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Table A.1.

Parameters from fitting the XMM-Newton, NuSTAR and Swift spectra with a model TBabs×(partcov×TBabs)(bbodyrad + mkcflow + gaussian). Unabsorbed luminosities are calculated in the 0.001-50 keV energy band. Luminosity and are determined assuming a distance of 914 pc. Elemental abundances are quoted in units of abundances from Wilms et al. (2000). Statistical errors are calculated at the 90% confidence level.

Obs1 Obs2 Obs3+Nu1 Obs4 Obs5 Obs6 Nu2+Swift Nu3+Swift Obs7
Soft Count rate 1 0.108 0.040 0.0064 0.0032 0.027 0.0088 0.003 0.006 0.002
Hard Count rate2 0.039 0.076 0.155 0.241 0.148 0.401 0.67/0.015 0.21/0.018 0.35
NH (F.C.) [1022 cm−2] 3 0.05±0.01 0.14±0.07 0.7 0.4 + 0.7 Mathematical equation: $ _{-0.4}^{+0.7} $ 0.07±0.03 0.12±0.01 0.11±0.01 19±10 43±15 0.07 0.06 + 0.09 Mathematical equation: $ _{-0.06}^{+0.09} $
NH (P.C.) [1022 cm−2] 4 68±3 46±3 29±2 53±3 29±1 40±1 65 16 + 40 Mathematical equation: $ _{-16}^{+40} $ 157 45 + 83 Mathematical equation: $ _{-45}^{+83} $ 45±1
Covering fraction 0.997±0.001 0.993±0.002 0.994 0.004 + 0.002 Mathematical equation: $ _{-0.004}^{+0.002} $ 0.999±0.001 0.993±0.002 0.998±0.001 0.6±0.2 0.7±0.1 0.999 (fixed)
kTbb[keV] 0.034±0.002 0.037±0.005 0.04±0.02 0.041±0.015 0.029±0.001 0.04±0.01 ... ... ...
Rbb[km] 2084±500 1000±20 1200±200 < 500 3200±200 450±200 ... ... ...
kTmax (keV) 12±3 28 2 + 3 Mathematical equation: $ _{-2}^{+3} $ 24 5 + 8 Mathematical equation: $ ^{+8}_{-5} $ 33±3 52±5 48±4 54 5 + 7 Mathematical equation: $ _{-5}^{+7} $ 35 8 + 10 Mathematical equation: $ _{-8}^{+10} $ 40±5
Z/Z 1.5±0.5 3.1±0.8 1.9±0.5 1.7±0.2 4±0.4 2.8±0.5 1.0±0.2 1.0±0.4 1.0±0.1
thin [10−9 M yr−1] 0.22±0.07 0.11±0.05 0.21±0.06 0.4±0.1 0.17±0.03 0.38±0.02 1.2±0.1 1.2±0.5 0.42±0.01
χ2/d.o.f 210/226 87/84 211/196 487/455 280/197 484/464 574/561 203/211 779/712
Log [Lbb] 35.9±0.7 35.5±0.7 35.9±0.8 35.4±1.2 36±1 34.8±1.1 ... ... ...
Log [Lcf] 32.74±0.03 32.92±0.03 33.12∼0.02 33.50±0.03 33.12±0.03 33.65±0.03 34.20±0.02 34.02±0.02 33.61±0.02

Notes. (1)Count rate in the 0.3-1.0 keV energy range. In the case of XMM-Newton we list the pn count rate. In this energy range we also list the Swift/XRT count rate in the case of NuSTAR+Swift spectra. (2)pn camera count rate in the 1-10 keV energy range in the case of XMM-Newton. Swift count rate in the 1-10 keV energy range while NuSTAR count rate were computed in the 3-50 keV energy range. (3)Absorption column of the full covering absorber model, TBabs. (4)Absorption column of the partial covering absorber model, partcov×TBabs.

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