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Fig. 4

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Comparison of effective collision strengths for Ar13+. Left: all excitations among the 15 levels of the n = 2 configurations at the temperature (Te = 4.0 × 106 K) of peak fractional abundance in ionization equilibrium. The “ × ” symbol corresponds to the 2s22p   2P3/2 − 2p3   2P3/2 (1–15) excitation shown in the righthand panel, which is linked for the two different previous calculations. Double-horizontal lines correspond to agreement within 20%. Right: the effective collision strength of the 1–15 transition as a function of temperature (K). ZGP94 and LBL10 correspond to the Breit-Pauli R-matrix works of Zhang et al. (1994) and Ludlow et al. (2010), respectively.

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