2020
DOI: 10.1103/physrevb.102.144422
|View full text |Cite
|
Sign up to set email alerts
|

Magnetic skyrmions, chiral kinks, and holomorphic functions

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1

Citation Types

6
52
0
5

Year Published

2021
2021
2024
2024

Publication Types

Select...
9

Relationship

0
9

Authors

Journals

citations
Cited by 63 publications
(63 citation statements)
references
References 27 publications
6
52
0
5
Order By: Relevance
“…This class of solutions has skyrmions acting as noninteracting particles with the energy of 4π each. A diverse array of multi-skyrmion configurations was constructed analytically and confirmed numerically [25]. The absolute ground states of the model are, unfortunately, not among these special states.…”
Section: Historical Notementioning
confidence: 86%
“…This class of solutions has skyrmions acting as noninteracting particles with the energy of 4π each. A diverse array of multi-skyrmion configurations was constructed analytically and confirmed numerically [25]. The absolute ground states of the model are, unfortunately, not among these special states.…”
Section: Historical Notementioning
confidence: 86%
“…It had been theoretically proposed in chiral magnets that the skyrmions, antiskyrmions, and other magnetic configurations can be naturally interpreted in terms of chiral kinks. These kinks carry a topological charge and allow to construct new topological particle-like states [15,31,32]. In addition, the previous studies demonstrated that some special magnetic textures often appear in the corners of the polygon geometries like triangles, squares, rectangles, in which the corners may also act as pinning sites for the domain wall motion [33][34][35][36].…”
Section: Introductionmentioning
confidence: 97%
“…Generally, the presence of edges and corners in nanostructures can be utilized to tailor the magnetic textures and modify their dynamics behaviors. For the skyrmion confined in ultrathin film nanostructures with Dzyaloshinskii-Moriya (DM) interaction, the boundary constrictions naturally make the magnetization orientation undergo the 180°rotation at the edges, forming the so-called kink or π domain wall configurations [2,15,[29][30][31][32]. Depending on the crystal symmetry of chiral magnets, two distinct types of chiral kinks, namely, Néel-type and Blochtype kinks, are favorable in interfacial and bulk DM interaction systems respectively [29,30].…”
Section: Introductionmentioning
confidence: 99%
“…Loosely speaking, topological stability does not imply energetic stability, as topologically distinct vacua are always separated by finite action barriers 5. For a recent discussion of stable soliton solutions of arbitrary topological charge in chiral magnets, see[50][51][52] 6. In principle, this would work similar to the previous section, by adding the Hopf charge to the loss function, L = S + λ H (H − H 0 ) 2 .…”
mentioning
confidence: 95%