By J. Topuszanski
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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. Kasuya: to be published in [3e] A. Yanase: J. Magn. Magn. Mat. 31-34, 453 (1983) H. Harima and T. Kasuya: to be published in [3e] M. Kasaya, F. Iga, M. Takigawa and T.
Ga) [57J. In fact, a similar estimate 31 as above yields vFs ~ 10 vFn. Hence, one can assume non-renormalized light electrons with very low Tc to coexist with the heavy quasiparticles, presumably conduction electrons dressed by their strong interaction with the localized 4f-electrons. Only the latter ones are responsible for the observed HFS. Again, these conclusions are in general agreement with recent theoretical results : A calculation of the renormalized bandstructure of CeCu 2Si 2 , which modifies LDA  by taking into account proper phase shifts for the Kondo scattering, shows that there remain portions of the Fermi surface which do not develop heavy masses and probably do not participate in the Cooper-pair formation.
Steglich, J. D. Bredl, W. Lieke, D. Meschede, W. Franz and H. Schafer: J. Magn. Magn. Mat. R. Stewart: Rev. Mod. Phys. J. B. V. Culbert: Phys. Rev. Lett. 34, 1019 (1975 ) K. E. R. Ott: Phys. Rev. Lett.
An Intro to Symmetry and Supersym. in Quantum Field Theory by J. Topuszanski