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Table 1

Spectral fit results.

Modela LMC NH Γ Normb kT Norm - c
[1020 cm-2] [10-4] [keV] -

PL 3.4 ± 1.0 0.925 ± 0.020 3.52 ± 0.09 0.953/975
PL+DiskBB 0.83 ± 0.04 0.917/973
PL+BBradd 0.83 ± 0.04 3.05 ± 0.18 0.24 ± 0.04 0.914/973
PL+BBrad2d 1.35 ± 0.13 0.007 ± 0.003 0.917/973
PL+mekal 0.86 ± 0.03 1.04 ± 0.3 × 10-5 0.924/973
PL+Gausse LMC NH Γ Norm k T BB Norm Gaussf
Phase [1020 cm] 10-4 keV keV/eV

0.00.2 3.55 ± 0.02 1.20 ± 0.05 2.86 ~0 1.47/129
0.20.4 ~0 0.88 ± 0.04 2.63 6.38/227 1.14/160
0.40.6 1.76 ± 0.02 0.75 ± 0.04 3.32 6.38/50 1.11/202
0.60.8 4.96 ± 0.02 0.89 ± 0.04 4.34 6.38/97 1.07/210
0.81.0 9.42 ± 0.03 1.02 ± 0.05 4.65 ~0 1.16/181

PL+BBradg LMC NH Γ Norm k T BB Norm Radiush
Phase [1020 cm] 10-4 keV km

0.00.2 0.83 ± 0.05 1.51 ± 0.16 0.24 ± 0.03 18.9 1.19/534
0.20.4 = = 2.24 ± 0.19 = 14.8
0.40.6 = = 3.55 ± 0.25 = 8.2
0.60.8 = = 3.99 ± 0.3 = 10.8
0.81.0 = = 3.62 ± 0.3 = 11.3

0.00.2 0.80± 0.05 0.276 13.7 1.19/530
0.20.4 = = 10.5
0.40.6 = = 4.7
0.60.8 = 3.8 ± 0.3 = 9.3
0.81.0 = 3.4 ± 0.3 = 11.0

Notes.

(a)

For definition of spectral models see text.

(b)

Photons keV-1 cm-2 s-1 at 1 keV.

(c)

Degrees of freedom (d.o.f.).

(d)

The black-body model could both be fitted with a low or a high temperature component, see text for more details.

(e)

Parameters for phase-resolved analyses, based on a power law plus Gaussian line.

(f)

Center and equivalent width of Fe line if present.

(g)

Parameters for phase resolved analyses, based on a power law plus a thermal component.

(h)

Radius of the emitting area, derived from the black-body normalization.

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