Advanced Magnetic Materials [mtls sci] by L. Malkinski

By L. Malkinski

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The line shows theoretical FMR fields based on Eq. (2) and the Ha and 4Ms 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 4Ms values obtained from the hysteresis loop measurements. (4) The FMR frequency-field curve 43 M-Type Barium Hexagonal Ferrite Films 4M (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.

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