\begin{table}%T2
\par
\caption{The parameters resulting from the fits to the spectra
of XMMU J004215.8+411924 and SWIFT J004217.4+411532. }
\label{tab:TR1}
\small%\centering
\par
\begin{tabular}{cccccccccccccc}
\hline
\hline
& \multicolumn{4}{c}{Power-law}& \multicolumn{4}{c}{Disc black-body} &\multicolumn{4}{c}{Bremsstrahlung} \\
%\hline
Obs & $L_{36}$ & $\Gamma$ & $N_{\rm H,21}$ & $\chi^2_\nu$ & $L_{36}$ & $T_{\rm in}$ & $N_{\rm H,21}$ & $\chi^2_\nu$
& $L_{36}$ & $T_{\rm b}$ & $N_{\rm H,21}$ & $\chi^2_\nu$\\
\noalign{\smallskip}\hline
\multicolumn{14}{c}{XMMU J004215.8+411924}\\
%\hline
2 & $<$$0.4$ & (1.57) & (4.2) & --& $<$$3.5$& (1.92) & (2.2) & --& $<$$3.8$& (12.2) & (3.6)& --\\
3 & $110\pm30$ & $1.77\pm0.33$ & 6.2 $\pm$ 3.7 & 0.98 &
$86\pm44$ & 1.55 $\pm$ 0.35 & 2.5 $\pm$ 2.3 & 1.05&
$100\pm50$ & 6.5 $\pm$ 4.0 & 5.2 $\pm$ 2.7 & 0.98&
\\
4 & $76\pm12$ & $1.57\pm0.08$ & 4.2 $\pm$ 0.5 & 0.84 &
$67\pm11$ & 1.92 $\pm$ 0.14 & 2.2 $\pm$ 0.3 & 0.87&
$73\pm12$ & 12.2 $\pm$ 4.0 & 3.6 $\pm$ 0.4 & 0.80&\\
5 & 21 $\pm$ 1 & (1.57) & (4.2) & --& $19\pm1$& (1.92) & (2.2) & --&  20 $\pm$ 1& (12.2)& (3.6)&--\\
6 & $<$$5.8$ & (1.57) & (4.2) & --& $<$$5.1$& (1.92) & (2.2) & --&  $<$$5.6$&(12.2) & (3.6) & --\\
7 & $<$$0.8$ & (1.57) & (4.2) & -- & $<$$0.7$ & (1.92) & (2.2) & -- & $<$$0.6$ & (12.2) & (3.6) & --\\
%\hline
\multicolumn{14}{c}{SWIFT J004217.4+411532}\\
%\hline
4 & $<$$2.1$ & (3.5) & (4.0) & -- & 
$<$$0.9$ & (0.50) & (0.67) & -- & $<$$0.9$ & (1.0) & (1.5) & --\\
5 & $580\pm70$ & $3.12\pm0.35$ & $4.4\pm1.3$ & 1.35 & 
$270\pm30$ & $0.61\pm0.05$ & (0.67) & 1.26 & $350\pm70$ & $1.26\pm0.26$ & $2.18\pm0.91$ & 1.28\\
6 & $450\pm70$ & $3.55\pm0.49$ & $4.0\pm1.7$ & 0.99
& $180\pm30$ & $0.50\pm0.06$ & (0.67) & 0.96 &$230\pm70$& $1.07\pm0.27$& $1.13\pm1.13$ & 0.86 \\
7  & $260\pm60$ & $3.47\pm0.31$ & $5.1\pm1.3$ & 0.87 &  $ 97\pm7$ & $0.57\pm0.04$ & (0.67) & 0.97&  $130\pm20$ &$1.15\pm0.11$  & $2.0\pm0.9$ & 0.88\\
8 & $290\pm10$ & (3.5) & (4.0) & -- & $ 140\pm10$ & (0.50) & (0.67) & -- &$ 122\pm4$ & (1.0) & (1.5) & --\\
9 & $163\pm7$ & (3.5) & (4.0) & -- & $ 80\pm4$ & (0.50) & (0.67) & -- & $69\pm3$ & (1.0) & (1.5) & --\\
10& $81\pm29$ & $4.50\pm0.65$ & $5.1\pm2.2$ & 1.26 &  $20\pm2$ & $0.35\pm0.03$ & (0.67) & 1.01& $28\pm15$ & 0.58$\pm0.12$ & 1.91$\pm1.33$ & 1.10\\
11 & $36\pm4$ & $4.34\pm0.33$ & $3.3\pm0.5$ & 1.56 &
$15\pm3$ & $0.27\pm0.02$ & (0.67) & 1.67 & $18\pm4$ & 0.49 $\pm$ 0.06 & $1.49\pm0.27$ & 1.52\\
12 & $20\pm3$ & $4.51\pm0.57$ & $3.2\pm0.8$ & 1.10&
$8.2\pm2.2$ & $0.25\pm0.03$ & (0.67) & 1.44 & 10 $\pm$ 4 & 0.42 $\pm$ 0.08 & $1.50\pm0.43$ & 1.29\\
13 & $<$$0.9$ & (3.5) & (4.0) & -- &
$<$$0.5$ & (0.50) & (0.67) & -- & $<$$0.4$ & (1.0) & (1.5) & --\\
\hline
\end{tabular} 
\end{table}