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Gate-dependent spin Hall induced nonlocal resistance and the symmetry of spin-orbit scattering in Au-clustered graphene

机译:与门相关的自旋霍尔效应引起的非团簇电阻和金簇石墨烯中自旋轨道散射的对称性

摘要

Engineering the electron dispersion of graphene to be spin-dependent is crucial for the realization of spin-based logic devices. Enhancing spin-orbit coupling in graphene can induce spin Hall effect, which can be adapted to generate or detect a spin current without a ferromagnet. Recently, both chemically and physically decorated graphenes have shown to exhibit large nonlocal resistance via the spin Hall and its inverse effects. However, these nonlocal transport results have raised critical debates due to the absence of field dependent Hanle curve in subsequent studies. Here, we introduce Au clusters on graphene to enhance spin-orbit coupling and employ a nonlocal geometry to study the spin Hall induced nonlocal resistance. Our results show that the nonlocal resistance highly depends on the applied gate voltage due to various current channels. However, the spin Hall induced nonlocal resistance becomes dominant at a particular carrier concentration, which is further confirmed through Hanle curves. The obtained spin Hall angle is as high as ∼0.09 at 2 K. Temperature dependence of spin relaxation time is governed by the symmetry of spin-orbit coupling, which also depends on the gate voltage: asymmetric near the charge neutral point and symmetric at high carrier concentration. These results inspire an effective method for generating spin currents in graphene and provide important insights for the spin Hall effect as well as the symmetry of spin scattering in physically decorated graphene.
机译:将石墨烯的电子色散设计为自旋相关性对于实现基于自旋的逻辑器件至关重要。增强石墨烯中的自旋-轨道耦合可引起自旋霍尔效应,该效应可适于在没有铁磁体的情况下产生或检测自旋电流。最近,化学和物理修饰的石墨烯都表现出通过自旋霍尔及其逆效应表现出较大的非局部电阻。然而,由于在随后的研究中缺乏依赖于场的Hanle曲线,因此这些非局部迁移的结果引起了激烈的争论。在这里,我们在石墨烯上引入金簇以增强自旋轨道耦合,并采用非局部几何学研究自旋霍尔效应引起的非局部电阻。我们的结果表明,由于各种电流通道,非局部电阻在很大程度上取决于施加的栅极电压。然而,自旋霍尔感应的非局部电阻在特定载流子浓度下变得占主导地位,这通过Hanle曲线进一步证实。在2 K下获得的自旋霍尔角高达〜0.09。自旋弛豫时间的温度依赖性由自旋轨道耦合的对称性决定,自旋轨道耦合的对称性还取决于栅极电压:电荷中性点附近不对称,高电荷点附近对称。载流子浓度。这些结果激发了一种在石墨烯中产生自旋电流的有效方法,并为自旋霍尔效应以及物理修饰的石墨烯中自旋散射的对称性提供了重要见解。

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