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This article has an erratum: [https://doi.org/10.1051/0004-6361/200912982e]


 

 

Table 3:

Quantified abundance results for MACHO 79.5501.13, MACHO 81.9728.14 and MACHO 81.8520.15.
  MACHO 79.5501.13 MACHO 81.9728.14 MACHO 81.8520.15    
  $\begin{array}{r@{~=~}l} T_{\rm eff} & 5750~{\rm K} \\
\log g & 0.5\ {\rm (cgs)} \\
\xi_{\rm t} & 3.0\ {\rm km~s}^{-1} \\
\end{array}$ $
\begin{array}{r@{~=~}l}
T_{\rm eff} & 5500~{\rm K} \\
\log g & 1.0\ {\rm (cgs)} \\
\xi_{\rm t} & 3.0\ {\rm km~s}^{-1} \\
\end{array}$ $\begin{array}{r@{~=~}l}
T_{\rm eff} & 6250~{\rm K} \\
\log g & 1.0\ {\rm (cgs)} \\
\xi_{\rm t} & 3.0\ {\rm km~s}^{-1} \\
\end{array}$    
Ion N $\log\epsilon$ $\sigma_{\rm ltl}$ [el/H] N $\log\epsilon$ $\sigma_{\rm ltl}$ [el/H] N $\log\epsilon$ $\sigma_{\rm ltl}$ [el/H] Sun $T_{\rm cond}$
C   I 6 7.65 0.12 -0.92 2 7.52 0.04 -1.05 8 8.08 0.08 -0.49 8.57 40.
Na  I         2 5.07 0.21 -1.26         6.33 958.
Mg  I 2 6.09 0.33 -1.45 1 6.78   -0.76 2 6.34 0.05 -1.20 7.54 1336.
Si  I 2 6.48 0.20 -1.06 4 6.69 0.12 -0.85         7.54 1310.
Si  II                 2 6.18 0.06 -1.36 7.54 1310.
S   I 5 6.71 0.06 -0.62                 7.33 664.
Ca  I 2 4.67 0.13 -1.69 9 5.25 0.14 -1.11 12 4.86 0.19 -1.50 6.36 1517.
Sc  II 1 0.19   -2.98 2 1.15 0.17 -2.02 5 1.23 0.20 -1.94 3.17 1659.
Ti  I                 1 3.13   -1.89 5.02 1582.
Ti  II 6 2.20 0.25 -2.82 4 3.26 0.29 -1.76 16 3.03 0.18 -1.99 5.02 1582.
Cr  I 3 3.85 0.02 -1.82 3 4.39 0.30 -1.28 4 3.91 0.16 -1.76 5.67 1296.
Cr  II 10 3.76 0.16 -1.91 11 4.70 0.18 -0.97 12 4.05 0.19 -1.62 5.67 1296.
Mn  I 6 4.34 0.21 -1.05 2 4.32 0.31 -1.07 1 3.58   -1.81 5.39 1158.
Fe  I 41 5.85 0.15 -1.66 73 6.43 0.16 -1.08 122 5.92 0.17 -1.59 7.51 1334.
Fe  II 14 5.56 0.22 -1.95 14 6.47 0.15 -1.04 23 5.95 0.15 -1.56 7.51 1334.
Ni  I 2 4.27 0.22 -1.98 10 4.99 0.11 -1.26 6 4.47 0.12 -1.78 6.25 1353.
Zn  I 3 3.98 0.04 -0.62 1 3.38   -1.22 1 3.21   -1.39 4.60 726.
Y   II 1 -0.26   -2.50 1 0.49   -1.75 2 0.11 0.01 -2.13 2.24 1659.
Zr  II         1 0.74   -1.86         2.60 1741.
Ba  II                 4 0.23 0.06 -1.90 2.13 1455.
Ce  II 1 -0.28   -1.86                 1.58 1478.
Eu  II         2 0.12 0.08 -0.40         0.52 1356.

Note: The explanation of the columns is as follows: N gives the number of lines used; $\log\epsilon$ is the absolute abundance derived $\log\epsilon = \log$(N(X)/N(H))+12; $\sigma_{\rm ltl}$ is the line-to-line scatter; and [el/H] is the abundance relative to the Sun. For the references of the solar abundances needed to calculate the [el/H] values: see Reyniers & Van Winckel (2007). The dust condensation temperatures are taken from Lodders (2003), and references therein. They are computed using a solar abundance mix at a pressure of 10-4 atm. The abundance table of MACHO 82.8405.15 can be found in Reyniers et al. (2007).


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