For pt.I see ibid., pp.1121-32 (1988). The states computed in the previous paper have been employed to calculate the oscillator strengths for the transitions between the 1.3 S e , 1.3 P e , 1.3 P o , 1.3 D e , 1.3 D o and 1.3 F o manifolds and the photoionisation cross sections from the 3s 2 1 S e , 3s3p 1 P o and 3s 3p 3 P o levels.
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Moccia et al. (1988) studied this question.
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