High-order above-threshold ionization beyond the electric dipole approximation

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Original languageEnglish
Article number094005
JournalJournal of Physics B: Atomic, Molecular and Optical Physics
Volume51
Issue number9
Early online date17 Apr 2018
Publication statusPublished - 14 May 2018

Abstract

Photoelectron momentum distributions from strong-field ionization are calculated by numerical solution of the one-electron time-dependent Schrödinger equation for a model atom including effects beyond the electric dipole approximation. We focus on the high-energy electrons from rescattering and analyze their momentum component along the field propagation direction. We show that the boundary of the calculated momentum distribution is deformed in accordance with the classical three-step model including the beyond-dipole Lorentz force. In addition, the momentum distribution exhibits an asymmetry in the signal strengths of electrons emitted in the forward/backward directions. Taken together, the two non-dipole effects give rise to a considerable average forward momentum component of the order of 0.1 a.u. for realistic laser parameters.

Keywords

    non-dipole effects, rescattering, strong-field ionization, time-dependent Schrodinger equation

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High-order above-threshold ionization beyond the electric dipole approximation. / Brennecke, Simon; Lein, Manfred.
In: Journal of Physics B: Atomic, Molecular and Optical Physics, Vol. 51, No. 9, 094005, 14.05.2018.

Research output: Contribution to journalArticleResearchpeer review

Brennecke S, Lein M. High-order above-threshold ionization beyond the electric dipole approximation. Journal of Physics B: Atomic, Molecular and Optical Physics. 2018 May 14;51(9):094005. Epub 2018 Apr 17. doi: 10.1088/1361-6455/aab91f, 10.15488/3772
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AU - Brennecke, Simon

AU - Lein, Manfred

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AB - Photoelectron momentum distributions from strong-field ionization are calculated by numerical solution of the one-electron time-dependent Schrödinger equation for a model atom including effects beyond the electric dipole approximation. We focus on the high-energy electrons from rescattering and analyze their momentum component along the field propagation direction. We show that the boundary of the calculated momentum distribution is deformed in accordance with the classical three-step model including the beyond-dipole Lorentz force. In addition, the momentum distribution exhibits an asymmetry in the signal strengths of electrons emitted in the forward/backward directions. Taken together, the two non-dipole effects give rise to a considerable average forward momentum component of the order of 0.1 a.u. for realistic laser parameters.

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