70 research outputs found
Gamma-Rays from Dark Matter Mini-Spikes in M31
The existence of a population of wandering Intermediate Mass Black Holes
(IMBHs) is a generic prediction of scenarios that seek to explain the formation
of Supermassive Black Holes in terms of growth from massive seeds. The growth
of IMBHs may lead to the formation of DM overdensities called "mini-spikes",
recently proposed as ideal targets for indirect DM searches. Current
ground-based gamma-ray experiments, however, cannot search for these objects
due to their limited field of view, and it might be challenging to discriminate
mini-spikes in the Milky Way from the many astrophysical sources that GLAST is
expected to observe. We show here that gamma-ray experiments can effectively
search for IMBHs in the nearby Andromeda galaxy (also known as M31), where
mini-spikes would appear as a distribution of point-sources, isotropically
distributed in a \thickapprox 3^{\circ} circle around the galactic center. For
a neutralino-like DM candidate with a mass m_{\chi}=150 GeV, up to 20 sources
would be detected with GLAST (at 5\sigma, in 2 months). With Air Cherenkov
Telescopes such as MAGIC and VERITAS, up to 10 sources might be detected,
provided that the mass of neutralino is in the TeV range or above.Comment: 9 pages, 5 figure
Darwin Tames an Andromeda Dwarf: Unraveling the Orbit of NGC 205 Using a Genetic Algorithm
NGC 205, a close satellite of the M31 galaxy, is our nearest example of a
dwarf elliptical galaxy. Photometric and kinematic observations suggest that
NGC 205 is undergoing tidal distortion from its interaction with M31. Despite
earlier attempts, the orbit and progenitor properties of NGC 205 are not well
known. We perform an optimized search for these unknowns by combining a genetic
algorithm with restricted N-body simulations of the interaction. This approach,
coupled with photometric and kinematic observations as constraints, allows for
an effective exploration of the parameter space. We represent NGC 205 as a
static Hernquist potential with embedded massless test particles that serve as
tracers of surface brightness. We explore 3 distinct, initially stable
configurations of test particles: cold rotating disk, warm rotating disk, and
hot, pressure-supported spheroid. Each model reproduces some, but not all, of
the observed features of NGC 205, leading us to speculate that a rotating
progenitor with substantial pressure support could match all of the
observables. Furthermore, plausible combinations of mass and scale length for
the pressure-supported spheroid progenitor model reproduce the observed
velocity dispersion profile. For all 3 models, orbits that best match the
observables place the satellite 11+/-9 kpc behind M31 moving at very large
velocities: 300-500 km/s on primarily radial orbits. Given that the observed
radial component is only 54 km/s, this implies a large tangential motion for
NGC 205, moving from the NW to the SE. These results suggest NGC 205 is not
associated with the stellar arc observed to the NE of NGC 205. Furthermore, NGC
205's velocity appears to be near or greater than its escape velocity,
signifying that the satellite is likely on its first M31 passage.Comment: 34 pages, 20 figures, accepted for publication in the Astrophysical
Journal, A pdf version with high-resolution figures may be obtained from
http://www.ucolick.org/~kirsten/ms.pd
Investigating the Andromeda Stream: II. Orbital Fits and Properties of the Progenitor
We construct test-particle orbits and simple N-body models that match the
properties of the giant stellar stream observed to the south of M31, using the
model of M31's potential derived in the companion paper by Geehan et al.
(2006). We introduce a simple approximation to account for the difference in
position between the stream and the orbit of the progenitor; this significantly
affects the best-fitting orbits. The progenitor orbits we derive have orbital
apocenter \sim 60 \kpc and pericenter \sim 3 \kpc, though these quantities
vary somewhat with the current orbital phase of the progenitor which is as yet
unknown. Our best combined fit to the stream and galaxy properties implies a
mass within 125 kpc of M31 of (7.4 \pm 1.2) \times 10^{11} \Msun. Based on
its length, width, luminosity, and velocity dispersion, we conclude that the
stream originates from a progenitor satellite with mass M_s \sim 10^9 \Msun,
and at most modest amounts of dark matter; the estimate of is again
correlated with the phase of the progenitor. M31 displays a large number of
faint features in its inner halo which may be progenitors or continuations of
the stream. While the orbital fits are not constrained enough for us to
conclusively identify the progenitor, we can identify several plausible
candidates, of which a feature in the planetary nebula distribution found by
Merrett et al. is the most plausible, and rule out several others. We make
predictions for the kinematic properties of the successful candidates. These
may aid in observational identification of the progenitor object, which would
greatly constrain the allowed models of the stream.Comment: 17 pages, 10 color figures, 4 tables. Accepted by Monthly Notices;
some minor revisions and corrected typo
The Once and Future Andromeda Stream
The interaction between an accreting satellite and the Andromeda galaxy (M31)
has been studied analytically and numerically, using a high-resolution N-body
simulation with particles. For the first time, we show the
self-gravitating response of the disk, the bulge, and the dark matter halo of
M31 to an accreting satellite. We reproduce the Stream and the shells at the
East and West side of M31, by following the evolution of the collision 4 Gyr
into the future, and show that recently discovered diffuse arcs on the south
