Zero density heavy quark SU(2) gauge theory and the Stefan-Boltzmann limit

dc.creatorLangfeld, Kurt
dc.creatorLages, Norbert
dc.creatorReinhardt, Hugo
dc.date2005-09-27
dc.date.accessioned2026-07-07T06:23:42Z
dc.date.available2026-07-07T06:23:42Z
dc.descriptionSU(2) lattice gauge theory is investigated where the traces of the Wilson lines at any lattice point and along each direction is constrained to zero. Hence, each of the lattice configurations possesses a vanishing density of heavy (anti-) quarks. The results are compared with those of pure SU(2) gauge theory which can be interpreted as the grand canonical realization of the heavy quark theory where only the ensemble average of the heavy quark density vanishes. The static quark anti-quark potential of the constrained theory is obtained from (spatially smeared) Wilson loops at zero temperature. We find that the potential coincides with that of pure SU(2) gauge theory (without constraints). Hence, the familiar "running" of the lattice spacing with beta is recovered.
dc.descriptionpresented at Lattice2005(Nonzero temperature and density), Dublin, July 25-30, 2005, 6 pages, 4 figures, to appear in Proceedings of Science
dc.identifierhttps://arxiv.org/abs/hep-lat/0509156
dc.identifierhttp://arxiv.org/abs/hep-lat/0509156
dc.identifierPoS LAT2005 (2005) 201
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/96328
dc.subjectHigh Energy Physics - Lattice
dc.titleZero density heavy quark SU(2) gauge theory and the Stefan-Boltzmann limit
dc.typetext

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