Table A.1
Line data for spectral lines used in the abundance analyses.
Wavelength | Transition | Jlow–Jupp | E low | log gf a | Ref. | Γ6 | ||||
[Å] | [eV] | [dex] | σ [a.u.] | α | ||||||
|
||||||||||
2103.017 | 3p 2P0 | – 14d 2D | 3/2 | –5/2 | 0.014 | −1.619 | 1 | |||
2103.024 | 3p 2P0 | – 14d 2D | 3/2 | –3/2 | 0.014 | −2.566 | 1 | |||
2118.312 | 3p 2P0 | – 11d 2D | 1/2 | –3/2 | 0.000 | −1.557 | ± 0.10 | 2 | ||
2134.732 | 3p 2P0 | – 10d 2D | 3/2 | –5/2 | 0.014 | −1.129 | ± 0.10 | 2 | ||
2134.760 | 3p 2P0 | – 10d 2D | 3/2 | –3/2 | 0.014 | −2.090 | ± 0.18 | 2 | ||
2145.555 | 3p 2P0 | – 9d 2D | 1/2 | –3/2 | 0.000 | −1.244 | ± 0.10 | 2 | ||
2174.027 | 3p 2P0 | – 8d 2D | 3/2 | –5/2 | 0.014 | −0.824 | ± 0.10 | 2 | ||
2174.113 | 3p 2P0 | – 8d 2D | 3/2 | –3/2 | 0.014 | −1.778 | ± 0.30 | 2 | ||
2204.590 | 3p 2P0 | – 8s 2S | 3/2 | –1/2 | 0.014 | −2.293 | ± 0.10 | 2 | ||
2204.660 | 3p 2P0 | – 7d 2D | 1/2 | –3/2 | 0.000 | −0.895 | ± 0.06 | 2 | 2340 | 1.07 |
2210.046 | 3p 2P0 | – 7d 2D | 3/2 | –5/2 | 0.014 | −0.641 | ± 0.06 | 2 | 2340 | 1.07 |
2210.130 | 3p 2P0 | – 7d 2D | 3/2 | –3/2 | 0.014 | −1.595 | ± 0.06 | 2 | 2340 | 1.07 |
2269.096 | 3p 2P0 | – 6d 2D | 3/2 | –5/2 | 0.014 | −0.454 | ± 0.04 | 2, 3 | 2084 | 0.960 |
2269.220 | 3p 2P0 | – 6d 2D | 3/2 | –3/2 | 0.014 | −1.409 | ± 0.06 | 3 | 2084 | 0.960 |
2367.052 | 3p 2P0 | – 5d 2D | 1/2 | –3/2 | 0.000 | −0.592 | ± 0.06 | 2 | ||
2372.070 | 3p 2P0 | – 6s 2S | 1/2 | –1/2 | 0.000 | −2.012 | ± 0.10 | 2 | ||
2373.124 | 3p 2P0 | – 5d 2D | 3/2 | –5/2 | 0.014 | −0.337 | ± 0.04 | 2 | ||
2373.349 | 3p 2P0 | – 5d 2D | 3/2 | –3/2 | 0.014 | −1.291 | ± 0.06 | 2 | ||
2567.984 | 3p 2P0 | – 4d 2D | 1/2 | –3/2 | 0.000 | −1.119 | ± 0.04 | 3 | 1385 | 0.249 |
2575.094 | 3p 2P0 | – 4d 2D | 3/2 | –5/2 | 0.014 | −0.668 | ± 0.06 | 2, 3 | 1387 | 0.249 |
2575.393 | 3p 2P0 | – 4d 2D | 3/2 | –3/2 | 0.014 | −1.623 | ± 0.06 | 3 | 1385 | 0.249 |
2652.484 | 3p 2P0 | – 5s 2S | 1/2 | –1/2 | 0.000 | −1.523 | ± 0.04 | 4 | 2150 | 0.307 |
2660.392 | 3p 2P0 | – 5s 2S | 3/2 | –1/2 | 0.014 | −1.219 | ± 0.04 | 4 | 2150 | 0.307 |
3082.153 | 3p 2P0 | – 3d 2D | 1/2 | –3/2 | 0.000 | −0.476 | ± 0.025 | 2, 3 | 576 | 0.292 |
3092.710 | 3p 2P0 | – 3d 2D | 3/2 | –5/2 | 0.014 | −0.202 | ± 0.025 | 2, 5 | 576 | 0.292 |
3092.839 | 3p 2P0 | – 3d 2D | 3/2 | –3/2 | 0.014 | −1.175 | ± 0.04 | 2 | 576 | 0.292 |
3944.006 | 3p 2P0 | – 4s 2S | 1/2 | –1/2 | 0.000 | −0.635 | ± 0.025 | 2, 5 | 655 | 0.243 |
3961.520 | 3p 2P0 | – 4s 2S | 3/2 | –1/2 | 0.014 | −0.333 | ± 0.025 | 2 | 655 | 0.243 |
6696.015 | 4s 2S | – 5p 2P0 | 1/2 | –3/2 | 3.143 | −1.569 | ± 0.06 | 2 | 1860 | 0.226 |
6698.672 | 4s 2S | – 5p 2P0 | 1/2 | –1/2 | 3.143 | −1.870 | ± 0.06 | 2 | 1860 | 0.226 |
7835.309 | 3d 2D | – 6f 2F0 | 3/2 | –5/2 | 4.022 | −0.689 | ± 0.04 | 2 | 3850 | 1.60 |
