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New topological invariants in non-Hermitian systems

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arxiv 1902.07972 v4 pith:7H6ITHVF submitted 2019-02-21 cond-mat.mes-hall cond-mat.quant-gasmath-phmath.MPphysics.opticsquant-ph

classification cond-mat.mes-hallcond-mat.quant-gasmath-phmath.MPphysics.opticsquant-ph
keywords topologicalinvariantsnon-hermitiansystemsuniquecomplexdiscussionsenergy
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Both theoretical and experimental studies of topological phases in non-Hermitian systems have made a remarkable progress in the last few years of research. In this article, we review the key concepts pertaining to topological phases in non-Hermitian Hamiltonians with relevant examples and realistic model setups. Discussions are devoted to both the adaptations of topological invariants from Hermitian to non-Hermitian systems, as well as origins of new topological invariants in the latter setup. Unique properties such as exceptional points and complex energy landscapes lead to new topological invariants including winding number/vorticity defined solely in the complex energy plane, and half-integer winding/Chern numbers. New forms of Kramers degeneracy appear here rendering distinct topological invariants. Modifications of adiabatic theory, time-evolution operator, biorthogonal bulk-boundary correspondence lead to unique features such as topological displacement of particles, `skin-effect', and edge-selective attenuated and amplified topological polarizations without chiral symmetry. Extension and realization of topological ideas in photonic systems are mentioned. We conclude with discussions on relevant future directions, and highlight potential applications of some of these unique topological features of the non-Hermitian Hamiltonians.

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Cited by 1 Pith paper

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Non-Hermitian Gravitational Wave Scattering

    gr-qc 2025-06 reject novelty 4.0 of 10

    The paper claims gravitational-wave frequencies at spectral singularities agree with the Hubble constant, but the agreement is obtained by freely choosing mode numbers and inserting H0 into the equations.

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