\begin{table}%t3
\caption{\label{tab_param0A}Reference results for the parameters of the radial p modes. }
%\centerline
{\begin{tabular}{ l c c c c c c c c c }
\hline \hline
$\ell$ \T \B & $\nu_{n,\ell}$ ($\mu$Hz) & agr.($\nu_{n,\ell}$) & $H_{0,n}$ (ppm$^2/\mu$Hz) & agr.($H_{0,n}$) & $\Gamma_n$ ($\mu$Hz) & agr.($\Gamma_n$) & $a_n$ (ppm) & agr.($a_n$) & $H_{\ell,n}/B(\nu_{n,\ell})$ \\
\hline
0 \T \B & $ 799.70\pm 0.27$ & $\bullet$ & $2.55^{\rm +0.80}_{-0.61}$ & $\bullet$ & $1.58^{\rm +0.42}_{-0.33}$ & $\bullet$ & $3.55^{\rm +0.67}_{-0.56}$ & $\bullet$  & 2.23 \\
0 \T \B& $ 855.30\pm 0.73$ & $\bullet$ & $2.10^{\rm +0.59}_{-0.46}$ & $\bullet$ & $2.97^{\rm +0.72}_{-0.58}$ & $\bullet$ & $4.42^{\rm +0.77}_{-0.65}$ & $\bullet$  & 1.94 \\
0 \T \B& $ 909.92\pm 0.26$ & $\bullet$ & $3.13^{\rm +0.82}_{-0.65}$ & $\bullet$ & $2.00^{\rm +0.43}_{-0.35}$ & $\bullet$ & $4.44^{\rm +0.70}_{-0.60}$ & $\bullet$  & 3.03 \\
0 \T & $ 965.16\pm 0.36$ & $\bullet$ & $4.05^{\rm +0.96}_{-0.78}$ & $\bullet$ & $2.37^{\rm +0.43}_{-0.37}$ & $\bullet$ & $5.49^{\rm +0.83}_{-0.72}$ & $\bullet$  & 4.09 \\
0 \T \B& $1021.81\pm 0.28$ & $\bullet$ & $4.56^{\rm +1.15}_{-0.92}$ & $\bullet$ & $2.03^{\rm +0.41}_{-0.34}$ & $\bullet$ & $5.40^{\rm +0.80}_{-0.70}$ & $\bullet$  & 4.78 \\
0 \T \B& $1078.97\pm 0.33$ & $\bullet$ & $4.77^{\rm +1.10}_{-0.90}$ & $\bullet$ & $2.08^{\rm +0.35}_{-0.30}$ & $\bullet$ & $5.58^{\rm +0.80}_{-0.70}$ & $\bullet$  & 5.18 \\
0 \T \B& $1135.32\pm 0.34$ & $\bullet$ & $3.49^{\rm +0.83}_{-0.67}$ & $\bullet$ & $2.37^{\rm +0.44}_{-0.37}$ & $\bullet$ & $5.09^{\rm +0.86}_{-0.73}$ & $\bullet$  & 3.90 \\
0 \T \B& $1192.12\pm 0.45$ & $\bullet$ & $2.29^{\rm +0.67}_{-0.52}$ & $\bullet$ & $2.51^{\rm +0.68}_{-0.53}$ & $1.8~\sigma$ & $4.25^{\rm +0.80}_{-0.67}$ & $\bullet$  & 2.63 \\
0 \T \B& $1250.12\pm 0.89$ & $\bullet$ & $1.15^{\rm +0.32}_{-0.25}$ & $\bullet$ & $3.90^{\rm +1.00}_{-0.80}$ & $\bullet$ & $3.76^{\rm +4.04}_{-1.95}$ & $\bullet$  & 1.36 \\
\hline
\end{tabular}}
\tablefoot{The heights given here are those of the $\ell=0$ modes (the heights of non-radial modes are computed using height ratios, 
see Sect.~\ref{sect_method}). The agreement (agr.) between the teams is given for each fitted parameter. Filled circles indicate that at least four of the five teams agreed on the value within 1 $\sigma$. 
$X~\sigma$ indicates that more than one team disagrees with the value, and that the five teams agree within $X~\sigma$ ($X>1$).}\vspace*{3.2mm}
\end{table}