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The Low-Luminosity End of the Radius-Luminosity Relationship for Active Galactic Nuclei

26 Pith papers cite this work, alongside 773 external citations. Polarity classification is still indexing.

26 Pith papers citing it
773 external citations · Pith
abstract

We present an updated and revised analysis of the relationship between the Hbeta broad-line region (BLR) radius and the luminosity of the active galactic nucleus (AGN). Specifically, we have carried out two-dimensional surface brightness decompositions of the host galaxies of 9 new AGNs imaged with the Hubble Space Telescope Wide Field Camera 3. The surface brightness decompositions allow us to create "AGN-free" images of the galaxies, from which we measure the starlight contribution to the optical luminosity measured through the ground-based spectroscopic aperture. We also incorporate 20 new reverberation-mapping measurements of the Hbeta time lag, which is assumed to yield the average Hbeta BLR radius. The final sample includes 41 AGNs covering four orders of magnitude in luminosity. The additions and updates incorporated here primarily affect the low-luminosity end of the R-L relationship. The best fit to the relationship using a Bayesian analysis finds a slope of alpha = 0.533 (+0.035/-0.033), consistent with previous work and with simple photoionization arguments. Only two AGNs appear to be outliers from the relationship, but both of them have monitoring light curves that raise doubt regarding the accuracy of their reported time lags. The scatter around the relationship is found to be 0.19(+/-0.02) dex, but would be decreased to 0.13 dex by the removal of these two suspect measurements. A large fraction of the remaining scatter in the relationship is likely due to the inaccurate distances to the AGN host galaxies. Our results help support the possibility that the R-L relationship could potentially be used to turn the BLRs of AGNs into standardizable candles. This would allow the cosmological expansion of the Universe to be probed by a separate population of objects, and over a larger range of redshifts.

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2026 25 2019 1

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representative citing papers

Tracing Active Galactic Nuclei Properties Through a Changing-look Event

astro-ph.GA · 2026-04-08 · unverdicted · novelty 7.0

A changing-look AGN exhibits a rapid accretion-driven spectral transition with broad-line region temperatures of approximately 11,800 K measured via Boltzmann plots and stable black hole mass estimates of 5 times 10 to the 7 solar masses across epochs.

Little Red Dots as Supermassive Analogs of SS 433

astro-ph.HE · 2026-06-19 · unverdicted · novelty 6.0

LRDs are interpreted as high-inclination hyper-Eddington accreting SMBHs analogous to SS 433, with V-shaped SEDs, X-ray weakness, and Balmer breaks emerging from disk self-shielding geometry.

A Magnetized Black Hole Envelope Model for Little Red Dots

astro-ph.GA · 2026-05-20 · unverdicted · novelty 6.0

A theoretical model of a magnetized black hole envelope is developed to explain the broad emission lines and X-ray faintness observed in little red dots using co-rotating plasma clumps and limited X-ray sources.

Radiation-pressure instability is an artifact of constant-$\alpha$ closure

astro-ph.HE · 2026-06-30 · unverdicted · novelty 5.0

Requiring thermal stability and single-valuedness in the thin-disk Ṁ-Σ plane produces a viscosity law α(X) with X = P_gas/P_rad that eliminates the radiation-pressure dominated instability while preserving the effective-temperature profile.

Locating the Production Sites of High-Energy Neutrinos in Blazar Jets

astro-ph.HE · 2026-06-01 · unverdicted · novelty 5.0

Efficient neutrino production requires an external radiation field stronger than the magnetic field near the broad-line region, but this conflicts with single-zone broadband emission, implying the neutrino site must be physically separated from the dominant electromagnetic zone in uncommon jet confi

Infrared Line Diagnostics Fail to Constrain Sgr A*'s UV Output

astro-ph.HE · 2026-05-13 · accept · novelty 5.0

Mid-infrared lines near Sgr A* exhibit no detectable variability during flares, because light-crossing and recombination timescales in the extended gas suppress responses, so the lines cannot constrain instantaneous UV flux.

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