Table D.1.
Individual abundances of the giant component in 56 UMa
| Z |  |
log ϵ | σs (N) | [X/Fe] ± σ[X/Fe] | |
|---|---|---|---|---|---|
| Cb | 6 | 8.43 | 8.20 | 0.06(4) | −0.18±0.15 |
| 12C/13C | 19 | ||||
| Nc | 7 | 7.83 | 8.40 | 0.09(30) | 0.62±0.21 |
| Od | 8 | 8.69 | 8.70 | 0.00(2) | 0.06±0.22 |
| Na I | 11 | 6.24 | 6.40 | 0.10(4) | 0.21±0.40 |
| Mg I | 12 | 7.60 | 7.50: | 0.10(2) | −0.05±0.16 |
| Fe I | 26 | 7.50 | 7.45 | 0.10(65) | – |
| Rb I | 37 | 2.52 | 2.50: | 0.00(2) | 0.03±0.10 |
| Sr I | 38 | 2.87 | 3.30: | 0.10(1) | 0.48±0.35 |
| Sr INLTE | 38 | 2.87 | 3.49: | 0.10(1) | 0.67±0.35 |
| Y II | 39 | 2.21 | 2.40 | 0.05(7) | 0.24±0.17 |
| Zr I | 40 | 2.58 | 2.43 | 0.13(3) | −0.10±0.30 |
| Zr II | 40 | 2.58 | 2.65 | 0.06(2) | 0.12±0.30 |
| Ba II | 56 | 2.18 | 2.72: | 0.09(2) | 0.59±0.11 |
| La II | 57 | 1.10 | 1.40 | 0.12(8) | 0.35±0.22 |
| Ce II | 58 | 1.58 | 1.70 | 0.13(8) | 0.17±0.24 |
| Pr II | 59 | 0.72 | 0.75 | 0.05(3) | 0.08±0.25 |
| Nd II | 60 | 1.42 | 1.72 | 0.13(13) | 0.35±0.22 |
| Sm II | 62 | 0.96 | 1.08 | 0.13(4) | 0.17±0.32 |
| Eu II | 63 | 0.52 | 0.70 | 0.00(2) | 0.23±0.32 |
| Gd II | 64 | 1.10 | 1.40 | 0.10 (1) | 0.35±0.21 |
| Dy II | 66 | 1.10 | 1.30 | 0.10 (1) | 0.25±0.18 |
| Hf II | 72 | 0.85 | 1.10: | 0.00(2) | 0.30±0.32 |
| Os II | 76 | 1.40 | 1.60: | 0.10 (1) | 0.25±0.20 |
aAsplund et al. (2009). bThe carbon abundance was derived from the CH molecular bands at 4300 Å and from the weak C2 molecular lines at 5165 Å and 5635 Å. cThe multiple CN bands longwards of 7000 Å were used to derive the nitrogen abundance and the 12C/13C ratio. dThe oxygen abundance was derived from the [O I] line at 6300 Åand from the O I resonance triplet at 7770 Å. Due to non-LTE effects, the second abundance is higher by 0.3 dex. We took the average of these values after applying non-LTE corrections.
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