Abstract
Temperature dependences of the paramagnetic resonance line-widths ΔH of ferrimagnetic (very nearly ferromagnetic) RbNiF3 and antiferromagnetic RbMnF3 have been observed in order to investigated the dynamics of the spin fluctuation near the critical points. Reflecting the importance of the anisotropy energy, by which the damping of K=0 transverse mode is influenced, no anomalous increase in widths occurs in isotropic antiferromagnet RbMnF3 on passing through the critical point. But in the case of uniaxial ferrimagnet RbNiF3, great narrowing of the width occurs with decreasing temperatures. The width is minimum at (1.025∼1.035)Tc and increases slightly with further decreasing temperatures. The product ΔH·x⊥, where x⊥ is the perpendicular susceptibilty, shows almost exactly the same temperature variation as that of MnF2 with the critical exponent −2⁄3, supporting the theory of Mori and Kawasaki pretty well.