2008MNRAS.386...65M


Query : 2008MNRAS.386...65M

2008MNRAS.386...65M - Mon. Not. R. Astron. Soc., 386, 65-95 (2008/May-1)

Black holes and core expansion in massive star clusters.

MacKEY A.D., WILKINSON M.I., DAVIES M.B. and GILMORE G.F.

Abstract (from CDS):

In this study we present the results from realistic N-body modelling of massive star clusters in the Magellanic Clouds. We have computed eight simulations with N ∼ 105 particles; six of these were evolved for at least a Hubble time. The aim of this modelling is to examine in detail the possibility of large-scale core expansion in massive star clusters, and search for a viable dynamical origin for the radius-age trend observed for such objects in the Magellanic Clouds. We identify two physical processes which can lead to significant and prolonged cluster core expansion - mass-loss due to rapid stellar evolution in a primordially mass-segregated cluster, and heating due to a retained population of stellar mass black holes, formed in the supernova explosions of the most massive cluster stars. These two processes operate over different time-scales and during different periods of a cluster's life. The former occurs only at early times and cannot drive core expansion for longer than a few hundred Myr, while the latter typically does not begin until several hundred Myr have passed, but can result in core expansion lasting for many Gyr. We investigate the behaviour of each of these expansion mechanisms under different circumstances - in clusters with varying degrees of primordial mass segregation, and in clusters with varying black hole retention fractions. In combination, the two processes can lead to a wide variety of evolutionary paths on the radius-age plane, which fully cover the observed cluster distribution and hence define a dynamical origin for the radius-age trend in the Magellanic Clouds. We discuss in some detail the implications of core expansion for various aspects of globular cluster research, as well as the possibility of observationally inferring the presence of a significant population of stellar mass black holes in a cluster.

Abstract Copyright: ©2008 The Authors. Journal compilation © 2008 RAS

Journal keyword(s): stellar dynamics - methods: {em N}-body simulations - globular clusters: general - Magellanic Clouds

Simbad objects: 25

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Number of rows : 25
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 Lindsay 1 Cl* 00 03 53.50 -73 28 15.0   11.7       ~ 125 0
2 M 31 AGN 00 42 44.330 +41 16 07.50 4.86 4.36 3.44     ~ 13622 1
3 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
4 NGC 330 Cl* 00 56 18.55 -72 27 45.1 9.37 9.76 9.55   8.89 ~ 445 0
5 NGC 339 OpC 00 57 47.62 -74 28 14.6 13.23 12.94 12.21   11.20 ~ 157 0
6 [BS95] 90 Cl* 00 59 07.25 -72 08 59.1 12.94 13.01 12.25   11.88 ~ 31 0
7 Cl Lindsay 113 Cl* 01 49 30.0 -73 43 40   11.9       ~ 97 0
8 NAME Fornax H1 Cl* 02 37 02.1 -34 11 00     16.59     ~ 107 0
9 MCG-06-07-001 G 02 39 59.3 -34 26 57   9.02 7.4     ~ 1894 1
10 NAME Magellanic Clouds GrG 03 00 -71.0           ~ 7988 0
11 NAME Ret GlC 04 36 10.15 -58 51 34.8   14.00 14.25 13.50   ~ 177 1
12 NGC 1841 GlC 04 45 24.38 -83 59 53.3   12.23 11.43     ~ 190 0
13 HD 268850 AB* 05 02 21.4730341272 -66 06 38.294439372   11.83 11.55 12.43   ~ 89 0
14 NGC 1805 GlC 05 02 21.690 -66 06 39.43           ~ 115 0
15 NGC 1818 GlC 05 04 13.300 -66 26 05.47           ~ 279 0
16 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
17 NGC 2005 Cl* 05 30 08.500 -69 45 14.42   12.30 11.57     ~ 103 0
18 NGC 2019 Cl* 05 31 56.48 -70 09 32.5   10.9 10.86     ~ 124 0
19 NAME Orion Nebula Cluster OpC 05 35.0 -05 29           ~ 2514 0
20 RMC 136 Cl* 05 38 42.396 -69 06 03.36   5.81 5.40     ~ 2236 2
21 Z 251-4 AG? 16 16 17.9000468088 +47 02 43.128874644   14.9       ~ 151 0
22 NAME Arches Cluster Cl* 17 45 50.5 -28 49 28           ~ 792 0
23 NAME Quintuplet Cluster OpC 17 46 13.9 -28 49 48           ~ 561 0
24 NAME SDG G 18 55 19.0 -30 32 43   4.5 3.6     ~ 2438 2
25 Cl Terzan 8 GlC 19 41 44.41 -33 59 58.1     11.54     ~ 357 0

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