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<title>ADS (text="CLUSTERS" "GLOBULAR")</title>
<link>http://cdsads.u-strasbg.fr/cgi-bin/nph-abs_connect?cookie=43feeef94418859</link>
<description>The SAO/NASA ADS Abstract service provides a search system for the Astronomy and Physics literature</description>
<image>
<url>http://adsabs.harvard.edu/figs/newlogo.gif</url>
<title>SAO/NASA ADS</title>
<link>http://ads.harvard.edu</link>
<width>144</width>
<height>69</height>
</image>
<item>

<title>Valenti, E.: High-resolution near-infrared spectra of NGC 6624 and 6569</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.414.2690V</link>
<description>We present the first abundance analysis based on high-resolution
infrared (IR) echelle spectra of NGC 6569 and 6624, two moderately
reddened globular clusters located in the outer bulge of the Galaxy.

We find [Fe/H]=-0.79 ± 0.02 and -0.69 ± 0.02 dex for NGC
6569 and 6624, respectively, and an average α-element enhancement
of ≈+0.43 ± 0.02 and +0.39 ± 0.02 dex, consistent with
previous measurements on other metal-rich bulge clusters. We measure
accurate radial velocities of &#60;v&lt;SUB&gt;r&lt;/SUB&gt;&#62;=-47 ± 4 and
+51 ± 3 km s&lt;SUP&gt;-1&lt;/SUP&gt; and velocity dispersions of ≈8 and 6
km s&lt;SUP&gt;-1&lt;/SUP&gt; for NGC 6569 and 6624, respectively.

Finally, we find very low &lt;SUP&gt;12&lt;/SUP&gt;C/&lt;SUP&gt;13&lt;/SUP&gt;C isotopic ratio
(≤7 in NGC 6624 and ≈5 in NGC 6569), confirming the presence of
extramixing mechanisms during the red giant branch evolution phase. Data
presented herein were obtained at the W. M. Keck Observatory, which is
operated as a scientific partnership among the California Institute of
Technology, the University of California and the National Aeronautics
and Space Administration. The observatory was made possible for studies
by the generous support of the W. M. Keck Foundation.</description>
</item>


<item>

<title>van Dokkum, P. G.: Confirmation of Enhanced Dwarf-sensitive Absorption Features in the Spectra of Massive Elliptical Galaxies: Further Evidence for a Non-universal Initial Mass Function</title>
<link>http://cdsads.u-strasbg.fr/abs/2011ApJ...735L..13V</link>
<description>We recently found that massive cluster elliptical galaxies have strong
Na I λ8183, 8195 and FeH λ9916 Wing-Ford band absorption,
indicating the presence of a very large population of stars with masses
&#60;~ 0.3 M &lt;SUB&gt;sun&lt;/SUB&gt;. Here we test this result by comparing the
elliptical galaxy spectra to those of luminous globular clusters
associated with M31. These globular clusters have similar metallicities,
abundance ratios, and ages as massive elliptical galaxies but their low
dynamical mass-to-light ratios rule out steep stellar initial mass
functions (IMFs). From high-quality Keck spectra we find that the
dwarf-sensitive absorption lines in globular clusters are significantly
weaker than in elliptical galaxies and consistent with normal IMFs. The
differences in the Na I and Wing-Ford indices are 0.027 ± 0.007
mag and 0.017 ± 0.006 mag, respectively. We directly compare the
two classes of objects by subtracting the averaged globular cluster
spectrum from the averaged elliptical galaxy spectrum. The difference
spectrum is well fit by the difference between a stellar population
synthesis model with a bottom-heavy IMF and one with a bottom-light IMF.
We speculate that the slope of the IMF may vary with velocity
dispersion, although it is not yet clear what physical mechanism would
be responsible for such a relation.</description>
</item>


<item>

<title>Coomber, G.: The Unusual X-Ray Binaries of the Globular Cluster NGC 6652</title>
<link>http://cdsads.u-strasbg.fr/abs/2011ApJ...735...95C</link>
<description>Our 5 ks Chandra ACIS-S observation of the globular cluster NGC 6652
detected seven X-ray sources, three of which were previously
unidentified. This cluster hosts a well-known bright low-mass X-ray
binary, source A (or XB 1832–330). Source B shows unusual rapid
flaring variability, with an average L&lt;SUB&gt;X&lt;/SUB&gt; (0.5-10 keV) ~2
× 10&lt;SUP&gt;34&lt;/SUP&gt; erg s&lt;SUP&gt;–1&lt;/SUP&gt;, but with minutes-long
flares up to L&lt;SUB&gt;X&lt;/SUB&gt; = 9 × 10&lt;SUP&gt;34&lt;/SUP&gt; erg
s&lt;SUP&gt;–1&lt;/SUP&gt;. Its spectrum can be fit by an absorbed power law
of photon index Γ ~ 1.24 and hardens as the count rate decreases.
This suggests that part or all of the variation might be due to
obscuration by the rim of a highly inclined accretion disk. Sources C
and D, with L&lt;SUB&gt;X&lt;/SUB&gt; ~ 10&lt;SUP&gt;33&lt;/SUP&gt; erg s&lt;SUP&gt;–1&lt;/SUP&gt;,
have soft and unusual spectra. Source C requires a very soft component,
with a spectrum peaking at 0.5 keV, which might be the hot polar cap of
a magnetically accreting polar cataclysmic variable. Source D shows a
soft spectrum (fit by a power law of photon index ~2.3) with marginal
evidence for an emission line around 1 keV its nature is unclear. The
faint new sources E, F, and G have luminosities of 1-2 ×
10&lt;SUP&gt;32&lt;/SUP&gt; erg s&lt;SUP&gt;–1&lt;/SUP&gt;, if associated with the cluster
(which is likely). E and F have relatively hard spectra (consistent with
power laws with photon index ~1.5). G lacks soft photons, suggesting
absorption with N&lt;SUB&gt;H&lt;/SUB&gt; &#62; 10&lt;SUP&gt;22&lt;/SUP&gt;
cm&lt;SUP&gt;–2&lt;/SUP&gt;.</description>
</item>


<item>

<title>Colucci, J. E.: Globular Cluster Abundances from High-resolution, Integrated-light Spectroscopy. III. The Large Magellanic Cloud: Fe and Ages</title>
<link>http://cdsads.u-strasbg.fr/abs/2011ApJ...735...55C</link>
<description>In this paper, we refine our method for the abundance analysis of
high-resolution spectroscopy of the integrated light of unresolved
globular clusters (GCs). This method was previously demonstrated for the
analysis of old (&#62;10 Gyr) Milky Way (MW) GCs. Here, we extend the
technique to young clusters using a training set of nine GCs in the
Large Magellanic Cloud. Depending on the signal-to-noise ratio of the
data, we use 20-100 Fe lines per cluster to successfully constrain the
ages of old clusters to within a ~5 Gyr range, the ages of ~2 Gyr
clusters to a 1-2 Gyr range, and the ages of the youngest clusters
(0.05-1 Gyr) to a ~200 Myr range. We also demonstrate that we can
measure [Fe/H] in clusters with any age less than 12 Gyr with similar or
only slightly larger uncertainties (0.1-0.25 dex) than those obtained
for old MW GCs (0.1 dex) the slightly larger uncertainties are due to
the rapid evolution in stellar populations at these ages. In this paper,
we present only Fe abundances and ages. In the next paper in this
series, we present our complete analysis of ~20 elements for which we
are able to measure abundances. For several of the clusters in this
sample, there are no high-resolution abundances in the literature from
individual member stars; our results are the first detailed chemical
abundances available. The spectra used in this paper were obtained at
Las Campanas with the echelle on the du Pont Telescope and with the MIKE
spectrograph on the Magellan Clay Telescope.

This paper includes data gathered with the 6.5 m Magellan Telescopes
located at Las Campanas Observatory, Chile.</description>
</item>


<item>

<title>Naiman, J. P.: External Mass Accumulation onto Core Potentials: Implications for Star Clusters, Galaxies, and Galaxy Clusters</title>
<link>http://cdsads.u-strasbg.fr/abs/2011ApJ...735...25N</link>
<description>Accretion studies have been focused on the flow around bodies with point
mass gravitational potentials, but few general results are available for
non-point mass distributions. Here, we study the accretion flow onto
non-divergent, core potentials moving through a background medium. We
use Plummer and Hernquist potentials as examples to study gas accretion
onto star clusters, dwarf and large galaxy halos, and galaxy clusters in
a variety of astrophysical environments. The general conditions required
for a core potential to collectively accrete large quantities of gas
from the external medium are derived using both simulations and analytic
results. The consequences of large mass accumulation in galaxy nuclei,
dwarf galaxies, and star clusters are twofold. First, if the gas cools
effectively star formation can be triggered, generating new stellar
members in the system. Second, if the collective potential of the system
is able to alter the ambient gas properties before the gas is accreted
onto the individual core members, the augmented mass supply rates could
significantly alter the state of the various accreting stellar
populations and result in an enhanced central black hole accretion
luminosity.</description>
</item>


<item>

<title>Abramowski, A.: H.E.S.S. Observations of the Globular Clusters NGC 6388 and M15 and Search for a Dark Matter Signal</title>
<link>http://cdsads.u-strasbg.fr/abs/2011ApJ...735...12A</link>
<description>Observations of the globular clusters (GCs) NGC 6388 and M15 were
carried out by the High Energy Stereoscopic System array of Cherenkov
telescopes for a live time of 27.2 and 15.2 hr, respectively. No
gamma-ray signal is found at the nominal target position of NGC 6388 and
M15. In the primordial formation scenario, GCs are formed in a dark
matter (DM) halo and DM could still be present in the baryon-dominated
environment of GCs. This opens the possibility of observing a DM
self-annihilation signal. The DM content of the GCs NGC 6388 and M15 is
modeled taking into account the astrophysical processes that can be
expected to influence the DM distribution during the evolution of the
GC: the adiabatic contraction of DM by baryons, the adiabatic growth of
a black hole in the DM halo, and the kinetic heating of DM by stars.
Ninety-five percent confidence level exclusion limits on the DM particle
velocity-weighted annihilation cross section are derived for these DM
halos. In the TeV range, the limits on the velocity-weighted
annihilation cross section are derived at the 10&lt;SUP&gt;-25&lt;/SUP&gt;
cm&lt;SUP&gt;3&lt;/SUP&gt; s&lt;SUP&gt;-1&lt;/SUP&gt; level and a few
10&lt;SUP&gt;-24&lt;/SUP&gt; cm&lt;SUP&gt;3&lt;/SUP&gt; s&lt;SUP&gt;-1&lt;/SUP&gt; for NGC 6388
and M15, respectively.</description>
</item>


<item>

<title>Roederer, I. U.: Heavy-element Dispersion in the Metal-poor Globular Cluster M92</title>
<link>http://cdsads.u-strasbg.fr/abs/2011AJ....142...22R</link>
<description>Dispersion among the light elements is common in globular clusters
(GCs), while dispersion among heavier elements is less common. We
present detection of r-process dispersion relative to Fe in 19 red
giants of the metal-poor GC M92. Using spectra obtained with the Hydra
multi-object spectrograph on the WIYN Telescope at Kitt Peak National
Observatory, we derive differential abundances for 21 species of 19
elements. The Fe-group elements, plus Y and Zr, are homogeneous at a
level of 0.07-0.16 dex. The heavy-elements La, Eu, and Ho exhibit clear
star-to-star dispersion spanning 0.5-0.8 dex. The abundances of these
elements are correlated with one another, and we demonstrate that they
were produced by r-process nucleosynthesis. This r-process dispersion is
not correlated with the dispersion in C, N, or Na in M92, indicating
that r-process inhomogeneities were present in the gas throughout star
formation. The r-process dispersion is similar to that previously
observed in the metal-poor GC M15, but its origin in M15 or M92 is
unknown at present.

The WIYN Observatory is a joint facility of the University of
Wisconsin-Madison, Indiana University, Yale University, and the National
Optical Astronomy Observatory.</description>
</item>


<item>

<title>Strader, J.: Star Clusters in M31. V. Internal Dynamical Trends: Some Troublesome, Some Reassuring</title>
<link>http://cdsads.u-strasbg.fr/abs/2011AJ....142....8S</link>
<description>We present internal velocity dispersions and precise radial velocities
for 200 globular clusters (GCs) in M31 that are derived using new
high-resolution spectra from MMT/Hectochelle. Of these, 163 also have
King model structural parameters that allow us to estimate their
mass-to-light ratios. This is, by far, the largest such data set
available for any galaxy, including the Milky Way. These data strongly
confirm earlier suggestions that the optical and near-infrared
mass-to-light ratios of M31 GCs decline with increasing metallicity.
This behavior is the opposite of that predicted by stellar population
models for a standard initial mass function. We show that this
phenomenon does not appear to be caused by standard dynamical evolution.
A shallower mass function for metal-rich GCs (with dN/dMvpropM
&lt;SUP&gt;-0.8&lt;/SUP&gt;-M &lt;SUP&gt;-1.3&lt;/SUP&gt; below 1 M &lt;SUB&gt;sun&lt;/SUB&gt;)
can explain the bulk of extant observations. We also observe a
consistent, monotonic correlation between mass-to-light ratio and
cluster mass. This correlation, in contrast to the correlation with
metallicity, is well explained by the accepted model of dynamical
evolution of GCs through mass segregation and the preferential loss of
low-mass stars, and these data are among the best available to constrain
this process.</description>
</item>


<item>

<title>Richtler, T.: The dark halo of the Hydra I galaxy cluster: core, cusp, cosmological? Dynamics of NGC 3311 and its globular cluster system</title>
<link>http://cdsads.u-strasbg.fr/abs/2011A%26A...531A.119R</link>
<description>Context. Some galaxy clusters exhibit shallow or even cored dark matter
density profiles in their central regions rather than the predicted
steep or cuspy profiles, conflicting with the standard understanding of
dark matter. NGC 3311 is the central cD galaxy of the Hydra I cluster
(Abell 1060). &lt;BR /&gt; Aims: We use globular clusters around NGC 3311,
combined with kinematical data of the galaxy itself, to investigate the
dark matter distribution in the central region of Hydra I. &lt;BR /&gt;
Methods: Radial velocities of 118 bright globular clusters, based on
VLT/VIMOS mask spectroscopy, are used to calculate velocity dispersions
which are well defined out to 100 kpc. NGC 3311 is the most distant
galaxy for which this kind of study has been performed. We also
determine the velocity dispersions of the stellar component from
long-slit spectroscopy of NGC 3311 acquired with VLT/FORS1 out to 20
kpc. We present a new photometric model for NGC 3311, based on deep
VLT/FORS1 images in the V-band. We search for a dark halo that, in the
context of a spherical Jeans model, can reproduce the kinematical data.
We also compare the radial velocity distributions of globular clusters
and planetary nebulae. &lt;BR /&gt; Results: The projected stellar velocity
dispersion rises from a central low value of about 185 km s&lt;SUP&gt;-1&lt;/SUP&gt;
to 350 km s&lt;SUP&gt;-1&lt;/SUP&gt; at a radius of 20 kpc. The globular cluster
dispersion rises as well from 500 km s&lt;SUP&gt;-1&lt;/SUP&gt; at 10 kpc to about
800 km s&lt;SUP&gt;-1&lt;/SUP&gt; at 100 kpc, comparable to the velocity dispersion
of the cluster galaxies. A dark matter halo with a core (Burkert halo)
closely reproduces the velocity dispersions of stars and globular
clusters simultaneously under isotropy. The central stellar velocity
dispersions predicted by cosmological NFW halos do not agree well with
those observed, while the globular clusters allow a wide range of halo
parameters. A suspected radial anisotropy of the stellar population
found in merger simulations aggravates the disagreement with
observations. A slight tangential anisotropy would enable the data to be
more accurately reproduced. However, we find discrepancies with previous
kinematical data that we cannot resolve, which may indicate a more
complicated velocity pattern. &lt;BR /&gt; Conclusions: Although one cannot
conclusively demonstrate that the dark matter halo of NGC 3311 has a
core rather than a cusp, a core seems to be most consistent with the
present data. A more complete coverage of the velocity field and a more
thorough analysis of the anisotropy is required to reach firm
conclusions.

Based on observations taken at the European Southern Observatory, Cerro
Paranal, Chile, under the programs 082.B-0680, 076.B-0154, 065.N-0166,
065.N-0459.</description>
</item>


<item>

<title>Pasquini, L.: Measuring helium abundance difference in giants of NGC 2808</title>
<link>http://cdsads.u-strasbg.fr/abs/2011A%26A...531A..35P</link>
<description>Context. Multiple populations have been detected in several globular
clusters (GC) that do not display a spread in metallicity. Unusual
features of their observed colour-magnitude diagrams (CMD) can be
interpreted in terms of differences in the helium content of the stars
belonging to the sub-populations. &lt;BR /&gt; Aims: Even if evidence gathered
so far is compelling, differences in He abundance have never been
directly observed. We attempt to measure these differences in two giant
stars of NGC 2808 with very similar astrophysical parameters but
different Na and O abundances, hence that presumably belong to different
sub-populations, by directly comparing their He I 10 830 Å lines.
&lt;BR /&gt; Methods: The He 10 830 Å line forms in the upper
chromosphere. Our detailed models derive the chromospheric structure
using the Ca II and Hα chromospheric lines, and simulate the
corresponding He I 10 830 line profiles as a function of the helium
abundance. We show that, at a given value of He abundance, the He I 10
830 equivalent width cannot significantly change without a corresponding
much larger change in the Ca II chromospheric lines. We have used the
VLT-CRIRES to obtain high-resolution spectra in the 10 830 Å
region, and the VLT-UVES to obtain spectra of the Ca II and Hα
lines of our target stars. &lt;BR /&gt; Results: The two target stars have
very similar Ca II and Hα chromospheric lines, but different
appearances in the He region. One line, blueshifted by 17 km
s&lt;SUP&gt;-1&lt;/SUP&gt; with respect to the He 10 830 rest wavelength, is
detected in the spectrum of the Na-rich star, whereas the Na-poor star
spectrum is consistent with a non-detection. From a detailed
chromospheric modeling, we show that the difference in the spectra is
consistent and most closely explained by an He abundance difference
between the two stars of ΔY ≥ 0.17. Our optical observations
bracket the infrared ones over a range of about 50 days and we do not
observe any substantial variability in the Ca II and Hα lines. &lt;BR
/&gt; Conclusions: We provide direct evidence of a significant He line
strength difference in giant stars of NGC 2808 belonging to different
sub-populations, which had been previously detected by other photometric
and spectroscopic means. The use of appropriate model chromospheres
allows us for the first time to provide an approximate quantitative
estimate of this difference, which is clearly consistent with the
expected difference in abundance required by the stellar evolution
theory to account for the observed peculiarities of this cluster's cmD.

