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Thermodynamics ofSU(3)gauge theory on anisotropic lattices
Author(s) -
Yusuke Namekawa,
S. Aoki,
R. Burkhalter,
Shinji Ejiri,
M. Fukugita,
S. Hashimoto,
N. Ishizuka,
Y. Iwasaki,
K. Kanaya,
T. Kaneko,
Y. Kuramashi,
V. Lesk,
M. Okamoto,
M. Okawa,
Y. Taniguchi,
A. Ukawa,
T. Yoshié
Publication year - 2001
Publication title -
physical review. d. particles, fields, gravitation, and cosmology/physical review. d. particles and fields
Language(s) - English
Resource type - Journals
eISSN - 1089-4918
pISSN - 0556-2821
DOI - 10.1103/physrevd.64.074507
Subject(s) - lattice (music) , isotropy , anisotropy , extrapolation , physics , scaling , equation of state , mathematical physics , lattice field theory , condensed matter physics , combinatorics , gauge theory , quantum mechanics , mathematical analysis , mathematics , geometry , acoustics
Finite temperature SU(3) gauge theory is studied on anisotropic latticesusing the standard plaquette gauge action. The equation of state is calculatedon $16^{3} \times 8$, $20^{3} \times 10$ and $24^{3} \times 12$ lattices withthe anisotropy $\xi \equiv a_s / a_t = 2$, where $a_s$ and $a_t$ are thespatial and temporal lattice spacings. Unlike the case of the isotropic latticeon which $N_t=4$ data deviate significantly from the leading scaling behavior,the pressure and energy density on an anisotropic lattice are found to satisfywell the leading $1/N_t^2$ scaling from our coarsest lattice, $N_t/\xi=4$. Withthree data points at $N_t/\xi=4$, 5 and 6, we perform a well controlledcontinuum extrapolation of the equation of state. Our results in the continuumlimit agree with a previous result from isotropic lattices using the sameaction, but have smaller and more reliable errors.Comment: RevTeX, 21 pages, 17 PS figures. A quantitative test about the benefit of anisotropic lattices added, minor errors corrected. Final version for PR

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