![\begin{figure}
\par\includegraphics[width=7.75cm,clip]{8093fig3a.eps}\hspace*{1....
...}\hspace*{1.1cm}
\includegraphics[width=7.7cm,clip]{8093fig3d.eps} \end{figure}](/articles/aa/full/2007/33/aa8093-07/Timg33.gif) |
Figure 3:
Top: luminosity to bolometric luminosity ratio in the radio ( left panel) and in the X-rays ( right panel). The ratio for H
is shown in both panels with its scale on the right y-axis and as small symbols in red. Bottom: similar as above, for surface fluxes. Ultracool dwarfs are shown in black (filled circles in the radio and diamonds in X-rays for detections, empty downward-pointing triangles for radio upper limits and downward-pointing arrows for X-ray upper limits), while M dwarfs are shown in blue (filled upward-pointing triangles for detections, empty downward-pointing triangles for upper limits).
The Kelu-1AB points (we assumed that the X-ray flux and radio upper limit were either due to Kelu-1A or to Kelu-1B) are shown as larger symbols. Note that flaring levels (if known) were purposely discarded. The dotted lines show the variations of
ratios or the surface fluxes vs.
for an arbitrary constant luminosity (in radio, X-rays, or H ). |