Table 1.
Atmospheric parameters and abundances of the two program stars.
Object | Teff | log(g) | vrad | v sin (i) | ζ | ξ | log(n(x)) | |||||||||||
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(K) | (cgs) | (km s−1) | He | C | N | O | Ne | Mg | Al | Si | S | Ar | Fe | |||||
PG 1610+062 | 14 800 | 4.054 | 157.4 (a) | 15.5 | 0.0 | 2.40 | −0.92 | −3.34 | −3.86 | −3.09 | −3.87 | −4.51 | −5.67 | −4.24 | −4.66 | −5.32 | −4.36 | |
Stat. |
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7.7 (a) |
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Sys. |
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...(a) |
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HD 137366 | 14 930 | 3.803 | −15.5 | 11.3 | 2.5 | 1.91 | −0.97 | −3.52 | −4.15 | −3.16 | −3.99 | −4.66 | −5.83 | −4.35 | −4.87 | −5.55 | −4.51 | |
Stat. |
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Sys. |
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Notes. The abundance n(x) is given as fractional particle number of species x with respect to all elements. Statistical uncertainties (“Stat.”) correspond to Δχ2 = 6.63 and are 99% confidence limits. Systematic uncertainties (“Sys.”) cover only the effects induced by additional variations of 2% in Teff and 0.1 in log(g) and are formally taken to be 99% confidence limits (see Irrgang et al. 2014 for details).
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