Please use this identifier to cite or link to this item:
|Title:||Topological effects on the magnetoconductivity in topological insulators||Authors:||Sacksteder, Vincent E.
Arnardottir, Kristin Bjorg
Shelykh, Ivan A.
|Keywords:||DRNTU::Science::Physics||Issue Date:||2014||Source:||Sacksteder, V. E., Arnardottir, K. B., Kettemann, S., & Shelykh, I. A. (2014). Topological effects on the magnetoconductivity in topological insulators. Physical review B, 90(23), 235148-.||Series/Report no.:||Physical review B||Abstract:||Three-dimensional strong topological insulators (TIs) guarantee the existence of a two-dimensional (2-D) conducting surface state which completely covers the surface of the TI. The TI surface state necessarily wraps around the TI's top, bottom, and two sidewalls, and is therefore topologically distinct from ordinary 2-D electron gases (2-DEGs) which are planar. This has several consequences for the magnetoconductivity Δσ, a frequently studied measure of weak antilocalization which is sensitive to the quantum coherence time τϕ and to temperature. We show that conduction on the TI sidewalls systematically reduces Δσ, multiplying it by a factor which is always less than one and decreases in thicker samples. In addition, we present both an analytical formula and numerical results for the tilted-field magnetoconductivity which has been measured in several experiments. Lastly, we predict that as the temperature is reduced Δσ will enter a wrapped regime where it is sensitive to diffusion processes which make one or more circuits around the TI. In this wrapped regime the magnetoconductivity's dependence on temperature, typically 1/T2 in 2-DEGs, disappears. We present numerical and analytical predictions for the wrapped regime at both small and large field strengths. The wrapped regime and topological signatures discussed here should be visible in the same samples and at the same temperatures where the Altshuler-Aronov-Spivak (AAS) effect has already been observed, when the measurements are repeated with the magnetic field pointed perpendicularly to the TI's top face.||URI:||https://hdl.handle.net/10356/104257
|ISSN:||1098-0121||DOI:||10.1103/PhysRevB.90.235148||Rights:||© 2014 American Physical Society. This paper was published in Physical Review B and is made available as an electronic reprint (preprint) with permission of American Physical Society. The paper can be found at the following official DOI: [http://dx.doi.org/10.1103/PhysRevB.90.235148]. One print or electronic copy may be made for personal use only. Systematic or multiple reproduction, distribution to multiple locations via electronic or other means, duplication of any material in this paper for a fee or for commercial purposes, or modification of the content of the paper is prohibited and is subject to penalties under law.||Fulltext Permission:||open||Fulltext Availability:||With Fulltext|
|Appears in Collections:||SPMS Journal Articles|
Updated on Nov 21, 2022
Web of ScienceTM
Updated on Nov 28, 2022
Updated on Nov 29, 2022
Updated on Nov 29, 2022
Items in DR-NTU are protected by copyright, with all rights reserved, unless otherwise indicated.