Jiang Jingwei, Louie Steven G
Department of Physics, University of California, Berkeley, California 94720, United States.
Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, United States.
Nano Lett. 2021 Jan 13;21(1):197-202. doi: 10.1021/acs.nanolett.0c03503. Epub 2020 Dec 15.
We apply the topological classification theory using chiral symmetry to graphene nanoribbons (GNRs). This approach eliminates the requirement of time-reversal and spatial symmetry in previous topology theory, resulting in a classification with the conventional index in a new vector-formed expression called "chiral phase index" (CPI). Our approach is applicable to GNRs of arbitrary terminations and any quasi one-dimensional chiral structures, including magnetism. It naturally solves a recent experimental puzzle of junction states at a class of asymmetric GNR junctions. We moreover derive a simple analytic formula for the CPI of armchair GNRs. Since this approach enables access to electron spin behavior, based on the CPI, we design a novel GNR with periodic localized moments and strong spin-spin exchange coupling.
我们将利用手性对称性的拓扑分类理论应用于石墨烯纳米带(GNRs)。这种方法消除了先前拓扑理论中对时间反演和空间对称性的要求,从而在一种称为“手性相位指数”(CPI)的新向量形式表达式中,用传统指数进行分类。我们的方法适用于任意终端的GNRs以及任何准一维手性结构,包括磁性结构。它自然地解决了最近一类不对称GNR结处的结态实验难题。此外,我们推导了扶手椅型GNRs的CPI的简单解析公式。由于这种方法能够研究电子自旋行为,基于CPI,我们设计了一种具有周期性局域磁矩和强自旋 - 自旋交换耦合的新型GNR。