Only few selected examples among the great diversity of anomalous rare earth skutterudite are reviewed. Focus is first given on PrFe4P12 in comparison with URu2Si2. For PrFe4P12, great progress has been made on determining the nature of the order parameter (OP). A non magnetic order parameter with a multipolar component emerges here while for URu2Si2 the nature of the so-called hidden order remains mysterious. The two systems have several similarities in their temperature-pressure (T , P ) and magnetic field-temperature (H, T ) phase diagrams, in their spin dynamics, in their nesting character and in their high sensitivity to impurities. Advances on one side must stimulate new views on the other. Besides general considerations on the choice of the OP, a simple basic problem is the treatment of the Kondo coupling in a system with low charge carrier number for the cases of uncompensated and compensated semi-metal. An interesting problem is also the possible decoupling between exciton modes and itinerant carriers.
KEYWORDS:The new skutterudite compounds such as PrFe 4 P 12 , SmOs 4 Sb 12 , SmFe 4 P 12 , CeOs 4 Sb 12 and CeFe 4 P 12 give new insights on the interplay between valence driven metal-insulator transitions, Kondo effect and magnetic long range order. A fancy point is that these compounds often seem to have an intermediate valence behaviour even when their valences are close to 3. The occurrence of well defined multipoles is often revealed by crossing the phase transition in temperature. Magnetic field will lead to recover the duality between localized and intermediate valence characters. To illustrate this particularity, a comparison is made with electronic conduction and magnetism in the intermediate valence system SmB 6 and TmSe and also with the ferromagnetic superconductor URhGe.