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Current shunting effects in Cd<sub>3</sub>As<sub>2</sub>: a closer look at the topological-ferromagnet interface

ORAL

Abstract

Topological materials, such as Cd3As2, are of great importance for next-generation computing systems where energy efficiency is paramount. For example, in spin-orbit torque magnetic random-access memory (SOT-MRAM), topological materials generate the spin-orbit torque necessary for magnetization switching of an adjacent magnetic layer. Current shunting at the ferromagnet-topological material interface can be detrimental for spin generation and overall SOT efficiency.1 Here, the current shunting effect is analyzed in permalloy- and gold-shunted Cd3As2 disk structures using angle-dependent magnetoresistance measurements. Shubnikov-de Haas oscillations and weak antilocalization effects are observed in the Cd3As2, and their presence is dampened upon incorporating a shunt onto the topological surface. Hakami-Larkin-Nagaoka and Tkachov-Hankiewicz models are used to evaluate the weak antilocalization.2,3 We confirm the effects of current shunting, and discuss its detriment to the efficiency of spin-based devices.

References:

1. Tang, W., Liu, H., Li, Z., Pan, A. & Zeng, Y. Adv. Sci. 8, 2100847 (2021).

2. Hikami, S., Larkin, A. I. & Nagaoka, Y. Prog. Theor. Phys. 63, 707–710 (1980).

3. Tkachov, G. & Hankiewicz, E. M. Phys. Rev. B 84, 035444 (2011).

Presenters

  • Nicholas A Blumenschein

    Laboratory for Physical Sciences

Authors

  • Nicholas A Blumenschein

    Laboratory for Physical Sciences

  • Gregory Stephen

    University of Maryland, Laboratory for Physical Sciences

  • Karen E Grutter

    Laboratory for Physical Sciences, College Park, MD 20740, USA, Laboratory for Physical Sciences

  • Erick C Sadler

    Laboratory for Physical Sciences

  • Jennifer E DeMell

    Laboratory for Physical Sciences

  • Binghao Guo

    University of California, Santa Barbara

  • Susanne Stemmer

    University of California, Santa Barbara

  • Aubrey T Hanbicki

    Laboratory for Physical Sciences

  • Adam L Friedman

    Laboratory for Physical Sciences