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Photoionization and photofragmentation of singly charged positive and negative Sc3N@C80 endohedral fullerene ions

A. Müller, M. Martins, A. L. D. Kilcoyne, R. A. Phaneuf, J. Hellhund, A. Borovik, Jr., K. Holste, S. Bari, T. Buhr, S. Klumpp, A. Perry-Sassmannshausen, S. Reinwardt, S. Ricz, K. Schubert, and S. Schippers
Phys. Rev. A 99, 063401 – Published 3 June 2019

Abstract

Photoprocesses of the endohedral fullerene ions Sc3N@C80+ and Sc3N@C80 in the gas phase have been investigated in the photon energy ranges 30–50 eV and 280–420 eV. Single and double ionization as well as single ionization accompanied by the release of a C2 dimer were observed as a function of the photon energy for the positive parent ion and double detachment was measured for the negative parent ion. The emphasis of the experiments was on the specific effects of the encapsulated trimetallic nitride cluster Sc3N on the observed reactions. Clear evidence of photoexcitation near the Sc L edge is obtained with the dominating contributions visible in the one- and two-electron-removal channels. K-vacancy production in the encapsulated central nitrogen atom is seen in the single ionization of Sc3N@C80+ but is much less pronounced in the photoionization-with-fragmentation channel. Comparison of the cross sections near the carbon K edge with the corresponding channels measured previously in the photoionization of Lu3N@C80+ reveal strong similarities. Previously predicted sharp resonance features in the ionization of Sc3N@C80+ ions below the Sc M edge are not confirmed. The experiments are accompanied by quantum-chemistry calculations in the Hartree-Fock approximation and by model calculations employing density functional theory (DFT).

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  • Received 25 February 2019

DOI:https://doi.org/10.1103/PhysRevA.99.063401

©2019 American Physical Society

Physics Subject Headings (PhySH)

Atomic, Molecular & Optical

Authors & Affiliations

A. Müller1,*, M. Martins2, A. L. D. Kilcoyne3, R. A. Phaneuf4, J. Hellhund1, A. Borovik, Jr.5, K. Holste5, S. Bari6, T. Buhr5, S. Klumpp6, A. Perry-Sassmannshausen5, S. Reinwardt2, S. Ricz7, K. Schubert6, and S. Schippers5

  • 1Institut für Atom- und Molekülphysik, Justus-Liebig-Universität Gießen, Leihgesterner Weg 217, 35392 Giessen, Germany
  • 2Institut für Experimentalphysik, Universität Hamburg, Luruper Chaussee 149, 22761 Hamburg, Germany
  • 3Advanced Light Source, Lawrence Berkeley National Laboratory, 1 Cyclotron Road, M.S. 7R0222, Berkeley, California 94720-8229, USA
  • 4Department of Physics, University of Nevada, Reno, Nevada 89557-0058, USA
  • 5I. Physikalisches Institut, Justus-Liebig-Universität Gießen, Heinrich-Buff-Ring 16, 35392 Giessen, Germany
  • 6Deutsches Elektronen-Synchrotron DESY, Notkestr. 85, 22607 Hamburg, Germany
  • 7Institute for Nuclear Research, Hungarian Academy of Sciences, P.O. Box 51, 4001 Debrecen, Hungary

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

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Issue

Vol. 99, Iss. 6 — June 2019

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