By J.X. Boucherle, J. Flouquet and C. Lacroix (Eds.)
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Extra info for Anomalous Rare Earths and Actinides. Valence Fluctuation and Heavy Fermions
43 (1979) 1892.  F. Steglich, Physica 130B (1985) 145.  E. Gratz, E. Bauer, B. Barbara, S. Zemirli, F. Steglich, C D . Bredl and W. Lieke, J. Phys. F 15 (1985) 1975.  D. Gignoux, F. Givord, R. Lemaire, H. Launois and F. Savetat, J. de Phys. 43 (1982) 173.  E. Bauer, E. Gratz and G. Adam, J. Phys. F 16 (1986) 493.  B. Cornut and B. Coqblin, Phys. Rev. B 5 (1972) 4541.  D. Wohlleben and B. Wittershagen, Advan. Phys. 34 (1985) 403.  U. Rauchschwalbe, U. Gottwick, U. M. Mayer and F.
The thermal conductivity λ ( Τ ) as a function of the temperature is plotted for CeCu 5 and LaCu 5 in fig. 2. While λ ( Τ ) of LaCu 5 shows a pronounced maximum in the low temperature region, typical for materials with minimal im purity scattering, the thermal conductivity of CeCu 5 shows no maximum and is considerably smaller over the whole temperature range. Recently we have shown that the lattice thermal conductivity for good metallic conductors is negligible . If we therefore neglect this con tribution, the low lying λ ( Τ ) curve in CeCu 5 must be attributed to scattering processes of the heat carrying electrons with the magnetic moments of the Ce 3 + ions.
We should like to thank P. Fulde for a critical reading of the manuscript and D. Wohlleben for stimulating discussions. L. Lin, J. E. Crow, T. Mihalisin, J. I. R. Stewart, Phys. Rev. Lett. 54 (1985) 2541.  C. Vettier, P. Morin and J. Flouquet, Phys. Rev. Lett. 56 (1986) 1980.  P. Lethuillier and J. Chaussy, J. de Phys. 37 (1976) 123.  D. Duerkop, E. Braun, B. Politt, H. Schmidt and D. Wohlleben, Z. Physik B63 (1986) 55. J. Birgeneau, J. Phys. Chem. Solids 33 (1972) 59.  D. Niki, W. Assmus, I.
Anomalous Rare Earths and Actinides. Valence Fluctuation and Heavy Fermions by J.X. Boucherle, J. Flouquet and C. Lacroix (Eds.)