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Direct double ionization of the Ar+ M shell by a single photon

A. Müller1,*, A. L. D. Kilcoyne2, R. A. Phaneuf3, K. Holste4, S. Schippers4, and A. S. Kheifets5

  • 1Institut für Atom- und Molekülphysik, Justus-Liebig-Universität Gießen, 35392 Giessen, Germany
  • 2Advanced Light Source, Lawrence Berkeley National Laboratory, Berkeley, California 94720-8225, USA
  • 3Department of Physics, University of Nevada, Reno, Nevada 89557-0058, USA
  • 4I. Physikalisches Institut, Justus-Liebig-Universität Gießen, 35392 Giessen, Germany
  • 5Research School of Physics, The Australian National University, Canberra, ACT 2600, Australia

  • *Alfred.Mueller@iamp.physik.uni-giessen.de

Phys. Rev. A 103, L031101 – Published 17 March, 2021

DOI: https://doi.org/10.1103/PhysRevA.103.L031101

Abstract

Direct double ionization of the Ar+(3p−1) ion by a single photon is investigated both experimentally and theoretically. The photon-ion merged-beams technique was employed at the Advanced Light Source in Berkeley, USA, to measure absolute cross sections in the energy range from 60 to 150 eV. In this range, three contributions to the double ionization of Ar+ are to be expected: the removal of two 3p electrons, of a 3s and a 3p electron, and of two 3s electrons. Among the possible mechanisms leading to double ionization, the TS1 (two-step one) process dominates in the near-threshold region. In TS1, a photoelectron is ejected and, on its way out, knocks out a secondary electron. This two-step mechanism is treated theoretically by multiplying the calculated cross section for direct single photoionization of a given subshell with the calculated (e,2e) ionization probability for the ejected photoelectron to knock off a secondary electron. The calculated cross section is in very good agreement with the experiment.

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