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Abstract
Two-dimensional arrays of magnetically coupled nanomagnets provide a mesoscopic platform for exploring collective phenomena as well as realizing a broad range of spintronic devices. In particular, the magnetic coupling plays a critical role in determining the nature of the cooperative behavior and providing new functionalities in nanomagnet-based devices. Here, we create coupled Ising-like nanomagnets in which the coupling between adjacent nanomagnetic regions can be reversibly converted between parallel and antiparallel through solid-state ionic gating. This is achieved with the voltage-control of the magnetic anisotropy in a nanosized region where the symmetric exchange interaction favors parallel alignment and the antisymmetric exchange interaction, namely the Dzyaloshinskii-Moriya interaction, favors antiparallel alignment of the nanomagnet magnetizations. Applying this concept to a two-dimensional lattice, we demonstrate a voltage-controlled phase transition in artificial spin ices. Furthermore, we achieve an addressable control of the individual couplings and realize an electrically programmable Ising network, which opens up new avenues to design nanomagnet-based logic devices and neuromorphic computers.
Arranging nanomagnets into a two-dimensional lattice provides access to a rich landscape of magnetic behaviours. Control of the interactions between the nanomagnets after fabrication is a challenge. Here, Yun et al demonstrate all-electrical control of magnetic couplings in a two-dimensional array of nanomagnets using ionic gating.
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1 Peking University, State Key Laboratory of Artificial Microstructure and Mesoscopic Physics, School of Physics, Beijing, China (GRID:grid.11135.37) (ISNI:0000 0001 2256 9319); Peking University, School of Materials Science and Engineering, Beijing, China (GRID:grid.11135.37) (ISNI:0000 0001 2256 9319)
2 Peking University, State Key Laboratory of Artificial Microstructure and Mesoscopic Physics, School of Physics, Beijing, China (GRID:grid.11135.37) (ISNI:0000 0001 2256 9319)
3 ETH Zurich, Laboratory for Mesoscopic Systems, Department of Materials, Zurich, Switzerland (GRID:grid.5801.c) (ISNI:0000 0001 2156 2780); Paul Scherrer Institute, Laboratory for Multiscale Materials Experiments, Villigen PSI, Switzerland (GRID:grid.5991.4) (ISNI:0000 0001 1090 7501); ETH Zurich, Laboratory for Magnetism and Interface Physics, Department of Materials, Zurich, Switzerland (GRID:grid.5801.c) (ISNI:0000 0001 2156 2780)
4 ETH Zurich, Laboratory for Mesoscopic Systems, Department of Materials, Zurich, Switzerland (GRID:grid.5801.c) (ISNI:0000 0001 2156 2780); Paul Scherrer Institute, Laboratory for Multiscale Materials Experiments, Villigen PSI, Switzerland (GRID:grid.5991.4) (ISNI:0000 0001 1090 7501)
5 Massachusetts Institute of Technology, Department of Materials Science and Engineering, Cambridge, USA (GRID:grid.116068.8) (ISNI:0000 0001 2341 2786)
6 Central Iron and Steel Research Institute Group, Division of Functional Materials, Beijing, China (GRID:grid.454824.b) (ISNI:0000 0004 0632 3169)
7 Peking University, School of Materials Science and Engineering, Beijing, China (GRID:grid.11135.37) (ISNI:0000 0001 2256 9319)
8 ETH Zurich, Laboratory for Magnetism and Interface Physics, Department of Materials, Zurich, Switzerland (GRID:grid.5801.c) (ISNI:0000 0001 2156 2780)