Table A.1
Mean difference of derived effective temperature, ΔTeff = Teff(ref i) − Teff(this work) and derived optical depth invariant, Δlog Q, for N objects from reference i,i = 1,8 in common with our sample (cf. Table A.2).
| ref# | N | ⟨ ΔTeff ⟩ | σ(ΔTeff) | ⟨ Δlog Q ⟩ | σ(Δlog Q) |
|
|
|||||
| 1 | 4 | –1.38 | 0.76 | ||
| 3 | 3 | 1.63 | 1.72 | –0.21 | 0.31 |
| 4 | 3 | 0.13 | 1.70 | 0.05 | 0.28 |
| 5 | 3 | –0.57 | 0.59 | 0.11 | 0.28 |
| 6 | 4 | 1.75 | 1.79 | –0.02 | 0.38 |
| 7 | 8 | –0.21 | 1.67 | –0.06∗ | 0.31∗ |
| 8 | 6 | –0.08 | 0.23 | ||
Notes. ΔTeff in kK, Δlog Q in dex. For ref# 1, we compare the Qres-values, whereas for the rest we compare the Q-values normalized by fv (see Eq. (A.1)). Positive values indicate that the results from the specific work are on average larger than the results derived here. σ is the dispersion of these differences. No values are given for ref# 2 (Kudritzki et al. 1999), since there is only one object in common. ∗ Mean difference and dispersion only for 7 objects, excluding the weak-winded object HD 37468.
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