\begin{table}%t1
  \caption{\label{slewtable}Details of the four XMM-Newton slew observations and the single (Rev.~1378) 
    dedicated XMM-Newton pointed observation.}
  %\centerline
{
\begin{tabular}{lccccrrrr}
\hline\hline
Rev  & Date & Obs.~ID & RA(J2000)   & Dec(J2000) & Counts    & Exposure & Count rate  & Lik. \\ 
     & (UT) &        &     &            &                & (s) & (s$^{-1}$)  &      \\ 
\hline 
 351 (slew) & 07/11/01 &  9035100003  &        &               & $<$3.6     & 8.8 & $<$0.41 & $<$$\sim$8      \\
 750 (slew) & 12/01/04 &  9075000003  &        &               & $<$3.2     & 17.3 & $<$0.18 & $<$$\sim$8      \\  
1210 (slew )& 18/07/06 &  9121000003  & 06:06:36.2 & --69:49:33 & 228.8 $\pm$ 14.1 & 9.8 & 23.4$\pm$1.4 & 1777.1   \\ 
1246 (slew) & 28/09/06 &  9121460003  & 06:06:36.5 & --69:49:38 &  12.9 $\pm$ 2.4  & 3.4 &  3.8$\pm$0.7 &   54.7   \\
\hline 
1378 (pointed) & 19/06/07 &  0510010501  & 06:06:36.5 & --69:49:37 & 1511.0 $\pm$ 44.8 & 8940.0 &  0.20 $\pm$ 0.01 & 4630.4          \\
\hline
\end{tabular}}
\smallskip
\par
 XMM-Newton revolution, date and observation ID 
    are tabulated, together with the 0.2$-$2.0~keV X-ray properties of XMMSL1~J060636.2-694933;  
    position, background-subtracted counts, exposure, count-rate, and detection likelihood. For the 
    Rev.~1378 dedicated observation, these properties are given for all the EPIC cameras combined. 
    For the slew observations, only the EPIC-pn values are given. In the first two slews the source 
    was not detected, and upper limits are shown in the table.
\end{table}