Table 3
Internal errors on abundance measurements due to uncertainties in stellar parameters.
TOI-1430 | Teff = 5075 K | log g = 4.55 dex | ξ = 0.79 km/s | [Fe/H]=−0.02 dex |
---|---|---|---|---|
ΔTeff = −/ + 70 K | Δ log g = −/ + 0.10 dex | Δξ = −/ + 0.10 km/s | Δ[Fe/H]= −/ + 0.10 dex | |
[Fe I/H] | −0.04/0.05 | 0.01/−0.01 | 0.03/−0.02 | .../... |
[Fe II/H] | 0.07/0.01 | 0.01/0.09 | 0.06/0.02 | .../... |
[C I/H] | 0.05/−0.06 | −0.04/0.06 | 0.00/0.00 | 0.01/0.01 |
[O I/H] | 0.08/−0.09 | −0.05/0.08 | 0.00/0.00 | −0.03/0.05 |
[Na I/H] | −0.05/0.05 | 0.02/−0.01 | 0.01/−0.01 | −0.01/0.01 |
[Mg I/H] | −0.02/0.03 | 0.02/−0.01 | 0.01/0.00 | −0.02/0.03 |
[Al I/H] | −0.04/0.04 | 0.01/−0.01 | 0.01/−0.01 | −0.01/0.01 |
[Si I/H] | 0.03/−0.02 | −0.01/0.02 | 0.00/0.00 | −0.02/0.03 |
[S I/H] | 0.04/−0.05 | −0.04/0.05 | 0.00/0.00 | 0.01/0.01 |
[Ca I/H] | −0.06/0.07 | 0.04/−0.04 | 0.02/−0.01 | −0.02/0.02 |
[Ti I/H] | −0.07/0.06 | 0.00/−0.02 | 0.02/−0.02 | 0.00/−0.01 |
[Ti II/H] | 0.04/0.02 | 0.00/0.08 | 0.06/0.01 | 0.00/0.07 |
[Cr I/H] | −0.06/0.07 | 0.02/−0.02 | 0.02/−0.02 | −0.02/0.02 |
[Cr II/H] | 0.04/−0.04 | −0.04/0.06 | 0.01/−0.01 | −0.02/0.04 |
[Ni I/H] | 0.00/0.01 | −0.01/0.02 | 0.02/−0.01 | −0.03/0.04 |
[Zn I/H] | 0.02/−0.01 | 0.00/0.02 | 0.03/−0.02 | −0.03/0.05 |
[Y II/H] | 0.00/0.01 | −0.03/0.04 | 0.04/−0.03 | −0.03/0.05 |
[Zr II/H] | 0.00/0.01 | −0.04/0.04 | 0.03/−0.02 | −0.04/0.05 |
[Ce I/H] | −0.01/0.01 | −0.04/0.05 | 0.01/0.00 | −0.03/0.04 |
[Nd II/H] | −0.01/0.02 | −0.04/0.05 | 0.01/0.00 | −0.04/0.04 |
TOI-5398 | Teff = 6000 K | log g = 4.44 dex | ξ = 1.12 km/s | [Fe/H]=0.09 dex |
ΔTeff = −/ + 70 K | Δ log g = −/ + 0.10 dex | Δξ = −/ + 0.10 km/s | Δ[Fe/H]= −/ + 0.10 dex | |
[Fe I/H] | −0.05/0.05 | 0.00/−0.01 | 0.02/−0.02 | .../... |
[Fe II/H] | 0.03/−0.01 | −0.03/0.04 | 0.03/−0.02 | .../... |
[C I/H] | 0.05/−0.03 | −0.03/0.03 | 0.00/0.00 | 0.00/0.00 |
[O I/H] | 0.07/−0.04 | −0.04/0.04 | 0.01/−0.01 | −0.04/0.03 |
[Na I/H] | −0.03/0.04 | 0.01/−0.02 | 0.01/−0.01 | 0.00/0.00 |
[Mg I/H] | −0.02/0.03 | 0.01/−0.01 | 0.01/−0.01 | 0.00/0.00 |
[Al I/H] | −0.02/0.03 | 0.00/0.00 | 0.00/0.00 | 0.00/0.00 |
[Si I/H] | −0.01/0.02 | 0.00/0.00 | 0.01/0.00 | 0.00/0.01 |
[S I/H] | 0.04/−0.02 | −0.02/0.03 | 0.00/0.00 | 0.00/0.00 |
[Ca I/H] | −0.04/0.05 | 0.02/−0.02 | 0.02/−0.02 | 0.00/0.00 |
[Ti I/H] | −0.06/0.07 | 0.00/0.00 | 0.02/−0.01 | 0.00/0.00 |
[Ti II/H] | 0.01/0.01 | −0.02/0.05 | 0.04/−0.01 | −0.02/0.04 |
[Cr I/H] | −0.05/0.05 | 0.00/0.00 | 0.02/−0.02 | 0.00/0.00 |
[Cr II/H] | 0.03/−0.01 | −0.03/0.04 | 0.02/−0.02 | −0.02/0.02 |
[Ni I/H] | −0.03/0.04 | 0.00/0.00 | 0.01/−0.01 | 0.00/0.00 |
[Zn I/H] | −0.01/0.02 | −0.01/0.00 | 0.05/−0.05 | −0.02/0.02 |
[Y II/H] | 0.00/0.01 | −0.04/0.04 | 0.04/−0.04 | −0.03/0.03 |
[Zr II/H] | 0.00/0.01 | −0.04/0.04 | 0.02/−0.02 | −0.03/0.03 |
[Ce I/H] | −0.01/0.02 | −0.04/0.04 | 0.01/−0.01 | −0.03/0.03 |
[Nd II/H] | −0.01/0.02 | −0.04/0.04 | 0.00/−0.01 | −0.03/0.03 |
Notes. Measurements were done for TOI-1430 (for all elements but Fe I, Fe II, Ti I and Ti II which refer to TOI-5082) and TOI-5398 (for all elements but Fe I, Fe II, Ti I and Ti II which refer to TOI-1136), respectively the coolest and the warmest stars in our sample. The values in table refer to the differences between the abundances obtained with (− and +) and without the uncertainties in stellar parameters.
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