1998
DOI: 10.1103/physreva.57.r709
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Eight- and nine-photon resonances in multiphoton ionization of xenon

Abstract: We have measured and analyzed the clear emergence of ac-Stark-shifted multiphoton resonances with successive photon orders in xenon. The remarkable quality of our data illustrates the unambiguous evolution through parity-allowed resonances at the eight-and subsequent nine-photon levels. This marks a significant advance in showing that the transient resonance model is valid and strong optical-field ionization remains multiphoton in character at higher intensities. Furthermore, a simple Landau-Zener picture is s… Show more

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Cited by 33 publications
(19 citation statements)
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“…4 (bottom) are 130 meV and 80 meV, respectively. The extracted numbers are in good agreement with previously reported values of 120 meV and 74 meV obtained by time-of-flight electron spectroscopy [13]. The main constrains on the photoelectron linewidth are imposed by the rather short lifetimes of dressed states leading to the Freeman resonances, typically 1-60 fs [24].…”
Section: Above-threshold Ionization In Xenonsupporting
confidence: 79%
“…4 (bottom) are 130 meV and 80 meV, respectively. The extracted numbers are in good agreement with previously reported values of 120 meV and 74 meV obtained by time-of-flight electron spectroscopy [13]. The main constrains on the photoelectron linewidth are imposed by the rather short lifetimes of dressed states leading to the Freeman resonances, typically 1-60 fs [24].…”
Section: Above-threshold Ionization In Xenonsupporting
confidence: 79%
“…Simultaneous measurements of electron energy and angular distributions enabled by photoelectron imaging techniques [4,5,6,7,8] and a careful quantitative comparison of experimental electronmomentum distributions with theoretical volume-integrated spectra allowed the identification of processes like channel switching, i.e. a change in the number of photons required for resonant population of a Rydberg series upon increase of the laser intensity, as well as multi-photon resonant and non-resonant ionization, and ac Stark splitting [9].…”
mentioning
confidence: 99%
“…Traditionally, the resonant ionization signal increases with rising peak intensity due to volumetric growth. 24,25 If the nonresonant population transfer dominates, this should result in the larger enhancement for peak 3, because peak 3 requires lower intensities to be shifted into the resonance than peak 2 and peak 1 do, occurs on the early time of the pulse, and hence more nonresonant time, leading to relatively larger amplitudes of photoelectron peak 3. It is the case in our experiment for intensities below 1.92 × 10 14 W/cm 2 The nonresonant ionization signal increases with peak laser intensities because of the increasing nonresonant time.…”
Section: 2mentioning
confidence: 99%