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Many-flavor phase diagram of the (2 + 1)d Gross-Neveu model at finite temperature

机译:(2 +1)d Gross-Neveu模型在有限温度下的多味相图

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We study the phase diagram of the Gross-Neveu model in d = 2 + 1 space-time dimensions in the plane spanned by temperature and the number of massless fermion flavors. We use a functional renormalization group approach based on a nonperturbative derivative expansion that accounts for fermionic as well as composite bosonic fluctuations. We map out the phase boundary separating the ordered massive low-temperature phase from the disordered high-temperature phase. The phases are separated by a second-order phase transition in the 2d Ising universality class. We determine the size of the Ginzburg region and show that it scales to zero for large Nf following a powerlaw, in agreement with large-Nf and lattice studies. We also study the regimes of local order above as well as the classical regime below the critical temperature. Our results could be of interest for the finite-temperature behavior of condensed-matter realizations of Dirac fermions, as e.g. electrons on the graphene honeycomb with a short-range interaction.
机译:我们研究了在d = 2 +1时空维度中,在温度和无质量费米子味剂跨越的平面中,Gross-Neveu模型的相图。我们使用基于非扰动导数展开的函数重整化组方法,该方法解决了铁离子以及复合玻色子涨落。我们绘制出将有序的大量低温相与无序高温相分离的相界。通过2d Ising通用性类别中的二阶相变将相分离。我们确定了金茨堡地区的大小,并表明与幂律和晶格研究一致,幂律遵循幂律将其缩放为零。我们还研究了高于临界温度的局部有序状态以及低于临界温度的经典状态。我们的结果可能对狄拉克费米子的凝聚态实现的有限温度行为感兴趣,例如石墨烯蜂窝上的电子具有短程相互作用。

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