\begin{table}%t7 %\centering \par \caption{\label{apex-ir-luminosity}Properties of the ATLASGAL sources with a counterpart in the mid-infrared emission, derived by fitting the 870 and 70~$\mu$m points with a modified black body.} \begin{tabular}{c c r c c c c c c } \hline\hline \noalign{\smallskip} Source & Radius & $d$\tablefootmark{a} & $F_{24~\mu{\rm m}}$ & $F_{70~\mu {\rm m}}$ & $T_d$ & $L$ & $M$ & $\Sigma$\\ &(pc) & (kpc) & (Jy) & (Jy) & (K) & ($\times$$10^4~L_{\odot}$) & ($\times$$ 10^2~M_{\odot}$) & (g~cm$^{-2}$)\\ (1)&(2)&(3)&(4)&(5)&(6)&(7)&(8)&(9)\\ \hline C2 & 0.7 & 12.6 & 7.6 $\pm$ 1.5 & 119.8 $\pm$ 24.0 & 25 & 5 & 60 & 0.81 \\ C3 & 0.7 & 12.6 & 4.0 $\pm$ 0.8 & 68.8 $\pm$ 13.8 & 25 & 3 & 30 & 0.41 \\ C4 & 0.7 & 12.6 & 2.1 $\pm$ 0.4 & 42.8 $\pm$ 8.6 & 27 & 2 & 10 & 0.14 \\ C5 & 0.7 & 12.6 & 3.8 $\pm$ 0.8 & 29.0 $\pm$ 5.8 & 26 & 1 & 10 & 0.14 \\ C7 & 0.7 & 11.7 & 9.1 $\pm$ 1.8 & 107.3 $\pm$ 21.5 & 28 & 3 & 20 & 0.27 \\ C8 & 0.7 & 11.7 & 7.2 $\pm$ 1.4 & 94.2 $\pm$ 18.8 & 33 & 2 & 6 & 0.08 \\ C10 & 0.7 & 11.7 & -- & 100.6 $\pm$ 20.1 & 29 & 3 & 10 & 0.14 \\ C11 & 0.7 & 11.7 & 6.8 $\pm$ 1.4 & 51.4 $\pm$ 10.3 & 28 & 2 & 9 & 0.12 \\ C13 & 0.6 & 11.7 & 2.6 $\pm$ 0.5 & 72.0 $\pm$ 14.4 & 32 & 1 & 4 & 0.07 \\ C14 & 0.5 & 4.7 & 5.1 $\pm$ 1.0 & 17.8 $\pm$ 3.6 & 20 & 0.3 & 9 & 0.24 \\ \hline \end{tabular} \tablefoot{Column~(1): ATLASGAL continuum source; Col.~(2): radius of the APEX continuum source; Col.~(3): distance of the source; Col.~(4): flux density at 24~$\mu$m of the IR source associated with the ATLASGAL 870~$\mu$m source; Col.~(5): flux density at 70~$\mu$m of the IR source associated with the ATLASGAL 870~$\mu$m source; Col.~(6)--(8): output of the modified black body fit. In particular: the dust temperature; the luminosity; the mass; and the surface density. \tablefoottext{a}{All the sources are assumed to be at the far kinematic distances, except C14.}} \end{table}