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Table 5:

Derived uniform disk and limb-darkened diameters, and stellar radii.
Target Instrument parallax mK Limb darkening coeff. $\theta_{\rm UD}$ $\theta_{\rm LD}$
    [mas]   K band [mas] [mas]

GJ 663 A
VINCI 168.54 $\pm$ 0.54 - [0.79, -0.56, 0.43, -0.15] 1.253 $\pm$ 0.025 1.282 $\pm$ 0.026
GJ 166 A AMBER 200.62 $\pm$ 0.23 2.39 $\pm$ 0.02 (a) [0.81, -0.53, 0.39, -0.13] 1.405 $\pm$ 0.038 1.437 $\pm$ 0.039
GJ 570 A VINCI 171.22 $\pm$ 0.94 3.15 $\pm$ 0.02 (a) [0.86, -0.52, 0.37, -0.12] 1.147 $\pm$ 0.029 1.177 $\pm$ 0.030
GJ 845 VINCI 276.06 $\pm$ 0.28 2.18 $\pm$ 0.02 (b) [0.86, -0.53, 0.38, -0.13] 1.834 $\pm$ 0.016 1.881 $\pm$ 0.017
GJ 879 AMBER 131.42 $\pm$ 0.62 3.95 $\pm$ 0.08 (a) [0.86, -0.53, 0.38, -0.13] 0.750 $\pm$ 0.066 0.769 $\pm$ 0.067
GJ 887 AMBER 305.26 $\pm$ 0.70 3.36 $\pm$ 0.02 (a) [1.61, -2.35, 2.00, -0.68] 1.284 $\pm$ 0.031 1.304 $\pm$ 0.032
GJ 551 AMBER 771.64 $\pm$ 2.60 4.38 $\pm$ 0.03 (c) [1.94, -2.80, 2.39, -0.81] 0.990 $\pm$ 0.050 1.011 $\pm$ 0.052
References: (a) Morel & Magnenat (1978); (b) Mould & Hyland (1976); (c) 2MASS (Cutri et al. 2003)
and (d) Ségransan et al. (2003). Parallaxes are from Hipparcos.

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