Table 1
Line parameters adopted in the abundance analysis of HD 84937 and HD 140283.
Spec | λair (nm) | χ (eV) | log gf | log γrad | σ | α |
---|---|---|---|---|---|---|
Mg I | 416.73 | 4.3458 | −0.746 | 8.69 | 5296 | 0.508 |
Mg I | 457.11 | 0.0000 | −5.732 | 6.00 | 222 | 0.253 |
Mg I | 470.30 | 4.3458 | −0.456 | 8.70 | 2827 | 0.264 |
Mg I | 473.00 | 4.3458 | −2.379 | 8.68 | 5928 | 0.435 |
Mg I | 516.73 | 2.7091 | −0.854 | 8.02 | 731 | 0.240 |
Mg I | 517.27 | 2.7116 | −0 363 | 8.02 | 731 | 0.240 |
Mg I | 518.36 | 2.7166 | −0.168 | 8.02 | 731 | 0.240 |
Mg I | 552.84 | 4.3458 | −0.547 | 8.69 | 1461 | 0.309 |
Mg I | 571.11 | 4.3458 | −1.742 | 8.69 | 1841 | 0.120 |
Mg I | 880.67 | 4.3458 | −0.144 | 8.69 | 530 | 0.277 |
Mg II | 448.11 | 8.8637 | +0.749 | 8.85 | – | – |
Mg II | 448.12 | 8.8637 | −0.553 | 8.85 | – | – |
Mg II | 448.13 | 8.8638 | +0.594 | 8.85 | – | – |
Notes. Oscillator strengths for Mg I lines come from Pehlivan Rhodin et al. (2017), with preference given to experimental values where available except for the 571 .1 nm line (theoretical value was adopted); for the 457.1 nm line, the theoretical value from Jönsson & Froese Fischer (1997) was used instead. As discussed in the text, the radiative transfer calculations assumed log gf = −5.397 for the 457.1 nm line, and log gf = −1.842 for the 571.1 nm. Oscillator strengths for the Mg II line comes from Froese Fischer et al. (2006) via NiST (Ralchenko & Kramida 2020). ABO broadening parameters (e.g. Barklem 2016a) obtained via interpolating extended tables at https://github.com/barklem/abo-cross with the value for the Mg I 473.0 nm line taken from the edge of the corresponding table.
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