\begin{table}%T1
	\caption{\label{table_simu_param}Input parameters used for the simulated spectra. }
\small%\centerline
{
\begin{tabular}{cccccc} 
\hline\hline
 & $\delta \nu_{02}$ ($\mu {\rm{Hz}}$) & $\nu_{\rm s}$ ($\mu {\rm{Hz}}$) & $\Gamma$ ($\mu {\rm{Hz}}$) & $H/N$ ($l=0$) & H Profile \\ \hline
1        & 8  & 2          & [1,5] & $>$30 & C\\
2        & 8  & 2          & [1,5] & $\simeq$$4$ & C \\
3        & 5  & 3.5        & [2,10] & $\simeq$$6$ & C\\
4        & 5  & 3.5        & [3,10] & 3$-$10 & G\\
5	 & 5  & 3.5        & [4,13] & 3$-$8 & G\\
6        & /  & 3.5        & [3,10] & 3$-$8 & G\\
\hline
\end{tabular}}
\smallskip
 The frequency separation $\delta \nu_{02}$ (see Eq.~(\ref{small_sep_grp})), the rotational splitting $\nu_{\rm s}$, the mode width~$\Gamma$ and the height-to-noise ratio $H/N$. Two kinds of mode height variation with frequency were tested: a constant height for all modes~(C) or a more realistic Gaussian profile (G).
\end{table}