Abstract

AbstractThe magnetic phase transition is investigated by a vibration magnetometer for the homogeneous ferrimagnet Fe3O4 and the structurally disordered ferrites ZnxNi1−xFe2O4 with x = 0, 0.25, 0.5, and 0.75. For both ordered and disordered ferrimagnets the asymptotic critical exponents are compatible with the ones of a homogeneous 3d‐Heisenberg ferromagnet. Outside the asymptotic critical regime there is a strong effect of the structural inhomogeneities on the thermodynamic behaviour. In close analogy to the case of disordered ferromagnets, the effective Kouvel‐Fisher exponent γ(T) first increases with increasing temperature T for disordered systems, as predicted by the correlated molecular field theory and by Monte Carlo computer simulations, whereas it initially decreases for a homogeneous ferrimagnet. Anomalies in the modified Arrott plots at low fields are discussed.

Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call