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Atoms exposed to high-frequency strong laser fields experience the ionization suppression due to the deformation of Kramers-Henneberger (KH) wave functions, which has not been confirmed yet in experiment. We propose a bichromatic pump-probe strategy to affirm the existence of KH states, which is formed by the pump pulse and ionized by the probe pulse. In the case of the single-photon ionization triggered by a vacuum ultra-violet probe pulse, the double-slit structure of KH atom is mapped to the photoelectron momentum distribution. In the case of the tunneling ionization induced by an infrared probe pulse, streaking in anisotropic Coulomb potential produces a characteristic momentum drift. Apart from bichromatic schemes, the non-Abelian geometric phase provides an alternative route to affirm the existence of KH states. Following specific loops in laser parameter space, a complete spin flipping transition could be achieved. Our proposal has advantages of being robust against focal-intensity average as well as ionization depletion, and is accessible with current laser facilities.
We apply Bogolyubovs averaging theorem to the motion of an electron of an atom driven by a linearly polarized laser field in the Kramers-Henneberger frame. We provide estimates of the differences between the original trajectories and the trajectories
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We have studied the interplay between disorder and cooperative scattering for single scattering limit in the presence of a driving laser. Analytical results have been derived and we have observed cooperative scattering effects in a variety of experim
Isolating neutral and charged particles from the environment is essential in precision experiments. For decades, this has been achieved by trapping ions with radio-frequency (rf) fields and neutral particles with optical fields. Recently, trapping of