Free Access
Issue
A&A
Volume 520, September-October 2010
Article Number A88
Number of page(s) 12
Section Stellar atmospheres
DOI https://doi.org/10.1051/0004-6361/200913750
Published online 08 October 2010

Online Material

\begin{figure}
\par\includegraphics[width=8.8cm,clip]{figures/13750f4.ps}
\end{figure} Figure 4:

Comparison between the observed and theoretical profiles for the Ba lines. Observations are shown with symbols, thick full line corresponds to the synthetic spectrum calculated with the best-fitting stratified abundance distribution and dashed line shows prediction of the spectrum synthesis with a homogeneous abundance.

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\begin{figure}
\par\includegraphics[width=8.8cm,clip]{figures/13750f5.ps}
\end{figure} Figure 5:

Same as in Fig. 4 but for Ca.

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\begin{figure}
\par\includegraphics[width=8.8cm,clip]{figures/13750f6.ps}
\end{figure} Figure 6:

Same as in Fig. 4 but for Si.

Open with DEXTER

\begin{figure}
\par\includegraphics[width=8.8cm,clip]{figures/13750f7.ps}
\end{figure} Figure 7:

Same as in Fig. 4 but for Fe.

Open with DEXTER

\begin{figure}
\par\includegraphics[angle=90,width=15.5cm,clip]{figures/13750f9.ps}
\end{figure} Figure 9:

Observed and theoretical energy distribution of HD 101065 calculated with scaled REE opacity from ISAN line list (see text). For comparison purpose the theoretical energy distribution of a normal F-type star HD 49933 is also shown. All theoretical calculations are smoothed with 20 Å Gaussian. Theoretical fluxes were scaled assuming radiuses: $R=1.98~R_\odot$ for HD 49933 and $T_{\rm eff}=6400$ K models; $R=1.90~R_{\odot}$ for $T_{\rm eff}=6500$ K; $R=1.82~R_{\odot}$for  $T_{\rm eff}=6600$ K.

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Table 3:   List of Si, Ca, Fe, and Ba spectral lines used for reconstruction of chemical stratification.

Table 4:   Abundances of individual elements.

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