Hybridization gap approaching the two-dimensional limit of topological insulator Bi$_x$Sb$_{1-x}$

Paul Corbae, Aaron N. Engel, Jason T. Dong, Wilson J. Yánez-Parreño, Donghui Lu, Makoto Hashimoto, Alexei Fedorov, Christopher J. Palmstrøm
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Abstract

Bismuth antimony alloys (Bi$_x$Sb$_{1-x}$) provide a tuneable materials platform to study topological transport and spin-polarized surface states resulting from the nontrivial bulk electronic structure. In the two-dimensional limit, it is a suitable system to study the quantum spin Hall effect. In this work we grow epitaxial, single orientation thin films of Bi$_x$Sb$_{1-x}$ on an InSb(111)B substrate down to two bilayers where hybridization effects should gap out the topological surface states. Supported by a tight-binding model, spin- and angle-resolved photoemission spectroscopy data shows pockets at the Fermi level from the topological surface states disappear as the bulk gap increases from confinement. Evidence for a gap opening in the topological surface states is shown in the ultrathin limit. Finally, we observe spin-polarization approaching unity from the topological surface states in 10 bilayer films. The growth and characterization of ultrathin Bi$_x$Sb$_{1-x}$ alloys suggest ultrathin films of this material system can be used to study two-dimensional topological physics as well as applications such as topological devices, low power electronics, and spintronics.
拓扑绝缘体 Bi$_x$Sb$_{1-x}$ 接近二维极限的杂化间隙
铋锑合金(Bi$_x$Sb$_{1-x}$)提供了一个可调整的材料平台,用于研究由非难体电子结构引起的拓扑输运和自旋极化表面态。在二维极限下,它是研究量子自旋霍尔效应的合适体系。在这项研究中,我们在 InSb(111)B 衬底上生长出 Bi$_x$Sb$_{1-x}$的外延单取向薄膜,直至两个双层膜,在这两个双层膜中,杂化效应会使拓扑表面态发生隙化。在紧密结合模型的支持下,自旋和角度分辨光发射光谱数据显示,拓扑表面态的费米级口袋随着束缚间隙的增大而消失。在超薄极限中,拓扑表面态的间隙开口也得到了证明。最后,我们在 10 层薄膜中观察到拓扑表面态的引脚极化接近统一。超薄 Bi$_x$Sb$_{1-x}$ 合金的生长和表征表明,这种材料体系的超薄薄膜可用于研究二维拓扑物理以及拓扑器件、低功率电子学和自旋电子学等应用。
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