Wandering intermediate-mass black holes and off-nuclear tidal disruption events from early star clusters

arXiv:2610.20719 · astro-ph.GA, astro-ph.HE · Submitted 2026-10-14 · Read on arXiv

astro-ph.GA, astro-ph.HE

Submitted: 2026-10-14

Updated: 2026-10-14

Comments: 27 pages, 11 figures

License: http://creativecommons.org/licenses/by/4.0/

The gist: Off-nuclear tidal disruption events (TDEs) reveal evidence for massive black holes outside galactic centers, but the origins of this wandering population remain uncertain.

Abstract

Off-nuclear tidal disruption events (TDEs) reveal evidence for massive black holes outside galactic centers, but the origins of this wandering population remain uncertain. We investigate wandering intermediate-mass black holes (IMBHs) formed through runaway stellar collisions in dense, high-redshift star clusters and predict their TDE signatures across cosmic time. Our semi-analytic model samples clusters associated with low-mass subhalos at 7<z<20 and uses merger trees from the IllustrisTNG TNG50 simulation to follow the assembly of 15 elliptical galaxies with stellar masses of 10 9-10 11 M. We compare two models for high-redshift cluster formation: a maximal model taken from a high-resolution simulation and a conservative model calibrated from local cluster relations. Off-nuclear TDEs produced through this mechanism occur in bursts within 10-100 Myr of IMBH formation as the loss-cone surrounding the black hole is depleted. We estimate the rate of off-nuclear TDEs expected across time per galaxy, and characterize these events as typically occurring between 10-10 cubed kpc from their host galaxy centers. Event rates increase with galaxy mass; in the maximal model, the progenitors of the most massive galaxies reach peak off-nuclear TDE rates of approximately 5 times10-4-4 times10-2 yr-1 per galaxy at 7 z 13. This work provides a framework for constraining the early population of star clusters that form IMBHs through runaway collapse via their contribution to the rate of off-nuclear TDEs in the high redshift Universe.

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