1999AJ....117.1792D


Query : 1999AJ....117.1792D

1999AJ....117.1792D - Astron. J., 117, 1792-1815 (1999/April-0)

Space velocities of globular clusters. III. Cluster orbits and halo substructure.

DINESCU D.I., GIRARD T.M. and VAN ALTENA W.F.

Abstract (from CDS):

We have compiled a catalog of absolute proper motions of globular clusters from various sources. The sample consists of 38 clusters, from which most of the southern ones (15 clusters) were measured in our previous papers in this series. We have integrated orbits assuming two different Galactic potential models adopted from the literature and have calculated orbital parameters. The uncertainties associated with the orbital parameters were derived in a Monte Carlo approach, and we conclude that, overall, at the present level of measurement errors, orbital differences due to Galactic potential models are not significant.

Three metal-poor clusters are found to have orbits similar to prototypical metal-rich disk clusters. These clusters are NGC 6254 (M10), NGC 6626 (M28), and NGC 6752. We interpret this as a potentially significant constraint on the formation of the disk. It is thus possible that part of the inner metal-poor halo is the low-metallicity tail of the thick disk. In this case, the ages of these clusters indicate that the formation of the disk partially overlapped with that of the halo. The clusters classified as ``young halo'' or ``red horizontal-branch'' by Zinn show a radially anisotropic velocity distribution, their orbits are of high total energy, with apocentric radii larger than 10 kpc and highly eccentric. In this sense they may represent an accreted component of our Galaxy. We also discuss ω Cen's orbit characteristics in the view of an accreted origin.

We investigate the effect of the orbital motion on the internal dynamics of clusters. Adopting the formalism from Gnedin & Ostriker and their destruction rates due to two-body relaxation, we find that, in most cases, this internal process is more important than the destruction processes due to disk and bulge shocking. Hubble Space Telescope (HST) observations argue that NGC 6397's luminosity function is depleted at the faint end, and this is blamed on its high total destruction rate. We propose a list of clusters with similar destruction rates that may also have depleted luminosity functions. We also note the bias toward deriving higher destruction rates in studies that statistically assign tangential velocities based on a kinematic model of the globular cluster system, in contrast to the rates derived from the measured tangential velocities. Clusters prone to such biases are those that have circular orbits (kinematically thick-disk clusters) and some of those with orbits of high total energy.


Abstract Copyright:

Journal keyword(s): Galaxy: Halo - Galaxy: Structure - Galaxy: Globular Clusters: General

Simbad objects: 45

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Number of rows : 45
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 NGC 104 GlC 00 24 05.359 -72 04 53.20     4.09     ~ 3917 0
2 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 11152 1
3 NGC 288 GlC 00 52 45.24 -26 34 57.4   10 8.13     ~ 1042 0
4 NGC 362 GlC 01 03 14.26 -70 50 55.6     6.58     ~ 1085 0
5 NGC 1851 GlC 05 14 06.76 -40 02 47.6           ~ 1430 0
6 M 79 GlC 05 24 10.59 -24 31 27.3     8.16     ~ 817 0
7 NGC 2298 GlC 06 48 59.41 -36 00 19.1     8.89     ~ 497 0
8 NAME Sextans C GlC 10 05 30.96 +00 04 15.4   15.5 13.9     ~ 328 1
9 NGC 4147 GlC 12 10 06.149 +18 32 31.78   11.45 10.74     ~ 573 0
10 M 68 GlC 12 39 27.98 -26 44 38.6     7.96     ~ 997 0
11 M 53 GlC 13 12 55.25 +18 10 05.4     7.79     ~ 836 0
12 NGC 5139 GlC 13 26 47.28 -47 28 46.1           ~ 3427 0
13 M 3 GlC 13 42 11.62 +28 22 38.2     6.39     ~ 2479 0
14 NGC 5466 GlC 14 05 27.29 +28 32 04.0     9.70     ~ 828 0
15 NAME Serpens Dwarf GlC 15 16 05.30 -00 06 41.0   15.1       ~ 734 1
16 NGC 5897 GlC 15 17 24.40 -21 00 36.4   10.16 8.52     ~ 389 0
17 M 5 GlC 15 18 33.22 +02 04 51.7     5.95     ~ 1978 0
18 M 80 GlC 16 17 02.41 -22 58 33.9           ~ 716 0
19 M 4 GlC 16 23 35.22 -26 31 32.7           ~ 1850 0
20 NGC 6144 GlC 16 27 13.86 -26 01 24.6           ~ 243 0
21 M 107 GlC 16 32 31.86 -13 03 13.6           ~ 786 0
22 M 13 GlC 16 41 41.634 +36 27 40.75     5.8     ~ 2193 0
23 M 12 GlC 16 47 14.18 -01 56 54.7     6.07     ~ 677 0
24 M 10 GlC 16 57 09.05 -04 06 01.1     4.98     ~ 789 0
25 M 92 GlC 17 17 07.39 +43 08 09.4     6.52     ~ 2116 0
26 NGC 6362 GlC 17 31 54.99 -67 02 54.0           ~ 585 0
27 NGC 6397 GlC 17 40 42.09 -53 40 27.6     5.17     ~ 1976 0
28 NAME Galactic Center reg 17 45 39.60213 -29 00 22.0000           ~ 14420 0
29 NGC 6584 GlC 18 18 37.60 -52 12 56.8     8.17     ~ 288 0
30 M 28 GlC 18 24 32.89 -24 52 11.4           ~ 770 0
31 M 22 GlC 18 36 23.94 -23 54 17.1           ~ 1379 0
32 NGC 6712 GlC 18 53 04.32 -08 42 21.5           ~ 519 0
33 M 54 GlC 18 55 03.33 -30 28 47.5           ~ 1069 0
34 NAME SDG G 18 55 19.0 -30 32 43   4.5 3.6     ~ 2189 2
35 NGC 6752 GlC 19 10 52.11 -59 59 04.4           ~ 2001 0
36 M 56 GlC 19 16 35.57 +30 11 00.5           ~ 422 0
37 Cl Terzan 7 GlC 19 17 43.92 -34 39 27.8           ~ 428 0
38 Cl Arp 2 GlC 19 28 44.11 -30 21 20.3     12.41     ~ 354 0
39 M 55 GlC 19 39 59.71 -30 57 53.1     6.49     ~ 854 0
40 Cl Terzan 8 GlC 19 41 44.41 -33 59 58.1     11.54     ~ 321 0
41 M 71 GlC 19 53 46.49 +18 46 45.1           ~ 1128 0
42 NGC 6934 GlC 20 34 11.37 +07 24 16.1           ~ 422 0
43 M 15 GlC 21 29 58.33 +12 10 01.2           ~ 3140 0
44 M 2 GlC 21 33 27.02 -00 49 23.7     6.25     ~ 1030 1
45 M 30 GlC 21 40 22.12 -23 10 47.5     7.10     ~ 1049 0

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