Issue |
A&A
Volume 397, Number 3, January III 2003
|
|
---|---|---|
Page(s) | 899 - 911 | |
Section | Galactic structure, stellar clusters, and populations | |
DOI | https://doi.org/10.1051/0004-6361:20021499 | |
Published online | 21 January 2003 |
The mass of the Milky Way: Limits from a newly assembled set of halo objects*
1
Department of Astronomical Science, The Graduate University for Advanced Studies, Mitaka, Tokyo 181-8588, Japan
2
National Astronomical Observatory, Mitaka, Tokyo 181-8588, Japan
3
Department of Physics & Astronomy, Michigan State University, East Lansing, MI 48824, USA
Corresponding author: T. Sakamoto, sakamoto@pluto.mtk.nao.ac.jp
Received:
7
August
2002
Accepted:
14
October
2002
We set new limits on the mass of the Milky Way, making use of the latest
kinematic information for Galactic satellites and halo objects. Our sample
consists of 11 satellite galaxies, 137 globular clusters, and 413 field
horizontal-branch (FHB) stars up to distances of 10 kpc from the Sun. Roughly
half of the objects in this sample have measured proper motions, permitting the
use of their full space motions in our analysis. In order to bind these sample
objects to the Galaxy, their rest-frame velocities must be lower than their
escape velocities at their estimated distances. This constraint enables us to
show that the mass estimate of the Galaxy is largely affected by several
high-velocity objects (Leo I, Pal 3, Draco, and a few FHB stars), not by
a single object alone (such as Leo I), as has often been the case in past
analyses. We also find that a gravitational potential that gives rise to a
declining rotation curve is insufficient to bind many of our sample objects to
the Galaxy; a possible lower limit on the mass of the Galaxy is about
. To be more quantitative, we adopt a Bayesian
likelihood approach to reproduce the observed distribution of the current
positions and motions of the sample, in a prescribed Galactic potential that
yields a flat rotation curve. This method enables a search for the most likely
total mass of the Galaxy, without undue influence in the final result arising
from the presence or absence of Leo I, provided that both radial velocities and
proper motions are used. Although the best mass estimate depends somewhat on
the model assumptions, such as the unknown prior probabilities for the model
parameters, the resultant systematic change in the mass estimate is confined to
a relatively narrow range of a few times
, owing to our
consideration of many FHB stars. The most likely total mass derived from this
method is
(including Leo I), and
(excluding Leo I). The
derived mass estimate of the Galaxy within the distance to the Large Magellanic
Cloud (∼50 kpc) is essentially independent of the model parameters,
yielding
(including Leo I) and
(excluding Leo I). Implications
for the origin of halo microlensing events (e.g., the possibility of brown
dwarfs as the origin of the microlensing events toward the LMC, may be excluded
by our lower mass limit) and prospects for more accurate estimates of the total
mass are also discussed.
Key words: Galaxy: halo / Galaxy: fundamental parameters / Galaxy: kinematics and dynamics / stars: horizontal-branch
© ESO, 2003
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