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Table A.2.

Sample of Type 1 AGNs used in this work.

Source name Log νp Log νpLνp Log MBH, fit λEdd, FIT σ FWHM τLT Log VPσ Log VPfwhm L5100 Å L1350 Å Log MBH, Hβ Log MBH, CIV
[Hz] [erg s−1] [M] [km s−1] [km s−1] [lt. days] [M] [M] [erg s−1] [erg s−1] [M] [M]
(1) (2) (3) (4) (5) (6) (7) (8) (9) (10) (11) (12) (13) (14)
3C 273 (a) 15.42 46.39 9.175 ± 0.450 0.26 ± 0.12 2742 ± 58 45.810 8.691
(b) 1777 ± 150 2598 ± 299 45.960 8.719

Ark 120 (a) 15.28 44.52 8.520 ± 0.450 0.016 ± 0.007 5850 ± 480 44.140 8.514
(b) 1959 ± 109 5536 ± 297 44.230 8.511
(b) 1884 ± 48 5284 ± 203 44.230 8.471

Fairall 9 (a) 15.42 44.60 8.280 ± 0.450 0.033 ± 0.015 5900 ± 650 44.140 8.522
(b) 3787 ± 197 6901 ± 707 44.250 8.713

MRK 142 (d) 15.40 43.92 7.980 ± 0.450 0.014 ± 0.006 859 ± 102 1368 ± 379 43.540 6.952
(e) 1647 ± 69 43.520 7.103

MRK 290 (g) 15.41 43.95 7.975 ± 0.450 0.015 ± 0.007 1606 ± 47 4270 ± 157 43.110 7.726

MRK 335 (a) 15.32 44.22 8.290 ± 0.450 0.014 ± 0.006 1260 ± 120 43.790 7.006
(b) 917 ± 52 1629 ± 145 43.860 7.264
(b) 948 ± 113 1375 ± 357 43.860 7.117
(c) 1293 ± 64 1025 ± 35 43.700 6.781
(e) 1997 ± 265 43.640 7.331

MRK 509 (a) 15.35 44.68 8.460 ± 0.450 0.026 ± 0.012 2860 ± 120 44.170 7.908
(b) 1276 ± 28 2715 ± 101 44.280 7.918

MRK 590 (a) 15.50 43.18 7.410 ± 0.450 0.009 ± 0.004 2170 ± 120 43.710 7.438
(b) 789 ± 74 1675 ± 587 43.810 7.263
(b) 1935 ± 52 2566 ± 106 43.810 7.634
(b) 1251 ± 72 2115 ± 575 43.810 7.466
(b) 1201 ± 130 1979 ± 386 43.810 7.408
MRK 877 (a) 15.20 44.91 8.875 ± 0.450 0.017 ± 0.008 3880 ± 650 44.370 8.273
(b) 2626 ± 211 4718 ± 991 44.480 8.498
MRK 1044 (e) 15.50 43.39 7.515 ± 0.450 0.012 ± 0.006 1211 ± 48 43.050 6.601

MRK 1383 (b) 15.56 45.32 8.360 ± 0.450 0.145 ± 0.067 3442 ± 308 6323 ± 1295 44.720 8.872

MRK 1501 (c) 15.34 44.69 8.485 ± 0.450 0.026 ± 0.012 3321 ± 107 5054 ± 145 44.320 8.477

NGC 3783 (a) 15.40 43.64 7.840 ± 0.450 0.010 ± 0.005 4100 ± 1160 43.250 7.761
(b) 1753 ± 141 3093 ± 529 43.260 7.521

NGC 4151 (a) 15.20 42.35 7.595 ± 0.450 0.001 ± 0.000 5230 ± 920 42.860 7.777
(b) 1914 ± 42 4248 ± 516 42.880 7.606

NGC 5548 (a) 15.33 43.52 7.920 ± 0.450 0.006 ± 0.003 5500 ± 400 43.430 8.106
(b) 1687 ± 56 4044 ± 199 43.510 7.879
(b) 2026 ± 68 5706 ± 357 43.510 8.178
(d) 4270 ± 292 11177 ± 2266 42.620 8.317
(g) 1822 ± 35 4849 ± 112 42.660 7.611

NGC 7469 (a) 15.40 43.69 7.865 ± 0.450 0.011 ± 0.005 3220 ± 1580 43.740 7.796
(b) 1456 ± 207 2169 ± 459 43.720 7.443
(e) 1722 ± 30 43.560 7.162

