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Table 1.

Best-fit continuum parameters with empirical models. Both models also include the line components described in Table 2, and the statistical fit value refers to the final model with all line components.

TBabs diskbb thcomp constant
Model NH kTin Norm Rin(a) Γ Cfrac kTe Crsl(b) F1 − 10 L1 − 10(c) Fit statistic
[1022 [erg s−1 10−4 C-stat
cm−2] [keV] [km] [keV] cm−2] [L/LEdd] /d.o.f.

Pure 0.15 1.77 0.14 0.41 / / / 1 . 0 0.04 + 0.03 Mathematical equation: $ 1.0_{-0.04}^{+0.03} $ 2.55 ⋅ 10−11 1.45 3212/3698
disk ±0.01 ±0.03 ±0.01 ±0.01

Compt. 0.16 1 . 65 0.12 + 0.11 Mathematical equation: $ 1.65_{-0.12}^{+0.11} $ 0 . 18 0.04 + 0.05 Mathematical equation: $ 0.18_{-0.04}^{+0.05} $ 0 . 47 0.05 + 0.06 Mathematical equation: $ 0.47_{-0.05}^{+0.06} $ 3 . 5 1.5 + 0.0 Mathematical equation: $ 3.5_{-1.5}^{+0.0}\dagger $ 0 . 57 0.5 + 0.16 Mathematical equation: $ 0.57_{-0.5}^{+0.16} $ 100 1 . 0 0.03 + 0.04 Mathematical equation: $ 1.0_{-0.03}^{+0.04} $ 2.55 ⋅ 10−11 1.45 3207/3696
disk ±0.01

Notes. The energy bands used for the flux and luminosity calculations are given in keV. † Parameters unconstrained within the allowed parameter space (2−3.5). ‡ Frozen parameter. (a) Computed from diskbb normalization assuming a distance of 6.2 kpc and an inclination of 72° (MacDonald et al. 2014). (b) Due to the broader energy band of Xtend and the potential uncertainty in the Ls events in Resolve, we froze the Xtend constant factor to 1 and allowed that of Resolve to vary freely. (c) Computed using the orbital parameters of MacDonald et al. (2014) (see Sect. 1).

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