Takagi Topological Insulator on the Honeycomb Lattice
arXiv:2205.05873 · doi:10.3389/fphy.2022.915764
Abstract
Recently, real topological phases protected by symmetry have been actively investigated. In two dimensions, the corresponding topological invariant is the Stiefel-Whitney number. A recent theoretical advance is that in the presence of the sublattice symmetry, the Stiefel-Whitney number can be equivalently formulated in terms of Takagi's factorization. The topological invariant gives rise to a novel second-order topological insulator with odd -related pairs of corner zero modes. In this article, we review the elements of this novel second-order topological insulator, and demonstrate the essential physics by a simple model on the honeycomb lattice.
References in corpus (12)
- Classification of topological insulators and superconductors in three spatial dimensions
- Topological Crystalline Insulators
- Electric Multipole Moments, Topological Multipole Moment Pumping, and Chiral Hinge States in Crystalline Insulators
- Topological Acoustics
- Topology of crystalline insulators and superconductors
- Classification of reflection symmetry protected topological semimetals and nodal superconductors
- Surface State Magnetization and Chiral Edge States on Topological Insulators
- Symmetric Real Dirac Fermions and Semimetals
- Boundary criticality of -invariant topology and second-order nodal-line semimetals
- Second-Order Real Nodal-Line Semimetal in Three-Dimensional Graphdiyne
- Inflated nodes and surface states in superconducting half-Heusler compounds
- Quasiparticle tunneling and 1/f charge noise in ultrastrongly coupled superconducting qubit and resonator