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Static mass scales in hot gauge theories

The static sectors of the electroweak Standard Model and QCD at finite temperatures are described by 3d SU(N) Higgs models with scalars in the fundamental and adjoint representation, respectively. I summarize the non-perturbative physics of these theories like mass spectrum, string tension, screenin...

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Autor principal: Philipsen, O.
Lenguaje:eng
Publicado: 1999
Materias:
Acceso en línea:http://cds.cern.ch/record/379670
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author Philipsen, O.
author_facet Philipsen, O.
author_sort Philipsen, O.
collection CERN
description The static sectors of the electroweak Standard Model and QCD at finite temperatures are described by 3d SU(N) Higgs models with scalars in the fundamental and adjoint representation, respectively. I summarize the non-perturbative physics of these theories like mass spectrum, string tension, screening of the static potential and non-perturbative corrections to the Debye mass, as obtained from recent lattice simulations. It is observed that in the 3d theory corresponding to the purely magnetic sector there is a larger hierarchy between different quantities than between the electric ($\sim gT$) and magnetic ($\sim g^2T$) sectors of finite T gauge theories, which are not generally well separated.
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institution Organización Europea para la Investigación Nuclear
language eng
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spelling cern-3796702023-03-14T17:10:49Zhttp://cds.cern.ch/record/379670engPhilipsen, O.Static mass scales in hot gauge theoriesParticle Physics - PhenomenologyThe static sectors of the electroweak Standard Model and QCD at finite temperatures are described by 3d SU(N) Higgs models with scalars in the fundamental and adjoint representation, respectively. I summarize the non-perturbative physics of these theories like mass spectrum, string tension, screening of the static potential and non-perturbative corrections to the Debye mass, as obtained from recent lattice simulations. It is observed that in the 3d theory corresponding to the purely magnetic sector there is a larger hierarchy between different quantities than between the electric ($\sim gT$) and magnetic ($\sim g^2T$) sectors of finite T gauge theories, which are not generally well separated.The static sectors of the electroweak Standard Model and QCD at finite temperatures are described by 3d SU(N) Higgs models with scalars in the fundamental and adjoint representation, respectively. I summarize the non-perturbative physics of these theories like mass spectrum, string tension, screening of the static potential and non-perturbative corrections to the Debye mass, as obtained from recent lattice simulations. It is observed that in the 3d theory corresponding to the purely magnetic sector there is a larger hierarchy between different quantities than between the electric ($\sim gT$) and magnetic ($\sim g^2T$) sectors of finite T gauge theories, which are not generally well separated.hep-ph/9902376oai:cds.cern.ch:3796701999-02-18
spellingShingle Particle Physics - Phenomenology
Philipsen, O.
Static mass scales in hot gauge theories
title Static mass scales in hot gauge theories
title_full Static mass scales in hot gauge theories
title_fullStr Static mass scales in hot gauge theories
title_full_unstemmed Static mass scales in hot gauge theories
title_short Static mass scales in hot gauge theories
title_sort static mass scales in hot gauge theories
topic Particle Physics - Phenomenology
url http://cds.cern.ch/record/379670
work_keys_str_mv AT philipseno staticmassscalesinhotgaugetheories