\begin{table}%t3
%\centering
\par
\caption{Results of separate fits to the $^{12}$C-line at 4.4 MeV and the $^{16}$O-line
line at 6.1 MeV assuming a thick-target interaction model and three different
energetic particle angular distributions around the flare axis. 
Rates and  fluences are expressed as in table I. Error bars on count
rates encompass the individual 1-sigma uncertainties of the different fits; a
10\% uncertainty has been quadratically added to the error bars of line
fluences.\label{table3}} 
\begin{tabular}  {clcccc} \hline \hline
& phase  & B & C & B-C & A-C  \\
\hline
$^{12}$C$^{\star}$ & $\alpha$/p & 0.19 & 0.04 & 0.10 & 0.09  \\
\par
& $\Delta \Theta$ & 25$^{\circ}$ & 40$^{\circ}$ & 35$^{\circ}$  &
30$^{\circ}$   
 \\
 & rate & $\rm 2.03^{+0.15}_{-0.17}$ &  $\rm 0.68^{+0.09}_{-0.06}$ &
 $\rm 1.09^{+0.09}_{-0.07}$ & $\rm 1.02^{+0.10}_{-0.05}$   
 \\
 & fluence & $\rm 76^{+9}_{-10}$  &  $\rm 58^{+9}_{-8}$ &  $\rm 127^{+16}_{-15}$ &
 $\rm 141^{+20}_{-16}$  
 \\
$^{16}$O$^{\star}$ & $\alpha$/p &  0.20 &  0.02 & 0.08 & 0.11   \\
&  $\Delta \Theta$ & 60$^{\circ}$ & 40$^{\circ}$ & 55$^{\circ}$ &
70$^{\circ}$   
   \\
 & rate & $\rm 1.62^{+0.12}_{-0.09} $  & $\rm 0.40^{+0.06}_{-0.03}$  &
 $\rm 0.77^{+0.06}_{-0.04}$ &  $\rm 0.74^{+0.06}_{-0.03}$    
 \\
 & fluence & $\rm 77^{+10}_{-9}$ &  $\rm 44^{+8}_{-6}$  &  $\rm 121^{+15}_{-14}$ &
 $\rm 130^{+17}_{-14}$    
 \\ 
\\
 $^{24}$Mg$^{\star}$ & fluence & $\rm 45^{+15}_{-14}$ &  $\rm 28^{+18}_{-18}$  & 
 $\rm 75^{+24}_{-24}$ & $\rm 74^{+28}_{-24}$   
\\
$^{20}$Ne$^{\star}$ & fluence & $\rm 34^{+13}_{-11}$ &  $\rm 30^{+14}_{-13}$  & 
 $\rm 63^{+24}_{-19}$ & $\rm 71^{+28}_{-20}$    
\\
$^{28}$Si$^{\star}$ & fluence & $\rm 21^{+10}_{-9}$ &  $\rm 20^{+11}_{-11}$  & 
 $\rm 43^{+17}_{-14}$ & $\rm 50^{+19}_{-16}$     
\\
 \hline
\end{tabular} 
\end{table}