Abstract
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 1.3Se, 1.3Pe, 1.3Po, 1.3De, 1.3Do and 1.3Fo manifolds and the photoionisation cross sections from the 3s2 1Se, 3s3p 1Po and 3s 3p3Po levels.

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