Abstract:
The longitudinal magnetic susceptibility of quasi-three-dimensional easy-axis ferromagnets has been found. In this case, the ferromagnetic structure is considered as a fractal object with the dimension $D$ = 3–$\varepsilon$, where $\varepsilon>$ 0. The approach is based on using a quasi-classical kinetic equation. The magnon dispersion strictly calculated using operations of the fractal differentiation is a strongly anisotropic (dependent on the parameter $\varepsilon$) function of angular variables, which leads to nontrivial frequency dependences of the magnetic susceptibility.