2012MNRAS.426..601C


Query : 2012MNRAS.426..601C

2012MNRAS.426..601C - Mon. Not. R. Astron. Soc., 426, 601-613 (2012/October-2)

The mass distribution of the Fornax dSph: constraints from its globular cluster distribution.

COLE D.R., DEHNEN W., READ J.I. and WILKINSON M.I.

Abstract (from CDS):

Uniquely among the dwarf spheroidal (dSph) satellite galaxies of the Milky Way, Fornax hosts globular clusters. It remains a puzzle as to why dynamical friction has not yet dragged any of Fornax's five globular clusters to the centre, and also why there is no evidence that any similar star cluster has been in the past (for Fornax or any other tidally undisrupted dSph). We set up a suite of 2800 N-body simulations that sample the full range of globular cluster orbits and mass models consistent with all existing observational constraints for Fornax. In agreement with previous work, we find that if Fornax has a large dark matter core, then its globular clusters remain close to their currently observed locations for long times. Furthermore, we find previously unreported behaviour for clusters that start inside the core region. These are pushed out of the core and gain orbital energy, a process we call `dynamical buoyancy'. Thus, a cored mass distribution in Fornax will naturally lead to a shell-like globular cluster distribution near the core radius, independent of the initial conditions. By contrast, cold dark matter-type cusped mass distributions lead to the rapid infall of at least one cluster within Δt = 1–2Gyr, except when picking unlikely initial conditions for the cluster orbits ( ∼ 2 per cent probability), and almost all clusters within Δt = 10Gyr. Alternatively, if Fornax has only a weakly cusped mass distribution, then dynamical friction is much reduced. While over Δt = 10Gyr this still leads to the infall of one to four clusters from their present orbits, the infall of any cluster within Δt = 1–2Gyr is much less likely (with probability 0–70 per cent, depending on Δt and the strength of the cusp). Such a solution to the timing problem requires (in addition to a shallow dark matter cusp) that in the past the globular clusters were somewhat further from Fornax than today; they most likely did not form within Fornax, but were accreted.

Abstract Copyright: © 2012 The Authors Monthly Notices of the Royal Astronomical Society © 2012 RAS

Journal keyword(s): galaxies: haloes - galaxies: kinematics and dynamics - galaxies: structure

Simbad objects: 11

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Number of rows : 11
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 Sculptor Dwarf Galaxy G 01 00 09.4 -33 42 32   9.79 8.6 8.81   ~ 1498 4
2 NAME Fornax H1 Cl* 02 37 02.1 -34 11 00     16.59     ~ 107 0
3 NAME Fornax H2 GlC 02 38 44.24 -34 48 30.5   14.5       ~ 93 0
4 NAME Fornax H3 GlC 02 39 48.16 -34 15 28.6   13.59       ~ 131 0
5 MCG-06-07-001 G 02 39 59.3 -34 26 57   9.02 7.4     ~ 1894 1
6 NAME Fornax H4 GlC 02 40 07.697 -34 32 10.59   15.18 13.91 14.08   ~ 112 0
7 NAME Fornax H5 GlC 02 42 21.111 -34 06 05.80   14.5       ~ 101 0
8 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
9 Z 318-18 G 15 09 08.0 +67 13 21   13.60 10.6     ~ 1459 0
10 M 54 GlC 18 55 03.33 -30 28 47.5           ~ 1164 0
11 NAME SDG G 18 55 19.0 -30 32 43   4.5 3.6     ~ 2438 2

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