2007
DOI: 10.1134/s1063783407100162
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Spin-wave resonance in a tangentially magnetized thin film

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Cited by 4 publications
(7 citation statements)
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“…98,100 In Ref. 94,98,106, the case of a significant interface anisotropy [115][116][117][118][119][120][121][122][123] was also accounted for, leading to the following form of the Barnaś-Mills boundary conditions 98,100 used in our calculations…”
Section: Introductionmentioning
confidence: 99%
“…98,100 In Ref. 94,98,106, the case of a significant interface anisotropy [115][116][117][118][119][120][121][122][123] was also accounted for, leading to the following form of the Barnaś-Mills boundary conditions 98,100 used in our calculations…”
Section: Introductionmentioning
confidence: 99%
“…However, in the ferromagnetic thin films, the D-E mode with 𝑞 ∥ = 0 is the ferromagnetic resonance (FMR) mode with a uniform distribution of the variable magnetization m through the thickness and in-plane direction of the film. This case corresponds to unpinning boundary conditions on both surfaces of thin films 42,43 . One should note that because of the limited numerical aperture of the focusing lens, all D-E modes with larger in-plane wavevectors contribute to the light scattering, which result in a continuous background spectrum (see Figure 3).…”
mentioning
confidence: 99%
“…is the sum of the external magnetic field 𝐻 0 and the anisotropy magnetic field 𝐻 𝑎 , 𝑞 is the wavevector of PSSW mode, and 4𝜋𝑀 0 = 2640 G −1 is the saturation magnetization of the film, respectively. The wave vectors of the spatially confined PSSW modes, 𝑞 𝑛 , are defined from the Landau-Lifshitz-Gilbert equation for the precession motion of the magnetization m with the following boundary conditions 42,43 :…”
mentioning
confidence: 99%
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