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{sub t}=2, 4, 6, and 8. For N{sub t}>4 the deconfinement transition line splits cleanly away from the bulk transition line. With increasing N{sub t} the thermal deconfinement transition lines shift to increasingly weaker coupling, joining onto the bulk transition line at increasingly larger {beta}{sub a} in a pattern consistent with the usual universality picture of lattice gauge theories. ((orig.)).
Blum, T;
[1]
DeTar, C;
[2]
Heller, U M;
[3]
Kaerkkaeinen, L;
[1]
Toussaint, D
[1]
- Arizona Univ., Tucson, AZ (United States). Dept. of Physics
- Department of Physics, University of Utah, Salt Lake City, UT 84112 (United States)
- SCRI, The Florida State University, Tallahassee, FL 32306-4052 (United States)
Citation Formats
Blum, T, DeTar, C, Heller, U M, Kaerkkaeinen, L, and Toussaint, D.
SU(3) lattice gauge theory with adjoint action at nonzero temperature.
Netherlands: N. p.,
1995.
Web.
doi:10.1016/0920-5632(95)00279-I.
Blum, T, DeTar, C, Heller, U M, Kaerkkaeinen, L, & Toussaint, D.
SU(3) lattice gauge theory with adjoint action at nonzero temperature.
Netherlands.
https://doi.org/10.1016/0920-5632(95)00279-I
Blum, T, DeTar, C, Heller, U M, Kaerkkaeinen, L, and Toussaint, D.
1995.
"SU(3) lattice gauge theory with adjoint action at nonzero temperature."
Netherlands.
https://doi.org/10.1016/0920-5632(95)00279-I.
@misc{etde_101161,
title = {SU(3) lattice gauge theory with adjoint action at nonzero temperature}
author = {Blum, T, DeTar, C, Heller, U M, Kaerkkaeinen, L, and Toussaint, D}
abstractNote = {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{sub t}=2, 4, 6, and 8. For N{sub t}>4 the deconfinement transition line splits cleanly away from the bulk transition line. With increasing N{sub t} the thermal deconfinement transition lines shift to increasingly weaker coupling, joining onto the bulk transition line at increasingly larger {beta}{sub a} in a pattern consistent with the usual universality picture of lattice gauge theories. ((orig.)).}
doi = {10.1016/0920-5632(95)00279-I}
journal = []
volume = {42}
journal type = {AC}
place = {Netherlands}
year = {1995}
month = {Apr}
}
title = {SU(3) lattice gauge theory with adjoint action at nonzero temperature}
author = {Blum, T, DeTar, C, Heller, U M, Kaerkkaeinen, L, and Toussaint, D}
abstractNote = {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{sub t}=2, 4, 6, and 8. For N{sub t}>4 the deconfinement transition line splits cleanly away from the bulk transition line. With increasing N{sub t} the thermal deconfinement transition lines shift to increasingly weaker coupling, joining onto the bulk transition line at increasingly larger {beta}{sub a} in a pattern consistent with the usual universality picture of lattice gauge theories. ((orig.)).}
doi = {10.1016/0920-5632(95)00279-I}
journal = []
volume = {42}
journal type = {AC}
place = {Netherlands}
year = {1995}
month = {Apr}
}