Table 1
Results of the XMM-Newton pn spectral fit for the highly obscured sources, sorted for decreasing NH.
XMM ID | z | Cl. | C | NH | F2−10 | Log (LI) | Log (LO) | Sc. % | EW | Cstat/d.o.f. | ||
(1) | (2) | (3) | (4) | (5) | (6) | (7) | (8) | (9) | (10) | (11) | ||
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60 361∗ | 1.73 | Ph | 49 |
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0.36 ± 0.14 |
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175.6/201 | ||
70 082∗ | 2.429 | Ph | 34 |
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<2.10 | <3.07 | 238.7/255 | ||
60 314 | 1.107 | Ph | 49 |
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<5.20 | <0.39 | 156.9/157 | ||
217 | 0.66 | Sp | 56 |
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<5.60 |
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144.7/157 | ||
60 152∗ | 0.579 | Sp | 74 |
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<0.80 |
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164.0/162 | ||
60 342∗ | 0.941 | Ph | 33 |
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<1.22 | <0.32 | 145.4/143 | ||
5511∗ | 1.023 | Ph | 101 |
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4.10 ± 3.50 | <0.38 | 215.5/246 | ||
54 514∗ | 0.707 | Sp | 121 |
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1.50 ± 0.70 |
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214.0/220 | ||
60 211∗ | 0.511 | Sp | 38 |
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1.42 ± 0.45 | <0.23 | 122.6/144 | ||
2608∗† | 0.125 | Sp | 142 |
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0.24 ± 0.08 |
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256.8/299 | ||
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202 | 1.32 | Sp | 115 |
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1.87 ± 1.32 | <0.92 | 233.0/270 | ||
60 043 | 1.73 | Ph | 35 |
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<3.80 | <1.31 | 187.0/200 | ||
54 490∗ | 0.908 | Sp | 63 |
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<2.60 | <0.93 | 196.5/206 | ||
258 | 1.748 | Ph | 66 |
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<2.62 | <1.51 | 198.8/203 | ||
70 145∗ | 2.548 | Ph | 50 |
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1.82 ± 0.87 | <3.67 | 135.5/111 | ||
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60 024 | 1.147 | Sp | 55 |
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<3.59 | <0.88 | 175.2/165 | ||
5006 | 2.417 | Sp | 80 |
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<2.82 | <1.55 | 293.4/293 | ||
5357 | 2.189 | Ph | 56 |
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<3.60 | <0.72 | 129.5/123 | ||
5185 | 2.19 | Ph | 32 |
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<5.34 | <2.46 | 105.7/111 | ||
5130 | 1.553 | Sp | 79 |
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3.05 ± 1.83 | <1.61 | 224.5/251 | ||
348 | 0.779 | Ph | 36 |
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<2.38 | <0.21 | 179.8/190 | ||
54 541 | 2.841 | Sp | 35 |
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<2.63 | <1.53 | 114.6/82 | ||
5534 | 2.12 | Ph | 33 |
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<10.00 | <1.71 | 134.2/129 | ||
60 492 | 1.914 | Ph | 41 |
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<2.91 | <0.75 | 193.5/208 | ||
70 084 | 1.27 | Ph | 54 |
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<4.66 | <1.36 | 132.8/119 | ||
5033 | 0.67 | Ph | 87 |
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<0.93 | <0.40 | 132.8/150 | ||
473 | 2.148 | Ph | 50 |
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5.80 ± 4.20 | <2.31 | 203./188 | ||
70 135 | 2.092 | Ph | 54 |
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<9.93 | <1.08 | 211.0/197 | ||
5496 | 0.694 | Sp | 81 |
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<1.76 | <0.53 | 166.5/152 | ||
5007 | 2.390 | Ph | 31 |
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<3.63 | <1.65 | 216.2/198 | ||
5222 | 0.332 | Ph | 120 |
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1.78 ± 0.53 | <0.37 | 243.3/235 | ||
70 007 | 1.848 | Sp | 38 |
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7.30 ± 5.15 | <2.15 | 125.0/109 | ||
302 | 0.186 | Sp | 72 |
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4.20 ± 1.70 | <1.43 | 157.1/166 | ||
5042 | 2.612 | Sp | 90 |
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<7.66 | <0.62 | 227.3/231 | ||
60 436 | 2.313 | Ph | 48 |
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<5.92 | <0.49 | 182.9/174 | ||
5562 | 2.626 | Sp | 64 |
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<10.00 | <0.90 | 145.9/160 | ||
5427 | 1.177 | Sp | 55 |
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<1.32 | <0.95 | 148.4/183 | ||
70 216 | 1.577 | Ph | 36 |
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<4.52 | <0.84 | 147.5/135 | ||
5014 | 0.213 | Sp | 155 |
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1.71 ± 0.35 | <0.54 | 209.4/218 |
Notes. The first group includes the ten sources belonging to the CTKi sample, the second and third groups include the 29 sources belonging to the CTNi sample, with the five sources in the second group being border line. Column: (1) XMM-Newton ID number; (2) redshift; (3) classification (photometric or spectroscopic redshift); (4) 0.3−10 keV net counts; (5) column density in units of 1024 cm-2; (6) 2−10 keV observed flux in units of 10-14 erg cm-2 s-1; (7) Log of the 2−10 keV rest frame intrinsic luminosity, in units of erg s-1. The errors are obtained taking into account the errors on the observed luminosity and on the column density; (8) Log of the 2−10 keV rest frame observed luminosity, in units of erg s-1; (9) intensity of the scatter component, relative to the primary power-law; (10) rest-frame equivalent width of the Fe Kα line, in units of keV, from the Pl fit; (11) best fit Cstat/d.o.f. ∗ Sources whose CT nature is confirmed by the combined analysis of XMM-Newton (pn and MOS) and Chandra data (see Table 2). †Source 2608 was already identified as a CT candidate in Hasinger et al. (2007) and Mainieri et al. (2007).
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