Table 4:

Mean NLTE abundances (on the scale in which $\log \epsilon$[H] = 12) and total 1-$\sigma $ uncertainties (in brackets), in units of the last digits.
  HD 180 642 B stars Sun 1-D Sun 3-D
He/H(4) 0.088(18) $\sim$0.089 0.085(1) 0.085(2)
$\log \epsilon$(C) (9) 8.21(10) $\sim$8.20 8.52(6) 8.39(5)
$\log \epsilon$(N) (21) 8.00(19) $\sim$7.79 7.92(6) 7.78(6)
$\log \epsilon$(O) (25) 8.53(14) $\sim$8.58 8.83(6) 8.66(5)
$\log \epsilon$(Ne) (6) 7.86(16)a $\sim$8.07 8.08(6) 7.84(6)
$\log \epsilon$(Mg) (1) 7.34(20) $\sim$7.48 7.58(5) 7.53(9)
$\log \epsilon$(Al) (3) 6.22(15) $\sim$6.08 6.47(7) 6.37(6)
$\log \epsilon$(Si) (7) 7.19(19) $\sim$7.20 7.55(5) 7.51(4)
$\log \epsilon$(S) (4) 7.10(34) $\sim$7.19 7.33(11) 7.14(5)
$\log \epsilon$(Fe) (21) 7.34(21) $\sim$7.36 7.50(5) 7.45(5)
${\rm [N/C]}$ -0.21(22) $\sim$-0.41 -0.60(9) -0.61(8)
${\rm [N/O]}$ -0.53(24) $\sim$-0.79 -0.91(9) -0.88(8)
Z 0.0099(16) $\sim$0.0108 0.0172(12) 0.0124(7)
The number of spectral lines used is given in brackets in the first column. For comparison purposes, we provide typical values found for early B dwarfs in the solar neighbourhood (Morel 2009, and references therein; B stars), the standard solar composition of Grevesse & Sauval (1998, Sun 1-D), and updated values derived from three-dimensional hydrodynamical models (Asplund et al. 2005, Sun 3-D). We define [N/C] and [N/O] as $\log$[$\epsilon$(N)/$\epsilon$(C)] and $\log$[$\epsilon$(N)/$\epsilon$(O)], respectively. The metallicity, Z, is given in the last row. To compute this quantity, we assumed the abundances of Grevesse & Sauval (1998) for the trace elements not under study.
a A negligible difference amounting to 0.01 dex is obtained when using the $T_{\rm eff}$ derived from the Ne ionisation balance (Morel & Butler 2008).

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