2020
DOI: 10.1103/physrevb.102.054419
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Dynamics of antiferromagnetic skyrmions in the absence or presence of pinning defects

Abstract: A theoretical study on the dynamics of an antiferromagnetic (AFM) skyrmion is indispensable for revealing the underlying physics and understanding the numerical and experimental observations. In this work, we present a reliable theoretical treatment of the spincurrent induced motion of an AFM skyrmion in the absence and presence of pinning defect. For an ideal AFM system free of defect, the skyrmion motion velocity as a function of the intrinsic parameters can be derived, based on the concept that the skyrmion… Show more

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Cited by 24 publications
(8 citation statements)
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References 54 publications
(66 reference statements)
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“…Moreover, the calculated skyrmion radii are also given to help one to understand the results easier. The same as our earlier theoretical calculations, the radius is increased with the increase of D [33,34]. On one hand, the interacting area between the spin wave and skyrmion is enlarged [35], resulting in the increase of interacting force and skyrmion speed.…”
Section: Resultssupporting
confidence: 83%
“…Moreover, the calculated skyrmion radii are also given to help one to understand the results easier. The same as our earlier theoretical calculations, the radius is increased with the increase of D [33,34]. On one hand, the interacting area between the spin wave and skyrmion is enlarged [35], resulting in the increase of interacting force and skyrmion speed.…”
Section: Resultssupporting
confidence: 83%
“…Similar to the earlier work [38], we study a two-dimensional AFM model in the xy-plane with two magnetic sublattices that have magnetic moments m1 and m2 respectively, satisfying condition |m1| = |m2| = S with spin length S. The normalized staggered Néel vector n is defined as n = (m1  m2)/2S [39] to describe the Lagrangian. Taking into account the exchange energy, the anisotropy energy, and the interfacial DMI as well, one has the Lagrangian density L given by [40]:…”
Section: Model and Methodsmentioning
confidence: 99%
“…In the ground state, the 2D AFM layer consists of two coupled sub-lattices (A) and (B) that are completely polarized to each other. The 2D topological soliton (AFM skyrmion) can also be nucleated, moved, and converted into an AFM DW pair in AFM systems 21,23 either by STTs, SOTs, or spin waves [24][25][26] as the FM skyrmion. Furthermore, the processing speed of AFM skyrmion is much higher than that of FM skyrmion 23 .…”
Section: Nucleation and Manipulation Of Single Skyrmions Using Spin-p...mentioning
confidence: 99%