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Spin–orbit proximity effect in graphene

机译:石墨烯的自旋轨道邻近效应

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摘要

The development of spintronics devices relies on efficient generation of spin-polarized currents and their electric-field-controlled manipulation. While observation of exceptionally long spin relaxation lengths makes graphene an intriguing material for spintronics studies, electric field modulation of spin currents is almost impossible due to negligible intrinsic spin–orbit coupling of graphene. In this work, we create an artificial interface between monolayer graphene and few-layer semiconducting tungsten disulphide . In these devices, we observe that graphene acquires spin–orbit coupling up to 17?meV, three orders of magnitude higher than its intrinsic value, without modifying the structure of the graphene. The proximity spin–orbit coupling leads to the spin Hall effect even at room temperature, and opens the door to spin field effect transistors. We show that intrinsic defects in tungsten disulphide play an important role in this proximity effect and that graphene can act as a probe to detect defects in semiconducting surfaces.
机译:自旋电子器件的发展依赖于自旋极化电流的有效产生及其电场控制的操纵方式。尽管观察到异常长的自旋弛豫长度使石墨烯成为自旋电子学研究的有趣材料,但由于石墨烯的固有自旋-轨道耦合可忽略不计,自旋电流的电场调制几乎是不可能的。在这项工作中,我们在单层石墨烯和几层半导体二硫化钨之间创建了一个人工界面。在这些器件中,我们观察到石墨烯获得高达17?meV的自旋-轨道耦合,比其固有值高三个数量级,而没有改变石墨烯的结构。即使在室温下,邻近自旋轨道耦合也会导致自旋霍尔效应,并为自旋场效应晶体管打开了大门。我们表明,二硫化钨中的固有缺陷在这种邻近效应中起着重要作用,并且石墨烯可以充当探针来检测半导体表面中的缺陷。

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