\begin{table}%t3 \caption{List of all companions detected within 10\arcsec\ (Ophiuchus) or 30\arcsec\ (Taurus) of our targets. Flux ratios are measured with respect to the brightest component in the $K$~band image, except for three systems where the Class~I source is the faintest component in the near-infrared ($\dagger$~symbol). The boldfaced entries represent systems that are likely to be physically bound (see Sect.~\ref{subsec:bf}). The two companions to IRS~54 listed in italics were detected by combining a short and a long exposure and are not included in our survey. Upper limits for flux ratios are at the 3$\sigma$~level. IRAS~04264+2433 was saturated in all of our images, so only a lower limit for the flux ratio to its companion can be obtained.}\label{tab:bin} %\centering \par \begin{tabular}{lccccccc} \hline \hline Object & $\rho$ & PA & $\Delta J$ & $\Delta H$ & $\Delta K$ & $\Sigma(K\leq K_{\rm B})$ & $P_{\rm bound}$ \\ & (\arcsec) & (\degr) & (mag) & (mag) & (mag) & ($10^{-4}$ arcsec$^{-2}$) & \\ \hline \multicolumn{8}{c}{Taurus ($0\farcs8<\rho<30$\arcsec)} \\ \hline IRAS~04016+2610 & 23.28 & 223.5 & & & 4.60 $\pm$ 0.05 & 1.6 & 0.76 \\ IRAS~04108+2803~B & 22.16 & 237.1 & & & 0.17 $\pm$ 0.02 & 0.4 & 0.94 \\ \hspace*{1.2cm}-- & 15.23 & 274.1 & & & 6.00 $\pm$ 0.05 & 1.2 & 0.92 \\ {\bf IRAS~04113+2758} & {\bf 4.03} & {\bf 152.9} & {\bf --0.94 $\pm$ 0.03} & {\bf --0.28 $\pm$ 0.03} & {\bf 0.12 $\pm$ 0.03} & {\bf 0.8} & {\bf 0.99} \\ \hspace*{1.2cm}-- & 24.80 & 279.8 & 2.96 $\pm$ 0.05 & 3.54 $\pm$ 0.05 & 3.90 $\pm$ 0.05 & 1.6 & 0.73 \\ IRAS~04158+2805 & 25.45 & 27.3 & --0.44 $\pm$ 0.02 & 0.05 $\pm$ 0.02 & 0.94 $\pm$ 0.02 & 0.8 & 0.85 \\ \hspace*{1.2cm}-- & 28.95 & 246.5 & 3.86 $\pm$ 0.05 & 4.23 $\pm$ 0.05 & 5.08 $\pm$ 0.05 & 5.3 & 0.25 \\ IRAS~04181+2654~B & 22.22 & 248.5 & & & 4.45 $\pm$ 0.05 & 2.5 & 0.68 \\ {\bf IRAS~04191+1523} & {\bf 6.09} & {\bf 303.7} & {\bf $>$2.05} & {\bf 2.15 $\pm$ 0.05} & {\bf 2.06 $\pm$ 0.03} & {\bf 0.8} & {\bf 0.99} \\ \hspace*{1.2cm}-- & 28.30 & 290.0 & $>$$2.05$ & $>$$4.50$ & 4.80 $\pm$ 0.10 & 6.5 & 0.20 \\ IRAS~04239+2436 & 22.12 & 319.9 & & & 4.80 $\pm$ 0.05 & 1.2 & 0.83 \\ {\bf IRAS~04248+2612} & {\bf 4.55} & {\bf 15.1} & & & {\bf 4.60 $\pm$ 0.10} & {\bf 3.7} & {\bf 0.98} \\ IRAS~04260+2642 & 12.30 & 279.4 & & & 5.67 $\pm$ 0.10 & 9.0 & 0.65 \\ {\bf IRAS~04263+2426} & {\bf 1.27} & {\bf 353.3} & & & {\bf 1.05 $\pm$ 0.05} & {\bf 0.4} & {\bf 0.99} \\ IRAS~04264+2433 & 10.93 & 295.6 & $>$$6.1$ & $>$$6.4$ & $>$$5.9$ & 2.5 & 0.91 \\ IRAS~04302+2247 & 