7836.134 | 3d 2D | – 6f 2F0 | 5/2 | –5/2 | 4.022 | −1.834 | ± 0.06 | 2 | 3850 | 1.60 |
7836.134 | 3d 2D | – 6f 2F0 | 5/2 | –7/2 | 4.022 | −0.534 | ± 0.025 | 2 | 3850 | 1.60 |
8772.866 | 3d 2D | – 5f 2F0 | 3/2 | –5/2 | 4.022 | −0.349 | ± 0.025 | 2 | 2983 | 0.344 |
8773.895 | 3d 2D | – 5f 2F0 | 5/2 | –5/2 | 4.022 | −1.495 | ± 0.06 | 2 | 2983 | 0.344 |
8773.895 | 3d 2D | – 5f 2F0 | 5/2 | –7/2 | 4.022 | −0.192 | ± 0.025 | 2 | 2983 | 0.344 |
8912.900 | 4p 2P0 | – 6d 2D | 1/2 | –3/2 | 4.085 | −1.963 | ± 0.06 | 2 | ||
8923.555 | 4p 2P0 | – 6d 2D | 3/2 | –5/2 | 4.087 | −1.709 | ± 0.06 | 2 | ||
8925.503 | 4p 2P0 | – 6d 2D | 3/2 | –3/2 | 4.087 | −2.663 | 2 | |||
10768.363 | 4p 2P0 | – 5d 2D | 1/2 | –3/2 | 4.085 | −2.020 | ± 0.06 | 2 | ||
10782.046 | 4p 2P0 | – 5d 2D | 3/2 | –5/2 | 4.087 | −1.764 | ± 0.06 | 2 | ||
10786.770 | 4p 2P0 | – 5d 2D | 3/2 | –3/2 | 4.087 | −2.719 | ± 0.10 | 2 | ||
10872.975 | 4p 2P0 | – 6s 2S | 1/2 | –1/2 | 4.085 | −1.326 | ± 0.06 | 2 | ||
10891.732 | 4p 2P0 | – 6s 2S | 3/2 | –1/2 | 4.087 | −1.027 | ± 0.04 | 2 | ||
13123.416 | 4s 2S | – 4p 2P0 | 1/2 | –3/2 | 3.143 | 0.219 | ± 0.013 | 2 | 815 | 0.223 |
13150.753 | 4s 2S | – 4p 2P0 | 1/2 | –1/2 | 3.143 | −0.083 | ± 0.013 | 2 | 815 | 0.223 |
16718.974 | 4p 2P0 | – 4d 2D | 1/2 | –3/2 | 4.085 | 0.220 | ± 0.013 | 2 | 1147 | 0.311 |
16750.519 | 4p 2P0 | – 4d 2D | 3/2 | –5/2 | 4.087 | 0.474 | ± 0.013 | 2 | 1147 | 0.311 |
16763.369 | 4p 2P0 | – 4d 2D | 3/2 | –3/2 | 4.087 | −0.480 | ± 0.025 | 2 | 1147 | 0.311 |
21093.082 | 4p 2P0 | – 5s 2S | 1/2 | –1/2 | 4.085 | −0.398 | ± 0.025 | 4 | 1838 | 0.279 |
21163.803 | 4p 2P0 | – 5s 2S | 3/2 | –1/2 | 4.087 | −0.093 | ± 0.025 | 4 | 1838 | 0.279 |
21208.171 | 4f 2F0 | – 7g 2G | 7/2 | –9/2 | 5.123 | −0.307 | 2 | 3260 | 1.68 | |
21208.171 | 4f 2F0 | – 7g 2G | 5/2 | –7/2 | 5.123 | −0.461 | 2 | 3260 | 1.68 | |
21208.191 | 4f 2F0 | – 7g 2G | 7/2 | –7/2 | 5.123 | −1.608 | 2 | 3260 | 1.68 | |
123349.6b | 6h 2H0 | – 7i 2I | 5.614 | 1.647 | 6 | 4830 | 1.84 |
Notes. Only lines used in the spectrum analyses are listed.
Uncertainties (90%) to the transition probabilities are taken from Kelleher & Podobedova (2008), when available.
Multiplet components with identical wavelength have been merged. We adopt the wavelength measured from the solar spectrum by Brault & Noyes (1983), and the oscillator strength has been adjusted accordingly.
Reference. (1) Wiese et al. (1969); (2) TOPbase: Mendoza et al. (1995) and C. Mendoza, W. Eissner, M. Le Dourneuf, & C. J. Zeippen (unpublished); (3) Davidson et al. (1990); (4) Vujnović et al. (2002); (5) Tachiev & Froese Fischer (2002); (6) Kurucz (2012, online data; http://kurucz.harvard.edu/atoms/1300/).
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