\begin{table}%t3 \caption{\label{tab_flux}Results of the H$_2$ S(1) line analysis.} \par %\centerline {\begin{tabular}{lcccccccccccccccccc} \hline \hline \noalign{\smallskip} Star & $\lambda _{\rm obs}$\tablefootmark{(a)}& Integrated flux\tablefootmark{(b)} & Intensity\tablefootmark{(b)} & \multicolumn{3}{c}{$N({\rm H}_2)$ upper limits\tablefootmark{(b)}} & & \multicolumn{3}{c}{H$_2$ mass upper limits\tablefootmark{(b, c)}} \\ HD & ($\mu$m) & (\flux) & (erg~s$^{-1}$~cm$^{-2}$~sr$^{-1}$) & \multicolumn{3}{c}{(cm$^{-2}$)} & & \multicolumn{3}{c}{ ($M_{\rm Jup}$)} \\ \cline{5-7} \cline{9-11} & & & & 150~K & 300~K & 1000~K & & 150 K & 300 K & 1000 K \\ \hline 142527 & 17.0351 & $<1.0\times 10^{-14}$ & $<$2.5~$\times$~10$^{-3}$ & 9.4~$\times$~10$^{22}$ & 6.1~$\times$~10$^{21}$ & 1.4~$\times$~10$^{21}$ & & 1.9~$\times$~10$^{-1}$ & 1.2~$\times$~10$^{-2}$ & 3.3~$\times$~10$^{-3}$ \\ 169142 & 17.0343 & $<$1.8~$\times$~10$^{-14}$ & $<$4.2~$\times$~10$^{-3}$ & 1.6~$\times$~10$^{23}$ & 1.0~$\times$~10$^{22}$ & 2.4~$\times$~10$^{21}$ & & 3.5~$\times$~10$^{-1}$ & 2.1~$\times$~10$^{-2}$ & 6.1~$\times$~10$^{-3}$ \\ 150193A & 17.0349 & $<$2.1~$\times$~10$^{-14}$ & $<$5.0~$\times$~10$^{-3}$ & 1.9~$\times$~10$^{23}$ & 1.2~$\times$~10$^{22}$ & 2.8~$\times$~10$^{21}$ & & 4.5~$\times$~10$^{-1}$ & 2.7~$\times$~10$^{-2}$ & 7.7~$\times$~10$^{-3}$ \\ 163296 & 17.0345 & $<$2.8~$\times$~10$^{-14}$ & $<$6.7~$\times$~10$^{-3}$ & 2.5~$\times$~10$^{23}$ & 1.6~$\times$~10$^{22}$ & 3.8~$\times$~10$^{21}$ & & 3.9~$\times$~10$^{-1}$ & 2.4~$\times$~10$^{-2}$ & 6.9~$\times$~10$^{-3}$ \\ 100546 & 17.0363 & $<$1.4~$\times$~10$^{-13}$ & $<$3.3~$\times$~10$^{-2}$ & 1.2~$\times$~10$^{24}$ & 7.9~$\times$~10$^{22}$ & 1.9~$\times$~10$^{22}$ & & 1.4 & 8.4~$\times$~10$^{-2}$ & 2.4~$\times$~10$^{-2}$ \\ \hline \end{tabular}} \tablefoot{\tablefoottext{a}{expected position of the line in the observed spectra by correcting the radial velocity of the star for the epoch of observation.} \tablefoottext{b} {3$\sigma$ upper confidence limits.} \tablefoottext{c} {masses of H$_2$ are calculated assuming the distances quoted in Table~\ref{param}.}}\vspace*{5mm} \end{table}