Table 2
Properties of the type I X-ray bursts observed by XMM-Newton.
| No. | Start time (MJD) | trec (s) | Fpers | Fpeak | ℱ | τ (s) | α |
|
|
|||||||
| I | 57 103.26624 | ... | 0.99(2) | 17(2) | 38(3) | 22.7 ± 3.4 | |
| II | 57 103.41516 | 12866 | 0.955(7) | 38(7) | 40(6) | 10.5 ± 2.6 | 86 ± 16 |
| III | 57 103.56912 | 13303 | 0.924(6) | 18(2) | 31(3) | 16.5 ± 3.0 | 111 ± 12 |
| IV | 57 103.67557 | 9197 | 0.91(1) | 21(3) | 42(5) | 20.4 ± 3.8 | 56 ± 6 |
| V | 57 103.84017 | 14221 | 0.868(4) | 29(4) | 44(5) | 18.8 ± 2.8 | 79 ± 9 |
| VI | 57 103.96830 | 11071 | 0.929(5) | 24(3) | 38(4) | 16.2 ± 2.8 | 76 ± 11 |
| VII | 57 104.10384 | 11710 | 0.922(4) | 22(3) | 37(4) | 17.1 ± 3.1 | 82 ± 12 |
Notes. The 0.5−10 keV persistent flux Fpers and the burst peak flux Fpeak are unabsorbed and expressed in units of 10-9 erg cm-2 s-1. The bolometric fluence ℱ is unabsorbed and given in units of 10-8 erg cm-2. The burst decay timescale was evaluated as τ = ℱ /Fpers, the parameter α as cbolFperstrec/ ℱ with cbol = 2.8 ± 0.3.
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