2010
DOI: 10.1134/s1054660x10190023
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Two-color ionization of hydrogen by short intense pulses

Abstract: Photoelectron energy spectra resulting by the interaction of hydrogen with two short pulses having carrier frequencies, respectively, in the range of the infrared and XUV regions have been calculated. The effects of the pulse duration and timing of the X-ray pulse on the photoelectron energy spectra are discussed. Analysis of the spectra obtained for very long pulses show that certain features may be explained in terms of quantum interferences in the time domain. It is found that, depending on the duration of … Show more

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Cited by 9 publications
(20 citation statements)
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(24 reference statements)
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“…In contrast to the case of forward emission, we find that transversal emission has relatively low probabilities, i.e., the PE energy range is highly reduced. However, we observe that the PE emission is non-vanishing in agreement with Bivona et al [33]. Moreover, the PE emission is due to the absorption and emission of an odd number of IR photons following one XUV photon absorption, whose photoionization line is absent in the PE spectrum.…”
Section: Introductionsupporting
confidence: 91%
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“…In contrast to the case of forward emission, we find that transversal emission has relatively low probabilities, i.e., the PE energy range is highly reduced. However, we observe that the PE emission is non-vanishing in agreement with Bivona et al [33]. Moreover, the PE emission is due to the absorption and emission of an odd number of IR photons following one XUV photon absorption, whose photoionization line is absent in the PE spectrum.…”
Section: Introductionsupporting
confidence: 91%
“…Several theories, like SPA, predict no emission in the direction perpendicular to the polarization axis. However, Bivona et al envisaged non-zero emission for XUV ionization of hydrogen by short intense pulses [33]. Therefore, in the present paper, we extend our previous work [34] for LAPE from H(1s) to study the emission in the direction perpendicular to the polarization axis of both XUV and laser fields.…”
Section: Introductionmentioning
confidence: 52%
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“…In this sense, the fact that the intracycle interference pattern modulates the sidebands in the energy distribution, albeit derived within the SCM, is also valid for the quantum calculations. The reason for this is under current investigation, however we note that it is in close relationship with previous work [8,18] where the PE spectra is factorized as two contributions. It is also worth to mention that, as within the SCM, there are frustrated SBs, i.e., close to E = 0.63, 1.03, 1.2, and 1.4 coinciding with the minima of the intracycle interference pattern In order to investigate the dependence of the intracycle interference pattern on the intensity of the laser pulse, we perform calculations of the energy distribution in the forward direction within the SCM in Fig.…”
Section: (B) and (D) We Show The Values Of A(t)supporting
confidence: 83%
“…where β ± (k), f ± (k) and ∆S ± are defined in equations (24), (31) and (30) of the appendix, respectively, and Θ is the Heaviside function. The ionization rate Γ(k ⊥ ) in equation (13) is identical for all subsequent ionization trajectories which depend on the perpendicular component of the final momenta k ⊥ , i.e.,…”
Section: Theory Of the Semiclassical Modelmentioning
confidence: 99%