Field dependence of non-reciprocal magnons in chiral MnSi
arXiv:1708.02098 · doi:10.1103/PhysRevB.97.224403
Abstract
Spin waves in chiral magnetic materials are strongly influenced by the Dzyaloshinskii-Moriya interaction resulting in intriguing phenomena like non-reciprocal magnon propagation and magnetochiral dichroism. Here, we study the non-reciprocal magnon spectrum of the archetypical chiral magnet MnSi and its evolution as a function of magnetic field covering the field-polarized and conical helix phase. Using inelastic neutron scattering, the magnon energies and their spectral weights are determined quantitatively after deconvolution with the instrumental resolution. In the field-polarized phase the imaginary part of the dynamical susceptibility is shown to be asymmetric with respect to wavevectors longitudinal to the applied magnetic field , which is a hallmark of chiral magnetism. In the helimagnetic phase, becomes increasingly symmetric with decreasing due to the formation of helimagnon bands and the activation of additional spinflip and non-spinflip scattering channels. The neutron spectra are in excellent quantitative agreement with the low-energy theory of cubic chiral magnets with a single fitting parameter being the damping rate of spin waves.
arXiv commentPaper: 10 pages, 5 figures Supplement: 8 pages, 11 figures
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- Spin excitation spectra in helimagnetic states: proper-screw, cycloid, vortex crystal, and hedgehog lattice
- Skyrmion crystals in centrosymmetric triangular magnets under hexagonal and trigonal single-ion anisotropy
- Kelvin modes of a skyrmion line in chiral magnets and the associated magnon transport
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- Frustration model and spin excitations in the helimagnet FeP
- Non-reciprocal magnons in non-centrosymmetric MnSi
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- Nonreciprocal magnon excitations by the Dzyaloshinskii-Moriya interaction on the basis of bond magnetic toroidal multipoles