By J.X. Boucherle, J. Flouquet and C. Lacroix (Eds.)
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Extra resources for Anomalous Rare Earths and Actinides. Valence Fluctuation and Heavy Fermions
V. (North-Holland Physics Publishing Division) U. Welp et al. e. almost equal to the Wilson ratio for a spin 1/2 particle carrying a magnetic moment of one Bohr magneton. In this sense CePb 3 behaves as a nonmagnetic heavy fermion system. On the contrary, for the archetype magnetic Kondo lattice one finds a huge value of χ/y since the magnetic ordering quenches the renormalization of γ (see for in stance ref. ). Clearly in CePb 3 a significant part of the f-electrons does not contribute to the sublattice magnetization.
Rev. Lett. 54 (1985) 2541. L. Lin, A. E. Crow, T. Mihalisin and P. Schlottmann, (preprint). L. W. E. Crow, T. Mihalisin, J. P. Guertin, in: Proc. , Hamilton, Canada (9-12 June 1986) to be published.  M. Nicolas-Francillon, A. C. Ac hard, O. Gorochov, B. Cornut, D. Jerome and B. Coqblin, Solid State Commun. 11 (1972) 845. S. A. D. D. Parks, J. Magn. Magn. Mat. 52 (1985) 385.  B. Cornut and B. Coqblin, Phys. Rev. B5 (1972) 4541.  S. Maekawa, S. Kashiba, S. Takahashi and M. Tachiki, ref. , page 90.
Renker et al. / Crystal-field-excitations assumes additional splitting of the Γ 8 level as proposed in ref. , one should not expect the matrix elements to change by a factor of two as long as this additional splitting is small compared to Ei. Our results are corroborated by very recent ultrasonic experiments by Niki et al. 5 meV with Γ 7 as lowest level. From the magnetic neutron-scattering cross section one can calculate the static magnetic susceptibility XQ(T) via a sum rule . In cubic symmetry it reads f dES(Q,E)/f(E) J—oo = (ye2/meC2)2F(Q)2 e" 2 W χ0(Τ)/(2μ2Β).
Anomalous Rare Earths and Actinides. Valence Fluctuation and Heavy Fermions by J.X. Boucherle, J. Flouquet and C. Lacroix (Eds.)