Abstract
Observations of the series due to simultaneous excitation of two valence electrons to 4p
ns
,
nd
in Ca i and 5p
ns
,
n
d in Sr I are reported. The importance of the angular momentum barrier for the doubly excited
n
d series and, by comparison, for the
n
d series of singly excited even parity states is inferred with the help of single configuration Hartree-Fock calculations. This contrasts with the situation in Mg Ι, where wavefunction collapse does not occur in the doubly excited 3p
n
d series.
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