Abstract
The process of ionization of a hydrogen atom by a short infrared laser pulse is studied in the regime of very large pulse intensity, in the dipole approximation. Let denote the integral of the electric field of the pulse over time at the location of the atomic nucleus. It is shown that, in the limit where , the ionization probability approaches unity and the electron is ejected into a cone opening in the direction of and of arbitrarily small opening angle. Asymptotics of various physical quantities in is studied carefully. Our results are in qualitative agreement with experimental data reported in \cite{1,2}.
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