By T. Kasuya (auth.), Professor Tadao Kasuya, Dr. Tetsuro Saso (eds.)

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**Extra info for Theory of Heavy Fermions and Valence Fluctuations: Proceedings of the Eighth Taniguchi Symposium, Shima Kanko, Japan, April 10–13, 1985**

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In [3a], p. 89 E. Wuilloud, H. R. Moser, W. -D. Schneider and Y. Baer: Phys. Rev. B28, 7354 (1983) D. M. Wieliczka, C. G. Olson and D. W. Lynch: Phys. Rev. B29, 3028 (1984) J. W. Allen and R. M. Martin: Phys. Rev. Lett. 49, 1106 (1982) R. M. Galera, D. Givord, J. Pierre, A. P. Murani, C. Vettier and K. R. A. Ziebeck: J. Magn. Magn. Mat. 47&48, 139 (1985), and to be published W. R. Johanson, G. W. Crabtree, D. D. Koelling, A. S. Edelstein and O. D. McMasters: J. Appl. Phys. 52, 2134 (1981) H. Harima and T.

Appendix We consider the case that the valence p-bands are rilled and the conduction d-bands separated rrom the valence bands with a gap are vacant. The model is also applicable to Ce-monopnictides treated in detail in the text. To make the calculation simpler, we pick up only one rare earth site rrom which an r-electron is removed and the surrounding nearest neighbour anions. We also consider only d-symmetry molecular orbits and assume that the ten-rold degenerate bonding orbits belong to the valence bands and are occupied.

4 and the data taken for CeCu 2 • 2 Si 2 in an overcritical field B = 2T in Fig. 6a. In the following we discuss some polycrystal results which suggest a distinct influence of the "coherence-gap" formation on superconducting properties of CeCu 2 Si 2 : (i) In the absence of a maximum in Cn(T)/T (cf. Fig. 4), no superconductivity is found down to 20mK. Thus, the existence of a coherence gap appears as a necessary condi tion for HFS in CeCu 2 S i 2. On the other hand, (ii) the pronounced C(T)/T variation as observed for the gapless-superconducting sample No.