Based on observations collected at ESO VLT, Chile, under programme
384.D-0283.</description>
</item>


<item>

<title>Misgeld, I.: A large population of ultra-compact dwarf galaxies in the Hydra I cluster</title>
<link>http://cdsads.u-strasbg.fr/abs/2011A%26A...531A...4M</link>
<description>&lt;BR /&gt; Aims: We performed a large spectroscopic survey of compact,
unresolved objects in the core of the Hydra I galaxy cluster (Abell
1060), with the aim of identifying ultra-compact dwarf galaxies (UCDs)
and investigating the properties of the globular cluster (GC) system
around the central cD galaxy NGC 3311. &lt;BR /&gt; Methods: We obtained VIMOS
medium-resolution spectra of about 1200 candidate objects with apparent
magnitudes 18.5 &#60; V &#60; 24.0 mag, covering both the bright end of
the GC luminosity function and the luminosity range of all known UCDs.
&lt;BR /&gt; Results: By means of spectroscopic redshift measurements, we
identified 118 cluster members, from which 52 are brighter than
M&lt;SUB&gt;V&lt;/SUB&gt; = -11.0 mag, and can therefore be termed UCDs. The
brightest UCD in our sample has an absolute magnitude of M&lt;SUB&gt;V&lt;/SUB&gt; =
-13.4 mag (corresponding to a mass of ≳ 5 × 10&lt;SUP&gt;7&lt;/SUP&gt;
M&lt;SUB&gt;ȯ&lt;/SUB&gt;) and a half-light radius of 25 pc. This places it
among the brightest and most massive UCDs ever discovered. Most of the
GCs/UCDs are both spatially and dynamically associated to the central cD
galaxy. The overall velocity dispersion of the GCs/UCDs is comparable to
what is found for the cluster galaxies. However, when splitting the
sample into a bright and a faint part, we observe a lower velocity
dispersion for the bright UCDs/GCs than for the fainter objects. At a
dividing magnitude of M&lt;SUB&gt;V&lt;/SUB&gt; = -10.75 mag, the dispersions differ
by more than 200 km s&lt;SUP&gt;-1&lt;/SUP&gt; and up to 300 km s&lt;SUP&gt;-1&lt;/SUP&gt; for
objects within 5' around NGC 3311. &lt;BR /&gt; Conclusions: We interpret
these results in the context of different UCD formation channels, and
conclude that interaction-driven formation seems to play an important
role in the centre of Hydra I.

Based on observations obtained at the European Southern Observatory,
Chile (Observing Programmes 082.B-0680 and 076.B-0154).</description>
</item>


<item>

<title>Ventura, P.: A deep insight into the Mg-Al-Si nucleosynthesis in massive asymptotic giant branch and super-asymptotic giant branch stars</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.tmp..947V</link>
<description>The stars in globular clusters are known to differ in their surface
chemistry: spectroscopic investigations in recent decades outlined the
presence of star-to-star differences in the abundances of the light
elements, up to aluminium (and possibly silicon), suggesting that some
stars were contaminated by an advanced proton-capture nucleosynthesis.
The asymptotic giant branch (AGB) stars are one of the most promising
candidates in producing the pollution of the intracluster medium, via
the ejection of gas processed by hot bottom burning, from which new
stellar generations are formed. This work is focused on the degree of
nucleosynthesis involving magnesium, aluminium and silicon that these
sources may experience. The key ingredient in determining the degree of
magnesium depletion, and the amount of aluminium that can be produced,
is the rate of proton capture on &lt;SUP&gt;25&lt;/SUP&gt;Mg, forming
&lt;SUP&gt;26&lt;/SUP&gt;Al; an increase in this cross-section by a factor of 2 with
respect to the highest value allowed by the NACRE compilation allows the
reproduction of the extent of the Mg depletion observed, and is in
qualitative agreement with the positive Al-Si correlation observed in a
few clusters. The main uncertainties associated with the macro- and
microphysics input are discussed and commented upon, and a comparison
with recent spectroscopic results for globular clusters showing some
degree of Mg-Al anticorrelation and Al-Si correlation is presented.</description>
</item>


<item>

<title>Faucher-Giguère, C.-A.: Pulsar-black hole binaries in the Galactic Centre</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.tmp..911F</link>
<description>Binaries consisting of a pulsar and a black hole (BH) are a holy grail
of astrophysics, both for their significance for stellar evolution and
for their potential application as probes of strong gravity. In spite of
extensive surveys of our Galaxy and its system of globular clusters, no
pulsar-black hole (PSR-BH) binary has been found to date. Clues as to
where such systems might exist are therefore important. We show that if
the central parsec around Sgr A&lt;SUP&gt;★&lt;/SUP&gt; harbours a cluster of
˜25 000 stellar BHs (as predicted by mass-segregation arguments)
and if it is also rich in recycled pulsar binaries (by analogy with
globular clusters), then three-body exchange interactions should produce
PSR-BHs in the Galactic Centre. Simple estimates of the formation rate
and survival time of these binaries suggest that a few PSR-BHs should be
present in the central parsec today. The proposed formation mechanism
makes unique predictions for the PSR-BH properties: (1) the binary would
reside within ˜1 pc of Sgr A&lt;SUP&gt;★&lt;/SUP&gt;; (2) the pulsar
would be recycled, with a period of ˜1 to a few tens of
milliseconds, and a low magnetic field B≲ 10&lt;SUP&gt;10&lt;/SUP&gt; G; (3)
the binary would have high eccentricity, e˜ 0.8, but with a large
scatter and (4) the binary would be relatively wide, with semimajor axis
a&lt;SUB&gt;b&lt;/SUB&gt;˜ 0.1 -≳3 au. The potential discovery of a
PSR-BH binary therefore provides a strong motivation for deep,
high-frequency radio searches for recycled pulsars towards the Galactic
Centre.</description>
</item>


<item>

<title>Leigh, N.: Dissecting the colour-magnitude diagram: a homogeneous catalogue of stellar populations in globular clusters</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.tmp..909L</link>
<description>We present a homogeneous catalogue for blue straggler, red giant branch,
horizontal branch and main-sequence turn-off stars in a sample of 35
clusters taken from the Advanced Camera for Surveys (ACS) Survey for
Globular Clusters. As a result of the superior photometry and relatively
large field of view offered by the ACS data, this new catalogue is a
significant improvement upon the one presented in our 2007 catalogue.
Using our catalogue, we study and compare the radial distributions of
the different stellar populations.

We have confirmed our previous result that there is a clear, but
sublinear, correlation between the number of blue stragglers found in
the cluster core and the total stellar mass contained within it. By
considering a larger spatial extent than just the core, our results
suggest that mass segregation is not the dominant effect contributing to
the observed sublinearity. We also investigate the radial distributions
of the different stellar populations in our sample of clusters. Our
results are consistent with a linear relationship between the number of
stars in these populations and the total mass enclosed within the same
radius. Therefore, we conclude that the cluster dynamics does not
significantly affect the relative distributions of these populations in
our sample.</description>
</item>


<item>

<title>Foster, C.: Global properties of 'ordinary' early-type galaxies: photometry and spectroscopy of stars and globular clusters in NGC 4494</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.tmp..906F</link>
<description>We present a comprehensive analysis of the spatial, kinematic and
chemical properties of stars and globular clusters (GCs) in the
'ordinary' elliptical galaxy NGC 4494 using data from the Keck and
Subaru telescopes. We derive galaxy surface brightness and colour
profiles out to large galactocentric radii. We compare the latter to
metallicities derived using the near-infrared Calcium Triplet. We obtain
stellar kinematics out to ˜3.5 effective radii. The latter appear
flattened or elongated beyond ˜1.8 effective radii in contrast to
the relatively round photometric isophotes. In fact, NGC 4494 may be a
flattened galaxy, possibly even an S0, seen at an inclination of
˜45°. We publish a catalogue of 431 GC candidates brighter
than i&lt;SUB&gt;0&lt;/SUB&gt;= 24 based on the photometry, of which 109 are
confirmed spectroscopically and 54 have measured spectroscopic
metallicities. We also report the discovery of three spectroscopically
confirmed ultra-compact dwarfs around NGC 4494 with measured
metallicities of -0.4 ≲[Fe/H]≲-0.3. Based on their properties,
we conclude that they are simply bright GCs. The metal-poor GCs are
found to be rotating with similar amplitude as the galaxy stars, while
the metal-rich GCs show marginal rotation. We supplement our analysis
with available literature data and results. Using model predictions of
galaxy formation, and a suite of merger simulations, we find that many
of the observational properties of NGC 4494 may be explained by
formation in a relatively recent gas-rich major merger. Complete studies
of individual galaxies incorporating a range of observational avenues
and methods such as the one presented here will be an invaluable tool
for constraining the fine details of galaxy formation models, especially
at large galactocentric radii.</description>
</item>


<item>

<title>Liu, L.: Two extreme contact binary systems in the nearest globular cluster M4</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.tmp..875L</link>
<description>We present the results of photometric solutions for two contact binaries
in the nearby globular cluster M4. We estimate their physical parameters
using the light-curve program of the Wilson-Devinney code. These systems
have quite different mass ratios, which indicates that they did not form
at the same time. V47 is an extreme mass-ratio system (q= 0.123 ±
0.002) being dissimilar to the same kind of field contact binaries. V53
is a high mass-ratio (q= 1.230 ± 0.004), deep-contact (f= 79.7
± 1.9 per cent) system. It is also a blue straggler.</description>
</item>


<item>

<title>Frank, M. J.: Spatially resolved kinematics of an ultracompact dwarf galaxy</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.414L..70F</link>
<description>We present the internal kinematics of UCD3, the brightest known
ultracompact dwarf galaxy (UCD) in the Fornax cluster, making this the
first UCD with spatially resolved spectroscopy. Our study is based on
seeing-limited observations obtained with the ARGUS Integral Field Unit
of the VLT/FLAMES spectrograph under excellent seeing conditions
(0.5-0.67 arcsec FWHM).

The velocity field of UCD3 shows the signature of weak rotation,
comparable to that found in massive globular clusters. Its velocity
dispersion profile is fully consistent with an isotropic velocity
distribution and the assumption that mass follows the light distribution
obtained from Hubble Space Telescope imaging. In particular, there is no
evidence for the presence of an extended dark matter halo contributing a
significant (≳33 per cent within R &#60; 200 pc) mass fraction, nor
for a central black hole more massive than ˜5 per cent of the
UCD's mass. While this result does not exclude a galaxian origin for
UCD3, we conclude that its internal kinematics are fully consistent with
it being a massive star cluster. Based on observations obtained at the
European Southern Observatory, Chile [Observing Programme
078.B-0496(B)].</description>
</item>


<item>

<title>Degenaar, N.: The accretion-heated crust of the transiently accreting 11-Hz X-ray pulsar in the globular cluster Terzan 5</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.414L..50D</link>
<description>We report on a Chandra Director's Discretionary Time observation of the
globular cluster Terzan 5, carried out ˜7 weeks after the
cessation of the 2010 outburst of the newly discovered transiently
accreting 11-Hz X-ray pulsar. We detect a thermal spectrum that can be
fitted with a neutron star atmosphere model with a temperature for an
observer at infinity of kT&lt;SUP&gt;∞&lt;/SUP&gt;˜ 100 eV and a
quiescent thermal bolometric luminosity of L&lt;SUB&gt;q&lt;/SUB&gt;˜ 2
× 10&lt;SUP&gt;33&lt;/SUP&gt; erg s&lt;SUP&gt;-1&lt;/SUP&gt; for an assumed distance of
5.5 kpc. The thermal emission is elevated above the quiescent base level
measured in 2003 and 2009, i.e. prior to the recent accretion outburst.
A likely explanation is that the neutron star crust was significantly
heated during the recent accretion episode and needs to cool until it
restores thermal equilibrium with the core. Although this has been
observed for neutron star low-mass X-ray binaries that undergo accretion
episodes of years to decades, it is the first time that evidence for
crustal heating is detected for a transient system with a regular
outburst duration of weeks. This opens up a new window to study heating
and cooling of transiently accreting neutron stars.</description>
</item>


<item>

<title>Fiocchi, M.: The 17-min orbital period in the ultracompact X-ray binary 4U 0513-40</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.414L..41F</link>
<description>The ultracompact low-mass X-ray binary 4U 0513-40 in the globular
cluster NGC1851 exhibits large amplitude X-ray flux variations with
spectral changes from low/hard to high/soft states which have not been
reported previously in other ultracompact X-ray binaries. Using
BeppoSAX, Chandra and XMM-Newton archival data together with recent
INTEGRAL observations, we reveal a clear sinusoidal periodic signal with
a period of ˜17 min when the source is in a typical high/soft
state with a dominant soft thermal component. The periodicity disappears
when the source is in a low/hard state and the thermal soft component is
not required any more to model the data. These properties indicate the
orbital nature of the detected signal and imply an high inclination
angle of the binary system (&#62;80°).</description>
</item>


<item>

<title>Motta, S.: X-ray bursts and burst oscillations from the slowly spinning X-ray pulsar IGR J17480-2446 (Terzan 5)</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.414.1508M</link>
<description>The newly discovered 11-Hz accreting pulsar, IGR J17480-2446, located in
the globular cluster Terzan 5, has shown several bursts with a
recurrence time as short as a few minutes. The source shows the shortest
recurrence time ever observed from a neutron star. Here we present a
study of the morphological, spectral and temporal properties of 107
bursts observed by the Rossi X-ray Timing Explorer. The recurrence time
and the fluence of the bursts clearly anticorrelate with the increase in
the persistent X-ray flux. The ratio between the energy generated by the
accretion of mass and that liberated during bursts indicates that helium
is ignited in a hydrogen-rich layer. Therefore, we conclude that all the
bursts shown by IGR J17480-2446 are Type I X-ray bursts. Pulsations
could be detected in all the brightest bursts and no drifts of the
frequency are observed within 0.25 Hz of the spin frequency of the
neutron star. These are also phase-locked with respect to the pulsations
observed during the persistent emission and no rise in the rms
associated to the pulse frequency is observed during the burst. This
behaviour would favour a scenario where the Type I burst, possibly
ignited at the polar caps, immediately propagates to the entire neutron
star surface.</description>
</item>


<item>

<title>Huxor, A. P.: Exploring the properties of the M31 halo globular cluster system</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.414..770H</link>
<description>Following on from our discovery of a significant population of M31 outer
halo globular clusters (GCs), and updates to the Revised Bologna
Catalogue of M31 GCs, we investigate the GC system of M31 out to an
unprecedented radius (≈120 kpc). We derive various ensemble
properties, including the magnitude, colour and metallicity
distributions, as well as the GC number density profile. One of our most
significant findings is evidence for a flattening in the radial GC
number density profile in the outer halo. Intriguingly, this occurs at a
galactocentric radius of ˜2° (˜30 kpc) which is the
radius at which the underlying stellar halo surface density has also
been shown to flatten. The GCs which lie beyond this radius are
remarkably uniform in terms of their blue (V-I)&lt;SUB&gt;0&lt;/SUB&gt; colours,
consistent with them belonging to an ancient population with little to
no metallicity gradient. Structural parameters are also derived for a
sample of 13 newly discovered extended clusters (ECs), and we find the
lowest luminosity ECs have magnitudes and sizes similar to Palomar-type
GCs in the Milky Way halo. We argue that our findings provide strong
support for a scenario in which a significant fraction of the outer halo
GC population of M31 has been accreted.</description>
</item>


<item>

<title>Norris, M. A.: The ubiquity and dual nature of ultra-compact dwarfs</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.414..739N</link>
<description>We present the discovery of several ultra-compact dwarfs (UCDs) located
in field/group environments. Examination of these objects, plus
literature UCDs, confirms the existence of two distinct formation
channels for these compact stellar systems. We find that the UCDs we
have discovered around the group elliptical NGC 3923 (and most UCDs in
general) have properties consistent with their being the most luminous
members of the host galaxy's globular cluster (GC) system. As with GCs
they are therefore likely to be the product of the most violent epochs
of galaxy formation. We describe UCDs of this type as giant GCs (GGCs).
In contrast, the UCD we have found associated with the isolated S0 NGC
4546 is clearly the result of the stripping of a nucleated companion
galaxy. The young age (˜3.4 Gyr) of the UCD, the lack of a
correspondingly young GC population, the apparently short dynamical
friction decay time-scale (˜0.5 Gyr) of the UCD and the presence
of a counter-rotating gas disc in the host galaxy (corotating with
respect to the UCD) together suggest that this UCD is the liberated
nucleus remaining after the recent stripping of a companion by NGC 4546.
We infer that the presence of UCDs of either category (GGCs formed in
major star-forming events, or stripped nuclei formed in minor mergers)
can provide a useful probe of the assembly history of the host galaxy.
We suggest a general scheme that unifies the formation of GCs, UCDs and
galaxy nuclei. In this picture, 'normal' GCs are a composite population,
composed of GCs formed in situ, GCs acquired from accreted galaxies and
a population of lower mass stripped dwarf nuclei masquerading as GCs.
Above a 'scaling onset mass' of 2 × 10&lt;SUP&gt;6&lt;/SUP&gt;
M&lt;SUB&gt;ȯ&lt;/SUB&gt; (M&lt;SUB&gt;V&lt;/SUB&gt;˜-10), UCDs emerge together with
a mass-size relation and a likely mass-metallicity relation (the 'blue
tilt'). In the mass range up to 7 × 10&lt;SUP&gt;7&lt;/SUP&gt;
M&lt;SUB&gt;ȯ&lt;/SUB&gt; (M&lt;SUB&gt;V&lt;/SUB&gt;˜-13) UCDs comprise a composite
population of GGCs and stripped nuclei. Interestingly, dwarf nuclei have
similar colours to blue GCs and UCDs across the scaling onset mass,
smoothly extending the blue tilt, while nuclei of more massive galaxies
and a prominent minority of UCDs extend the red locus of GCs. Above 7
× 10&lt;SUP&gt;7&lt;/SUP&gt; M&lt;SUB&gt;ȯ&lt;/SUB&gt;, UCDs must be almost
exclusively stripped nuclei, as no sufficiently rich GC systems exist to
populate such an extreme of the GCLF.</description>
</item>


<item>

<title>Hourihane, A. P.: Ground- and space-based study of two globular cluster cataclysmic variables: M22 CV1 and M5 V101</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.414..184H</link>
<description>As a class of compact binaries with large binding energy, cataclysmic
variables (CVs) formed through close encounters play an important role
in the dynamical evolution of globular clusters. As part of a systematic
search for CVs undergoing dwarf nova (DN) eruptions in globular
clusters, our 2004 monitoring programme of M22 detected an outburst of
the DN candidate CV1 during May. We implement the ISIS image subtraction
routine to obtain a light curve for an outburst of CV1. We present the
outburst light curve as well as Hubble Space Telescope/Wide-Field
Planetary Camera 2 (WFPC2) photometry in the V, U and near-ultraviolet
(nUV) bands and a Chandra/Advanced CCD Imaging Spectrometer (ACIS)
spectrum of the object. Our results confirm the DN nature of the
outburst and the CV status of the object. We also present the results of
a ground-based study of another globular cluster CV, M5 V101 - including
quiescent medium-resolution William Herschel Telescope
(WHT)/Intermediate dispersion Spectrograph and Imaging System (ISIS)
spectroscopy in the B and R bands, displaying prominent Balmer and He I
emission, and R-band photometry.</description>
</item>


