Interplay between Coulomb-focusing and non-dipole effects in strong-field ionization with elliptical polarization

• Published in: Journal of physics. B, Atomic, molecular, and optical physics Atomic, molecular, and optical physics, 2018-06, Vol.51 (11), p.114001
• Main Authors: Dan k, J, Klaiber, M, Hatsagortsyan, K Z, Keitel, C H, Willenberg, B, Maurer, J, Mayer, B W, Phillips, C R, Gallmann, L, Keller, U
• Format: Article
• Language: English
• Subjects: Coulomb focusing cusp; elliptical polarization; laser magnetic field induced drift; non-dipole; rescattering; tunneling ionization
• ISSN: 0953-4075; 1361-6455
• DOI: 10.1088/1361-6455/aaba42

We study strong-field ionization and rescattering beyond the long-wavelength limit of the dipole approximation with elliptically polarized mid-IR laser pulses. Full three-dimensional photoelectron momentum distributions (PMDs) measured with velocity map imaging and tomographic reconstruction revealed an unexpected sharp ridge structure in the polarization plane (2018 Phys. Rev. A 97 013404). This thin line-shaped ridge structure for low-energy photoelectrons is correlated with the ellipticity-dependent asymmetry of the PMD along the beam propagation direction. The peak of the projection of the PMD onto the beam propagation axis is shifted from negative to positive values when the sharp ridge fades away with increasing ellipticity. With classical trajectory Monte Carlo simulations and analytical analysis, we study the underlying physics of this feature. The underlying physics is based on the interplay between the lateral drift of the ionized electron, the laser magnetic field induced drift in the laser propagation direction, and Coulomb focusing. To apply our observations to emerging techniques relying on strong-field ionization processes, including time-resolved holography and molecular imaging, we present a detailed classical trajectory-based analysis of our observations. The analysis leads to the explanation of the fine structure of the ridge and its non-dipole behavior upon rescattering while introducing restrictions on the ellipticity. These restrictions as well as the ionization and recollision phases provide additional observables to gain information on the timing of the ionization and recollision process and non-dipole properties of the ionization process.