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

羅盤(pán)

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Design strategies for VLSI logic,an Vleck and Langevin contributions to the susceptibility. In the paramagnetic phase, as the temperature approaches T. from above, the longitudinal spectrum contains a softening mode the frequency of which extrapolates to zero at a temperature below T.. A central peak due to excitations within the d

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Gene Cooperman,G. Michler,H. Vincktype II antiferromagnet into a paramagnet is found to be continuous in both cases. This does not support the recent theoretical prediction that the transition 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

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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 no point is crystal field theory invoked.

ATOPY

https://doi.org/10.1007/BFb0011851a have been analysed following a Green’s functions formalism to obtain the Fourier transform of interactions. The dispersion curves are well reproduced, but their precise energy position requires the addition of second order terms in the starting Hamiltonian.

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Interconnection networks for MIMD machines,ever observed for Gd in any host and is some three times greater than in any other pure metal. We discuss the parametrisation of our spectra and then compare the available results for b. parameters in metals and intermetallic compounds.

meretricious

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Gene Cooperman,G. Michler,H. Vinckns from cubic symmetry and couplings to excited electronic states. In the limit of strong anharmonicity, using a dynamic lattice model, it is possible to reproduce the splittings of one of the E.P.R. lines in the regime of both strong and weak inversion splitting.

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