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Table 4

Best fits to the 210 keV EPIC pn spectra for observations 14 using Model 3 (see caption of Table 3 for definitions).

Observation No. 1 2 3 4T 4B

Comp.
Parameter
tbabs
(1022 cm-2) 7.81 ± 0.02 7.74  7.85 ± 0.02 7.84 ± 0.04 8.19 ± 0.07
diskbb
kTdbb (keV) 1.403 ± 0.002 1.435 ± 0.003 1.471 ± 0.003 1.572 ± 0.004 1.73 ± 0.01
kdbb [(Rin/D10)2 cosθ] 215 ± 2 218 ± 3 200 ± 1 194 ± 3 103 ± 3
warmabs
(1022 cm-2) 13.5 ± 0.6 12.0  11.0 ± 0.8 9.3  3.4 
log (ξ)(erg cm s-1) 4.27  4.37  4.33  4.40  4.02 
S 15 ± 5 16 ± 7 16 ± 6 21  25 
σv(km s-1) 1565  2400  1880  2035  720 
v (km s-1) 3570 ± 30 2100 ± 120 3480  3480  3870 
kdblur
rin (rg) 19  11 ± 2 14 ± 3 <5 <17
rfxconv
re l refl 0.60 ± 0.05 0.44 ± 0.05 0.30 ± 0.04 0.15 ± 0.05 0.08 

(10-8 erg cm-2 s-1) 1.07 1.20 1.23 1.60 1.30
(10-8 erg cm-2 s-1) 1.18 1.31 1.32 1.67 1.34

(d.o.f.) 1.01 (123) 0.87 (122) 0.95 (122) 0.70 (123) 0.93 (122)

Notes. rin is the inner disc radius at which the reflection component is located (in units of rg) and relrefl the reflection fraction. The inclination has been fixed to 65° both for the kdblur and rfxconv components and the ionisation parameter to log (ξ) = 4 for the rfxconv component. In addition, the power law emissivity index has been fixed to 3 and the outer radius to 400 rg for the kdblur component (see text). The flux has been calculated both including (Ftot) and excluding (Fdisc) the reflection component.

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