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Electrical detection of charge-current-induced spin polarization due to spin-momentum locking in Bi_2Se_3

机译:电检测Bi_2Se_3中自旋动量锁定导致的电荷电流诱导的自旋极化

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摘要

Topological insulators exhibit metallic surface states populated by massless Dirac fermions with spin-momentum locking, where the carrier spin lies in-plane, locked at right angles to the carrier momentum. Here, we show that a charge current produces a net spin polarization via spin-momentum locking in Bi_2Se_3 films, and this polarization is directly manifested as a voltage on a ferromagnetic contact. This voltage is proportional to the projection of the spin polarization onto the contact magnetization, is determined by the direction and magnitude of the charge current, scales inversely with Bi_2Se_3 film thickness, and its sign is that expected from spin-momentum locking rather than Rashba effects. Similar data are obtained for two different ferromagnetic contacts, demonstrating that these behaviours are independent of the details of the ferromagnetic contact. These results demonstrate direct electrical access to the topological insulators' surface-state spin system and enable utilization of its remarkable properties for future technological applications.
机译:拓扑绝缘体表现出金属表面状态,该表面状态由无质量的狄拉克费米子构成,具有自旋动量锁,载流子自旋位于平面内,与载流子动量成直角。在这里,我们表明电荷电流通过Bi_2Se_3薄膜中的自旋动量锁定产生净自旋极化,并且这种极化直接表现为铁磁触点上的电压。该电压与自旋极化在接触磁化强度上的投影成比例,由充电电流的方向和大小决定,与Bi_2Se_3膜厚度成反比,其符号是自旋动量锁定而非Rashba效应所预期的。对于两个不同的铁磁接触点,获得了相似的数据,表明这些行为与铁磁接触点的细节无关。这些结果表明,电气可以直接进入拓扑绝缘子的表面状态自旋系统,并且可以利用其卓越的性能来满足未来的技术应用。

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