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Dielectronic and Trielectronic Recombination Rate Coefficients of Be-like Ar14+

  • Authors: Z. K. Huang, W. Q. Wen, X. Xu, S. Mahmood, S. X. Wang, H. B. Wang, L. J. Dou, N. Khan, N. R. Badnell, S. P. Preval, S. Schippers, T. H. Xu, Y. Yang, K. Yao, W. Q. Xu, X. Y. Chuai, X. L. Zhu, D. M. Zhao, L. J. Mao, X. M. Ma, J. Li, R. S. Mao, Y. J. Yuan, B. Wu, L. N. Sheng, J. C. Yang, H. S. Xu, L. F. Zhu, and X. Ma

2018 The Astrophysical Journal Supplement Series 235 2.

  • Provider: AAS Journals

Caption: Figure 3.

Plasma rate coefficients of Be-like Ar14+ as a function of the electron temperature. The solid red line is the experimentally derived ΔN = 0 DR and TR rate coefficients. The theoretical results deduced from the AUTOSTRUCTURE code for ΔN = 0 DR and for TR are shown as a dotted black line and a dashed–dotted blue line, respectively. The calculated sum of DR and TR is shown as a short-dashed red line. The experimentally derived field-ionization-free plasma rate coefficient is shown as a gray area. The approximate temperature ranges where Ar14+ is expected to form in photoionized plasmas and collisionally ionized plasmas are indicated by vertical dashed bars and associated arrows (Kallman & Bautista 2001; Bryans et al. 2009).

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