Thermodynamics of SU(3) gauge theory on anisotropic lattices

dc.creatorPACS Collaboration
dc.creatorNamekawa, Y.
dc.creatorAoki, S.
dc.creatorBurkhalter, R.
dc.creatorEjiri, S.
dc.creatorFukugita, M.
dc.creatorHashimoto, S.
dc.creatorIshizuka, N.
dc.creatorIwasaki, Y.
dc.creatorKanaya, K.
dc.creatorKaneko, T.
dc.creatorKuramashi, Y.
dc.creatorLesk, V.
dc.creatorOkamoto, M.
dc.creatorOkawa, M.
dc.creatorTaniguchi, Y.
dc.creatorUkawa, A.
dc.creatorYoshié, T.
dc.date2001-05-15
dc.date2001-07-02
dc.date.accessioned2026-07-07T10:32:29Z
dc.date.available2026-07-07T10:32:29Z
dc.descriptionFinite temperature SU(3) gauge theory is studied on anisotropic lattices using the standard plaquette gauge action. The equation of state is calculated on $16^{3} \times 8$, $20^{3} \times 10$ and $24^{3} \times 12$ lattices with the anisotropy $ξ\equiv a_s / a_t = 2$, where $a_s$ and $a_t$ are the spatial and temporal lattice spacings. Unlike the case of the isotropic lattice on which $N_t=4$ data deviate significantly from the leading scaling behavior, the pressure and energy density on an anisotropic lattice are found to satisfy well the leading $1/N_t^2$ scaling from our coarsest lattice, $N_t/ξ=4$. With three data points at $N_t/ξ=4$, 5 and 6, we perform a well controlled continuum extrapolation of the equation of state. Our results in the continuum limit agree with a previous result from isotropic lattices using the same action, but have smaller and more reliable errors.
dc.descriptionRevTeX, 21 pages, 17 PS figures. A quantitative test about the benefit of anisotropic lattices added, minor errors corrected. Final version for PRD
dc.identifierhttps://arxiv.org/abs/hep-lat/0105012
dc.identifierhttp://arxiv.org/abs/hep-lat/0105012
dc.identifierPhys.Rev.D64:074507,2001
dc.identifierdoi:10.1103/PhysRevD.64.074507
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/178770
dc.subjectHigh Energy Physics - Lattice
dc.titleThermodynamics of SU(3) gauge theory on anisotropic lattices
dc.typetext

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