<item>

<title>Forbes, D. A.: Evidence for two phases of galaxy formation from radial trends in the globular cluster system of NGC 1407</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.413.2943F</link>
<description>Here we present the colours of individual globular clusters (GCs) around
the massive elliptical galaxy NGC 1407 out to a projected galactocentric
radius of 140 kpc or 17 galaxy effective radii (R&lt;SUB&gt;e&lt;/SUB&gt;). Such
data are a proxy for the halo metallicity. We find steep, and similar,
metallicity gradients of ˜-0.4 dex dex&lt;SUP&gt;-1&lt;/SUP&gt; for both the
blue (metal poor) and red (metal rich) GC subpopulations within 5-8.5
R&lt;SUB&gt;e&lt;/SUB&gt; (40-70 kpc). At larger radii the mean GC colours
(metallicity) are constant. A similar behaviour is seen in a wide-field
study of M87's GC system, and in our own Galaxy. We interpret these
radial metallicity trends to indicate an inner region formed by early in
situ dissipative processes and an outer halo formed by the ongoing
accretion of low-mass galaxies and their GCs. These results provide
observational support for the model of galaxy formation whereby massive
galaxies form inside-out in two phases. We have also searched the
literature for other massive early-type galaxies with reported GC
metallicity gradients in their inner regions. No obvious correlation
with galaxy mass or environment is found but the sample is currently
small.</description>
</item>


<item>

<title>Assmann, P.: Star cluster collisions - a formation scenario for the extended globular cluster Scl-dE1 GC1</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.413.2606A</link>
<description>Recent observations of the dwarf elliptical galaxy Scl-dE1 (Sc22) in the
Sculptor group of galaxies revealed an extended globular cluster
(Scl-dE1 GC1), which exhibits an extremely large core radius of about
21.2 pc. The authors of the discovery paper speculate on whether this
object could reside in its own dark matter halo and/or if it might have
formed through the merging of two or more star clusters. In this paper,
we present N-body simulations to explore thoroughly this particular
formation scenario. We follow the merger of two star clusters within
dark matter haloes of a range of masses (as well as in the absence of a
dark matter halo). In order to obtain a remnant which resembles the
observed extended star cluster, we find that the star formation
efficiency has to be quite high (around 33 per cent) and the dark matter
halo, if present at all, has to be of very low mass, i.e. raising the
mass-to-light ratio of the object within the body of the stellar
distribution by at most a factor of a few. We also find that expansion
of a single star cluster following mass loss provides another viable
formation path. Finally, we show that future measurements of the
velocity dispersion of this system may be able to distinguish between
the various scenarios we have explored.</description>
</item>


<item>

<title>Gieles, M.: The life cycle of star clusters in a tidal field</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.413.2509G</link>
<description>The evolution of globular clusters due to two-body relaxation results in
an outward flow of energy and at some stage all clusters need a central
energy source to sustain their evolution. Hénon provided the
insight that we do not need to know the details of the energy production
in order to understand the relaxation-driven evolution of the cluster,
at least outside the core. He provided two self-similar solutions for
the evolution of clusters based on the view that the cluster as a whole
determines the amount of energy that is produced in the core: steady
expansion for isolated clusters, and homologous contraction for clusters
evaporating in a tidal field. The amount of expansion or evaporation per
relaxation time-scale is set by the instantaneous radius or number of
stars, respectively. We combine these two approximate models and propose
a pair of Unified Equations of Evolution (UEE) for the life cycle of
initially compact clusters in a tidal field. The half-mass radius
increases during the first part (roughly half) of the evolution, and
decreases in the second half, while the escape rate approaches a
constant value set by the tidal field. We refer to these phases as
'expansion dominated' and 'evaporation dominated'. These simple
analytical solutions of the UEE immediately allow us to construct
evolutionary tracks and isochrones in terms of cluster half-mass
density, cluster mass and galactocentric radius. From a comparison to
the Milky Way globular clusters we find that roughly one-third of them
are in the second, evaporation-dominated phase and for these clusters
the density inside the half-mass radius varies with the galactocentric
distance R&lt;SUB&gt;G&lt;/SUB&gt; as
ρ&lt;SUB&gt;h&lt;/SUB&gt;∝R&lt;SUP&gt;-2&lt;/SUP&gt;&lt;SUB&gt;G&lt;/SUB&gt;. The remaining
two-thirds are still in the first, expansion-dominated phase and their
isochrones follow the environment-independent scaling
ρ&lt;SUB&gt;h&lt;/SUB&gt;∝M&lt;SUP&gt;2&lt;/SUP&gt;, where M is the cluster mass; that
is, a constant relaxation time-scale. We find substantial agreement
between Milky Way globular cluster parameters and the isochrones, which
suggests that there is, as Hénon suggested, a balance between the
flow of energy and the central energy production for almost all globular
clusters.</description>
</item>


<item>

<title>Majaess, D. J.: Anchoring the Universal Distance Scale Via a Wesenheit Template</title>
<link>http://cdsads.u-strasbg.fr/abs/2011JAVSO..39..122M</link>
<description>A VI Wesenheit diagram featuring SX Phoenicis, δ Scuti, RR Lyrae,
and type II and classical Cepheid variables is calibrated by means of
geometric-based distances inferred from HST, Hipparcos, and VLBA
observations (n = 30). The distance to a target population follows from
the offset between the observed Wesenheit magnitudes and the calibrated
template. The method is evaluated by ascertaining the distance moduli
for the LMC (μ0 = 18.43 ± 0.03 σx) and the globular
clusters ω Cen, M54, M13, M3, and M15. The results agree with
estimates cited in the literature, although a nearer distance to M13 is
favored (pending confirmation of the data's
photometric zero-point) and observations of variables near the core of
M15 suffer from photometric contamination. The calibrated LMC data are
subsequently added to the Wesenheit template since that galaxy exhibits
precise OGLE photometry for innumerable variables of differing classes,
that includes recent observations for δ Scuti variables indicating
the stars follow a steeper VI Wesenheit function than classical Cepheids
pulsating in the fundamental mode. VI photometry for the calibrators is
tabulated to facilitate further research, and includes new observations
acquired via the AAVSO's robotic telescope network (e.g., VY Pyx:
&#60;V&#62; = 7.25 and &#60;V&#62; -  = 0.67). The approach outlined here
supercedes the lead author's prior first-order effort
to unify variables of the instability strip in order to establish
reliable distances.</description>
</item>


<item>

<title>Sivakoff, G. R.: Chandra HRC confirms that M15 X-2 is the currently flaring source in M15</title>
<link>http://cdsads.u-strasbg.fr/abs/2011ATel.3393....1S</link>
<description>Radio observations of the ongoing X-ray flare in the globular cluster
M15 (ATel #3356, #3363), suggested that the ultracompact X-ray binary
M15 X-2 was the flaring source (ATel #3378). This is surprising as
ultracompact X-ray binaries such as M15 X-2 (22 minute period, Dieball
et al. 2005, ApJ, 634, L105) are generally not expected to show factors
of &#62;10 flux variations over timescales of days to weeks.</description>
</item>


<item>

<title>Lynch, R. S.: Six New Recycled Globular Cluster Pulsars Discovered with the Green Bank Telescope</title>
<link>http://cdsads.u-strasbg.fr/abs/2011ApJ...734...89L</link>
<description>We have completed sensitive searches for new pulsars in seven globular
clusters using the Robert C. Byrd Green Bank Telescope, and have
discovered six new recycled pulsars (four in NGC 6517 and two in M22),
five of which are fully recycled millisecond pulsars with P &#60; 10 ms.
We report full timing solutions for all six new pulsars and provide
estimates of their flux densities and spectral indices. None of the
pulsars is detected in archival Chandra data down to L &lt;SUB&gt;X&lt;/SUB&gt; ~
10&lt;SUP&gt;32&lt;/SUP&gt; erg s&lt;SUP&gt;-1&lt;/SUP&gt; for NGC 6517 and L &lt;SUB&gt;X&lt;/SUB&gt;
~ 10&lt;SUP&gt;31&lt;/SUP&gt; erg s&lt;SUP&gt;-1&lt;/SUP&gt; for M22. One of the
millisecond pulsars in M22 appears to have a very low mass companion,
and is likely a new &quot;black widow.&quot; A second binary pulsar in NGC 6517 is
in a long-period, mildly eccentric orbit. We are able to set some lower
limits on the age of the system, and find that it may be less than a few
hundred million years old, which would indicate recent pulsar recycling
in NGC 6517. An isolated pulsar in NGC 6517 that lies about 20 core
radii from the cluster center appears to have been ejected from the core
by interacting with a massive binary. By analyzing the luminosity
function of the pulsars in NGC 6517, we predict the cluster to harbor
roughly a dozen pulsars. We use the observed period derivatives of three
pulsars to set lower limits on the mass-to-light ratios in the cores of
their host clusters, and find no evidence for large amounts of
low-luminosity matter. We also discuss reasons for non-detections in
some of the clusters we searched.</description>
</item>


<item>

<title>Barnard, R.: Four New Black Hole Candidates Identified in M31 Globular Clusters with Chandra and XMM-Newton</title>
<link>http://cdsads.u-strasbg.fr/abs/2011ApJ...734...79B</link>
<description>We have identified four new black hole candidates (BHCs) in M31 globular
clusters (GCs) using 123 Chandra and 4 XMM-Newton observations of the
M31 central region. The X-ray source associated with Bo 163 (XB163) is a
recurrent transient with the highest observed luminosity, ~1.4×
10&lt;SUP&gt;38&lt;/SUP&gt; erg s&lt;SUP&gt;-1&lt;/SUP&gt;, considerably brighter than any
outbursts from neutron star transients Aql X-1 or 4U 1608-452; the
outburst apparently started ~45 days earlier than the observed peak, and
hence the luminosity may have been considerably higher. We identified
XB082, XB153, and XB185 as BHCs by observing &quot;low state&quot; emission
spectra at luminosities that exceed the threshold for neutron star
binaries. The probability that these are neutron star systems with
anisotropic emission beamed toward us is &#60;~ 4 ×
10&lt;SUP&gt;-4&lt;/SUP&gt;, and their variability suggests emission from a
single source. We therefore conclude that these systems likely contain
black holes rather than neutron stars. We have now identified four
persistently bright BHCs in the region; the probability that these are
all background active galactic nuclei is
lsim1×10&lt;SUP&gt;-20&lt;/SUP&gt;. According to theory, the donors
could be tidally captured main-sequence stars or white dwarfs in
ultracompact binaries. We find that GCs that are particularly massive
(XB082) or metal-rich (XB144) can host bright X-ray sources in addition
to GCs that are both (XB163). Our method may reveal BHCs in other bright
X-ray sources.</description>
</item>


<item>

<title>Coelho, P.: Chemical Abundance Anticorrelations in Globular Cluster Stars: The Effect on Cluster Integrated Spectra</title>
<link>http://cdsads.u-strasbg.fr/abs/2011ApJ...734...72C</link>
<description>It is widely accepted that individual Galactic globular clusters harbor
two coeval generations of stars, the first one born with the &quot;standard&quot;
α-enhanced metal mixture observed in field halo objects and the
second one characterized by an anticorrelated CNONa abundance pattern
overimposed on the first generation, α-enhanced metal mixture. We
have investigated with appropriate stellar population synthesis models
how this second generation of stars affects the integrated spectrum of a
typical metal-rich Galactic globular cluster, like 47 Tuc, focusing our
analysis on the widely used Lick-type indices. We find that the only
indices appreciably affected by the abundance anticorrelations are
Ca4227, G4300, CN&lt;SUB&gt;1&lt;/SUB&gt;, CN&lt;SUB&gt;2&lt;/SUB&gt;, and NaD. The
age-sensitive Balmer line, Fe line, and the [MgFe] indices widely used
to determine age, Fe, and total metallicity of extragalactic systems are
largely insensitive to the second generation population. Enhanced He in
second generation stars affects also the Balmer line indices of the
integrated spectra, through the change of the turnoff temperature
and—with the assumption that the mass-loss history of both stellar
generations is the same—the horizontal branch morphology of the
underlying isochrones.</description>
</item>


<item>

<title>Schlaufman, K. C.: Insight into the Formation of the Milky Way through Cold Halo Substructure. II. The Elemental Abundances of ECHOS</title>
<link>http://cdsads.u-strasbg.fr/abs/2011ApJ...734...49S</link>
<description>We determine the average metallicities of the elements of cold halo
substructure (ECHOS) that we previously identified in the inner halo of
the Milky Way within 17.5 kpc of the Sun. As a population, we find that
stars kinematically associated with ECHOS are chemically distinct from
the background kinematically smooth inner halo stellar population along
the same Sloan Extension for Galactic Understanding and Exploration
(SEGUE) line of sight. ECHOS are systematically more iron-rich, but less
α-enhanced than the kinematically smooth component of the inner
halo. ECHOS are also chemically distinct from other Milky Way
components: more iron-poor than typical thick-disk stars and both more
iron-poor and α-enhanced than typical thin-disk stars. In
addition, the radial velocity dispersion distribution of ECHOS extends
beyond σ ~ 20 km s&lt;SUP&gt;-1&lt;/SUP&gt;. Globular clusters are
unlikely ECHOS progenitors, as ECHOS have large velocity dispersions and
are found in a region of the Galaxy in which iron-rich globular clusters
are very rare. Likewise, the chemical composition of stars in ECHOS does
not match predictions for stars formed in the Milky Way and subsequently
scattered into the inner halo. Dwarf spheroidal (dSph) galaxies are
possible ECHOS progenitors, and if ECHOS are formed through the tidal
disruption of one or more dSph galaxies, the typical ECHOS [Fe/H] ~
- 1.0 and radial velocity dispersion σ ~ 20 km
s&lt;SUP&gt;-1&lt;/SUP&gt; implies a dSph with M &lt;SUB&gt;tot&lt;/SUB&gt; &#62;~
10&lt;SUP&gt;9&lt;/SUP&gt; M &lt;SUB&gt;sun&lt;/SUB&gt;. Our observations confirm the
predictions of theoretical models of Milky Way halo formation that
suggest that prominent substructures are likely to be metal-rich, and
our result implies that the most likely metallicity for a recently
accreted star currently in the inner halo is [Fe/H] ~ - 1.0.</description>
</item>


<item>

<title>Roh, D.-G.: Two Distinct Red Giant Branches in the Globular Cluster NGC 288</title>
<link>http://cdsads.u-strasbg.fr/abs/2011ApJ...733L..45R</link>
<description>We report the presence of two distinct red giant branches (RGBs) in the
globular cluster NGC 288 from the narrowband calcium and Strömgren
b and y photometry obtained at the CTIO 4 m Blanco telescope. The RGB of
NGC 288 is clearly split into two in the hk [=(Ca - b) - (b
- y)] index, while the split is not shown in the b - y
color. Unlike other globular clusters with multiple populations reported
thus far, the horizontal branch of NGC 288 is only mildly extended. Our
stellar population models show that this and the presence of two
distinct RGBs in NGC 288 can be reproduced if slightly metal-rich
(Δ[m/H] ≈ 0.16) second generation stars are also enhanced in
helium by small amount (ΔY ≈ 0.03) and younger by ~1.5 Gyr. The
RGB split in the hk index is most likely indicating that the second
generation stars were affected by supernovae enrichment, together with
the pollution of lighter elements by intermediate-mass asymptotic giant
branch stars or fast-rotating massive stars. In order to confirm this,
however, spectroscopy of stars in the two distinct RGB groups is
urgently required.</description>
</item>


<item>

<title>Clausen, D.: How to Make a Singleton sdB Star via Accelerated Stellar Evolution</title>
<link>http://cdsads.u-strasbg.fr/abs/2011ApJ...733L..42C</link>
<description>Many hot subdwarf B stars (sdBs) are in close binaries, and the favored
formation channels for subdwarfs rely on mass transfer in a binary
system to strip a core He-burning star of its envelope. However, these
channels cannot account for sdBs that have been observed in long-period
binaries nor the narrow mass distribution of isolated (or &quot;singleton&quot;)
sdBs. We propose a new formation channel involving the merger of a
helium white dwarf and a low-mass, hydrogen-burning star, which
addresses these issues. Hierarchical triples whose inner binaries merge
and form sdBs by this process could explain the observed long-period
subdwarf+main-sequence binaries. This process would also naturally
explain the observed slow rotational speeds of singleton sdBs. We also
briefly discuss the implications of this formation channel for extreme
horizontal branch morphology in globular clusters and the UV upturn in
elliptical galaxies.</description>
</item>


<item>

<title>Linares, M.: On the Cooling Tails of Thermonuclear X-ray Bursts: The IGR J17480-2446 Link</title>
<link>http://cdsads.u-strasbg.fr/abs/2011ApJ...733L..17L</link>
<description>The neutron star transient and 11 Hz X-ray pulsar IGR J17480-2446,
recently discovered in the globular cluster Terzan 5, showed
unprecedented bursting activity during its 2010 October-November
outburst. We analyzed all X-ray bursts detected with the Rossi X-ray
Timing Explorer and find strong evidence that they all have a
thermonuclear origin, despite the fact that many do not show the
canonical spectral softening along the decay imprinted on type I X-ray
bursts by the cooling of the neutron star photosphere. We show that the
persistent-to-burst power ratio is fully consistent with the
accretion-to-thermonuclear efficiency ratio along the whole outburst, as
is typical for type I X-ray bursts. The burst energy, peak luminosity,
and daily-averaged spectral profiles all evolve smoothly throughout the
outburst, in parallel with the persistent (non-burst) luminosity. We
also find that the peak-burst to persistent luminosity ratio determines
whether or not cooling is present in the bursts from IGR
J17480-2446, and argue that the apparent lack of cooling is due to
the &quot;non-cooling&quot; bursts having both a lower peak temperature and a
higher non-burst (persistent) emission. We conclude that the detection
of cooling along the decay is a sufficient, but not a necessary
condition to identify an X-ray burst as thermonuclear. Finally, we
compare these findings with X-ray bursts from other rapidly accreting
neutron stars.</description>
</item>


