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Implications of the continuous radio-loudness distribution among active galactic nuclei in the local Universe

A. WójtowiczAstronomical Observatory, Jagiellonian University, ul. Orla 171N. Vale AsariDepartamento de Física–CFM, Universidade Federal de Santa Catarina, C.P. 5064Ł. StawarzAstronomical Observatory, Jagiellonian University, ul. Orla 171G. StasińskaLUX, Observatoire de Paris, Université PSL, Sorbonne Université, CNRSD. Kozieł-WierzbowskaAstronomical Observatory, Jagiellonian University, ul. Orla 171
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Aims. We investigate the radio loudness (ℛ) distribution in a large, homogeneous sample of radio galaxies. Methods. The sample is composed of galaxies from the ROGUE I/II catalogue that belongs to the SDSS main galaxy sample and is divided into optically inactive radio galaxies (OPIRGs), optically active ones (OPARGs), and ’radio Seyferts’. We used optical, mid-infrared, and radio data to calculate the active galactic nucleus bolometric luminosities, accretion rate ( λ ), black-hole mass ( M BH ), and ℛ. Results. Contrary to some previous studies based on restricted samples, using our complete sample of objects with redshifts z < 0.4, we find no evidence of bimodality in ℛ. The highest ℛ values are associated with extended radio structures. We find that ℛ is anti-correlated with λ , and spans ∼2 dex at fixed λ . Radio Seyferts, OPARGs, and OPIRGs form a sequence of increasing M BH with substantial overlap. Radio Seyferts show no correlation ℛ– M BH , whereas OPARGs and OPIRGs show a weak positive trend. From theoretical considerations, the observed ∼2-dex spread in radio luminosity and ℛ can be reproduced by only an approximately four-fold variation in the dimensionless magnetic flux φ assuming realistic black-hole spins. Conclusions. The smooth distribution of radio loudness supports a common evolutionary path for all radio sources, with black-hole spin and magnetic field varying continuously. The radio loudness depends on black-hole mass and accretion rate, while moderate variations in φ may account for the observed scatter in this relation.

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