side of the minor axis are the remnants of a similar collision that occurred
3-4 Gyr earlier than the Stream event. The present day integrity of the M31
disk constrains the satellite mass to be . The
stars that were originally in the center of the satellite are now in the east
shell. Therefore, observations in this region might reveal additional clues
about the nature of satellite, such as the central core and any metallicity
gradient.Comment: 5 pages, 4 figures, accepted for publication in ApJL; see
http://www.isc.senshu-u.ac.jp/~thj0613/M31/M31.html for high-resolution
figures and movi
Strangers in the night: Discovery of a dwarf spheroidal galaxy on its first Local Group infall
We present spectroscopic observations of the AndXII dwarf spheroidal galaxy
using DEIMOS/Keck-II, showing it to be moving rapidly through the Local Group
(-556 km/s heliocentric velocity, -281 km/s relative to Andromeda from the MW),
falling into the Local Group from ~115 kpc beyond Andromeda's nucleus. AndXII
therefore represents a dwarf galaxy plausibly falling into the Local Group for
the first time, and never having experienced a dense galactic environment. From
Green Bank Telescope observations, a limit on the H{I} gas mass of <3000 Msun
suggests that AndXII's gas could have been removed prior to experiencing the
tides of the Local Group galaxies. Orbit models suggest the dwarf is close to
the escape velocity of M31 for published mass models. AndXII is our best direct
evidence for the late infall of satellite galaxies, a prediction of
cosmological simulations.Comment: 4 pages 5 figures 1 table, accepted in ApJ, july issu
Tracing Galaxy Formation with Stellar Halos II: Relating Substructure in Phase- and Abundance-Space to Accretion Histories
This paper explores the mapping between the observable properties of a
stellar halo in phase- and abundance-space and the parent galaxy's accretion
history in terms of the characteristic epoch of accretion and mass and orbits
of progenitor objects. The study utilizes a suite of eleven stellar halo models
constructed within the context of a standard LCDM cosmology. The results
demonstrate that coordinate-space studies are sensitive to the recent (0-8
Gyears ago) merger histories of galaxies (this timescale corresponds to the
last few to tens of percent of mass accretion for a Milky-Way-type galaxy).
Specifically, the {\it frequency, sky coverage} and {\it fraction of stars} in
substructures in the stellar halo as a function of surface brightness are
indicators of the importance of recent merging and of the luminosity function
of infalling dwarfs. The {\it morphology} of features serves as a guide to the
orbital distribution of those dwarfs. Constraints on the earlier merger history
(> 8 Gyears ago) can be gleaned from the abundance patterns in halo stars:
within our models, dramatic differences in the dominant epoch of accretion or
luminosity function of progenitor objects leave clear signatures in the
[alpha/Fe] and [Fe/H] distributions of the stellar halo - halos dominated by
very early accretion have higher average [alpha/Fe], while those dominated by
high luminosity satellites have higher [Fe/H]. This intuition can be applied to
reconstruct much about the merger histories of nearby galaxies from current and
future data sets.Comment: 21 pages, 20 figures. To appear in the Astrophysical Journa
A kinematically selected, metal-poor stellar halo in the outskirts of M31
We present evidence for a metal-poor, [Fe/H] =0.2 dex,
stellar halo component detectable at radii from 10 kpc to 70 kpc, in our
nearest giant spiral neighbor, the Andromeda galaxy. This metal-poor sample
underlies the recently-discovered extended rotating component, and has no
detected metallicity gradient. This discovery uses a large sample of 9861
radial velocities of Red Giant Branch (RGB) stars obtained with the Keck-II
telescope and DEIMOS spectrograph, with 827 stars with robust radial velocity
measurements isolated kinematically to lie in the halo component primarily by
windowing out the extended rotating component which dominates the photometric
profile of Andromeda out to 50 kpc (de-projected). The stars lie in 54
spectroscopic fields spread over an 8 square degree region, and are expected to
fairly sample the halo to a radius of 70 kpc. The halo sample shows no
significant evidence for rotation. Fitting a simple model in which the velocity
dispersion of the component decreases with radius, we find a central velocity
dispersion of 152\kms decreasing by -0.90\kms/\kpc. By fitting a
cosmologically-motivated NFW halo model to the halo stars we constrain the
virial mass of M31 to be greater than 9.0 \times 10^{11} \msun with 99%
confidence. The properties of this halo component are very similar to that
found in our Milky Way, revealing that these roughly equal mass galaxies may
have led similar accretion and evolutionary paths in the early Universe.Comment: 13 pages, 12 figures, accepted in ApJ. substantially revised versio
The Flattened Dark Matter Halo of M31 as Deduced from the Observed HI Scale Heights
In this paper, we use the outer-galactic HI scale height data as well as the
observed rotation curve as constraints to determine the halo density
distribution of the Andromeda galaxy (M31). We model the galaxy as a
gravitationally-coupled system of stars and gas, responding to the external
force-field of a known Hernquist bulge and the dark matter halo, the density
profile of the latter being characterized by four free parameters. The
parameter space of the halo is optimized so as to match the observed HI
thickness distribution as well as the rotation curve on an equal footing,
unlike the previous studies of M31 which were based on rotation curves alone.
