Abstract
By making use of the “velocity bunching” effect in collinear laser-ion beam spectroscopy, the hfs of the 5 p 5 2 P 3 2 5 d[ 3 2 ] 0 2→ 2 P 3 2 6 p[ 3 2 ] 2 transition in Cs II has been determined. A 30% reduction in linewidth compared with measurements using perpendicular laser-ion beam geometry is observed. The results for the 6 p[ 3 2 ] 2 level are compared with semi-empirical calculations.
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