<item>

<title>Servillat, M.: A Dwarf Nova in the Globular Cluster M13</title>
<link>http://cdsads.u-strasbg.fr/abs/2011ApJ...733..106S</link>
<description>Dwarf novae (DNe) in globular clusters (GCs) seem to be rare with only
13 detections in the 157 known Galactic GCs. We report the
identification of a new DN in M13, the 14th DN identified in a GC to
date. Using the 2 m Faulkes Telescope North, we conducted a search for
stars in M13 that show variability over a year (2005-2006) on timescales
of days and months. This led to the detection of one DN showing several
outbursts. A Chandra X-ray source is coincident with this DN and shows
both a spectrum and variability consistent with that expected from a DN,
thus supporting the identification. We searched for a counterpart in
Hubble Space Telescope Advanced Camera for Surveys/Wide Field Camera
archived images and found at least 11 candidates, of which we could
characterize only the 7 brightest, including one with a 3σ
Hα excess and a faint blue star. The detection of one DN when more
could have been expected likely indicates that our knowledge of the
global Galactic population of cataclysmic variables is too limited. The
proportion of DNe may be lower than found in catalogs, or they may have
a much smaller mean duty cycle (~1%) as proposed by some population
synthesis models and recent observations in the field.</description>
</item>


<item>

<title>Gray, W. J.: Formation of Compact Stellar Clusters by High-redshift Galaxy Outflows. II. Effect of Turbulence and Metal-line Cooling</title>
<link>http://cdsads.u-strasbg.fr/abs/2011ApJ...733...88G</link>
<description>In the primordial universe, low-mass structures with virial temperatures
less than 10&lt;SUP&gt;4&lt;/SUP&gt; K were unable to cool by atomic line
transitions, leading to a strong suppression of star formation. On the
other hand, these &quot;minihalos&quot; were highly prone to triggered star
formation by interactions from nearby galaxy outflows. In Gray &#38;
Scannapieco, we explored the impact of nonequilibrium chemistry on these
interactions. Here we turn our attention to the role of metals, carrying
out a series of high-resolution three-dimensional adaptive mesh
refinement simulations that include both metal cooling and a subgrid
turbulent mixing model. Despite the presence of an additional coolant,
we again find that outflow-minihalo interactions produce a distribution
of dense, massive stellar clusters. We also find that these clusters are
evenly enriched with metals to a final abundance of Z ≈
10&lt;SUP&gt;-2&lt;/SUP&gt; Z &lt;SUB&gt;sun&lt;/SUB&gt;. As in our previous simulations,
all of these properties suggest that these interactions may have given
rise to present-day halo globular clusters.</description>
</item>


<item>

<title>Martell, S. L.: Light-element abundance variations in globular clusters</title>
<link>http://cdsads.u-strasbg.fr/abs/2011AN....332..467M</link>
<description>Star-to-star variations in abundances of the light elements carbon,
nitrogen, oxygen, and sodium have been observed in stars of all
evolutionary phases in all Galactic globular clusters that have been
thoroughly studied. The data available for studying this phenomenon, and
the hypotheses as to its origin, have both co-evolved with observing
technology; once high-resolution spectra were available even for
main-sequence stars in globular clusters, scenarios involving multiple
closely spaced stellar generations enriched by feedback from moderate-
and high-mass stars began to gain traction in the literature. This paper
briefly reviews the observational history of globular cluster abundance
inhomogeneities, discusses the presently favored models of their origin,
and considers several aspects of this problem that require further
study.

Highlight talk Astronomische Gesellschaft 2010</description>
</item>


<item>

<title>Sobeck, J. S.: The Abundances of Neutron-capture Species in the Very Metal-poor Globular Cluster M15: A Uniform Analysis of Red Giant Branch and Red Horizontal Branch Stars</title>
<link>http://cdsads.u-strasbg.fr/abs/2011AJ....141..175S</link>
<description>The globular cluster M15 is unique in its display of star-to-star
variations in the neutron-capture elements. Comprehensive abundance
surveys have been previously conducted for handfuls of M15 red giant
branch (RGB) and red horizontal branch (RHB) stars. No attempt has been
made to perform a single, self-consistent analysis of these stars, which
exhibit a wide range in atmospheric parameters. In the current effort, a
new comparative abundance derivation is presented for three RGB and six
RHB members of the cluster. The analysis employs an updated version of
the line transfer code MOOG, which now appropriately treats coherent,
isotropic scattering. The apparent discrepancy in the previously
reported values for the metallicity of M15 RGB and RHB stars is
addressed and a resolute disparity of Δ(RHB - RGB) ≈ 0.1
dex in the iron abundance was found. The anti-correlative behavior of
the light neutron-capture elements (Sr, Y, Zr) is clearly demonstrated
with both Ba and Eu, standard markers of the s- and r-process,
respectively. No conclusive detection of Pb was made in the RGB targets.
Consequently for the M15 cluster, this suggests that the main component
of the s-process has made a negligible contribution to those elements
normally dominated by this process in solar system material.
Additionally for the M15 sample, a large Eu abundance spread is
confirmed, which is comparable to that of the halo field at the same
metallicity. These abundance results are considered in the discussion of
the chemical inhomogeneity and nucleosynthetic history of M15.</description>
</item>


<item>

<title>Gonzalez, O. A.: Alpha element abundances and gradients in the Milky Way bulge from FLAMES-GIRAFFE spectra of 650 K giants</title>
<link>http://cdsads.u-strasbg.fr/abs/2011A%26A...530A..54G</link>
<description>&lt;BR /&gt; Aims: We present the analysis of the [α/Fe] abundance
ratios for a large number of stars at several locations in the Milky Way
bulge with the aim of constraining its formation scenario. &lt;BR /&gt;
Methods: We obtained FLAMES-GIRAFFE spectra (R = 22 500) at the ESO Very
Large Telescope for 650 bulge red giant branch (RGB) stars and performed
spectral synthesis to measure Mg, Ca, Ti, and Si abundances. This sample
is composed of 474 giant stars observed in 3 fields along the minor axis
of the Galactic bulge and at latitudes b = -4°, b = -6°, b =
-12°. Another 176 stars belong to a field containing the globular
cluster NGC 6553, located at b = -3° and 5° away from the other
three fields along the major axis. Stellar parameters and metallicities
for these stars were presented in Zoccali et al. (2008, A&#38;A, 486,
177). We have also re-derived stellar parameters and abundances for the
sample of thick and thin disk red giants analyzed in Alves-Brito et al.
(2010, A&#38;A, 513, A35). Therefore using a homogeneous abundance
database for the bulge, thick and thin disk, we have performed a
differential analysis minimizing systematic errors, to compare the
formation scenarios of these Galactic components. &lt;BR /&gt; Results: Our
results confirm, with large number statistics, the chemical similarity
between the Galactic bulge and thick disk, which are both enhanced in
alpha elements when compared to the thin disk. In the same context, we
analyze [α/Fe] vs. [Fe/H] trends across different bulge regions.
The most metal rich stars, showing low [α/Fe] ratios at b =
-4° disappear at higher Galactic latitudes in agreement with the
observed metallicity gradient in the bulge. Metal-poor stars ([Fe/H]
&#60; -0.2) show a remarkable homogeneity at different bulge locations.
&lt;BR /&gt; Conclusions: We have obtained further constrains for the
formation scenario of the Galactic bulge. A metal-poor component
chemically indistinguishable from the thick disk hints for a fast and
early formation for both the bulge and the thick disk. Such a component
shows no variation, neither in abundances nor kinematics, among
different bulge regions. A metal-rich component showing low [α/Fe]
similar to those of the thin disk disappears at larger latitudes. This
allows us to trace a component formed through fast early mergers
(classical bulge) and a disk/bar component formed on a more extended
timescale.

Based on observations collected at the European Southern Observatory,
Paranal, Chile (ESO programmes 071.B-0617 and 073.B-0074.Full Table 4 is
only available at the CDS via anonymous ftp to cdsarc.u-strasbg.fr
(130.79.128.5) or via &lt;A
href=&quot;http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/530/A54&quot;&gt;http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/530/A54&lt;/A&gt;</description>
</item>


<item>

<title>Lane, R. R.: AAOmega spectroscopy of 29 351 stars in fields centered on ten Galactic globular clusters</title>
<link>http://cdsads.u-strasbg.fr/abs/2011A%26A...530A..31L</link>
<description>Galactic globular clusters have been pivotal in our understanding of
many astrophysical phenomena. Here we publish the extracted stellar
parameters from a recent large spectroscopic survey of ten globular
clusters. A brief review of the project is also presented. Stellar
parameters have been extracted from individual stellar spectra using
both a modified version of the RAdial Velocity Experiment (RAVE)
pipeline and a pipeline based on the parameter estimation method of
RAVE. We publish here all parameters extracted from both pipelines. We
calibrate the metallicity and convert this to [Fe/H] for each star and,
furthermore, we compare the velocities and velocity dispersions of the
Galactic stars in each field to the Besançon Galaxy model. We
find that the model does not correspond well with the data, indicating
that the model is probably of little use for comparisons with pencil
beam survey data such as this.

The data described in Tables 1-3 are only available at the CDS via
anonymous ftp to cdsarc.u-strasbg.fr (130.79.128.5) or via &lt;A
href=&quot;http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/530/A31&quot;&gt;http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/530/A31&lt;/A&gt;</description>
</item>


<item>

<title>Pipino, A.: An empirical calibration of Lick indices using Milky Way globular clusters</title>
<link>http://cdsads.u-strasbg.fr/abs/2011A%26A...530A..22P</link>
<description>&lt;BR /&gt; Aims: We provide an empirical calibration relation to convert
Lick indices into abundances for the integrated light of old, simple
stellar populations for a large range in the observed [Fe/H] and
[α/Fe]. This calibration supersedes the previously adopted ones
because it is based on the real abundance pattern of the stars instead
of the commonly adopted metallicity scale derived from the colours. &lt;BR
/&gt; Methods: We carried out a long-slit spectroscopic study of 23
Galactic globular clusters (GCs) for which detailed chemical abundances
in stars have previously been measured. The line-strength indices, as
defined by the Lick system and Serven and collaborators, were measured
in low-resolution integrated spectra of the GC light. The results were
compared to average abundances and abundance ratios in stars taken from
the compilation by Pritzl and collaborators, as well as synthetic
models. &lt;BR /&gt; Results: The Fe-related indices increase linearly as a
function of [Fe/H] for [Fe/H] &#62; - 2. The Mg-related indices respond
in a similar way to [Mg/H] variations, although Mgb turns out to be a
less reliable metallicity indicator for [Z/H] &#60; - 1.5. Despite our
knowledge of the Mg overabundance with respect to Fe in GC stars, we are
unable to infer a mean [Mg/Fe] for the integrated spectra that
correlates with the resolved stars properties, because the sensitivity
of the indices to [Mg/Fe] is smaller at lower metallicities. We present
empirical calibrations for Ca, TiO, Ba, and Eu indices, as well as the
measurements of H&lt;SUB&gt;α&lt;/SUB&gt; and NaD.

Based on observations collected at the European Southern Observatory,
Chile, programs 0.77B0195(A) and (B).Appendices are available in
electronic form at &lt;A
href=&quot;http://www.aanda.org&quot;&gt;http://www.aanda.org&lt;/A&gt;</description>
</item>


<item>

<title>Froebrich, D.: Old star clusters in the FSR catalogue (Froebrich+, 2010)</title>
<link>http://cdsads.u-strasbg.fr/abs/2011yCat..74091281F</link>
<description>The sample of clusters analysed in this work is based on the FSR
catalogue. They determined a star density map based on 2MASS data
(Skrutskie et al. 2006, Cat. VII/233) along the entire Galactic plane
with |b|&#60;20°. Star cluster candidates were selected as local star
density enhancements and a total of 1788 objects were found. These
candidates were cross-referenced with the SIMBAD data base.

(3 data files).</description>
</item>


<item>

<title>McDonald, I.: Fundamental stellar parameters in 47 Tucanae (Mcdonald+, 2011)</title>
<link>http://cdsads.u-strasbg.fr/abs/2011yCat..21930023M</link>
<description>The photometric data used in the SEDs come from a variety of different
sources covering different fields of view. These data are summarized in
Figure 1 and Table 1.

(2 data files).</description>
</item>


<item>

<title>Howe, R.: Imaging M15 with a Small Aperture Telescope by Treating the Core as a Single Star</title>
<link>http://cdsads.u-strasbg.fr/abs/2011SASS...30..115H</link>
<description>The objective for this study will be to explore various time series
methods using CCD photometry for use with amateur telescope observations
of the dense globular cluster M15. Amateur telescopes are defined here
as having an aperture of less than 40 cm, and are collecting photometric
filtered observations over time. Specifically, we attempt to determine
the light curve of the core of M15 as a &quot;single star&quot;. This requires
selection of comparison and check stars to perform differential
photometry; i.e. subtraction of flux density measures between a
nonvariable (reference star) and the variable &quot;single star&quot; of the M15
core as it changes in magnitudes over time. We explore the possibility
of measuring the M15 periodicity as an aggregate of many standard stars
as identified in the Stetson catalog for NGC7078 (2010). In this paper
we'd like to propose methods and techniques for aggregating different
cluster region's flux densities (luminosity) and periods.</description>
</item>


<item>

<title>Kryachko, T.: New Variable Stars in the Field of the Globular Cluster NGC5466</title>
<link>http://cdsads.u-strasbg.fr/abs/2011PZP....11...20K</link>
<description>Not Available</description>
</item>


<item>

<title>di Criscienzo, M.: NGC 2419: a large and extreme second generation in a currently undisturbed cluster</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.tmp..791D</link>
<description>We analyse complementary Hubble Space Telescope and Subaru data for the
globular cluster NGC 2419. We make a detailed analysis of the horizontal
branch (HB), which is composed of two main groups of stars: the luminous
blue HB stars, which extend by evolution into the RR Lyrae and red HB
region, and a fainter, extremely blue population. We examine the
possible models for the latter group and conclude that a plausible
explanation is that they correspond to a significant (˜30 per
cent) extreme second generation with a strong helium enhancement
(Y˜ 0.4). We also show that the colour dispersion of the red giant
branch is consistent with this hypothesis, while the main-sequence data
are compatible with it, although the large observational error blurs the
possible underlying splitting.

While it is common to find an even larger (50-80) percentage of second
generation in a globular cluster, the presence of a substantial and
extreme fraction of these stars in NGC 2419 might be surprising, as the
cluster is at present well inside the radius beyond which the Galactic
tidal field would be dominant. If a similar situation had been present
in the first stages of the cluster life, then the cluster would have
retained its initial mass and the percentage of second-generation stars
would have been quite small (up to ˜10 per cent). Such a large
fraction of extreme second-generation stars implies that the system must
have been initially much more massive and in different dynamical
conditions from what it is today. We discuss this issue in the light of
existing models of the formation of multiple populations in globular
clusters.</description>
</item>


<item>

<title>D'Ercole, A.: Formation of multiple populations in globular clusters: constraints on the dilution by pristine gas</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.tmp..736D</link>
<description>The star-to-star differences in the abundance of light elements observed
in the globular clusters (GCs) can be explained assuming that a second
generation (SG) of stars form in the gas ejected by the asymptotic giant
branch (AGB) stars belonging to a first stellar generation. However,
while Na and O appear to be anticorrelated in the cluster stars, from
the stellar models they turn out to be correlated in the AGB ejecta. In
order to reconcile the stellar theory with the observational findings,
all the GC models invoke an early dilution of AGB ejecta with pristine
gas occurring during the SG formation. Despite a vast consensus about
the occurrence of such a dilution, the physical process behind it is
still unknown. In the present paper we set some general constraints on
the pristine gas dynamics and on the possible amount of pristine gas
involved in the SG formation, making use of a one-zone chemical model.
We find that such a dilution is a necessary ingredient in the SG star
formation to explain the observed abundance patterns. We confirm the
conclusion of our previous works showing that clusters must have been
initially much more massive. We also show that models assuming that
clusters had an initial mass similar to their current one, and adopting
a large fraction of pristine gas to form SG stars, fail to reproduce the
observed Na-O anticorrelation and are not viable. We finally show that
the dilution event should be restricted in time, rather than extended
for the full duration of SG formation.</description>
</item>


<item>

<title>Das, P.: Using NMAGIC to probe the dark matter halo and orbital structure of the X-ray bright, massive elliptical galaxy, NGC 4649</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.tmp..715D</link>
<description>We create dynamical models of the massive elliptical galaxy, NGC 4649,
using the N-body made-to-measure code, NMAGIC, and kinematic constraints
from long-slit and planetary nebula (PN) data. We explore a range of
potentials based on previous determinations from X-ray observations and
a dynamical model fitting globular cluster (GC) velocities and a stellar
density profile. The X-ray mass distributions are similar in the central
region but have varying outer slopes, while the GC mass profile is
higher in the central region and on the upper end of the range further
out. Our models cannot differentiate between the potentials in the
central region, and therefore if non-thermal pressures or multi-phase
components are present in the hot gas, they must be smaller than
previously inferred. In the halo, we find that the PN velocities are
sensitive tracers of the mass, preferring a less massive halo than that
derived from the GC mass profile, but similar to one of the mass
distributions derived from X-rays. Our results show that the GCs may
form a dynamically distinct system, and that the properties of the hot
gas derived from X-rays in the outer halo have considerable
uncertainties that need to be better understood. Estimating the mass in
stars using photometric information and a stellar population
mass-to-light ratio, we infer a dark matter mass fraction in NGC 4649 of
˜0.39 at 1R&lt;SUB&gt;e&lt;/SUB&gt; (10.5 kpc) and ˜0.78 at
4R&lt;SUB&gt;e&lt;/SUB&gt;. We find that the stellar orbits are isotropic to mildly
radial in the central ˜6 kpc depending on the potential assumed.
Further out, the orbital structure becomes slightly more radial along R
and more isotropic along z, regardless of the potential assumed. In the
equatorial plane, azimuthal velocity dispersions dominate over
meridional velocity dispersions, implying that meridional velocity
anisotropy is the mechanism for flattening the stellar system.</description>
</item>


<item>

<title>Walker, A. R.: Constraints on the formation of the globular cluster IC 4499 from multiwavelength photometry</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.tmp..702W</link>
<description>We present new multiband photometry for the Galactic globular cluster IC
4499 extending well past the main-sequence turn-off in the U, B, V, R, I
and DDO 51 bands. This photometry is used to determine that IC 4499 has
an age of 12 ± 1 Gyr and a cluster reddening of E(B-V) = 0.22
± 0.02. Hence, IC 4499 is coeval with the majority of Galactic
globular clusters, in contrast to suggestions of a younger age. The
density profile of the cluster is observed to not flatten out to at
least r˜ 800 arcsec, implying that either the tidal radius of this
cluster is larger than previously estimated, or that IC 4499 is
surrounded by a halo. Unlike the situation in some other, more massive,
globular clusters, no anomalous colour spreads in the ultraviolet are
detected among the red giant branch stars. The small uncertainties in
our photometry should allow the detection of such signatures apparently
associated with variations of light elements within the cluster,
suggesting that IC 4499 consists of a single stellar population. Based
in part on observations made with the European Southern Observatory
telescopes obtained from the ESO/ST-ECF Science Archive Facility.</description>
</item>


