\begin{table} %t1
\caption{\label{tab1}Summary
properties of the X-ray sources in the region of \object{KUG 0214-057}.}
%\centerline
{
\begin{tabular}{cccrrrrrrr} 
\hline\hline 
Source$^a$  & RA & Dec & \multicolumn{1}{c}{Count rate$^b$ } & \multicolumn{1}{c}{HR1$^c$ }
&\multicolumn{1}{c}{HR2} &\multicolumn{1}{c}{HR3} & $\log_{10}
f_{\rm X}$$^d$ &
\multicolumn{1}{c}{$z$$^e$}&$\log_{10}
L_X$$^f$\\
name       & \multicolumn{2}{c}{J2000.0}  &
       \multicolumn{1}{c}{[count
       s$^{-1}$]} &  &  &  & & &  \\
              \hline
A&02 17 20.60&$-$05 28 55.1&
0.00499\ $\pm$\ 0.00043&0.83\ $\pm$ 0.07&$-$0.59\ $\pm$\ 0.07&$-$0.59\
$\pm$\ 0.29&$-$13.87&0.018& 39.98\\
B&02 17 19.88&$-$05 28 39.8&
0.00377\ $\pm$\ 0.00039&0.81\ $\pm$\ 0.08&$-$0.59\ $\pm$\ 0.07&$-$0.41\
$\pm$\ 0.34&$-$13.99&0.018& 39.86\\
C&02 17 18.13&$-$05 28 30.5&0.00370\ $\pm$\ 0.00044&0.63\ $\pm$\ 0.09&$-$0.68\ $\pm$\ 0.08&$-$0.25\
$\pm$\ 0.38&$-$14.00&0.018& 39.85\\
D&02 17 16.77&$-$05 28 40.8&
0.00245\ $\pm$\ 0.00036&1.00\ $\pm$\ 0.04&$-$0.50\ $\pm$\ 0.12&$-$0.44\
$\pm$\ 0.37&$-$14.17&0.018&39.67\\
E&02 17 18.62&$-$05 29 21.3&
0.12428\ $\pm$\ 0.00131&0.57\ $\pm$\ 0.01&$-$0.73\ $\pm$\ 0.01&$-$0.42\
$\pm$\ 0.02&$-$12.47&0.634& 44.76\\
\hline
\end{tabular}}
\smallskip
$^a$  IAU designations of 
sources are as follows:
{\bf A}~XMMU J021729.6-052855;
{\bf B}~XMMU J021719.9-052840; {\bf C} XMMU J021718.1-052831;
{\bf D}~XMMU J021716.8-052841;
{\bf E}~XMMU J021718.6-052921.\\
$^b$ X-ray count rate in 0.3$-$10~keV
band expressed in EPIC~pn~count~s$^{-1}$.\\
 $^c$ Hardness ratios HR1,
HR2 and HR3 are defined in the caption to Fig.~\ref{fig3}.\\
$^d$ X-ray flux in 0.3$-$10~keV band [$\rm erg\ cm^{-2}\
s^{-1}$] assuming a nominal power-law spectrum with $\Gamma =1.7$ and
absorption column density $N_{\rm H}=2.5\times 10^{20}~\rm cm^{-2}$.\\
$^e$  Assumed redshift (see text).\\
$^f$  X-ray luminosity in 0.3$-$10 keV band [$\rm erg\
s^{-1}$].
\end{table}