\begin{table}%t3
\caption{\label{tab:pl_212}Spectral fitting results. I: power law model applied to the
  hard band (2--12~keV). 1001$+$054 is excluded due to the very poor
  statistics in this energy range.}
%\centering
\par
\begin{tabular}{c c c l |c c c l}
\hline \hline 
PG name   &   $\Gamma_{\rm 2-12}$   &  $\chi^2$   &  
d.o.f.   &   PG name   &   $\Gamma_{\rm 2-12}$   &  $\chi^2$   &     d.o.f. \\
\hline
0007$+$106  &  $\rm 1.61^{+0.05}_{-0.04}$  &  135    &   179  &  1307$+$085   &  
$\rm 1.46^{+0.07}_{-0.08}$	  &  117   &   92 \\ 0050$+$124  &   $\rm 2.28^{+0.03}_{-0.03}$
  &   276   &   266  &  1309$+$355  &  $\rm 1.72^{+0.07}_{-0.06}$  &  95  &   87   \\ 0157$+$001  &  
$\rm 2.1^{+0.2}_{-0.2}$   &   31   &  
48  &  1322$+$659  &  $\rm 2.2^{+0.2}_{-0.2}$  &  91  &  88\\
0804$+$761  &  $\rm 2.05^{+0.07}_{-0.07}$  &     148            &    135  &  1352$+$183    &  
$\rm 1.91^{+0.09}_{-0.09}$  &  	126   &   97 \\ 0844$+$349   &  
$\rm 2.11^{+0.05}_{-0.05}$   &   106   &   109  &  1402$+$261  &   $\rm 2.06^{+0.09}_{-0.08}$
  &   77   &   92\\ 0947$+$396  &   $\rm 1.81^{+0.06}_{-0.06}$   &   121   &  
137  &  1404$+$226  &  $\rm 2.3^{+0.8}_{-0.8}$  &    5             &  9       \\
0953$+$414  &  $\rm 2.01^{+0.07}_{-0.06}$  &  64  &  69  &  1407$+$265  &  $\rm 2.19^{+0.07}_{-0.07}$  &  83
  &   118      \\
1001$+$054  &  $-$  &  $-$  &  $-$  &  1411$+$442  &  $\rm 0.38^{+0.11}_{-0.13}$  &  111  &   67    \\
1048$+$342  &  $\rm 1.77^{+0.05}_{-0.05}$  &  113  &  149  &   1415$+$451   &  
$\rm 2.03^{+0.08}_{-0.08}$   &   65   &   105\\ 1100$+$772  &  
$\rm 1.65^{+0.05}_{-0.05}$  &  180    &   220  &  1427$+$480  &   $\rm 1.90^{+0.07}_{-0.05}$
  &   115   &   155\\ 1114$+$445  &  $\rm 1.48^{+0.04}_{-0.03}$  &    255  &  241  &  1440+356   &  
$\rm 2.03^{+0.06}_{-0.07}$    &   173   &   104\\ 1115$+$080   &  
$\rm 2.00^{+0.11}_{-0.11}$	  &  87   &   87  &   1444$+$407   &   $\rm 2.12^{+0.12}_{-0.12}$    &  
30   &   48\\ 1115$+$407  &  $\rm 2.16^{+0.07}_{-0.07}$  &  94   &  100  &  1501$+$106   &  
$\rm 1.88^{+0.03}_{-0.03}$    &   164   &   154\\ 1116$+$215  &   $\rm 2.14^{+0.08}_{-0.08}$
  &   105   &   106  &  1512$+$370  &  $\rm 1.82^{+0.06}_{-0.07}$  &  97  &  130       \\
1202$+$281   &    $\rm 1.69^{+0.05}_{-0.05}$   &   189   &   195  &  
1613$+$658  &  $\rm 1.70^{+0.10}_{-0.10}$  &       48   &  66 \\
1206$+$459  &  $\rm 2.0^{+0.4}_{-0.5}$  &  15  &  12  &  1626$+$554  &  $\rm 1.95^{+0.10}_{-0.10}$  &  130
  &   137      \\ 1211$+$143 &  $\rm 1.76^{+0.03}_{-0.03}$  &  380  & 
278 & 1630$+$377 & $\rm 2.2^{+0.2}_{-0.4}$ &   17            &     10   \\
1216$+$069 & $\rm 1.73^{+0.08}_{-0.10}$ & 54 & 79 & 1634$+$706 & $\rm 2.04^{+0.09}_{-0.09}$   &  79  & 84\\ 
1226$+$023 & $\rm 1.634^{+0.009}_{-0.009}$ & 260              & 193
 & 2214$+$139 & $\rm 0.94^{+0.04}_{-0.04}$ &    469 & 256\\ 
1244$+$026 & $\rm 2.55^{+0.11}_{-0.11}$  &  69  &  55 &  2302$+$029   &  $\rm 2.2^{+0.3}_{-0.2}$  & 13  &  23\\ 
\hline
\end{tabular}
\end{table}