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Topological phase transitions in stanene and stanene-like systems by scaling the spin-orbit coupling
被引:7
|作者:
Wang, Xiaoxiong
[1
]
Wang, Peng
[2
]
Bian, Guang
[3
]
Chiang, T. -C.
[4
,5
]
机构:
[1] Nanjing Univ Sci & Technol, Coll Sci, Nanjing 210094, Jiangsu, Peoples R China
[2] Shandong Univ Sci & Technol, Coll Elect Commun & Phys, Qingdao 266590, Peoples R China
[3] Univ Missouri, Dept Phys & Astron, Columbia, MO 65211 USA
[4] Univ Illinois, Dept Phys, 1110 West Green St, Urbana, IL 61801 USA
[5] Univ Illinois, Frederick Seitz Mat Res Lab, 104 South Goodwin Ave, Urbana, IL 61801 USA
来源:
基金:
中国国家自然科学基金;
关键词:
SINGLE DIRAC CONE;
INSULATOR;
BI2SE3;
D O I:
10.1209/0295-5075/115/37010
中图分类号:
O4 [物理学];
学科分类号:
0702 ;
摘要:
We employ first-principles methods to study the topological properties of stanene and stanene-like materials by scaling stanene's natural intrinsic (atomic) spin-orbit-coupling (SOC) strength from 0 to 600%. Quantum phase transitions are observed in this two-dimensional system involving two different gaps. Stanene with zero SOC is a Dirac semimetal with a Dirac cone located at (K) over bar. An infinitesimal SOC opens up a gap at (K) over bar and the system becomes a two-dimensional topological insulator. Increasing the SOC to 333.3% causes the system to become a Dirac semimetal again with a Dirac cone located at (Gamma) over bar. Further increasing the SOC causes a gap opening at (Gamma) over bar, and the system becomes topologically trivial. This behavior is contrasted with that exhibited by three-dimensional topological insulators such as Bi2Se3, for which a strong SOC is a necessary but not a sufficient condition for the formation of topological phases. The similarities and differences are discussed. Copyright (C) EPLA, 2016
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页数:5
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