\begin{table}%t2
%\centering
\par
\caption{\label{Photometry_2M0310}Resolved component properties of 2MASS~0310+1648~AB.}
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\par
\begin{tabular}{l c c c c}     
\hline\hline
\noalign{\medskip}
Property & Flux ratio  &$\Delta$ mag & 2M0310+1648~A & 2M0310+1648~B \\
\hline
\noalign{\smallskip}
F108N   &  0.892~$\pm$~0.008  & 0.12~$\pm$~0.02   & 17.42~$\pm$~0.07 & 17.54~$\pm$~0.08\\ 
F113N  &  0.891~$\pm$~0.008  & 0.12~$\pm$~0.02 &17.51~$\pm$~0.06 & 17.63~$\pm$~0.05 \\[0.5ex]
\emph{J}~\tablefootmark{*} & 0.908~$\pm$~0.020  & 0.10~$\pm$~0.06 & 16.73~$\pm$~0.11  & 16.83~$\pm$~0.13 \\ 
\emph{H}  & 0.947~$\pm$~0.012 & 0.059~$\pm$~0.013 & 15.66~$\pm$~0.08  & 15.71~$\pm$~0.08 \\ 
\emph{K$_{\rm S}$} & 1.008~$\pm$~0.005 & $-$0.009~$\pm$~0.005  &15.07~$\pm$~0.07  & 15.06~$\pm$~0.07 \\ [0.5ex]
\emph{J~--~H}  &  &  &1.07~$\pm$~0.14  &  1.12~$\pm$~0.15\\
\emph{H~--~K$_{\rm S}$}  &  & &0.59~$\pm$~0.11 & 0.65~$\pm$~0.11 \\
\emph{J~--~K$_{\rm S}$}  & & &  1.66~$\pm$~0.13& 1.77~$\pm$~0.15\\[1.0ex]
\hline
\end{tabular}
\tablefoot{\tablefoottext{*}{The resolved \emph{J}-band magnitudes are based on an estimated flux ratio due to the lack of observations (see description in the text).}}\vspace*{2.4mm}
\end{table}