Table 2.
Results of the X-ray spectral analysis and derived quantities.
| Source | HR | Γ | C/ν | NH(z) | ΔC | F2 − 10 keV | log L2 keV | αox | Δαox |
|---|---|---|---|---|---|---|---|---|---|
| J0303−00 |
 |
1.87 |
553/608 | < 1.2 | 0.0 | 3.61 |
27.59 |
−1.68 | +0.02 |
| J0304−00 |
 |
1.99 |
596/660 | 1.1 |
−2.5 | 4.55 |
27.75 |
−1.64 | +0.07 |
| J0826+31 |
 |
1.56 |
186/213 | < 0.9 | 0.0 | 1.44 |
27.03 |
−1.87 | −0.17 |
| J0835+21 |
 |
1.77 |
569/676 | < 0.3 | 0.0 | 3.97 |
27.55 |
−1.67 | +0.03 |
| J0900+42 |
 |
1.83 |
868/1034 | < 0.1 | 0.0 | 17.09 |
28.27 |
−1.56 | +0.20 |
| J0901+35 |
 |
1.60 |
527/563 | 0.6 |
−0.5 | 2.14 |
27.22 |
−1.82 | −0.12 |
| J0905+30 |
 |
2.12 |
668/710 | < 0.3 | 0.0 | 5.14 |
27.76 |
−1.60 | +0.11 |
| J0942+04 |
 |
2.11 |
385/417 | < 1.6 | 0.0 | 3.39 |
27.66 |
−1.70 | +0.02 |
| J0945+23 | < −0.13 | 1.8(f) | 109/123 | 14 |
−1.4 | < 0.44 | < 26.65 | −1.97 | −0.30 |
| J0947+14 |
 |
1.88 |
643/680 | 1.1 |
−3.2 | 4.90 |
27.66 |
−1.71 | +0.03 |
| J1014+43 |
 |
2.21 |
395/479 | < 0.3 | 0.0 | 3.19 |
27.61 |
−1.83 | −0.05 |
| J1027+35 |
 |
1.91 |
632/683 | < 0.2 | 0.0 | 7.08 |
27.86 |
−1.71 | +0.05 |
| J1111−15 |
 |
1.71 |
326/394 | < 0.8 | 0.0 | 1.00 |
26.91 |
−1.88 | −0.20 |
| J1111+24 |
 |
1.77 |
376/383 | < 0.3 | 0.0 | 1.33 |
27.10 |
−1.91 | −0.19 |
| J1143+34 |
 |
1.94 |
674/734 | < 0.1 | 0.0 | 4.52 |
27.69 |
−1.68 | +0.04 |
| J1148+23 |
 |
1.16 |
338/317 | < 1.6 | 0.0 | 1.21 |
26.79 |
−2.12 | −0.35 |
| J1159+31 |
 |
1.8(f) | 186/163 | < 9.3 | 0.0 | < 0.34 | < 26.46 | −2.14 | −0.42 |
| J1201+01 |
 |
1.60 |
320/348 | 4.0 |
−3.0 | 0.71 |
26.78 |
−2.00 | −0.30 |
| J1220+45 |
 |
1.70 |
221/240 | < 5.7 | 0.0 | 0.47 |
26.66 |
−2.04 | −0.34 |
| J1225+48 |
 |
1.89 |
813/882 | < 0.2 | 0.0 | 6.70 |
27.82 |
−1.59 | +0.12 |
| J1246+26 |
 |
2.00 |
458/565 | 0.9 |
−1.2 | 2.56 |
27.44 |
−1.75 | −0.04 |
| J1246+11 |
 |
2.14 |
449/504 | < 0.8 | 0.0 | 1.97 |
27.39 |
−1.70 | −0.02 |
| J1407+64 |
 |
2.07 |
482/555 | < 0.3 | 0.0 | 3.89 |
27.65 |
−1.71 | +0.02 |
| J1425+54 | > 0.31 | 1.8(f) | 182/182 | 10 |
−2.8 | < 0.74 | < 26.88 | −1.99 | −0.28 |
| J1426+60 |
 |
1.81 |
685/795 | < 0.5 | 0.0 | 8.03 |
27.90 |
−1.74 | +0.04 |
| J1459+00 |
 |
1.72 |
199/204 | 3.0 |
−0.7 | 1.21 |
26.99 |
−1.91 | −0.20 |
| J1507+24 |
 |
1.8(f) | 92/121 | < 2.3 | 0.0 | < 0.24 | < 26.30 | −1.96 | −0.34 |
| J1532+37 |
 |
1.69 |
336/407 | < 1.5 | 0.0 | 1.59 |
27.12 |
−1.92 | −0.18 |
| J1712+57 |
 |
1.68 |
663/794 | 0.9 |
−2.7 | 7.54 |
27.76 |
−1.62 | +0.09 |
| J2234+00 |
 |
1.86 |
646/694 | < 0.2 | 0.0 | 5.49 |
27.70 |
−1.68 | +0.05 |
Notes. Columns: (1) source ID; (2) hardness ratio relative to the 0.5−2 keV (soft) and 2−8 keV (hard) bands, based on EPIC/pn events only and computed following the Bayesian estimation method of Park et al. (2006); (3) photon index of the continuum in the unabsorbed (baseline) model, phabs × zpowerlw, where (f) means that the parameter is frozen; (4) best-fit statistics of the baseline model; (5) column density local to the source in the absorbed model, phabs × zphabs × zpowerlw; (6) statistical improvement after allowing for local absorption, whose inclusion is always less significant than the (nominal) 95% level; (7) intrinsic rest-frame 2−10 keV flux/upper limit as inferred from the baseline/absorbed model, in 10−14 erg s−1 cm−2; (8) intrinsic monochromatic luminosity at rest-frame 2 keV, in erg s−1 Hz−1; (9) two-point UV (2500 Å) to X-ray (2 keV) spectral index; (10) deviation of αox from the LX/LUV relation of Risaliti & Lusso (2019). Typical statistical uncertainties on αox and Δαox are 0.02 and 0.04, respectively. Entries in italics are upper limits.
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