1991
DOI: 10.1103/physreva.44.1884
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Excitation of the hydrogen atom by fast-electron impact in the presence of a laser field

Abstract: An approach has been developed to study the excitation of a ground-state H atom to the n =2 level under the simultaneous action of fast-electron impact and a monochromatic, linearly polarized, homogeneous laser beam. The laser frequency is assumed to be low (soft-photon limit) so that a stationarystate perturbation theory can be applied as is done in the adiabatic theory. An elegant method has been developed in the present work to construct the dressed excited-state wave functions of the H atom using first-ord… Show more

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Cited by 9 publications
(5 citation statements)
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“…Regarding the shape of the DCS curves, it may be noted from figures 1 and 2 that the field free (FF) DCS curves fall off monotonically with increasing scattering angle while the field assisted (for l = 0, +1) curves exhibit some oscillations arising due to the occurrence of the Bessel functions J l (x) in the expression for the transition amplitude (see equation (22)). However, the number of oscillations in the l = 0, ±1 curves is found to increase (see figures 1 and 2) with the increasing field strength for the following reason.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…Regarding the shape of the DCS curves, it may be noted from figures 1 and 2 that the field free (FF) DCS curves fall off monotonically with increasing scattering angle while the field assisted (for l = 0, +1) curves exhibit some oscillations arising due to the occurrence of the Bessel functions J l (x) in the expression for the transition amplitude (see equation (22)). However, the number of oscillations in the l = 0, ±1 curves is found to increase (see figures 1 and 2) with the increasing field strength for the following reason.…”
Section: Resultsmentioning
confidence: 99%
“…In later works the Coulomb-Volkov (CV) wavefunction was also used by several workers [12,14,15] in the context of different laser assisted/induced procssses. Although the approximate CV solution presents the advantage of containing the field to all orders (inherent in the plane wave Volkov solution [11,[16][17][18][19][20][21][22][23]), it completely decouples the electron-laser and the electron-screened-ion interactions [18]. The laser-ion interaction (i.e.…”
Section: Introductionmentioning
confidence: 99%
“…It is well known that by increasing the atomic excitation the laser-dressing effects induced by the dipole polarizability [15] should increase in importance [16,17,18], and therefore with an increasing probability of experimental detection. As far as we known the first theoretical works on the laser-assisted inelastic scattering of electrons by atoms taking into account the atomic "dressing" (i.e., the dipole distortion of the atom by the laser field) were performed in different approaches such as first-order perturbation theory [19,20,21,22], non-perturbative Floquet theory [23], or relativistic method [24].…”
Section: Introductionmentioning
confidence: 99%
“…Theoretical works on the laser-assisted inelastic scattering of electrons by the hydrogen atom in its ground state by taking into account the atomic "dressing" (i.e. the dipole distortion of the atom by the laser field) in first-order perturbation theory were performed by Jetzke and co-workers [12], Francken and co-workers [13], Bhattacharya and co-workers [14], and Cionga and Florescu [15]. Lately Voitkiv and co-workers [16] have considered laser-assisted inelastic collisions of relativistic electrons with atomic targets in their ground state.…”
Section: Introductionmentioning
confidence: 99%