Assuming the initial population in the hydrogenic 50s state, we simulate Rydberg-state redistribution and photoionization by a nonresonant opticalfrequency pulse versus the number of different n manifolds included. The inclusion of additional n manifolds, around the n = 50 manifold distinguished by the initial-state choice, is shown to invalidate the photoionization predictions based on the single-n manifold approximation. The calculations are performed assuming a linearly polarized, 620 nm pulse, turned on and off suddenly, of ten-optical-period duration and peak intensity 10 9 W cm −2 ensuring effective transient mixing of both-parity Rydberg states around n = 50.