1994
DOI: 10.1103/physreva.50.r3585
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High-harmonic generation and correlated two-electron multiphoton ionization with elliptically polarized light

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Cited by 314 publications
(175 citation statements)
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“…At the same time, the peaks were found to be compatible with the "antenna" (Kuchiev 1987) or the "recollision" mechanism (Corkum 1993) as was first shown within classical considerations Moshammer et al 2000;Weber et al 2000). Subsequently, a variety of theoretical predictions (see the detailed discussion and references in Dörner et al (2002)) based on S-matrix theory, on the numerical solution of the time dependent Schrödinger equation (TDSE) as well as on the classical or semi-classical approximations essentially established the double peakstructure and recollision as the dominant NS double ionisation mechanism (see also earlier measurements with circularly polarized light by Fittinghoff et al (1994) and Dietrich et al (1994)). In the sequential regime a broader distribution is observed with a single peak at zero momentum along the field axis (see (3) in Figure 17).…”
Section: Double Ionisation: Non-sequential and Sequentialmentioning
confidence: 99%
“…At the same time, the peaks were found to be compatible with the "antenna" (Kuchiev 1987) or the "recollision" mechanism (Corkum 1993) as was first shown within classical considerations Moshammer et al 2000;Weber et al 2000). Subsequently, a variety of theoretical predictions (see the detailed discussion and references in Dörner et al (2002)) based on S-matrix theory, on the numerical solution of the time dependent Schrödinger equation (TDSE) as well as on the classical or semi-classical approximations essentially established the double peakstructure and recollision as the dominant NS double ionisation mechanism (see also earlier measurements with circularly polarized light by Fittinghoff et al (1994) and Dietrich et al (1994)). In the sequential regime a broader distribution is observed with a single peak at zero momentum along the field axis (see (3) in Figure 17).…”
Section: Double Ionisation: Non-sequential and Sequentialmentioning
confidence: 99%
“…As the high-harmonic beam polarization follows the atomic dipole direction, which is directly related to the driving laser polarization, one should expect to control the harmonic ellipticity by the driving laser ellipticity [3][4][5] . However, the recombination probability and consequently the harmonic generation efficiency drops dramatically with this latter 6,7 . Several methods were proposed to overcome this restriction [8][9][10][11][12][13][14][15][16] , but only three of them really show the production of high harmonics with elliptical polarization and non-negligible efficiency.…”
mentioning
confidence: 99%
“…Since laser photon energies are low compared to I p , the rate is independent of the laser frequency. 2.0x10 21 4.0x10 21 6.0x10 21 8.0x10 21 10 22 The dissociation rates (solid line), defined as P diss = p ( p 5fs , 800 nm), where P diss is the dissociation probability at the end of the laser pulse, calculated from the time-dependent Schrö dinger equation, are compared with tunneling rates (dotted line) in the dc field rate, and with the cycle averaged tunneling rate [18] (dashed line).…”
mentioning
confidence: 99%
“…(3) g g R; t and u u R; t are nuclear wave functions corresponding to the gerade and ungerade [18] by replacing the electron mass by the muon reduced mass m 0 , plotted as a function of the peak laser field. Since laser photon energies are low compared to I p , the rate is independent of the laser frequency.…”
mentioning
confidence: 99%