Abstract

Rydberg states of atoms with two valence electrons exhibit three markedly different features compared to alkali systems. First of all, the coupling between the two valence electrons is most crucial for the properties of the Rydberg states and, in general, we have to distinguish between series with predominant singlet or triplet character. Secondly, low-lying states of doubly excited configurations cause strong perturbations of the Rydberg series belonging to one excited valence electron. This can lead to both singlet-triplet mixing and/or configuration mixing more or less local in energy. The third feature involves the interaction between the ms valence electron of the ion and the nucleus. The electro-static part of it reveals itself through the field shift, while for nuclei with I=0 the magnetic interaction causes a hyperfine splitting as well as a higher-order shift.

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