scholarly journals Topological phase transition and quantum spin Hall edge states of antimony few layers

2016 ◽  
Vol 6 (1) ◽  
Author(s):  
Sung Hwan Kim ◽  
Kyung-Hwan Jin ◽  
Joonbum Park ◽  
Jun Sung Kim ◽  
Seung-Hoon Jhi ◽  
...  
2016 ◽  
Vol 18 (5) ◽  
pp. 3669-3674 ◽  
Author(s):  
Rosalba Juarez-Mosqueda ◽  
Yandong Ma ◽  
Thomas Heine

Quantum spin Hall (QSH) insulators exhibit a bulk insulting gap and metallic edge states characterized by nontrivial topology.


2017 ◽  
Vol 19 (7) ◽  
pp. 073031 ◽  
Author(s):  
Zhigang Song ◽  
Sumanta Bose ◽  
Weijun Fan ◽  
Dao Hua Zhang ◽  
Yan Yang Zhang ◽  
...  

2014 ◽  
Vol 116 (3) ◽  
pp. 033704 ◽  
Author(s):  
Bahadur Singh ◽  
Hsin Lin ◽  
R. Prasad ◽  
A. Bansil

2021 ◽  
Vol 11 (1) ◽  
Author(s):  
Milad Jangjan ◽  
Mir Vahid Hosseini

AbstractWe theoretically report the finding of a new kind of topological phase transition between a normal insulator and a topological metal state where the closing-reopening of bandgap is accompanied by passing the Fermi level through an additional band. The resulting nontrivial topological metal phase is characterized by stable zero-energy localized edge states that exist within the full gapless bulk states. Such states living on a quasi-one-dimensional system with three sublattices per unit cell are protected by hidden inversion symmetry. While other required symmetries such as chiral, particle-hole, or full inversion symmetry are absent in the system.


2021 ◽  
Author(s):  
Milad Jangjan ◽  
Mir Vahid Hosseini

Abstract We theoretically report the finding of a new kind of topological phase transition between a normal insulator and topological metal state where the closing-reopening of bandgap is accompanied by passing the Fermi level through an additional band. The resulting nontrivial topological metal phase is characterized by stable zero-energy localized edge states that exist within the full gapless bulk states. Such states living on a quasi-one-dimensional system with three sublattices per unit cell are protected by hidden inversion symmetry. While other required symmetries such as chiral, particle-hole, or full inversion symmetry are absent in the system.


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