Research progress of two-dimensional organic topological insulators

被引:5
|
作者
Gao Yi-Xuan [1 ,3 ]
Zhang Li-Zhi [1 ]
Zhang Yu-Yang [1 ,2 ,3 ]
Du Shi-Xuan [1 ,2 ,3 ]
机构
[1] Chinese Acad Sci, Inst Phys, Nanoscale Phys & Devices Lab, Beijing 100190, Peoples R China
[2] Chinese Acad Sci, Inst Phys, Songshan Lake Mat Lab, Dongguan 523808, Peoples R China
[3] Univ Chinese Acad Sci, Key Lab Vacuum Phys, Ctr Excellence Topol Quantum Computat, Beijing 100049, Peoples R China
基金
中国国家自然科学基金;
关键词
topological insulators; metal-organic framework; Dirac band; edge states; SPIN HALL INSULATOR; DIRAC CONES; PREDICTION; FRAMEWORK; NETWORK;
D O I
10.7498/aps.67.20181711
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
The discovery of new materials promotes the progress in science and technique. Among these new materials, topological materials have received much attention in recent years. Topological phases represent the advances both in the fundamental understanding of materials and in the broad applications in spintronics and quantum computing. The two-dimensional (2D) topological insulator (TI), also called quantum spin Hall insulator, is a promising material which has potential applications in future electronic devices with low energy consumption. The 2D TI has a bulk energy gap and a pair of gapless metallic edge states that are protected by the time reversal symmetry. To date, most of topological insulators are inorganic materials. Organic materials have potential advantages of low cost, easy fabrications, and mechanical flexibility. Historically, inorganic materials and devices have always found their organic counterparts, such as organic superconductors, organic light emitting diodes and organic spintronics. Recently, it has been predicted that some metal-organic lattices belong in an interesting class of 2D organic topological insulator (OTI). In this review, we present the progress of OTIs mainly in two typical types of them. In the first group, metal atoms bond with three neighboring molecules to form a hexagonal lattice, while they bond with two neighboring molecules to form a Kagome lattice. The electronic properties show that the Dirac band around Fermi level mainly comes from the hexagonal sites, and the flat band around Fermi level mainly is from Kagome lattice. It has been found that some of the materials from the first group could be intrinsic OTIs. However, none of the 2D OTIs predicted in the second group with a Kagome lattice is intrinsic. To obtain intrinsic OTIs from those non-intrinsic ones, in the heavy doping of material (one or two electrons per unit cell) it is required to move the Fermi level inside the gap opened by spin-orbit coupling, which is hard to realize in experiment. Therefore, many efforts have been made to search for intrinsic OTIs. It has been reported that the first group of 2D OTIs with a hexagonal lattice is found to be more possible to be intrinsic. By performing an electron counting and analyzing the orbital hybridization, an existing experimentally synthesized Cu-dicyanoanthracene (DCA) metal-organic framework is predicted to be an intrinsic OTI. Furthermore, like Cu-DCA, the structures consisting of molecules with cyanogen groups and noble metal atoms could be intrinsic OTIs. Finally, we discuss briefly possible future research directions in experimental synthesis and computational design of topological materials. We envision that OTIs will greatly broaden the scientific and technological influence of topological insulators and become a hot research topic in condensed matter physics.
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页数:9
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共 64 条
  • [1] Quantum spin Hall effect and topological phase transition in HgTe quantum wells
    Bernevig, B. Andrei
    Hughes, Taylor L.
    Zhang, Shou-Cheng
    [J]. SCIENCE, 2006, 314 (5806) : 1757 - 1761
  • [2] Cu3(hexaiminotriphenylene)2: An Electrically Conductive 2D Metal-Organic Framework for Chemiresistive Sensing
    Campbell, Michael G.
    Sheberla, Dennis
    Liu, Sophie F.
    Swager, Timothy M.
    Dinca, Mircea
    [J]. ANGEWANDTE CHEMIE-INTERNATIONAL EDITION, 2015, 54 (14) : 4349 - 4352
  • [3] Oriented 2D Covalent Organic Framework Thin Films on Single-Layer Graphene
    Colson, John W.
    Woll, Arthur R.
    Mukherjee, Arnab
    Levendorf, Mark P.
    Spitler, Eric L.
    Shields, Virgil B.
    Spencer, Michael G.
    Park, Jiwoong
    Dichtel, William R.
    [J]. SCIENCE, 2011, 332 (6026) : 228 - 231
  • [4] Porous, crystalline, covalent organic frameworks
    Côté, AP
    Benin, AI
    Ockwig, NW
    O'Keeffe, M
    Matzger, AJ
    Yaghi, OM
    [J]. SCIENCE, 2005, 310 (5751) : 1166 - 1170
  • [5] An electroactive porous network from covalent metal-dithiolene links
    Cui, Jieshun
    Xu, Zhengtao
    [J]. CHEMICAL COMMUNICATIONS, 2014, 50 (30) : 3986 - 3988
  • [6] Two-Dimensional π-Conjugated Covalent-Organic Frameworks as Quantum Anomalous Hall Topological Insulators
    Dong, Liang
    Kim, Youngkuk
    Er, Dequan
    Rappe, Andrew M.
    Shenoy, Vivek B.
    [J]. PHYSICAL REVIEW LETTERS, 2016, 116 (09)
  • [7] Nano-architectures by covalent assembly of molecular building blocks
    Grill, Leonhard
    Dyer, Matthew
    Lafferentz, Leif
    Persson, Mats
    Peters, Maike V.
    Hecht, Stefan
    [J]. NATURE NANOTECHNOLOGY, 2007, 2 (11) : 687 - 691
  • [8] Colloquium: Topological insulators
    Hasan, M. Z.
    Kane, C. L.
    [J]. REVIEWS OF MODERN PHYSICS, 2010, 82 (04) : 3045 - 3067
  • [9] Interfacing 2D and 3D Topological Insulators: Bi(111) Bilayer on Bi2Te3
    Hirahara, Toru
    Bihlmayer, Gustav
    Sakamoto, Yusuke
    Yamada, Manabu
    Miyazaki, Hidetoshi
    Kimura, Shin-ichi
    Bluegel, Stefan
    Hasegawa, Shuji
    [J]. PHYSICAL REVIEW LETTERS, 2011, 107 (16)
  • [10] The nontrivial electronic structure of Bi/Sb honeycombs on SiC(0001)
    Hsu, Chia-Hsiu
    Huang, Zhi-Quan
    Chuang, Feng-Chuan
    Kuo, Chien-Cheng
    Liu, Yu-Tzu
    Lin, Hsin
    Bansil, Arun
    [J]. NEW JOURNAL OF PHYSICS, 2015, 17