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New classes of three-dimensional topological crystalline insulators: Nonsymmorphic and magnetic

2015/01/22 by Chen Fang, Liang Fu · 12 citations
Materials Science · Mathematics · Physics and Astronomy · #Advanced Condensed Matter Physics #Condensed matter physics #Geometry #Graphene research and applications #Homogeneous space #Mathematics #Phase transition #Physics #Quantum #Quantum mechanics #Quantum phase transition #Quantum phases #Symmetry protected topological order #Topological Materials and Phenomena #Topological insulator #Topological order #Topology (electrical circuits) #cond-mat.mes-hall

paper · pdf · doi:10.1103/physrevb.91.161105

published as Phys. Rev. B 91, 161105 (2015) · 4 pages plus supplementary materials

arxiv created 2015/01/22 · openalex publication_date 2015/04/15 · arxiv updated 2015/04/16 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05

Abstract

We theoretically predict two new classes of three-dimensional topological crystalline insulators (TCIs), which have an odd number of unpinned surface Dirac cones protected by crystal symmetries. The first class is protected by a single nonsymmorphic glide plane symmetry; the second class is protected by a composition of a twofold rotation and time-reversal symmetry (a magnetic group symmetry). Both classes of TCIs are characterized by a quantized \ensuremathπ-Berry phase associated with surface states and a Z2 topological invariant associated with the bulk bands. In the presence of disorder, these TCI surface states are protected against localization by the average crystal symmetries, and exhibit critical conductivity in the universality class of the quantum Hall plateau transition. These new TCIs exist in time-reversal-breaking systems with or without spin-orbital coupling, and their material realizations are discussed.

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