Abstract
Many of the phenomena observed1 in a strong-field laser-atom interaction, such as high-harmonic generation, above-threshold ionization, and stabilization, can be obtained in simple models that invoke a picture of one electron under the influence of an effective potential; the observed phenomena are also found in numerical experiments that integrate the time-dependent Schrödinger equation for one-electron systems under fairly realistic conditions.
© 1995 Optical Society of America
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