论文标题

三维基塔夫自旋液体的热力学分类

Thermodynamic classification of three-dimensional Kitaev spin liquids

论文作者

Eschmann, Tim, Mishchenko, Petr A., O'Brien, Kevin, Bojesen, Troels A., Kato, Yasuyuki, Hermanns, Maria, Motome, Yukitoshi, Trebst, Simon

论文摘要

在沮丧的磁性领域中,基塔耶夫模型提供了一个独特的框架,以研究自旋分数化的现象和两个空间维度的新兴晶格量表。他们的接地状态是量子旋转液体,通常可以用Majorana带结构和基础$ \ Mathbb {Z} _2 $量规结构进行描述。在这里,我们提供了基础三维Kitaev模型家族的“量规物理学”的全面分类,讨论了它们的热力学和基态秩序如何取决于基本的晶格几何形状。使用大型,无标志的量子蒙特卡洛模拟,我们表明,基本规格顺序通常可以从基本斑点的长度来理解 - 这一结果扩展了Lieb定理对晶状体几何形状的适用性,超出了其原始范围。在有限的温度下,(间隙)Vison激发的增殖会以临界温度尺度摧毁量规序,我们表明,这与三维Kitaev模型家族的Vison间隙的大小相关。我们还讨论了两个值得注意的例外,其中晶格结构引起了“尺寸挫败感”,或者与时间反向对称性破裂相结合。在更一般的情况下,此类3D Kitaev模型中的热力学量规转换是超出标准Landau-Ginzburg-Wilson范式以外的相变的最自然设置之一。

In the field of frustrated magnetism, Kitaev models provide a unique framework to study the phenomena of spin fractionalization and emergent lattice gauge theories in two and three spatial dimensions. Their ground states are quantum spin liquids, which can typically be described in terms of a Majorana band structure and an ordering of the underlying $\mathbb{Z}_2$ gauge structure. Here we provide a comprehensive classification of the "gauge physics" of a family of elementary three-dimensional Kitaev models, discussing how their thermodynamics and ground state order depends on the underlying lattice geometry. Using large-scale, sign-free quantum Monte Carlo simulations we show that the ground-state gauge order can generally be understood in terms of the length of elementary plaquettes -- a result which extends the applicability of Lieb's theorem to lattice geometries beyond its original scope. At finite temperatures, the proliferation of (gapped) vison excitations destroys the gauge order at a critical temperature scale, which we show to correlate with the size of vison gap for the family of three-dimensional Kitaev models. We also discuss two notable exceptions where the lattice structure gives rise to "gauge frustration" or intertwines the gauge ordering with time-reversal symmetry breaking. In a more general context, the thermodynamic gauge transitions in such 3D Kitaev models are one of the most natural settings for phase transitions beyond the standard Landau-Ginzburg-Wilson paradigm.

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