Table 2.
Results of the best-fit continuum modelling.
| Parameter | Archive-only | All-times | 0921360101 | 0921360201 |
|---|---|---|---|---|
| Model: hot*(bb+comt) | ||||
| LX,bb (1039 erg/s) | 0.35 ± 0.04 | ![]() |
1.0 ± 0.2 | < 0.16 |
| LX,comt (1039 erg/s) | 4.9 ± 0.3 | ![]() |
4.0 ± 0.3 | 5.9 ± 0.6 |
| kTbb (keV) | ![]() |
![]() |
0.14 ± 0.01 | 0.12 ± 0.01 |
| kTin, comt (keV) | 0.1(b) | 0.1(b) | 0.14(b) | 0.12(b) |
| kTe, comt (keV) | 2.44
|
2.68
|
![]() |
![]() |
| τcomt | 5.8 ± 0.3 | 5.4 ± 0.2 | ![]() |
![]() |
| C-stat/d.o.f. | 850/714 | 903/756 | 942/769 | 1002/846 |
Notes. The X-ray luminosities of the plasma emission components are computed in the 0.3 − 10 keV energy range, assuming a distance of 4.5 Mpc. (a)indicates that the parameter is pegged at the lower boundary of the allowed range. (b)indicates coupled parameters: for each dataset, kTbb = kTin, comt. The hydrogen column density, NH, of the interstellar medium is fixed at 5.4 × 1020 cm−2, as obtained for the time-averaged data.
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