\begin{table}%t2 %%\centering \par \caption{\label{table_mir_continuum}Parameters from the Spitzer IRS spectra.} %\centerline {\small \begin{tabular}{lrrrrrr} \hline \hline 2MASS & $LW$2 / & $F$15 & $F$24 & $F$35 &[Ne~III]&[S~III] \\ & 6--10~$\mu$m & mJy & mJy & mJy & 15.55 & 18.71 \\ \hline 00285431$-$7726146 & 0.57 & 7.03 & 9.3 & 27.2 & 6.1 & 16.0 \\ % 264 00445167$-$2653191 & & & 4.8 & 11.7 & -- & -- \\ % 7672 01051501$-$2612466 & 0.49 & 2.88 & 4.6 & 11.6 & 5.8 & 12.0 \\ % 7729 02542961$+$1509122 & 0.52 & 2.15 & 3.0 & 8.1 & 1.6 & 4.2 \\ %11224 03574895$-$1340458 & 0.61 &14.48 & 25.2 & 85.0 & 3.6 & 19.1 \\ % 9160 06033357$-$4509412 & & & 89.3 & 468.5 & -- & -- \\ % 5223 12482307$-$0344102 & & & 4.7 & 12.0 & -- & 2.4 \\ % 9959 13165999$-$3336459 & & & 5.3 & 14.2 & -- & 2.6 \\ % 6153 13371721$+$0904430 & & & 6.2 & 22.8 & -- & 2.1 \\ %10888 15160785$-$1608098 & & & 3.3 & 9.5 & -- & 3.0 \\ % 9023 15554606$+$1532218\parbox{0cm}{$^{\rm ~*}$} & 0.40 & 2.88 & 5.3 & 13.7 & 2.5 & 5.9 \\ %11233 16132299$+$4203418 & & & 13.6 & 51.4 & -- & 6.1 \\ %13447 19184395$-$3815471 & & & 7.7 & 24.8 & -- & 0.8 \\ % 5792 21573517$+$0114331 & 0.42 & 3.06 & 3.9 & 9.6 & $<$0.7 & 3.2 \\ %10416 22023161$-$5657577 & 0.58 & 4.34 & 7.6 & 18.7 & $<$2.0 & 8.1 \\ % 4261 22565483$-$3649515 & 0.58 & 1.60 & 2.2 & 6.0 & $<$1.0 & 5.2 \\ % 5973 23055422$-$3539591 & & & 3.0 & 7.7 & -- & -- \\ % 6039 23075850$+$0537063 & & & 3.2 & 9.5 & -- & -- \\ %10702 23080919$+$0538305 & 0.41 & 3.22 & 4.6 & 11.6 & $<$0.7 & 4.1 \\ %10707 \hline \end{tabular}} \medskip The second column gives the fraction of the 6--10~$\mu$m flux seen in the $LW2$ passband (5--8.5~$\mu$m). F15 refers to the flux integrated over the ISOCAM $LW3$ passband (12--18~$\mu$m). The uncertainty of the continua F15, F24, and F35 are about 10\%. Emission line fluxes are given in 10$^{\rm -15}$~erg/s/cm$^{2}$ with $\sim$10--20\% uncertainties; $^*$)~absolute photometry uncertain, see footnote in Sect.~\ref{sect_data_mir_spectroscopy}. \end{table}