Topological edge states of continuous Hamiltonians

Abstract This paper concerns the topological classification of continuous Hamiltonians that find applications in biased cold plasmas and photonics. Besides a magnetic bias, the Hamiltonians are parameterized by a plasma frequency and a fixed vertical wavenumber. Eight distinct phases of matter are identified as these parameters vary. When insulating gaps are shared by two such phases, asymmetric edge modes propagate along interfaces separating the two phases. Here we apply the notion of a bulk difference invariant (BDI) to this Hamiltonian, and show by numerical diagonalizations of interface Hamiltonians that after an appropriate regularization our BDI correctly predicts edge transport as described by a bulk edge correspondence (BEC). We also derive theoretical tools to compute the BDI and show the limitations of the BEC when the phase transition is too singular.

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Publication Details

Journal
New Journal of Physics
Published
2025-09-19
DOI
https://doi.org/10.1088/1367-2630/ae095d
Citations
1
Primary Topic
Quantum chaos and dynamical systems
Type
article
Field-Weighted Citation Impact
1.32
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article

Topological edge states of continuous Hamiltonians

Guillaume Bal, Matthew James Frazier
1 citations
New Journal of Physics
Quantum chaos and dynamical systems
1.32
article

Topological edge states of continuous Hamiltonians

Guillaume Bal, Matthew James Frazier
article en
1 citations

Abstract

Abstract This paper concerns the topological classification of continuous Hamiltonians that find applications in biased cold plasmas and photonics. Besides a magnetic bias, the Hamiltonians are parameterized by a plasma frequency and a fixed vertical wavenumber. Eight distinct phases of matter are identified as these parameters vary. When insulating gaps are shared by two such phases, asymmetric edge modes propagate along interfaces separating the two phases. Here we apply the notion of a bulk difference invariant (BDI) to this Hamiltonian, and show by numerical diagonalizations of interface Hamiltonians that after an appropriate regularization our BDI correctly predicts edge transport as described by a bulk edge correspondence (BEC). We also derive theoretical tools to compute the BDI and show the limitations of the BEC when the phase transition is too singular.

New Journal of PhysicsVol. 27(10)
University of Illinois Chicago (US), University of Chicago (US), Applied Mathematics (United States) (US)
Openalex Percentile: Top 16%
Quantum chaos and dynamical systems
1.32
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Topological edge states of continuous Hamiltonians — Guillaume Bal, Matthew James Frazier · New Journal of Physics (2025) | TGRS Research Map | TGRS