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通过自旋轨道扭矩实现垂直磁化的确定性切换的手征对称性破缺

Chiral Symmetry Breaking for Deterministic Switching of Perpendicular Magnetization by Spin-Orbit Torque.

作者信息

Wu Hao, Nance John, Razavi Seyed Armin, Lujan David, Dai Bingqian, Liu Yuxiang, He Haoran, Cui Baoshan, Wu Di, Wong Kin, Sobotkiewich Kemal, Li Xiaoqin, Carman Gregory P, Wang Kang L

机构信息

Department of Electrical and Computer Engineering, and Department of Physics and Astronomy, University of California, Los Angeles, California 90095, United States.

Department of Mechanical and Aerospace Engineering, University of California, Los Angeles, California 90095, United States.

出版信息

Nano Lett. 2021 Jan 13;21(1):515-521. doi: 10.1021/acs.nanolett.0c03972. Epub 2020 Dec 18.

Abstract

Symmetry breaking is a characteristic to determine which branch of a bifurcation system follows upon crossing a critical point. Specifically, in spin-orbit torque (SOT) devices, a fundamental question arises: how can the symmetry of the perpendicular magnetic moment be broken by the in-plane spin polarization? Here, we show that the chiral symmetry breaking by the antisymmetric Dzyaloshinskii-Moriya interaction (DMI) can induce the deterministic SOT switching of the perpendicular magnetization. By introducing a gradient of saturation magnetization or magnetic anisotropy, the dynamic noncollinear spin textures are formed under the current-driven SOT, and thus, the chiral symmetry of these dynamic spin textures is broken by the DMI, resulting in the deterministic magnetization switching. We introduce a strategy to induce an out-of-plane () gradient of magnetic properties as a practical solution for the wafer-scale manufacture of SOT devices.

摘要

对称性破缺是确定分叉系统在越过临界点后遵循哪个分支的一个特征。具体而言,在自旋轨道矩(SOT)器件中,出现了一个基本问题:面内自旋极化如何打破垂直磁矩的对称性?在此,我们表明,由反对称的Dzyaloshinskii-Moriya相互作用(DMI)引起的手性对称性破缺可诱导垂直磁化的确定性SOT切换。通过引入饱和磁化强度或磁各向异性的梯度,在电流驱动的SOT下形成动态非共线自旋纹理,因此,这些动态自旋纹理的手性对称性被DMI打破,从而导致确定性的磁化切换。我们引入一种策略来诱导磁特性的面外()梯度,作为SOT器件晶圆级制造的一种实际解决方案。

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