2025MNRAS.539...45S


Query : 2025MNRAS.539...45S

2025MNRAS.539...45S - Mon. Not. R. Astron. Soc., 539, 45-68 (2025/May-1)

The role of massive black holes in merging star clusters: dynamical evolution, stellar and compact object ejections, and gravitational waves.

SOUVAITZIS L., RANTALA A. and NAAB T.

Abstract (from CDS):

Star clusters can interact and merge in galactic discs, haloes, or centres. We present direct N-body simulations of binary mergers of star clusters with $M_{\star } = 2.7 \times 10^4 \, \mathrm{M_{\odot }}$ each, using the N-body code BIFROST with subsystem regularization and post-Newtonian dynamics. We include 500 $\mathrm{M_{\odot }}$ massive black holes (MBHs) in the progenitors to investigate their impact on remnant evolution. The MBHs form hard binaries interacting with stars and stellar black holes (BHs). A few Myr after the cluster merger, this produces sizable populations of runaway stars ($\sim$800 with $v_{\mathrm{ej}} \gtrsim 50 \, \mathrm{km\, s^{-1}}$) and stellar BHs ($\sim$30) escaping within 100 Myr. The remnants lose $\sim 30{{\ \rm per\ cent}}$ of their BH population and $\sim 3{{\ \rm per\ cent}}$ of their stars, with $\sim$30 stars accelerated to high velocities $\gtrsim 300 \, \mathrm{km\, s^{-1}}$. Comparison simulations of isolated clusters with central hard MBH binaries and cluster mergers without MBHs show that the process is driven by MBH binaries, while those with a single 1000 $\mathrm{M_{\odot }}$ MBH in isolated or merging clusters produce fewer runaway stars at lower velocities. Low-eccentricity merger orbits yield rotating remnants ($v_{\mathrm{rot}} \sim 3 \, \mathrm{km\, s^{-1}}$), but probing the presence of MBHs via kinematics alone remains challenging. We expect the binary MBHs to merge within a Hubble time, producing observable gravitational-wave (GW) events detectable by future GW detectors such as the Einstein Telescope and Laser Interferometer Space Antenna. The results suggest that interactions with low-mass MBH binaries formed in merging star clusters are an important additional channel for producing runaway and high-velocity stars, free-floating stellar BHs, and compact objects.

Abstract Copyright: © 2025 The Author(s). Published by Oxford University Press on behalf of Royal Astronomical Society.

Journal keyword(s): stars: black holes - stars: kinematics and dynamics - galaxies: star clusters: general - black hole physics - gravitational waves - methods: numerical

Simbad objects: 14

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Number of rows : 14
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 NGC 104 GlC 00 24 05.359 -72 04 53.20     4.09     ~ 4158 0
2 Bol 23 GlC 00 41 01.151 +41 13 45.41 16.040 15.400 14.17 13.560 12.570 ~ 98 0
3 M 31 AGN 00 42 44.330 +41 16 07.50 4.86 4.36 3.44     ~ 13622 1
4 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
5 Gaia DR3 898707303799931392 HV* 07 31 27.2676683432 +37 17 04.354368492           ~ 1 0
6 UCAC4 154-126202 SB* 13 50 16.7477601784 -59 14 20.330701044   13.995 12.711 12.366   ~ 58 0
7 GALEX J172841.0-003451 SB* 17 28 41.0966126056 -00 34 51.523377959       13.977   ~ 64 0
8 NGC 6388 GlC 17 36 17.461 -44 44 08.34           ~ 988 1
9 NGC 6397 GlC 17 40 42.09 -53 40 27.6     5.17     ~ 2103 0
10 NAME Galactic Center reg 17 45 39.60213 -29 00 22.0000           ~ 16269 0
11 NAME Sgr A* X 17 45 40.03599 -29 00 28.1699           ~ 4970 3
12 LS II +14 13 SB? 19 39 18.7115474496 +14 55 54.010991712   11.9   10.9   B 61 0
13 M 15 GlC 21 29 58.33 +12 10 01.2           ~ 3274 0
14 GrW 190521 GWE ~ ~           ~ 409 0

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