Hydrodynamic Simulations of Eccentric Black Hole Encounters in AGN Discs
astro-ph.HE, astro-ph.GA
Submitted: 2026-09-16
Updated: 2026-09-16
Comments: 15 pages, 10 figures, submitted to MNRAS
License: http://creativecommons.org/licenses/by/4.0/
The gist: We investigate close encounters between stellar-mass black holes (BHs) in the gaseous discs of active galactic nuclei (AGNs), during which binary black holes (BBHs) may form.
Terminology
Abstract
We investigate close encounters between stellar-mass black holes (BHs) in the gaseous discs of active galactic nuclei (AGNs), during which binary black holes (BBHs) may form. We perform a suite of 483 2D adiabatic viscous hydrodynamic simulations within a shearing box prescription using the Eulerian grid code Athena++. We co-evolve the two embedded BHs with the gas. To probe the dependence of capture on non-circular initial conditions, we vary the initial radial separation b, the eccentricity e of one of the stellar BHs around the central supermassive black hole, and the eccentric phase angle ϕ e. We consider eccentricities from e=0 to e=0.1 and compare them with the local disc aspect ratio h=H/R 0 0.005. We find that small eccentricities shift the capture window in the parameter space. Eccentricities of order the disc aspect ratio, in particular e about h -- 2h, produce successful captures at initial separations that do not capture in the circular models. By contrast, systems with e h retain less gas before encounter and have lower capture fractions across the sampled parameter grid. We find that the first periapsis distance is a useful predictor of direct capture. Predicting direct capture for r p<0.1r H correctly classifies 92.7% of Hill sphere encounters. The Hill sphere gas mass helps identify gas-poor failures, but provides no clear additional capture boundary within this suite, in which the initial disc density, temperature, and viscosity parameter are held fixed. Pre-encounter eccentricity modifies gas-assisted BBH formation through its combined effects on the first-encounter geometry and the gas reservoir available for orbital energy dissipation.
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