Abstract

Periodic 3G lattices made of oriented magnetic nanowires are considered under the magnetic resonance in the millimeter-wavelength range. The propagation of electromagnetic waves in anisotropic nanostructured materials based on these lattices is mathematically modeled using the method of autonomous blocks with virtual Floquet channels. The real and imaginary parts of propagation coefficients of longitudinal (clockwiseand counterclockwise polarized) and transverse (ordinary and extraordinary) waves for the zero spatial harmonic of 26 GHz are electrodynamically calculated. These waves propagate in 3D lattices of magnetic (Co80Ni20, Fe) nanowires. The obtained results depend on the intensity of the external constant magnetic field and the lattice period. The methods of control of the frequency dispersion in the millimeter-wavelength range under the influence of the external magnetic field and under the change of the geometry of lattices are determined. It is considered that the direction and intensity of the magnetic bias, its orientation with respect to the nanowire axis, and the mutual orientation of the constant and high-frequency magnetic fields vary.

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