\begin{table}%t1
\caption{Red-giant targets.}\label{runs}
%%\centering

\par
\begin{tabular}{lccccc}
\hline\hline
\noalign{\smallskip}
Run  & $T$ (d)&$\nzero$& $\nun$ & $\nde$& $\ntr$ \\
\hline
%LRc1 & 150 d&      & 1228   & 875   & 520\\
%LRa1 & 125 d& 1380 & 1271   &  498   & 219\\
%LRc1 & 150 d& 9938 & 1228   & 875   & 520\\
LRc01 & 142 d& 9938 & 3388   & 1399    & 710    \\
LRa01 & 128 d& 2826 & 1271   &  428    & 219    \\
\hline
total&  --  &12764 & 4659   & 1827    & 929    \\
\hline
\multicolumn{2}{l}{ratio (\%)} &  --   &100\% & 39\%  & 20\% \\
\hline
\end{tabular}
\tablefoot{Among $\nzero$ targets a priori identified as red giants in the input catalog of each field, $\nun$ light curves were available and analyzed in each run. Among these, $\nde$ targets show solar-like oscillation patterns for which we can derive precise values of $\dnumoy$ and $\numax$. Envelope parameters can be precisely determined for $\ntr$ targets.}
\end{table}