\begin{table}%t3
%\centering
\par
\caption{\label{table:3}Newly derived masses and dissolution times for the studied clusters.}
%\centering
 \small \begin{tabular}  {@{}l@{}cccccccc@{}}
  \hline \hline\noalign{\smallskip}
Name  &  $\alpha_{J2000}$ &  $\delta_{J2000}$ & $J$ &  $H$  & $K$ &  $\log$ Mass & $\varepsilon$log Mass &  $t_{\rm diss}^{\rm Pap-III}$\\    
& & & & & & ($M_{\odot}$)& ($M_{\odot}$) & (Myr)  \\   % [Myr] & [Myr]
 \hline \noalign{\smallskip}
B015D-D041  & ~$00^{\rm h}$$41^{\rm m}$$02.74^{\rm s}$ & $+41\degr$$06\arcmin$$36.63\arcsec$ & 17.03  $\pm$  0.42  & 15.37  $\pm$  0.27  & 14.89  $\pm$  0.25  & 4.2    & 0.09  & 112      \\ [1ex]    
B040-G102   & ~$00^{\rm h}$$41^{\rm m}$$38.90^{\rm s}$ & $+40\degr$$40\arcmin$$54.15\arcsec$ & 15.48  $\pm$  0.08  & 14.90  $\pm$  0.19  & 14.50  $\pm$  0.15  & 4.6    & 0.07  & 631      \\ [1ex]    
B043-G106   & $00^{\rm h}$$41^{\rm m}$$42.31^{\rm s}$ & $+40\degr$$42\arcmin$$39.86\arcsec$ & 15.58  $\pm$  0.07  & 15.50  $\pm$  0.31  & 15.08  $\pm$  1.00  & 4.4    & 0.10  & 3467     \\ [1ex]    
B066-G128   & $00^{\rm h}$$42^{\rm m}$$03.14^{\rm s}$ & $+40\degr$$44\arcmin$$48.55\arcsec$ & 16.25  $\pm$  0.19  & 15.81  $\pm$  0.47  & 16.06  $\pm$  1.00  & 4.2    & 0.08  & 891      \\ [1ex]    
B081-G142   & $00^{\rm h}$$42^{\rm m}$$13.59^{\rm s}$ & $+40\degr$$48\arcmin$$38.96\arcsec$ & 14.55  $\pm$  0.05  & 13.77  $\pm$  0.07  & 13.76  $\pm$  0.06  & 5.1    & 0.04  & 955      \\ [1ex]    
B257D-D073  &  $00^{\rm h}$$44^{\rm m}$$59.35^{\rm s}$ & $+41\degr$$54\arcmin$$47.47\arcsec$ & 15.28  $\pm$  0.10  & 14.77  $\pm$  0.20  & 15.53  $\pm$  1.00  & 4.6    & 0.09  & 302      \\ [1ex]    
B318-G042   &  $00^{\rm h}$$40^{\rm m}$$00.80^{\rm s}$ & $+40\degr$$34\arcmin$$09.06\arcsec$ & 16.17 $\pm$ 1.00  & 16.39 $\pm$ 0.66  & 15.49 $\pm$ 1.00  & 3.8    & 0.29  & 1905     \\ [1ex]    
B321-G046   &  $00^{\rm h}$$40^{\rm m}$$15.33^{\rm s}$ & $+40\degr$$27\arcmin$$45.98\arcsec$ & 17.11 $\pm$ 0.45  & 15.88 $\pm$ 0.57  & 15.18 $\pm$ 0.29  & 4.2    & 0.13  & 200      \\ [1ex]    
B327-G053   & ~$00^{\rm h}$$40^{\rm m}$$24.12^{\rm s}$ & $+40\degr$$36\arcmin$$22.38\arcsec$ & 14.91 $\pm$ 0.07  & 14.32 $\pm$ 0.10  & 14.14 $\pm$ 0.15  & 4.5    & 0.06  & 2754     \\ [1ex]    
B376-G309   & ~$00^{\rm h}$$45^{\rm m}$$48.38^{\rm s}$ & $+41\degr$$42\arcmin$$39.87\arcsec$ & 16.59 $\pm$ 0.18  & 16.07 $\pm$ 0.80  & 16.02 $\pm$ 1.00  & 4.1    & 0.09  & 295      \\ [1ex]    
B448-D035   & ~$00^{\rm h}$$40^{\rm m}$$36.52^{\rm s}$ & $+40\degr$$40\arcmin$$14.94\arcsec$ & 16.51 $\pm$ 0.34  & 16.45 $\pm$ 1.00  & 15.66 $\pm$ 1.22  & 4.1    & 0.16  & 115      \\ [1ex]    
B475-V128   & ~$00^{\rm h}$$44^{\rm m}$$55.92^{\rm s}$ & $+41\degr$$54\arcmin$$00.33\arcsec$ & 15.10 $\pm$ 0.08  & 14.68 $\pm$ 0.12  & 14.38 $\pm$ 0.17  & 4.7    & 0.07  & 1445     \\ [1ex]    
V031        & ~$00^{\rm h}$$41^{\rm m}$$12.17^{\rm s}$ & $+41\degr$$05\arcmin$$30.21\arcsec$ & 14.80 $\pm$ 0.06  & 14.42 $\pm$ 1.00  & 13.77 $\pm$ 0.11  & 4.8    & 0.10  & 1230     \\ [1ex]    
B083-G146   & ~$00^{\rm h}$$42^{\rm m}$$16.46^{\rm s}$ & $+41\degr$$45\arcmin$$20.53\arcsec$ & 14.88 $\pm$ 0.05  & 14.62 $\pm$ 0.12  & 14.07 $\pm$ 0.13  & $>$4.7 & $\dots$ & $\dots$  \\ [1ex] % 19055 
