Table 4: Abundances for HD 139409, in the scale where $\log \epsilon$(H) = 12, and normalized with respect to the solar abundances (Grevesse & Sauval 1998). The standard deviations $\sigma $ and the number N of lines used in the analysis are also given.
Element(X) Z $\log \epsilon$(X) $\sigma $ N [X/Fe]
I 6 8.46 0.10 4 +0.36
Na  I 11 6.02 0.05 5 +0.11
Mg  I 12 7.31 0.12 6 +0.15
Si  I 14 7.33 0.06 20 +0.20
Ca  I 20 6.20 0.07 6 +0.26
Sc  II 21 2.79 0.06 10 +0.04
Ti  I 22 4.77 0.09 51 +0.17
Ti  II 22 4.72 0.11 4 +0.12
I 23 3.76 0.11 23 +0.18
Cr  I 24 5.21 0.11 11 -0.04
Cr  II 24 5.36 0.09 3 +0.11
Mn  I 25 5.13 0.11 9 +0.16
Fe  I 26 7.08 0.08 136 -
Fe  II 26 7.08 0.12 14 -
Ni  I 28 5.86 0.07 44 +0.03
I 39 2.22 0.10 2 +0.40
II 39 2.41 0.07 6 +0.59
Zr  I 40 2.58 0.09 3 +0.40
Zr  II 40 2.78 0.12 3 +0.60
Ba  II 56 1.89 0.12 3 +0.18
La  II 57 1.05 0.12 3 +0.30
Ce  II 58 1.46 0.14 5 +0.30
Nd  II 60 1.38 0.09 6 +0.30


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