| Home > Publications database > Paradoxical Topological Soliton Lattice in Anisotropic Frustrated Chiral Magnets |
| Typ | Amount | VAT | Currency | Share | Status | Cost centre |
| APC | 3000.00 | 0.00 | EUR | 66.49 % | (Zahlung erfolgt) | ZB |
| APC | 1512.00 | 0.00 | EUR | 33.51 % | (Zahlung erfolgt) | 57210 |
| Sum | 4512.00 | 0.00 | EUR | |||
| Total | 4512.00 |
| Journal Article | FZJ-2026-01803 |
; ;
2026
Wiley-VCH
Weinheim
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Please use a persistent id in citations: doi:10.1002/advs.202514568 doi:10.34734/FZJ-2026-01803
Abstract: Two-dimensional chiral magnets are known to host avariety of skyrmions, characterized by an integer topological charge (Q ∈ Z). However, these systems typically favor uniform lattices as a thermodynamically stable phase composed of either skyrmions (Q = −1) or antiskyrmions (Q = 1). In isotropic chiral magnets, skyrmion-antiskyrmion coexistence is typically transient due to mutual annihilation, making the observation of a stable, long-range ordered lattice a significant challenge. Here, we address this challenge by demon-strating a skyrmion-antiskyrmion lattice as a magnetic field-induced topological ground state in chiral magnets with competing anisotropic interactions, specifically Dzyaloshinskii-Moriya and frustrated exchange interactions. This unique lattice exhibits a net-zero global topological charge due to the balanced populations of skyrmions and antiskyrmions. Furthermore, density functional theory and spin-lattice simulations identify 2Fe/InSb(110) as an ideal candidate material for realizing this phase. This finding reveals new possibilities for manipulating magnetic solitons and establishes anisotropic frustrated chiral magnets as a promising material class for future spintronic applications.
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