2017
DOI: 10.1103/physrevb.95.134415
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Spin-wave dynamics in the helimagnet FeGe studied by small-angle neutron scattering

Abstract: We have studied the spin-wave stiffness of the Dzyaloshinskii-Moriya helimagnet FeGe in a temperature range from 225 K up to TC ≈ 278.7 K by small-angle neutron scattering. The method we have used is based on [S. V. Grigoriev et al. Phys. Rev. B 92 220415(R) (2015)] and was extended here for the application in polycrystalline samples. We confirm the validity of the anisotropic spin-wave dispersion for FeGe caused by the Dzyaloshinskii-Moriya interaction. We have shown that the spinwave stiffness A for FeGe hel… Show more

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Cited by 24 publications
(17 citation statements)
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“…2c. This vector lies in the plane of the lamella along a preferred axis determined by the present cubic anisotropy 20 . Upon application of an out-of-plane magnetic field, the SkL state is formed, illustrated in Fig.…”
mentioning
confidence: 83%
“…2c. This vector lies in the plane of the lamella along a preferred axis determined by the present cubic anisotropy 20 . Upon application of an out-of-plane magnetic field, the SkL state is formed, illustrated in Fig.…”
mentioning
confidence: 83%
“…FeGe also has the closest lattice match to Si [111] substrate and it can be grown by magnetron sputtering for a scalable fabrication of relevant applications. 22,24,26 While FeGe has been the object of great interest in recent imaging, transport, and neutron scattering experiments, 9,10,25,27,28 the spin dynamics of its many magnetic phases are relatively unexplored.The single crystal of B20 FeGe was grown by chemical vapor transport as described by Richardson. 29 We determined the structure and crystallographic orientation of a millimetersized, pyramid-shaped B20 FeGe crystal using Laue X-ray diffraction prior to MAS experiments (see Fig.…”
mentioning
confidence: 99%
“…Однако величина зависящего от температуры параметра межмодового взаимодействия, определяется электронной структурой, параметрами межэлектронного взаимодействия и магнитными моментами основного состояния, которые окончательно не определены. Спиновые корреляции в окрестности T C , которые приводят к возникновению области киральных флуктуаций [6,9] и к их кроссоверу с ферромагнитными флуктуациями, исследованы недостаточно. Не рассмотрен вопрос о возможной аномалии температурной зависимости неоднородной магнитной восприимчивости при переходе в парамагнитное состояние.…”
Section: Introductionunclassified