Ionization Probabilities through ultra-intense Fields in the extreme Limit

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dc.creatorFring, A.
dc.creatorKostrykin, V.
dc.creatorSchrader, R.
dc.date1997-07-31
dc.date.accessioned2026-07-07T10:59:10Z
dc.date.available2026-07-07T10:59:10Z
dc.descriptionWe continue our investigation concerning the question of whether atomic bound states begin to stabilize in the ultra-intense field limit. The pulses considered are essentially arbitrary, but we distinguish between three situations. First the total classical momentum transfer is non-vanishing, second not both the total classical momentum transfer and the total classical displacement are vanishing together with the requirement that the potential has a finite number of bound states and third both the total classical momentum transfer and the total classical displacement are vanishing. For the first two cases we rigorously prove, that the ionization probability tends to one when the amplitude of the pulse tends to infinity and the pulse shape remains fixed. In the third case the limit is strictly smaller than one. This case is also related to the high frequency limit considered by Gavrila et al.
dc.description16 pages LateX, 2 figures
dc.identifierhttps://arxiv.org/abs/quant-ph/9707059
dc.identifierhttp://arxiv.org/abs/quant-ph/9707059
dc.identifierJ.Phys.A30:8599-8610,1997
dc.identifierdoi:10.1088/0305-4470/30/24/020
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/187356
dc.subjectQuantum Physics
dc.subjectAtomic Physics
dc.titleIonization Probabilities through ultra-intense Fields in the extreme Limit
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