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Table 4:

The XIS spectra from the second and fifth intervals.

Interval
$\Gamma$ log $\xi$a $N_{\rm W}^{{b}}$  
2 $1.75\pm 0.07$ $1.6\pm 0.5$ $1.1\pm 0.2$  
5 $1.23\pm 0.07$ $1.0\pm 0.1$ $2.4\pm 0.3$  
$\Gamma$ - $1.56\pm 0.09$ $1.47\pm 0.09$  
log $\xi$a $1.4\pm 0.3$ - $1.1\pm 0.2$  
$N_{\rm W}^{{b}}$ $2.2\pm 0.5$ $2.3\pm 0.3$ -  
$\chi^2$/d.o.f. 281.8/309 293.2/309 283.4/309  
Interval $\Gamma$ log $\xi$a $N_{\rm W}$b $\chi^2$/d.o.f.
2 $1.65\pm 0.08$ $1.5\pm 0.2$ $2.2\pm 0.4$ 275.0/308
5 $1.34\pm 0.10$ $1.0\pm 0.2$ as above  
2 $1.66\pm 0.09$ $1.3\pm 0.2$ $1.8\pm 0.2$ 275.5/308
5 $1.34\pm 0.09$ as above $2.3\pm 0.3$  

Notes. Results of joint model fitting to the XIS spectra from the second and fifth intervals are shown. For the spectral fitting, the procedure is the same as that described in Table 3. The lower part shows the results when the spectral slope and the warm absorber parameters ($N_{\rm W}$, log $\xi$) are left to vary, but either of the two warm absorber parameters is tied between the two spectra. (a) In unit of erg s-1 cm. (b) In unit of 1022 cm-2.


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