Tight-binding theory of surface spin states on bismuth thin films
arXiv:1507.06783 · doi:10.1103/PhysRevB.93.041301
Abstract
The surface spin states for bismuth thin films were investigated using an tight-binding model. The model explains the experimental observations using angle-resolved photoemission spectroscopy, including the Fermi surface, the band structure with Rashba spin splitting, and the quantum confinement in the energy band gap of the surface states. A large out-of-plane spin component also appears. The surface states penetrate inside the film to within approximately a few bilayers near the Brillouin-zone center, whereas they reach the center of the film near the Brillouin-zone boundary.
7 pages, 5 figures
References in corpus (5)
- Surface States of the Topological Insulator Bi_{1-x}Sb_x
- Strong spin-orbit splitting on Bi surfaces
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- Visualization of spin-polarized electronic states by imaging-type spin-resolved photoemission microscopy
- Localized Wannier function based tight-binding models for two-dimensional allotropes of bismuth
- Theory of spin and orbital charge conversion at the surface states of Bi_{1-x}Sb_x topological insulator
- Quantum Confinement and Heavy Surface States of Dirac Fermions in Bismuth (111) Films: an Analytical Approach
- Moiré superlattices of antimonene on a Bi(111) substrate with van Hove singularity and Rashba-type spin polarization
- Topological blocking at the Bi(111) surface due to surface relaxation
- Long-range permeation of wave function and superficial surface state due to strong quantum size effects in topological Bi/BiSb heterojunctions