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Table 3
Stellar characterisation.
Parameter | Value | Source |
---|---|---|
Teff ∕K | 3548 ± 70 | HIRES |
3600 ± 150 | SED+Mann | |
3533 ± 45 | EXOFASTv2 | |
3570 ± 100 | TRES | |
[Fe/H] | −0.24 ± 0.09 | HIRES |
−0.5 ± 0.5 | SED+Mann | |
−0.03 ± 0.18 | TRES | |
M* ∕M⊙ | 0.45 ± 0.03 | Mann |
0.447 ± 0.023 | EXOFASTv2 | |
0.48 ± 0.10 | TRES | |
R* ∕R⊙ | 0.43 ± 0.02 | HIRES |
0.420 ± 0.037 | SED+Mann | |
0.428 ± 0.012 | EXOFASTv2 | |
0.43 ± 0.10 | TRES | |
0.42 ± 0.02 | This work | |
log g / dex | 4.85 ± 0.08 | SED+Mann |
4.826 ± 0.024 | EXOFASTv2 | |
4.78 ± 0.10 | TRES | |
4.85 ± 0.05 | This work | |
ρ* ∕g cm−3 | 8.7 ± 2.3 | SED+Mann |
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EXOFASTv2 | |
8.99 ± 1.25 | This work | |
Spectral type | M3 | TRES |
Fbol / rm erg s−1 cm−2 | (6.72 ± 0.16) × 10−10 | SED+Mann |
Notes. SED+Mannuse the empirical relations of Mann et al. (2019). Parameters in bold are the adopted stellar values. We use the SED+Mannmass and metallicity as priors in our global analysis presented in Sect. 5.1.2, where we also derive the other parameters that appear in bold.
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