Coulomb Rescattering in Nondipole Interaction of Atoms with Intense Laser Fields
arXiv:1612.04939 · doi:10.1103/PhysRevA.95.011402
Abstract
We investigate the ionization dynamics of atoms irradiated by an intense laser field using a semiclassical model that includes magnetic Lorentz force in the rescattering process. We find that, the electrons tunneled with different initial transverse momenta (i.e., perpendicular to the instantaneous electric field direction) distributed on a specific circle in the momentum plane can finally converge to the same transverse momentum after experiencing Coulomb forward scattering. These electron trajectories lead to a bright spot structure in the 2D transverse momentum distribution, and particularly in the long-wavelength limit, a nonzero momentum peak in the direction antiparallel to the laser propagation (or radiation pressure) direction. Making analysis of the subcycle dynamics of rescattering trajectories, we unveil the underlying mechanism of the anti-intuitive peak. Beyond the strong field approximation and the dipole approximation, we quantitatively predict the spot center and the peak position. Our results are compared with a recent experiment and some theoretical predictions are given.
arXiv comment5 pages, 4 figures
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- Deuterium-tritium fusion process in strong laser fields: Semiclassical simulation
- Analytical approach to Coulomb focusing in strong field ionization
- Photon-momentum transfer in diatomic molecules: an ab initio study
- Sub-cycle time-resolved nondipole dynamics in tunneling ionization
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- Relativistic analytical R-matrix (ARM) theory for strong-field ionization