\begin{table}%T12
\par
	\caption{\label{table_HD49933_posterior_individual_Amplitude_M2A}Energy posterior estimates for HD~49933, model 
	$M^2_{\rm A}$. $n$ is given for the $l=0$~modes.}
 \small%\centering
\par
\begin{tabular}{c|c c c}
	\hline\hline
& \multicolumn{3}{c}{Model $M^2_{\rm A}$ (ppm)}\\
$n$
	& $ median $
	& $ 1 \sigma_+/1 \sigma_- $
	& $ 2 \sigma_+/2 \sigma_- $\\ \hline
	     13 & $3.16$ & 0.51 / 0.48 & 1.01 / 0.94\\
             14 & $2.29$ & 0.39 / 0.36 & 0.79 / 0.73\\
             15 & $2.83$ & 0.30 / 0.30 & 0.63 / 0.59\\
             16 & $2.98$ & 0.40 / 0.41 & 0.79 / 0.80\\
             17 & $3.63$ & 0.34 / 0.34 & 0.68 / 0.69\\
             18 & $3.83$ & 0.33 / 0.33 & 0.67 / 0.66\\
             19 & $4.48$ & 0.34 / 0.34 & 0.68 / 0.68\\
             20 & $3.55$ & 0.31 / 0.30 & 0.63 / 0.62\\
             21 & $3.18$ & 0.31 / 0.31 & 0.62 / 0.63\\
             22 & $3.18$ & 0.30 / 0.30 & 0.62 / 0.58\\
             23 & $2.81$ & 0.29 / 0.29 & 0.59 / 0.59\\
             24 & $2.53$ & 0.30 / 0.30 & 0.61 / 0.60\\
             25 & $2.65$ & 0.30 / 0.29 & 0.60 / 0.59\\
             26 & $2.32$ & 0.28 / 0.28 & 0.57 / 0.56\\
             27 & $1.79$ & 0.34 / 0.32 & 0.69 / 0.62\\\hline
\end{tabular}
\end{table}