Table 4
Catalogue (Compton Thicks only).
ID | RA | Dec | counts | z | L 2−10 keV | N H | Γ | f scat | R | KL | NH | Notes |
(1) | (2) | (3) | (4) | (5) | (6) | (7) | (8) | (9) | (10) | (11) | (12) |
|
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460 | 3:32:23.41 | –27:42:55.89 | 194 | 2.145 |
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0.61 | CT |
420 | 3:32:23.60 | –27:46:01.23 | 48 | 1.033 |
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0.91 | CT |
412 | 3:32:42.87 | –27:48:09.44 | 67 |
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0.59 | CT |
448 | 3:32:19.41 | –27:40:51.76 | 528 | 0.682 |
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0.37 | CT |
474 | 3:32:15.81 | –27:42:06.78 | 339 |
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0.55 | CT |
271 | 3:32:33.86 | –27:42:04.30 | 306 |
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0.25 | CT |
478 | 3:32:14.60 | –27:52:57.06 | 164 |
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0.36 | CT |
467 | 3:32:00.80 | –27:53:33.84 | 541 |
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0.85 | CT |
437 | 3:32:39.15 | –27:48:32.26 | 54 | 2.470 |
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0.84 | CT |
345 | 3:32:24.67 | –27:54:43.24 | 255 | 0.123 |
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0.16 | CT |
451 | 3:32:31.49 | –27:50:28.64 | 38 | 1.613 |
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0.11 | CT |
266 | 3:32:14.94 | –27:42:24.83 | 976 |
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0.35 | CT |
416 | 3:32:21.77 | –27:46:56.99 | 64 |
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1.08 | CT |
406 | 3:31:45.16 | –27:49:48.72 | 571 | 3.153 |
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0.45 | CT |
400 | 3:32:25.18 | –27:54:49.72 | 346 | 1.090 |
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0.46 | CT |
404 | 3:32:36.15 | –27:50:36.97 | 108 | 1.608 |
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0.91 | CT |
401 | 3:31:50.45 | –27:52:11.49 | 592 | 1.370 |
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0.27 | CT |
158 | 3:32:22.59 | –27:44:25.97 | 129 | 0.738 |
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0.73 | CT |
77 | 3:32:35.71 | –27:49:16.18 | 95 | 2.578 |
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0.75 | CT |
417 | 3:32:21.97 | –27:46:56.00 | 35 | 0.670 |
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0.41 | CT |
570 | 3:33:00.76 | –27:48:57.46 | 438 |
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0.64 | CT |
226 | 3:32:14.42 | –27:51:10.43 | 141 | 1.544 |
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0.94 | CT |
441 | 3:32:22.79 | –27:45:28.54 | 46 |
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0.26 | CT |
408 | 3:32:33.22 | –27:49:15.92 | 38 |
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0.40 | CT |
459 | 3:32:29.48 | –27:43:22.27 | 143 | 1.609 |
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0.60 | CT |
384 | 3:32:42.02 | –27:39:49.95 | 507 | 0.152 |
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0.22 | CT |
Notes. The parameters are derived using the torus+pexmon+scattering model. (1) XID, (2,3) right ascension and declination (JD2000) in degrees, (4) photon counts obtained in the analysed 0.5−8 keV range. (5) Redshift with (posterior) uncertainties if photometric (shortened to 3 significant digits). (6) Intrinsic luminosity (2-10 keV) in erg/s. (7) logarithm of the column density NH in cm-2. (8) Photon index; the prior was 1.95 ± 0.15, so if no information was gained this value remains. (9) Scattering normalization relative to the intrinsic power law. (10) Reflection normalization of the pexmon component relative to the intrinsic power law. (11) Information gain measured from the NH posterior in bans. As a reference, the narrowing of a Gaussian from prior to posterior by a factor of 2 corresponds to 0.13ban, and thus values higher than that correspond to significant discriminatory information in the data. (12) Annotations; S when fscat > 3%, s when fscat> 0.5% with ≥90% probability; R when R> 0.3 with ≥90% probability, i.e. strong additional pexmon reflection; Compton-thick (CT) if NH > 1024 cm-2, Compton-thin (O) if 1022 cm-2<NH< 1024 cm-2, unobscured (U), NH < 1022 cm-2, each with ≥50% probability. Only Compton-thick sources are shown here.
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