Weak localization and weak antilocalization in doped Ge1-y Sny layers with up to 8% Sn

Weisshaupt D, Funk HS, Kern M, Dettling MM, Schwarz D, Oehme M, Suergers C, Van Slageren J, Fischer IA, Schulze J (2020)


Publication Type: Journal article

Publication year: 2020

Journal

Book Volume: 33

Article Number: 085703

Journal Issue: 8

DOI: 10.1088/1361-648X/abcb68

Abstract

Low-temperature magnetoresistance measurements of n- and p-doped germanium-tin (Ge1-y Sn y ) layers with Sn concentrations up to 8% show contributions arising from effects of weak localization for n-type and weak antilocalization for p-type doped samples independent of the Sn concentration. Calculations of the magnetoresistance using the Hikami-Larkin-Nagaoka model for two-dimensional transport allow us to extract the phase-coherence length for all samples as well as the spin-orbit length for the p-type doped samples. For pure Ge, we find phase-coherence lengths as long as (349.0 ± 1.4) nm and (614.0 ± 0.9) nm for n-type and p-type doped samples, respectively. The phase-coherence length decreases with increasing Sn concentration. From the spin-orbit scattering length, we determine the spin-diffusion scattering length in the range of 20-30 nm for all highly degenerate p-type doped samples irrespective of Sn concentration. These results show that Ge1-y Sn y is a promising material for future spintronic applications.

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APA:

Weisshaupt, D., Funk, H.S., Kern, M., Dettling, M.M., Schwarz, D., Oehme, M.,... Schulze, J. (2020). Weak localization and weak antilocalization in doped Ge1-y Sny layers with up to 8% Sn. Journal of Physics: Condensed Matter, 33(8). https://doi.org/10.1088/1361-648X/abcb68

MLA:

Weisshaupt, David, et al. "Weak localization and weak antilocalization in doped Ge1-y Sny layers with up to 8% Sn." Journal of Physics: Condensed Matter 33.8 (2020).

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