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Table 1:

Spectral fit to the Suzaku XIS time-averaged spectrum.

Data
$\Gamma$ $N_{\rm H}$ $N_{\rm H,W}$ $\xi$ $E_{\rm FeK}$ $\sigma$ $I_{\rm FeK}$ $\chi^2$/d.o.f.
    cm-2 cm-2 ergs-1cm keV keV phs-1cm-2  
Total $\rm 1.40^{+0.05}_{-0.04}$ $5.4^{+2.8}_{-3.0}\times 10^{20}$ $2.1^{+0.3}_{-0.2}\times 10^{22}$ $\rm 34^{+5}_{-4}$ $\rm 6.36^{+0.04}_{-0.04}$ $\rm0.09^{+0.05}_{-0.05}$ $6.4^{+2.2}_{-1.8}\times 10^{-6}$ 406.0/407

Notes. The spectrum was obtained by combining the XIS0 and XIS3 data. The model consists of a power law with a Gaussian for the Fe K$\alpha$ line, modified by warm and cold absorption. The cold absorption column is denoted by $N_{\rm H}$, which is in excess of the Galactic column of $1.85\times 10^{20}$ cm-2. Tim Kallman's XSTAR grid tables (``grid 25'') with the turbulent velocity of 200 km s-1 is adopted for the warm absorber modelling.


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