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Table 4.

Best-fit continuum parameters for the individual orbits using a partially covered disk model.

Component Parameter [unit] Disk-only model
Orbit 1 Orbit 2 Orbit 3 Orbit 4 Orbit 5
TBabs NH [1022 cm−2] 0.15
cabs*pcfabs NH [1022 cm−2] 8 . 5 1.7 + 2.1 Mathematical equation: $ 8.5_{-1.7}^{+2.1} $ 63 22 + 50 Mathematical equation: $ 63_{-22}^{+50} $ 94 38 + 106 Mathematical equation: $ 94_{-38}^{+106\dagger} $ 101 65 + 99 Mathematical equation: $ 101_{-65}^{+99\dagger} $ 0
f 0 . 56 0.03 + 0.02 Mathematical equation: $ 0.56_{-0.03}^{+0.02} $ 0 . 34 0.03 + 0.02 Mathematical equation: $ 0.34_{-0.03}^{+0.02} $ 0 . 27 0.03 + 0.02 Mathematical equation: $ 0.27_{-0.03}^{+0.02} $ 0.16 ± 0.04 0
diskbb kTin [keV] 1.66 ± 0.03
norm 0.23 ± 0.02

FX(a) [10−11 erg s−1 cm−2] 2.19 2.17 2.33 2.65 3.13
LX(a) [10−4LEdd] 1.25 1.24 1.33 1.51 1.79

HR(b) / 2.18 1.43 1.37 1.36 1.33
Fit statistic Xtend 97/71 98/70 93/70 53/66 72/66
Fit statistic Resolve 1180/1345 1208/1346 975/1342 864/1341 1251/1350

Notes. ( † )parameter frozen or at the limit of its allowable interval.

(a)

1−10 keV flux and luminosity after removal of the ISM contribution (TBabs). The Eddington ratio is calculated according to the orbital parameters of MacDonald et al. (2014).

(b)

3−10/1−3 keV flux hardness ratio after removal of the ISM contribution.

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