Electron-correlation effects on the 3C to 3D line-intensity ratio in the Ne-like ions Ar8+ to Kr26+

Juan A. Santana, Jaan K. Lepson, Elmar Träbert, and Peter Beiersdorfer
Phys. Rev. A 91, 012502 – Published 7 January 2015

Abstract

We present a theoretical and experimental investigation of the 3d2p resonance to the intercombination line ratio in low- to mid-Z neonlike ions of astrophysical interest, i.e., of the 2p1/22p3/243d3/21P1o2p61S0 and 2p1/222p3/233d5/23D1o2p61S0 transitions commonly labeled 3C and 3D, respectively. In particular, we have employed the configuration-interaction method with three different numbers of basis states and the many-body perturbation theory method to calculate oscillator strengths and energies for neonlike ions from Z=18 to 36. Combining our calculations with a systematic study of previous works in the literature, we show that these methods can predict accurate and converged energies for these transitions. We also find convergence for the oscillator strengths, but the ratio of oscillator strengths, which can be compared to experimental values of the relative intensity ratios of these lines, appears to converge to values higher than measured. We speculate that this is due to the role of electron-electron correlations. While the amount of electron correlations associated with the intercombination line 3D appears to be well described, it seems that the contributions from highly excited states are not sufficiently accounted for in the case of the resonance line 3C. In order to augment the body of available experimental data for neonlike ions, we present a measurement of the 3C and 3D lines in neonlike Ar8+. We report a wavelength of 41.480±0.001 Å for line 3C and 42.005±0.001 Å for line 3D. The intensity ratio of the two lines was determined to be I(3C)/I(3D)=11.32±1.40.

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  • Received 11 August 2014

DOI:https://doi.org/10.1103/PhysRevA.91.012502

©2015 American Physical Society

Authors & Affiliations

Juan A. Santana1,*, Jaan K. Lepson1, Elmar Träbert2,3, and Peter Beiersdorfer1,2,†

  • 1Space Science Laboratory, University of California, Berkeley, 7 Gauss Way, Berkeley, California 94720, USA
  • 2Physics Division, Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94551, USA
  • 3Astronomisches Institut, Ruhr-Universität Bochum, D-44780 Bochum, Germany

  • *Present address: Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA.
  • beiersdorfer1@llnl.gov

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Vol. 91, Iss. 1 — January 2015

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