By L. Malkinski
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The line shows theoretical FMR fields based on Eq. (2) and the Ha and 4Ms values cited above. These data show four results. (1) The film has a narrow FMR linewidth. 8,9 (2) There is a very good match between the experimental FMR profiles and the Lorentzian fits. (3) The theoretical FMR fields match nicely with the experimental values. This match confirms the Ha and 4Ms values obtained from the hysteresis loop measurements. (4) The FMR frequency-field curve 43 M-Type Barium Hexagonal Ferrite Films 4M (kG) 4 Easy axis 2 Ha -20 -10 0 Hard axis 10 20 H (kOe) -2 -4 Fig.
Ababei, G. -A. (2011b). Rapidly Solidified Amorphous Nanowires. ; Lupu, N. -A. (2011a). Magnetic Characterization of Submicron Wires and Nanowires Using Digital Integration Techniques. 10, (October 2011), pp. ; Chiriac, H. -A. (2011b). Accurate Measurement of Domain Wall Velocity in Amorphous Microwires, Submicron Wires, and Nanowires. ; Torres, L. & Azzerboni, B. (2010). Domain Wall Dynamics Driven by a Localized Injection of a Spin-Polarized Current. 6, (June 2010), pp. -X. & Vázquez, M. (2000).
The underlying physical effects in microwave magnetic devices include ferromagnetic resonance (FMR), magnetostatic wave (MSW) propagation, Faraday rotation, and field displacement. Whatever the basis for a given device, the operation frequency is determined essentially by the FMR frequency of the garnet material. The magnetic garnets are low-magnetization, low-magnetocrystalline-anisotropy materials and, therefore, typically have a low FMR frequency in the GHz range. This imposes an upper limit on the practical operation frequency of compact YIG-based devices in the 10-18 GHz frequency range.