Abstract
The charge and spin excitation spectra in the degenerate Anderson model are calculated by means of the exact solution. We investigate a crossover behavior in the excitation spectra. When the f -level position shifts from the valence fluctuation regime to the Kondo regime, the broad asymmetric peak structure in the charge excitation spectrum changes into the universal one around the bare f -level position. In the case of the spin excitation, the spectrum gets narrower and forms the sharp Kondo resonance with the hump structure arising from the orbital degeneracy. The crystal-field effects on the spin excitation spectra are also investigated in the Kondo limit. As the crystal-field splitting is increased, the Kondo resonance gets narrower and the hump structure disappears.
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