2014
DOI: 10.1103/physreva.89.031401
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Attosecond evolution of energy- and angle-resolved photoemission spectra in two-color (XUV+IR) ionization of rare gases

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Cited by 14 publications
(45 citation statements)
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References 21 publications
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“…For instance, the use of coincidence detection devices [32][33][34] typically requires about 10 5 -10 8 photons∕pulse [32], which matches the number of photons obtained in a single harmonic in the plateau when the short trajectory is phase matched with our sources. This opens the route to the investigation of, e.g., time delays in molecular photoionization [35].…”
Section: Resultsmentioning
confidence: 72%
“…For instance, the use of coincidence detection devices [32][33][34] typically requires about 10 5 -10 8 photons∕pulse [32], which matches the number of photons obtained in a single harmonic in the plateau when the short trajectory is phase matched with our sources. This opens the route to the investigation of, e.g., time delays in molecular photoionization [35].…”
Section: Resultsmentioning
confidence: 72%
“…When an atom with ionization potential I p is ionized by an XUV attosecond pulse train (APT), photoelectrons are released in the continuum at discrete kinetic energies equal to E kin = E HH − I p , where E HH = (2 q +1) ħω defines the XUV photon energy comb of the APT ( ω is the IR laser frequency). When an IR dressing field is added, we obtain two-color two-photon transitions with a photoelectron spectrum that exhibits additional sidebands (SBs) at energies in-between two consecutive APT comb peaks 38 . These energies correspond to the absorption of an XUV photon combined with the additional absorption or emission of an IR photon.…”
Section: Resultsmentioning
confidence: 99%
“…However, as explained below, since it is based upon two-photon XUV-IR transitions, it also changes the angular momentum of the final states and consequently the photoelectron angular distributions. 38 , 47 . For any ionization channel leading to the same final state, our experimental measurement involves three two-photon pathways: 3 p → λ →ℓ, with ( λ , ℓ ) = (0,1),(2,1),(2,3).…”
Section: Discussionmentioning
confidence: 99%
“…Nowadays, models able to describe reactions assisted by a stronger NIR are available. Among them, the soft-photon approximation [7] was successfully applied to study angular distributions (ADs) in laser-assisted atomic photoionization by photons from free electron laser [8] or high harmonic generation (HHG) [6,9] sources. Also, it was established in previous studies for atomic/molecular targets [10][11][12] that the Separable Coulomb-Volkov model (SCV) may provide results in qualitative agreement with ab-initio calculations.…”
mentioning
confidence: 99%
“…The sophisticated techniques involved in the measurement of energy-and angle-resolved spectra have evolved in an outstanding way. The long-term stability of the ATPT-NIR synchronization, necessary for this kind of experiment in cold target recoil ion momentum spectroscopy devices, was reduced to about 60 attoseconds [9,13], enabling thus the determination of the AD of photoelectrons with a given energy and an almost fixed ATPT-NIR delay. Experimental studies concerned with the photoelectron ADs, although scarce, showed a critical dependence with the ATPT-NIR delay [9,[13][14][15][16][17].…”
mentioning
confidence: 99%