凝聚态物理
磁化
物理
对称性破坏
磁各向异性
自旋极化
对称(几何)
磁场
量子力学
几何学
数学
电子
作者
Hao Wu,John Nance,Seyed Armin Razavi,David Lujan,Bingqian Dai,Yuxiang Liu,Haoran He,Baoshan Cui,Di Wu,Kin Wong,Kemal Sobotkiewich,Xiaoqin Li,Gregory P. Carman,Kang L. Wang
出处
期刊:Nano Letters
[American Chemical Society]
日期:2020-12-18
卷期号:21 (1): 515-521
被引量:103
标识
DOI:10.1021/acs.nanolett.0c03972
摘要
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 (z) gradient of magnetic properties as a practical solution for the wafer-scale manufacture of SOT devices.
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