Abstract

Angular distributions of photoelectrons from resonant two-photon ionization of sodium have been measured. Excitation and ionization were carried out with two pulsed lasers, one with a frequency resonant with the $3s^{2}S_{\frac{1}{2}}\ensuremath{\rightarrow}3p^{2}P_{\frac{3}{2}}$ transition. The hyperfine levels in the intermediate state were excited coherently; hyperfine coupling affects the photoelectron distributions through a dependence on the time interval between excitation and ionization. The results are analyzed to give values of three microscopic parameters: the ratio of the radial dipole matrix elements for the production of $l=0$ and $l=2$ final states from the $3p$ level, the difference of the phase shifts of the outgoing electron in the final channels, and a parameter which expresses the depolarizing effect of the nuclear spin on the intermediate state. The phase-shift difference agrees with extrapolated bound-state data, but the final state has more $s$ character than theoretical quantum-defect calculations suggest.

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