Abstract

The rich variety of crystalline symmetries in solids leads to a plethora of topological crystalline insulators (TCIs) featuring distinct physical properties, which are conventionally understood in terms of bulk invariants specialized to the symmetries at hand. While isolated examples of TCI have been identified and studied, the same variety demands a unified theoretical framework. In this work, we show how the surfaces of TCIs can be analyzed within a general surface theory with multiple flavors of Dirac fermions, whose mass terms transform in specific ways under crystalline symmetries. We identify global obstructions to achieving a fully gapped surface, which typically lead to gapless domain walls on suitably chosen surface geometries. We perform this analysis for all 32 point groups, and subsequently for all 230 space groups, for spin-orbit-coupled electrons. We recover all previously discussed TCIs in this symmetry class, including those with "hinge" surface states. Finally, we make connections to the bulk band topology as diagnosed through symmetry-based indicators. We show that spin-orbit-coupled band insulators with nontrivial symmetry indicators are always accompanied by surface states that must be gapless somewhere on suitably chosen surfaces. We provide an explicit mapping between symmetry indicators, which can be readily calculated, and the characteristic surface states of the resulting TCIs.

Highlights

  • Topological phases of free fermions protected by internal symmetries feature a gapped bulk and symmetry-protected gapless surface states [1]

  • The rich variety of crystalline symmetries in solids leads to a plethora of topological crystalline insulators (TCIs), featuring distinct physical properties, which are conventionally understood in terms of bulk invariants specialized to the symmetries at hand

  • We show how the surfaces of TCIs can be analyzed within a general surface theory with multiple flavors of Dirac fermions, whose mass terms transform in specific ways under crystalline symmetries

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Summary

INTRODUCTION

Topological phases of free fermions protected by internal symmetries (such as time reversal) feature a gapped bulk and symmetry-protected gapless surface states [1]. We note that a nontrivial symmetry indicator constitutes a sufficient, but not necessary, condition for the presence of band topology, and we discuss examples of topological phases that have gapless surface states predicted by our Dirac approach, the symmetry indicator is trivial. A common theme is to embrace a real-space perspective, where “topological crystals” are built by repeating motifs that are, by themselves, topological phases of some lower dimension and are potentially protected by internal symmetries or spatial symmetries that leave certain regions invariant (say, on a mirror plane) [38,41] Such a picture allows one to readily deduce the interaction stability of the phases we describe [43], and we briefly discuss how our Dirac surface theory analysis can be reconciled with such general frameworks

SYMMETRY INDICATORS AND BULK TOPOLOGY
Review of familiar indices
Z4 index for inversion symmetry
Combination of κ1 and κ4
Summary of XBS
SURFACE STATES
Stacked strong TIs
Crystallographic point groups
Crystallographic point-group symmetries
Classification of sTCIs in the 32 crystallographic point groups
Space groups
Nonsymmorphic symmetries
Lattice translation
Classification of sTCIs in the 230 space groups
Surface dispersion at special planes
Single mirror or glide plane
Rotation axis
Multiple mirror or glide planes
BULK-SURFACE CORRESPONDENCE
DISCUSSION
Justification for the simplifying assumption
Surface-state ambiguity
Table for the sTCI classification and surface-state ambiguity
Full Text
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