1989
DOI: 10.1103/physreva.39.6178
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Electron-impact ionization of atomic hydrogen in the presence of a laser field

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Cited by 65 publications
(43 citation statements)
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“…enhancement or diminution of the peak just seems to be reversed! It would be interesting to compare our experimental data with the results of more refined non-perturbative calculations taking target polarization or dressing of the initial state into account [24][25][26][27][28].…”
Section: Finally We Present Triply Differential Cross Sections Tdcsmentioning
confidence: 99%
“…enhancement or diminution of the peak just seems to be reversed! It would be interesting to compare our experimental data with the results of more refined non-perturbative calculations taking target polarization or dressing of the initial state into account [24][25][26][27][28].…”
Section: Finally We Present Triply Differential Cross Sections Tdcsmentioning
confidence: 99%
“…This oscillatory phenomenon can be explained by the changes of the Bessel function, i.e., the sign of the argument of the Bessel function changes depending on the sign of the summation over N coming from equation (19). This behavior can be traced back to the fact that the argument of the Bessel functions, entering the expressions of the amplitudes equations (19) and (20), grows with 0  and varies with the scattering angle. Accordingly, at higher field strengths, every other laser parameter being fixed, one explores more zeros of the Bessel functions when varying the scattering angle.…”
Section: =´-)mentioning
confidence: 99%
“…to enhance or suppress the ionization cross section as per the requirement in a particular physical process. Since the laser field can act as a reservoir of energy and its polarization vector introduces a new axis of symmetry, the laser-assisted ionization cross sections could differ strongly in shape and magnitude from the field-free cross sections as predicted in several theoretical studies on this topic [18][19][20][21][22][23][24].…”
Section: Introductionmentioning
confidence: 99%
“…This particular scattering geometry is called the co-planar asymmetric geometry. In [10][11][12][13] the states of the projectile electron are then described by Volkov wavefunctions [14] whereas for the slow ejected electron the combined influence of the laser field and the Coulomb field of the residual ion is taken into account [10]. The influence of the laser on the target states is treated using a first-order perturbation approach.…”
Section: Introductionmentioning
confidence: 99%