<item>

<title>Misgeld, I.: Families of dynamically hot stellar systems over 10 orders of magnitude in mass</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.tmp..694M</link>
<description>Dynamically hot stellar systems, whether star clusters or early-type
galaxies, follow well-defined scaling relations over many orders of
magnitudes in mass. These Fundamental Plane relations have been subject
of several studies, which have been mostly confined to certain types of
galaxies and/or star clusters so far. Here, we present a complete
picture of hot stellar systems ranging from faint galaxies and star
clusters of only a few hundred solar masses up to giant ellipticals
(gEs) with 10&lt;SUP&gt;12&lt;/SUP&gt; M&lt;SUB&gt;ȯ&lt;/SUB&gt;, in particular including -
for the first time - large samples of compact ellipticals (cEs),
ultracompact dwarf galaxies (UCDs), dwarf ellipticals (dEs) of nearby
galaxy clusters and Local Group ultrafaint dwarf spheroidals (dSphs).
For all those stellar systems we show the effective radius luminosity,
effective radius stellar mass and effective mass surface density stellar
mass plane. Two clear families of hot stellar systems can be
differentiated: the 'galaxian' family, ranging from gEs over ellipticals
(Es) and dEs to dSphs, and the 'star cluster' family, comprising
globular clusters (GCs), UCDs and nuclear star clusters (NCs).
Interestingly, massive Es have a similar size-mass relation as cEs, UCDs
and NCs, with a clear common boundary towards minimum sizes, which can
be approximated by R&lt;SUB&gt;eff&lt;/SUB&gt;≥ 2.24 ×
10&lt;SUP&gt;-6&lt;/SUP&gt;M&lt;SUP&gt;4/5&lt;/SUP&gt;&lt;SUB&gt;★&lt;/SUB&gt; pc. No object of either
family is located in the 'zone of avoidance' beyond this limit. Even the
majority of early-type galaxies at high redshift obeys this relation.
The sizes of dEs and dSphs (R&lt;SUB&gt;eff&lt;/SUB&gt;˜ 1.0 kpc) as well as
GCs (R&lt;SUB&gt;eff&lt;/SUB&gt;˜ 3 pc) barely vary with mass over several
orders of magnitude. We use the constant galaxy sizes to derive the
distances of several local galaxy clusters. The size gap between star
clusters and dwarf galaxies gets filled in by low mass, resolving star
clusters and the faintest dSphs at the low mass end, and by GCs/UCDs,
NCs and cEs in the mass range 10&lt;SUP&gt;6&lt;/SUP&gt; &#60; M&lt;SUB&gt;★&lt;/SUB&gt;
&#60; 10&lt;SUP&gt;9&lt;/SUP&gt; M&lt;SUB&gt;ȯ&lt;/SUB&gt;. In the surface density-mass
plane the sequences of star clusters and galaxies show the same slope,
but are displaced with respect to each other by 10&lt;SUP&gt;3&lt;/SUP&gt; in mass
and 10&lt;SUP&gt;2&lt;/SUP&gt; in surface density. Objects that fall in between both
sequences include cEs, UCDs, NCs and ultrafaint dSphs. Both, galaxies
and star clusters, do not exceed a surface density of
Σ&lt;SUB&gt;eff&lt;/SUB&gt;= 3.17 ×
10&lt;SUP&gt;10&lt;/SUP&gt;M&lt;SUP&gt;-3/5&lt;/SUP&gt;&lt;SUB&gt;★&lt;/SUB&gt; M&lt;SUB&gt;ȯ&lt;/SUB&gt;
pc&lt;SUP&gt;-2&lt;/SUP&gt;, causing an orthogonal kink in the galaxy sequence for
Es more massive than 10&lt;SUP&gt;11&lt;/SUP&gt; M&lt;SUB&gt;ȯ&lt;/SUB&gt;. The densest
stellar systems (within their effective radius) are NCs.</description>
</item>


<item>

<title>Schaerer, D.: A new perspective on globular clusters, their initial mass function and their contribution to the stellar halo and the cosmic reionization</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.413.2297S</link>
<description>We examine various implications from a dynamical and chemical model of
globular clusters (GCs), which successfully reproduces the observed
abundance patterns and the multiple populations of stars in these
systems assuming chemical enrichment from fast-rotating massive stars.
Using the model of Decressin et al., we determine the ratio between the
observed, present-day mass of GCs and their initial stellar mass as a
function of the stellar initial mass function (IMF). We also compute the
mass of low-mass stars ejected and the amount of hydrogen ionizing
photons emitted by the proto-GCs. Typically, we find that the initial
masses of GCs must be ˜8-10 times (or up to 25 times, if
second-generation stars also escape from GCs) larger than the
present-day stellar mass. The present-day Galactic GC population must
then have contributed to approximately 5-8 per cent (10-20 per cent) of
the low-mass stars in the Galactic halo. We also show that the detection
of second-generation stars in the Galactic halo, recently announced by
different groups, provides a new constraint on the GC IMF (GCIMF). These
observations appear to rule out a power-law GCIMF, whereas they are
compatible with a lognormal one. Finally, the high initial masses also
imply that GCs must have emitted a large amount of ionizing photons in
the early Universe. Our results reopen the question on the IMF of GCs
and reinforce earlier conclusions that old GCs could have represented a
significant contribution to reionize the intergalactic medium at high
redshift.</description>
</item>


<item>

<title>Church, R. P.: Implications for the origin of short gamma-ray bursts from their observed positions around their host galaxies</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.413.2004C</link>
<description>We present the observed offsets of short-duration gamma-ray bursts
(SGRBs) from their putative host galaxies and compare them with the
expected distributions of merging compact object binaries, given the
observed properties of the hosts. We find that for all but one burst in
our sample the offsets are consistent with this model. For the case of
bursts with massive elliptical host galaxies, the circular velocities of
the hosts' haloes exceed the natal velocities of almost all our compact
object binaries. Hence, the extents of the predicted offset
distributions for elliptical galaxies are determined largely by their
spatial extents. In contrast, for spiral hosts, the galactic rotation
velocities are smaller than typical binary natal velocities and the
predicted burst offset distributions are more extended than the
galaxies.

One SGRB, 060502B, apparently has a large radial offset that is
inconsistent with an origin in a merging galactic compact binary.
Although it is plausible that the host of GRB 060502B is misidentified,
our results show that the large offset is compatible with a scenario
where at least a few per cent of SGRBs are created by the merger of
compact binaries that form dynamically in globular clusters.</description>
</item>


<item>

<title>Paudel, S.: Nuclei of early-type dwarf galaxies: insights from stellar populations</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.413.1764P</link>
<description>We present a comprehensive analysis of the spatially resolved stellar
population properties of 26 early-type dwarf galaxies (dEs) in the Virgo
cluster. Using Lick/IDS absorption line indices we derive simple stellar
population (SSP) equivalent age, metallicity and [α/Fe] abundance
ratio. In particular, we focus on the comparison of the stellar
populations between the central nucleus and the surrounding galactic
main body. The stellar populations of the nuclei are, for most dEs,
significantly younger than those of the respective galactic main bodies,
with an average difference of 3.5 Gyr. We find only five dEs with
significantly older nuclei than their galactic main bodies. Furthermore,
we observe most dE nuclei to be more metal rich compared to their host
galaxies. These age and metallicity behaviours are shown by almost all
dEs brighter than M&lt;SUB&gt;r&lt;/SUB&gt;=-17 mag.

The metallicity of both nuclei and galactic main bodies correlates with
the total luminosity of the dEs. However, the metallicity of the nuclei
covers a larger range (+0.18 to -1.22 dex) than that of the galactic
main bodies, which all have subsolar metallicity. The ages of dE nuclei
show a statistically significant correlation with the local projected
galaxy density within the cluster, such that younger ages are
predominantly observed outside of the high-density central cluster
region. The α-element abundance ratios are consistent with solar
for both nuclei and galactic main bodies.

We also examine the presence of radial gradients in the SSP parameters
for a subset of 13 dEs (up to 1.2 kpc or 15 arcsec radius). We notice
two different types of gradients, namely smooth profiles that include
the nucleus, and profiles where a break occurs between the nucleus and
the rest of the galaxy. Nevertheless, an overall trend of increasing age
and decreasing metallicity with radius exists, consistent with earlier
studies. The α-abundance ratio as function of radius is consistent
with no gradient.

Possible formation scenarios for the nuclei of dEs are discussed. The
young and metal-enhanced population of nuclei suggests that these might
have formed at later epochs, or the termination of star formation
activity in the nuclei might have occurred relatively late, perhaps due
to continuous infall of gas into the central potential well. Our stellar
population analysis suggests that the merging of globular clusters is
not an appropriate scenario for the formation of most dE nuclei, at
least not for the brighter dEs. We speculate that there might be
different formation processes which are responsible for the formation of
dEs and their nuclei depending on their luminosity. Based on
observations collected at the European Organization for Astronomical
Research in the Southern hemisphere, Chile (programme 078.B-0178).</description>
</item>


<item>

<title>Bramich, D. M.: CCD time-series photometry of the globular cluster NGC 6981: variable star census and physical parameter estimates</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.413.1275B</link>
<description>We present the results from 10 nights of observations of the globular
cluster NGC 6981 (M72) in the V, R and I Johnson wavebands. We employed
the technique of difference image analysis to perform precision
differential photometry on the time-series images, which enabled us to
carry out a census of the understudied variable star population of the
cluster. We show that 20 suspected variables in the literature are
actually non-variable, and we confirm the variable nature of another 29
variables while refining their ephemerides. We also detect 11 new RR
Lyrae variables and three new SX Phe variables, bringing the total
confirmed variable star count in NGC 6981 to 43. We performed Fourier
decomposition of the light curves for a subset of RR Lyrae stars and
used the Fourier parameters to estimate the fundamental physical
parameters of the stars using relations available in the literature.
Mean values of these physical parameters have allowed us to estimate the
physical parameters of the parent cluster. We derive a metallicity of
[Fe/H]&lt;SUB&gt;ZW&lt;/SUB&gt;≈-1.48 ± 0.03 on the Zinn &#38; West scale
(or [Fe/H]&lt;SUB&gt;UVES&lt;/SUB&gt;≈-1.38 ± 0.03 on the new Carretta et
al. scale) for NGC 6981, and distances of ˜16.73 ± 0.36 and
˜16.68 ± 0.36 kpc from analysis of the RR0 and RR1 stars
separately. We also confirm the Oosterhoff type I classification for the
cluster, and show that our colour-magnitude data are consistent with the
age of ˜12.75 ± 0.75 Gyr derived by Dotter et al.</description>
</item>


<item>

<title>Küpper, A. H. W.: The curious case of Palomar 13: the influence of the orbital phase on the appearance of galactic satellites</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.413..863K</link>
<description>We investigate the dynamical status of the low-mass globular cluster
Palomar 13 by means of N-body computations to test whether its unusually
high mass-to-light ratio of about 40 and its peculiarly shallow surface
density profile can be caused by tidal shocking. Alternatively, we test
- by varying the assumed proper motion - if the orbital phase of Palomar
13 within its orbit about the Milky Way can influence its appearance and
thus may be the origin of these peculiarities, as has been suggested by
Küpper et al. We find that, of these two scenarios, only the latter
can explain the observed mass-to-light ratio and surface density
profile. We note, however, that the particular orbit that best
reproduces those observed parameters has a proper motion inconsistent
with the available literature value. We discuss this discrepancy and
suggest that it may be caused by an underestimation of the observational
uncertainties in the proper motion determination. We demonstrate that
Palomar 13 is most likely near apogalacticon, which makes the cluster
appear supervirial and blown-up due to orbital compression of its tidal
debris. Since the satellites of the Milky Way are on average closer to
apogalacticon than perigalacticon, their internal dynamics may be
influenced by the same effect, and we advocate that this needs to be
taken into account when interpreting their kinematical data. Moreover,
we briefly discuss the influence of a possible binary population on such
measurements.</description>
</item>


<item>

<title>Mucciarelli, A.: NGC 1866: a milestone for understanding the chemical evolution of stellar populations in the Large Magellanic Cloud</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.413..837M</link>
<description>We present new FLAMES@VLT spectroscopic observations of 30 stars in the
field of the Large Magellanic Cloud (LMC) stellar cluster NGC 1866. NGC
1866 is one of the few young and massive globular clusters that is close
enough so that its stars can be individually studied in detail. Radial
velocities have been used to separate stars belonging to the cluster and
to the LMC field, and the same spectra have been used to derive chemical
abundances for a variety of elements, from [Fe/H] to the light (i.e. Na,
O, Mg, etc.) to the heavy ones. The average iron abundance of NGC 1866
turns out to be [Fe/H]=-0.43 ± 0.01 dex (with a dispersion
σ= 0.04 dex), from the analysis of 14 cluster member stars. Within
our uncertainties, the cluster stars are homogeneous, as far as chemical
composition is concerned, independent of the evolutionary status. The
observed cluster stars do not show any sign of the light elements'
‘anticorrelation’ present in all the Galactic globular
clusters so far studied and are also found in the old LMC stellar
clusters. A similar lack of anticorrelations has been detected in the
massive intermediate-age LMC clusters, indicating a different
formation/evolution scenario for the LMC massive clusters younger than
˜3 Gyr with respect to the old ones.

Also opposite to the Galactic globulars, the chemical composition of the
older red giant branch field stars and of the young post-main-sequence
cluster stars show robust homogeneity suggesting a quite similar process
of chemical evolution. The field and cluster abundances are in agreement
with recent chemical analysis of LMC stars, which show a distinctive
chemical pattern for this galaxy with respect to the Milky Way. We
discuss these findings in light of the theoretical scenario of chemical
evolution of the LMC.</description>
</item>


<item>

<title>Matsunaga, N.: Period-luminosity relations of type II Cepheids in the Magellanic Clouds</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.413..223M</link>
<description>Period-luminosity relations (PLRs) of type II Cepheids (T2Cs) in the
Small Magellanic Cloud (SMC) are derived based on OGLE-III, IRSF/SIRIUS
and other data, and these are compared with results for the Large
Magellanic Cloud (LMC) and Galactic globular clusters. Evidence is found
for a change of the PLR slopes from system to system. Treating the
longer period T2Cs (W Vir stars) separately gives an SMC-LMC modulus
difference of 0.39 ± 0.05 mag without any metallicity corrections
being applied. This agrees well with the difference in moduli based on
different distance indicators, in particular the PLRs of classical
Cepheids. The shorter period T2Cs (BL Her stars) give a smaller SMC-LMC
difference suggesting that their absolute magnitudes might be affected
either by metallicity or by age effects. It is shown that the frequency
distribution of T2C periods also changes from system to system.</description>
</item>


<item>

<title>Sharaf, M. A.: Analytical Solution for Stellar Density in Globular Clusters</title>
<link>http://cdsads.u-strasbg.fr/abs/2011JApA..tmp....1S</link>
<description>In this paper, four parameters analytical solution will be established
for the stellar density function in globular clusters. The solution
could be used for any arbitrary order of outward decrease of the
cluster's density.</description>
</item>


<item>

<title>Miller-Jones, J. C. A.: EVLA observations suggest that M15 X-2 is the currently flaring source in M15</title>
<link>http://cdsads.u-strasbg.fr/abs/2011ATel.3378....1M</link>
<description>Following the detection of an X-ray flare in the globular cluster M15
(ATel #3356) and its subsequent Swift XRT localization to the cluster
core (ATel #3363), we undertook EVLA observations to determine the
source of the flaring event. The 1-hour observation on 2011 May 22
(12:11-13:11 UT) comprises of two 1024-MHz bands centred at 5.0 and 7.0
GHz. The array was in its BnA configuration, providing an angular
resolution of 1.25 x 0.63 srq arcsec at 5 GHz and 0.92 x 0.50 sqr arcsec
at 7 GHz.</description>
</item>


<item>

<title>Heinke, C. O.: Swift/XRT measurement of position and X-ray spectrum of M15 X-ray binary</title>
<link>http://cdsads.u-strasbg.fr/abs/2011ATel.3363....1H</link>
<description>Following the MAXI/GSC detection of a recent flux increase and two X-ray
bursts from the position of the globular cluster M15 (Atel #3356), a
Swift XRT observation was conducted May 18 at 03:44 UT for 1.0 ks. The
XRT data are heavily piled up, and affected by a bad column. We find the
position by fitting a circle to the pileup ring, estimating a center at
RA, Dec (J2000)=21:29:57.9, +12:10:06 with a 90% conf.</description>
</item>


<item>

<title>Bazzano, A.: Announcement of INTEGRAL Galactic Plane monitoring program and detection of 2 new hard X-ray sources.</title>
<link>http://cdsads.u-strasbg.fr/abs/2011ATel.3361....1B</link>
<description>INTEGRAL commenced a new series of Galactic Plane Scans on May 14th
2011. Under an approved INTEGRAL AO-8 proposal (PI: Bazzano) the part of
the Galactic Plane visible by INTEGRAL will be scanned regularly, during
every INTEGRAL revolution (about every 3 days), for parts of AO-8, for a
total exposure time of 2Msec. &lt;BR /&gt;  We here report on quick-look
analysis of the observations performed in revolution 1048, covering the
period from UT 2011-05-14 at 05:21:38 to 2011-05-15 at 07:51:04 and
later from 2011-05-16 at 08:28:28 ending at 21:13:12 on two different
regions of the sky for a total duration 64 of and 41 ks, respectively.</description>
</item>


<item>

<title>Morii, M.: MAXI/GSC detection of X-ray activities in the globular cluster M15</title>
<link>http://cdsads.u-strasbg.fr/abs/2011ATel.3356....1M</link>
<description>We report recent activities of the globular cluster M15. MAXI/GSC
detected an X-ray burst at the scan transit centered at UT
2011-05-16T23:23:41. The burst was detected at least for 30.0 seconds
within the 50.5 seconds triangular transit response of MAXI/GSC. The
nominal location of the source, assuming that the source flux was
constant over the transit (which probably was not), is determined as &lt;BR
/&gt; &lt;BR /&gt; (R.A., Dec) = (+322.27 deg, +12.14 deg) = (21 29 6, +12 08
23)(J2000) &lt;BR /&gt; &lt;BR /&gt; with a rectangular 90% statistical error box
with the following corners: &lt;BR /&gt; &lt;BR /&gt; (R.A., Dec) = (+322.31 deg,
+11.95 deg) = (21 29 14, +11 57 11)(J2000) &lt;BR /&gt; (R.A., Dec) = (+322.06
deg, +12.10 deg) = (21 28 15, +12 06 9)(J2000) &lt;BR /&gt; (R.A., Dec) =
(+322.24 deg, +12.32 deg) = (21 28 57, +12 19 23)(J2000) &lt;BR /&gt; (R.A.,
Dec) = (+322.48 deg, +12.17 deg) = (21 29 56, +12 10 24)(J2000)&lt;BR /&gt; 
&lt;BR /&gt; There is additional systematic uncertainty of 0.2 degree (90%
containment radius).</description>
</item>


