Abstract

We classify insulators by generalized symmetries that combine space-time transformations with quasimomentum translations. Our group-cohomological classification generalizes the nonsymmorphic space groups, which extend point groups by real-space translations; i.e., nonsymmorphic symmetries unavoidably translate the spatial origin by a fraction of the lattice period. Here, we further extend nonsymmorphic groups by reciprocal translations, thus placing real and quasimomentum space on equal footing. We propose that group cohomology provides a symmetry-based classification of quasimomentum manifolds, which in turn determines the band topology. In this sense, cohomology underlies band topology. Our claim is exemplified by the first theory of time-reversal-invariant insulators with nonsymmorphic spatial symmetries. These insulators may be described as “piecewise topological,” in the sense that subtopologies describe the different high-symmetry submanifolds of the Brillouin zone, and the various subtopologies must be pieced together to form a globally consistent topology. The subtopologies that we discover include a glide-symmetric analog of the quantum spin Hall effect, an hourglass-flow topology (exemplified by our recently proposed KHgSb material class), and quantized non-Abelian polarizations. Our cohomological classification results in an atypical bulk-boundary correspondence for our topological insulators.7 MoreReceived 24 November 2015DOI:https://doi.org/10.1103/PhysRevX.6.021008This article is available under the terms of the Creative Commons Attribution 3.0 License. Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI.Published by the American Physical SocietyPhysics Subject Headings (PhySH)Physical SystemsInsulatorsTopological insulatorsTopological materialsCondensed Matter, Materials & Applied Physics

Highlights

  • Spatial symmetries have enriched the topological classification of insulators and superconductors [1,2,3,4,5,6,7,8,9,10]

  • While we primarily focus on the symmetries (i)–(iii), they do not generate the full group of D46h; e.g., there exists a sixfold screw symmetry whose implications have been explored in our companion paper [21]

  • In our companion work [21], we have identified a criterion on the surface group that characterizes all robust surface states that are protected by space-time symmetries [1,2,4,7,8,18,19,25,40,41,42,43,54]

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Summary

Introduction

Spatial symmetries have enriched the topological classification of insulators and superconductors [1,2,3,4,5,6,7,8,9,10]. A basic geometric property that distinguishes spatial symmetries regards their transformation of the spatial origin: symmorphic symmetries preserve the origin, while nonsymmorphic symmetries unavoidably translate the origin by a fraction of the lattice period [11]. This fractional translation is responsible for band topologies that have no analog in symmorphic crystals. Motivated by our recently proposed KHgX material class (X 1⁄4 Sb, Bi, As) [21], we present here a complete classification of spin-orbit-coupled insulators with the space group (D46h) of KHgX

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