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Edge states and topological phases in non-Hermitian systems

2011/07/20 by Kenta Esaki, Masatoshi Sato, Kazuki Hasebe +1 · 11 citations
Mathematics · Physics and Astronomy · #Atiyah–Singer index theorem #Combinatorics #Condensed matter physics #Gapless playback #Hamiltonian (control theory) #Hermitian matrix #Lattice (music) #Mathematical analysis #Mathematical physics #Mathematics #Physics #Pure mathematics #Quantum Mechanics and Non-Hermitian Physics #Quantum mechanics #Quantum, superfluid, helium dynamics #Topological Materials and Phenomena #Topology (electrical circuits) #Winding number #cond-mat.mes-hall #cond-mat.other #math-ph #math.MP #quant-ph

paper · pdf · doi:10.1103/physrevb.84.205128

published as Phys. Rev. B 84, 205128 (2011) · 29 pages, 19 figures, typos fixed

arxiv created 2011/07/20 · openalex publication_date 2011/11/17 · arxiv updated 2012/01/04 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05

Abstract

Topological stability of the edge states is investigated for non-Hermitian systems. We examine two classes of non-Hermitian Hamiltonians supporting real bulk eigenenergies in weak non-Hermiticity: SU(1,1) and SO(3,2) Hamiltonians. As an SU(1,1) Hamiltonian, the tight-binding model on the honeycomb lattice with imaginary onsite potentials is examined. Edge states with ReE=0 and their topological stability are discussed by the winding number and the index theorem based on the pseudo-anti-Hermiticity of the system. As a higher-symmetric generalization of SU(1,1) Hamiltonians, we also consider SO(3,2) models. We investigate non-Hermitian generalization of the Luttinger Hamiltonian on the square lattice and that of the Kane-Mele model on the honeycomb lattice, respectively. Using the generalized Kramers theorem for the time-reversal operator \ensuremathΘ with \ensuremathΘ2=+1 [M. Sato et al., e-print arXiv:1106.1806], we introduce a time-reversal-invariant Chern number from which topological stability of gapless edge modes is argued.

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