\begin{table}%t6
\caption{Broad-band  fluxes 
and power-law fit ($F_{\nu}=F_{\nu_0}(\nu/\nu_0)^{-\alpha_{\nu}}$) 
parameters of the emission from different regions of the PWN marked in Fig.~\ref{f:PWNstady}.  
Their offsets from the pulsar and areas are given in the 2nd and 3rd columns. 
Upper and lower 
values for each entry of the fluxes are the measured and dereddened fluxes 
with $E(B-V)=0.20$ ($A_V=0.62$), respectively. }
\label{t:PWN-phot}
%\begin{center}
{
\begin{tabular}{lllccccccc}
\hline
\hline
\multicolumn{3}{c}{Source}&  &\multicolumn{3}{c}{Band} & &\multicolumn{2}{c}{Power-law fit} \wideru \\
\cline{1-3} \cline{5-7} \cline{9-10} 
%\hline
%      &   &   &  &    &    &   & &          \\ 
Region   & Offset & Area &  & {\it F336W}    & {\it F547M}  &  {\it F791W} & &$\alpha_{\nu}$&${\rm log}~F_{\nu_0}$, $\nu_0=5.47\times10^{14}$ Hz   \\
         &        &arcsec$^2$ &  & \multicolumn{3}{c}{ Log flux from the area~~~{\rm $\mu$Jy} }      & & &  {\rm $\mu$Jy}       \\  
\cline{1-3} \cline{5-7} \cline{9-10}         
%\hline 
%      &   &     &  &  &    &   & & &         \\ 
Full PWN   &  0\farcs000 N  &10.92  &    &   1.688(6)   &   2.177(7) & 2.482(8)  & & --  & --         \\
             &  0\farcs000 W  &       &    &   2.093(6)   &   2.426(7) & 2.640(8)  & & $\rm 1.48^{+(9)}_{-(8)}$  & 2.414(12)   \\
 %     &   &     &  &  &    &   & & &         \\ 
Area 1           &  0\farcs455 S   &  0.33  &  & 0.350(116)   &0.647(94)    &0.991(48)   & & --  &  --        \\ 
             & 0\farcs409  W   &        &  &0.755(116)   & 0.896(94)   &1.144(48)   & &$\rm 1.09^{+(33)}_{-(30)}$ &  0.949(50)   \\  
 %     &   &     &  &  &    &   & & &         \\        
Area 2           &  1\farcs001 S   &  0.33  &  & 0.224(146)   &0.766(35)    &1.054(30)   & & --  &  --        \\ 
             & 0\farcs910  W   &        &  &0.629(146)   & 1.015(35)   &1.207(48)   & &$\rm 1.58^{+(43)}_{-(42)}$ & 0.980(45)    \\
 %     &   &     &  &  &    &   & & &         \\        
Area 3           &  1\farcs456 S   &  0.33  &  & 0.176(147)   &0.628(60)    &0.892(45)   & & --  &  --        \\ 
             & 1\farcs365  W   &        &  &0.581(147)   &0.877(60)   &1.045(45)   & &$\rm 1.28^{+(43)}_{-(41)}$ &  0.856(49)   \\
 %     &   &     &  &  &    &   & & &         \\        
Area 4           &  0\farcs409 N   &  0.33  &  & 0.114(236)   &0.582(128)    &0.868(102)   & & --  &  --        \\ 
             & 0\farcs364 E   &        &  &0.519(236)   &0.831(128)   &1.021(102)   & &$\rm 1.49^{+(67)}_{-(59)}$ &  0.806(58)   \\
 %     &   &     &  &  &    &   & & &         \\        
Area 5           &  1\farcs046 N   &  0.33  &  & 0.252(140)   &0.485(106)    &0.791(64)   & & --  &  --        \\ 
             & 0\farcs865 E   &        &  &0.657(140)   &0.734(128)   &0.944(64)   & &$\rm 0.92^{+(37)}_{-(33)}$ &  0.786(58)    \\
 %      &   &     &  &  &    &   & & &         \\        
Area 6          &  1\farcs775 N    &  0.33  &  & $\le$0.032$^a$ &0.239(98)   &0.377(102)   & & --  &  --        \\ 
             & 1\farcs365 E   &        &  & $\le$0.437     &0.488(98)   &0.530(102)   & &$\rm 0.27^{+(91)}_{-(90)}$ &  0.488(98)   \\
  %    &   &     &  &  &    &   & & &         \\   
North Jet    & 1\farcs001 N    &  0.96  &  & $\le$0.265$^a$ &0.642(50)   &0.875(68)   & & --  &  --        \\ 
             & 2\farcs366 W    &        &  & $\le$0.670     &0.891(50)   &1.028(68)   & &$\rm 0.87^{+(56)}_{-(54)}$ &  0.891(51)   \\
 %      &   &     &  &  &    &   & & &         \\   
South Jet    & 1\farcs274 S    &  0.96  &  & 0.483(128)     &0.796(43)   &1.105(33)   & & --  &  --        \\ 
             & 1\farcs547 W    &        &  & 0.888(128)     &1.045(43)   &1.258(33)   & &$\rm 1.03^{+(35)}_{-(30)}$ &  1.077(38) \\  
\hline
\end{tabular}}
$^a$~3$\sigma$ upper limit.
%\end{center}
\end{table}