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 ‘*’.
Source | A | log NH (cm−2) | kT (keV) | χ2/ν | Prob |
XMM J021908.37−044731.4 | 2.4+0.5−0.5 | 22.1+0.2−0.2 | 0.23+0.07−0.07 | 10/12 | 0.64 |
XMM J021939.22−051133.7 | 3.8+1.1−1.0 | 22.8+0.2−0.2 | 0.30+0.11−0.08 | 3/7 | 0.88 |
XMM J080625.35+244326.0 | 1.9+0.7−0.7 | 22.4+0.2−0.5 | 0.43+0.40−0.23 | 1/3 | 0.93 |
XMM J083139.11+524206.2 | 7.2+1.2−1.2 | 23.3+0.1−0.1 | 1.00+0.00*−0.11 | 77/40 | 8.6 × 10−5 |
XMM J094239.79+465005.3 | 1.4+0.4−0.4 | 22.5+0.1−0.2 | 1.00+0.00*−0.18 | 16/8 | 4.9 × 10−2 |
XMM J122656.53+013125.2 | 5.7+1.0−0.8 | 22.4+0.1−0.1 | 1.00+0.00*−0.90* | 37/15 | 1.2 × 10−3 |
XMM J133026.09+241356.7 | 2.9+0.4−0.4 | 22.5+0.1−0.1 | 0.29+0.06−0.05 | 44/32 | 7.5 × 10−2 |
XMM J150339.60+101605.6 | 7.3+2.3−1.7 | 22.8+0.2−0.1 | 1.00+0.00*−0.21 | 27/11 | 4.0 × 10−3 |
XMM J161736.21+122901.5 | 2.1+0.8−0.6 | 22.3+0.3−0.2 | 0.41+0.59−0.20 | 17/8 | 2.9 × 10−2 |
Source | A | log NH (cm−2) | kT (keV) | χ2/ν | Prob |
XMM J021908.37−044731.4 | 2.4+0.5−0.5 | 22.1+0.2−0.2 | 0.23+0.07−0.07 | 10/12 | 0.64 |
XMM J021939.22−051133.7 | 3.8+1.1−1.0 | 22.8+0.2−0.2 | 0.30+0.11−0.08 | 3/7 | 0.88 |
XMM J080625.35+244326.0 | 1.9+0.7−0.7 | 22.4+0.2−0.5 | 0.43+0.40−0.23 | 1/3 | 0.93 |
XMM J083139.11+524206.2 | 7.2+1.2−1.2 | 23.3+0.1−0.1 | 1.00+0.00*−0.11 | 77/40 | 8.6 × 10−5 |
XMM J094239.79+465005.3 | 1.4+0.4−0.4 | 22.5+0.1−0.2 | 1.00+0.00*−0.18 | 16/8 | 4.9 × 10−2 |
XMM J122656.53+013125.2 | 5.7+1.0−0.8 | 22.4+0.1−0.1 | 1.00+0.00*−0.90* | 37/15 | 1.2 × 10−3 |
XMM J133026.09+241356.7 | 2.9+0.4−0.4 | 22.5+0.1−0.1 | 0.29+0.06−0.05 | 44/32 | 7.5 × 10−2 |
XMM J150339.60+101605.6 | 7.3+2.3−1.7 | 22.8+0.2−0.1 | 1.00+0.00*−0.21 | 27/11 | 4.0 × 10−3 |
XMM J161736.21+122901.5 | 2.1+0.8−0.6 | 22.3+0.3−0.2 | 0.41+0.59−0.20 | 17/8 | 2.9 × 10−2 |
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 ‘*’.
Source | A | log NH (cm−2) | kT (keV) | χ2/ν | Prob |
XMM J021908.37−044731.4 | 2.4+0.5−0.5 | 22.1+0.2−0.2 | 0.23+0.07−0.07 | 10/12 | 0.64 |
XMM J021939.22−051133.7 | 3.8+1.1−1.0 | 22.8+0.2−0.2 | 0.30+0.11−0.08 | 3/7 | 0.88 |
XMM J080625.35+244326.0 | 1.9+0.7−0.7 | 22.4+0.2−0.5 | 0.43+0.40−0.23 | 1/3 | 0.93 |
XMM J083139.11+524206.2 | 7.2+1.2−1.2 | 23.3+0.1−0.1 | 1.00+0.00*−0.11 | 77/40 | 8.6 × 10−5 |
XMM J094239.79+465005.3 | 1.4+0.4−0.4 | 22.5+0.1−0.2 | 1.00+0.00*−0.18 | 16/8 | 4.9 × 10−2 |
XMM J122656.53+013125.2 | 5.7+1.0−0.8 | 22.4+0.1−0.1 | 1.00+0.00*−0.90* | 37/15 | 1.2 × 10−3 |
XMM J133026.09+241356.7 | 2.9+0.4−0.4 | 22.5+0.1−0.1 | 0.29+0.06−0.05 | 44/32 | 7.5 × 10−2 |
XMM J150339.60+101605.6 | 7.3+2.3−1.7 | 22.8+0.2−0.1 | 1.00+0.00*−0.21 | 27/11 | 4.0 × 10−3 |
XMM J161736.21+122901.5 | 2.1+0.8−0.6 | 22.3+0.3−0.2 | 0.41+0.59−0.20 | 17/8 | 2.9 × 10−2 |
Source | A | log NH (cm−2) | kT (keV) | χ2/ν | Prob |
XMM J021908.37−044731.4 | 2.4+0.5−0.5 | 22.1+0.2−0.2 | 0.23+0.07−0.07 | 10/12 | 0.64 |
XMM J021939.22−051133.7 | 3.8+1.1−1.0 | 22.8+0.2−0.2 | 0.30+0.11−0.08 | 3/7 | 0.88 |
XMM J080625.35+244326.0 | 1.9+0.7−0.7 | 22.4+0.2−0.5 | 0.43+0.40−0.23 | 1/3 | 0.93 |
XMM J083139.11+524206.2 | 7.2+1.2−1.2 | 23.3+0.1−0.1 | 1.00+0.00*−0.11 | 77/40 | 8.6 × 10−5 |
XMM J094239.79+465005.3 | 1.4+0.4−0.4 | 22.5+0.1−0.2 | 1.00+0.00*−0.18 | 16/8 | 4.9 × 10−2 |
XMM J122656.53+013125.2 | 5.7+1.0−0.8 | 22.4+0.1−0.1 | 1.00+0.00*−0.90* | 37/15 | 1.2 × 10−3 |
XMM J133026.09+241356.7 | 2.9+0.4−0.4 | 22.5+0.1−0.1 | 0.29+0.06−0.05 | 44/32 | 7.5 × 10−2 |
XMM J150339.60+101605.6 | 7.3+2.3−1.7 | 22.8+0.2−0.1 | 1.00+0.00*−0.21 | 27/11 | 4.0 × 10−3 |
XMM J161736.21+122901.5 | 2.1+0.8−0.6 | 22.3+0.3−0.2 | 0.41+0.59−0.20 | 17/8 | 2.9 × 10−2 |
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