Hopfion rings in a cubic chiral magnet
Magnetic skyrmions and hopfions are topological solitons 1 —well-localized field configurations that have gained considerable attention over the past decade owing to their unique particle-like properties, which make them promising objects for spintronic applications. Skyrmions 2 , 3 are two-dimensio...
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Veröffentlicht in: | Nature (London) 2023-11, Vol.623 (7988), p.718-723 |
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Sprache: | eng |
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Zusammenfassung: | Magnetic skyrmions and hopfions are topological solitons
1
—well-localized field configurations that have gained considerable attention over the past decade owing to their unique particle-like properties, which make them promising objects for spintronic applications. Skyrmions
2
,
3
are two-dimensional solitons resembling vortex-like string structures that can penetrate an entire sample. Hopfions
4
–
9
are three-dimensional solitons confined within a magnetic sample volume and can be considered as closed twisted skyrmion strings that take the shape of a ring in the simplest case. Despite extensive research on magnetic skyrmions, the direct observation of magnetic hopfions is challenging
10
and has only been reported in a synthetic material
11
. Here we present direct observations of hopfions in crystals. In our experiment, we use transmission electron microscopy to observe hopfions forming coupled states with skyrmion strings in B20-type FeGe plates. We provide a protocol for nucleating such hopfion rings, which we verify using Lorentz imaging and electron holography. Our results are highly reproducible and in full agreement with micromagnetic simulations. We provide a unified skyrmion–hopfion homotopy classification and offer insight into the diversity of topological solitons in three-dimensional chiral magnets.
Transmission electron microscopy is used to observe three-dimensional topological solitons known as hopfions that in a chiral magnet are found to form rings around skyrmion strings, and a nucleation protocol for these rings is provided. |
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ISSN: | 0028-0836 1476-4687 1476-4687 |
DOI: | 10.1038/s41586-023-06658-5 |