“…large uncertainties on the Eddington ratio could also explain the high accretion rate of this source. The detection of jet radio emission spatially coincident with hard X-ray emission has been often used to estimate the BH mass by means of the fundamental plane of accreting BHs (e.g., Reines et al 2011Reines et al , 2014Mezcua & Lobanov 2011;Webb et al 2012;Hlavacek-Larrondo et al 2012;Koliopanos et al 2017;Mezcua et al 2013aMezcua et al ,b, 2015Mezcua et al , 2018, which is a correlation between nuclear X-ray luminosity, core radio luminosity, and BH mass valid from stellar-mass BHs to SMBHs in the hard X-ray spectral state (e.g., Falcke et al 2004). Several correlations with different scatters exist based on different samples with varied properties: e.g., the correlation from Merloni et al (2003) has the largest scatter (0.88 dex) as it includes both flat and steep radio sources, different accretion rates, and BH masses estimated using different methods; Gültekin et al (2009) use only dynamical BH masses and nuclear radio sources, which reduces the scatter to 0.77 dex; Plotkin et al (2012) include only sub-Eddington accreting sources and a Bayesian approach, which yields a scatter of 0.07 dex (see e.g., Mezcua et al 2018 for a brief review).…”