\begin{table}%t2 \caption{\label{tab2}Sources parameters.} \par \small%\centerline { \begin{tabular}{lrc|lrc|lrc} \hline \hline \s MSX6C Name &\s $\alpha$ &\s $EM$ &\s MSX6C Name &\s $\alpha$ &\s $EM$ &\s MSX6C Name &\s $\alpha$ &\s $EM$ \\ & &\s $\times 10 ^7$ [pc cm$^{-6}$] & & &\s $\times 10 ^7$ [pc cm$^{-6}$] & & &\s $\times 10 ^7$ [pc cm$^{-6}$] \\ \hline &&&&&&&& \\[-8pt] \s$17.2231+0.3952^{\dag}$ &\s$0.54$ &\s${>}3.12~~~~$ &\s$26.0905-0.0578$ &\s$0.11$ &\s$0.11$ &\s$31.0702+0.0498$ &\s$0.34$ &\s$0.19$ \\ \s$16.9440-0.0736$ &\s$0.23$ &\s$6.17 $ &\s$26.6085-0.2122$ &\s$-0.09$ &\s$0.26$ &\s$31.2803+0.0615$ &\s$0.01$ &\s$0.21$ \\ \s$18.4608-0.0034$ &\s$0.02$ &\s$3.39 $ &\s$27.4938+0.1893$ &\s$0.31$ &\s$0.03$ &\s$30.6671-0.3316$ &\s$0.13$ &\s$4.77$ \\ \s$18.7104+0.0001^{\dag}$ &\s$0.45$ &\s${>}12.80~~~~~~$ &\s$27.9777+0.0780$ &\s$0.27$ &\s$0.11$ &\s$31.2430-0.1108$ &\s$0.16$ &\s$1.12$ \\ \s$18.3029-0.3910$ &\s$-0.13$ &\s$0.11 $ &\s$28.2461+0.0134$ &\s$0.24$ &\s$0.10$ &\s$32.1514+0.1317$ &\s$-0.14$ &\s$0.06$ \\ \s$18.7084-0.1263$ &\s$-0.03$ &\s$3.76 $ &\s$28.2007-0.0494^{\dag}$ &\s$0.58$ &\s${>}2.21~~~~$ &\s$31.3948-0.2585$ &\s$0.53$ &\s$0.13$ \\ \s$19.7403+0.2799$ &\s$0.07$ &\s$0.03 $ &\s$28.6096+0.0170$ &\s$0.21$ &\s$3.25$ &\s$32.4727+0.2041$ &\s$0.34$ &\s$3.12$ \\ \s$18.8330-0.3004$ &\s$0.41$ &\s$0.50 $ &\s$28.6520+0.0271$ &\s$0.09$ &\s$0.61$ &\s$32.7977+0.1903^{\dag}$ &\s$0.31$ &\s${>}3.41~~~~$ \\ \s$21.8732+0.0076$ &\s$-0.03$ &\s$0.13 $ &\s$28.2875-0.3639$ &\s$-0.06$ &\s$1.89$ &\s$32.2718-0.2260$ &\s$-0.15$ &\s$0.25$ \\ \s$21.3853-0.2537^{\dag}$ &\s$0.32$ &\s${>}2.49~~~~$ &\s$29.2113-0.0690$ &\s$0.08$ &\s$0.73$ &\s$33.8104-0.1869$ &\s$0.32$ &\s$0.03$ \\ \s$22.7253-0.0106$ &\s$0.28$ &\s$0.07 $ &\s$29.9564-0.0174$ &\s$0.09$ &\s$3.00$ &\s$35.4672+0.1381$ &\s$0.04$ &\s$0.76$ \\ \s$23.9548+0.1494$ &\s$-0.10$ &\s$0.12 $ &\s$30.5345+0.0209$ &\s$0.08$ &\s$1.24$ &\s$35.5736+0.0678$ &\s$0.19$ &\s$0.26$ \\ \s$24.5076-0.2222^{\dag}$ &\s$0.35$ &\s${>}0.76~~~~$ &\s$30.2340-0.1392$ &\s$-0.15$ &\s$3.16$ &\s$35.5789-0.0304^{\dag}$ &\s$0.62$ &\s${>}8.96~~~~$ \\ \s$25.5196+0.2156$ &\s$0.04$ &\s$0.29 $ &\s$30.8667+0.1141$ &\s$0.34$ &\s$5.38$ &\s$38.5497+0.1636$ &\s$0.03$ &\s$0.03$ \\ \s$25.2666-0.1584$ &\s$-0.09$ &\s$10.71~$ &\s$31.4134+0.3092$ &\s$-0.13$ &\s$0.56$ &\s$38.8750+0.3088$ &\s$0.08$ &\s$2.25$ \\ \s$25.3977-0.1406$ &\s$0.00$ &\s$0.60 $ &\s$30.6877-0.0729$ &\s$0.06$ &\s$1.72$ &\s$39.8821-0.3457$ &\s$-0.07$ &\s$1.75$ \\ \s$25.3820-0.1813$ &\s$0.29$ &\s$0.80 $ &\s$30.7206-0.0826$ &\s$0.11$ &\s$3.76$ &\s$41.7410+0.0972$ &\s$-0.09$ &\s$0.08$ \\ \hline \end{tabular}} \medskip $^{\dag}$ For these sources the simulated radio spectra indicate that the emission is optically thick up to 7~mm, the derived $EM$ has to be considered as a lower limit. \vspace*{3mm} \end{table}