Non-local sidewall response and deviation from exact quantization of the topological magnetoelectric effect in axion-insulator thin films
arXiv:2107.02410 · doi:10.1103/PhysRevB.104.L201102
Abstract
Topological insulator (TI) thin films with surface magnetism are expected to exhibit a quantized anomalous Hall effect (QAHE) when the magnetizations on the top and bottom surfaces are parallel, and a quantized topological magnetoelectric (QTME) response when the magnetizations have opposing orientations (axion insulator phase) and the films are sufficiently thick. We present a unified picture of both effects that associates deviations from exact quantization of the QTME caused by finite thickness with non-locality in the side-wall current response function. Using realistic tight-binding model calculations, we show that in TI thin films deviations from quantization in the axion insulator-phase are reduced in size when the exchange coupling of tight-binding model basis states to the local magnetization near the surface is strengthened. Stronger exchange coupling also reduces the effect of potential disorder, which is unimportant for the QAHE but detrimental for the QTME, which requires that the Fermi energy lie inside the gap at all positions.
arXiv comment5 pages, 4 figures
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- Engineering axion insulator phase in superlattices with inversion symmetry breaking
- Symmetry, topology, and geometry: The many faces of the topological magnetoelectric effect
- Capacitive scheme to detect the topological magnetoelectric effect
- Chiral edge transport along domain walls in magnetic topological insulator nanoribbons
- Surface Reconstructions in Thin-Films of Magnetic Topological Insulator MnBiTe
- Generalized method of image dyons for quasi-two dimensional slabs with ordinary-topological insulator interfaces