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Thermodynamics and heavy-quark free energies at finite temperature and density with two flavors of improved Wilson quarks

机译:有限温度和密度下的热力学和重夸克自由能,以及两种改进的威尔逊夸克口味

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摘要

Thermodynamics of two-flavor QCD at finite temperature and density is studied on a $16^3 \times 4$ lattice, using a renormalization group improved gauge action and the clover improved Wilson quark action. In the simulations along lines of constant $m_{\rm PS}/m_{\rm V}$, we calculate the Taylor expansion coefficients of the heavy-quark free energy with respect to the quark chemical potential ($\mu_q$) up to the second order. By comparing the expansion coefficients of the free energies between quark($Q$)and antiquark($\bar{Q}$), and between $Q$ and $Q$, we find a characteristic difference at finite $\mu_q$ due to the first order coefficient of the Taylor expansion. We also calculate the quark number and isospin susceptibilities, and find that the second order coefficient of the quark number susceptibility shows enhancement around the pseudo-critical temperature.
机译:使用重归一化组改进的规范作用和三叶草改进的Wilson夸克作用,在$ 16 ^ 3 \乘以4 $晶格上研究了两种风味QCD在有限温度和密度下的热力学。在沿着常数$ m _ {\ rm PS} / m _ {\ rm V} $的模拟中,我们计算了重夸克自由能相对于夸克化学势($ \ mu_q $)的泰勒膨胀系数到第二顺序。通过比较夸克($ Q $)和反夸克($ \ bar {Q} $)之间以及$ Q $和$ Q $之间的自由能的膨胀系数,我们发现在有限的$ \ mu_q $上存在特征差异到泰勒展开式的一阶系数。我们还计算了夸克数和同位旋磁化率,发现夸克数磁化率的二阶系数在伪临界温度附近显示出增强。

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