Magnetic component of Yang-Mills plasma

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dc.creatorChernodub, M. N.
dc.creatorZakharov, V. I.
dc.date2006-11-17
dc.date2007-02-22
dc.date.accessioned2026-07-07T10:37:24Z
dc.date.available2026-07-07T10:37:24Z
dc.descriptionConfinement in non-Abelian gauge theories is commonly ascribed to percolation of magnetic monopoles, or strings in the vacuum. At the deconfinement phase transition the condensed magnetic degrees of freedom are released into gluon plasma as thermal magnetic monopoles. We point out that within the percolation picture lattice simulations can be used to estimate the monopole content of the gluon plasma. We show that right above the critical temperature the monopole density remains a constant function of temperature, as for a liquid, and then grows, like for a gas.
dc.description4 pages, no figures; replaced to match published version
dc.identifierhttps://arxiv.org/abs/hep-ph/0611228
dc.identifierhttp://arxiv.org/abs/hep-ph/0611228
dc.identifierPhys.Rev.Lett.98:082002,2007
dc.identifierdoi:10.1103/PhysRevLett.98.082002
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/180371
dc.subjectHigh Energy Physics - Phenomenology
dc.subjectOther Condensed Matter
dc.subjectHigh Energy Physics - Lattice
dc.subjectHigh Energy Physics - Theory
dc.subjectPlasma Physics
dc.titleMagnetic component of Yang-Mills plasma
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