\begin{table}%t1
%\centering
\par
\caption{\label{table1}Physical properties of the warm H$_2$ component from H$_2$ $v=0{-}0$ S(2)--S(7) lines extracted at the SL (3.5$\arcsec$) scale.}
\begin{tabular}{cccccc}
\hline \hline\noalign{\smallskip}%\\[-3.2mm]
Position & Offsets & H$_2$ 0--0 S(5)& $T$ & $N$(H$_2$)   & $\dot{M}$\tablefootmark{a} \\
		& (\arcsec) &	(10$^{-11}$ W~cm$^{-2}$ sr$^{-1}$)		& (K)  & 	( 10$^{19}$~cm$^{-2}$) & (10$^{-7}~M_{\odot}$~yr$^{-1}$)\\
\hline
%
R1 &[--20.1, 13.3] & 3.3 &1100 $\pm$ 70 & 1.15  & 1.1\\
R2 &[--29.9, 17.0] & 2.3 &1050 $\pm$ 75 & 1.3 & 1.2\\
B1 &[12.2, --4.7] & 1.3 &860 $\pm$ 40 & 1.1 & 1.1\\
B2 &[26.9, --10.3] & 2.0 &950 $\pm$ 70 & 1.5 & 1.4\\
B3 &[35.1, --10.6] & 1.9 &980 $\pm$ 75 & 1.4 & 1.4\\
%
\hline 
\end{tabular} 
\tablefoot{\tablefoottext{a}{$\dot{M}$ is proportional to ($V_{\rm jet}$/100~km~s$^{-1}$)~$\times$~(3.5$\arcsec$/$l_{\rm t}$) and is not
corrected for postshock compression.}}
\end{table}