Abstract

We propose a two-dimensional non-Hermitian Chern insulator with inversion symmetry, which is anisotropic and has staggered gain and loss in both x and y directions. In this system, conventional bulk-boundary correspondence holds. The Chern number is a topological invariant that accurately predicts the topological phase transition and the existence of helical edge states in the topologically nontrivial gapped phase. In the gapless phase, the band touching points are isolated and protected by the symmetry. The degenerate points alter the system topology, and the exceptional points can destroy the existence of helical edge states. Topologically protected helical edge states exist in the gapless phase for the system under open boundary condition in one direction, which are predicted by the winding number associated with the vector field of average values of Pauli matrices. The winding number also identifies the detaching points between the edge states and the bulk states in the energy bands. The non-Hermiticity also supports a topological phase with zero Chern number, where a pair of in-gap helical edge states exists. Our findings provide insights into the symmetry protected non-Hermitian topological insulators.

Highlights

  • The topological phase of matter in condensed matter physics has been attracting considerable research interest and has been widely explored [1,2,3,4,5,6,7]

  • Protected helical edge states exist in the gapless phase for the system under open boundary condition in one direction, which are predicted by the winding number associated with the vector field of average values of Pauli matrices

  • Open systems ubiquitously exist in physics [8,9,10], the optical and photonic systems; these are mostly non-Hermitian because they interact with the environment [11,12,13,14,15,16]

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Summary

INTRODUCTION

The topological phase of matter in condensed matter physics has been attracting considerable research interest and has been widely explored [1,2,3,4,5,6,7]. [58,59,60,61,62], an inversion symmetric 2D non-Hermitian Chern insulator is proposed and the validity of conventional bulk-boundary correspondence is predicted in the end of Ref. Different from the anomalous edge states that are localized in a single unit cell [129], and those that cannot be predicted by the bulk topology [60], a pair of helical edge states appear in the topologically nontrivial phase of the inversion symmetric Chern insulator under OBC. Non-Hermiticity creates a pair of topologically protected in-gap helical edge states in a novel phase with zero Chern number.

INVERSION SYMMETRIC NON-HERMITIAN CHERN INSULATOR
PHASE DIAGRAM AND TOPOLOGICAL CHARACTERIZATION
ENERGY BANDS AND EDGE STATES OF THE EDGE HAMILTONIAN
DISCUSSION
SUMMARY
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