B222-G277   & $00^{\rm h}$$44^{\rm m}$$25.29^{\rm s}$  & $+41\degr$$14\arcmin$$11.62\arcsec$ & 15.27 $\pm$ 0.13  & 14.41 $\pm$ 0.09  & 14.16 $\pm$ 0.08  & $>$4.6 & $\dots$ & $\dots$  \\ [1ex] % 19055 
B347-G154   & $00^{\rm h}$$42^{\rm m}$$22.89^{\rm s}$  & $+41\degr$$54\arcmin$$27.40\arcsec$ & 14.68 $\pm$ 0.05  & 14.17 $\pm$ 0.04  & 14.17 $\pm$ 0.18  & $>$4.7 & $\dots$ & $\dots$  \\ [1ex] % 19055 
B374-G306   & $00^{\rm h}$$45^{\rm m}$$44.53^{\rm s}$  & $+41\degr$$41\arcmin$$55.10\arcsec$ & 17.21 $\pm$ 0.50  & 18.50 $\pm$ 0.82  & 16.32 $\pm$ 0.84  & $>$3.9 & $\dots$ & $\dots$  \\ [1ex] % 14791 
NB16        & $00^{\rm h}$$42^{\rm m}$$33.11^{\rm s}$  & $+41\degr$$20\arcmin$$16.48\arcsec$ & 14.91 $\pm$ 0.09  & 14.11 $\pm$ 0.07  & 13.46 $\pm$ 0.11  & $>$4.8 & $\dots$ & $\dots$  \\ [1ex] % 19055 
\hline
P09b\\
%\hline
B049-G112   & $00^{\rm h}$$41^{\rm m}$$45.59^{\rm s}$ & $+40\degr$$49\arcmin$$54.53\arcsec$ & 15.53 $\pm$ 0.13  & 15.27 $\pm$ 0.23  & 14.42 $\pm$ 0.06  & 4.5       & 0.09        & $\dots$  \\ [1ex]       
B367-G292   & $\dots$ & $\dots$ & $\dots$           &  $\dots$          &  $\dots$          & [4.3]$^a$   & [0.11]    & $\dots$  \\ [1ex]    
B458-D049   & $00^{\rm h}$$41^{\rm m}$$44.60^{\rm s}$ & $+40\degr$$51\arcmin$$20.40\arcsec$ & 16.69 $\pm$ 0.35  & 15.04 $\pm$ 0.15  & 14.96 $\pm$ 0.15  & 4.1       & 0.15        & $\dots$  \\ [1ex]       
B521        & $00^{\rm h}$$41^{\rm m}$$41.80^{\rm s}$ & $+40\degr$$52\arcmin$$02.41\arcsec$ & 17.32 $\pm$ 0.51  & 16.27 $\pm$ 0.43  & 16.28 $\pm$ 0.60  & 3.9       & 0.16        & $\dots$  \\ [1ex]       
M039        & $\dots                $ & $\dots$                               & $\dots$           & $\dots$           & $\dots$           & [3.8]$^a$   & [0.16]    & $\dots$  \\ [1ex]    
M050        & $00^{\rm h}$$44^{\rm m}$$40.83^{\rm s}$ & $+41\degr$$30\arcmin$$09.68\arcsec$ & 16.14 $\pm$ 0.14  & 14.90 $\pm$ 0.19  & 15.01 $\pm$ 0.31  & 4.3       & 0.13        & $\dots$  \\ [1ex]       
\hline
WH01\\
%\hline  								    
B315-G038   & $00^{\rm h}$$39^{\rm m}$$48.51^{\rm s}$ & $+40\degr$$31\arcmin$$30.33\arcsec$ & 14.99 $\pm$ 0.09  & 14.49 $\pm$ 0.10  & 14.24 $\pm$ 0.09  & 4.6       & 0.05    &  4074    \\ [1ex]   
B319-G044   & $00^{\rm h}$$40^{\rm m}$$03.03^{\rm s}$ & $+40\degr$$33\arcmin$$58.25\arcsec$ & 16.30 $\pm$ 0.12  & 15.94 $\pm$ 0.47  & 16.78 $\pm$ 0.52  & 3.9       & 0.10    &  182    \\ [1ex]   
B342-G094   & $00^{\rm h}$$41^{\rm m}$$24.15^{\rm s}$ & $+40\degr$$36\arcmin$$48.55\arcsec$ & 16.67 $\pm$ 0.48  & 15.57 $\pm$ 0.38  & 16.94 $\pm$ 1.00  & 4.0       & 0.17    &  214    \\ [1ex]   
B368-G293   & $00^{\rm h}$$44^{\rm m}$$47.50^{\rm s}$ & $+41\degr$$51\arcmin$$09.39\arcsec$ & 15.89 $\pm$ 0.27  & 15.14 $\pm$ 0.35  & 14.60 $\pm$ 0.21  & 4.4       & 0.08    &  251    \\ [1ex]   
\hline  
\end{tabular}
\tablefoot{In a few cases the data allowed us to obtain only a lower limit to the  mass. $\alpha_{J2000}$ and $\delta_{J2000}$ are from 2MASS-6X-PSC 
catalog, $J, H, K$ are from $r$ = 10\farcs0 ap. phot. in the 2MASS-6X-PSC 
catalog. Note that $err_{JHK} = 1.00$ corresponds to  $err_{JHK}$=null in the 
2MASS-6X-PSC catalog.
\tablefoottext{a}{Estimated from Fig.~\ref{Mvage}, as these clusters lack NIR photometry. These mass estimates will not  be used in the following to preserve the homogeneity of the sample.}}
\vspace*{4mm}
\end{table}