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Table 3

Stellar parameters of the sample stars.

ID# Object Teff log g y ξ υ sin i ζ RV E (BV) B.C. MV Mbol Mevol R log L/L log τevol dspec dGaia(a)

kK (cgs) km s−1 mag mag mag mag M R yr pc pc
1 Sher 25 20.9 2.61 0.117 16 60 35 3.40 1.66 −1.920 −7.05 −8.97 25.5 42 5.48 6.86 5440 5740
± 0.5 0.06 0.015 2 5 5 0.1 0.03 0.34 0.34 1.7 7 0.14 0.04 700 800 420
2 HD 13854 20.5 2.62 0.111 15 57 47 3.02 0.52 −1.871 −6.91 −8.78 23.7 40 5.41 6.88 2320 2140
± 0.3 0.04 0.010 2 6 5 0.1 0.03 0.21 0.22 1.0 4 0.09 0.03 200 110 100
3 HD 14956 19.2 2.37 0.127 16 49 55 2.69 0.97 −1.722 −7.55 −9.27 27.2 57 5.60 6.81 2680 2720
± 0.3 0.04 0.010 2 7 5 0.1 0.03 0.24 0.24 1.5 7 0.10 0.03 250 150 130
4 HD 91316 21.7 2.87 0.092 15 43 62 2.81 0.09 −2.007 −6.19 −8.20 19.9 28 5.18 6.96 900 660
± 0.2 0.04 0.009 2 5 5 0.1 0.03 0.20 0.20 1.0 3 0.08 0.04 70 170 140
4a(b,c) −5.51 −7.52 10.6 20 4.90
± 0.52 0.53 5.3 5 0.21
5 HD 114199 25.6 3.42 0.119 14 135 50 3.21 0.59 −2.436 −4.86 −7.29 15.7 13 4.81 7.03 3070 2630
± 0.4 0.05 0.010 2 9 10 0.1 0.03 0.27 0.27 2.0 2 0.11 0.05 340 100 100
6 HD 152235 21.6 2.68 0.085 16 59 50 3.00 0.80 −2.006 −6.89 −8.89 24.5 38 5.45 6.87 1460 1620
± 0.3 0.05 0.008 2 4 5 0.1 0.03 0.24 0.25 1.3 4 0.10 0.04 140 130 90

Notes. Uncertainties are 1σ-values, except where noted otherwise. (a)Gaia Collaboration (2016, 2021) – distances and uncertainties correspond to ‘photogeometric distances’ and associated 14th and 86th confidence percentiles (Bailer-Jones et al. 2021).(b) Alternative solution, adopting the Gaia distance for the calculation of the fundamental stellar parameters instead of the spectroscopic distance, starting from MV. (c)HD 91316 is in fact a binary star with the V magnitude difference of the two components in the range ~1 to 1.5 mag at similar Teff as discussed in Sect. 5. As the Gaia parallax is likely affected by the binary orbital motion (indicated by a high Renormalised Unit Weight Error of 2.457) and in the absence of a second line system, a further determination of the parameters of the binary components is beyond the scope of the present paper.

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