2016MNRAS.459.3432M


Query : 2016MNRAS.459.3432M

2016MNRAS.459.3432M - Mon. Not. R. Astron. Soc., 459, 3432-3446 (2016/July-2)

Massive black hole binaries from runaway collisions: the impact of metallicity.

MAPELLI M.

Abstract (from CDS):

The runaway collision scenario is one of the most promising mechanisms to explain the formation of intermediate-mass black holes (IMBHs) in young dense star clusters. On the other hand, the massive stars that participate in the runaway collisions lose mass by stellar winds. In this paper, we discuss new N-body simulations of massive (6.5 x 104 M☉) star clusters, in which we added upgraded recipes for stellar winds and supernova explosion at different metallicity. We follow the evolution of the principal collision product (PCP), through dynamics and stellar evolution, till it forms a stellar remnant. At solar metallicity, the mass of the final merger product spans from few solar masses up to ∼30 M☉. At low metallicity (0.01-0.1 Z☉) the maximum remnant mass is ∼250 M☉, in the range of IMBHs. A large fraction (∼0.6) of the PCPs are not ejected from the parent star cluster and acquire stellar or black hole (BH) companions. Most of the long-lived binaries hosting a PCP are BH-BH binaries. We discuss the importance of this result for gravitational wave detection.

Abstract Copyright: © 2016 The Author Published by Oxford University Press on behalf of the Royal Astronomical Society

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

Simbad objects: 4

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Number of rows : 4
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 Cl Trumpler 14 OpC 10 43 56.0 -59 33 07   5.70 5.5     ~ 547 0
2 NAME Galactic Center reg 17 45 39.60213 -29 00 22.0000           ~ 16269 0
3 NAME Arches Cluster Cl* 17 45 50.5 -28 49 28           ~ 792 0
4 NAME Quintuplet Cluster OpC 17 46 13.9 -28 49 48           ~ 561 0

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