双极扩散
超电流
凝聚态物理
场效应晶体管
拓扑绝缘体
超导电性
约瑟夫森效应
材料科学
晶体管
拓扑(电路)
物理
光电子学
电子
电气工程
量子力学
工程类
电压
作者
Yulu Liu,Ruoyu Chen,Zheneng Zhang,Marc Bockrath,Chun Ning Lau,Yan-Feng Zhou,Chiho Yoon,Li Sheng,Xiaoyuan Liu,Nikhil Dhale,Bing Lv,Fan Zhang,Kenji Watanabe,Takashi Taniguchi,Jianwei Huang,Ming Yi,Ji Seop Oh,R. J. Birgeneau
出处
期刊:Nano Letters
[American Chemical Society]
日期:2022-01-25
卷期号:22 (3): 1151-1158
被引量:12
标识
DOI:10.1021/acs.nanolett.1c04264
摘要
Bi4I4 belongs to a novel family of quasi-one-dimensional (1D) topological insulators (TIs). While its β phase was demonstrated to be a prototypical weak TI, the α phase, long thought to be a trivial insulator, was recently predicted to be a rare higher order TI. Here, we report the first gate tunable transport together with evidence for unconventional band topology in exfoliated α-Bi4I4 field effect transistors. We observe a Dirac-like longitudinal resistance peak and a sign change in the Hall resistance; their temperature dependences suggest competing transport mechanisms: a hole-doped insulating bulk and one or more gate-tunable ambipolar boundary channels. Our combined transport, photoemission, and theoretical results indicate that the gate-tunable channels likely arise from novel gapped side surface states, two-dimensional (2D) TI in the bottommost layer, and/or helical hinge states of the upper layers. Markedly, a gate-tunable supercurrent is observed in an α-Bi4I4 Josephson junction, underscoring the potential of these boundary channels to mediate topological superconductivity.
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