<item>

<title>De Propris, R.: Separating the Conjoined Red Clump in the Galactic Bulge: Kinematics and Abundances</title>
<link>http://cdsads.u-strasbg.fr/abs/2011ApJ...732L..36D</link>
<description>We have used the AAOMEGA spectrograph to obtain R ~ 1500 spectra of 714
stars that are members of two red clumps in the Plaut Window Galactic
bulge field (l, b) = (0°, - 8°). We discern no difference
between the clump populations based on radial velocities or abundances
measured from the Mgb index. The velocity dispersion has a strong trend
with Mgb-index metallicity, in the sense of a declining velocity
dispersion at higher metallicity. We also find a strong trend in mean
radial velocity with abundance. Our red clump sample shows distinctly
different kinematics for stars with [Fe/H] &#60;-1, which may
plausibly be attributable to a minority classical bulge or inner halo
population. The transition between the two groups is smooth. The
chemo-dynamical properties of our sample are reminiscent of those of the
Milky Way globular cluster system. If correct, this argues for no
bulge/halo dichotomy and a relatively rapid star formation history.
Large surveys of the composition and kinematics of the bulge clump and
red giant branch are needed to further define these trends.</description>
</item>


<item>

<title>King, A.: The Brightest Cluster X-ray Sources</title>
<link>http://cdsads.u-strasbg.fr/abs/2011ApJ...732L..28K</link>
<description>There have been several recent claims of black hole binaries in globular
clusters. I show that these candidate systems could instead be
ultracompact X-ray binaries (UCXBs) in which a neutron star accretes
from a white dwarf. They would represent a slightly earlier evolutionary
stage of known globular cluster UCXBs such as 4U 1820-30, with white
dwarf masses ~0.2 M &lt;SUB&gt;sun&lt;/SUB&gt; and orbital periods below 5 minutes.
Accretion is slightly super-Eddington and makes these systems
ultraluminous sources with rather mild beaming factors b ~ 0.3. Their
theoretical luminosity function flattens slightly just above L
&lt;SUB&gt;Edd&lt;/SUB&gt; and then steepens at ~3L &lt;SUB&gt;Edd&lt;/SUB&gt;. It predicts of
order two detections in elliptical galaxies such as NGC 4472, as
observed. The very bright X-ray source HLX-1 lies off the plane of its
host S0a galaxy. If this is an indication of globular cluster
membership, it could conceivably be a more extreme example of a UCXB
with white dwarf mass M &lt;SUB&gt;2&lt;/SUB&gt; ~= 0.34 M &lt;SUB&gt;sun&lt;/SUB&gt;. The
beaming here is tighter (b ~ (2.5-9) × 10&lt;SUP&gt;-3&lt;/SUP&gt;), but
the system's distance of 95 Mpc easily eliminates any need to invoke
improbable alignment of the beam for detection. If its position instead
indicates membership of a satellite dwarf galaxy, HLX-1 could have a
much higher accretor mass ~1000 M &lt;SUB&gt;sun&lt;/SUB&gt;</description>
</item>


<item>

<title>Roederer, I. U.: Primordial r-process Dispersion in Metal-poor Globular Clusters</title>
<link>http://cdsads.u-strasbg.fr/abs/2011ApJ...732L..17R</link>
<description>Heavy elements, those produced by neutron-capture reactions, have
traditionally shown no star-to-star dispersion in all but a handful of
metal-poor globular clusters (GCs). Recent detections of low [Pb/Eu]
ratios or upper limits in several metal-poor GCs indicate that the heavy
elements in these GCs were produced exclusively by an r-process.
Re-examining GC heavy element abundances from the literature, we find
unmistakable correlations between the [La/Fe] and [Eu/Fe] ratios in four
metal-poor GCs (M5, M15, M92, and NGC 3201), only two of which were
known previously. This indicates that the total r-process abundances
vary from star to star (by factors of 2-6) relative to Fe within each
GC. We also identify potential dispersion in two other GCs (M3 and M13).
Several GCs (M12, M80, and NGC 6752) show no evidence of r-process
dispersion. The r-process dispersion is not correlated with the
well-known light element dispersion, indicating that it was present in
the gas throughout the duration of star formation. The observations
available at present suggest that star-to-star r-process dispersion
within metal-poor GCs may be a common but not ubiquitous phenomenon that
is neither predicted by nor accounted for in current models of GC
formation and evolution.</description>
</item>


<item>

<title>Guillot, S.: Neutron Star Radius Measurement with the Quiescent Low-mass X-ray Binary U24 in NGC 6397</title>
<link>http://cdsads.u-strasbg.fr/abs/2011ApJ...732...88G</link>
<description>This paper reports the spectral and timing analyses of the quiescent
low-mass X-ray binary (qLMXB) U24 observed during five archived
Chandra/ACIS exposures of the nearby globular cluster NGC 6397, for a
total of 350 ks. We find that the X-ray flux and the parameters of the
hydrogen atmosphere spectral model are consistent with those previously
published for this source. On short timescales, we find no evidence of
aperiodic intensity variability, with 90% confidence upper limits during
five observations ranging between &#60;8.6% rms and &#60;19% rms, in the
0.0001-0.1 Hz frequency range (0.5-8.0 keV); and no evidence of periodic
variability, with maximum observed powers in this frequency range having
a chance probability of occurrence from a Poisson-deviated light curve
in excess of 10%. We also report the improved neutron star (NS) physical
radius measurement, with statistical accuracy of the order of ~10%: R
&lt;SUB&gt;NS&lt;/SUB&gt; = 8.9&lt;SUP&gt;+0.9&lt;/SUP&gt; &lt;SUB&gt;-0.6&lt;/SUB&gt; km for M
&lt;SUB&gt;NS&lt;/SUB&gt; = 1.4 M &lt;SUB&gt;sun&lt;/SUB&gt;. Alternatively, we provide the
confidence regions in mass-radius space as well as the best-fit
projected radius R &lt;SUB&gt;∞&lt;/SUB&gt; = 11.9&lt;SUP&gt;+1.0&lt;/SUP&gt;
&lt;SUB&gt;-0.8&lt;/SUB&gt; km, as seen by an observer at infinity. The
best-fit effective temperature, kT &lt;SUB&gt;eff&lt;/SUB&gt; = 80&lt;SUP&gt;+4&lt;/SUP&gt;
&lt;SUB&gt;-5&lt;/SUB&gt; eV, is used to estimate the NS core temperature
which falls in the range T &lt;SUB&gt;core&lt;/SUB&gt; = (3.0-9.8) ×
10&lt;SUP&gt;7&lt;/SUP&gt; K, depending on the atmosphere model considered. This
makes U24 the third most precisely measured NS radius among qLMXBs,
after those in ω Cen and M13.</description>
</item>


<item>

<title>Murphy, B. W.: Fokker-Planck Models for M15 Without a Central Black Hole: The Role of the Mass Function</title>
<link>http://cdsads.u-strasbg.fr/abs/2011ApJ...732...67M</link>
<description>We have developed a set of dynamically evolving Fokker-Planck models for
the collapsed-core globular star cluster M15, which directly address the
issue of whether a central black hole is required to fit Hubble Space
Telescope (HST) observations of the stellar spatial distribution and
kinematics. As in our previous work reported by Dull et al., we find
that a central black hole is not needed. Using local mass-function data
from HST studies, we have also inferred the global initial stellar mass
function. As a consequence of extreme mass segregation, the local mass
functions differ from the global mass function at every location. In
addition to reproducing the observed mass functions, the models also
provide good fits to the star-count and velocity-dispersion profiles,
and to the millisecond pulsar accelerations. We address concerns about
the large neutron star populations adopted in our previous Fokker-Planck
models for M15. We find that good model fits can be obtained with as few
as 1600 neutron stars; this corresponds to a retention fraction of 5% of
the initial population for our best-fit initial mass function. The
models contain a substantial population of massive white dwarfs, that
range in mass up to 1.2M&lt;SUB&gt;sun&lt;/SUB&gt; . The combined contribution by
the massive white dwarfs and neutron stars provides the gravitational
potential needed to reproduce HST measurements of the central
velocity-dispersion profile.</description>
</item>


<item>

<title>Stacey, W. S.: Transient Extremely Soft X-ray Emission from the Unusually Bright Cataclysmic Variable in the Globular Cluster M3: A New CV X-ray Luminosity Record?</title>
<link>http://cdsads.u-strasbg.fr/abs/2011ApJ...732...46S</link>
<description>We observed the accreting white dwarf (WD) 1E1339.8+2837 (1E1339) in the
globular cluster M3 in 2003 November, 2004 May, and 2005 January, using
the Chandra ACIS-S detector. The source was observed in 1992 to possess
traits of a supersoft X-ray source (SSS), with a 0.1-2.4 keV luminosity
as large as 2 × 10&lt;SUP&gt;35&lt;/SUP&gt; erg s&lt;SUP&gt;-1&lt;/SUP&gt;, after
which time the source's luminosity fell by roughly two orders of
magnitude, adopting a hard X-ray spectrum more typical of cataclysmic
variables (CVs). Our observations confirm 1E1339's hard CV-like
spectrum, with photon index Γ = 1.3 ± 0.2. We found 1E1339
to be highly variable, with a 0.5-10 keV luminosity ranging from (1.4
± 0.3) × 10&lt;SUP&gt;34&lt;/SUP&gt; erg s&lt;SUP&gt;-1&lt;/SUP&gt; to
8.5&lt;SUP&gt;+4.9&lt;/SUP&gt; &lt;SUB&gt;- 4.6&lt;/SUB&gt; × 10&lt;SUP&gt;32&lt;/SUP&gt; erg
s&lt;SUP&gt;-1&lt;/SUP&gt;, with 1E1339's maximum luminosity being perhaps the
highest yet recorded for hard X-ray emission from a WD. In 2005 January,
1E1339 displayed substantial low-energy emission below ~0.3 keV.
Although current Chandra responses cannot properly model this emission,
its bolometric luminosity appears comparable to or greater than that of
the hard spectral component. This raises the possibility that the
supersoft X-ray emission seen from 1E1339 in 1992 may have shifted to
the far-UV.</description>
</item>


<item>

<title>Alonso-García, J.: Mapping Differential Reddening in the Inner Galactic Globular Cluster System</title>
<link>http://cdsads.u-strasbg.fr/abs/2011AJ....141..146A</link>
<description>A serious limitation in the study of many globular
clusters—especially those located near the Galactic
center—has been the existence of large and differential extinction
by foreground dust. In a series of papers, we intend to map the
differential extinction and remove its effects, using a new dereddening
technique, in a sample of clusters in the direction of the inner Galaxy,
observed using the Magellan 6.5 m telescope and the Hubble Space
Telescope. These observations and their analysis will let us produce
high-quality color-magnitude diagrams of these poorly studied clusters
that will allow us to determine these clusters' relative ages,
distances, and chemistry and to address important questions about the
formation and the evolution of the inner Galaxy. We also intend to use
the maps of the differential extinction to sample and characterize the
interstellar medium along the numerous low-latitude lines of sight where
the clusters in our sample lie. In this first paper, we describe in
detail our dereddening method along with the powerful statistics tools
that allow us to apply it, and we show the kind of results that we can
expect, applying the method to M62, one of the clusters in our sample.
The width of the main sequence and lower red giant branch narrows by a
factor of two after applying our dereddening technique, which will
significantly help to constrain the age, distance, and metallicity of
the cluster.

Based partly on observations with the NASA/ESA Hubble Space Telescope,
obtained at the Space Telescope Science Institute, which is operated by
the Association of Universities for Research in Astronomy, Inc., under
NASA contract NAS 5-26555. This paper also includes data gathered with
the 6.5 m Magellan Telescopes located at Las Campanas Observatory,
Chile.</description>
</item>


<item>

<title>Lin, C.-C.: Search For And Characterization Of Galactic Star Clusters With 2MASS And Pan-STARRS 1</title>
<link>http://cdsads.u-strasbg.fr/abs/2011AAS...21840712L</link>
<description>We plan to conduct a comprehensive search for uncatalogued galactic open
clusters using Pan-STARRS (Panoramic Survey Telescope And Rapid Response
System) data in five optical bands (g, r, i, z, y) to a depth of  24
magnitude, about 100 times more sensitive than currently available
surveys. A ``star-count'' pipeline has been tested on the 2MASS
point-source catalog. In a demonstration region with a sky coverage
between galactic longitude 2 &#60; l &#60; 358 degrees and galactic
latitude |b| &#60; 50 degrees, we identified 502 cluster candidates. Of
these, two are galaxies, 32 (6.3%) are cluster of galaxies, 91 (18.1%)
are globular clusters, and 360 (71.7%) are open clusters. Seventeen
(3.3%) of our candidates are newly identified. Overall, the detection
rate of stellar clusters using our algorithm is about 90%. In addition,
we have characterized some of the fundamental parameters of clusters,
such as age and distance, using the Pan-STARRS 1 photometry, and the
results are in good agreement with previous results.</description>
</item>


<item>

<title>Cohen, R.: The Connection Between SX Phe and Blue Stragglers: Globular Cluster Variables as Period-Luminosity Relation Calibrators</title>
<link>http://cdsads.u-strasbg.fr/abs/2011AAS...21832209C</link>
<description>The number of known SX Phoenicis (SX Phe) pulsators in Galactic globular
clusters (GGCs) and the Local Group has more than doubled in recent
years. Because all SX Phe in GGCs are likely blue stragglers, it has
been suggested that their pulsational properties can constrain their
evolutionary histories. We investigate the connection between SX Phe and
blue stragglers via period-luminosity and color-magnitude diagrams. In
particular, we verify distances to a large set of GGCs by fitting a
carefully chosen set of nearby, unevolved subdwarfs to the cluster main
sequences. We use these distances to analyze the pulsational properties
of all known SX Phe, including SX Phe period-luminosity relations
obtained using the SX Phe in these GGCs as calibrators, together with
those in Local Group dwarf galaxies and their clusters. Finally, we
discuss implications for blue straggler formation and evolution, and
address both observational and theoretical avenues for further
investigation.</description>
</item>


<item>

<title>Majaess, D.: Securing the Distance Scale via a Universal VI Wesenheit Template and Deep Infrared ZAMS</title>
<link>http://cdsads.u-strasbg.fr/abs/2011AAS...21832208M</link>
<description>HST, VLBA, and HIP geometric distances to SX Phe, Delta Scuti, RR Lyrae,
Type II and classical Cepheid variables are used to construct a
universal VI Wesenheit template. The template uses the statistical
weight of the entire variable star demographic to establish precise
(&#60;5%) distances to nearby galaxies, star clusters, etc. The
reddening-free nature of the Wesenheit approach obviates the propagation
of uncertainties tied to tentative total/differential extinction
corrections, ensuring that further calibration may ensue directly from
published or forthcoming geometric-based distances (masers, HST, GAIA,
SIM). An empirical JHKs ZAMS established from deep 2MASS photometry and
precise HIP parallaxes for nearby stars provides a concurrent means of
securing absolute Wesenheit magnitudes for variables in stellar clusters
(calibrators). The infrared ZAMS is comparatively insensitive to stellar
age and [Fe/H], and yields distances to 7 of 9 benchmark open clusters
that agree with the van Leeuwen (2009) revised HIP estimates (the
Pleiades and Blanco 1 are discrepant cases, but should not detract from
the broader consensus). In sum, the distance scale is secured to a
geometrically anchored framework that consists of results from several
key surveys (OGLE, NOMAD, ASAS, etc.) united by a universal VI Wesenheit
template and deep infrared ZAMS. Future research entails populating the
universal Wesenheit template with lower-temperature calibrators
(variable red giants, Miras, longer period Cepheids, etc.) using
observations acquired from the ARO, SRO (AAVSO), OMM, and DAO, and
further characterizing insidious photometric contamination associated
with variables occupying crowded regions near the cores of globular
clusters and galaxies (including the Milky Way).</description>
</item>


<item>

<title>Linares, M.: On The Cooling Tails Of Thermonuclear X-ray Bursts: News From Terzan 5</title>
<link>http://cdsads.u-strasbg.fr/abs/2011AAS...21832006L</link>
<description>The neutron star transient and 11 Hz X-ray pulsar IGR J17480-2446,
recently discovered in the globular cluster Terzan 5, showed
unprecedented bursting activity during its 2010 October-November
outburst. We analyzed all X-ray bursts detected with the Rossi X-ray
Timing Explorer and find strong evidence that they all have a
thermonuclear origin, despite the fact that many do not show the
canonical spectral softening along the decay imprinted on type I X-ray
bursts by the cooling of the neutron star photosphere. We show that the
persistent-to-burst power ratio is fully consistent with the
accretion-to-thermonuclear efficiency ratio along the whole outburst, as
is typical for type I X-ray bursts. The burst energy, peak luminosity
and daily-averaged spectral profiles all evolve smoothly throughout the
outburst, in parallel with the persistent (non-burst) luminosity. We
also find that the peak burst to persistent luminosity ratio determines
whether or not cooling is present in the bursts from IGR J17480-2446,
and argue that the apparent lack of cooling is due to the
``non-cooling'' bursts having both a lower peak temperature and a higher
non-burst (persistent) emission. We conclude that the detection of
cooling along the decay is a sufficient, but not a necessary condition
to identify an X-ray burst as thermonuclear. Finally, we compare these
findings with X-ray bursts from other rapidly accreting neutron stars.</description>
</item>


<item>

<title>Maccarone, T. J.: Compact Object Formation in Globular Clusters, the Milky Way and External Galaxies</title>
<link>http://cdsads.u-strasbg.fr/abs/2011AAS...21820901M</link>
<description>I will review the key contributions of Chandra, and associated
multi-wavelength facilities, to our understanding of formation and
evolution of compact objects, with a focus on compact binaries. I will
discuss the key results from both studies of Galactic and extragalactic
globular cluster sources and field X-ray sources, showing how Chandra
observations have both solved long-standing puzzles, and created some
new, interesting problems to be solved.</description>
</item>


<item>

<title>Barmby, P.: Globular Cluster Colors Versus Population Synthesis Models</title>
<link>http://cdsads.u-strasbg.fr/abs/2011AAS...21813312B</link>
<description>Although the stellar populations of globular clusters are not as simple
as we used to believe, they are still the simplest populations available
in the nearby universe. As such, they are extremely useful for testing
stellar population synthesis models. Using recent mass estimates for
Local Group globular clusters, we have compiled a sample of clusters
with masses large enough that stochastic effects on integrated
photometry should be minimal. We have measured integrated colors in the
Spitzer/IRAC bands for as many of these as possible, paying careful
attention to systematics in order to get the most accurate colors. We
present a comparison of the results with the predictions of the latest
generation of population synthesis models, including GALEV and FSPS.

