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Table A.2.
Results of the fitting of the light curves of the XMM-Newton burst in different energy bands, with their 1σ uncertainties.
Energy band | Quiescent rate (×10−2 s−1) | Start time (h) | Rise time (h) | Peak time (h) | Peak rate (×10−2 s−1) | χ2/DoF |
---|---|---|---|---|---|---|
0.30 – 0.45 keV | 0.79 ± 0.13 | 3.9 ± 0.05 | 3.76 ± 0.14 | 7.66 ± 0.19 | 96.4 ± 2.2 | 70.3 / 58 |
0.45 – 0.60 keV | 0.36 ± 0.08 | 4.48 ± 0.04 | 2.96 ± 0.13 | 7.44 ± 0.17 | 67.7 ± 1.6 | 57.8 / 54 |
0.60 – 0.75 keV | 0.21 ± 0.09 | 4.95 ± 0.05 | 2.24 ± 0.15 | 7.19 ± 0.2 | 36.8 ± 1.1 | 44.5 / 40 |
0.75 – 0.90 keV | 0.23 ± 0.05 | 5.15 ± 0.06 | 1.92 ± 0.14 | 7.07 ± 0.2 | 18.6 ± 0.5 | 20.9 / 39 |
0.30 – 0.90 keV | 1.68 ± 0.16 | 4.3 ± 0.03 | 3.27 ± 0.08 | 7.56 ± 0.11 | 221.4 ± 3.1 | 61.9 / 58 |
Notes. The burst model used was a Gaussian rise between two plateau phases. The start and peak times are expressed with respect to the start of the observation.
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