2008
DOI: 10.1080/00107510802332908
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Many-electron strong-field physics

Abstract: Double and multiple ionisation cannot be understood without the contribution of a non-sequential mechanism, which is due to electron-electron correlation. This paper discusses the experimental manifestations of this effect, from its first footprint in the total yields of multiply charged ions to the highly differential cross-sections for ion and electron production, and the theoretical models that have been set up for their description. Except for the ab initio solution of the time-dependent Schro¨dinger equat… Show more

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Cited by 63 publications
(85 citation statements)
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“…It is impossible, at present, to simulate this process based on the time dependent Schrödinger equation (TDSE) because of exceedingly large computing time requirements 5 . Instead one describes the process usually in terms of simplifying mechanisms, which can be classified as sequential double ionization (SDI) or non-sequential double ionization (NSDI; ref.…”
mentioning
confidence: 99%
“…It is impossible, at present, to simulate this process based on the time dependent Schrödinger equation (TDSE) because of exceedingly large computing time requirements 5 . Instead one describes the process usually in terms of simplifying mechanisms, which can be classified as sequential double ionization (SDI) or non-sequential double ionization (NSDI; ref.…”
mentioning
confidence: 99%
“…However, in the early 90's, experiments using intense laser pulses found double ionization yields which departed from these treatments by several orders of magnitude [1], thereby casting doubt on the uniqueness of the sequential (uncorrelated) multiple ionization channel. These results constitute one of the most striking surprises of recent years in intense laser-matter interactions, and this new ionization channel ("nonsequential double ionization" (NSDI) [1]) has emerged as one of the most dramatic manifestations of electron-electron correlation in nature [2].…”
mentioning
confidence: 99%
“…A complete description of a two-electron system in an elliptically polarized field requires to simulate the motion for each electron in at least two dimensions, which is almost impossible at present [17]. To overcome the enormous computational challenge, the so-called crapola quantum model [18] was introduced, which has excellently reproduced the "knee" structure of NSDI [6,19].…”
mentioning
confidence: 99%