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Table 2:

Selected Na IX satellite lines excited by dielectronic recombination: data from the Cowan HFR code.

Wavelength (Å)a
Line labelb Transition $B_{\rm sat}$ (s-1)c $E_{\rm sat}$ (Ry)
11.043 d15 $\rm 1s^2 3p~ ^2P_{1/2} {-} 1{\rm s} 2p 3p~ (^1P)~^2D_{3/2}$ 3.33(13) 73.5
11.044 d13 $\rm 1s^2 3p~ ^2P_{3/2} {-} 1{\rm s} 2p 3p~ (^1P)~^2D_{5/2}$ 5.77(13) 73.5
11.077d s $\rm 1s^2 2s~ ^2S_{1/2} {-} 1{\rm s} 2p^2~ (^3S)~^2P_{3/2}$ 4.64(12) 60.0
11.078d t $\rm 1s^2 2s~ ^2S_{1/2} {-} 1{\rm s}2s2p~(^3S)~^2P_{1/2}$ 2.90(12) 60.0
11.105 n $\rm 1s^2 2p~ ^2P_{1/2} {-} 1{\rm s} 2p^2~ ^2S_{1/2}$ 3.11(12) 60.6
11.108 m $\rm 1s^2 2p~ ^2P_{3/2} {-} 1{\rm s} 2p^2~ ^2S_{1/2}$ 8.19(12) 60.6
11.152d q $\rm 1s^2 2s~ ^2S_{1/2} {-} 1{\rm s}2s2p~(^1S)~^2P_{3/2}$ 1.66(13) 60.6
11.155d r $\rm 1s^2 2s~ ^2S_{1/2} {-} 1{\rm s}2s2p~(^1S)~^2P_{1/2}$ 9.61(12) 60.6
11.165 b $\rm 1s^2 2p~ ^2P_{1/2} {-} 1{\rm s} 2p^2~ ^2P_{3/2}$ 3.28(11) 60.6
11.168 d $\rm 1s^2 2p~ ^2P_{1/2} {-} 1{\rm s} 2p^2~ ^2P_{1/2}$ 7.12(10) 60.6
11.168 a $\rm 1s^2 2p~ ^2P_{3/2} {-} 1{\rm s} 2p^2~ ^2P_{3/2}$ 2.13(12) 60.6
11.171 c $\rm 1s^2 2p~ ^2P_{3/2} {-} 1{\rm s} 2p^2~ ^2P_{1/2}$ 3.25(10) 60.6
11.188 k $\rm 1s^2 2p~ ^2P_{1/2} {-} 1{\rm s} 2p^2~ ^2D_{3/2}$ 2.31(13) 60.6
11.191 j $\rm 1s^2 2p~ ^2P_{3/2} {-} 1{\rm s} 2p^2~ ^2D_{5/2}$ 3.70(13) 60.6
11.192 l $\rm 1s^2 2p~ ^2P_{3/2} {-} 1{\rm s} 2p^2~ ^2D_{3/2}$ 1.90(12) 60.6
11.286 e $\rm 1s^2 2p~ ^2P_{3/2} {-} 1{\rm s} 2p^2~ ^4P_{5/2}$ 1.74(10) 60.6
11.298d u $\rm 1s^2 2s~ ^2S_{1/2} {-} 1{\rm s} 2p^2~ (^3S)^4P_{3/2}$ 3.45(9) 60.0
11.300d v $\rm 1s^2 2s~ ^2S_{1/2} {-} 1{\rm s}2s2p~ (^3S)^4P_{1/2}$ 6.64(8) 60.0

Notes. (a) Wavelengths from Cowan code + 0.001 Å; (b) Notation of Gabriel (1972); Bely-Dubau et al. (1979); (c) Numbers in parentheses are powers of ten; (d) Lines also formed by inner-shell excitation.


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