Confinement bubble wall velocity via quasiparticle determination

Abstract Lattice simulations reveal that the deconfinement-confinement phase transition (PT) of the hot pure SU(N > 2) Yang-Mills system is first order. This system can be described by a pool of quasigluons moving in the Polyakov loop background, and in this picture, we establish an effective dis...

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Main Authors: Zhaofeng Kang, Jiang Zhu
Format: Article
Language:English
Published: SpringerOpen 2025-05-01
Series:Journal of High Energy Physics
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Online Access:https://doi.org/10.1007/JHEP05(2025)056
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author Zhaofeng Kang
Jiang Zhu
author_facet Zhaofeng Kang
Jiang Zhu
author_sort Zhaofeng Kang
collection DOAJ
description Abstract Lattice simulations reveal that the deconfinement-confinement phase transition (PT) of the hot pure SU(N > 2) Yang-Mills system is first order. This system can be described by a pool of quasigluons moving in the Polyakov loop background, and in this picture, we establish an effective distribution function for quasigluons, which encodes interactions among quasigluons and in particular the confinement effect. With it, we made the first attempt to calculate the confinement bubble wall velocity v w at the microscopical level, and we obtained a small velocity v w ~ 0.04 using two different approaches, which is qualitatively consistent with others results like holography.
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issn 1029-8479
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spelling doaj-art-22dd95d802b9471bb3953ed8a6e9bcc62025-08-20T03:10:38ZengSpringerOpenJournal of High Energy Physics1029-84792025-05-012025512110.1007/JHEP05(2025)056Confinement bubble wall velocity via quasiparticle determinationZhaofeng Kang0Jiang Zhu1School of Physics, Huazhong University of Science and TechnologySchool of Physics, Huazhong University of Science and TechnologyAbstract Lattice simulations reveal that the deconfinement-confinement phase transition (PT) of the hot pure SU(N > 2) Yang-Mills system is first order. This system can be described by a pool of quasigluons moving in the Polyakov loop background, and in this picture, we establish an effective distribution function for quasigluons, which encodes interactions among quasigluons and in particular the confinement effect. With it, we made the first attempt to calculate the confinement bubble wall velocity v w at the microscopical level, and we obtained a small velocity v w ~ 0.04 using two different approaches, which is qualitatively consistent with others results like holography.https://doi.org/10.1007/JHEP05(2025)056Phase Transitions in the Early UniverseCosmology of Theories BSMNew Gauge InteractionsSpecific BSM Phenomenology
spellingShingle Zhaofeng Kang
Jiang Zhu
Confinement bubble wall velocity via quasiparticle determination
Journal of High Energy Physics
Phase Transitions in the Early Universe
Cosmology of Theories BSM
New Gauge Interactions
Specific BSM Phenomenology
title Confinement bubble wall velocity via quasiparticle determination
title_full Confinement bubble wall velocity via quasiparticle determination
title_fullStr Confinement bubble wall velocity via quasiparticle determination
title_full_unstemmed Confinement bubble wall velocity via quasiparticle determination
title_short Confinement bubble wall velocity via quasiparticle determination
title_sort confinement bubble wall velocity via quasiparticle determination
topic Phase Transitions in the Early Universe
Cosmology of Theories BSM
New Gauge Interactions
Specific BSM Phenomenology
url https://doi.org/10.1007/JHEP05(2025)056
work_keys_str_mv AT zhaofengkang confinementbubblewallvelocityviaquasiparticledetermination
AT jiangzhu confinementbubblewallvelocityviaquasiparticledetermination