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Photoinduced pure spin-current injection in graphene with Rashba spin-orbit interaction

机译:具有Rashba自旋轨道相互作用的石墨烯中光诱导的纯自旋电流注入

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We propose a photoexcitation scheme for pure spin-current generation in graphene subject to a Rashba spin-orbit coupling. Although excitation using circularly polarized light does not result in optical orientation of spins in graphene unless an additional magnetic field is present, we show that excitation with linearly polarized light at normal incidence yields spin-current injection without magnetic field. Spins are polarized within the graphene plane and are displaced in opposite directions, with no net charge displacement. The direction of the spin current is determined by the linear polarization axis of the light, and the injection rate is proportional to the intensity. The technique is tunable via an applied bias voltage and is accessible over a wide frequency range. We predict a spin-current polarization as high as 75% for photon frequencies comparable to the Rashba frequency. Spin-current injection via optical methods removes the need for ferromagnetic contacts, which have been identified as a possible source of spin scattering in electrical spin injection in graphene.
机译:我们提出了一种受Rashba自旋-轨道耦合作用的石墨烯中纯自旋电流产生的光激发方案。尽管使用圆偏振光激发不会导致石墨烯中自旋的光学取向,除非存在额外的磁场,但我们显示,在垂直入射时使用线性偏振光激发会产生自旋电流注入而没有磁场。自旋在石墨烯平面内极化,并在相反方向上位移,没有净电荷位移。自旋电流的方向由光的线性偏振轴确定,注入速率与强度成正比。该技术可通过施加偏置电压进行调节,并且可以在很宽的频率范围内使用。我们预测,与Rashba频率相当的光子频率,自旋电流极化将高达75%。通过光学方法自旋电流注入消除了对铁磁接触的需求,铁磁接触已被确定为石墨烯电自旋注入中自旋散射的可能来源。

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