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Table 2

Spectroscopic stellar parameters and iron abundance derived with MOOG for low-rotating stars observed at high resolution.

Star Teff log g ξ [Fe i/H]* # Lines [Fe ii/H]** # Lines
(K) (dex) (km s-1) (dex) (dex)

X-Clump 0534+22
2MASS J05263833+2231546 4750 4.4 2.0  −0.08 ± 0.15 43  −0.08 ± 0.15 3
2MASS J05263826+2231434 4750 4.0 1.9  −0.07 ± 0.12 42  −0.06 ± 0.11 5
2MASS J05214684+2400444 5000 4.3 2.2  −0.04 ± 0.11 44  −0.02 ± 0.06 4

X-Clump 0430−08
2MASS J04431640−0937052 6000 4.6 1.4  + 0.22 ± 0.08 66  + 0.22 ± 0.10 9
" 6050 4.6 1.4 +0.26  ±  0.08 78 +0.22  ±  0.10 9
2MASS J04443859−0724378 5900 4.4 1.5  + 0.03 ± 0.09 64  + 0.03 ± 0.08 11

Strip
2MASS J03494386 − 1353108 5400 4.5 1.4  + 0.00 ± 0.09 64  −0.01 ± 0.12 9
" 5500 4.6 1.6 +0.05  ±  0.09 70  + 0.03 ± 0.13 10
2MASS J05274490+0313161 5000 4.3 1.7  −0.02 ± 0.17 51  −0.01 ± 0.23 3
2MASS J06134773+0846022 5050 3.6 1.6  −0.25 ± 0.13 59  −0.24 ± 0.13 9
2MASS J06203205+1331125 5350 4.4 0.3  −0.23 ± 0.17 44  −0.24 ± 0.25 4
2MASS J06350191+1211359 6100 4.3 1.5  + 0.01 ± 0.13 45  + 0.00 ± 0.19 9
2MASS J06513955+1828080 5100 4.7 1.5  −0.07 ± 0.09 60  −0.07 ± 0.13 5

Alcalá et al. (2000) Sample
RX J0515.6 − 0930 5650 4.5 2.3  −0.04 ± 0.12 41  −0.06 ± 0.23 4
RX J0517.9 − 0708 5100 4.2 1.8  + 0.06 ± 0.13 47  + 0.05 ± 0.14 4
RX J0531.6 − 0326 5250 4.3 1.7  −0.02 ± 0.09 53  −0.03 ± 0.08 5
RX J0538.9 − 0624 5550 4.4 1.3  + 0.01 ± 0.11 58  + 0.02 ± 0.20 10
RX J0518.3+0829 5300 4.2 2.0  −0.04 ± 0.11 21  −0.02 ± 0.15 3
RX J0510.1 − 0427 4950 4.6 1.9  −0.10 ± 0.12 34  −0.00 ± 0.24 2
RX J0520.0+0612 4750 4.1 2.2  −0.17 ± 0.12 45  −0.17 ± 0.30 5
RX J0520.5+0616 4900 4.1 2.4  −0.08 ± 0.17 29  −0.07 ± 0.04 3

Notes. The two stars observed with FEROS are indicated in italics.

(*)

The iron abundances are relative to the Sun. Adopting  K, log g ⊙  = 4.44, and ξ ⊙  = 1.1 km s-1, we obtain log n ⊙ (Fe   i) = 7.53 ± 0.04 and log n ⊙ (Fe   ii) = 7.53 ± 0.06 from a FOCES spectrum, and log n ⊙ (Fe   i) = 7.50 ± 0.05 and log n ⊙ (Fe   ii) = 7.50 ± 0.06 from a FEROS spectrum.

(**)

The listed errors are the internal ones in EW, represented by the standard deviation on the mean abundance determined from all lines. The other source of internal error includes uncertainties in stellar parameters (Biazzo et al. 2011a). Taking into account typical errors in Teff (~70 K), log g (~0.2 dex), and ξ (~0.2 dex), we derive an error of  ~0.05 dex in [Fe/H] due to uncertainties on stellar parameters.

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