共振自旋轨道转矩系统中的水平吸引和异常点

I. Proskurin, R. Stamps
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引用次数: 2

摘要

水平吸引可以出现在驱动系统中,其中两个模式在由两个例外点分开的区域内合并而不是排斥。这种行为被提出于光力学和光磁系统中,并且最近在耗散腔磁非极化中被观察到。我们证明了在一个磁振子与电子库共振耦合的自旋轨道转矩系统中存在这样的状态。通过施加电场可以提供模吸引所必需的不稳定机制。磁场激发了自旋轨道分裂带间的带间跃迁,导致了磁振子的不稳定性。然后在振子能谱和不稳定区域出现两个异常点。我们讨论了可能发生这种情况的条件,并估计了具有Rashba耦合的自旋-轨道转矩振荡器到达吸引区所需的电场强度。提出了利用磁化率测量进行实验检测的建议。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Level attraction and exceptional points in a resonant spin-orbit torque system
Level attraction can appear in driven systems where instead of repulsion two modes coalesce in a region separated by two exceptional points. This behavior was proposed for optomechanical and optomagnonic systems, and recently observed for dissipative cavity magnon-polaritons. We demonstrate that such a regime exists in a spin-orbit torque system where a magnetic oscillator is resonantly coupled to an electron reservoir. An instability mechanism necessary for mode attraction can be provided by applying an electric field. The field excites interband transitions between spin-orbit split bands leading to an instability of the magnetic oscillator. Two exceptional points then appear in the oscillator energy spectrum and the region of instability. We discuss conditions under which this can occur and estimate the electric field strength necessary for reaching the attraction region for a spin-orbit torque oscillator with Rashba coupling. A proposal for experimental detection is made using magnetic susceptibility measurements.
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