\begin{table}%t4 %\centering \par \caption{\label{param_cont}Physical parameters of the sources identified in the APEX 870~$\mu$m continuum emission.} \smallskip \begin{tabular}{l c c c r r r r r r r} \hline\hline \noalign{\smallskip} Source & \multicolumn{2}{c}{Peak Position} & $\Theta_{\rm C}$\tablefootmark{a} & $F_{\rm peak}$ & $v_{^{13}{\rm CO}}$ & Flux & Counterpart & $d_{\rm FAR}$ & $d_{\rm NEAR}$ & $M_{\rm cont}$\tablefootmark{b}\\ & RA[J2000.0] & Dec[J2000.0] & (arcsec) & (Jy/beam) & (km~s$^{-1}$) & (Jy) &&(kpc) & (kpc) & ($\times $$10^2~M_{\odot}$) \\ (1)&(2)&(3)&(4)&(5)&(6)&(7)&(8)&(9)&(10)&(11)\\ \hline C1 & 18:27:38.05 & --11:56:38.3 & 15.2 & 16.3 & 42.9 & 14.1 & co1 & 12.6 & 3.4 & 203.4 \\ C2 & 18:27:43.88 & --11:57:07.9 & 36.9 & 1.4 & 42.8 & 3.6 & co2 & 12.6 & 3.4 & 52.5 \\ C3 & 18:27:55.43 & --11:52:39.7 & 30.6 & 1.6 & 41.0 & 2.9 & co3 & 12.6 & 3.4 & 42.1 \\ C4 & 18:27:50.42 & --11:51:45.7 & 38.1 & 0.7 & 41.0 & 1.7 & co3 & 12.6 & 3.4 & 23.8 \\ C5 & 18:28:23.88 & --11:47:36.8 & 24.7 & 0.9 & 44.7 & 1.2 & co5 & 12.6 & 3.4 & 17.1 \\ C6 & 18:27:16.91 & --12:02:06.3 & 32.8 & 0.5 & 38.7 & 1.1 & co6 & 12.6 & 3.4 & 15.2 \\ C7 & 18:27:17.36 & --11:53:53.7 & 21.6 & 2.2 & 59.0 & 2.5 & co7 & 11.7 & 4.3 & 31.5 \\ C8 & 18:27:14.08 & --11:53:23.5 & 20.5 & 0.8 & 57.7 & 0.9 & -- & 11.7 & 4.3 & 11.1 \\ C9 & 18:27:05.36 & --11:54:54.3 & 29.0 & 0.4 & 62.5 & 0.8 & -- & 11.6 & 4.4 & 9.5 \\ C10 & 18:27:31.77 & --11:45:59.5 & 20.5 & 1.5 & 57.7 & 1.7 & co10 & 11.7 & 4.3 & 21.2 \\ C11 & 18:27:25.62 & --11:46:59.9 & 22.7 & 0.9 & 59.8 & 1.1 & co11 & 11.7 & 4.3 & 13.5 \\ C12 & 18:27:23.58 & --11:49:31.7 & 45.4 & 0.5 & 58.2 & 1.9 & co12 & 11.7 & 4.3 & 24.1 \\ C13 & 18:27:25.13 & --11:53:29.9 & 25.6 & 0.4 & 57.6 & 0.6 & co13 & 11.7 & 4.3 & 7.3 \\ C14 & 18:28:19.32 & --11:40:37.2 & 27.4 & 2.4 & 65.4 & 3.8 & co14 & 11.3 & 4.7 & 7.6 \\ \hline \end{tabular} \tablefoot{Column~(1): Sources; Cols.~(2)--(3): peak positions of the emission; Col.~(4): deconvolved angular diameters of the sources; Col.~(5): Peak flux densities of the sources; Col.~(6): velocity of the sources from the association with the FCRAO $^{13}$CO(1--0) emission; Col.~(7): integrated emission from the $FWHM$ contour of the sources; Col.~(8): FCRAO $^{13}$CO(1--0) counterpart; Col.~(9): far distance of the source from the $^{13}$CO(1--0) emission (see Table~\ref{param_nubi}); Col.~(10): near distance of the source from the $^{13}$CO(1--0) emission (see Table~\ref{param_nubi}); Col.~(11): mass from the continuum emission of the sources, assuming $T=20$~K. \tablefoottext{a}{deconvolved;} \tablefoottext{b}{all the sources are assumed to be at the far kinematic distances, except C14 (see text).}}\vspace*{2mm} \end{table}