Abstract

The magnetic relaxation of the disordered exchange interacting random anisotropy systems is investigated based on the Monte Carlo method. Similar to the dipolar interacting systems [M. Ulrich, J. García-Otero, J. Rivas, A. Bunde, Phys. Rev. B 67 (2003) 024416], the logarithmic relaxation rate decays by a universal power law, W ( t ) = A t − n . The exponent n increases monotonically with the decreasing temperature as well as the increasing exchange interaction. Depending on the value of n , short-range ferromagnetic correlations (or spin-glass-like behaviour) and superferromagnetic order are suggested.

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