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Electrically-tunable tunneling anisotropy magnetoresistance in few-layer CrPS<sub>4</sub>

ORAL

Abstract

Electrical control of spin degree of freedom in magnetic materials lays the foundation of modern spintronics and information technology. Two-dimensional (2D) magnets with stable 2D magnetism have bought new opportunities to manipulate magnetism down to the 2D limit1,2. For instance, recently gate-induced magnetic phase transition in bilayer CrI33,4 and multiferroism in monolayer NiI25 have been successfully demonstrated. Despite these progresses, the realization of electrically manipulated magnetization in other 2D magnets is still desirable. In this talk, we report the electrically tunable tunneling anisotropy magnetoresistance (TAMR) in CrPS4-based magnetic tunnel junctions with a structure of graphite (top gate)/h-BN/graphene/few-layer CrPS4/graphene/h-BN/graphite (bottom gate). We will first discuss the layer-dependent magnetism in few-layer CrPS4 through the electrical tunneling magnetotransport measurements. Then, we will focus on the gate dependences of tunneling magnetoresistance and TAMR of the magnetic tunnel junctions. Strikingly, we find that the polarity of the TAMR can be successfully changed by either the applied bias or gate voltage, suggesting that the magnetic anisotropy in CrPS4 can be modulated by electrical means. Our findings suggest that few-layer CrPS4 may feature strong magnetoelectric coupling, thus offering a potential platform for realizing nonvolatile memory devices.

1. Gong, C. et al. Nature 546, 265–269 (2017).

2. Huang, B. et al. Nature 546, 270–273 (2017).

3. Huang, B. et al. Nature Nanotechnology 13, 544–548 (2018).

4. Jiang, S. et al. Nature Nanotechnology 13, 549–553 (2018).

5. Song, Q. et al. Nature. 26, 1–17 (2021).

Publication: None

Presenters

  • Zhuangen Fu

    University of Wyoming

Authors

  • Zhuangen Fu

    University of Wyoming

  • Jifa Tian

    University of Wyoming

  • Piumi I Samarawickrama

    University of Wyoming

  • John Ackerman

    Department of Chemical Engineering, University of Wyoming & Resonance Sciences, Beaver Creek Oh, Department of Chemical Engineering, University of Wyoming, University of Wyoming, Department of Chemical Engineering, University of Wyoming

  • Wenyong Wang

    Department of Physics and Astronomy, University of Wyoming, University of Wyoming

  • Kenji Watanabe

    National Institute for Materials Science, Research Center for Functional Materials, National Institute of Materials Science, Research Center for Functional Materials, National Institute for Materials Science, 1-1 Namiki, Tsukuba 305-044, Japan, NIMS, Research Center for Functional Materials, National Institute for Materials Science, National Institute for Materials Science, Japan, Research Center for Functional Materials, National Institute for Materials Science, Tsukuba, Japan, NIMS Japan

  • Takashi Taniguchi

    National Institute for Materials Science, Kyoto Univ, International Center for Materials Nanoarchitectonics, National Institute of Materials Science, Kyoto University, International Center for Materials Nanoarchitectonics, National Institute for Materials Science, 1-1 Namiki, Tsukuba 305-044, Japan, International Center for Materials Nanoarchitectonics, National Institute for Materials Science, National Institute for Materials Science, Japan, National Institute For Materials Science, NIMS, National Institute for Material Science, International Center for Materials Nanoarchitectonics, National Institute for Materials Science, Tsukuba, Japan, NIMS Japan