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The consequences of the degeneracy between configurations with different populations of atomiclike f states are studied systematically for a number of light rare-earth materials (Ba, LaF₃, La₂{O}₃$, La, ${CeO}₂$, ${CeCo}₂$, CeN, {α}-Ce, and {γ}-Ce) using high-energy spectroscopies. The Anderson impurity model applied to this problem (Gunnarsson-Sch\"onhammer model) is found to describe convincingly a variety of electron-spectroscopic excitations, such as, x-ray photoemission and bremsstrahlung isochromat spectroscopy. We have extended this many-body formalism to account for electron-energy loss spectroscopy and LIII absorption edges. The parameters resulting from the calculation are analyzed within the framework of a simplified Hamiltonian containing no coupling terms between f and band states. This approach reveals in a natural way the importance of the conventional concept of hybridization. The energy degeneracy and the wave-function overlap of quantum states give rise to a mixing and to a continuous energy distribution of excitations. For electronic transitions described within the sudden approximation the impurity model provides a sound and unified description of the ``satellite complex'' encountered in the high-energy excitation spectra of such systems.
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Schneider et al. (1985) studied this question.
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