传播自旋波中手性的形成

Cody Trevillian, Vasyl Tyberkevych
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引用次数: 0

摘要

我们开发了一种量化自旋波手性或缺乏奇偶对称性的通用方法,并将其应用于在斜磁化铁磁薄膜中传播的自旋波。理论论证和数值计算表明,随着自旋波波矢量的增加,最初的非手性自旋波通过 "奇偶性交换 "机制发展出手性特性,这尤其意味着手性自旋波成对出现。奇偶性交换机制最显著的例子是同时形成两种手性波:磁静表面波和最近发现的异对称自旋波,而这两种波之前被认为是相互独立的。奇偶性交换的另一种表现形式是在不对称自旋波分支的反交叉点附近形成强手性波。这些发现说明了设计具有规定手性谱的自旋波系统的可行途径,而这是以前从未考虑过的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。

Formation of chirality in propagating spin waves

Formation of chirality in propagating spin waves
A general approach to quantify chirality, or absence of parity symmetry, of spin waves has been developed and applied to spin waves propagating in obliquely magnetized ferromagnetic films. Using theoretical arguments and numerical calculations, it is shown that, upon increasing spin wave wavevector, initially achiral spin waves develop chiral properties through the “parity exchange” mechanism, which implies, in particular, that chiral spin waves appear in pairs. The most striking example of the parity exchange mechanism is the simultaneous formation of two chiral waves: the magnetostatic surface wave and the recently discovered heterosymmetric spin wave, which were previously considered independent of each other. Another manifestation of the parity exchange is the formation of strongly chiral waves near the anti-crossings of spin wave branches of unequal symmetry. These findings illustrate viable paths to engineering spin wave systems with prescribed chiral spectra that had not previously been considered.
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