SU(3) lattice gauge theory with adjoint action at nonzero temperature

T. Blum; Carleton DeTar; Urs M. Heller; Leo Kärkkäinen; D. Toussaint

doi:10.1016/0920-5632(95)00279-I

SU(3) lattice gauge theory with adjoint action at nonzero temperature

T. Blum, Carleton DeTar, Urs M. Heller, Leo Kärkkäinen, D. Toussaint

Research output: Contribution to journal › Article › peer-review

5 Scopus citations

Abstract

We study the thermal phase diagram of pure SU(3) gauge theory with fundamental and adjoint couplings. We improve previous estimates of the position of the bulk transition line and determine the thermal deconfinement transition lines for N_t = 2, 4, 6, and 8. For N_t > 4 the deconfinement transition line splits cleanly away from the bulk transition line. With increasing N_t the thermal deconfinement transition lines shift to increasingly weaker coupling, joining onto the bulk transition line at increasingly larger β_a in a pattern consistent with the usual universality picture of lattice gauge theories.

Original language	English (US)
Pages (from-to)	457-459
Number of pages	3
Journal	Nuclear Physics B (Proceedings Supplements)
Volume	42
Issue number	1-3
DOIs	https://doi.org/10.1016/0920-5632(95)00279-I
State	Published - Apr 1995
Externally published	Yes

ASJC Scopus subject areas

Atomic and Molecular Physics, and Optics
Nuclear and High Energy Physics

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10.1016/0920-5632(95)00279-I

Cite this

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title = "SU(3) lattice gauge theory with adjoint action at nonzero temperature",

abstract = "We study the thermal phase diagram of pure SU(3) gauge theory with fundamental and adjoint couplings. We improve previous estimates of the position of the bulk transition line and determine the thermal deconfinement transition lines for Nt = 2, 4, 6, and 8. For Nt > 4 the deconfinement transition line splits cleanly away from the bulk transition line. With increasing Nt the thermal deconfinement transition lines shift to increasingly weaker coupling, joining onto the bulk transition line at increasingly larger βa in a pattern consistent with the usual universality picture of lattice gauge theories.",

author = "T. Blum and Carleton DeTar and Heller, {Urs M.} and Leo K{\"a}rkk{\"a}inen and D. Toussaint",

note = "Funding Information: This work was partly supported by the DOE under grants No. DE-FG02-8SER40213, # DE-FG05-85ER250000 and # DE-FG05-92ER40742 and the U.S. National Science Foundation under grant. PHY9309458. Computations were supported by SCRI, PSC and the Cornell Theory Center.",

year = "1995",

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doi = "10.1016/0920-5632(95)00279-I",

language = "English (US)",

volume = "42",

pages = "457--459",

journal = "Nuclear Physics B (Proceedings Supplements)",

issn = "0920-5632",

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T1 - SU(3) lattice gauge theory with adjoint action at nonzero temperature

AU - Blum, T.

AU - DeTar, Carleton

AU - Heller, Urs M.

AU - Kärkkäinen, Leo

AU - Toussaint, D.

N1 - Funding Information: This work was partly supported by the DOE under grants No. DE-FG02-8SER40213, # DE-FG05-85ER250000 and # DE-FG05-92ER40742 and the U.S. National Science Foundation under grant. PHY9309458. Computations were supported by SCRI, PSC and the Cornell Theory Center.

PY - 1995/4

Y1 - 1995/4

N2 - We study the thermal phase diagram of pure SU(3) gauge theory with fundamental and adjoint couplings. We improve previous estimates of the position of the bulk transition line and determine the thermal deconfinement transition lines for Nt = 2, 4, 6, and 8. For Nt > 4 the deconfinement transition line splits cleanly away from the bulk transition line. With increasing Nt the thermal deconfinement transition lines shift to increasingly weaker coupling, joining onto the bulk transition line at increasingly larger βa in a pattern consistent with the usual universality picture of lattice gauge theories.

AB - We study the thermal phase diagram of pure SU(3) gauge theory with fundamental and adjoint couplings. We improve previous estimates of the position of the bulk transition line and determine the thermal deconfinement transition lines for Nt = 2, 4, 6, and 8. For Nt > 4 the deconfinement transition line splits cleanly away from the bulk transition line. With increasing Nt the thermal deconfinement transition lines shift to increasingly weaker coupling, joining onto the bulk transition line at increasingly larger βa in a pattern consistent with the usual universality picture of lattice gauge theories.

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JO - Nuclear Physics B (Proceedings Supplements)

JF - Nuclear Physics B (Proceedings Supplements)

IS - 1-3

ER -

SU(3) lattice gauge theory with adjoint action at nonzero temperature

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