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| Hauptseite > Publikationsdatenbank > Magnon spectrum of the helimagnetic insulator Cu$_{2}$OSeO$_{3}$ > print |
| Hauptseite > Publikationsdatenbank > Magnon spectrum of the helimagnetic insulator Cu$_{2}$OSeO$_{3}$ > print |
| 001 | 283357 | ||
| 005 | 20210129222300.0 | ||
| 024 | 7 | _ | |a 10.1038/ncomms10725 |2 doi |
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| 100 | 1 | _ | |a Portnichenko, P. Y. |0 P:(DE-HGF)0 |b 0 |
| 245 | _ | _ | |a Magnon spectrum of the helimagnetic insulator Cu$_{2}$OSeO$_{3}$ |
| 260 | _ | _ | |a London |c 2016 |b Nature Publishing Group |
| 336 | 7 | _ | |a article |2 DRIVER |
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| 520 | _ | _ | |a Complex low-temperature-ordered states in chiral magnets are typically governed by acompetition between multiple magnetic interactions. The chiral-lattice multiferroic Cu2OSeO3became the first insulating helimagnetic material in which a long-range order of topologicallystable spin vortices known as skyrmions was established. Here we employ state-of-the-artinelastic neutron scattering to comprehend the full three-dimensional spin-excitation spectrumof Cu2OSeO3 over a broad range of energies. Distinct types of high- and low-energydispersive magnon modes separated by an extensive energy gap are observed in excellentagreement with the previously suggested microscopic theory based on a model of entangledCu4 tetrahedra. The comparison of our neutron spectroscopy data with model spin-dynamicalcalculations based on these theoretical proposals enables an accurate quantitative verificationof the fundamental magnetic interactions in Cu2OSeO3 that are essential for understandingits abundant low-temperature magnetically ordered phases. |
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| 700 | 1 | _ | |a Inosov, D. S. |0 P:(DE-HGF)0 |b 13 |e Corresponding author |
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