@article{5e1bb7c4935c409aa39b3f402b6e4a49,
title = "Thermodynamics of lattice QCD with 2 light dynamical (staggered) quark flavours on a 163 × 8 lattice",
abstract = "Lattice QCD with 2 light staggered quark flavours is being simulated on a 163 × 8 lattice to study the transition from hadronic matter to a quark gluon plasma. We have completed runs at mq = 0.0125 and are extending this to mq = 0.00625. We also examine the addition of a non-dynamical {"}strange{"} quark. Thermodynamic order parameters are being measured across the transition and further into the plasma phase, as are various screening lengths. No evidence for a first order transition is seen, and we estimate the transition temperature to be Tc = 143(7)MeV.",
author = "Steven Gottlieb and Heller, \{U. M.\} and Kennedy, \{A. D.\} and Kogut, \{J. B.\} and A. Krasnitz and W. Liu and Renken, \{R. L.\} and Sinclair, \{D. K.\} and Sugar, \{R. L.\} and D. Toussaint and Wang, \{K. C.\}",
note = "Funding Information: close to \textbackslash{}/8-ir/Nt. This suggests that these states are collections of unbound quarks of the lowest allowed Matsubara frequency (7r/Nt), while the (7r,Q) multiplet remains bound [9] . Hadronic wave function measurements by the MILC collaboration [7] and the area law we observe for spatial Wilson line correlations cast doubt on this simple picture . Finally, we have measured the topological susceptibility by the cooling method, [10] and find good agreement with the anomalous Ward identity [11] . We thank the Pittsburgh Supercomputer Center for access to their CM-2 on which these simulations were performed . This research was supported by DOE contracts W-31-109-ENG-38, DE-{\'A}C02-84ER 40125, DE-FC05-85ER250000, DE-FG02-85ER40213, and NSF contracts NSF-PHY87-01775, NSF-PHY86-14185 .",
year = "1992",
doi = "10.1016/0920-5632(92)90261-P",
language = "English (US)",
volume = "26",
pages = "308--310",
journal = "Nuclear Physics B (Proceedings Supplements)",
issn = "0920-5632",
publisher = "Elsevier",
number = "C",
}