Table 7

Two component fits to the XMM–Newton spectra consisting of an absorbed, Γ= 1.9 power law, and an optically thin thermal plasma. A is the power-law normalization in units of 10−5 photons cm−2 s−1 keV−1. The ‘Prob’ column gives the null hypothesis probability corresponding to χ2/ν. Confidence limits are given at 95 per cent for one interesting parameter (Δχ2= 4); confidence limits that are truncated by the allowed fit range of the parameter, rather than by Δχ2= 4 are labelled with ‘*’.

SourceAlog NH (cm−2)kT (keV)χ2Prob
XMM J021908.37−044731.42.4+0.5−0.522.1+0.2−0.20.23+0.07−0.0710/120.64
XMM J021939.22−051133.73.8+1.1−1.022.8+0.2−0.20.30+0.11−0.083/70.88
XMM J080625.35+244326.01.9+0.7−0.722.4+0.2−0.50.43+0.40−0.231/30.93
XMM J083139.11+524206.27.2+1.2−1.223.3+0.1−0.11.00+0.00*−0.1177/408.6 × 10−5
XMM J094239.79+465005.31.4+0.4−0.422.5+0.1−0.21.00+0.00*−0.1816/84.9 × 10−2
XMM J122656.53+013125.25.7+1.0−0.822.4+0.1−0.11.00+0.00*−0.90*37/151.2 × 10−3
XMM J133026.09+241356.72.9+0.4−0.422.5+0.1−0.10.29+0.06−0.0544/327.5 × 10−2
XMM J150339.60+101605.67.3+2.3−1.722.8+0.2−0.11.00+0.00*−0.2127/114.0 × 10−3
XMM J161736.21+122901.52.1+0.8−0.622.3+0.3−0.20.41+0.59−0.2017/82.9 × 10−2
SourceAlog NH (cm−2)kT (keV)χ2Prob
XMM J021908.37−044731.42.4+0.5−0.522.1+0.2−0.20.23+0.07−0.0710/120.64
XMM J021939.22−051133.73.8+1.1−1.022.8+0.2−0.20.30+0.11−0.083/70.88
XMM J080625.35+244326.01.9+0.7−0.722.4+0.2−0.50.43+0.40−0.231/30.93
XMM J083139.11+524206.27.2+1.2−1.223.3+0.1−0.11.00+0.00*−0.1177/408.6 × 10−5
XMM J094239.79+465005.31.4+0.4−0.422.5+0.1−0.21.00+0.00*−0.1816/84.9 × 10−2
XMM J122656.53+013125.25.7+1.0−0.822.4+0.1−0.11.00+0.00*−0.90*37/151.2 × 10−3
XMM J133026.09+241356.72.9+0.4−0.422.5+0.1−0.10.29+0.06−0.0544/327.5 × 10−2
XMM J150339.60+101605.67.3+2.3−1.722.8+0.2−0.11.00+0.00*−0.2127/114.0 × 10−3
XMM J161736.21+122901.52.1+0.8−0.622.3+0.3−0.20.41+0.59−0.2017/82.9 × 10−2
Table 7

Two component fits to the XMM–Newton spectra consisting of an absorbed, Γ= 1.9 power law, and an optically thin thermal plasma. A is the power-law normalization in units of 10−5 photons cm−2 s−1 keV−1. The ‘Prob’ column gives the null hypothesis probability corresponding to χ2/ν. Confidence limits are given at 95 per cent for one interesting parameter (Δχ2= 4); confidence limits that are truncated by the allowed fit range of the parameter, rather than by Δχ2= 4 are labelled with ‘*’.

SourceAlog NH (cm−2)kT (keV)χ2Prob
XMM J021908.37−044731.42.4+0.5−0.522.1+0.2−0.20.23+0.07−0.0710/120.64
XMM J021939.22−051133.73.8+1.1−1.022.8+0.2−0.20.30+0.11−0.083/70.88
XMM J080625.35+244326.01.9+0.7−0.722.4+0.2−0.50.43+0.40−0.231/30.93
XMM J083139.11+524206.27.2+1.2−1.223.3+0.1−0.11.00+0.00*−0.1177/408.6 × 10−5
XMM J094239.79+465005.31.4+0.4−0.422.5+0.1−0.21.00+0.00*−0.1816/84.9 × 10−2
XMM J122656.53+013125.25.7+1.0−0.822.4+0.1−0.11.00+0.00*−0.90*37/151.2 × 10−3
XMM J133026.09+241356.72.9+0.4−0.422.5+0.1−0.10.29+0.06−0.0544/327.5 × 10−2
XMM J150339.60+101605.67.3+2.3−1.722.8+0.2−0.11.00+0.00*−0.2127/114.0 × 10−3
XMM J161736.21+122901.52.1+0.8−0.622.3+0.3−0.20.41+0.59−0.2017/82.9 × 10−2
SourceAlog NH (cm−2)kT (keV)χ2Prob
XMM J021908.37−044731.42.4+0.5−0.522.1+0.2−0.20.23+0.07−0.0710/120.64
XMM J021939.22−051133.73.8+1.1−1.022.8+0.2−0.20.30+0.11−0.083/70.88
XMM J080625.35+244326.01.9+0.7−0.722.4+0.2−0.50.43+0.40−0.231/30.93
XMM J083139.11+524206.27.2+1.2−1.223.3+0.1−0.11.00+0.00*−0.1177/408.6 × 10−5
XMM J094239.79+465005.31.4+0.4−0.422.5+0.1−0.21.00+0.00*−0.1816/84.9 × 10−2
XMM J122656.53+013125.25.7+1.0−0.822.4+0.1−0.11.00+0.00*−0.90*37/151.2 × 10−3
XMM J133026.09+241356.72.9+0.4−0.422.5+0.1−0.10.29+0.06−0.0544/327.5 × 10−2
XMM J150339.60+101605.67.3+2.3−1.722.8+0.2−0.11.00+0.00*−0.2127/114.0 × 10−3
XMM J161736.21+122901.52.1+0.8−0.622.3+0.3−0.20.41+0.59−0.2017/82.9 × 10−2
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