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Table 16:

Results from the abundance analysis of HD 36629 (B2 V).

HD 36629 		$T_{\rm eff}$ = 20 000 K, log g = 4.1 dex $\xi_{\rm t}$(Si)=1.0

Line 		EW $\Delta$EW $\epsilon_{\rm Si}$ $\Delta\epsilon_{\rm Si}$
  (mÅ) (mÅ) (dex) (dex)

SiII3856 		52 2 7.58 0.07
SiII3862 42 2 7.55 0.08
SiII6347 65 3 7.62 0.07
SiII6371 48 2 7.53 0.06
SiIII4552 90 1 7.52 0.02
SiIII4567 73 1 7.49 0.02
SiIII4574 46 1 7.51 0.03
SiIII5739 42 2 7.53 0.06
  $\epsilon_{\rm Si}$ =  7.54 $\Delta\epsilon_{\rm Si}$($\sigma $) = 0.04
  $\Delta$ $\xi_{\rm t}$(Si) = 0.5 $\Rightarrow$ $\Delta\epsilon_{\rm Si}$( $\xi_{\rm t}$) = 0.05

HD 36629 		$T_{\rm eff}$ = 20 000 K, log g = 4.1 dex $\xi_{\rm t}$(O)=6.0
OII3945 24 2 8.91 0.09
OII3954 28 2 8.68 0.07
OII4317 37 3 8.77 0.09
OII4319 30 2 8.63 0.07
OII4366 30 2 8.59 0.07
OII4414 50 2 8.69 0.05
OII4416 40 2 8.75 0.06
OII4452 16 1 8.74 0.06
OII4638 36 1 8.95 0.03
OII4641 41 1 8.63 0.03
OII4650 59 3 8.65 0.07
OII4661 32 2 8.72 0.07
OII4673 11 3 8.82 0.23
OII4676 27 2 8.65 0.07
OII4069 64 3 8.88 0.06
OII4072 45 2 8.83 0.06
OII4076 55 3 8.85 0.08
OII4078 15 2 8.79 0.13
OII4943 16 3 8.83 0.17
  $\epsilon_{\rm O}$ =  8.76 $\Delta\epsilon_{\rm O}$($\sigma $) = 0.10
  $\Delta$ $\xi_{\rm t}$(O) = 1.7 $\Rightarrow$ $\Delta\epsilon_{\rm O}$( $\xi_{\rm t}$) = 0.06


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