Assuming the initial population in the hydrogenic 50s state, we simulate Ry
dberg-state redistribution and photoionization by a nonresonant optical-fre
quency pulse versus the number of different n manifolds included. The inclu
sion of additional n manifolds, around the n = 50 manifold distinguished by
the initial-state choice, is shown to invalidate the photoionization predi
ctions based on the single-n manifold approximation. The calculations are p
erformed assuming a linearly polarized, 620 nm. pulse, turned on and off su
ddenly, of ten-optical-period duration and peak intensity 10(9) W cm(-2) en
suring effective transient mixing of both-parity Rydberg states around n =
50.