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arXiv 2410.09354cond-mat.mes-hall
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反铁磁链的拓扑磁子性质

Topological magnonic properties of an antiferromagnetic chain

Topojit Debnath, Shri Hari Soundararaj, Sohee Kwon, Alexander A. Balandin, Roger K. Lake

AI总结:

本文研究了二聚化一维反铁磁链的磁子激发,发现其平庸或拓扑性质取决于交替交换耦合和各向异性的符号与大小,且该拓扑相与SSH模型不同,并基于DFT参数分析了准一维材料MoI$_3$的磁基态与激发。

摘要:

二聚化一维反铁磁链的磁子激发可以是平庸的或拓扑的,这取决于交替交换耦合和各向异性的符号与大小。当两种不同交换耦合的符号交替时出现的拓扑相,在性质上不同于 Su-Schrieffer-Heeger 模型。可能展现这些性质的材料是准一维材料 MoI$_3$,它由与相邻链弱耦合的二聚化链组成。利用从密度泛函理论计算中提取的交换和各向异性参数,对磁基态及其激发进行了分析和数值分析。

英文摘要:

The magnonic excitations of a dimerized, one-dimensional, antiferromagnetic chain can be trivial or topological depending on the signs and magnitudes of the alternating exchange couplings and the anisotropy. The topological phase that occurs when the signs of the two different exchange couplings alternate is qualitatively different from that of the Su-Schrieffer-Heeger model. A material that may exhibit these properties is the quasi-one-dimensional material MoI$_3$ that consists of dimerized chains weakly coupled to adjacent chains. The magnetic ground state and its excitations are analyzed both analytically and numerically using exchange and anisotropy parameters extracted from density functional theory calculations.

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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