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 Ṁ 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![]() |
0.07±0.03 | 0.12±0.01 | 0.11±0.01 | 19±10 | 43±15 | 0.07![]() |
| NH (P.C.) [1022 cm−2] 4 | 68±3 | 46±3 | 29±2 | 53±3 | 29±1 | 40±1 | 65![]() |
157![]() |
45±1 |
| Covering fraction | 0.997±0.001 | 0.993±0.002 | 0.994![]() |
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![]() |
24![]() |
33±3 | 52±5 | 48±4 | 54![]() |
35![]() |
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 |
| Ṁthin [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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