Magnetostriction of Dilute Magnetic Alloys

Abstract
Measurements of the magnetostriction and magnetization of two ferromagnetic PtFe alloys and a paramagnetic PdNi alloy are presented. The Belov equation for the free energy of a weak itinerant ferromagnet including magnetoelastic terms is used to estimate the volume dependence of the Curie temperature TC. For the alloy Pt0.99 Fe0.01, the resultant value is lnTCω=47, where ω, is the volume strain. The volume dependence of the magnetization M, determined from the magnetostriction, is field dependent and decreases monotonically from lnMω=1.6 at 35 kOe to lnMω=37 at 2 kOe, where it is still decreasing rapidly. This behavior is in disagreement with the sd interaction model, which was found to explain satisfactorily the behavior of PdFe alloys. The model predicts that lnMω should be field independent and of the same order of magnitude as lnTCω. In the alloy Pt0.97 Fe0.03, it is not possible to estimate lnTCω from the Belov plots, because of domain effects. The value of lnMω is constant and equal to - 0.5 above about 15 kOe, but increases considerably at lower fields, as in Pt0.99 Fe0.01, before domain effects intervene. The Belov equation is modified to describe the magnetostriction and magnetization of the paramagnetic alloy Pd0.9811 Ni0.0189, and thereby to estimate the value, lnχAω=19, of the volume dependence of its susceptibility χA. The Belov equation and its modification for a strongly paramagnetic metal describe satisfactorily the field dependence of the magnetostriction, but not the magnetization, both for the ferromagnetic PtFe alloys and the PdNi alloy.

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