\begin{table}%t5 \caption{\label{tab5}Integrated optical depths of optically thin lines (see Sects.~4.1.2 and 4.1.3) and resulting excitation temperatures.} \par %\centerline { \begin{tabular}{ccccccc} \hline\hline Species & \multicolumn{3}{c}{$\int \tau {\rm d} V$} & \multicolumn{3}{c}{Excitation temperature} \\ & $J=1\leftarrow0$ & $J=2\leftarrow1^a$ & $J=2\leftarrow1/J=1\leftarrow0^a$ & $T_{\rm ex, 1-0}^b$ & $T_{\rm ex, 2-1}^{a,b}$ & $T_{\rm ex,LTE}^c$ \\ & \multicolumn{2}{c}{(km~s$^{-1}$)} & & \multicolumn{3}{c}{(K)} \\ \hline SiO & $0.412\pm0.021$ & $1.440\pm0.270$ & $3.495\pm0.679$ & 5.51 & 5.21 & 23 \\ C$^{34}$S$^a$ & $0.292\pm0.020$ & $0.440\pm0.040$ & $1.507\pm0.172$ & 5.83 & 5.27 & $7.2\pm0.4$ \\ H$^{13}$CO$^+$& $2.804\pm0.259$ & $2.500\pm0.050$ & $0.892\pm0.084$ & 5.20 & 5.17 & $3.8\pm0.3$ \\ H$^{13}$CN & $1.791\pm0.243$ & $2.100\pm0.080$ & $1.173\pm0.165$ & 5.37 & 5.24 & $4.8\pm0.5$ \\ HN$^{13}$C & $0.307\pm0.181$ & $0.900\pm0.070$ & $2.932\pm1.743$ & 5.20 & 5.17 & -- \\ & & & & & \\ CS-NE$^d$ & $0.080\pm0.010$ & $0.280\pm0.080$ & $3.500\pm1.092$ & -- & -- & $11 \pm 3 $ \\ \hline \end{tabular}} \medskip \par $^a$ In the cases of C$^{34}$S and CS, $J =2 \leftarrow 1$ should be replaced by $J =4 \leftarrow3$. With the exception of the SiO $J =2 \leftarrow 1$ line (Fig.~\ref{fig3}), the $J =2 \leftarrow 1$ and $4\leftarrow3$ data were taken from Muller et~al. (\cite{muller06}). $^b$ LVG excitation temperatures of optically thin lines with $T_{\rm kin} = 80$~K, $T_{\rm CMB} = 5.14$~K, and $n$(H$_2) = 2000$~cm$^{-3}$. $^c$ Excitation temperatures under conditions of Local Thermodynamical Equilibrium (LTE). For the uncertainty in the estimate from SiO (this includes so far unpublished SiO $J=4$--3 data), see Sect.~4.1.2. $^d$ CS absorption toward the north-eastern continuum component, displaced from the main absorption line by --147~km~s$^{-1}$. Since no spatial density has been derived for this feature, Cols.~5 and 6 are left empty. \end{table}