Topological Surface States in Paramagnetic and Antiferromagnetic Iron Pnictides
arXiv:1305.1770 · doi:10.1103/PhysRevB.88.165402
Abstract
The electronic structure of iron pnictides is topologically nontrivial, leading to the appearance of Dirac cones in the band structure for the antiferromagnetic phase. Motivated by the analogy with Dirac cones in graphene, we explore the possible existence of topologically protected surface states. Surprisingly, bands of surface states exist even in the paramagnetic state. A realistic five-orbital model predicts two such bands. In the antiferromagnetic phase, these surface bands survive but split. We obtain the bulk and surface dispersion from exact diagonalization of two- and five-orbital models in a strip geometry and discuss the results based on topology.
5 pages, 4 figures
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- Magnetic interactions in iron superconductors: A review
- Topological Mirror Insulators in One Dimension
- Topological Edge States with Zero Hall Conductivity in a Dimerized Hofstadter Model
- Topological superconductivity and Majorana states in low-dimensional systems
- Spin-orbital interplay and topology in the nematic phase of iron pnictides
- Topological flat bands in optical checkerboard-like lattices
- One-dimensional Dirac electrons on the surface of weak topological insulators
- Topological surface states and Andreev bound states in superconducting iron pnictides
- Semimetallic spin-density wave state in iron pnictides
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