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QCD Phase Transition and Hadron Bubble Formation in the Dual Ginzburg-Landau Theory

1996/02/27 by H. Ichie, Ichie, H., H. Monden +6
Physics and Astronomy · #Cosmology and Gravitation Theories #FOS: Physical sciences #High Energy Physics - Phenomenology (hep-ph) #High-Energy Particle Collisions Research #Theoretical and Computational Physics #hep-ph

paper · pdf · doi:10.48550/arxiv.hep-ph/9602413

Talk presented by H. Ichie at International Symposium on 'Nuclear Reaction Dynamics of Nucleon-Hadron Manybody System', Dec. 1995, RCNP Osaka. 5 pages, Revtex, (10 figures - available on request from [email protected] )

arxiv created 1996/02/27 · openalex publication_date 1996/02/27 · arxiv updated 2009/11/30 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28

Abstract

We study the QCD phase transition at finite temperature and discuss the hadron bubble formation in the dual Ginzburg-Landau theory, which is an effective theory of QCD and describes the color confinement via QCD-monopole condensation. We formulate the effective potential at various temperatures and find that thermal effects reduce the QCD-monopole condensate and bring a first-order deconfinement phase transition. Based on this effective potential at finite temperature, we investigate properties of hadron bubbles created in the early Universe and discuss the hadron bubble formation process.

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