TY - JOUR
T1 - What is going on with Wilson quarks at high temperature?
AU - Bernard, Claude
AU - DeGrand, Tom
AU - DeTar, Carleton
AU - Gottlieb, Steven
AU - Hasenfratz, Anna
AU - Kärkkäinen, Leo
AU - Sugar, Bob
AU - Toussaint, Doug
N1 - Funding Information:
Calculations were carried out on Paragons, 1 iPSC/860's, CM-5's and workstations at PSC, NCSA, SDSC, ORNL and our universities. We thank Akira Ukawa and Frithjof Karsch for help-ful discussions. We thank the Institute for Nu-clear Theory, the Institute for Theoretical Physics and the UCSB Physics department, where parts of this work were done. This research was sup-ported by the United States NSF and DOE.
PY - 1994/4
Y1 - 1994/4
N2 - We present results of a series of simulations of high temperature QCD with two flovors of Wilson quarks, using four and six time slices. With four time sslices the thermal crossover or transition gets steeper with increasing κ until about κ≈0.19, and then becomes less steep as κ increases further. Several observables are studied in detail to explore the nature of the high temperature phase. With six time slices we find strong metastability with hot and cold starts at κ=0.17, 0.18 and 0.19. At κ=0.17 and 0.18 the plaquette, ψψ and the Polyakov loop all have very different values with the hot and cold starts, while at κ=0.19 the plaquette and ψψ have different values but the Polyakov loop is small for both hot and cold starts.
AB - We present results of a series of simulations of high temperature QCD with two flovors of Wilson quarks, using four and six time slices. With four time sslices the thermal crossover or transition gets steeper with increasing κ until about κ≈0.19, and then becomes less steep as κ increases further. Several observables are studied in detail to explore the nature of the high temperature phase. With six time slices we find strong metastability with hot and cold starts at κ=0.17, 0.18 and 0.19. At κ=0.17 and 0.18 the plaquette, ψψ and the Polyakov loop all have very different values with the hot and cold starts, while at κ=0.19 the plaquette and ψψ have different values but the Polyakov loop is small for both hot and cold starts.
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U2 - 10.1016/0920-5632(94)90380-8
DO - 10.1016/0920-5632(94)90380-8
M3 - Article
AN - SCOPUS:4244100527
SN - 0920-5632
VL - 34
SP - 324
EP - 327
JO - Nuclear Physics B (Proceedings Supplements)
JF - Nuclear Physics B (Proceedings Supplements)
IS - C
ER -