Table 1.
Properties of the QSO2s.
SDSS ID | Short | SDSS | Scale | AV | log Lbol | log L1.4GHz | log MBH | log![]() |
log M* | SFR | |
---|---|---|---|---|---|---|---|---|---|---|---|
ID | z | (kpc/ ″) | (mag) | (erg s−1) | (W Hz−1) | (M⊙) | (M⊙) | (M⊙yr−1) | |||
J101043.36+061201.4 | J1010 | 0.0977 | 1.807 | 1.1 | 45.6 | 24.4 | 8.4±0.8 | –0.8±0.8 | 11.0±0.2 | 32 | 34 |
J110012.39+084616.3 | J1100 | 0.1004 | 1.851 | 0.6 | 45.9 | 24.2 | 7.8±0.4 | 0.0±0.5 | 11.0±0.2 | 36 | 13 |
J135646.10+102609.0 | J1356 | 0.1232 | 2.213 | 0.9 | 45.5 | 24.4 | 8.6±0.3 | –1.0±0.4 | 11.3±0.2 | 73 | 1 |
J143029.88+133912.0 | J1430 | 0.0851 | 1.597 | 0.9 | 45.8 | 23.7 | 8.2±0.4 | –0.4±0.4 | 11.2±0.1 | 13 | 3 |
J150904.22+043441.8 | J1509 | 0.1115 | 2.028 | 2.2 | 46.0 | 23.8 | 8.3±0.8 | –0.2±0.8 | 10.9±0.3 | 36 | 3 |
Notes. The AV values were measured using Hα/Hβ reported by Kong & Ho (2018), and the extinction law is from Cardelli et al. (1989). The only exception is J1356, whose AV value is unrealistically low (0.1 mag), and therefore we use the value measured from VLT/MUSE data instead, as in Zanchettin et al. (2025). Bolometric luminosities were calculated by applying the correction factor of 474 from Lamastra et al. (2009) to the extinction-corrected [O III]5007 Å luminosities from Kong & Ho (2018), and 1.4 GHz luminosities and stellar masses are from Ramos Almeida et al. (2022). The BH masses and Eddington ratios are from Kong & Ho (2018). The last two columns are the global SFRs derived from total IR luminosities from Ramos Almeida et al. (2022), divided by 0.94 to convert them from a Chabrier to a Kroupa initial mass function, and the SFRs were derived by Bessiere et al. (2024) from spectral synthesis modeling of the SDSS spectra (3″ ∼ 5–6 kpc) shown in Fig. A.1..
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