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Abstract
A magnetic bimeron is an in-plane topological counterpart of a magnetic skyrmion. Despite the topological equivalence, their statics and dynamics could be distinct, making them attractive from the perspectives of both physics and spintronic applications. In this work, we demonstrate the stabilization of bimeron solitons and clusters in the antiferromagnetic (AFM) thin film with interfacial Dzyaloshinskii–Moriya interaction (DMI). Bimerons demonstrate high current-driven mobility as generic AFM solitons, while featuring anisotropic and relativistic dynamics excited by currents with in-plane and out-of-plane polarizations, respectively. Moreover, these spin textures can absorb other bimeron solitons or clusters along the translational direction to acquire a wide range of Néel topological numbers. The clustering involves the rearrangement of topological structures, and gives rise to remarkable changes in static and dynamical properties. The merits of AFM bimeron clusters reveal a potential path to unify multibit data creation, transmission, storage, and even topology-based computation within the same material system, and may stimulate spintronic devices enabling innovative paradigms of data manipulations.
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1 The Chinese University of Hong Kong, School of Science and Engineering, Shenzhen, China (GRID:grid.10784.3a) (ISNI:0000 0004 1937 0482); University of Science and Technology of China, Hefei National Laboratory for Physical Sciences at the Microscale, Department of Physics, Hefei, China (GRID:grid.59053.3a) (ISNI:0000000121679639)
2 The Chinese University of Hong Kong, School of Science and Engineering, Shenzhen, China (GRID:grid.10784.3a) (ISNI:0000 0004 1937 0482)
3 Research Institute of Materials Science of Shanxi Normal University & Collaborative Innovation Center for Shanxi Advanced Permanent Magnetic Materials and Technology, Linfen, China (GRID:grid.10784.3a); Shanxi Normal University, School of Physics and Electronic Information, Linfen, China (GRID:grid.412498.2) (ISNI:0000 0004 1759 8395)
4 University of York, Department of Physics, York, UK (GRID:grid.5685.e) (ISNI:0000 0004 1936 9668); Nanjing University, York-Nanjing International Center of Spintronics (YNICS), Nanjing, China (GRID:grid.41156.37) (ISNI:0000 0001 2314 964X)
5 The Chinese University of Hong Kong, School of Science and Engineering, Shenzhen, China (GRID:grid.10784.3a) (ISNI:0000 0004 1937 0482); Nanjing University, York-Nanjing International Center of Spintronics (YNICS), Nanjing, China (GRID:grid.41156.37) (ISNI:0000 0001 2314 964X)
6 The University of Tokyo, Department of Applied Physics, Tokyo, Japan (GRID:grid.26999.3d) (ISNI:0000 0001 2151 536X)
7 The University of New South Wales, School of Physics, Sydney, Australia (GRID:grid.1005.4) (ISNI:0000 0004 4902 0432); National University of Science and Technology ‘MISiS’, Moscow, Russia (GRID:grid.35043.31) (ISNI:0000 0001 0010 3972)
8 Research Institute of Materials Science of Shanxi Normal University & Collaborative Innovation Center for Shanxi Advanced Permanent Magnetic Materials and Technology, Linfen, China (GRID:grid.35043.31); School of Chemistry and Materials Science of Shanxi Normal University & Key Laboratory of Magnetic Molecules and Magnetic Information Materials of Ministry of Education, Linfen, China (GRID:grid.35043.31)
9 Slovak Academy of Sciences, Institute of Electrical Engineering, Bratislava, Slovakia (GRID:grid.419303.c) (ISNI:0000 0001 2180 9405); Slovak Academy of Sciences, Centre for Advanced Materials Application CEMEA, Bratislava, Slovakia (GRID:grid.419303.c) (ISNI:0000 0001 2180 9405)
10 Adam Mickiewicz University in Poznan, Faculty of Physics, Poznan, Poland (GRID:grid.5633.3) (ISNI:0000 0001 2097 3545)
11 University of York, Department of Physics, York, UK (GRID:grid.5685.e) (ISNI:0000 0004 1936 9668)