\begin{table}%t1
\caption{\label{tab:ResBin}Optically resolved binaries (41~objects).}
\par
\small%\centerline
 {
\begin{tabular}{lcrrrcrr}
   \hline \hline
&&&&&&& \\[-8pt]
    Designation & $d_{{\rm proj}}$~[$\arcsec$] & $\overline{d}$ [pc] & $d_{{\rm proj}}$ [AU] & $d_{{\rm proj}}^{{\rm corr}}$~[AU] & $M_{{\rm M}}$~[$M_{\odot}$] & $P ~{\rm [yr]} \ga$ & $P^{{\rm corr}}$~[yr]\\
&&&&&&& \\[-8pt]
    \hline
     J0017$-$0009          & 1.4 &        500 &        700 &   1000 & 0.46 &        16~000 &  33~000 \\
     J0122+1542            & 1.0 &        300 &        300 &      500 & 0.17 &         6500 &  13~000 \\
     J0151$-$0800          & 1.0 &        350 &        350 &      600 & 0.17 &         8000 &  16~000 \\
     J0215+1418            & 0.9 &        700 &        600 &      900 & 0.27 &        16~000 &  30~000 \\
     J0249+3342            & 1.4 &        500 &        700 &   1200 & 0.17 &        23~000 &  45~000 \\
     J0348$-$0614          & 1.1 &        500 &        600 &      900 & 0.17 &        16~000 &  31~000 \\
     J0725+4145            & 1.3 &        400 &        500 &      900 & 0.17 &        15~000 &  29~000 \\
     J0729+4304            & 1.5 &        150 &        250 &      400 & 0.12 &         5000 &  10~000 \\
     J0739+2743            & 0.6 &        700 &        350 &      600 & 0.17 &         8000 &  16~000 \\
     J0740+3859            & 1.1 &        300 &        350 &      600 & 0.12 &         8000 &  15~000 \\
     J0741+3808            & 0.9 &        300 &        250 &      400 & 0.17 &         5000 &   9000 \\
     J0752+4332            & 1.3 &        600 &        800 &   1200 & 0.18 &        23~000 &  46~000 \\
     J0800+5002            & 1.1 &        700 &        800 &   1200 & 0.27 &        22~000 &  44~000 \\
     J0801+2216            & 1.3 &        500 &        700 &   1100 & 0.17 &        20~000 &  40~000 \\
     J0806+4035            & 1.2 &        350 &        450 &      700 & 0.17 &        11~000 &  21~000 \\
     J0809+1251            & 1.3 &        400 &        500 &      800 & 0.17 &        14~000 &  27~000 \\
     J0813+2152            & 0.9 &        900 &        800 &   1300 & 0.18 &        28~000 &  55~000 \\
     J0829+2701            & 1.4 &     1000 &     1400 &   2200 & 0.27 &        55~000 & 110~000 \\
     J0845+2348            & 1.1 &     1400 &     1400 &   2200 & 0.46 &        50~000 & 100~000 \\
     J0904+5621$^{\dag}$   & 1.5 &        200 &        300 &      450 & 0.10 &         6000 &  12~000 \\
     J0931+3941            & 1.4 &        350 &        500 &      800 & 0.17 &        13~000 &  26~000 \\
     J0939+5729            & 1.3 &        250 &        300 &      500 & 0.17 &         6000 &  12~000 \\
     J0942+1846            & 1.3 &        600 &        700 &   1200 & 0.17 &        23~000 &  45~000 \\
     J1001+3203            & 1.3 &        250 &        350 &      500 & 0.17 &         7000 &  13~000 \\
     J1006+5633            & 1.4 &     1200 &     1700 &   2700 & 0.46 &        70~000 & 135~000 \\
     J1032+3722            & 1.3 &        350 &        450 &      700 & 0.17 &        10~000 &  20~000 \\
     J1127$-$0028$^{\dag}$ & 1.5 &        200 &        250 &      400 & 0.10 &         4500 &   9000 \\
     J1127+4249            & 1.2 &        350 &        400 &      600 & 0.12 &         9000 &  18~000 \\
     J1205+0312            & 1.4 &        250 &        400 &      600 & 0.17 &         8500 &  17~000 \\
     J1209+6510$^{\dag}$   & 1.4 &        250 &        350 &      500 & 0.10 &         7500 &  14~000 \\
     J1210+0549            & 1.4 &        350 &        500 &      800 & 0.17 &        12~000 &  24~000 \\
     J1216+4328            & 1.5 &        900 &     1300 &   2000 & 0.46 &        46~000 &  90~000 \\
     J1242+4506            & 1.5 &        450 &        700 &   1100 & 0.17 &        20~000 &  40~000 \\
     J1253+5813            & 1.4 &        400 &        600 &      900 & 0.27 &        14~000 &  28~000 \\
     J1304+1449            & 1.3 &        500 &        600 &   1000 & 0.17 &        18~000 &  35~000 \\
     J1347+4129            & 1.3 &     1200 &     1600 &   2500 & 0.46 &        65~000 & 125~000 \\
     J1456+4824            & 1.4 &        450 &        600 &   1000 & 0.17 &        18~000 &  35~000 \\
     J1606+4217            & 1.1 &        500 &        600 &      900 & 0.17 &        17~000 &  35~000 \\
     J1630+1302            & 1.4 &        600 &        900 &   1420 & 0.17 &        31~000 &  60~000 \\
     J1744+2442            & 1.4 &     1100 &     1500 &   2400 & 0.46 &        55~000 & 115~000 \\
     J2200$-$0715$^{\dag}$ & 1.5 &        200 &        250 &      400 & 0.10 &         5000 &  10~000 \\
    \hline
  \end{tabular}}
\medskip
We use the mathematically exact values of $d_{{\rm proj}}$ and $d_{{\rm proj}}^{{\rm corr}}$ to compute the lower limit for $P$ and the statistically corrected $P^{{\rm corr}}$. But for this table, distances greater than 500~pc or 500~AU are rounded to the next hundred and else to the next fifty. Periods are rounded to the next 500~yr for $P < 10~000$~yr, to the next 1000~yr for 10~000~yr~$< P <$ 50~000~yr and else to the next 5000~yr. $^{\dag}$: VLMO candidates.
\end{table}