2004
DOI: 10.1103/physrevlett.93.263001
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Nonsequential Double Ionization at the Single-Optical-Cycle Limit

Abstract: We report differential measurements of Ar++ ion momentum distributions from nonsequential double ionization in phase-stabilized few-cycle laser pulses. The distributions depend strongly on the carrier-envelope (CE) phase. Via control over the CE phase one is able to direct the nonsequential double-ionization dynamics. Data analysis through a classical model calculation reveals that the influence of the optical phase enters via (i) the cycle dependent electric field ionization rate, (ii) the electron recollisio… Show more

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Cited by 166 publications
(126 citation statements)
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“…In earlier work, the (e, 2e) mechanism was invoked to explain the CEPdependent Ar 2 + recoil-ion spectra at about twice the intensity 16,28 .…”
Section: Comparison Of Measured and Calculated Asymmetriesmentioning
confidence: 99%
See 1 more Smart Citation
“…In earlier work, the (e, 2e) mechanism was invoked to explain the CEPdependent Ar 2 + recoil-ion spectra at about twice the intensity 16,28 .…”
Section: Comparison Of Measured and Calculated Asymmetriesmentioning
confidence: 99%
“…Even more insight into the process was gained in kinematically complete studies where the correlated two-electron momentum distributions were measured 11 and investigated for different laser parameters [12][13][14][15] . Measurements of the dynamics of NSDI in near-single cycle laser pulses have been restricted to recoil-ion spectra, which did not allow for the direct retrieval of the correlated electron-emission dynamics 16,17 . The sub-cycle dependence of electron correlation spectra has been explored by various theoretical studies, where the double-ionization dynamics were confined to a single cycle of a laser pulse 12,18 .…”
mentioning
confidence: 99%
“…where ω a = 4.13·10 16 1/s is the atomic frequency unit, E a = 5.145·10 11 V/m the atomic unit of the electric field, and E opt the optical field strength. U H ion = 13.6 eV and U N2 ion = 15.6 eV denote the ionisation potentials of atomic hydrogen and molecular nitrogen, respectively.…”
Section: Ionisation Model Employed In the Simulationsmentioning
confidence: 99%
“…Many of the phenomena studied depend critically on the CE phase. Examples include the dynamics of above-threshold ionisation (ATI) 4 , light-induced non-sequential double ionisation 16 , Gouy phase observation 17 , and quantum interference in photocurrents 18 . An exciting prospect is the application of the CE phase as a coherent-control tool, e.g., to steer bound electrons in molecules 19 .…”
mentioning
confidence: 99%
“…The precisely controllable CEP of a near-infrared driving waveform could be used to adjust both the ionization yield [28] in each field half-cycle and the classical excursion of the ionized electron in the continuum to generate, upon recombination with the parent ion, single or twin soft x-ray attosecond bursts of radiation near the cutoff of the emitted spectra. This first essential paradigm of attosecond control was followed by equally crisp demonstrations of strong-field controlled electron emission from atoms [29,30], their double ionization [31], the sub-cycle control and the dissociation in simple molecular species [32]. More recently, this paradigm was further extended to field sensitive control of chemical dynamics in more Figure 2.…”
Section: Attosecond Strong-field Physics In the Few-cycle Regimementioning
confidence: 99%