Fits to the XMM–Newton spectra with a power law of Γ= 1.9 passing through an ionized medium. A is the power-law normalization in units of 10−5 photons cm−2 s−1 keV−1. The ionization parameter ξ is in units of erg cm s−1. 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 ‘*’. The ‘Prob’ column gives the null hypothesis probability corresponding to χ2/ν.
| Source | A | log NH (cm−2) | log ξ | χ2/ν | Prob |
| XMM J021908.37−044731.4 | 2.4+0.4−0.4 | 22.2+0.1−0.2 | 0.8+0.3−0.5 | 11/13 | 0.59 |
| XMM J021939.22−051133.7 | 3.8+1.1−1.0 | 23.0+0.2−0.2 | 1.4+0.2−0.2 | 13/8 | 0.11 |
| XMM J080625.35+244326.0 | 2.0+0.8−0.7 | 22.9+0.4−0.5 | 2.4+0.5−0.7 | 1/4 | 0.97 |
| XMM J083139.11+524206.2 | 6.7+1.2−1.1 | 23.4+0.1−0.1 | 1.6+0.1−0.1 | 128/37 | 6.6 × 10−12 |
| XMM J094239.79+465005.3 | 1.2+0.4−0.4 | 22.4+0.2−0.3 | 0.2+0.8−2.2* | 25/9 | 2.7 × 10−3 |
| XMM J122656.53+013125.2 | 5.8+1.0−0.8 | 22.5+0.2−0.1 | −1.2+2.4−0.8 | 37/16 | 2.4 × 10−3 |
| XMM J133026.09+241356.7 | 2.7+0.4−0.4 | 22.6+0.1−0.1 | 1.0+0.1−0.2 | 82/33 | 4.9 × 10−6 |
| XMM J150339.60+101605.6 | 7.3+2.0−1.7 | 23.0+0.1−0.2 | 1.3+0.2−0.3 | 40/12 | 8.8 × 10−5 |
| XMM J161736.21+122901.5 | 1.9+0.6−0.5 | 22.3+0.2−0.2 | 0.6+0.5−0.9 | 19/9 | 2.8 × 10−2 |
| Source | A | log NH (cm−2) | log ξ | χ2/ν | Prob |
| XMM J021908.37−044731.4 | 2.4+0.4−0.4 | 22.2+0.1−0.2 | 0.8+0.3−0.5 | 11/13 | 0.59 |
| XMM J021939.22−051133.7 | 3.8+1.1−1.0 | 23.0+0.2−0.2 | 1.4+0.2−0.2 | 13/8 | 0.11 |
| XMM J080625.35+244326.0 | 2.0+0.8−0.7 | 22.9+0.4−0.5 | 2.4+0.5−0.7 | 1/4 | 0.97 |
| XMM J083139.11+524206.2 | 6.7+1.2−1.1 | 23.4+0.1−0.1 | 1.6+0.1−0.1 | 128/37 | 6.6 × 10−12 |
| XMM J094239.79+465005.3 | 1.2+0.4−0.4 | 22.4+0.2−0.3 | 0.2+0.8−2.2* | 25/9 | 2.7 × 10−3 |
| XMM J122656.53+013125.2 | 5.8+1.0−0.8 | 22.5+0.2−0.1 | −1.2+2.4−0.8 | 37/16 | 2.4 × 10−3 |
| XMM J133026.09+241356.7 | 2.7+0.4−0.4 | 22.6+0.1−0.1 | 1.0+0.1−0.2 | 82/33 | 4.9 × 10−6 |
| XMM J150339.60+101605.6 | 7.3+2.0−1.7 | 23.0+0.1−0.2 | 1.3+0.2−0.3 | 40/12 | 8.8 × 10−5 |
| XMM J161736.21+122901.5 | 1.9+0.6−0.5 | 22.3+0.2−0.2 | 0.6+0.5−0.9 | 19/9 | 2.8 × 10−2 |
Fits to the XMM–Newton spectra with a power law of Γ= 1.9 passing through an ionized medium. A is the power-law normalization in units of 10−5 photons cm−2 s−1 keV−1. The ionization parameter ξ is in units of erg cm s−1. 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 ‘*’. The ‘Prob’ column gives the null hypothesis probability corresponding to χ2/ν.
