Strong electronic correlations on partially filled 4f or 5f shells,
weakly hybridized with the itinerant ligand states, cause the
formation of extremely heavy quasiparticles composed of a dominating
local spin part and delocalized charge carrier contributions. As
discovered in 1979 for CeCu2Si2 [1], these
"heavy fermions" (HF) may form Cooper pairs, the
superconducting glue presumably being of magnetic origin, at least
in most cases [2]. This could be convincingly demonstrated with the
aid of tunneling and neutron-scattering experiments on
UPd2Al3 [3].
For a number of Ce-based HF metals superconductivity was found to be
intimately related to the existence of an antiferromagnetic
instability, most likely of the (3D) spin-density-wave type [4]. On
the other hand, a quantum critical point of the local-moment variety
at which the "composite fermions" appear to break up, as
recently established in YbRh2(Si,Ge)2
[5], appears to be unfavorable for superconductivity.
Work done in collaboration with J. Custers, P. Gegenwart, C. Geibel,
F.M. Grosche, R. Küchler, K. Neumaier, N.K. Sato, J.
Sichelschmidt, G. Sparn, O. Stockert, Y. Tokiwa, H. Wilhelm, H.Q.
Yuan, P. Coleman, C. Pepin, Q. Si, P. Thalmeier and G. Zwicknagl.
[1] F. Steglich et al., Phys. Rev. Lett 43, 1892 (1979).
[2] H.Q. Yuan et al., Science 302, 2104 (2003).
[3] N.K. Sato et al., Nature 410, 340 (2001).
[4] O. Stockert et al., Phys. Rev. Lett. 92, 136402 (2004).
[5] J. Custers et al., Nature 424, 524 (2003).
R. Küchler et al., Phys. Rev. Lett. 91, 066405 (2003).
J. Sichelschmidt et al., Phys. Rev. Lett. 91, 156401 (2003).
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