\begin{table}%t4
\par
\caption{\label{nuc_numax}Scaling with $\numax$.}
%%\centering

\par
\begin{tabular}{lllll}
\hline\hline
\noalign{\smallskip}
$f(\numax)$       & $\dnumoy$            & $\Teff$         & $\Rsis$       &  $\nuc$        \\
exponent          & $\beta$              & $\gamma$        & $\delta$      &  $\alpha$      \\
\hline
    giants        & 0.75 $\pm$ 0.01        &\ \ 0.04 $\pm$ 0.01& $-$0.48 $\pm$ 0.01& 1.00 $\pm$ 0.02 \\
subgiants$^{(1)}$& 0.71 $\pm$ 0.02        & $-$0.02 $\pm$ 0.02& $-$0.58 $\pm$ 0.06& 0.83 $\pm$ 0.10 \\
                  & 0.77 $\pm$ 0.01\tablefootmark{\star}&                 &               &   0.97 $\pm$ 0.10 \\
dwarfs$^{(2)}$    & 0.76 $\pm$ 0.02        & $-$0.18 $\pm$ 0.02& $-$0.64 $\pm$ 0.03& 0.97 $\pm$ 0.04 \\
                  & 0.77 $\pm$ 0.01\tablefootmark{\star}&                 &               &   0.99 $\pm$ 0.04 \\
\hline
\end{tabular}
\tablefoot{\tablefoottext{\star}{Value from \cite{2009MNRAS.400L..80S}.}} \vspace{-5mm}
\tablebib{(1) \cite{2009ASPC..404..307K}; \cite{Deheuvels2010};
(2) \cite{2009ASPC..404..307K}; \cite{2008AetA...488..635M}; \cite{2009AetA...494..237T}; \cite{Mathur2010}; \cite{Gaulme2010}; J. Ballot, private communication.}
\end{table}