Table 2.
Best-fits of the XMM-Newton EPIC-pn plus NuSTAR data.
| Model | Γ | NH | Cf | EFeKα | R | σ | EW | C/d.o.f. | Cpn, 2 | Cpn, 3 | CFPMA/B, 1 | CFPMA/B, 2 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|
| (1022 cm−2) | (keV) | (eV) | (eV) | |||||||||
| PC1 | 1.65 ± 0.02 | 12.5 ± 1.7 | 0.23 ± 0.02 | 6.39 ± 0.03 | – | 102 ± 40 | 68 ± 3 | 2555/2422 | 1.03 ± 0.01 | 1.11 ± 0.02 | 1.24 ± 0.02 | 1.27 ± 0.02 |
| PC2 | 1.76 ± 0.02 | 12.1 ± 1.2 | 0.31 ± 0.03 | – | 0.38 ± 0.04 | – | – | 2529/2424 | 1.03 ± 0.01 | 1.11 ± 0.01 | 1.24 ± 0.02 | 1.27 ± 0.02 |
| Model | NH | Cf | Γ | rin | log ξ | R | a | C/d.o.f. | Cpn, 2 | Cpn, 3 | CFPMA/B, 1 | CFPMA/B, 2 |
| (1022 cm−2) | (ISCO) | |||||||||||
| RR1 | – | – | 1.47
|
1* | 4.28
|
0.74
|
> 0.85 | 2683/2422 | 1.03 ± 0.01 | 1.11 ± 0.01 | 1.24 ± 0.02 | 1.27 ± 0.02 |
| RR2 | 10.35 ± 2.10 | 0.20
|
1.59
|
1* | 3.56
|
0.41
|
0.99u | 2519/2420 | 1.03 ± 0.01 | 1.11 ± 0.01 | 1.24 ± 0.02 | 1.27 ± 0.02 |
Notes. Upper table: Col. I: Model name; Col. II: Photon index of the primary emission; Col. III: Column density of the partial absorber; Col. IV: Covering factor; Col. V: Energy of the emission line; Col. VI: direct-to-reflected continuum ratio; Col. VII: Width of the emission line; Col. VIII: Equivalent width of the emission line; Col. IX: Cash statistics over degrees of freedom. Lower table: Col. I: Model name; Col. II: Column density of the partial absorber; Col. III: Covering factor; Col. IV: Photon index of the primary emission; Col. V: Inner radius of the accretion disk; Col. VI: Ionization of the accretion disk; Col. VII: Reflection fraction parameter; Col. VIII: Spin of the BH; Col. IX: Cash statistics over degrees of freedom. Cols. X-XIII: Cross-normalization constants between XMM-Newton EPIC-pn and NuSTAR. Reported errors are at the 90% confidence level. In models RR1-RR2, the line energy and σ are fixed at 6.4 keV and 20 eV, respectively. Model PC1: constant × TBabs × zpcfabs(cutoffpl + line); Model PC2: TBabs(cutoffpl + pexmon + (1 + constant) × zTBabs(cutoffpl)); Model RR1: constant × TBabs(zgauss + relxill), with Rbr = 15, AFe = 1; Model RR2: constant × TBabs × zpcfabs(relxill + zgauss).
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