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Table 2.

Parameters of the flux curve fitting.

Lmax(a) Tmax Tdec Tris Ltot(a)
(1034 erg s−1) (ks) (s) (s) (1038 erg)
1 22.8 ± 3.1 62.9 ± 0.1 646 ± 205 1377 ± 195 30.5
2 12.7 ± 3.4 64.6 ± 0.1 527 ± 187 468 ± 273 9.6
3 19.2 ± 5.3 67.9 ± 0.2 303 ± 249 755 ± 201 13.0
4 11.1 ± 2.4 69.3 ± 0.2 778 ± 210 869 ± 413 13.5
5 13.5 ± 2.7 73.0 ± 0.2 1857 ± 1019 598 ± 176 29.1
6(b) 21.6 ± 5.3 74.74 ± 0.04 200 ± 114 7.5
7 4.8 ± 1.4 77.6 ± 0.6 7216 ± 2010 1946 ± 1279 38.4
8(b) 39.3 ± 0.5 80.71 ± 0.02 221 ± 37 15.4
9 17.5 ± 6.3 81.4 ± 0.3 326 ± 199 317 ± 799 8.4
10 8.4 ± 1.7 94.0 ± 0.3 1883 ± 526 863 ± 561 19.4

Notes. Parameters of the best-fitted model for the active part of the XMM-Newton EXTraS flux curve. Each row reports the parameters of a different FRED component, the maximum luminosity, the time of the maximum (after T0+61.5 ks), the exponential decay time, the linear rising time, and the integral of the model component, respectively. This fit is statistically acceptable, with χ2 = 146.9, 111 dof, and nhp = 1.3×10−2.

(a)

Assuming a 10 kpc distance.

(b)

Here, we fitted a Gaussian model. We report the 2–12 keV maximum luminosity, the time of the maximum and the sigma of the Gaussian, respectively.

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