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Table 3.

Best-fitting model parameters of the fits to the NuSTAR and NuSTAR+IXPE data.

Parameter
diskbb
kTin (keV) 0 . 93 0.03 + 0.01 $ 0.93^{+0.01}_{-0.03} $
R in cos i $ R_{\mathrm{in}} \sqrt{\cos i} $ (km) 13 . 1 0.4 + 0.2 $ 13.1^{+0.2}_{-0.4} $

bbodyrad
kTbb (keV) 1 . 38 0.05 + 0.02 $ 1.38^{+0.02}_{-0.05} $
Rbb (km) 7 . 7 0.5 + 0.2 $ 7.7^{+0.2}_{-0.5} $

thcomp
τ 8 . 1 0.2 + 0.3 $ 8.1^{+0.3}_{-0.2} $
kTe (keV) 2 . 92 0.04 + 0.03 $ 2.92^{+0.03}_{-0.04} $

relxillns
qem 2.26 ± 0.09
a [0.2]
incl (deg) 25 . 1 1.5 + 1.3 $ 25.1^{+1.3}_{-1.5} $
Rin (units of RISCO) 1 . 6 0.5 + 0.3 $ 1.6^{+0.3}_{-0.5} $
kTbb (keV) [=kTbb, bbodyrad]
log(ξ/erg cm s−1) 2.88 ± 0.07
AFe 5 . 0 0.3 + 1.1 $ 5.0^{+1.1}_{-0.3} $
log ne [18]
Nr (10−3) 1 . 37 0.08 + 0.09 $ 1.37^{+0.09}_{-0.08} $

Cross-calibration
CDU1 − FPMA 0 . 881 0.007 + 0.005 $ 0.881^{+0.005}_{-0.007} $
CDU2 − FPMA 0 . 880 0.005 + 0.006 $ 0.880^{+0.006}_{-0.005} $
CDU3 − FPMA 0 . 861 0.006 + 0.005 $ 0.861^{+0.005}_{-0.006} $
CFPMB − FPMA 0.987 ± 0.001
CXTI − FPMA 0.929 ± 0.001
Gain shift
αDU1 1 . 013 0.003 + 0.002 $ 1.013^{+0.002}_{-0.003} $
βDU1 (eV) 53 10 + 12 $ -53^{+12}_{-10} $
αDU2 1 . 008 0.003 + 0.002 $ 1.008^{+0.002}_{-0.003} $
βDU2 (eV) 30 11 + 12 $ -30^{+12}_{-11} $
αDU3 1 . 007 0.003 + 0.002 $ 1.007^{+0.002}_{-0.003} $
βDU3 (eV) 33 11 + 12 $ -33^{+12}_{-11} $
αXTI 1.032 ± 0.001
βXTI (eV) 65 3 + 2 $ -65^{+2}_{-3} $

χ2/d.o.f. 1031/962

Photon flux ratios (a)
2–8 keV
Fdiskbb/Ftot 0.44
Fbbodyrad/Ftot 0.47
Frelxillns/Ftot 0.09
2–4 keV
Fdiskbb/Ftot 0.58
Fbbodyrad/Ftot 0.35
Frelxillns/Ftot 0.07
4–8 keV
Fdiskbb/Ftot 0.19
Fbbodyrad/Ftot 0.69
Frelxillns/Ftot 0.12
Energy flux (2–8 keV)
Ftot (erg s−1 cm−2) 5.1 × 10−9

Notes. Uncertainties are given at the 68% confidence level for one parameter of interest. Parameters in square brackets were kept frozen during the fit. The normalizations of diskbb and bbodyrad are computed assuming a source distance of 7.7 kpc.

(a)

The photon fluxes are in units of photon cm−2 s−1.

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