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The phase transition to the quark-gluon plasma from lattice QCD

机译:从晶格QCD到夸克胶子等离子体的相变

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摘要

In the first period after the start of finite temperature studies for QCD on the lattice, in 1981, essentially pure SU(2) and SU(3) gauge theory results and a few quenched (i.e., without dynamical quarks) full QCD results were available, all on small lattices. Since then large lattices have come into use for pure SU(2) and SU(3) investigations. On medium size lattices full QCD simulations incorporating dynamical quarks of 0.5 up to 12 flavours and for many differnet quark mass values have been performed. Thsi survey does not cover all of the existing papers on the subject. So we shall omit any details of fermion updates, do not discuss Wilson fermions and other topics, which might be of interest. Also, the attempts made so far to include non-zero chemical potential will not be reviewed, because up to now no realistic (not strong coupling) calculations exist. For more information we suggest to read the conference reviews of fall 1988 by A. Ukawa~1, M.Fukugita~2 and F.Karsch~3. There are some promising new developments since the Lattice 88 and Quark Matter 88 conferences on which we shall report: - the order of the finite temperature transition in models related to the pure SU(3) gauge theory; - first results for full QCD on lattices with large time extend (N_r=8); - the solution of the continuum and lattice perturbation theory discrepancy for the full QCD energy density.
机译:在开始对格架上的QCD进行有限温度研究之后的第一阶段,1981年,获得了基本纯的SU(2)和SU(3)规范理论结果以及一些淬火(即,没有动态夸克)的完全QCD结果,全部放在小格子上。从那时起,大型晶格已用于纯SU(2)和SU(3)研究。在中等大小的晶格上,已经进行了完整的QCD模拟,该模拟结合了0.5到12种风味的动态夸克,并针对许多不同的净夸克质量值进行了模拟。该调查并未涵盖有关该主题的所有现有论文。因此,我们将省略有关费米子更新的任何详细信息,不要讨论可能引起人们兴趣的威尔逊费米子和其他主题。另外,由于迄今为止还不存在任何实际(不强耦合)的计算,因此将不复述迄今为止尝试包括非零化学势的尝试。有关更多信息,我们建议阅读A. Ukawa〜1,M.Fukugita〜2和F.Karsch〜3于1988年秋季发表的会议回顾。自从Lattice 88和Quark Matter 88会议以来,我们将报告一些有希望的新进展:-与纯SU(3)规范理论相关的模型中有限温度转变的顺序; -具有较大时间扩展的点阵上的完整QCD的第一个结果(N_r = 8); -完整QCD能量密度的连续体和晶格摄动理论差异的解。

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