Biharmonic (ω, 2ω) ionization of atoms by elliptically-polarized light. Carving the photoelectron angular distributions

The biharmonic ( ω , 2 ω ) photoionization of atomic inner-shell electrons opens up new perspectives for studying nonlinear light–atom interactions at intensities in the transition regime from weak to strong-field physics. In particular, the control of the frequency and polarization of biharmonic be...

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Main Authors: S Fritzsche, J Hofbrucker
Format: Article
Language:English
Published: IOP Publishing 2022-01-01
Series:New Journal of Physics
Subjects:
Online Access:https://doi.org/10.1088/1367-2630/ac9803
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author S Fritzsche
J Hofbrucker
author_facet S Fritzsche
J Hofbrucker
author_sort S Fritzsche
collection DOAJ
description The biharmonic ( ω , 2 ω ) photoionization of atomic inner-shell electrons opens up new perspectives for studying nonlinear light–atom interactions at intensities in the transition regime from weak to strong-field physics. In particular, the control of the frequency and polarization of biharmonic beams enables one to carve the photoelectron angular distribution and to enhance the resolution of ionization measurements by the (simultaneous) absorption of photons. Apart from its quite obvious polarization dependence, the photoelectron angular distributions are sensitive also to the (relative) intensity, the phase difference and the temporal structure of the incoming beam components, both at resonant and nonresonant frequencies. Here, we describe and analyze several characteristic features of biharmonic ionization in the framework of second-order perturbation theory and (so-called) ionization pathways , as they are readily derived from the interaction of inner-shell electrons with the electric-dipole field of the incident beam. We show how the photoelectron angular distribution and elliptical dichroism can be shaped in rather an unprecedented way by just tuning the properties of the biharmonic field. Since such fields are nowadays accessible from high-harmonic sources or free-electron lasers, these and further investigations might help extract photoionization amplitudes or the phase difference of incoming beams.
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spelling doaj.art-dc606dc0cb44488daaa12209c45448232023-08-09T14:09:23ZengIOP PublishingNew Journal of Physics1367-26302022-01-01241010303110.1088/1367-2630/ac9803Biharmonic (ω, 2ω) ionization of atoms by elliptically-polarized light. Carving the photoelectron angular distributionsS Fritzsche0https://orcid.org/0000-0003-3101-2824J Hofbrucker1https://orcid.org/0000-0002-5917-3649Helmholtz-Institut Jena , D-07743 Jena, Germany; GSI Helmholtzzentrum für Schwerionenforschung GmbH , D-64291 Darmstadt, Germany; Theoretisch-Physikalisches Institut, Friedrich-Schiller-Universität Jena , D-07743 Jena, GermanyHelmholtz-Institut Jena , D-07743 Jena, Germany; GSI Helmholtzzentrum für Schwerionenforschung GmbH , D-64291 Darmstadt, GermanyThe biharmonic ( ω , 2 ω ) photoionization of atomic inner-shell electrons opens up new perspectives for studying nonlinear light–atom interactions at intensities in the transition regime from weak to strong-field physics. In particular, the control of the frequency and polarization of biharmonic beams enables one to carve the photoelectron angular distribution and to enhance the resolution of ionization measurements by the (simultaneous) absorption of photons. Apart from its quite obvious polarization dependence, the photoelectron angular distributions are sensitive also to the (relative) intensity, the phase difference and the temporal structure of the incoming beam components, both at resonant and nonresonant frequencies. Here, we describe and analyze several characteristic features of biharmonic ionization in the framework of second-order perturbation theory and (so-called) ionization pathways , as they are readily derived from the interaction of inner-shell electrons with the electric-dipole field of the incident beam. We show how the photoelectron angular distribution and elliptical dichroism can be shaped in rather an unprecedented way by just tuning the properties of the biharmonic field. Since such fields are nowadays accessible from high-harmonic sources or free-electron lasers, these and further investigations might help extract photoionization amplitudes or the phase difference of incoming beams.https://doi.org/10.1088/1367-2630/ac9803biharmonic ionizationtwo-photon ionizationatomic structure theorycircular dichroismelliptical dichroismphotoelectron angular distribution
spellingShingle S Fritzsche
J Hofbrucker
Biharmonic (ω, 2ω) ionization of atoms by elliptically-polarized light. Carving the photoelectron angular distributions
New Journal of Physics
biharmonic ionization
two-photon ionization
atomic structure theory
circular dichroism
elliptical dichroism
photoelectron angular distribution
title Biharmonic (ω, 2ω) ionization of atoms by elliptically-polarized light. Carving the photoelectron angular distributions
title_full Biharmonic (ω, 2ω) ionization of atoms by elliptically-polarized light. Carving the photoelectron angular distributions
title_fullStr Biharmonic (ω, 2ω) ionization of atoms by elliptically-polarized light. Carving the photoelectron angular distributions
title_full_unstemmed Biharmonic (ω, 2ω) ionization of atoms by elliptically-polarized light. Carving the photoelectron angular distributions
title_short Biharmonic (ω, 2ω) ionization of atoms by elliptically-polarized light. Carving the photoelectron angular distributions
title_sort biharmonic ω 2ω ionization of atoms by elliptically polarized light carving the photoelectron angular distributions
topic biharmonic ionization
two-photon ionization
atomic structure theory
circular dichroism
elliptical dichroism
photoelectron angular distribution
url https://doi.org/10.1088/1367-2630/ac9803
work_keys_str_mv AT sfritzsche biharmonicō2ōionizationofatomsbyellipticallypolarizedlightcarvingthephotoelectronangulardistributions
AT jhofbrucker biharmonicō2ōionizationofatomsbyellipticallypolarizedlightcarvingthephotoelectronangulardistributions