J.H. Spreen, B.E. Argyle
Journal of Applied Physics
Thermal expansivity and magnetostriction of an EuO single crystal were determined by using the strain gauge method in the temperature ranges 20°to 250°K and 4.2°to 150°K, respectively, and in magnetic fields up to 20 kOe. The magnetoelastic component of expansivity αme is observed to be proportional to the magnetic specific heat Cm. 1 As a result we obtain a temperature independent "magnetic" Grüneisen constant ∂ ln Um/∂ ln V=[minus]5.3 given by -3αmeCm-1B T using BT (isothermal bulk modulus) =1.07×10 12 dyn/cm2. For Um, the internal magnetic energy, we derive also the variation with temperature and magnetic field U m(T, H)/Um(0), the variation with pressure ∂ ln Um/∂ P=4.9×10-12 dyn-1cm 2, and the value Um(0) = -4.9×108 erg·cm-3 at 0°K. These results are obtained from treating various combinations of measurables including magnetization, isotropic forced magnetostriction, and zero-temperature volume anomaly as well as αme and Cm. The manner of suppression of the λ-transition by a magnetic field is also revealed by the data. Linear magnetostriction coefficients extrapolated to 0°K are λ 100=-22×10-6 and λ111= 55×10-6. Their decrease with increasing temperature is explained by a 1:1 admixture of single-ion and two-ion magnetoelastic coupling as described by λ(T)=·λ(0){Î5/2[L -1(m)]} and λ(T)=·λ(0)m2, respectively.2 © 1967 The American Institute of Physics.
J.H. Spreen, B.E. Argyle
Journal of Applied Physics
M.W. Shafer, T.R. McGuire, et al.
Applied Physics Letters
P.L. Trouilloud, B. Petek, et al.
IEEE Transactions on Magnetics
W. Jantz, B.E. Argyle, et al.
Journal of Magnetism and Magnetic Materials