\begin{table}%t1 %\centering \par \caption {\label{TabFit}CH$^{+}$ $(0{-}1)$ and $^{13}$CH$^{+}$ $(0{-}1)$ absorption lines analysis. The column densities are derived assuming an excitation temperature $T_{\rm ex} = 3$~K.} \begin{tabular}{l l c c c c c c c c} \hline\hline \noalign{\smallskip} Source & Velocity component & $\upsilon_{\rm min}$ & $\upsilon_{\rm max}$ & $N$(CH$^{+}$) & $N$($^{13}$CH$^{+}$) & $50\times N$($^{13}$CH$^{+}$) & $N({\rm HCO}^{+})$\tablefootmark{a} & $\frac{N({\rm CH}^{+})}{N({\rm HCO}^{+})}$ & $N_{\rm H}$\tablefootmark{b} \\ & & km s$^{-1}$ & km s$^{-1}$ & $10^{13}$ cm$^{-2}$ & $10^{12}$ cm$^{-2}$ & $10^{13}$ cm$^{-2}$ & $10^{12}$ cm$^{-2}$ & & $10^{22}$ cm$^{-2}$ \\ \hline {\bf \object{W33A}} & $\left. \begin{array}{l l l} {\rm star~~forming~~region} \\ {\rm foreground} \end{array} \right. $ & $\left. \begin{array}{c c c} 19 \\ -4 \end{array} \right. $ & $\left. \begin{array}{c c c} 60 \\ 19 \end{array} \right. $ & $\left. \begin{array}{c c c} {>} 16.7 \\ 0.8 \pm 0.1 \end{array} \right. $ & $\left. \begin{array}{c c c} - \\ - \end{array} \right. $ & $\left. \begin{array}{c c c} - \\ - \end{array} \right. $ & $\left. \begin{array}{c c c} - \\ - \end{array} \right. $ & $\left. \begin{array}{c c c} - \\ - \end{array} \right. $ & $0.8 \pm 0.4$ \\[0.4cm] {\bf \object{W49N}} & $\left. \begin{array}{l l l} {\rm star~~forming~~region} \\ {\rm foreground} \end{array} \right. $ & $\left. \begin{array}{c c c} -20 \\ 30 \end{array} \right. $ & $\left. \begin{array}{c c c} 30 \\ 80 \end{array} \right. $ & $\left. \begin{array}{c c c} {>} 16.6 \\ {>}27.7 \end{array} \right. $ & $\left. \begin{array}{c c c} {>} 6.7 \\ 7.8 \pm 0.6 \end{array} \right. $ & $\left. \begin{array}{c c c} {>} 33.5 \\ 39 \pm 3 \end{array} \right. $ & $\left. \begin{array}{c c c} - \\ 25 \pm 1 \end{array} \right. $ & $\left. \begin{array}{c c c} - \\ {>} 11 \end{array} \right. $ & $4.1 \pm 0.4$ \\[0.4cm] {\bf \object{W51}} & $\left. \begin{array}{l l l} {\rm star~~forming~~region} \\ {\rm foreground} \\ {\rm foreground} \end{array} \right. $ & $\left. \begin{array}{c c c} 43 \\ 15 \\ -2 \end{array} \right. $ & $\left. \begin{array}{c c c} 80 \\ 43 \\ 15 \end{array} \right. $ & $\left. \begin{array}{c c c} {>} 12.8 \\ 1.0 \pm 0.1 \\ 1.7 \pm 0.1 \end{array} \right. $ & $\left. \begin{array}{c c c} {>} 5.4 \\ - \\ - \end{array} \right. $ & $\left. \begin{array}{c c c} {>} 27.0 \\ - \\ - \end{array} \right. $ & $\left. \begin{array}{c c c} - \\ {<} 0.25 \\ 4.1 \pm 0.4 \end{array} \right. $ & $\left. \begin{array}{c c c} - \\ {>} 40 \\ 4 \end{array} \right. $ & $2.5 \pm 0.6$ \\ \hline \end{tabular} \tablefoot { \tablefootmark {a}{From Godard et~al. (2010).} \tablefootmark {b}{From models of the extinction at 2 $\mu$m by Marshall et~al. (2006).}} \end{table}