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Table 2.

Measured physical properties of GPs with X-ray detections.

Source X-ray FX(0.5 − 8 keV)(1) log(LX(0.5 − 8 keV)) (1) log(LX(2 − 10 keV))(1) log(SFR) SFR 12 + log(O/H) Metal log(M) (2) Age(2) BPT
survey 10−14 erg s−1 cm−2 (erg s−1) (erg s−1) M yr−1 source method log(M) (Gyr)
J1330-0043 XMM-Newton 0.18 ± 0.06 41 . 94 0.16 + 0.12 $ 41.94^{+0.12}_{-0.16} $ 42 . 33 0.16 + 0.12 $ 42.33^{+0.12}_{-0.16} $ 0 . 27 0.05 + 0.04 $ 0.27^{+0.04}_{-0.05} $ SED 8.63±0.22 O3N2 9.91 ± 0.02 1.5 SF
J0035+0431 XMM-Newton 1.04 ± 0.26 42 . 26 0.12 + 0.10 $ 42.26^{+0.10}_{-0.12} $ 42 . 65 0.12 + 0.10 $ 42.65^{+0.10}_{-0.12} $ 0 . 34 0.03 + 0.02 $ 0.34^{+0.02}_{-0.03} $ SED 7.88±0.30 R23 10.22 ± 0.02 1.0
J0205+1504 Swift 16.83 ± 6.73 43 . 51 0.22 + 0.15 $ 43.51^{+0.15}_{-0.22} $ 43 . 90 0.22 + 0.15 $ 43.90^{+0.15}_{-0.22} $ 0.62 ± 0.02 SED 8.51 ± 0.35 O3N2 9.49 ± 0.02 0.8 SF
J0227+2355 Swift 1 . 21 0.31 + 0.36 $ 1.21^{+0.36}_{-0.31} $ 42 . 40 0.13 + 0.11 $ 42.40^{+0.11}_{-0.13} $ 42 . 80 0.13 + 0.11 $ 42.80^{+0.11}_{-0.13} $ 0.42 ± 0.02 SED 8.91 ± 0.15 SB98(3) 10.05 ± 0.02 4.0 AGN
J1605+4405 Chandra 3 . 03 0.89 + 0.84 $ 3.03^{+0.84}_{-0.89} $ 43 . 02 0.15 + 0.11 $ 43.02^{+0.11}_{-0.15} $ 43 . 41 0.15 + 0.10 $ 43.41^{+0.10}_{-0.15} $ 1.05 ± 0.02 SED 8.63 ± 0.04 SB98(3) 10.51 ± 0.02 1.8 AGN
J0906+0242 eROSITA 5.52 ± 2.18 43 . 10 0.22 + 0.14 $ 43.10^{+0.14}_{-0.22} $ 43 . 49 0.22 + 0.14 $ 43.49^{+0.14}_{-0.22} $ 0.21 ± 0.02 SED 8.42±0.08 O3N2 9.59 ± 0.02 1.0 SF

J0749+3337 XMM-Newton 0.5±0.15 42 . 08 0.18 + 0.12 $ 42.08^{+0.12}_{-0.18} $ < 41.42 1.77 NUV+W4 8.3 O3N2 9.8 SF
J0822+2241 XMM-Newton 0 . 8 0.15 + 0.18 $ 0.8 ^{+0.18}_{-0.15} $ 42 . 08 0.12 + 0.07 $ 42.08^{+0.07}_{-0.12} $ 41 . 79 0.30 + 0.25 $ 41.79^{+0.25}_{-0.30} $ 1.57 NUV+W4 8.1 O3N2 9.6 SF
J1339+1516 XMM-Newton < 41.11 1.27 NUV+W4 8.1 O3N2 9.3 SF

Notes. (1)The X-ray flux and the luminosity in 0.5–8 keV band, as well as the X-ray luminosity in 2–10 keV band, are measured in the rest frame, assuming Γ = 2.0.

(2)The stellar mass and age are obtained based on the CIGALE fitting result.

(3) The metallicities for the sources that are classified as AGNs from the BPT diagram (see Fig. 4) were determined using the method from Storchi-Bergmann et al. (1998).

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