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拓扑表面态在锑超薄膜中的演化。

Evolution of topological surface states in antimony ultra-thin films.

机构信息

Department of Physics, National University of Singapore, Singapore.

出版信息

Sci Rep. 2013;3:2010. doi: 10.1038/srep02010.

Abstract

Based on an inverted bulk band order, antimony thin films presumably could become topological insulators if quantum confinement effect opens up a gap in the bulk bands. Coupling between topological surface states (TSS) from opposite surfaces, however, tends to degrade or even destroy their novel characters. Here the evolution and coupling of TSS on Sb(111) thin films from 30 bilayers down to 4 bilayers was investigated using in-situ Fourier-transform scanning tunneling spectroscopy and density functional theory computations. On a 30-bilayer sample, quasi-particle interference patterns are generated by the scattering of TSS from the top surface only. As the thickness decreases, inter-surface coupling degrades spin polarisation of TSS and opens up new wavevector-dependent scattering channels, resulting in spin degenerate states in most part of the surface Brillouin zone, whereas the TSS near the zone centre exhibit little inter-surface coupling, so they remain spin-polarised without opening a gap at the Dirac point.

摘要

基于反型体带序,如果量子限制效应在体带中打开一个能隙,那么锑薄膜有望成为拓扑绝缘体。然而,来自相反表面的拓扑表面态(TSS)之间的耦合往往会降低甚至破坏它们的新奇特性。在这里,使用原位傅里叶变换扫描隧道光谱和密度泛函理论计算研究了 Sb(111)薄膜从 30 层减少到 4 层时 TSS 的演化和耦合。在 30 层的样品中,准粒子干涉图案是由来自顶层的 TSS 散射产生的。随着厚度的减小,界面间的耦合降低了 TSS 的自旋极化,并打开了新的与波矢相关的散射通道,导致在表面布里渊区的大部分区域中出现自旋简并态,而在区中心附近的 TSS 几乎没有界面间的耦合,因此它们保持自旋极化,而在狄拉克点处没有打开能隙。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/221d/3684810/0948f9fc8b53/srep02010-f1.jpg

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