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Non-Bloch topological phases in a Hermitian system
被引:2
|作者:
Shi, Kaiye
[1
,2
]
Tian, Mingsheng
[3
,4
]
Sun, Feng-Xiao
[3
,4
]
Zhang, Wei
[1
,2
,5
]
机构:
[1] Renmin Univ China, Dept Phys, Beijing Key Lab Optoelect Funct Mat & Micronano De, Beijing 100872, Peoples R China
[2] Renmin Univ China, Key Lab Quantum State Construct & Manipulat, Minist Educ, Beijing 100872, Peoples R China
[3] Peking Univ, Frontiers Sci Ctr Nanooptoelectron, Sch Phys, Beijing 100871, Peoples R China
[4] Peking Univ, Frontiers Sci Ctr Nanooptoelectron, Sch Phys, State Key Lab Mesoscop Phys, Beijing 100871, Peoples R China
[5] Beijing Acad Quantum Informat Sci, Beijing 100193, Peoples R China
基金:
中国博士后科学基金;
中国国家自然科学基金;
国家重点研发计划;
北京市自然科学基金;
关键词:
SEMIMETAL;
D O I:
10.1103/PhysRevB.107.205154
中图分类号:
T [工业技术];
学科分类号:
08 ;
摘要:
The search for novel topological states of matter remains to be a research focus in the past several decades. While a topology theory based on Bloch bands is thoroughly investigated in systems with finite-range hopping, mostly in the context of condensed matter physics, here we study a generalized one-dimensional Su-SchriefferHeeger model with semi-infinite long-range hopping, and demonstrate another type of topological phase referred to as a Hermitian non-Bloch topological phase. This phase presents a pair of symmetry-protected edge modes, and can be characterized by a topological invariant defined upon real-space wave functions. Interestingly, we also find a large number of localized bulk modes near the band edges, residing at specific positions determined by the ratio between hopping range and system size. The proposed phenomena of a Hermitian non-Bloch topological phase can be realized in metamaterials such as topolectrical circuits and mechanical oscillator lattices.
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页数:7
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