Support for this work was provided by a Discovery Grant and an
Undergraduate Summer Research Award from NSERC and by an Ontario Early
Researcher Award.</description>
</item>


<item>

<title>Yoon, S.-J.: Color Bimodality of Extragalactic Globular Clusters: A Test for the Nonlinear Color-Metallicity Relation Scenario via the u-band Colors</title>
<link>http://cdsads.u-strasbg.fr/abs/2011AAS...21813311Y</link>
<description>The colors of globular clusters (GCs) in most large elliptical galaxies
are bimodal. Based on the observed linear relations between GC colors
and their metallicities, the bimodality is taken as evidence of two GC
subsystems with different metallicities in each galaxy and has led to a
number of theories in the context of galaxy formation. More recent
observations and modeling of GCs, however, suggest that colors likely
trace metallicities in a subtly nonlinear manner. The nonlinearity could
even transform a broad, unimodal metallicity spread into a strongly
bimodal color distribution. Despite the far-reaching implications,
whether color-metallicity relations (CMRs) are nonlinear and whether the
nonlinearity indeed causes the color bimodality are still open
questions. Given that the spectroscopic refinement of CMRs is still very
challenging, we here propose a new photometric tool to probe the
possible nonlinear nature of CMRs. In essence, a color distribution of
GCs is a &quot;projected” distribution of their metallicities based on
a given CMR. Since the form of CMRs hinges on which color is used, the
shape of color distributions varies depending significantly on colors in
use. Among other optical colors, the u-band colors (e.g., u-g and u-z)
are theoretically predicted to exhibit the most distinctive CMRs from
other preferred CMRs (e.g., for g-z). As a case study, we performed the
HST/WFPC2 archival u-band photometry for the M87 GC system with
confirmed color bimodality. We show that any weak yet discernible
feature on CMRs is amplified appreciably on the color domain by the
projection effect, and hence, under the assumption of the nonlinear
CMRs, the u-band color distributions are significantly different and
readily distinguishable from those under the assumption of the
conventional linear CMRs. With more data, this method will support or
rule out the nonlinear-CMR scenario for GC color bimodality with high
confidence.</description>
</item>


<item>

<title>Wei, L. H.: Bound Cluster Formation in the Antennae</title>
<link>http://cdsads.u-strasbg.fr/abs/2011AAS...21812913W</link>
<description>Observations by the Hubble Space Telescope have revealed a wealth of
super star clusters (SSCs) in lower extinction areas between dust lanes
of starburst galaxies. These SSCs may be present-day analogues of young
globular clusters, and are thought to form directly from giant molecular
clouds. The mode of formation (efficient compression from shocks vs.
slow compression within super giant molecular clouds), however, is still
not well-understood. We report on high-spatial resolution CO(2-1)
observations of the Antennae Galaxies with the Submillimeter Array (SMA)
and the IRAM Plateau de Bure Interferometer (PdBI). We discuss the
implications of our results on the various formation scenarios of SSCs
in starburst galaxies.</description>
</item>


<item>

<title>Sanna, N.: The Wfpc2 Uv Survey Of Globular Clusters: The Case Of Ngc 6229</title>
<link>http://cdsads.u-strasbg.fr/abs/2011AAS...21812503S</link>
<description>One of the valedictory projects undertaken by WFPC2 was a survey of UV
bright objects in 30 globular clusters. Eventually these results will be
combined with similar results obtained by our group for 15 clusters. For
most of these clusters observations were obtained with 4 or more
filters. For a subset of clusters we also have observations from GALEX
which will allow us see if the sort radial variations previously found
in blue straggler stars (BSS) also exists in the hottest stellar
populations. Here we present the case of NGC 6229. The data set has been
obtained by combining high-resolution (HST/WFPC2 and ACS) and wide-field
space (GALEX) observations and ground-based (MegaCam-CFHT) images. The
photometric sample covers the entire cluster extension from the very
central regions up to the tidal radius and beyond. We determine the
radial density profile and we study the BSS population and its radial
distribution.</description>
</item>


<item>

<title>Barnard, R.: Chandra Watches Over A Decade Of Variability In M31 Globular Clusters</title>
<link>http://cdsads.u-strasbg.fr/abs/2011AAS...21812202B</link>
<description>The central region of M31 has been monitored with Chandra &#62; 120 times
over the last  11 years. In this region we find X-ray sources
corresponding to 35 out of  420 globular clusters; these are highly
likely to be X-ray binaries. We have created long-term, calibrated
lightcurves for all 35 sources, and will present highlights of our
variability survey. We have detected significant variability in all the
sources with 0.3-10 keV luminosity &#62;  2x10E+36 erg/s. Since the
emission spectra of background active galaxies often resemble those of
X-ray binaries, the long term variability will be a valuable tool for
identifying X-ray binaries in the remaining 400 sources in our field.
This work is funded by Chandra grant GO9-0100X and HST grant GO-1101.</description>
</item>


<item>

<title>Shull, J. M.: Astro2010 Science in the Galactic Neighborhood (Redshift z &#60; 0.1)</title>
<link>http://cdsads.u-strasbg.fr/abs/2011AAS...21810403S</link>
<description>The GAN (Galactic Neighborhood) Science Frontier Panel of the Astro2010
decadal study provided 4 science questions and 2 discovery areas ripe
for investment. Defining our &quot;neighborhood&quot; out to redshift z = 0.1 (420
Mpc), we focused on:

(1) Flows of matter and energy in and out of galaxies

(2) Cycles of mass, energy, and chemistry within galaxies and their ISM

(3) Fossil record of galaxy assembly, from the first stars to the
present

(4) Connections between dark and luminous matter in galaxies and black
holes.

Our panel was excited about the promise of two Discovery Areas:

(A) Time-Domain Astronomy, to explore the transient sky and stellar
populations, including spectroscopic follow-up; and

(B) Astrometry of objects ranging from extra-solar planets to halo
stars, masers, globular clusters, galaxies, and quasars (maser disks,
bound stars).</description>
</item>


<item>

<title>Brüns, R. C.: A parametric study on the formation of extended star clusters and ultra-compact dwarf galaxies</title>
<link>http://cdsads.u-strasbg.fr/abs/2011A%26A...529A.138B</link>
<description>Context. In the last decade, very extended old stellar clusters with
masses in the range from a few 10&lt;SUP&gt;4&lt;/SUP&gt; to 10&lt;SUP&gt;8&lt;/SUP&gt;
M&lt;SUB&gt;ȯ&lt;/SUB&gt; have been found in various types of galaxies in
different environments. Objects with masses comparable to normal
globular clusters (GCs) are called extended clusters (ECs), while
objects with masses in the dwarf galaxy regime are called ultra-compact
dwarf galaxies (UCDs). In heavily interacting galaxies star clusters
tend to form in larger conglomerations called star cluster complexes
(CCs). The individual star clusters in a CC can merge and form a variety
of spheroidal stellar objects. &lt;BR /&gt; Aims: The parametric study aims to
analyze how the structural parameters of the final merger objects
correlate with the underlying CC parameter space. &lt;BR /&gt; Methods: In
this work we systematically scan a suitable parameter space for CCs and
perform numerical simulations to study their further fate. The varied
sizes and masses of the CCs cover a matrix of 5 × 6 values with CC
Plummer radii between 10-160 pc and CC masses between
10&lt;SUP&gt;5.5&lt;/SUP&gt;-10&lt;SUP&gt;8&lt;/SUP&gt; M&lt;SUB&gt;ȯ&lt;/SUB&gt;, which are consistent
with observed CC parameters. The CCs of the parametric study are on
orbits with galactocentric distances between 20 kpc and 60 kpc. In
addition, we studied also the evolution of CCs on a circular orbit at a
galactocentric distance of 60 kpc to verify that also extremely extended
ECs and UCDs can be explained by our formation scenario. &lt;BR /&gt; Results:
All 54 simulations end up with stable merger objects, wherein 26 to 97%
of the initial CC mass is bound. The objects show a general trend of
increasing effective radii with increasing mass. Despite the large range
of input Plummer radii of the CCs (10 to 160 pc) the effective radii of
the merger objects are constrained to values between 10 and 20 pc at the
low mass end and to values between 15 and 55 pc at the high mass end.
The structural parameters of the models are comparable to those of the
observed ECs and UCDs. The results of the circular orbits demonstrate
that even very extended objects like the M 31 ECs found by Huxor in 2005
and the very extended (r&lt;SUB&gt;eff&lt;/SUB&gt; &#62; 80 pc), high-mass UCDs can
be explained by merged cluster complexes in regions with low
gravitational fields at large galactocentric radii. &lt;BR /&gt; Conclusions:
We conclude that the observed ECs and UCDs can be well explained as
evolved star cluster complexes.</description>
</item>


<item>

<title>Lebzelter, T.: Long period variables and mass loss in the globular clusters NGC 362 and NGC 2808</title>
<link>http://cdsads.u-strasbg.fr/abs/2011A%26A...529A.137L</link>
<description>Context. The pulsation periods of long period variables (LPVs) depend on
their mass and helium abundance as well as on their luminosity and metal
abundance. Comparison of the observed periods of LPVs in globular
clusters with models is capable of revealing the amount of mass lost on
the giant branch and the helium abundance. &lt;BR /&gt; Aims: We aim to
determine the amount of mass loss that has occurred on the giant
branches of the low metallicity globular clusters NGC 362 and NGC 2808.
We also aim to see if the LPVs in NGC 2808 can tell us about helium
abundance variations in this cluster. &lt;BR /&gt; Methods: We have used
optical monitoring of NGC 362 and NGC 2808 to determine periods for the
LPVs in these clusters. We have made linear pulsation models for the
pulsating stars in these clusters taking into account variations in mass
and helium abundance. &lt;BR /&gt; Results: Reliable periods have been
determined for 11 LPVs in NGC 362 and 15 LPVs in NGC 2808. Comparison of
the observed variables with models in the log P-K diagram shows that
mass loss of ~0.15-0.2 M&lt;SUB&gt;ȯ&lt;/SUB&gt; is required on the first giant
branch in these clusters, in agreement with estimates from other
methods. In NGC 2808, there is evidence that a high helium abundance of
Y ~ 0.4 is required to explain the periods of several of the LPVs. &lt;BR
/&gt; Conclusions: It would be interesting to determine periods for LPVs in
other Galactic globular clusters where a helium abundance variation is
suspected to see if the completely independent test for a high helium
abundance provided by the LPVs can confirm the high helium abundance
estimates.</description>
</item>


<item>

<title>Church, R. P.: Coordinates and 2MASS and OGLE identifications for all stars in Arp's 1965 finding chart for Baade's Window</title>
<link>http://cdsads.u-strasbg.fr/abs/2011A%26A...529A.104C</link>
<description>&lt;BR /&gt; Aims: We seek to provide 2MASS and OGLE identifications and
coordinates for all stars in the finding chart published by Arp (1965,
ApJ, 141, 43). This chart covers the low extinction area around NGC
6522, also known as Baade's window, at coordinates (l,b) = (1.02,
-3.92). &lt;BR /&gt; Methods: A cross correlation, using numerical techniques,
was performed between a scan of the original finding chart from Arp and
2MASS and OGLE-II images and stellar coordinates. &lt;BR /&gt; Results: We
provide coordinates for all stars in Arp's finding chart and 2MASS and
OGLE identifications wherever possible. Two identifications in quadrant
II do not appear in the original finding chart.

Table 1 is only available in electronic form at the CDS via anonymous
ftp to cdsarc.u-strasbg.fr (130.79.128.5) or via &lt;A
href=&quot;http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/529/A104&quot;&gt;http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/529/A104&lt;/A&gt;</description>
</item>


<item>

<title>Michaud, G.: Horizontal branch evolution, metallicity, and sdB stars</title>
<link>http://cdsads.u-strasbg.fr/abs/2011A%26A...529A..60M</link>
<description>Context. Abundance anomalies have been observed in field sdB stars and
in nearly all horizontal branch (HB) stars of globular clusters with
T&lt;SUB&gt;eff&lt;/SUB&gt; &#62; 11 000 K, whatever be the cluster metallicity. &lt;BR
/&gt; Aims: We aim to determine the abundance variations that are expected
in sdB stars and in HB stars of metallicities Z ≥ 10&lt;SUP&gt;-4&lt;/SUP&gt; and
investigate what the observed abundances teach us about hydrodynamical
processes competing with atomic diffusion. &lt;BR /&gt; Methods: Complete
stellar evolution models, including the effects of atomic diffusion and
radiative acceleration, have been computed from the zero age
main-sequence for metallicities of Z&lt;SUB&gt;0&lt;/SUB&gt; = 0.0001, 0.001, 0.004
and 0.02. On the HB the masses were selected to cover the
T&lt;SUB&gt;eff&lt;/SUB&gt; interval from 7000 to 37 000 K. Some 60 evolutionary HB
models were calculated. The calculations of surface abundance anomalies
during the horizontal branch depend on one parameter, the surface mixed
mass. &lt;BR /&gt; Results: For sdB stars with T&lt;SUB&gt;eff&lt;/SUB&gt; &#60; 37 000 K
and for HB stars with T&lt;SUB&gt;eff&lt;/SUB&gt; &#62; 11 000 K in all observed
clusters, independent of metallicity, we found that most observed
abundance anomalies (even up to ~ × 200) were compatible, within
error bars, with expected abundances. A mixed mass of was determined by
comparison with observations. &lt;BR /&gt; Conclusions: Observations of
globular cluster HB stars with T&lt;SUB&gt;eff&lt;/SUB&gt; &#62; 11 000 K and of sdB
stars with T&lt;SUB&gt;eff&lt;/SUB&gt; &#60; 37 000 K suggest that most observed
abundance anomalies can be explained by element separation driven by
radiative acceleration occuring at a mass fraction of . Mass loss or
turbulence appear to limit the separation between and the surface.

Appendices are only available in electronic form at &lt;A
href=&quot;http://www.aanda.org&quot;&gt;http://www.aanda.org&lt;/A&gt;</description>
</item>


<item>

<title>Cenarro, A. J.: MgI and sTiO index definitions (Cenarro+, 2009)</title>
<link>http://cdsads.u-strasbg.fr/abs/2011yCat..73961895C</link>
<description>Using the near-infrared spectral stellar library of Cenarro et al.
(J/MNRAS/326/959), the behaviour of the MgI line at 8807Å and
nearby TiO bands is analyzed in terms of the effective temperature,
surface gravity and metallicity of the library stars. New spectroscopic
indices for both spectral features - namely MgI and sTiO - are defined,
and their sensitivities to different signal-to-noise ratios, spectral
resolutions, flux calibrations and sky emission-line residuals are
characterized. The two new indices exhibit interesting properties. In
particular, MgI is a good indicator of the Mg abundance, whereas sTiO is
a powerful dwarf-to-giant discriminator for cold spectral types.
Empirical fitting polynomials that reproduce the strength of the new
indices as a function of the stellar atmospheric parameters are
computed, and a fortran routine with the fitting function predictions is
made available. A thorough study of several error sources, non-solar
[Mg/Fe] ratios and their influence on the fitting function residuals is
also presented. From this analysis, an [Mg/Fe] underabundance of ~-0.04
is derived for the Galactic open cluster M67.

(2 data files).</description>
</item>


<item>

<title>Lane, R. R.: Stellar parameters from 10 Galactic GC fields (Lane+, 2011)</title>
<link>http://cdsads.u-strasbg.fr/abs/2011yCat..35309031L</link>
<description>Various stellar parameters were extracted, using two different reduction
pipelines, from individual stellar spectra obtained with AAOmega on the
Anglo-Australia Telescope. These spectra were obtained from ten fields
centered on Galactic globular clusters, namely M4, M12, M22, M30, M53,
M55, M68, NGC 288, NGC 6752 and 47 Tuc. Stellar parameters provided
include the radial velocity, sum of the equivalent widths of the calcium
triplet lines, equatorial coordinates, I magnitude, V magnitude,
effective temperature, surface gravity, metallicity, rotational
velocity, J magnitude, H magnitude, K magnitude, distance from the
cluster centre, position angle with respect to the cluster centre and
whether each star was determined to be a member of the cluster.

(3 data files).</description>
</item>


<item>

<title>Kouvaris, C.: Constraining asymmetric dark matter through observations of compact stars</title>
<link>http://cdsads.u-strasbg.fr/abs/2011PhRvD..83h3512K</link>
<description>We put constraints on asymmetric dark matter candidates with
spin-dependent interactions based on the simple existence of white
dwarfs and neutron stars in globular clusters. For a wide range of the
parameters (WIMP mass and WIMP-nucleon cross section), weakly
interacting massive particles (WIMPs) can be trapped in progenitors in
large numbers and once the original star collapses to a white dwarf or a
neutron star, these WIMPs might self-gravitate and eventually collapse
forming a mini-black hole that eventually destroys the star. We
impose constraints competitive to direct dark matter search experiments,
for WIMPs with masses down to the TeV scale.</description>
</item>


<item>

<title>Saha, A.: Calibration of B V R I Photometry for the Wide Field Channel of the HST Advanced Camera for Surveys</title>
<link>http://cdsads.u-strasbg.fr/abs/2011PASP..123..481S</link>
<description>We present new observations of two Galactic globular clusters, PAL4 and
PAL14, using the Wide Field Channel of the Advanced Camera for Surveys
(ACS) on board the Hubble Space Telescope (HST) and reanalyze archival
data from a third, NGC2419. We matched our photometry of hundreds of
stars in these fields from the ACS images to existing ground-based
photometry of faint sequences that were calibrated on the standard B V R
I system of Landolt. These stars are significantly fainter than those
generally used for HST calibration purposes and therefore are much
better matched to supporting precision photometry of ACS science
targets. We were able to derive more accurate photometric transformation
coefficients for the commonly used ACS broadband filters, compared with
those published by Sirianni et al., due to the use of a factor of
several more calibration stars that span a greater range of color. We
find that the inferred transformations from each cluster individually do
not vary significantly from the average, except for a small offset of
the photometric zero point in the F850LP filter. Our results suggest
that the published prescriptions for the time-dependent correction of
CCD charge transfer efficiency appear to work very well over the ˜
3.5 yr interval that spans our observations of PAL4 and PAL14 and the
archived images of NGC2419.</description>
</item>


<item>

<title>Chiappini, C.: Imprints of fast-rotating massive stars in the Galactic Bulge</title>
<link>http://cdsads.u-strasbg.fr/abs/2011Natur.472..454C</link>
<description>The first stars that formed after the Big Bang were probably massive,
and they provided the Universe with the first elements heavier than
helium (`metals'), which were incorporated into low-mass stars that have
survived to the present. Eight stars in the oldest globular cluster in
the Galaxy, NGC6522, were found to have surface abundances consistent
with the gas from which they formed being enriched by massive stars
(that is, with higher α-element/Fe and Eu/Fe ratios than those of
the Sun). However, the same stars have anomalously high abundances of Ba
and La with respect to Fe, which usually arises through nucleosynthesis
in low-mass stars (via the slow-neutron-capture process, or s-process).
Recent theory suggests that metal-poor fast-rotating massive stars are
able to boost the s-process yields by up to four orders of magnitude,
which might provide a solution to this contradiction. Here we report a
reanalysis of the earlier spectra, which reveals that Y and Sr are also
overabundant with respect to Fe, showing a large scatter similar to that
observed in extremely metal-poor stars, whereas C abundances are not
enhanced. This pattern is best explained as originating in metal-poor
fast-rotating massive stars, which might point to a common property of
the first stellar generations and even of the `first stars'.</description>
</item>


