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Hadron resonance gas and nonperturbative QCD vacuum at finite temperature

  • Fields, Particles, and Nuclei
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Abstract

Nonperturbative QCD vacuum with two light quarks at finite temperature was studied in a hadron resonance-gas model. Temperature dependences of the quark and gluon condensates in the confined phase were obtained. It is shown that the quark condensate and one-half (chromoelectric component) of the gluon condensate are evaporated at the same temperature corresponding to the quark-hadron phase transition. With allowance for the temperature shift of hadron masses, the critical temperature was found to be T c ≃190 MeV.

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Translated from Pis’ma v Zhurnal Éksperimental’no\(\overset{\lower0.5em\hbox{$\smash{\scriptscriptstyle\smile}$}}{l} \) i Teoretichesko\(\overset{\lower0.5em\hbox{$\smash{\scriptscriptstyle\smile}$}}{l} \) Fiziki, Vol. 78, No. 10, 2003, pp. 1099–1102.

Original Russian Text Copyright © 2003 by Agasian, Fedorov.

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Agasian, N.O., Fedorov, S.M. Hadron resonance gas and nonperturbative QCD vacuum at finite temperature. Jetp Lett. 78, 607–610 (2003). https://doi.org/10.1134/1.1644301

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  • DOI: https://doi.org/10.1134/1.1644301

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