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3 Reductions and measurements


  \begin{figure}
\par\includegraphics[width=8.3cm,clip]{H2231.1.ps}\end{figure} Figure 1: Comparison of measurements of $W_{\lambda }$ (Å) in this work and in Feltzing & Gustafsson (1998) for HD 32147 and HD 182572

The spectra were reduced with the standard software available within the CCDRED and ECHELLE packages of NOAO IRAF[*]. The steps included bias subtraction, flat fielding, extraction of one-dimensional spectra, wavelength calibration, and continuum normalization. Additional details concerning the quality of the data resulting from the Sandiford spectrograph can be found in Gonzalez & Lambert (1996) and Gonzalez (1998).

Equivalent widths ( $W_{\lambda }$) were measured using the SPLOT task in IRAF. The lines were measured both by simply integrating the line and also by fitting a Gaussian to the line profile. Most lines were measured twice and some up to four times due to overlap of the spectral orders. As the final adopted value of $W_{\lambda }$ we used the mean of the measurements. In these cases the measurement errors are typically no more than a few percent.

In Fig. 1 we compare the measured values of $W_{\lambda }$ for HD 32147 and HD 182572 with those measured by Feltzing & Gustafsson (1998). For HD 182572 the agreement is good, while for HD 32147, our coolest star, we measure significantly larger $W_{\lambda }$. This difference is most likely due to the lower resolution used in this work. See also the two examples of stellar spectra shown in Fig. 3 from which it is clear that HD 32147, but also to some extent HD 145675, shows a much richer spectrum than the other stars. Since these stars are cool, there will naturally be more molecular lines and low-excitation atomic lines that will cause blending problems.


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