Heavy fermion superconductors can be classified into the following two
types based on their structures: (1) ternary transition metal carbide
s, borides, and silicides containing f-block metals exhibiting stable
multiple oxidation states such as cerium in CeCu2Si2, CeRu3B2, and CeR
u3Si2 or uranium in URu2Si2 and U2PtC2; (2) binary alloys containing m
ultiple oxidation state actinides (particularly uranium) and nonactini
de polyhedral clusters such as Be-13 centered icosahedra in UBe13 and
Pt-6/2 octahedra in UPt3. The f-block metals in heavy fermion supercon
ductors not only exhibit multiple oxidation states but are also dilute
d enough by the other elements so that the separation between f-block
metals in the structure is at least 4 Angstrom. The f-block metals bec
ome part of the conducting skeletons of heavy fermion superconductors
so that their conductivities arise at least partially through valence
fluctuations involving f-electrons. (C) 1997 Academic Press.