22.64 & 120.5 & & & 3.88 $\pm$ 0.05 & 5.3 & 0.43 \\ \hspace*{1.2cm}-- & 27.27 & 263.2 & & & 4.20 $\pm$ 0.05 & 7.8 & 0.16 \\ \hspace*{1.2cm}-- & 19.34 & 114.4 & & & 4.40 $\pm$ 0.08 & 8.6 & 0.37 \\ {\bf IRAS~04325+2402} & {\bf 8.15} & {\bf 350.5} & & {\bf 2.42 $\pm$ 0.10} & {\bf 2.43 $\pm$ 0.05} & {\bf 1.2} & {\bf 0.98} \\ IRAS~04365+2535 & 12.48 & 133.6 & & & 6.25 $\pm$ 0.15 & 5.7 & 0.76 \\ IRAS~04381+2540 & 25.92 & 177.4 & & & 6.80 $\pm$ 0.15 & 5.3 & 0.33 \\ {\bf IRAS~04385+2550} & {\bf 18.90} & {\bf 342.0} & {\bf 2.73 $\pm$ 0.03} & {\bf 2.90 $\pm$ 0.03} & {\bf 3.20 $\pm$ 0.03} & {\bf 0.4} & {\bf 0.96} \\ IRAS~04889+3042 & 12.32 & 20.5 & & & 4.46 $\pm$ 0.05 & 2.4 & 0.89 \\ \hspace*{1.2cm}-- & 20.67 & 295.9 & & & 6.05 $\pm$ 0.10 & 6.9 & 0.40 \\ \hline \multicolumn{8}{c}{Ophiuchus ($0\farcs8<\rho<10$\arcsec)} \\ \hline {\bf LFAM~1$ \dagger$} & {\bf 9.35} & {\bf 104.9} & & & {\bf --4.03 $\pm$ 0.10} & {\bf 1.1} & {\bf 0.97} \\ {\bf GY~11} & {\bf 6.20} & {\bf 86.1} & & & {\bf 0.76 $\pm$ 0.05} & {\bf 3.2} & {\bf 0.96} \\ \hspace*{0.4cm}-- & 6.73 & 40.9 & & & 2.10 $\pm$ 0.10 & 4.5 & 0.94 \\ {\bf VSSG~27} & {\bf 1.22} & {\bf 64.3} & & {\bf 0.84 $\pm$ 0.10} & {\bf 1.32 $\pm$ 0.05} & {\bf 0.7} & {\bf 0.99} \\ {\bf \hspace*{0.4cm}--} & {\bf 5.73} & {\bf 95.7} & & {\bf 4.81 $\pm$ 0.15} & {\bf 5.29 $\pm$ 0.05} & {\bf 2.4} & {\bf 0.98} \\ {\bf WL~2} & {\bf 4.24} & {\bf 341.1} & & {\bf 1.35 $\pm$ 0.03} & {\bf 1.36 $\pm$ 0.02} & {\bf 0.4} & {\bf 0.99} \\ {\bf WL~20$ \dagger$} & {\bf 3.66} & {\bf 51.5} & & & {\bf --3.13 $\pm$ 0.03} & {\bf 0.2} & {\bf 0.99} \\ {\bf \hspace*{0.4cm}--} & {\bf 2.24} & {\bf 351.9} & & & {\bf --2.89 $\pm$ 0.03} & {\bf 0.2} & {\bf 0.99} \\ {\bf IRS~37 $\dagger$} & {\bf 8.68} & {\bf 63.7} & & & {\bf --1.60 $\pm$ 0.03} & {\bf 0.2} & {\bf 0.99} \\ {\bf IRS~43} & {\bf 7.12} & {\bf 321.5} & & & {\bf 2.98 $\pm$ 0.05} & {\bf 1.3} & {\bf 0.98} \\ {\bf IRS~51} & {\bf 1.62} & {\bf 9.0} & & & {\bf 3.67 $\pm$ 0.05} & {\bf 1.1} & {\bf 0.99} \\ {\bf IRS~54} & {\bf 7.17} & {\bf 323.1} & & {\bf 5.40 $\pm$ 0.10} & {\bf 5.10 $\pm$ 0.03} & {\bf 1.9} & {\bf 0.97} \\ \hspace*{0.4cm}-- & \it 9.01 & \it 86.4 & \it & $>$${\it 5.9}$ & \it 7.97 $\pm$ 0.05 & \it ${\it 7.8}$ & \it 0.82 \\ \hspace*{0.4cm}-- & \it 7.14 & \it 202.4 & \it & $>$${\it 5.9}$ & \it 9.09 $\pm$ 0.10 & \it ${\it 2.0}$ & \it 0.73 \\ {\bf IRS~67} & {\bf 2.83} & {\bf 300.0} & & & {\bf 4.13 $\pm$ 0.10} & {\bf 9.1} & {\bf 0.98} \\ ISO~1632021-245616 & 7.78 & 179.8 & & & 6.7 $\pm$ 0.2 & 15. & 0.75 \\ \hline \end{tabular} \end{table}