2010MNRAS.407.1098A


Query : 2010MNRAS.407.1098A

2010MNRAS.407.1098A - Mon. Not. R. Astron. Soc., 407, 1098-1107 (2010/September-2)

The early dynamical evolution of cool, clumpy star clusters.

ALLISON R.J., GOODWIN S.P., PARKER R.J., PORTEGIES ZWART S.F. and DE GRIJS R.

Abstract (from CDS):

Observations and theory both suggest that star clusters form subvirial (cool) with highly substructured distributions. We perform a large ensemble of N-body simulations of moderate-sized (N = 1000) cool, fractal clusters to investigate their early dynamical evolution. We find that cool, clumpy clusters dynamically mass segregate on a short time-scale, that Trapezium-like massive higher order multiples are commonly formed, and that massive stars are often ejected from clusters with velocities >10 km/s (cf. the average escape velocity of 2.5 km/s). The properties of clusters also change rapidly on very short time-scales. Young clusters may also undergo core collapse events, in which a dense core containing massive stars is hardened due to energy losses to a halo of lower mass stars. Such events can blow young clusters apart with no need for gas expulsion. The warmer and less substructured a cluster is initially, the less extreme its evolution.

Abstract Copyright: © 2010 The Authors. Journal compilation © 2010 RAS

Journal keyword(s): stars: formation - stars: kinematics and dynamics

Simbad objects: 9

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Number of rows : 9
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 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
2 NGC 1893 OpC 05 22 52.8 +33 26 32           ~ 270 0
3 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
4 Cl Stock 8 OpC 05 27 54.1 +34 28 41           ~ 93 0
5 NAME Orion Nebula Cluster OpC 05 35.0 -05 29           ~ 2514 0
6 NAME Ori Trapezium OpC 05 35 16.5 -05 23 14           ~ 1708 1
7 Cl Trumpler 14 OpC 10 43 56.0 -59 33 07   5.70 5.5     ~ 547 0
8 NGC 3603 OpC 11 14 57.9 -61 14 32           ~ 1136 1
9 NGC 6231 OpC 16 54 14.4 -41 48 53           ~ 562 0

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