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    Control of attosecond light polarization in two-color bicircular fields

    Á. Jiménez-Galán1,*, N. Zhavoronkov1, D. Ayuso1, F. Morales1, S. Patchkovskii1, M. Schloz1, E. Pisanty1,2, O. Smirnova1,3, and M. Ivanov1,4,5

    • 1Max-Born Institute for Nonlinear Optics and Short Pulse Spectroscopy, Max-Born-Straße 2A, D-12489 Berlin, Germany
    • 2ICFO–Institut de Ciències Fotòniques, The Barcelona Institute of Science and Technology, 08860 Castelldefels (Barcelona), Spain
    • 3Technische Universität Berlin, Ernst-Ruska-Gebäude, Hardenbergstraße 36A, 10623 Berlin, Germany
    • 4Department of Physics, Imperial College London, South Kensington Campus, SW72AZ London, United Kingdom
    • 5Institute für Physik, Humboldt-Universität zu Berlin, Newtonstraße 15, D-12489 Berlin, Germany

    • *jimenez@mbi-berlin.de

    Phys. Rev. A 97, 023409 – Published 8 February, 2018

    DOI: https://doi.org/10.1103/PhysRevA.97.023409

    Abstract

    We develop theoretically and confirm both numerically and experimentally a comprehensive analytical model which describes the propensity rules in the emission of circularly polarized high harmonics by systems driven by two-color counter-rotating fields, a fundamental and its second harmonic. We identify and confirm the three propensity rules responsible for the contrast between the 3N+1 and 3N+2 harmonic lines in the HHG spectra of noble gas atoms. We demonstrate how these rules depend on the laser parameters and how they can be used in the experiment to shape the polarization properties of the emitted attosecond pulses.

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