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T. Blum, C. DeTar, S. Gottlieb, U.M. Heller, J.E. Hetrick, K. Rummukainen, R. L. Sugar, D. Toussaint, and M. Wingate, Phys. Rev. D 55, 1133 (1997). It may be possible to effectively eliminate flavor symmetry breaking in lattice simulations altogether.See T. Blum and A. Soni, Phys. Rev. D (to be published), and references therein.
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The energy density in the SU(3) pure gauge case is also substantial below (Formula presented) [F. Karsch (private communication)]
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The energy density in the SU(3) pure gauge case is also substantial below (Formula presented) [F. Karsch (private communication)].
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For the critical temperature of the SU(3) pure gauge transition see G. Boyd, J. Engels, F. Karsch, E. Laermann, C. Legeland, M. Lüetgemeier, and B. Petersson, Nucl. Phys. B469, 419 (1996).
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edited by R. Hwa (World Scientific, Singapore, 1995)
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85038306331
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Problems with O(4) scaling were reported by by A. Ukawa, in Lattice ’96 [3], Report No. hep-lat/9612011
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Problems with O(4) scaling were reported by by A. Ukawa, in Lattice ’96 [3], Report No. hep-lat/9612011;
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32
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33750193338
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We are currently carrying out simulations at (Formula presented) with (Formula presented) on lattices with spatial sizes (Formula presented), (Formula presented), and (Formula presented). Our preliminary results are consistent with the above
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G. Boyd reported similar findings by the Bielefeld group, “Two flavour QCD phase transition,” Report No. (unpublished).We are currently carrying out simulations at (Formula presented) with (Formula presented) on lattices with spatial sizes (Formula presented), (Formula presented), and (Formula presented). Our preliminary results are consistent with the above.
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Two flavour QCD phase transition
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