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Table 7.

Hβ-based, Hα-based, and MgII-based SMBH mass, Hβ-based and Hα-based Eddington ratio of the SUPER AGNs (see Sect. 4.3 for details).

ID Log (/M) Log (/ M) Log(/M)
(1) (2) (3) (4) (5) (6)
X_N_160_22 9.07 ± 0.30 9.16 ± 0.30 8.95 ± 0.30 0.31 ± 0.21 0.25 ± 0.17
X_N_81_44 9.05 ± 0.30 9.28 ± 0.30 8.91 ± 0.31 0.37 ± 0.26 0.22 ± 0.15
X_N_53_3 8.53 ± 0.30 8.68 ± 0.31 0.32 ± 0.22
X_N_66_23 8.94 ± 0.30 8.49 ± 0.39 0.08 ± 0.06
X_N_35_20 8.41 ± 0.38 0.07 ± 0.06
X_N_12_26 8.87 ± 0.30 8.91 ± 0.30 0.30 ± 0.21 0.27 ± 0.19
X_N_44_64 8.76 ± 0.31 0.04 ± 0.03
X_N_4_48 8.91 ± 0.31 9.37 ± 0.30 9.33 ± 0.32 0.12 ± 0.09 0.04 ± 0.03
X_N_102_35 8.85 ± 0.30 8.96 ± 0.30 9.03 ± 0.30 0.62 ± 0.43 0.48 ± 0.34
X_N_115_23 9.11 ± 0.30 9.24 ± 0.30 8.78 ± 0.32 0.16 ± 0.11 0.12 ± 0.08
cid_166 9.33 ± 0.30 9.53 ± 0.30 9.39 ± 0.31 0.26 ± 0.18 0.17 ± 0.12
cid_1605 8.55 ± 0.31 8.32 ± 0.31 8.60 ± 0.31 0.20 ± 0.14 0.34 ± 0.24
cid_346 9.13 ± 0.30 9.21 ± 0.30 9.06 ± 0.32 0.23 ± 0.16 0.19 ± 0.13
cid_1205 8.60 ± 0.30 0.10 ± 0.07
cid_467 9.28 ± 0.31 9.37 ± 0.30 9.11 ± 0.36 0.12 ± 0.08 0.10 ± 0.07
J1333+1649 9.99 ± 0.30 9.98 ± 0.30 9.47 ± 0.30 0.56 ± 0.39 0.57 ± 0.39
J1441+0454 9.27 ± 0.30 9.40 ± 0.30 9.33 ± 0.30 1.27 ± 0.88 0.95 ± 0.66
J1549+1245 10.75 ± 0.30 10.17 ± 0.30 9.17 ± 0.30 0.06 ± 0.04 0.24 ± 0.17
S82X1905 8.90 ± 0.30 8.89 ± 0.30 8.89 ± 0.34 0.27 ± 0.18 0.27 ± 0.19
S82X1940 8.36 ± 0.30 8.91 ± 0.30 7.48 ± 0.43 0.31 ± 0.22 0.09 ± 0.06
S82X2058 9.12 ± 0.30 9.16 ± 0.30 8.95 ± 0.33 0.12 ± 0.09 0.11 ± 0.08

Notes. Columns give the following information: (1) target identification, (2) logarithm of Hβ-based BH mass, (3) logarithm of Hα-based BH mass, (4) logarithm of MgII-based BH mass, (5) Eddington ratio derived from Hβ-based BH mass and (6) Eddington ratio derived from Hα-based BH mass. The error associated with the BH masses and hence Eddington ratios includes both the statistical uncertainties affecting the continuum or line luminosities and FWHM values and the systematic uncertainty in the virial relations (∼0.3 dex, e.g. Bongiorno et al. 2014).

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