2009
DOI: 10.1103/physrevlett.102.103201
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Plateau Structure in Resonant Laser-Assisted Electron-Atom Scattering

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Cited by 8 publications
(12 citation statements)
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“…The results in this paper become inapplicable for resonant electron energies, E ≈ µhω − |E 0 | − u p , at which the electron may be temporarily captured in a bound state ψ κlm l (r) of the potential U (r) by emitting µ photons [43], and for threshold energies, E = khω, k = 1,2, . .…”
Section: Discussionmentioning
confidence: 97%
“…The results in this paper become inapplicable for resonant electron energies, E ≈ µhω − |E 0 | − u p , at which the electron may be temporarily captured in a bound state ψ κlm l (r) of the potential U (r) by emitting µ photons [43], and for threshold energies, E = khω, k = 1,2, . .…”
Section: Discussionmentioning
confidence: 97%
“…This latter momentum ensures the condition for the electron return by the laser field back to the atom at the time moment t, followed by the recollision. We note that the saddle points t ′ k are functions of the time t (t ′ k ≡ t ′ k (t)) implicitly defined by equation (22).…”
Section: Low-frequency Analysis Of the Labrs Amplitudementioning
confidence: 99%
“…Both equations (34) and (35) follow from the saddle point equation (22). Let us consider now the rescattering approximation for the dipole momentd n given by (13).…”
Section: Of the Labrs Amplitudementioning
confidence: 99%
“…For example, significant enhancements of the cross sections for laser-assisted electron-atom scattering accompanied by absorption or emission of laser quanta was predicted in Ref. [6]. Also, the occurrence of resonant enhancements (by orders of magnitude) of the high-energy part of laser-assisted radiative recombination (LARR) or laser-assisted radiative attachment (LARA) spectra have been predicted in Ref.…”
Section: Introductionmentioning
confidence: 97%