Download scientific diagram | Two-dimensional higher-order topological insulator tight-binding model. a Bulk band-structure and spin Hall conductivity (σ z xy ) as a function of the Fermi energy. b Eigenvalues for a square flake geometry (open boundary conditions) with 32 × 32 sites. The red circles represent the degenerate corner states, with the inset showing a narrow energy window to emphasize their degeneracy. c Corner states realspace projection. The model parameters of equation (1) are M = 2t = 2ξ = 1 and Δ = 0.25. d Spin Hall conductivity as a function of the model parameters (0 ≤ t ≤ 2), (0 ≤ Δ ≤ 1) and (0 < M ≤ 10). e, f, g Spin Hall conductivity for fixed values of Δ = 0, 0.25, and 0.75, respectively. from publication: Discovery of higher-order topological insulators using the spin Hall conductivity as a topology signature | The discovery and realization of topological insulators, a phase of matter which hosts metallic boundary states when the d-dimension insulating bulk is confined to (d − 1)-dimensions, led to several potential applications. Recently, it was shown that protected topological | Topology, Conductivity and Discovery | ResearchGate, the professional network for scientists.
Frontiers Bound states at disclinations: an additive rule of real and reciprocal space topology
Discovery of higher-order topological insulators using the spin Hall conductivity as a topology signature
Carlos ACOSTA, PostDoc Position, PhD, University of Colorado Boulder, CO, CUB, Renewable & Sustainable Energy Institute (RASEI)
Higher-order topological insulators a, In contrast to conventional TIs
3 Topological Twistronics, Frontiers in Synthetic Moiré Quantum Matter: Proceedings of a Workshop
Temperature Dependence of Spin–Orbit Torques in Nearly Compensated Tb21Co79 Films by a Topological Insulator Sb2Te3
Atomic scale TEM analysis and 1D ¹²⁵Te NMR a Cross-sectional HAADF-ABF
Experimental results for one point on the surface h0 = −0.1ξ0 in Case
Two-dimensional higher-order topological insulator tight-binding model.
