All Figures

$\begin{figure} \par\includegraphics[width=8.8cm,clip]{He061_f1.eps} \end{figure}$ Figure 1: Radial velocity smoothed using splines. A. Radial velocity data points, as a function of pulsation phase (0-phase defined as the maximum of light). This set was extracted using a cross-correlation technique (Bersier et al. 1994). The solid line is a 4-knot periodic cubic spline fit. B. Residuals of the fit.
Open with DEXTER

In the text

$\begin{figure} \par\includegraphics[width=8.8cm,clip]{He061_f2.eps}\end{figure}$ Figure 2: p-factor determination. A. Our angular diameter measurements (points). Crosses correspond to the medium baseline (E2-W1), while circles correspond to the largest baseline (E1-W1). The continuous line is the integration of the 4-knots periodic cubic spline fitted to the radial velocities (Fig. 1). Integration parameters: $\overline{\theta}=1.475~{\rm mas}$ , p=1.269 and $d=274~{\rm pc}$ . B. Residuals of the fit.
Open with DEXTER

In the text

$\begin{figure} \par\includegraphics[width=8.8cm,clip]{He061_f1.eps} \end{figure}$	Figure 1: Radial velocity smoothed using splines. A. Radial velocity data points, as a function of pulsation phase (0-phase defined as the maximum of light). This set was extracted using a cross-correlation technique (Bersier et al. 1994). The solid line is a 4-knot periodic cubic spline fit. B. Residuals of the fit.
Open with DEXTER