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Table 6

Spectroscopic parameters adopted for each star.

Star Teff log g [FeI/H] [FeII/H] [Fe/H]model ξ #Fe i #Fe ii ΔII−I aEW bEW aexc bexc
(K) [cgs] (km s-1)

221 4620 2.0 0.88 ± 0.24 0.91 ± 0.17 0.90 1.0 31 2 0.035 +0.00 ± 0.12 +6.63 ± 0.55 +0.004 ± 0.045 +6.61 ± 0.15
224 5000 3.5 0.62 ± 0.36 0.60 ± 0.30 0.65 0.8 61 4 +0.015 +0.02 ± 0.10 +6.96 ± 0.48 +0.013 ± 0.044 +6.84 ± 0.15
230 4960 3.0 1.04 ± 0.40 1.03 ± 0.18 1.10 0.8 58 5 +0.0038 +0.02 ± 0.11 +6.57 ± 0.52 +0.087 ± 0.056 +6.17 ± 0.19
235 4680 2.2 0.94 ± 0.15 0.95 ± 0.09 0.95 1.1 45 7 0.012 +0.00 ± 0.03 +6.59 ± 0.17 0.002 ± 0.024 +6.57 ± 0.08
238 4720 2.9 0.43 ± 0.18 0.42 ± 0.07 0.50 1.0 33 5 0.0077 +0.00 ± 0.07 +7.07 ± 0.35 +0.027 ± 0.031 +6.98 ± 0.11

Notes. We also present the number of iron lines used for each star to derive the atmospheric parameters. The difference ΔII−I = [Fe ii/ H] − [Fe i/ H] shows the quality in the ionization equilibrium, and the parameters from the linear fitting [Fe i/ H] = aEW ∗ log (EW/λ) + bEW for microturbulence and [Fe i/ H] = aexcexc.pot + bexc for effective temperature.

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