Antiunitary symmetry protected higher-order topological phases

Higher-order topological (HOT) phases feature boundary (such as corner and hinge) modes of codimension d_{c}>1. We here identify an antiunitary operator that ensures the spectral symmetry of a two-dimensional HOT insulator and the existence of cornered localized states (d_{c}=2) at precise zero e...

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Main Author: Bitan Roy
Format: Article
Language:English
Published: American Physical Society 2019-12-01
Series:Physical Review Research
Online Access:http://doi.org/10.1103/PhysRevResearch.1.032048
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author Bitan Roy
author_facet Bitan Roy
author_sort Bitan Roy
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description Higher-order topological (HOT) phases feature boundary (such as corner and hinge) modes of codimension d_{c}>1. We here identify an antiunitary operator that ensures the spectral symmetry of a two-dimensional HOT insulator and the existence of cornered localized states (d_{c}=2) at precise zero energy. Such an antiunitary symmetry allows us to construct a generalized HOT insulator that continues to host corner modes even in the presence of a weak anomalous Hall insulator and spin-orbital density-wave orderings, and is characterized by a quantized quadrupolar moment Q_{xy}=0.5. Similar conclusions can be drawn for the time-reversal symmetry breaking HOT p+id superconductor and the corner localized Majorana zero modes survive even in the presence of weak Zeeman coupling and s-wave pairing. Such HOT insulators also serve as the building blocks of three-dimensional second-order Weyl semimetals, supporting one-dimensional hinge modes.
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spelling doaj.art-fd10a51a73ad423bb6e559774061948f2024-04-12T16:48:04ZengAmerican Physical SocietyPhysical Review Research2643-15642019-12-011303204810.1103/PhysRevResearch.1.032048Antiunitary symmetry protected higher-order topological phasesBitan RoyHigher-order topological (HOT) phases feature boundary (such as corner and hinge) modes of codimension d_{c}>1. We here identify an antiunitary operator that ensures the spectral symmetry of a two-dimensional HOT insulator and the existence of cornered localized states (d_{c}=2) at precise zero energy. Such an antiunitary symmetry allows us to construct a generalized HOT insulator that continues to host corner modes even in the presence of a weak anomalous Hall insulator and spin-orbital density-wave orderings, and is characterized by a quantized quadrupolar moment Q_{xy}=0.5. Similar conclusions can be drawn for the time-reversal symmetry breaking HOT p+id superconductor and the corner localized Majorana zero modes survive even in the presence of weak Zeeman coupling and s-wave pairing. Such HOT insulators also serve as the building blocks of three-dimensional second-order Weyl semimetals, supporting one-dimensional hinge modes.http://doi.org/10.1103/PhysRevResearch.1.032048
spellingShingle Bitan Roy
Antiunitary symmetry protected higher-order topological phases
Physical Review Research
title Antiunitary symmetry protected higher-order topological phases
title_full Antiunitary symmetry protected higher-order topological phases
title_fullStr Antiunitary symmetry protected higher-order topological phases
title_full_unstemmed Antiunitary symmetry protected higher-order topological phases
title_short Antiunitary symmetry protected higher-order topological phases
title_sort antiunitary symmetry protected higher order topological phases
url http://doi.org/10.1103/PhysRevResearch.1.032048
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