Photonic topological Anderson insulator in a two-dimensional atomic lattice

Disorder in atomic positions can induce a topologically nontrivial phase—topological Anderson insulator (TAI)—for transverse electric optical quasimodes of a two-dimensional honeycomb lattice of immobile atoms. TAI requires both time-reversal and inversion symmetries to be broken to similar extents....

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Main Authors: Skipetrov, Sergey E., Wulles, Pierre
Format: Article
Language:English
Published: Académie des sciences 2023-04-01
Series:Comptes Rendus. Physique
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Online Access:https://comptes-rendus.academie-sciences.fr/physique/articles/10.5802/crphys.147/
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author Skipetrov, Sergey E.
Wulles, Pierre
author_facet Skipetrov, Sergey E.
Wulles, Pierre
author_sort Skipetrov, Sergey E.
collection DOAJ
description Disorder in atomic positions can induce a topologically nontrivial phase—topological Anderson insulator (TAI)—for transverse electric optical quasimodes of a two-dimensional honeycomb lattice of immobile atoms. TAI requires both time-reversal and inversion symmetries to be broken to similar extents. It is characterized by a nonzero topological invariant, a reduced density of states and spatially localized quasimodes in the bulk, as well as propagating edge states. A transition from TAI to the topological insulator (TI) phase can take place at a constant value of the topological invariant, showing that TAI and TI represent the same topological phase.
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spelling doaj-art-d22b8531936a4332b2cba02f67861b662025-02-07T13:53:11ZengAcadémie des sciencesComptes Rendus. Physique1878-15352023-04-0124S3395410.5802/crphys.14710.5802/crphys.147Photonic topological Anderson insulator in a two-dimensional atomic latticeSkipetrov, Sergey E.0https://orcid.org/0000-0001-6186-1929Wulles, Pierre1https://orcid.org/0000-0002-0810-3464Univ. Grenoble Alpes, CNRS, LPMMC, 38000 Grenoble, FranceUniv. Grenoble Alpes, CNRS, LPMMC, 38000 Grenoble, FranceDisorder in atomic positions can induce a topologically nontrivial phase—topological Anderson insulator (TAI)—for transverse electric optical quasimodes of a two-dimensional honeycomb lattice of immobile atoms. TAI requires both time-reversal and inversion symmetries to be broken to similar extents. It is characterized by a nonzero topological invariant, a reduced density of states and spatially localized quasimodes in the bulk, as well as propagating edge states. A transition from TAI to the topological insulator (TI) phase can take place at a constant value of the topological invariant, showing that TAI and TI represent the same topological phase.https://comptes-rendus.academie-sciences.fr/physique/articles/10.5802/crphys.147/Topological photonicsLight scattering by atomsDisorderTopological Anderson insulatorBott index
spellingShingle Skipetrov, Sergey E.
Wulles, Pierre
Photonic topological Anderson insulator in a two-dimensional atomic lattice
Comptes Rendus. Physique
Topological photonics
Light scattering by atoms
Disorder
Topological Anderson insulator
Bott index
title Photonic topological Anderson insulator in a two-dimensional atomic lattice
title_full Photonic topological Anderson insulator in a two-dimensional atomic lattice
title_fullStr Photonic topological Anderson insulator in a two-dimensional atomic lattice
title_full_unstemmed Photonic topological Anderson insulator in a two-dimensional atomic lattice
title_short Photonic topological Anderson insulator in a two-dimensional atomic lattice
title_sort photonic topological anderson insulator in a two dimensional atomic lattice
topic Topological photonics
Light scattering by atoms
Disorder
Topological Anderson insulator
Bott index
url https://comptes-rendus.academie-sciences.fr/physique/articles/10.5802/crphys.147/
work_keys_str_mv AT skipetrovsergeye photonictopologicalandersoninsulatorinatwodimensionalatomiclattice
AT wullespierre photonictopologicalandersoninsulatorinatwodimensionalatomiclattice