PG 0026+129 (a) 15.47 45.31 8.535 ± 0.450 0.095 ± 0.044 1358 ± 91 44.850 7.601
(b) 1773 ± 285 1719 ± 495 45.020 7.891
(e) 2544 ± 56 44.840 8.141

PG 0052+251 (a) 15.35 45.40 8.820 ± 0.450 0.060 ± 0.028 4550 ± 270 44.810 8.631
(b) 1783 ± 86 4165 ± 381 44.960 8.629

PG 0804+761 (a) 15.40 45.34 8.690 ± 0.450 0.071 ± 0.033 2430 ± 42 44.820 8.091
(b) 1971 ± 105 2012 ± 845 44.940 7.987
PG 0844+349 (a) 15.44 45.00 8.440 ± 0.450 0.058 ± 0.027 2830 ± 120 44.240 7.934
(b) 1448 ± 79 2148 ± 612 44.350 7.749
(e) 2694 ± 58 44.150 7.846

PG 0953+414 (a) 15.45 45.88 8.860 ± 0.450 0.167 ± 0.077 2723 ± 62 45.080 8.320
(b) 1306 ± 144 3002 ± 398 45.220 8.475

PG 1211+143 (a) 15.37 45.20 8.680 ± 0.450 0.053 ± 0.024 1479 ± 66 44.690 7.595
(b) 1080 ± 102 1317 ± 138 44.750 7.524
(e) 2012 ± 37 44.660 7.847
PG 1247+267 (h) 15.39 47.58 9.830 ± 0.450 0.895 ± 0.414 2104 ± 540 4568 ± 1338 47.590 9.882

PG 1307+085 (a) 15.55 45.38 8.410 ± 0.450 0.148 ± 0.069 5260 ± 270 44.720 8.712
(b) 1820 ± 122 5058 ± 524 44.880 8.758

PG 1411+442 (a) 15.24 44.90 8.790 ± 0.450 0.020 ± 0.009 2740 ± 110 44.510 8.040
(b) 1607 ± 169 2398 ± 353 44.630 7.985

PG 1700+518 (a) 15.04 45.65 9.565 ± 0.450 0.019 ± 0.009 1970 ± 150 45.430 8.214
(b) 1700 ± 123 1846 ± 682 45.630 8.257
(e) 2252 ± 85 45.440 8.335

PG 2130+099 (a) 15.39 44.70 8.390 ± 0.450 0.032 ± 0.015 3010 ± 180 44.330 8.032
(b) 1623 ± 86 2912 ± 231 44.460 8.068
(c) 1825 ± 65 2097 ± 102 44.150 7.628
(e) 2450 ± 188 44.130 7.753

S5 0836+71 (i) 15.46 47.22 9.510 ± 0.450 0.816 ± 0.377 9700 ± 0 47.050 10.250

Notes. (1) Name of the sources. (2) and (3) Logarithmic value of the spectrum peak frequency νp in Hz and luminosity νpLνp in erg s−1 inferred from the SED fitting procedure. (4) and (5) BH mass in solar masses and Eddington ratio λEdd computed from the SED fitting procedure; the mean uncertainties are connected to different quantities (i.e., BH spin, viewing angle, uncertainty on the spectrum peak position). (6) and (7) velocity dispersion and FWHM in km s−1 related to the Hβ line (for PG 1247+267 and S5 0836+71, these measurements are related to the CIV line). (8) Light travel time in the rest-frame expressed in days. (9) and (10) Logarithmic value of the VP in solar masses computed using the velocity dispersion and the FWHM; the uncertainties are connected to τLT and σline (or FWHM); the systematic uncertainty is ∼0.5 dex (Peterson 2010). (11) and (12) Continuum luminosity at 5100 Å and 1350 Å in erg s−1 as reported in the corresponding reference paper. (13) and (14) Logarithmic value of the BH mass in solar masses computed using the Hβ (CIV) line FWHM and the luminosity at 5100 Å (1350 Å) as reported in the reference paper, through the SE relations described in Vestergaard & Peterson (2006). SE BH mass estimates have a systematic uncertainty of ∼0.5 dex (VesterOs). When a lower error is absent, it means that for that source only an upper limit is present.

References. (a)from Kaspi et al. (2000); (b)from Peterson et al. (2004); (c)from Grier et al. (2012); (d)from Bentz et al. (2009); (e)from Wang et al. (2014); (f)from Bentz et al. (2014); (g)from Denney et al. (2010); (h)from Trevese et al. (2014); (i)from Kaspi et al. (2007).

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