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Table 3.

Continuum luminosities at 5100 Å and BLR radii for the IMBH and low-mass AGN regime.

log MBH/M Lbol/LEdd L5100 [erg s−1] k bol ( 5100 Å ) $ k_{\mathrm{bol}}(5100\,\AA) $ RBLR,  Hα(AD face-on) [lt − days] RBLR,  Hα(θ = 45° ) [lt − days]
5.0 1.04 5.80e40 480 1 . 06 0.40 + 0.65 $ 1.06^{+0.65}_{-0.40} $ 0 . 78 0.29 + 0.49 $ 0.78^{+0.49}_{-0.29} $
5.5 0.328 2.24e41 124 2 . 21 0.81 + 1.32 $ 2.21^{+1.32}_{-0.81} $ 1 . 62 0.60 + 0.97 $ 1.62^{+0.97}_{-0.60} $
6.0 0.104 6.63e41 42 3 . 96 1.41 + 2.34 $ 3.96^{+2.34}_{-1.41} $ 2 . 90 1.05 + 1.71 $ 2.90^{+1.71}_{-1.05} $

Notes. Bolometric corrections k bol ( 5100 Å ) $ k_{\mathrm{bol}}(5100\,\AA) $ and L5100 [erg s−1] luminosity of the AD are calculated as an extension of Netzer (2019) using the Slone & Netzer (2012) model. θ is the inclination of the AD to the line of sight. The AD model adopts a spin parameter = 0.7, and an accretion rate of 2.6 ⋅ 10−3 M/year, corresponding to Lbol = 1.56 ⋅ 1043 erg/s. The BLR radii uncertainties correspond to the 68% confidence interval and are calculated using Monte Carlo sampling, incorporating the inner scatter and coefficients’ uncertainties for the RBLR,  (L5100) relation (Bentz et al. 2013).

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