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arxiv: 1708.03636 · v2 · pith:4PSFEY7Cnew · submitted 2017-08-11 · ❄️ cond-mat.mes-hall · cond-mat.mtrl-sci· cond-mat.str-el

Higher-Order Topological Insulators

classification ❄️ cond-mat.mes-hall cond-mat.mtrl-scicond-mat.str-el
keywords topologicalinsulatorsstatesprotectedhigher-orderhingebulksymmetries
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Three-dimensional topological (crystalline) insulators are materials with an insulating bulk, but conducting surface states which are topologically protected by time-reversal (or spatial) symmetries. Here, we extend the notion of three-dimensional topological insulators to systems that host no gapless surface states, but exhibit topologically protected gapless hinge states. Their topological character is protected by spatio-temporal symmetries, of which we present two cases: (1) Chiral higher-order topological insulators protected by the combination of time-reversal and a four-fold rotation symmetry. Their hinge states are chiral modes and the bulk topology is $\mathbb{Z}_2$-classified. (2) Helical higher-order topological insulators protected by time-reversal and mirror symmetries. Their hinge states come in Kramers pairs and the bulk topology is $\mathbb{Z}$-classified. We provide the topological invariants for both cases. Furthermore we show that SnTe as well as surface-modified Bi$_2$TeI, BiSe, and BiTe are helical higher-order topological insulators and propose a realistic experimental setup to detect the hinge states.

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  1. Boundary Condition Analysis of First and Second Order Topological Insulators

    cond-mat.mes-hall 2022-05 unverdicted novelty 4.0

    Derives dispersion relations for edge and hinge states from boundary conditions on Dirac lattice models and shows that nontrivial topology of a gapped edge state ensures a gapless hinge state.