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通过磁性掺杂拓扑绝缘体异质结构中的巨自旋轨道扭矩实现磁化翻转。

Magnetization switching through giant spin-orbit torque in a magnetically doped topological insulator heterostructure.

机构信息

1] Department of Electrical Engineering, University of California, Los Angeles, California 90095, USA [2].

Department of Electrical Engineering, University of California, Los Angeles, California 90095, USA.

出版信息

Nat Mater. 2014 Jul;13(7):699-704. doi: 10.1038/nmat3973. Epub 2014 Apr 28.

DOI:10.1038/nmat3973
PMID:24776536
Abstract

Recent demonstrations of magnetization switching induced by in-plane current in heavy metal/ferromagnetic heterostructures (HMFHs) have drawn great attention to spin torques arising from large spin-orbit coupling (SOC). Given the intrinsic strong SOC, topological insulators (TIs) are expected to be promising candidates for exploring spin-orbit torque (SOT)-related physics. Here we demonstrate experimentally the magnetization switching through giant SOT induced by an in-plane current in a chromium-doped TI bilayer heterostructure. The critical current density required for switching is below 8.9 × 10(4) A cm(-2) at 1.9 K. Moreover, the SOT is calibrated by measuring the effective spin-orbit field using second-harmonic methods. The effective field to current ratio and the spin-Hall angle tangent are almost three orders of magnitude larger than those reported for HMFHs. The giant SOT and efficient current-induced magnetization switching exhibited by the bilayer heterostructure may lead to innovative spintronics applications such as ultralow power dissipation memory and logic devices.

摘要

最近在重金属/铁磁异质结构(HMFHs)中展示的平面电流诱导磁化翻转引起了人们对大自旋轨道耦合(SOC)产生的自旋扭矩的极大关注。鉴于固有强 SOC,拓扑绝缘体(TIs)有望成为探索自旋轨道扭矩(SOT)相关物理的有前途的候选者。在这里,我们通过在掺杂铬的 TI 双层异质结构中平面电流诱导的巨大 SOT 实验证明了磁化切换。在 1.9 K 下,切换所需的临界电流密度低于 8.9×10(4) A cm(-2)。此外,通过使用二次谐波方法测量有效自旋轨道场来校准 SOT。有效场与电流比和自旋霍尔角正切值几乎比 HMFHs 报道的大三个数量级。双层异质结构表现出的巨大 SOT 和高效电流诱导的磁化翻转可能会导致创新的自旋电子学应用,例如超低功耗存储和逻辑器件。

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