QCD Phase Transition at Finite Temperature in the Dual Ginzburg-Landau Theory

Details QCD Phase Transition at Finite Temperature in the Dual Ginzburg-Landau Theory QCD Phase Transition at Finite Temperature in the Dual Ginzburg-Landau Theory

1995-02-11

arxiv.org/abs/hep-ph/9502278v1

Phys.Rev. D52 (1995) 2944-2950

Physics

High Energy Physics

High Energy Physics - Phenomenology

13 pages, uses PHYZZX ( 5 figures - available on request from ichie@atlas.phys.metro-u.ac.jp )

Scientific paper

10.1103/PhysRevD.52.2944

We study the pure-gauge QCD phase transition at finite temperatures in the dual Ginzburg-Landau theory, an effective theory of QCD based on the dual Higgs mechanism. We formulate the effective potential at various temperatures by introducing the quadratic source term, which is a new useful method to obtain the effective potential in the negative-curvature region. Thermal effects reduce the QCD-monopole condensate and bring a first-order deconfinement phase transition. We find a large reduction of the self-interaction among QCD-monopoles and the glueball masses near the critical temperature by considering the temperature dependence of the self-interaction. We also calculate the string tension at finite temperatures.

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