<item>

<title>Nipoti, C.: Radial-orbit instability in modified Newtonian dynamics</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.tmp..608N</link>
<description>The stability of radially anisotropic spherical stellar systems in
modified Newtonian dynamics (MOND) is explored by means of numerical
simulations performed with the N-body code N-MODY. We find that
Osipkov-Merritt MOND models require for stability larger minimum
anisotropy radii than equivalent Newtonian systems (ENSs) with the dark
matter, and also than purely baryonic Newtonian models with the same
density profile. The maximum value for stability of the
Fridman-Polyachenko-Shukhman parameter in MOND models is lower than in
ENSs, but higher than in Newtonian models with no dark matter. We
conclude that MOND systems are substantially more prone to radial-orbit
instability than ENSs with dark matter, while they are able to support a
larger amount of kinetic energy stored in radial orbits than purely
baryonic Newtonian systems. An explanation of these results is attempted
and their relevance to the MOND interpretation of the observed
kinematics of globular clusters, dwarf spheroidal and elliptical
galaxies is briefly discussed.</description>
</item>


<item>

<title>Freire, P. C. C.: On the nature and evolution of the unique binary pulsar J1903+0327</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.412.2763F</link>
<description>PSR J1903+0327, a millisecond pulsar in an eccentric (e= 0.44) 95-d
orbit with an ˜1 M&lt;SUB&gt;ȯ&lt;/SUB&gt; companion poses a challenge to
our understanding of stellar evolution in binary and multiple-star
systems. Here we describe optical and radio observations which rule out
most of the scenarios proposed to explain formation of this system.
Radio timing measurements of three post-Keplerian effects yield the most
precise measurement of the mass of a millisecond pulsar to date: 1.667
± 0.021 solar masses (99.7 per cent confidence limit). This rules
out some equations of state for superdense matter; furthermore, it is
consistent with the spin-up of the pulsar by mass accretion, as
suggested by its short spin period and low magnetic field. Optical
spectroscopy of a proposed main-sequence counterpart shows that its
orbital motion mirrors the pulsar's 95-d orbit; being therefore its
binary companion. This finding rules out a previously suggested scenario
which proposes that the system is presently a hierarchical triple.
Conventional binary evolution scenarios predict that, after recycling a
neutron star into a millisecond pulsar, the binary companion should
become a white dwarf and its orbit should be nearly circular. This
suggests that if PSR J1903+0327 was recycled, its present companion was
not responsible for it. The optical detection also provides a
measurement of the systemic radial velocity of the binary; this and the
proper motion measured from pulsar timing allow the determination of the
systemic 3D velocity in the Galaxy. We find that the system is always
within 270 pc of the plane of the Galaxy, but always more than 3 kpc
away from the Galactic Centre. Thus an exchange interaction in a dense
stellar environment (like a globular cluster or the Galactic Centre) is
not likely to be the origin of this system. We suggest that after the
supernova that formed it, the neutron star was in a tight orbit with a
main-sequence star and the present companion was a tertiary farther out.
The neutron star then accreted matter from its evolving inner companion,
forming a millisecond pulsar. The inner companion then disappeared,
either due to a chaotic three-body interaction with the outer star
(caused by the expansion of the inner orbit that necessarily results
from mass transfer), or in the case of a very compact inner system, due
to ablation/accretion by the newly formed millisecond pulsar. We discuss
in detail the possible evolution of such a system before the supernova.</description>
</item>


<item>

<title>Percival, S. M.: Modelling realistic horizontal branch morphologies and their impact on spectroscopic ages of unresolved stellar systems</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.412.2445P</link>
<description>The presence of an extended blue horizontal branch (HB) in a stellar
population is known to affect the age inferred from spectral fitting to
stellar population synthesis models. This is due to the hot blue
component which increases the strength of the Balmer lines and can make
an old population look spuriously young. However, most population
synthesis models still rely on theoretical isochrones, which do not
include realistic modelling of extended HBs. In this work, we create
detailed models for a range of old simple stellar populations (SSPs),
with metallicities ranging from [Fe/H]=-1.3 to solar, to create a
variety of realistic HB morphologies, from extended red clumps, to
extreme blue HBs. We achieve this by utilizing stellar tracks from the
BaSTI data base and implementing a different mass-loss prescription for
each SSP created. This includes setting an average mass and a Gaussian
spread in masses of individual stars coming on to the zero-age HB for
each model, and hence resulting in different HB morphologies. We find
that, for each metallicity, there is some HB morphology which maximizes
Hβ, making an underlying 14-Gyr population look ˜5-6 Gyr old
for the low- and intermediate-metallicity cases, and as young as 2 Gyr
in the case of the solar metallicity SSP. We explore whether there are
any spectral indices capable of breaking the degeneracy between an old
SSP with extended blue HB and a truly young or intermediate-age SSP, and
find that the Ca II index of Rose and the strength of the Mg II doublet
at 2800 Å are promising candidates, in combination with Hβ
and other metallicity indicators, such as Mgb and Fe5406. We also run
Monte Carlo simulations to investigate the level of statistical
fluctuations in the spectra of typical stellar clusters. We find that
fluctuations in spectral indices are significant even for average to
large globular clusters and that various spectral indices are affected
in different ways, which has implications for full-spectrum fitting
methods. Hence, we urge caution if these types of stellar clusters are
to be used as empirical calibrating objects for various aspects of
stellar population synthesis models.</description>
</item>


<item>

<title>Bekki, K.: Secondary star formation within massive star clusters: origin of multiple stellar populations in globular clusters</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.412.2241B</link>
<description>We numerically investigate whether and how gaseous ejecta from AGB stars
can be converted into new stars within originally massive star clusters
(MSCs) in order to understand the origin of multiple stellar populations
in globular clusters (GCs). We adopt a scenario in which (i) MSCs with
masses of M&lt;SUB&gt;s&lt;/SUB&gt; can be formed from high-mass, high-density giant
molecular clouds (GMCs) in their host galactic building blocks embedded
in dark matter haloes at high redshifts, and (ii) their evolution
therefore can be significantly influenced by M&lt;SUB&gt;s&lt;/SUB&gt;, their
initial locations and physical properties of their hosts. Our 3D
hydrodynamical simulations show that gaseous ejecta from AGB stars can
be retained within MSCs and consequently converted into new stars very
efficiently in the central regions of MSCs, only if M&lt;SUB&gt;s&lt;/SUB&gt;
exceeds a threshold mass (M&lt;SUB&gt;th&lt;/SUB&gt;) of ≈10&lt;SUP&gt;6&lt;/SUP&gt;
M&lt;SUB&gt;ȯ&lt;/SUB&gt;. The new stars can correspond to the 'second
generation (SG)' of stars with higher Na and lower O abundances observed
in GCs. Star formation efficiencies during the formation of SG stars
within MSCs with M&lt;SUB&gt;s&lt;/SUB&gt;≥M&lt;SUB&gt;th&lt;/SUB&gt; can be rather high
(0.3-0.9) so that very compact new clusters within original MSCs can be
formed. M&lt;SUB&gt;s&lt;/SUB&gt; should be as large as
10&lt;SUP&gt;6&lt;/SUP&gt;-10&lt;SUP&gt;7&lt;/SUP&gt; M&lt;SUB&gt;ȯ&lt;/SUB&gt; to explain the observed
large fraction of SG stars in the present ordinary Galactic GCs, because
new stars can consist of only 1-4 per cent among all stars for the
standard initial mass function. Nuclear MSCs are found to retain much
more effectively the AGB ejecta and convert more efficiently the gas
into new stars, owing to the much deeper gravitational potential of
their hosts. Capture and accretion of cold molecular gas (or small GMCs)
by forming MSCs themselves can be mechanisms for mixing (i.e., dilution)
of AGB ejecta with cold pristine gas. We suggest that both M&lt;SUB&gt;s&lt;/SUB&gt;
and their locations within their hosts can determine whether abundance
spread can be seen only in light elements or even in heavy ones. We
discuss how and in what time-scale MSCs preferentially lose old stars
owing to tidal stripping by their host galactic building blocks. We also
suggest that the origin of the intermediate-age GCs with possible age
spread of ˜100 Myr yet apparently no/little abundance spread in
light elements in the LMC is closely associated with their incapability
to retain the AGB ejecta owing to their low masses.</description>
</item>


<item>

<title>Thomas, D.: Chemical abundance ratios of galactic globular clusters from modelling integrated light spectroscopy</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.412.2199T</link>
<description>In a companion paper we present new, flux-calibrated stellar population
models of Lick absorption-line indices with variable element abundance
ratios. The model includes a large variety of individual element
variations, which allows the derivation of the abundances for the
elements C, N, O, Mg, Ca, Ti and Fe besides total metallicity and age.
We use this model to obtain estimates of these quantities from
integrated light spectroscopy of galactic globular clusters. We show
that the model fits to a number of indices improve considerably when
various variable element ratios are considered. The ages we derive agree
well with the literature and are all consistent with the age of the
Universe within the measurement errors. There is a considerable scatter
in the ages, though, and we overestimate the ages preferentially for the
metal-rich globular clusters. Our derived total metallicities agree
generally very well with literature values on the Zinn &#38; West scale
once corrected for α enhancement, in particular for those cluster
where the ages agree with the colour-magnitude diagram ages. We tend to
slightly underestimate the metallicity for those clusters where we
overestimate the age, in line with the age-metallicity degeneracy. It
turns out that the derivation of individual element abundance ratios is
not reliable at an iron abundance [Fe/H] &#60; -1 dex where line
strengths become weaker, while the [α/Fe] ratio is robust at all
metallicities. The discussion of individual element ratios focuses
therefore on globular clusters with [Fe/H] &#62; -1 dex. We find general
enhancement of light and α elements, as expected, with significant
variations for some elements. The elements O and Mg follow the same
general enhancement with almost identical distributions of [O/Fe] and
[Mg/Fe]. We obtain slightly lower [C/Fe] and very high [N/Fe] ratios,
instead. This chemical anomaly, commonly attributed to self-enrichment,
is well known in globular clusters from individual stellar spectroscopy.
It is the first time that this pattern is obtained also from the
integrated light. The α elements follow a pattern such that the
heavier elements Ca and Ti are less enhanced. More specifically, the
[Ca/Fe] and [Ti/Fe] ratios are lower than [O/Fe] and [Mg/Fe] by about
0.2 dex. Most interestingly this trend of element abundance with atomic
number is also seen in recent determinations of element abundances in
globular cluster and field stars of the Milky Way. This suggests that
Type Ia supernovae contribute significantly to the enrichment of the
heavier α elements as predicted by nucleosynthesis calculations
and galactic chemical evolution models.</description>
</item>


<item>

<title>Thomas, D.: Flux-calibrated stellar population models of Lick absorption-line indices with variable element abundance ratios</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.412.2183T</link>
<description>We present new stellar population models of Lick absorption-line indices
with variable element abundance ratios. The models are based on our new
calibrations of absorption-line indices with stellar parameters derived
from the MILES stellar library. The key novelty compared to our previous
models is that they are now available at the higher spectral resolution
of MILES (2.5 Å full width at half-maximum) and flux calibrated,
hence not tied anymore to the Lick/IDS system. This is essential for the
interpretation of galaxy spectra where calibration stars are not
available, such as large galaxy redshift surveys or other high-redshift
observations. We note that the MILES resolution appears to be comparable
to Sloan Digital Sky Survey (SDSS) resolution, so that our models can be
applied to SDSS data without any corrections for instrumental spectral
resolution. For the first time we provide random errors for the model
predictions based on the uncertainties in the calibration functions and
the underlying stellar parameter estimates. We show that random errors
are small except at the edges of the parameter space (high/low
metallicities and young ages ≲1 Gyr) where the stellar library is
undersampled. We calibrate the base model for the parameters age,
metallicity and α/Fe ratio with galactic globular cluster and
galaxy gradient data. We discuss two model flavours with different input
stellar evolutionary tracks from the Frascati and Padova groups. The new
model release now includes abundance variations of the elements C, N,
Mg, Na, Si, Ca, Ti, Cr and Fe. The individual elements that are best
accessible with these models and the standard set of Lick absorption
features are C, N, Mg, Ca, Ti and Fe. The model data are available at
˜thomasd.</description>
</item>


<item>

<title>Chilingarian, I. V.: Dynamical versus stellar masses of ultracompact dwarf galaxies in the Fornax cluster</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.412.1627C</link>
<description>The origin of ultracompact dwarf (UCD) galaxies, compact extragalactic
stellar systems, is still a puzzle for present galaxy formation models.
We present the comprehensive analysis of high-resolution multi-object
spectroscopic data for a sample of 24 Fornax cluster UCDs obtained with
VLT with Fibre Large Array Multi Element Spectrograph (FLAMES). It
comprises previously published data for 19 objects which we re-analysed,
including 13 with available Hubble Space Telescope (HST) photometric
data. Using Virtual Observatory technologies we found archival HST
images for two more UCDs and then determined their structural
properties. For all objects we derived internal velocity dispersions,
stellar population parameters and stellar mass-to-light ratios
(M/L)&lt;SUB&gt;*&lt;/SUB&gt; by fitting individual simple stellar population (SSP)
synthetic spectra convolved with a Gaussian against the observed spectra
using the NBURSTS full spectral fitting technique. For 14 objects we
estimated dynamical masses suggesting no dark matter (DM) in 12 of them
and no more than 40 per cent DM mass fraction in the remaining two, in
contrast to findings for several UCDs in the Virgo cluster. Some Fornax
UCDs even have too high values of (M/L)&lt;SUB&gt;*&lt;/SUB&gt; estimated using the
Kroupa stellar initial mass function (IMF) resulting in negative
formally computed DM mass fractions. The objects with too high
(M/L)&lt;SUB&gt;*&lt;/SUB&gt; ratios compared to the dynamical ones have relatively
short dynamical relaxation time-scales, close to the Hubble time or
below. We therefore suggest that their lower dynamical ratios
(M/L)&lt;SUB&gt;dyn&lt;/SUB&gt; are caused by low-mass star depletion due to
dynamical evolution. Overall, the observed UCD characteristics suggest
at least two formation channels: tidal threshing of nucleated dwarf
galaxies for massive UCDs (≃10&lt;SUP&gt;8&lt;/SUP&gt; M&lt;SUB&gt;ȯ&lt;/SUB&gt;), and
a classical scenario of red globular cluster formation for lower-mass
UCDs (≲10&lt;SUP&gt;7&lt;/SUP&gt; M&lt;SUB&gt;ȯ&lt;/SUB&gt;). Based on the archival
ESO VLT with Fibre Large Array Multi Element Spectrograph (FLAMES)
(programme 078.B-0496) available through and Hubble Space Telescope
archival data (programmes 8090 and 10129) available through</description>
</item>


<item>

<title>Carraro, G.: An analysis of the blue straggler population in the Sgr dSph globular cluster Arp 2</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.412.1361C</link>
<description>We present and discuss new BVI CCD photometry in the field of the
globular cluster Arp 2, which is considered a member of the Sagittarius
dwarf spheroidal galaxy. The main goal of this investigation is to study
the statistics and spatial distribution of blue straggler stars in the
cluster. Blue stragglers are stars observed to be hotter and bluer than
other stars with the same luminosity in their environments. As such,
they appear to be much younger than the rest of the stellar population.
Two main channels have been suggested to produce such stars: (1)
collisions between stars in clusters; or (2) mass transfer between, or
merger of, the components of primordial short-period binaries. The
spatial distribution of these stars inside a star cluster, compared with
the distribution of stars in different evolutionary stages, can cast
light on the most efficient production mechanism at work. In the case of
Arp 2, we found that blue straggler stars are significantly more
concentrated than main-sequence stars, while they show the same degree
of concentration as evolved stars (either red giants or horizontal
branch stars). Since Arp 2 is not a very concentrated cluster, we
suggest that this high central concentration is an indication that blue
stragglers are mostly primordial binary stars. Based on observations
carried out at ESO La Silla under programme 081.C-0087(A).</description>
</item>


<item>

<title>Weidner, C.: Top-heavy integrated galactic stellar initial mass functions in starbursts</title>
<link>http://cdsads.u-strasbg.fr/abs/2011MNRAS.412..979W</link>
<description>Star formation rates (SFRs) larger than 1000 M&lt;SUB&gt;ȯ&lt;/SUB&gt;
yr&lt;SUP&gt;-1&lt;/SUP&gt; are observed in extreme starbursts. This leads to the
formation of star clusters with masses &#62;10&lt;SUP&gt;6&lt;/SUP&gt;
M&lt;SUB&gt;ȯ&lt;/SUB&gt; in which crowding of the pre-stellar cores may lead
to a change of the stellar initial mass function (IMF). Indeed, the
large mass-to-light ratios of ultracompact dwarf galaxies and recent
results on globular clusters suggest the IMF to become top-heavy with
increasing star-forming density. We explore the implications of
top-heavy IMFs in these very massive and compact systems for the
integrated galactic initial mass function (IGIMF), which is the
galaxy-wide IMF, in dependence of the SFR of galaxies. The resulting
IGIMFs can have slopes, α&lt;SUB&gt;3&lt;/SUB&gt;, for stars more massive than
about 1 M&lt;SUB&gt;ȯ&lt;/SUB&gt; between 1.5 and the Salpeter slope of 2.3 for
an embedded cluster mass function (ECMF) slope (β) of 2.0, but only
if the ECMF has no low-mass clusters in galaxies with major starbursts.
Alternatively, β would have to decrease with increasing SFR &#62; 10
M&lt;SUB&gt;ȯ&lt;/SUB&gt; yr&lt;SUP&gt;-1&lt;/SUP&gt; such that galaxies with major
starbursts have a top-heavy ECMF. The resulting IGIMFs are within the
range of observationally deduced IMF variations with redshift.</description>
</item>


<item>

<title>Gnedin, O. Y.: Modeling Formation of Globular Clusters: Beacons of Galactic Star Formation</title>
<link>http://cdsads.u-strasbg.fr/abs/2011IAUS..270..381G</link>
<description>Modern hydrodynamic simulations of galaxy formation are able to predict
accurately the rates and locations of the assembly of giant molecular
clouds in early galaxies. These clouds could host star clusters with the
masses and sizes of real globular clusters. I describe current
state-of-the-art simulations aimed at understanding the origin of the
cluster mass function and metallicity distribution. Metallicity
bimodality of globular cluster systems appears to be a natural outcome
of hierarchical formation and gradually declining fraction of cold gas
in galaxies. Globular cluster formation was most prominent at redshifts
z &#62; 3, when massive star clusters may have contributed as much as 20%
of all galactic star formation.</description>
</item>


</channel>
</rss>
