Table 4: 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 $^{\prime \prime }$ beam.
      Peak Flux (Jy/beam) 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)
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$^{\rm a}$
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$^{\rm a}$
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$^{\rm b}$
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$^{\rm b}$
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$^{\rm b}$
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$^{\rm b}$
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$^{\rm b}$
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$^{\rm b}$
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.

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