Table 2: Best-fit spectral parameters of the time-averaged pn spectrum in the 2-12 keV energy range with an absorbed (Galactic, $N_{\rm H}=6.8\times 10^{20}$ cm-2) power-law (PL) component plus a line profile: zgauss: Gaussian profile; and DISKLINE and LAOR: line profile emitted by a relativistic accretion disk for a non-rotating black hole (Fabian et al. 1989) and a maximally rotating black hole (Laor 1991), respectively. The line fluxes are expressed in 10-6 photons cm-2 s-1. We assume an emissivity index q equal to -2. (a): $R_{\rm in}=6$ $R_{\rm g}$ and $R_{\rm out}=1000$ $R_{\rm g}$. (b): $R_{\rm in}=1.235$ $R_{\rm g}$ and $R_{\rm out}=400$ $R_{\rm g}$.

Model
$\Gamma$ Line parameters $\chi^{2}$/d.o.f. F-test
    E (keV) $\sigma $ (keV) $\theta$ (deg) Flux EW (eV)    
PL $1.56\pm0.04$ - - - - - 634.0/621 -
PL + zgauss 1.57 $\pm$ 0.04 6.4 (f) 0.01 (f) - 2.2 $\pm$ 1.2 54 $\pm$ 29 624.5/620 99.78$\%$
PL + zgauss 1.57 $\pm$ 0.04 6.33 $\pm$ 0.05 <0.10 - 2.9 $\pm$ 1.4 $\rm 69^{+36}_{-31}$ 619.6/618 99.74$\%$
PL + DISKLINE(A) $1.58\pm0.04$ 6.40 $\pm$ 0.05 - <22 3.9 $\pm$ 1.7 107 $\pm$ 46 619.3/618 99.77$\%$
PL + LAOR(b) 1.58$\pm0.04$ $\rm 6.40^{+0.05}_{-0.10}$ - <22 4.4 $\pm$ 2.1 $\rm 119^{+59}_{-55}$ 621.7/618 99.30$\%$


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