We show that an oblate halo, with an isothermal density profile, provides the
best fit to the observed data. This gives a central density of 0.011 M_sun
/pc^3, a core radius of 21 kpc, and an axis ratio of 0.4. The main result from
this work is the flattened dark matter halo for M31, which is required to match
the outer galactic HI scale height data. Interestingly, such flattened halos
lie at the most oblate end of the distribution of halo shapes found in recent
cosmological simulations.Comment: 21 pages, 6 figures, accepted for publication in the Astrophysical
Journa
The Detailed Star Formation History in the Spheroid, Outer Disk, and Tidal Stream of the Andromeda Galaxy
Using the Advanced Camera for Surveys on the Hubble Space Telescope, we have
obtained deep optical images reaching stars well below the oldest main sequence
turnoff in the spheroid, tidal stream, and outer disk of the Andromeda Galaxy.
We have reconstructed the star formation history in these fields by comparing
their color-magnitude diagrams to a grid of isochrones calibrated to Galactic
globular clusters observed in the same bands. Each field exhibits an extended
star formation history, with many stars younger than 10 Gyr but few younger
than 4 Gyr. Considered together, the star counts, kinematics, and population
characteristics of the spheroid argue against some explanations for its
intermediate-age, metal-rich population, such as a significant contribution
from stars residing in the disk or a chance intersection with the stream's
orbit. Instead, it is likely that this population is intrinsic to the inner
spheroid, whose highly-disturbed structure is clearly distinct from the
pressure-supported metal-poor halo that dominates farther from the galaxy's
center. The stream and spheroid populations are similar, but not identical,
with the stream's mean age being ~1 Gyr younger; this similarity suggests that
the inner spheroid is largely polluted by material stripped from either the
stream's progenitor or similar objects. The disk population is considerably
younger and more metal-rich than the stream and spheroid populations, but not
as young as the thin disk population of the solar neighborhood; instead, the
outer disk of Andromeda is dominated by stars of age 4 - 8 Gyr, resembling the
Milky Way's thick disk. The disk data are inconsistent with a population
dominated by ages older than 10 Gyr, and in fact do not require any stars older
than 10 Gyr.Comment: Accepted for publication in The Astrophysical Journal. 29 pages, 23
figures (including 9 in color), latex. Updated for minor edits and additional
references. Images and CMDs are significantly smoothed and degraded in this
version; a version with high-quality figures is available at
http://www.stsci.edu/~tbrown/m31sfh/preprint.pd
Stellar Kinematics in the Complicated Inner Spheroid of M31: Discovery of Substructure Along the Southeastern Minor Axis and its Relationship to the Giant Southern Stream
We present the discovery of a kinematically-cold stellar population along the
SE minor axis of the Andromeda galaxy (M31) that is likely the forward
continuation of M31's giant southern stream. This discovery was made in the
course of an on-going spectroscopic survey of red giant branch (RGB) stars in
M31 using the DEIMOS instrument on the Keck II 10-m telescope. Stellar
kinematics are investigated in eight fields located 9-30 kpc from M31's center
(in projection). A likelihood method based on photometric and spectroscopic
diagnostics is used to isolate confirmed M31 RGB stars from foreground Milky
Way dwarf stars: for the first time, this is done without using radial velocity
as a selection criterion, allowing an unbiased study of M31's stellar
kinematics. The radial velocity distribution of the 1013 M31 RGB stars shows
evidence for the presence of two components. The broad (hot) component has a
velocity dispersion of 129 km/s and presumably represents M31's virialized
spheroid. A significant fraction (19%) of the population is in a narrow (cold)
component centered near M31's systemic velocity with a velocity dispersion that
decreases with increasing radial distance, from 55.5 km/s at R_proj=12 kpc to
10.6 km/s at R_proj=18 kpc. The spatial and velocity distribution of the cold
component matches that of the "Southeast shelf" predicted by the Fardal et al.
(2007) orbital model of the progenitor of the giant southern stream. The
metallicity distribution of the cold component matches that of the giant
southern stream, but is about 0.2 dex more metal rich on average than that of
the hot spheroidal component. We discuss the implications of our discovery on
the interpretation of the intermediate-age spheroid population found in this
region in recent ultra-deep HST imaging studies.Comment: 23 pages, 16 figures, 2 tables, accepted for publication in the
Astrophysical Journal. Changes from previous version: expanded discussion in
sections 4.2 and 7.2, removal of section 7.1.4 and associated figure
(discussion moved to section 7.1.2
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