2017MNRAS.468.1453D


Query : 2017MNRAS.468.1453D

2017MNRAS.468.1453D - Mon. Not. R. Astron. Soc., 468, 1453-1473 (2017/June-3)

An approximate analytic model of a star cluster with potential escapers.

DANIEL K.J., HEGGIE D.C. and VARRI A.L.

Abstract (from CDS):

In the context of a star cluster moving on a circular galactic orbit, a 'potential escaper' is a cluster star that has orbital energy greater than the escape energy, and yet is confined within the Jacobi radius of the stellar system. On the other hand, analytic models of stellar clusters typically have a truncation energy equal to the cluster escape energy, and therefore explicitly exclude these energetically unbound stars. Starting from the landmark analysis performed by Henon of periodic orbits of the circular Hill equations, we present a numerical exploration of the population of 'non-escapers', defined here as those stars that remain within two Jacobi radii for several galactic periods, with energy above the escape energy. We show that they can be characterized by the Jacobi integral and two further approximate integrals, which are based on perturbation theory and ideas drawn from Lidov-Kozai theory. Finally, we use these results to construct an approximate analytic model that includes a phase-space description of a population resembling that of potential escapers, in addition to the usual bound population.

Abstract Copyright: © 2017 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society

Journal keyword(s): methods: analytical - galaxies: star clusters: general - galaxies: star clusters: general

Simbad objects: 6

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Number of rows : 6
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 M 31 AGN 00 42 44.330 +41 16 07.50 4.86 4.36 3.44     ~ 13622 1
2 NAME Centaurus A BLL 13 25 27.61521044 -43 01 08.8050291   8.18 6.84 6.66   ~ 4774 3
3 NGC 5139 GlC 13 26 47.28 -47 28 46.1           ~ 3677 0
4 NGC 5694 GlC 14 39 36.52 -26 32 18.0           ~ 323 0
5 M 92 GlC 17 17 07.39 +43 08 09.4     6.52     ~ 2240 0
6 M 15 GlC 21 29 58.33 +12 10 01.2           ~ 3274 0

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