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arXiv 1707.04098cond-mat.mes-hall
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两端和四端石墨烯纳米带中磁性吸附原子自旋极化输运的比较

Magnetic adatoms in two and four terminal graphene nanoribbons: A comparison between their spin polarized transport

Sudin Ganguly, Saurabh Basu

摘要:

我们研究了在两端和四端石墨烯纳米带(GNR)中随机分布磁性吸附原子的电荷和自旋输运。在没有Rashba自旋-轨道相互作用(SOI)的情况下,磁性吸附原子的加入仅通过交换偏置产生自旋极化电导的$z$分量,而在存在Rashba SOI的情况下,能够产生所有三个($x$、$y$和$z$)分量。这对可能的自旋电子学应用具有重要的影响。电荷电导在费米能为零附近表现出有趣的行为。在磁性吸附原子的存在下,熟悉的$2e^2/h$平台消失,从而将量子自旋霍尔绝缘相转变为普通绝缘体。局域电荷流和局域自旋流提供了系统电导特性的直观概念。我们发现,局域电荷电流与Rashba SOI无关,而局域自旋电流的三个分量对Rashba SOI敏感。此外,自旋极化电导的波动被发现是有用的量,因为它们显示出特定的趋势,即它们随着吸附原子密度的增加而增强。双端GNR器件似乎更适合于可能的自旋电子学应用。

英文摘要:

We study the charge and spin transport in two and four terminal graphene nanoribbons (GNR) decorated with random distribution of magnetic adatoms. The inclusion of the magnetic adatoms generates only the $z$-component of the spin polarized conductance via an exchange bias in the absence of Rashba spin-orbit interaction (SOI), while in presence of Rashba SOI, one is able to create all the three ($x$, $y$ and $z$) components. This has important consequences for possible spintronic applications. The charge conductance shows interesting behaviour near the zero of the Fermi energy. Where in presence of magnetic adatoms the familiar plateau at $2e^2/h$ vanishes, thereby transforming a quantum spin Hall insulating phase to an ordinary insulator. The local charge current and the local spin current provide an intuitive idea on the conductance features of the system. We found that, the local charge current is independent of Rashba SOI, while the three components of the local spin currents are sensitive to Rashba SOI. Moreover the fluctuations of the spin polarized conductance are found to be useful quantities as they show specific trends, that is, they enhance with increasing adatom densities. A two terminal GNR device seems to be better suited for possible spintronic applications.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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