Intercombination transition rates in N+

Xiaozhi Shen, Juan Liu, Cuicui Sang, and Per Jönsson
Phys. Rev. A 97, 012510 – Published 22 January 2018

Abstract

Accurate intercombination transition rates (A), arising from the 2s22pnl (n = 3, 4, 5; l = s,p,d) and 2s2p3 configurations of N+, are reported. Wavefunctions for the studied states in N+ are determined using the multiconfiguration Dirac-Hartree-Fock (MCDHF) method and account for the effects of valence, core-valence (CV), and core-core (CC) correlations. It is found that the combined CV and CC correlation effects are important for accurate predictions of intercombination rates of N+. A strong spin-orbit mixing between the states P1o3 and P1o1 of 2s22p3s causes that the intercombination rates on its states P1o1,3 are exceedingly sensitive to electron correlations and other corrections. The strong visible intercombination lines of N+ arise from the 2s22p3s2s22p3p and 2s22p3p2s22p3d transitions. There are also strong infrared and ultraviolet intercombination lines that have important applications in plasma diagnosis of radiative cooling coefficient and abundance. Different systematic methods are used to evaluate the intercombination rates and their uncertainties. For relatively strong lines (gf>0.01) of 2s22p3l(l = s,p,d), 2s22p4l(l = s,p,d) and 2s22p5s the uncertainties are separately estimated to be within 7%, 12%, and 20%. The rates of extremely weak lines, gf<106, are of interests in the temperature and density diagnostic in nebulae, but are remarkably difficult to accurately calculate. The present calculations have included appropriate electron correlations to deal with them and provide guidance for further studies.

  • Figure
  • Figure
  • Received 20 November 2017

DOI:https://doi.org/10.1103/PhysRevA.97.012510

©2018 American Physical Society

Physics Subject Headings (PhySH)

Atomic, Molecular & OpticalPlasma Physics

Authors & Affiliations

Xiaozhi Shen*

  • School of Mechanical and Electrical Engineering, Handan University, Handan 056005, China and School of Physics and Nuclear Energy Engineering, Beihang University, Beijing 100191, China

Juan Liu

  • School of Mathematics and Physics, Handan University, Handan 056005, China and School of Information, Renmin University of China, Beijing 100872, China

Cuicui Sang

  • College of Science, Lanzhou University of Technology, Lanzhou 730050, China and Department of Physics, Qinghai Normal University, Xining 81001, China

Per Jönsson

  • Materials Science and Applied Mathematics, Malmö University, 205 06 Malmö, Sweden

  • *shenxz@buaa.edu.cn
  • juanliu@ruc.edu.cn
  • per.jonsson@mah.se

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Issue

Vol. 97, Iss. 1 — January 2018

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