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    Semiclassical two-step model for strong-field ionization

    N. I. Shvetsov-Shilovski1,*, M. Lein1, L. B. Madsen2, E. Räsänen3, C. Lemell4, J. Burgdörfer4,5, D. G. Arbó6, and K. Tőkési5,7

    • 1Institut für Theoretische Physik and Centre for Quantum Engineering and Space-Time Research, Leibniz Universität Hannover, D-30167 Hannover, Germany
    • 2Department of Physics and Astronomy, Aarhus University, 8000 Århus C, Denmark
    • 3Department of Physics, Tampere University of Technology, FI-33101 Tampere, Finland
    • 4Institute for Theoretical Physics, Vienna University of Technology, A-1040 Vienna, Austria, European Union
    • 5Institute for Nuclear Research, Hungarian Academy of Sciences, H-4001 Debrecen, Hungary, European Union
    • 6Institute for Astronomy and Space Physics, IAFE (UBA-Conicet), Buenos Aires, Argentina
    • 7ELI-HU Nonprofit Ltd., Dugonics tér 13, 6720 Szeged, Hungary
    • *n79@narod.ru

    Phys. Rev. A 94, 013415 – Published 19 July, 2016

    DOI: https://doi.org/10.1103/PhysRevA.94.013415

    Abstract

    We present a semiclassical two-step model for strong-field ionization that accounts for path interferences of tunnel-ionized electrons in the ionic potential beyond perturbation theory. Within the framework of a classical trajectory Monte Carlo representation of the phase-space dynamics, the model employs the semiclassical approximation to the phase of the full quantum propagator in the exit channel. By comparison with the exact numerical solution of the time-dependent Schrödinger equation for strong-field ionization of hydrogen, we show that for suitable choices of the momentum distribution after the first tunneling step, the model yields good quantitative agreement with the full quantum simulation. The two-dimensional photoelectron momentum distributions, the energy spectra, and the angular distributions are found to be in good agreement with the corresponding quantum results. Specifically, the model quantitatively reproduces the fanlike interference patterns in the low-energy part of the two-dimensional momentum distributions, as well as the modulations in the photoelectron angular distributions.

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