Flux crystals, Majorana metals, and flat bands in exactly solvable spin-orbital liquids

Sreejith Chulliparambil, L. Janssen, M. Vojta, Hong-Hao Tu, Urban F. P. Seifert
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引用次数: 10

Abstract

Spin-orbital liquids are quantum disordered states in systems with entangled spin and orbital degrees of freedom. We study exactly solvable spin-orbital models in two dimensions with selected Heisenberg-, Kitaev-, and $\Gamma$-type interactions, as well as external magnetic fields. These models realize a variety of spin-orbital-liquid phases featuring dispersing Majorana fermions with Fermi surfaces, nodal Dirac or quadratic band touching points, or full gaps. In particular, we show that Zeeman magnetic fields can stabilize nontrivial flux patterns and induce metamagnetic transitions between states with different topological character. Solvable nearest-neighbor biquadratic spin-orbital perturbations can be tuned to stabilize zero-energy flat bands. We discuss in detail the examples of $\mathrm{SO}(2)$- and $\mathrm{SO}(3)$-symmetric spin-orbital models on the square and honeycomb lattices, and use group-theoretical arguments to generalize to $\mathrm{SO}(\nu)$-symmetric models with arbitrary integer $\nu > 1$. These results extend the list of exactly solvable models with spin-orbital-liquid ground states and highlight the intriguing general features of such exotic phases. Our models are thus excellent starting points for more realistic modellings of candidate materials.
通量晶体,马约拉纳金属,以及精确可溶自旋轨道液体中的平带
自旋轨道液体是具有纠缠自旋和轨道自由度系统中的量子无序态。我们研究了精确可解的自旋轨道模型在二维选择海森堡-,基塔耶夫-和$\Gamma$型相互作用,以及外部磁场。这些模型实现了各种自旋轨道液相,其特征是具有费米面、节点狄拉克或二次带接触点或全间隙的分散马约拉纳费米子。特别地,我们证明了塞曼磁场可以稳定非平凡的磁流模式,并诱导具有不同拓扑特征的状态之间的超磁跃迁。可解的最近邻双二次自旋轨道微扰可以调谐以稳定零能量平带。我们详细讨论了正方形和蜂窝格上的$\mathrm{SO}(2)$和$\mathrm{SO}(3)$对称自旋轨道模型的例子,并利用群论论证推广到具有任意整数$\nu > 1$的$\mathrm{SO}(\nu)$对称模型。这些结果扩展了具有自旋轨道-液体基态的精确可解模型的列表,并突出了这些奇异相的有趣的一般特征。因此,我们的模型是候选材料更现实建模的极好起点。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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