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Table A.1.

Fitting parameters with the corresponding uncertainties, classifications, physical parameters, and measured redshift.

Name Type Flux FWHM Type Flux FWHM Class. F22 New class. log(MBH/M) REdd Methods zm
[10−17erg s−1] [km s−1] [10−17erg s−1] [km s−1]
Hβ [O III]λ5007

J0422−0644 Gn 43 ± 6 572* Gc 58 ± 3 572 ± 36 FSRQ NLS1 7.05 ± 0.53 0.13 ± 0.07 (A,D) 0.2417 ± 0.0007
Gb 224 ± 46 2265 ± 385 - - -

J0442−0017 L 120 ± 14 3518 ± 1218 Gc 81 ± 5 @ NLS1 BLS1 7.60 ± 0.43 0.23 ± 0.10 (A,D) 0.8467 ± 0.0016

J0515−4556 Gn 24 ± 2 192* Gc 116 ± 1 192 ± 6 AMB NLS1/IS 7.09 ± 0.66 0.05 ± 0.03 (A,D) 0.1946 ± 0.0004
Gb 126 ± 5 1807 ± 291 - - -

J0521−1734 Gn 14 ± 1 845* Gc 43 ± 1 845 ± 30 FSRQ SY2 < 10.23 < 0.01 (B,E) 0.3472 ± 0.0002

J0932+5306 Gn 36 ± 4 267* Gc 316 ± 2 267 ± 5 NLS1 NLS1 7.74 ± 0.50 0.11 ± 0.06 (A,D) 0.5967 ± 0.0002
Gb 174 ± 10 1813 ± 359 - - -

J1048−1912 Gn 19 ± 1 @* Gc 115 ± 1 @ NLS1 IS 8.01 ± 0.94 < 0.09 (A,D) 0.5953 ± 0.0002
Gb 124 ± 3 6040 ± 189 - - -

J1102+5251 Gn 28 ± 3 @* Gc 143 ± 2 @ NLS1 IS 7.38 ± 1.61 < 0.49 (A,D) 0.6899 ± 0.0009
Gb 80 ± 5 3043 ± 293 - - -

J1202−0528 Gn 174 ± 18 @* Gc 791 ± 23 @ NLS1 NLS1 7.86 ± 0.39 0.14 ± 0.06 (A,D) 0.3805 ± 0.0002
Gb 954 ± 80 1843 ± 401 Go 498 ± 24 1069 ± 45

J1246−2548 Gn 86 ± 7 @* Gc 247 ± 5 @ NLS1 NLS1 8.22 ± 0.88 0.10 ± 0.09 (A,D) 0.6372 ± 0.0002
Gb 518 ± 14 4779 ± 149 - - -

J1331−1325 Gn 15 ± 2 @* Gc 84 ± 1 @ FSRQ IS 6.48 ± 1.55 < 0.20 (A,D) 0.2514 ± 0.0002
Gb 23 ± 3 1175 ± 485 - - -

J1818+0903 L 91 ± 8 1418 ± 335 Gc 120 ± 3 @ NLS1 NLS1 6.25 ± 0.40 0.79 ± 0.32 (A,D) 0.3542 ± 0.0004

J1902−6748 Gn 55 ± 3 @* Gc 432 ± 2 @ FSRQ NLS1/IS 7.21 ± 0.78 < 0.11 (A,D) 0.2542 ± 0.0002
Gb 137 ± 11 1850 ± 799 - - -

J2325−3559 L 212 ± 3 971 ± 75 Gc 125 ± 7 @ AMB NLS1 6.32 ± 0.37 1.36 ± 0.51 (A,D) 0.3666 ± 0.0004
- - - Go 70 ± 13 1424 ± 963

Mg IIλ2800 [O II]λ3727

J0102+4214 L 65 ± 1 2771 ± 82 - - - NLS1 NLS1 7.89 ± 0.06 0.74 ± 0.01 (C,F) 0.8773 ± 0.0005

J0224+0700 L 86 ± 9 1408 ± 229 Gc 41 ± 4 @ NLS1 NLS1 7.08 ± 0.34 2.07 ± 0.16 (C,F) 0.5119 ± 0.0007

J1154+4037 L 223 ± 3 10098 ± 297 Gc 4 ± 1 < 454 NLS1 AMB 9.32 ± 0.06 0.08 ± 0.01 (C,F) 0.9251 ± 0.0004

J1310+5514 L 97 ± 1 2271 ± 38 - - - NLS1 NLS1 7.84 ± 0.04 1.28 ± 0.01 (C,F) 0.9251 ± 0.0004

J2354−0958 L 42.5 ± 0.9 4540 ± 158 Gc 6.0 ± 0.3 541 ± 56 AMB AMB 7.62 ± 0.07 0.10 ± 0.01 (C,F) 0.9884 ± 0.0005

Notes. Columns: name of the object, type of curve used to fit the components of the line (Lorentzian - L, narrow Gaussian - Gn, broad Gaussian - Gb, core Gaussian - Gc, and outflow Gaussian - Go), flux, FWHM of the line along with the uncertainty, old classification from Foschini et al. (2022) (F22), the new proposed classification, MBH, REdd, the used methods, and measured redshift. The FWHM values marked with * correspond to those associated with the narrow lines, while values marked with @ correspond to FWHM totally dominated by the instrumental contribution. The table is divided horizontally into two sections: the Hβ–[O III]λ5007 section and the Mg IIλ2800–[O II]λ3727 section. The classifications highlighted in bold correspond to cases in which the new spectra were useful either to confirm the classification proposed by Foschini et al. (2022) or to propose a new one. Methods: (A) for Dalla Bontà et al. (2020), (B) for Ho & Kim (2014), and (C) for Trakhtenbrot & Netzer (2012). The same is valid for the Eddington ratio, due its dependence on MBH. In this case the methods are: (D) for the classical derivation of REdd from Hβ, (E) for the derivation of REdd from [O III]λ5007, and (F) for the derivation of REdd from Mg IIλ2800.

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