Non-sequential double ionization of Ar: from the single- to the many-cycle regime

dc.citation.doi10.1088/1367-2630/16/3/033008
dc.citation.issn1367-2630
dc.citation.issue3
dc.citation.jtitleNew Journal of Physics
dc.citation.volume16
dc.contributor.authorKübel, M.
dc.contributor.authorBetsch, K. J.
dc.contributor.authorKling, Nora G.
dc.contributor.authorAlnaser, A. S.
dc.contributor.authorSchmidt, J.
dc.contributor.authorKleineberg, U.
dc.contributor.authorDeng, Y.
dc.contributor.authorBen-Itzhak, I.
dc.contributor.authorPaulus, G. G.
dc.contributor.authorPfeifer, T.
dc.contributor.authorUllrich, J.
dc.contributor.authorMoshammer, R.
dc.contributor.authorKling, M. F.
dc.contributor.authorBergues, B.
dc.date.accessioned2023-12-07T22:33:18Z
dc.date.available2023-12-07T22:33:18Z
dc.date.issued2014-03-01
dc.date.published2014-03-01
dc.description.abstractThe transition from the near-single to the multi-cycle regime in non-sequential double ionization of argon is investigated experimentally. Argon atoms are exposed to intense laser pulses with a center wavelength around 790 nm and the momenta of electrons and ions generated in the double ionization process are measured in coincidence using a reaction microscope. The duration of the near transform-limited pulses is varied from 4 to 30 fs. We observe an abrupt collapse of the cross-shaped two-electron momentum distribution [17] in the few-cycle regime. The transition to longer pulses is further accompanied by a strong increase in the fraction of anti-correlated to correlated electrons.
dc.identifier.urihttps://hdl.handle.net/2097/43935
dc.relation.urihttps://dx.doi.org/10.1088/1367-2630/16/3/033008
dc.rightsCreative Commons Attribution 3.0 licence
dc.rights.urihttps://creativecommons.org/licenses/by/3.0/
dc.titleNon-sequential double ionization of Ar: from the single- to the many-cycle regime
dc.typeText

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