Band structure engineering of multinary chalcogenide topological insulators

被引:60
作者
Chen, Shiyou [1 ,2 ,3 ]
Gong, X. G. [2 ,3 ]
Duan, Chun-Gang [1 ]
Zhu, Zi-Qiang [1 ]
Chu, Jun-Hao [1 ]
Walsh, Aron [4 ]
Yao, Yu-Gui [5 ]
Ma, Jie [6 ]
Wei, Su-Huai [6 ]
机构
[1] E China Normal Univ, Lab Polar Mat & Devices, Shanghai 200241, Peoples R China
[2] Fudan Univ, Lab Computat Phys Sci, Shanghai 200433, Peoples R China
[3] Fudan Univ, Surface Phys Lab, Shanghai 200433, Peoples R China
[4] UCL, Dept Chem, London WC1E 6BT, England
[5] Chinese Acad Sci, Inst Phys, Beijing 100190, Peoples R China
[6] Natl Renewable Energy Lab, Golden, CO 80401 USA
关键词
SINGLE DIRAC CONE;
D O I
10.1103/PhysRevB.83.245202
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Topological insulators (TIs) have been found in strained binary HgTe and ternary I-III-VI2 chalcopyrite compounds such as CuTlSe2 which have inverted band structures. However, the nontrivial band gaps of these existing binary and ternary TIs are limited to small values, usually around 10 meV or less. In this work, we reveal that a large nontrivial band gap requires the material to have a large negative crystal field splitting Delta(CF) at the top of the valence band and a moderately large negative s-p band gap E-g(s-p). These parameters can be better tuned through chemical ordering in multinary compounds. Based on this understanding, we show that a series of quaternary I-2-II-IV-VI4 compounds, including Cu2HgPbSe4, Cu2CdPbSe4, Ag2HgPbSe4, and Ag2CdPbTe4, are TIs, in which Ag2HgPbSe4 has the largest TI band gap of 47 meV because it combines the optimal values of Delta(CF) and E-g(s-p).
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页数:5
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