Abstract
The problem of strong-field photoionization of a three-dimensional Rydberg hydrogen atom is solved numerically. The results are compared with those of the newest version of an analytical theory based on the quasiclassical approach. The probabilities of ionization calculated numerically and analytically are found to agree perfectly. The results obtained confirm the existence of strong-field interference stabilization interpreted in terms of Raman \ensuremath{\Lambda}-type transitions via the continuum.
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