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arXiv 2301.07754cond-mat.mes-hallcond-mat.other
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拓扑绝缘体表面上的带电磁振子

Charged magnons on the surface of a topological insulator

I. Martinez-Berumen, W. A. Coish, T. Pereg-Barnea

AI总结:

研究3D拓扑绝缘体表面二维Dirac电子与铁磁自旋阵列耦合系统,发现非局域磁振子可束缚能隙内电子态形成JRM激发,其与电子库耦合产生极化激元并引发量子相变。

摘要:

我们研究了一个二维 Dirac 电子系统(如在 3D 拓扑绝缘体表面实现的系统)与局域自旋阵列耦合的体系。这些自旋之间通过铁磁耦合相互连接,形成具有低能自旋波激发(magnons)的有序基态。Dirac 电子通过依赖于自旋的有效 Zeeman 场与自旋耦合。因此,面外有效 Zeeman 场充当 Dirac 质量,使电子能谱产生能隙。一旦某个自旋翻转,它会在其周围产生一个畴,在该畴内 Dirac 质量的符号与样品其余部分相反。因此,正如 Jackiw 和 Rebbi 所预言的,畴壁上会出现一个电子束缚态。然而,在量子磁体中,局域自旋翻转并不能产生本征态。相反,本征态对应于非局域化的自旋波(magnons)。与单个翻转自旋的情况类似,非局域化的 magnon 也会束缚一个能隙内的电子态。我们将这种激发命名为“Jackiw-Rebbi-Magnon”(JRM),并研究了它在动态自旋磁化率中的特征。当样品通过隧穿耦合到电子库时,在一个没有任何电子的系统中产生的 magnon 会与 JRM(束缚单个电子)杂化,产生 magnon-JRM 极化激元。对于这样的系统,我们识别出当 magnon-JRM 极化激元的能量低于完全极化的铁磁基态能量时,系统发生量子相变。

英文摘要:

We study a system of two-dimensional Dirac electrons (as is realized on the surface of a 3D topological insulator) coupled to an array of localized spins. The spins are coupled ferromagnetically to each other, forming an ordered ground state with low-energy spin-wave excitations (magnons). The Dirac electrons couple to the spins through a spin-dependent effective Zeeman field. The out-of-plane effective Zeeman field therefore serves as a Dirac mass that gaps the electronic spectrum. Once a spin is flipped, it creates a surrounding domain in which the sign of the Dirac mass is opposite to that of the rest of the sample. Therefore, an electronic bound state appears on the domain wall, as predicted by Jackiw and Rebbi. However, in a quantum magnet, a localized spin flip does not produce an eigenstate. Instead, the eigenstates correspond to delocalized spin waves (magnons). As in the case of the single flipped spin, the delocalized magnon also binds an in-gap electronic state. We name this excitation a `Jackiw-Rebbi-Magnon' (JRM) and study its signature in the dynamic spin susceptibility. When the sample is tunnel-coupled to an electronic reservoir, a magnon produced in a system without any electrons hybridizes with a JRM (which binds a single electron), producing magnon-JRM polaritons. For such a system, we identify a quantum phase transition when the magnon-JRM polariton energy falls below that of the fully polarized ferromagnetic ground state.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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