2020
DOI: 10.1103/physrevapplied.13.054038
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Anomalous Refraction of Spin Waves as a Way to Guide Signals in Curved Magnonic Multimode Waveguides

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Cited by 21 publications
(17 citation statements)
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“…Moreover, the assumed field vari-ation of 0.1 T over 10 μm length scales is also quantitatively challenging to implement, although the strong demagnetizing fields in patterned magnetic structures [19,20] and the stray field from the magnetic tip in FMRFM [26] suggest realistic ways forward. Yet, as with spin-wave Bloch oscillations [67], the effects described here are not restricted to graded magnetic fields [68] but could be generalized to other magnonic media with spatially varying characteristics, produced using the toolbox of graded index magnonics [69,70]. For instance, we note the two recent papers, which appeared while our paper was in review, studying spin-wave nonreciprocity in media with graded exchange [71] and magnetization [72].…”
Section: Discussionmentioning
confidence: 92%
“…Moreover, the assumed field vari-ation of 0.1 T over 10 μm length scales is also quantitatively challenging to implement, although the strong demagnetizing fields in patterned magnetic structures [19,20] and the stray field from the magnetic tip in FMRFM [26] suggest realistic ways forward. Yet, as with spin-wave Bloch oscillations [67], the effects described here are not restricted to graded magnetic fields [68] but could be generalized to other magnonic media with spatially varying characteristics, produced using the toolbox of graded index magnonics [69,70]. For instance, we note the two recent papers, which appeared while our paper was in review, studying spin-wave nonreciprocity in media with graded exchange [71] and magnetization [72].…”
Section: Discussionmentioning
confidence: 92%
“…However, a translation symmetry break or a curved waveguide can convert symmetric into antisymmetric modes during wave propagation. [35][36][37] Here, the width of the signal line is much larger compared to the waveguide width, thus, the distribution of the RF field B CW can be assumed homogeneous across the lateral dimension. Nevertheless, the mode profile of k 2 reveals direct excitation of the antisymmetric mode n = 2 with a phase shift of Δφ = π. k 1a and k 1b show the expected symmetric mode profiles.…”
Section: Resultsmentioning
confidence: 99%
“…(4.6) or Ref. 40). The appearance of the phase ψ in the resonance conditions is related to the additional phase shift, which is acquired by an SW reflected from a boundary due to a nonzero polarization mismatch.…”
Section: B Finite Region With Different Sw Dispersion and Polarizationmentioning
confidence: 99%
“…Starting from seminal work by Rado and Weertman 28 there were many research interest to the boundary conditions at the ferromagnet interface, including study of the effect of magnetoelastic interaction 29 , finite width and diffusive character of interfaces [30][31][32] , nonuniform dipolar fields 33,34 , Dzyaloshinski-Moriya interaction 35 , magnetic anisotropy of interface 36,37 , etc. The problem of the SW reflection from a sharp boundary was studied in details for exchange-dominated SWs in isotropic, uniaxial and biaxial anisotropic ferromagnets [38][39][40] . The case of smooth interface was studied for both dipolar 6,7 and exchange-dominated SWs 30,31 .…”
Section: Introductionmentioning
confidence: 99%