\begin{table}%t3
%\centering
\par
\caption{\label{Halpha} Free fitting parameters for the H$_{\alpha}$~line. The wavelength 
difference
$\Delta\lambda$ between the narrow component and the broad component is also given.
The amplitude of the narrow component is fitted manually and so no error estimate is
given for this value. Since the peak of the narrow line was not included in the fitting process,
no error computation of the central wavelength was carried out. We estimate the error
to be similar to the values found for the other Balmer lines. Especially the value for the
narrow component seems to be quite accurate compared to the rest wavelength of 6562.817~\AA{} 
of the line \citep{Moore}.}
\begin{tabular}{cccccccc}
\hline\hline
sp & $A_{\rm n}$ & \multicolumn{1}{c}{$A_{\rm b}$} &${\rm \sigma_{n}}$ &${\rm \sigma_{b}}$ & ${\rm \lambda_{n}}$ & ${\rm \lambda_{b}}$ & ${\rm \Delta\lambda}$ \\  
  & [ $10^{3}$ electrons]& \multicolumn{1}{c}{[$10^{3}$ electrons]} & [\AA]& [\AA]& [\AA]&[\AA]&[\AA]\\
\hline
1&2150 &1232 $\pm$ 2& 0.40 $\pm$ 0.04 & 1.91 $\pm$ 0.05& 6562.80 & 6562.81& 0.01\\
2&1950 & 807$\pm$  1&0.41 $\pm$ 0.03 & 1.78 $\pm$ 0.01&6562.78 & 6563.30 & 0.52\\
3&1150 & 419 $\pm$ 1& 0.40 $\pm$ 0.04& 1.68 $\pm$ 0.08& 6562.79 & 6563.65& 0.86\\ 
4&350 & 88  $\pm$  0.5& 0.39 $\pm$ 0.04&1.59 $\pm$ 0.15&6562.79& 6563.55& 0.76\\
5&330 & 46 $\pm$   0.4& 0.36 $\pm$ 0.03&1.16 $\pm$ 0.16&6562.79 & 6563.28& 0.49\\
6&310 & 31  $\pm$  0.4& 0.35 $\pm$ 0.04&1.80 & 6562.79&6562.85& 0.06\\
7&510 & 130 $\pm$  0.7&0.38 $\pm$ 0.04&1.62 $\pm$ 0.16&6562.82&6562.30& $-$0.52\\
8&810 & 319 $\pm$  0.9& 0.38 $\pm$ 0.04& 1.76 $\pm$ 0.02& 6562.82 & 6562.62 & $-$0.20\\
\hline
\end{tabular}
\end{table}