Feature-energy duality of topological boundary states in multilayer quantum spin Hall insulator
arXiv:2312.11794 · doi:10.1103/PhysRevB.109.155143
Abstract
Gapless topological boundary states characterize nontrivial topological phases arising from the bulk-boundary correspondence in symmetry-protected topological materials, such as the emergence of helical edge states in a two-dimensional topological insulator. However, the incorporation of symmetry-breaking perturbation terms in the Hamiltonian leads to the gapping of these edge bands, resulting in missing these crucial topological boundary states. In this work, we systematically investigate the robustness of bulk-boundary correspondence in the quantum spin Hall insulator via recently introduced feature spectrum topology. Our findings present a comprehensive understanding of feature-energy duality, illustrating that the aggregate number of gapless edge states in the energy-momentum () map and the non-trivial edge states in the feature spectrum equals the spin Chern number of multilayer quantum spin Hall insulator. We identify a van der Waals material bismuth bromide as a promising candidate through first-principles calculations. Our work not only unravels the intricacies of bulk-boundary correspondence but also charts a course for exploring quantum spin Hall insulators with high spin-Chern number.
References in corpus (8)
- Topological Insulators with Inversion Symmetry
- Valley-Polarized Metals and Quantum Anomalous Hall Effect in Silicene
- Quantum Spin Hall Effect and Topologically Invariant Chern Numbers
- Colloquium: Quantum anomalous Hall effect
- Robustness of the Spin-Chern number
- Large-Gap Quantum Spin Hall Insulator in single layer bismuth monobromide BiBr
- Spin-Resolved Topology and Partial Axion Angles in Three-Dimensional Insulators
- Topological edge states in single- and multi-layer BiBr