Abstract
Critical behavior in La 0.7Pb 0.05Na 0.25MnO 3 has been investigated by dc magnetization measurements. Magnetic data indicate that the compound exhibits a continuous (second-order) paramagnetic (PM) to ferromagnetic (FM) phase transition. Estimates of critical exponents yield δ = 4.80 ± 0.01 , γ = 1.296 ± 0.002 and β = 0.344 ± 0.007 (consistent with both the predictions for the three-dimensional-Heisenberg model and with those reported for materials when the FM transition is ascribed to the double exchange (DE) mechanism as a major origin) with T C = 334.54 ± 0.08 . The critical exponent γ is slightly inferior than predicted from the 3D Heisenberg model. Such a difference may be due, within the context of the quenched disorder, to the presence of some alterations of short-range magnetic order of FM clusters in the PM phase. The temperature variation in the effective exponent ( γ e f f ) is similar to those for disordered ferromagnets.
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