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Table 2

Atmospheric parameters and small-scale magnetic field.

Target Teff (K) log g (dex) [M/H] (dex) v sin i (km s−1) i (°)a ζRT(km s−1)b B〉 (kG)
DS Leo 3797 ± 30 4.67 ± 0.05 −0.02 ± 0.10 1.5 51 ± 48 3.01 ± 0.07 0.79 ± 0.02
AD Leo 3475 ± 30 4.81 ± 0.05 0.23 ± 0.10 3.0 20 ± 11 2.19 ± 0.15 3.13 ± 0.05
EV Lac 3342 ± 30 4.75 ± 0.05 0.02 ± 0.10 3.0 57 ± 57 4.22 ± 0.14 4.54 ± 0.09
Barnard’s star 3300 ± 31 4.71 ± 0.06 −0.54 ± 0.10c <0.1d ... 3.79 ± 0.17 0.51 ± 0.08
PM J18482+0741 3102 ± 32 4.97 ± 0.06 0.01 ± 0.10 2.4 40 ± 27 5.51 ± 0.18 1.27 ± 0.14
CN Leo 2912 ± 31 5.00 ± 0.07 0.22 ± 0.11 2.0 55 ± 45 4.94 ± 0.29 3.08 ± 0.26

Notes. Projected rotational velocities (υ sin i) for our analyses were taken from Morin et al. (2008) for AD Leo and Reiners et al. (2018) for PM J18482+0741. For CN Leo, EV Lac, and DS Leo, v sin i estimates were taken from Cristofari et al. (2023a), who revised some values based on rotation periods and radii. Inclinations were derived from υ sin i, Prot and radii. a Inclinations computed assuming a 1.0 km s−1 uncertainty on υ sin i. b In the present analysis, we fixed υ sin i and fit ζRT. Consequently, broadening arising from non-physical or unidentified sources may lead to larger ζRT estimates. c For Barnard’s star, we additionally fit for the [α/Fe] parameter (see Cristofari et al. 2022a), yielding [α/Fe] = 0.09 ± 0.10 dex. d Maximum υ sin i assuming an inclination of 90°.

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