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Magnon spectrum of the helimagnetic insulator Cu(2)OSeO(3)

Complex low-temperature-ordered states in chiral magnets are typically governed by a competition between multiple magnetic interactions. The chiral-lattice multiferroic Cu(2)OSeO(3) became the first insulating helimagnetic material in which a long-range order of topologically stable spin vortices kn...

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Detalles Bibliográficos
Autores principales: Portnichenko, P. Y., Romhányi, J., Onykiienko, Y. A., Henschel, A., Schmidt, M., Cameron, A. S., Surmach, M. A., Lim, J. A., Park, J. T., Schneidewind, A., Abernathy, D. L., Rosner, H., van den Brink, Jeroen, Inosov, D. S.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2016
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4773425/
https://www.ncbi.nlm.nih.gov/pubmed/26911567
http://dx.doi.org/10.1038/ncomms10725
Descripción
Sumario:Complex low-temperature-ordered states in chiral magnets are typically governed by a competition between multiple magnetic interactions. The chiral-lattice multiferroic Cu(2)OSeO(3) became the first insulating helimagnetic material in which a long-range order of topologically stable spin vortices known as skyrmions was established. Here we employ state-of-the-art inelastic neutron scattering to comprehend the full three-dimensional spin-excitation spectrum of Cu(2)OSeO(3) over a broad range of energies. Distinct types of high- and low-energy dispersive magnon modes separated by an extensive energy gap are observed in excellent agreement with the previously suggested microscopic theory based on a model of entangled Cu(4) tetrahedra. The comparison of our neutron spectroscopy data with model spin-dynamical calculations based on these theoretical proposals enables an accurate quantitative verification of the fundamental magnetic interactions in Cu(2)OSeO(3) that are essential for understanding its abundant low-temperature magnetically ordered phases.