We have measured the angular distribution of electrons ejected from doubly excited autoionizing Rydberg 3pns J=1 states of magnesium, where n=10–20. Two dye lasers cross an atomic beam and excite 3${\mathit{sns}}^1$${\mathit{S}}_0$ states of Mg. A third linearly polarized laser excites the 3pns states. The angular distribution is of the form (σ/4π)[1+β${\mathit{P}}_2$(cosθ)]. We measure β as a function of the energy of the third laser. The β parameter varies over its full range of values, -1 to 2. Our data agree quite well with the predictions of the reaction-matrix–multichannel-quantum-defect theory.

• Received 5 August 1991

DOI:https://doi.org/10.1103/PhysRevA.45.231