| Source | A | log NH (cm−2) | log ξ | χ2/ν | Prob |
| XMM J021908.37−044731.4 | 2.4+0.4−0.4 | 22.2+0.1−0.2 | 0.8+0.3−0.5 | 11/13 | 0.59 |
| XMM J021939.22−051133.7 | 3.8+1.1−1.0 | 23.0+0.2−0.2 | 1.4+0.2−0.2 | 13/8 | 0.11 |
| XMM J080625.35+244326.0 | 2.0+0.8−0.7 | 22.9+0.4−0.5 | 2.4+0.5−0.7 | 1/4 | 0.97 |
| XMM J083139.11+524206.2 | 6.7+1.2−1.1 | 23.4+0.1−0.1 | 1.6+0.1−0.1 | 128/37 | 6.6 × 10−12 |
| XMM J094239.79+465005.3 | 1.2+0.4−0.4 | 22.4+0.2−0.3 | 0.2+0.8−2.2* | 25/9 | 2.7 × 10−3 |
| XMM J122656.53+013125.2 | 5.8+1.0−0.8 | 22.5+0.2−0.1 | −1.2+2.4−0.8 | 37/16 | 2.4 × 10−3 |
| XMM J133026.09+241356.7 | 2.7+0.4−0.4 | 22.6+0.1−0.1 | 1.0+0.1−0.2 | 82/33 | 4.9 × 10−6 |
| XMM J150339.60+101605.6 | 7.3+2.0−1.7 | 23.0+0.1−0.2 | 1.3+0.2−0.3 | 40/12 | 8.8 × 10−5 |
| XMM J161736.21+122901.5 | 1.9+0.6−0.5 | 22.3+0.2−0.2 | 0.6+0.5−0.9 | 19/9 | 2.8 × 10−2 |
| Source | A | log NH (cm−2) | log ξ | χ2/ν | Prob |
| XMM J021908.37−044731.4 | 2.4+0.4−0.4 | 22.2+0.1−0.2 | 0.8+0.3−0.5 | 11/13 | 0.59 |
| XMM J021939.22−051133.7 | 3.8+1.1−1.0 | 23.0+0.2−0.2 | 1.4+0.2−0.2 | 13/8 | 0.11 |
| XMM J080625.35+244326.0 | 2.0+0.8−0.7 | 22.9+0.4−0.5 | 2.4+0.5−0.7 | 1/4 | 0.97 |
| XMM J083139.11+524206.2 | 6.7+1.2−1.1 | 23.4+0.1−0.1 | 1.6+0.1−0.1 | 128/37 | 6.6 × 10−12 |
| XMM J094239.79+465005.3 | 1.2+0.4−0.4 | 22.4+0.2−0.3 | 0.2+0.8−2.2* | 25/9 | 2.7 × 10−3 |
| XMM J122656.53+013125.2 | 5.8+1.0−0.8 | 22.5+0.2−0.1 | −1.2+2.4−0.8 | 37/16 | 2.4 × 10−3 |
| XMM J133026.09+241356.7 | 2.7+0.4−0.4 | 22.6+0.1−0.1 | 1.0+0.1−0.2 | 82/33 | 4.9 × 10−6 |
| XMM J150339.60+101605.6 | 7.3+2.0−1.7 | 23.0+0.1−0.2 | 1.3+0.2−0.3 | 40/12 | 8.8 × 10−5 |
| XMM J161736.21+122901.5 | 1.9+0.6−0.5 | 22.3+0.2−0.2 | 0.6+0.5−0.9 | 19/9 | 2.8 × 10−2 |
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