Non-linear hybrid surface-defect states in defective BiSe
arXiv:2201.03320 · doi:10.1021/acs.jpcc.2c03142
Abstract
Surface-states of topological insulators are assumed to be robust against non-magnetic defects in the crystal. However, recent theoretical models and experiments indicate that even non-magnetic defects can perturb these states. Our first-principles calculations demonstrate that the presence of Se vacancies in BiSe, has a greater impact than a mere n-doping of the structure, which would just shift the Fermi level relative to the Dirac point. We observe the emergence of a non-linear band pinned near the Fermi level, while the Dirac cone shifts deeper into the valence band. We attribute these features in the bandstructure to the interaction between the surface and defect states, with the resulting hybridization between these states itself depending on the position and symmetry of the Se vacancy relative to the surfaces. Our results bring us a step closer to understanding the exotic physics emerging from defects in BiSe that remained unexplored in prior studies.
References in corpus (6)
- Quantum Spin Hall Effect and Topological Phase Transition in HgTe Quantum Wells
- Discovery (theoretical prediction and experimental observation) of a large-gap topological-insulator class with spin-polarized single-Dirac-cone on the surface
- A topological Dirac insulator in a quantum spin Hall phase : Experimental observation of first strong topological insulator
- Coexistence of the topological state and a two-dimensional electron gas on the surface of Bi2Se3
- Disorder enabled band structure engineering of a topological insulator surface
- Topological surface states of Bi2Se3 with the coexistence of Se vacancies