Table 6

Two component fits to the XMM–Newton spectra consisting of two power laws, of which one is absorbed by cold material, and the other is not. A1 is the normalization of the absorbed power law and A2 is the normalization of the unabsorbed component, in units of 10−5 photons cm−2 s−1 keV−1. Both power laws have fixed Γ= 1.9. 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.

SourceA1A2log NH (cm−2)χ2Prob
XMM J021908.37−044731.42.2+0.5−0.50.32+0.12−0.1322.3+0.2−0.216/130.27
XMM J021939.22−051133.74.1+1.3−1.10.11+0.05−0.0522.9+0.3−0.37/80.54
XMM J080625.35+244326.01.5+1.1−0.90.56+0.23−0.2722.7+0.6−0.54/40.47
XMM J083139.11+524206.27.6+1.4−1.30.13+0.02−0.0323.4+0.1−0.139/370.38
XMM J094239.79+465005.31.3+0.4−0.40.05+0.05−0.0522.4+0.3−0.323/95.5 × 10−3
XMM J122656.53+013125.25.7+0.7−0.80.00+0.09−0.00*22.4+0.1−0.137/162.0 × 10−3
XMM J133026.09+241356.73.0+0.5−0.40.20+0.05−0.0422.6+0.1−0.127/330.78
XMM J150339.60+101605.67.9+2.2−1.90.21+0.09−0.0822.9+0.1−0.122/123.7 × 10−2
XMM J161736.21+122901.52.4+1.1−0.80.23+0.09−0.1022.5+0.3−0.311/90.30
SourceA1A2log NH (cm−2)χ2Prob
XMM J021908.37−044731.42.2+0.5−0.50.32+0.12−0.1322.3+0.2−0.216/130.27
XMM J021939.22−051133.74.1+1.3−1.10.11+0.05−0.0522.9+0.3−0.37/80.54
XMM J080625.35+244326.01.5+1.1−0.90.56+0.23−0.2722.7+0.6−0.54/40.47
XMM J083139.11+524206.27.6+1.4−1.30.13+0.02−0.0323.4+0.1−0.139/370.38
XMM J094239.79+465005.31.3+0.4−0.40.05+0.05−0.0522.4+0.3−0.323/95.5 × 10−3
XMM J122656.53+013125.25.7+0.7−0.80.00+0.09−0.00*22.4+0.1−0.137/162.0 × 10−3
XMM J133026.09+241356.73.0+0.5−0.40.20+0.05−0.0422.6+0.1−0.127/330.78
XMM J150339.60+101605.67.9+2.2−1.90.21+0.09−0.0822.9+0.1−0.122/123.7 × 10−2
XMM J161736.21+122901.52.4+1.1−0.80.23+0.09−0.1022.5+0.3−0.311/90.30
Table 6

Two component fits to the XMM–Newton spectra consisting of two power laws, of which one is absorbed by cold material, and the other is not. A1 is the normalization of the absorbed power law and A2 is the normalization of the unabsorbed component, in units of 10−5 photons cm−2 s−1 keV−1. Both power laws have fixed Γ= 1.9. 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.

SourceA1A2log NH (cm−2)χ2Prob
XMM J021908.37−044731.42.2+0.5−0.50.32+0.12−0.1322.3+0.2−0.216/130.27
XMM J021939.22−051133.74.1+1.3−1.10.11+0.05−0.0522.9+0.3−0.37/80.54
XMM J080625.35+244326.01.5+1.1−0.90.56+0.23−0.2722.7+0.6−0.54/40.47
XMM J083139.11+524206.27.6+1.4−1.30.13+0.02−0.0323.4+0.1−0.139/370.38
XMM J094239.79+465005.31.3+0.4−0.40.05+0.05−0.0522.4+0.3−0.323/95.5 × 10−3
XMM J122656.53+013125.25.7+0.7−0.80.00+0.09−0.00*22.4+0.1−0.137/162.0 × 10−3
XMM J133026.09+241356.73.0+0.5−0.40.20+0.05−0.0422.6+0.1−0.127/330.78
XMM J150339.60+101605.67.9+2.2−1.90.21+0.09−0.0822.9+0.1−0.122/123.7 × 10−2
XMM J161736.21+122901.52.4+1.1−0.80.23+0.09−0.1022.5+0.3−0.311/90.30
SourceA1A2log NH (cm−2)χ2Prob
XMM J021908.37−044731.42.2+0.5−0.50.32+0.12−0.1322.3+0.2−0.216/130.27
XMM J021939.22−051133.74.1+1.3−1.10.11+0.05−0.0522.9+0.3−0.37/80.54
XMM J080625.35+244326.01.5+1.1−0.90.56+0.23−0.2722.7+0.6−0.54/40.47
XMM J083139.11+524206.27.6+1.4−1.30.13+0.02−0.0323.4+0.1−0.139/370.38
XMM J094239.79+465005.31.3+0.4−0.40.05+0.05−0.0522.4+0.3−0.323/95.5 × 10−3
XMM J122656.53+013125.25.7+0.7−0.80.00+0.09−0.00*22.4+0.1−0.137/162.0 × 10−3
XMM J133026.09+241356.73.0+0.5−0.40.20+0.05−0.0422.6+0.1−0.127/330.78
XMM J150339.60+101605.67.9+2.2−1.90.21+0.09−0.0822.9+0.1−0.122/123.7 × 10−2
XMM J161736.21+122901.52.4+1.1−0.80.23+0.09−0.1022.5+0.3−0.311/90.30
Close
This Feature Is Available To Subscribers Only

Sign In or Create an Account

Close

This PDF is available to Subscribers Only

View Article Abstract & Purchase Options

For full access to this pdf, sign in to an existing account, or purchase an annual subscription.

Close