MAGICS III. Seeds sink swiftly: nuclear star clusters dramatically accelerate seed black hole mergers
Merger rate predictions of Massive Black Hole (MBH) seeds from large-scale cosmological simulations differ widely, with recent studies highlighting the challenge of low-mass MBH seeds failing to reach the galactic center, a phenomenon known as the seed sinking problem. In this work, we tackle this i...
Gespeichert in:
Hauptverfasser: | , , , , |
---|---|
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext bestellen |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
Zusammenfassung: | Merger rate predictions of Massive Black Hole (MBH) seeds from large-scale
cosmological simulations differ widely, with recent studies highlighting the
challenge of low-mass MBH seeds failing to reach the galactic center, a
phenomenon known as the seed sinking problem. In this work, we tackle this
issue by integrating cosmological simulations and galaxy merger simulations
from the MAGICS-I and MAGICS-II resimulation suites with high-resolution
$N$-body simulations. Building on the findings of MAGICS-II, which showed that
only MBH seeds embedded in stellar systems are able to sink to the center, we
extend the investigation by incorporating nuclear star clusters (NSCs) into our
models. Utilizing $N$-body resimulations with up to $10^7$ particles, we
demonstrate that interactions between NSCs and their surrounding galactic
environment, particularly tidal forces triggered by cluster interactions,
significantly accelerate the sinking of MBHs to the galactic center. This
process leads to the formation of a hard binary in $\lesssim 500$ Myr after the
onset of a galaxy merger. Our results show that in 8 out of 12 models, the high
stellar density of the surrounding NSCs enhances MBH hardening, facilitating
gravitational wave (GW) mergers by redshift $z = 4$. We conclude that at $z >
4$, dense NSCs serve as the dominant channel for MBH seed mergers, producing a
merger rate of $0.3$--$0.6\, \mathrm{yr}^{-1}$ at $z = 4$, which is
approximately 300--600 times higher than in non-NSC environments. In contrast,
in environments without NSCs, surrounding dark matter plays a more significant
role in loss-cone scattering. |
---|---|
DOI: | 10.48550/arxiv.2409.19095 |