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拓扑绝缘体与平凡相和真空界面处形成的电子态之间的区别。

Distinction between electron states formed at topological insulator interfaces with the trivial phase and vacuum.

作者信息

Kazakov A S, Galeeva A V, Artamkin A I, Ikonnikov A V, Ryabova L I, Dvoretsky S A, Mikhailov N N, Bannikov M I, Danilov S N, Khokhlov D R

机构信息

Physics Department, M.V. Lomonosov Moscow State University, Moscow, 119991, Russia.

Chemistry Department, M.V. Lomonosov Moscow State University, Moscow, 119991, Russia.

出版信息

Sci Rep. 2021 Jun 2;11(1):11638. doi: 10.1038/s41598-021-91141-2.

DOI:10.1038/s41598-021-91141-2
PMID:34079020
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC8172881/
Abstract

In this paper, we show that electron states formed in topological insulators at the interfaces topological phase-trivial phase and topological phase-vacuum may possess different properties. This is demonstrated on an example of heterostructures based on thick topological HgCdTe films, in which the PT-symmetric terahertz photoconductivity is observed. It is shown that the effect originates from features of the interface topological film-trivial buffer/cap layer. The PT-symmetric terahertz photoconductivity is not provided by electron states formed at the interface topological film-vacuum.

摘要

在本文中,我们表明,拓扑绝缘体在拓扑相 - 平凡相和拓扑相 - 真空界面处形成的电子态可能具有不同的性质。这在基于厚拓扑HgCdTe薄膜的异质结构示例中得到了证明,其中观察到了PT对称太赫兹光电导率。结果表明,该效应源于界面拓扑薄膜 - 平凡缓冲层/帽层的特性。PT对称太赫兹光电导率并非由拓扑薄膜 - 真空界面处形成的电子态产生。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4846/8172881/a9308fc935ae/41598_2021_91141_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4846/8172881/5ad596ddb52a/41598_2021_91141_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4846/8172881/b19b14ceb90d/41598_2021_91141_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4846/8172881/ce34bf916597/41598_2021_91141_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4846/8172881/b53d51a3fa35/41598_2021_91141_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4846/8172881/a9308fc935ae/41598_2021_91141_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4846/8172881/5ad596ddb52a/41598_2021_91141_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4846/8172881/b19b14ceb90d/41598_2021_91141_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4846/8172881/ce34bf916597/41598_2021_91141_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4846/8172881/b53d51a3fa35/41598_2021_91141_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4846/8172881/a9308fc935ae/41598_2021_91141_Fig5_HTML.jpg

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本文引用的文献

1
Non-local terahertz photoconductivity in the topological phase of HgCdTe.HgCdTe拓扑相中的非局域太赫兹光电导性。
Sci Rep. 2021 Jan 15;11(1):1587. doi: 10.1038/s41598-021-81099-6.
2
Apparent PT-symmetric terahertz photoconductivity in the topological phase of HgCdTe-based structures.基于HgCdTe结构拓扑相的表观PT对称太赫兹光电导率
Sci Rep. 2020 Feb 11;10(1):2377. doi: 10.1038/s41598-020-59280-0.
3
Non-equilibrium electron transport induced by terahertz radiation in the topological and trivial phases of Hg Cd Te.太赫兹辐射在Hg Cd Te的拓扑相和平庸相中诱导的非平衡电子输运。
Beilstein J Nanotechnol. 2018 Mar 29;9:1035-1039. doi: 10.3762/bjnano.9.96. eCollection 2018.
4
Temperature-driven massless Kane fermions in HgCdTe crystals.HgCdTe 晶体中的温度驱动无质量 Kane 费米子。
Nat Commun. 2016 Aug 30;7:12576. doi: 10.1038/ncomms12576.
5
Quantum Hall effect from the topological surface states of strained bulk HgTe.应变体 HgTe 的拓扑表面态中的量子霍尔效应。
Phys Rev Lett. 2011 Mar 25;106(12):126803. doi: 10.1103/PhysRevLett.106.126803. Epub 2011 Mar 22.
6
A tunable topological insulator in the spin helical Dirac transport regime.自旋螺旋狄拉克输运 regime 中的可调谐拓扑绝缘体。 (注:“regime”常见释义为“政权;政体;管理制度;统治方式;生活状况;养生法;(军队的)特别训练计划;(自然现象或过程的)物理条件范围;(学科、活动等的)领域;状态” ,这里结合语境可能是“状态”等意思,由于不清楚确切所指,保留英文未翻译完整 )
Nature. 2009 Aug 27;460(7259):1101-5. doi: 10.1038/nature08234. Epub 2009 Jul 20.
7
A topological Dirac insulator in a quantum spin Hall phase.处于量子自旋霍尔相的拓扑狄拉克绝缘体。
Nature. 2008 Apr 24;452(7190):970-4. doi: 10.1038/nature06843.
8
Quantum spin Hall effect and topological phase transition in HgTe quantum wells.碲化汞量子阱中的量子自旋霍尔效应与拓扑相变
Science. 2006 Dec 15;314(5806):1757-61. doi: 10.1126/science.1133734.