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Table A.1

Program star coordinates, photometry (from K98), adopted atmospheric parameters, and iron and lithium abundances.

ID α(J2000) δ(J2000) V B − V Teff log g ξ [Fe/H] A(Li) S/N v helio
K km s-1 at 607 nm km s-1

1318 06:36:53.5 09:25:34.6 15.01 1.55 4730 2.20 1.20 −0.49 1.23a 33 48.1 ± 0.3e
3416c 06:36:40.2 09:29:47.8 15.04 1.52 4850 2.20 1.28 −0.51 (3.75/3.75)b 36 49.8 ± 0.1e
(3.60/3.66)a
3416d 06:36:40.2 09:29:47.8 15.04 1.52 4870 2.05 1.33 −0.53 103 50.5 ± 0.2f
4649 06:36:48.0 09:32:33.5 15.00 1.55 4750 2.25 1.02 −0.27 14 47.3 ± 0.1e
4791 06:36:33.1 09:33:03.7 15.00 1.53 4800 1.90 1.30 −0.48 <1.30a 11 50.0 ± 0.1e
6223 06:36:38.6 09:38:52.6 15.08 1.49 4830 2.40 1.21 −0.42 <1.18a 30 50.8 ± 0.4e

Notes. The spectra signal-to-noise ratios are also indicated, as well as the measured radial velocities. Lithium abundances are derived from the 670.78 nm line for all stars but for #3416, for which the values from both the 670.78 nm and the 610.36 nm lines are reported as (A(Li)670.78 nm/A(Li)610.36 nm).

(a)

Abundance derived with 1D-LTE analysis plus NLTE corrections calculated according to Lind et al. (2009). Owing to the grid boundaries, NLTE corrections were adopted assuming ξ = 2.0km s-1.

(b)

Value measured from 3D-NLTE analysis.

(c)

Analysis based on UVES spectrum.

(d)

Analysis based on MIKE spectrum.

(e)

Radial velocity uncertainty calculated as the difference between the two epochs vhelio multiplied by 0.63 (small sample statistics, see Keeping 1962).

(f)

Formal error on radial velocity determination from cross-correlation analysis.

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