1994
DOI: 10.1103/physreva.49.4837
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Atomic hydrogen in a strong optical radiation field

Abstract: Experimental energy spectra and energy-resolved angular distributions of photoelectrons produced by multiphoton ionization of atomic hydrogen are presented for several wavelengths between 596 and 630 nm, peak intensities of about 10 W/cm, and laser pulse durations of about 0.5 ps.Resonant ionization processes via ac Stark-shift-induced resonances with excited states dominate the spectra. The results of Sturmian-Floquet calculations of these spectra and angular distributions are presented; they are in fair agre… Show more

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Cited by 50 publications
(53 citation statements)
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“…Therefore, in order to observe pronounced oscillations of the partial ionization rates in higher photon channels (as found numerically in results of Refs. [25,26,[28][29][30][31][32] (27) and (28), one sees that a − b α β does not depend on c 1 , whereas α − iβ = det M − is 2 M 11 − 2ic 1 (M 22 − is 2 ) is a nonzero complex number in the limit c 1 → 0. Hence, one deduces that the second term in Eq.…”
Section: -5mentioning
confidence: 98%
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“…Therefore, in order to observe pronounced oscillations of the partial ionization rates in higher photon channels (as found numerically in results of Refs. [25,26,[28][29][30][31][32] (27) and (28), one sees that a − b α β does not depend on c 1 , whereas α − iβ = det M − is 2 M 11 − 2ic 1 (M 22 − is 2 ) is a nonzero complex number in the limit c 1 → 0. Hence, one deduces that the second term in Eq.…”
Section: -5mentioning
confidence: 98%
“…[8,9,13,[25][26][27][28][29][30][31][32]). Note that for fixed parameters of the laser field, the amount of energy that has to be delivered in order to ionize a laser-dressed atom must be at least E min = −Re E + U p .…”
Section: Floquet Theorymentioning
confidence: 99%
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“…Extensive investigations have been performed both theoretically [11][12][13][14][15][16][17][18] and experimentally [7,12,14,[19][20][21][22][23][24][25][26][27][28][29][30][31] for a comprehensive understanding of the laser-induced atomic ATI for laser fields with wavelengths from visible lights (4×10 2 nm) to infrared radiations (1×10 5 nm). With the recent development of intense and ultrashort-wavelength free-electron lasers [32][33][34], the study of multiphoton * zyzhou@ku.edu † sichu@ku.edu processes in the high-frequency and strong-field regime becomes increasingly important [35][36][37].…”
Section: Introductionmentioning
confidence: 99%