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具有自旋轨道耦合的石墨烯锯齿形纳米带中的双极自旋过滤效应。

A bipolar spin-filtering effect in graphene zigzag nanoribbons with spin-orbit coupling.

机构信息

Department of Physics and Materials Science, City University of Hong Kong, Kowloon, Hong Kong, People's Republic of China.

出版信息

Nanotechnology. 2012 Mar 9;23(9):095201. doi: 10.1088/0957-4484/23/9/095201. Epub 2012 Feb 10.

Abstract

We predict a large spin-filtering effect in graphene zigzag nanoribbons in the presence of Rashba spin-orbit coupling. The spin polarization of the transmitted current reaches a maximum when the incoming electrons occupy only one subband and the outgoing electrons occupy two subbands (spin is not taken into account). This situation can be reached by applying a potential barrier or a width constriction to the incoming lead of the ribbon. A simple physical picture is provided to explain the spin-filtering effect. Because of the electron-hole symmetry and the time-reversal symmetry, the spin-filtering is antisymmetric for the hole when compared with that for the electron. So the bipolar spin-polarized current can be generated by tuning the Fermi energy across the Dirac point. Besides, the wedge-shaped constriction can modify the conductance spin polarization.

摘要

我们预测在存在拉什巴自旋轨道耦合的情况下,石墨烯锯齿形纳米带会产生很大的自旋过滤效应。当入射电子只占据一个子带而出射电子占据两个子带时(不考虑自旋),透射电流的自旋极化达到最大值。这种情况可以通过在 ribbon 的入射引线施加势垒或宽度限制来实现。我们提供了一个简单的物理图像来解释自旋过滤效应。由于电子-空穴对称性和时间反演对称性,与电子相比,空穴的自旋过滤是反称的。因此,通过调节费米能越过狄拉克点,可以产生双极自旋极化电流。此外,楔形限制可以改变电导自旋极化。

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