Muon spin relaxation has been measured in CeCoGe3-xSi(x) at the magnetic/nonmagnetic boundary compositions of x = 1.2 and x = 1.5. Both the alloys are found to exhibit an ordered region and a disordered region. At x = 1.2, short-range magnetic ordering is observed below 0.86 K in the ordered region. The disordered region is paramagnetic and the muon spin-lattice relaxation rate lambda2 in this region displays non-Fermi-liquid (NFL) spin dynamics, i.e., the power law lambda2 proportional to T0.72 which shows the formation of Griffiths phase. lambda2 in the x = 1.5 alloy displays logarithmic (NFL) scaling below 1 K, in agreement with the theory of a T = 0 K magnetic transition.
By the resonant inverse photoemission spectroscopy ͑RIPES͒, we study the crossover from mixed-valent to heavy-fermion and Kondo regime in CeCoGe 3Ϫx Si x (0рxр3). We have measured the RIPE spectra as functions of composition and temperature. The strong composition dependence of 4 f state ͑''f 1 peak''͒ just above the Fermi level shows that the localized 4 f electrons in the compound become itinerant due to the enhanced Kondo effect within the range 1.0рxр1.5. Temperature dependence of the f 1 peak indicates a transition from the paramagnetic state at room temperature to a coherent Fermi-liquid regime at low temperatures where the Kondo effect dominates. The most remarkable variation of the spectra has been observed above 200 K with increasing temperature in CeCoSi 3 which has a very high Kondo temperature T K of about 900 K. This suggests that the change in the 4 f-electronic state of CeCoSi 3 may be scaled by the coherence transition temperature rather than T K. ͓S0163-1829͑99͒50638-3͔
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