Table 3: Results of separate fits to the 12C-line at 4.4 MeV and the 16O-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.
  phase B C B-C A-C
12C$^{\star}$ $\alpha $/p 0.19 0.04 0.10 0.09
  $\Delta \Theta $ 25$^{\circ }$ 40$^{\circ }$ 35$^{\circ }$ 30$^{\circ }$
  rate $\rm 2.03^{+0.15}_{-0.17}$ $\rm0.68^{+0.09}_{-0.06}$ $\rm 1.09^{+0.09}_{-0.07}$ $\rm 1.02^{+0.10}_{-0.05}$
  fluence $\rm 76^{+9}_{-10}$ $\rm 58^{+9}_{-8}$ $\rm 127^{+16}_{-15}$ $\rm 141^{+20}_{-16}$
16O$^{\star}$ $\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} $ $\rm0.40^{+0.06}_{-0.03}$ $\rm0.77^{+0.06}_{-0.04}$ $\rm0.74^{+0.06}_{-0.03}$
  fluence $\rm 77^{+10}_{-9}$ $\rm 44^{+8}_{-6}$ $\rm 121^{+15}_{-14}$ $\rm 130^{+17}_{-14}$
24Mg$^{\star}$ fluence $\rm 45^{+15}_{-14}$ $\rm 28^{+18}_{-18}$ $\rm 75^{+24}_{-24}$ $\rm 74^{+28}_{-24}$
20Ne$^{\star}$ fluence $\rm 34^{+13}_{-11}$ $\rm 30^{+14}_{-13}$ $\rm 63^{+24}_{-19}$ $\rm 71^{+28}_{-20}$
28Si$^{\star}$ fluence $\rm 21^{+10}_{-9}$ $\rm 20^{+11}_{-11}$ $\rm 43^{+17}_{-14}$ $\rm 50^{+19}_{-16}$


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