\begin{table}%t4
\caption{Positions, peak and integrated sub-mm fluxes for the detected cores. The
effective diameters of the sub-mm cores are also given as~$D_{\rm eff}$. Note that the
peak fluxes for both 450 and 850~$\mu$m observations are measured in Jy~per~14\arcsec\
beam.}\label{tbl:fluxes}
%\centerline
{
\begin{tabular}{lccccccl}
\hline  \hline
 & & & \multicolumn{2}{c}{Peak Flux (Jy/beam)} & \multicolumn{2}{c}{Integrated Flux (Jy)} & $D_{\rm eff}$  \\
Clump ID & $\alpha_{\rm 2000}$ & $\delta_{\rm 2000}$ & 450 $\mu$m & 850 $\mu$m & 450 $\mu$m & 850 $\mu$m & (pc) \\ 
\hline
 \object{SFO 11 SMM1} & 02 51 33.7 & +60 03 54 & 1.2 $\pm$ 0.2 & 0.23 $\pm$ 0.01 & 8.1 $\pm$ 1.4 & 1.42 $\pm$ 0.15 & 0.28$^{\rm a}$ \\
 \object{SFO 11 SMM2} & 02 51 25.0 & +60 03 42 & 0.7 $\pm$ 0.2 & 0.15 $\pm$ 0.01 & 5.2 $\pm$ 0.9 &  0.53 $\pm$ 0.06 & 0.20$^{\rm a}$ \\
 \object{SFO 11 SMM3} & 02 51 29.6 & +60 03 01 & 0.7 $\pm$ 0.2& 0.13 $\pm$ 0.01 & 2.5 $\pm$ 0.6 & 0.27 $\pm$ 0.05 & 0.20$^{\rm b}$\\
& & & & & & &  \\
 \object{SFO 11NE SMM1} & 02 51 53.6 & +60 07 00 & 1.6 $\pm$ 0.1& 0.34 $\pm$ 0.02 & 4.0 $\pm$ 0.5 & 0.92 $\pm$ 0.10  & 0.24$^{\rm b}$ \\
 \object{SFO 11NE SMM2} & 02 51 59.5 & +60 06 27 & 1.0 $\pm$ 0.1 & 0.25 $\pm$ 0.02 & 2.7 $\pm$ 0.3 & 0.54 $\pm$ 0.08 & 0.16$^{\rm b}$ \\
& & & & & & &  \\
 \object{SFO 11E SMM1} & 02 52 16.8 & +60 03 19 & 5.8 $\pm$ 0.3 & 0.48 $\pm$ 0.02 & 15.5 $\pm$ 1.4 & 1.29 $\pm$ 0.10 & 0.27$^{\rm b}$ \\
 \object{SFO 11E SMM2} & 02 52 15.9 & +60 02 29 & -- & 0.21 $\pm$ 0.02 & 3.9 $\pm$ 0.7$^{\rm c}$ & 0.34 $\pm$ 0.25 & 0.12$^{\rm b}$ \\
 \object{ \object{SFO 11E SMM3}} & 02 52 19.0 & +60 02 17 & 2.7 $\pm$ 0.3 & 0.26 $\pm$ 0.02 & 3.2 $\pm$ 0.5 & 0.40 $\pm$ 0.23 & 0.11$^{\rm b}$ \\
 \hline
\end{tabular}}
\medskip
$^a$ $D_{\rm eff}$ estimated from FWHM flux contours. \\ 
$^b$ $D_{\rm eff}$ measured from Gaussian fit to azimuthal flux average. \\
$^c$ 450 $\mu$m flux measured by integrating over the same solid angle as for 850 $\mu$m.
\end{table}