A simple semiclassical formula is given for the oscillator strengths o
f high Rydberg states of a hydrogen atom in an electric field. The osc
illator strength of a state is; proportional to the square of the func
tion representing the quantum angular distribution of outgoing waves,
evaluated at the classical angle of ejection from the atom that sends
the electron into a semiclassically quantized eigentrajectory. The for
mula gives an interpretation of the envelopes of Stark manifolds in ph
otoabsorption spectra; it is in good agreement with quantum calculatio
ns. The formula may also be used for other integrable or near-integrab
le systems.