (2017, background): “[10, 11, 12] for phenomenological implications of the Polyakov loop to the QGP physics.”
- The phase diagram of dense QCD (2010, background): “For the topics not covered in the present article, readers may consult other reviews [7, 8, 9, 10, 11, 12, 13, 14, 15, 16, 17, 18, 19].”
- Hybrid Stars that Masquerade as Neutron Stars (2004, background): “This costs free energy, which is offset by the pairing contribution ¼ 3 2 2 2 þ O( 4): ð9Þ Calculations of with effective interactions yield values in the range 10–100 MeV (Rajagopal & Wilczek 2001; Alford 2001; Rischke 2004; Schäfer 2003; Reddy 2002; Shovkovy 2004) for in the range 300–600 MeV.”