The laser-synchrotron radiation combination technique has recently been inc
orporated into an apparatus for two-dimensional photoelectron spectroscopy
of atoms and molecules in order to investigate photoionization dynamics of
polarized atoms. Ground state Ar atoms are excited with linearly polarized
synchrotron radiation to Rydberg states lying below the first ionization po
tential. The aligned atoms thus formed are ionized by irradiation of a lase
r which is also linearly polarized. Photoelectrons emitted in the direction
of the electric vector of the synchrotron radiation are sampled and energy
analysed. The photoelectron angular distribution is measured with respect
to the electric vector of the laser. Expressions which correlate the asymme
tric coefficients for the angular distribution with theoretical dynamic par
ameters involving transition dipole matrix elements are derived. The anisot
ropy of the present angular distribution can bt reasonably explained, assum
ing that the matrix elements and phase shift differences are essentially in
dependent of the total angular momentum quantum number of the final state a
nd that the spin-orbit interaction in the continuous spectrum is small.