Titlebook: Crystal Field Effects in Metals and Alloys; A. Furrer Book 1977 Plenum Press, New York 1977 Holmium.Praseodym.Terbium.Ytterbium.cobalt.cry

背書(shū)

Spin Dynamics of the S = 2 Magnet in a Cubic Crystal Fieldtric; consequently the two modes are strongly mixed at long wavelengths and the low frequency response may be expressed in Debye form with a relaxation time that diverges at T.. Results are in agreement with dynamic susceptibility theories of Buyers and Lines.

Metastasis

恭維

https://doi.org/10.1007/BFb0011851al-field and the effects of bilinear and quadrupolar pair interactions. At U.2 K excitedstate spin waves have been observed which correspond to transitions from the upper member of the ground-state doublet Γ... The stability of the unusual flopside spin structure is discussed.

FER

胰島素

暗諷

A. Bertoni,G. Mauri,N. Sabadinior the axial crystal field parameter D = 3B.: . and the isothermal g-factors: . Sc:Gd is strongly bottlenecked, leading to an anormal angular dependence of the resonance field, which is explained in terms of available theories.

infatuation

Exterior

Gene Cooperman,G. Michler,H. Vinckansition in TbSb should be of first order, since the Hamiltonian shows no stable fixed point within the ε-expansion. In pure TbSb we find the critical exponent β = 0.20±0.01 in the region 4×10. < (T.-T)/T.<2×10.. In Tb.Y.Sb the exponent is significantly different, we find a sharp transition with β = 0.37±0.05.

皺痕

Lecture Notes in Earth Scienceslectrons. The problem of beginning with a very basic Hamiltonian, and recasting it to show localized moments and conduction properties is considered using degenerate perturbation theory. The result is a spin-Hamiltonian of typical form for the localized moments, with conduction electrons as well. At

Mri485