We revisit the question of whether a two-dimensional topological insulatormay arise in a commensurate N\'eel antiferromagnet, where staggeredmagnetization breaks both the elementary translation and time reversal, butretains their product as a symmetry. In contrast to the so-called $Z_2$topological insulators, an exhaustive characterization of antiferromagnetictopological phases with the help of a topological invariant has been missing.We analyze a simple model of an antiferromagnetic topological insulator andchart its phase diagram based on a recently proposed criterion forcentrosymmetric systems [Fang et al., Phys. Rev. B 88, 085406 (2013)]. We thenadapt two methods, originally designed for paramagnetic systems, and makeantiferromagnetic topological phases manifest. The proposed methods apply farbeyond the particular example treated in this work, and admit straightforwardgeneralization. We illustrate this by considering a non-centrosymmetric system,where there are no simple criteria to identify topological phases. We alsopresent an explicit construction of edge states in an antiferromagnetictopological insulator.
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机译:我们重新讨论在相应的N'elel反铁磁体中是否可能出现二维拓扑绝缘体的问题,在该磁体中,交错磁化会破坏基本平移和时间反转,但会将它们的乘积保持对称。与所谓的$ Z_2 $拓扑绝缘子相反,缺少借助拓扑不变量的反铁磁拓扑相的详尽描述。中心对称系统[Fang et al。,Phys。 B 88,085406(2013)。然后,我们采用了两种方法,这些方法最初是为顺磁系统设计的,并且出现了顺磁和逆磁的拓扑相。所提出的方法的适用范围远远超出了本工作中要处理的特定示例,并且允许简单概括。我们通过考虑一个非中心对称的系统来说明这一点,在该系统中没有简单的标准来识别拓扑阶段。我们还提出了反铁磁拓扑绝缘体中边缘态的显式构造。
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