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An experiment is described in which the absorption spectrum of the Rydberg series of sodium (principal quantum number, n>or=4) is studied in a strong non-resonant laser field. The field is generated from a PTM laser oscillator/amplifier system operating at 1.06 mu m, producing 250 MW in a 10 ns pulse. After splitting, most of the beam is focused into a sodium heat pipe oven where field strengths up to 8*10 7 V m -1 are generated. The other fraction of the beam is used to form a plasma from a solid lead target which is used as a continuum source for absorption spectroscopic measurements. Quenching of high-lying state (n>11) has been studied, the lowest quenched state being found to be dependent on laser intensity I l in the form I l varies as n -(3.9+or-0.8) . Such quenching is significantly different from that observed in a DC field. Additionally, line broadening, profile asymmetry and intensity dependent shifts are observed.
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Dewhurst et al. (1980) studied this question.
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