Higher-order modulations in the skyrmion-lattice phase of CuOSeO
arXiv:2204.08614 · doi:10.1103/PhysRevB.106.104406
Abstract
Using small angle neutron scattering, we have investigated higher-order peaks in the skyrmion-lattice phase of CuOSeO, in which two different skyrmion lattices, SkX1 and SkX2, are known to form. For each skyrmion-lattice phase, we observed two sets of symmetrically inequivalent peaks at the higher-order-reflection positions with the indices and . Under the condition where the SkX1 and SkX2 coexist, we confirmed the absence of the scattering at positions combining reflections from the two phases, indicating a significantly weak double-scattering component. Detailed analysis of the peak profile, as well as the temperature and magnetic-field dependence of the peak intensity, also supports the intrinsic higher-order modulation rather than the parasitic double scattering. The two higher-order modulations show contrasting magnetic-field dependence; the former increases as the field is increased, whereas the latter decreases. This indicates that, in CuOSeO, skyrmions are weakly distorted, and the distortion is field-dependent in a way that the dominant higher-order modulation switches from to under field. Monte Carlo simulations under sweeping external magnetic field qualitatively reproduce the observed magnetic-field dependence, and suggests that the higher-order modulations correspond to the superlattices of weak swirlings appearing in the middle of the original triangular-latticed skyrmions.
13 pages, 14 figures
References in corpus (6)
- Advances in the Physics of Magnetic Skyrmions and Perspective for Technology
- Skyrmion Hall Effect Revealed by Direct Time-Resolved X-Ray Microscopy
- A new class of chiral materials hosting magnetic skyrmions beyond room temperature
- Long wavelength helimagnetic order and skyrmion lattice phase in Cu2OSeO3
- Skyrmions and Anomalous Hall Effect in a Dzyloshinskii-Moriya Spiral Magnet
- Formation and rotation of skyrmion crystal in the chiral-lattice insulator Cu2OSeO3