Unravelling the edge spectra of non-Hermitian Chern insulators
arXiv:2209.06774 · doi:10.1103/PhysRevB.107.035101
Abstract
Non-Hermitian Chern insulators differ from their Hermitian cousins in one key aspect: their edge spectra are incredibly rich and confounding. For example, even in the simple case where the bulk spectrum consists of two bands with Chern number , the edge spectrum in the slab geometry may have one or two edge states on both edges, or only at one of the edges, depending on the model parameters. This blatant violation of the familiar bulk-edge correspondence casts doubt on whether the bulk Chern number can still be a useful topological invariant, and demands a working theory that can predict and explain the myriad of edge spectra from the bulk Hamiltonian to restore the bulk-edge correspondence. We outline how such a theory can be set up to yield a thorough understanding of the edge phase diagram based on the notion of the generalized Brillouin zone (GBZ) and the asymptotic properties of block Toeplitz matrices. The procedure is illustrated by solving and comparing three non-Hermitian generalizations of the Qi-Wu-Zhang model, a canonical example of two-band Chern insulators. We find that, surprisingly, in many cases the phase boundaries and the number and location of the edge states can be obtained analytically. Our analysis also reveals a non-Hermitian semimetal phase whose energy-momentum spectrum forms a continuous membrane with the edge modes transversing the hole, or genus, of the membrane. Subtleties in defining the Chern number over GBZ, which in general is not a smooth manifold and may have singularities, are demonstrated using examples. The approach presented here can be generalized to more complicated models of non-Hermitian insulators or semimetals in two or three dimensions.
19 pages, 12 figures
References in corpus (23)
- Topological Origin of Non-Hermitian Skin Effects
- Loss-induced suppression and revival of lasing
- Edge Modes, Degeneracies, and Topological Numbers in Non-Hermitian Systems
- Topological phases in the non-Hermitian Su-Schrieffer-Heeger model
- Weyl Exceptional Rings in a Three-Dimensional Dissipative Cold Atomic Gas
- Reversing the Pump-Dependence of a Laser at an Exceptional Point
- Topological phase transition in non-Hermitian quasicrystals
- Observation of parity-time symmetry breaking in a single spin system
- Periodic Table for Topological Bands with Non-Hermitian Bernard-LeClair Symmetries
- Universal non-Hermitian skin effect in two and higher dimensions
- New topological invariants in non-Hermitian systems
- Active topological photonics
- Gain and loss induced topological insulating phase in a non Hermitian electrical circuit
- Measuring the knot of non-Hermitian degeneracies and non-commuting braids
- Experimental Realization of Weyl Exceptional Rings in a Synthetic Three-Dimensional Non-Hermitian Phononic Crystal
- Fundamental limits for reciprocal and non-reciprocal non-Hermitian quantum sensing
- Non-Hermitian physics without gain or loss: the skin effect of reflected waves
- Nonlinear non-Hermitian higher-order topological laser
- Connections between the Open-boundary Spectrum and Generalized Brillouin Zone in Non-Hermitian Systems
- Quantum Fisher Information Perspective on Sensing in Anti-PT Symmetric Systems
- Single-mode lasing based on PT-breaking of two-dimensional photonic higher-order topological insulator
- Dynamical signatures of point-gap Weyl semimetal
- Cosine Edge Mode in a Periodically Driven Quantum System
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- Non-Hermitian Floquet Topological Matter -- A Review
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- Nontrivial worldline winding in non-Hermitian quantum systems
- Edge-selective extremal damping from topological heritage of dissipative Chern insulators
- Topological Invariant for Multi-Band Non-hermitian Systems with Chiral Symmetry
- Measuring topological invariants of even-dimensional line-gapped non-Hermitian systems through quench dynamics