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Table 2:

Fit results.
X-rays (0.2-10 keV)
Instrument Model $\Gamma$ or $\Gamma_1$ Additional parameters $F_{\rm 2-10~keV}$ $\chi^2_{\rm r}$/d.o.f.
XMM/EPIC wabs*zpo $1.42 \pm 0.01$     $0.56 \pm 0.01$ 1.08/977
Swift/XRT (OBS. 1) wabs*zpo $1.44\pm 0.07$     $1.2 \pm 0.1$ 1.24/29
Swift/XRT (OBS. 2) wabs*zpo $1.38 \pm 0.09$     $\rm 1.04^{+0.06}_{-0.09}$ 1.63/15
  wabs*zwabs*zpo $\rm 1.55^{+0.17}_{-0.16}$ $N_z=1.0^{\rm +1.1}_{-0.8}$ 1022 cm-2   $\rm0.97^{+0.5}_{-0.08}$ 1.42/14
  wabs*bknpo $\rm0.98_{-0.41}^{+0.29}$ $E_{\rm break}= 1.9_{\rm -0.6}^{+1.5}$ keV $\Gamma_2=1.86_{-0.31}^{+1.19}$ $0.8 \pm 0.1$ 0.98/13

Hard X-rays (20-100 keV)
Instrument Model $\Gamma$     $F_{\rm 20-100~keV}$ $\chi^2_{\rm r}$/d.o.f.

INTEGRAL/ISGRI
zpo 1.5-0.8+0.9     $2.1 \pm 0.2$ 0.51/3
Swift/BAT zpo $1.5\pm 0.4$     $4.8 \pm 0.5$ 0.48/2

Joint fit (0.2-100 keV)
Instrument Model $\Gamma$ or $\Gamma_1$ Additional parameters $F_{\rm 2-100~keV}$ $\chi^2_{\rm r}$/d.o.f.

EPIC+ISGRI
wabs*zpo $1.42 \pm 0.01$     $\rm 3.13^{+0.05}_{-0.04}$ 1.08/980
XRT (OBS. 1) + BAT wabs*zpo $1.44\pm 0.07$     $\rm 6.4^{+0.9}_{-0.8}$ 1.2/32
XRT (OBS. 2) + BAT wabs*bknpo $\rm0.9^{+0.3}_{-0.4} $ $E_{\rm break}=1.6^{\rm +0.9}_{-0.4}$ keV $\Gamma_2=1.7^{+0.3}_{-0.2}$ $3 \pm 1$ 0.92/16
Models and parameters for single instruments and joint fit. Applied models are: a power-law in the source rest frame (zpo), a power-law with an absorption component in the object rest frame (zwabs*zpo) and a broken power-law (bknpo). All models include Galactic absorption (wabs) with column density $N_{\rm H}=1.63\times 10^{20}$ cm-2 (Kalberla et al. 2005). Flux is given in units of 10-11 erg cm-2 s-1.

Source LaTeX | All tables | In the text

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