300 research outputs found
Blue Stragglers in Globular Clusters: Observations, Statistics and Physics
This chapter explores how we might use the observed {\em statistics} of blue
stragglers in globular clusters to shed light on their formation. This means we
will touch on topics also discussed elsewhere in this book, such as the
discovery and implications of bimodal radial distributions and the "double
sequences" of blue stragglers that have recently been found in some clusters.
However, we will focus particularly on the search for a "smoking gun"
correlation between the number of blue stragglers in a given globular cluster
and a physical cluster parameter that would point towards a particular
formation channel. As we shall see, there is little evidence for an intrinsic
correlation between blue straggler numbers and stellar collision rates, even in
dense cluster cores. On the other hand, there is a clear correlation between
blue straggler numbers and the total (core) mass of the cluster. This would
seem to point towards a formation channel involving binaries, rather than
dynamical encounters. However, the correlation between blue straggler numbers
and actual binary numbers - which relies on recently determined empirical
binary fractions - is actually weaker than that with core mass. We explain how
this surprising result may be reconciled with a binary formation channel if
binary fractions depend almost uniquely on core mass. If this is actually the
case, it would have significant implications for globular cluster dynamics more
generally.Comment: Chapter 13, in Ecology of Blue Straggler Stars, H.M.J. Boffin, G.
Carraro & G. Beccari (Eds), Astrophysics and Space Science Library, Springe
The radial effective temperature distribution of steady-state, mass-losing accretion disks
Mass loss appears to be a common phenomenon among disk-accreting
astrophysical systems. An outflow emanating from an accretion disk can act as a
sink for mass, angular momentum and energy and can therefore alter the
dissipation rates and effective temperatures across the disk. Here, the radial
distributions of dissipation rate and effective temperature across a Keplerian,
steady-state, mass-losing accretion disk are derived, using a simple,
parametric approach that is sufficiently general to be applicable to many types
of dynamical disk wind models.
Effective temperature distributions for mass-losing accretion disks in
cataclysmic variables are shown explicitly, with parameters chosen to describe
both radiation-driven and centrifugally-driven outflows. For realistic wind
mass-loss rates of a few percent, only centrifugally-driven outflows --
particularly those in which mass loss is concentrated in the inner disk -- are
likely to alter the disk's effective temperature distribution significantly.
Accretion disks that drive such outflows could produce spectra and eclipse
light curves that are noticeably different from those produced by standard,
conservative disks.Comment: 14 pages, 3 figures, accepted for publication in MNRA
The orbital period and system parameters of the recurrent nova T Pyx
T Pyx is a luminous recurrent nova that accretes at a much higher rate than is expected for its photometrically determined orbital period of about 1.8 h. We here provide the first spectroscopic confirmation of the orbital period, P = 1.8295 h (f = 13.118368 +/- 1.1 x 10(-5) c d(-1)), based on time-resolved optical spectroscopy obtained at the Very Large Telescope and the Magellan telescope. We also derive an upper limit of the velocity semi-amplitude of the white dwarf, K 1 = 17.9 +/- 1.6 kms(-1), and estimate amass ratio of q = 0.20 +/- 0.03. If the mass of the donor star is estimated using the period-density relation and theoretical main-sequence mass-radius relation for a slightly inflated donor star, we find M-2 = 0.14 +/- 0.03 M-circle dot. This implies a mass of the primary white dwarf of M-1 = 0.7 +/- 0.2 M-circle dot. If the white-dwarf mass is > 1 M-circle dot, as classical nova models imply, the donor mass must be even higher. We therefore rule out the possibility that T Pyx has evolved beyond the period minimum for cataclysmic variables. We find that the system inclination is constrained to be i approximate to 10 degrees, confirming the expectation that T Pyx is a low-inclination system. We also discuss some of the evolutionary implications of the emerging physical picture of T Pyx. In particular, we show that epochs of enhanced mass transfer (like the present) may accelerate or even dominate the overall evolution of the system, even if they are relatively short-lived. We also point out that such phases may be relevant to the evolution of cataclysmic variables more generally
Nuclear Star Clusters and the Stellar Spheroids of their Host Galaxies
(Abridged) We combine published photometry for the nuclear star clusters
(NSCs) and stellar spheroids of 51 low-mass, early-type galaxies in the Virgo
cluster with empirical mass-to-light ratios, in order to complement previous
studies that explore the dependence of NSC masses (M_{NSC}) on various
properties of their host galaxies. We confirm a roughly linear relationship
between M_{NSC} and luminous host spheroid mass (M_{Sph}), albeit with
considerable scatter (0.57 dex). We estimate velocity dispersions from the
virial theorem, assuming all galaxies in our sample share a common DM fraction
and are dynamically relaxed. We then find that M_{NSC} \sim \sigma^{2.73\pm
0.29}, with a slightly reduced scatter of 0.54 dex.
This confirms recent results that the shape of the M_{CMO} - \sigma relation
is different for NSCs and super-massive black holes (SMBHs). We discuss this
result in the context of the generalized idea of "central massive objects"
(CMOs).
In order to assess which physical parameters drive the observed NSC masses,
we also carry out a joint multi-variate power-law fit to the data. In this, we
allow M_{NSC} to depend on M_{Sph} and R_{Sph} (and hence implicitly on
\sigma), as well as on the size of the globular cluster reservoir. When
considered together, the dependences on M_{Sph} and R_{Sph} are roughly
consistent with the virial theorem, and hence M_{NSC} \propto \sigma^2.
However, the only statistically significant correlation is a linear scaling
between M_{NSC} and M_{Sph}.
We compare M_{NSC} with predictions for two popular models for NSC formation,
namely i) globular cluster infall due to dynamical friction, and ii) in-situ
formation during the early phases of galaxy formation that is regulated via
momentum feedback from stellar winds and/or supernovae. Neither model can
directly predict the observations, and we discuss possible interpretations of
our findings.Comment: 10 pages, 2 tables, 6 figures; accepted for publication in MNRAS;
edited to match published versio
Inflation after WMAP3
I discuss the current status of inflationary cosmology in light of the recent
WMAP 3-year data release. The basic predictions of inflation are all supported
by the data. Inflation also makes predictions which have not been well tested
by current data but can be by future experiments, most notably a deviation from
a scale-invariant power spectrum and the production of primordial gravitational
waves. A scale-invariant spectrum is disfavored by current data, but not
conclusively. Tensor modes are currently poorly constrained, and slow-roll
inflation does not make an unambiguous prediction of the expected amplitude of
primordial gravitational waves. A tensor/scalar ratio of is
within reach of near-future measurements.Comment: To appear in the proceedings of Colliders to Cosmic Rays 2007. 8
pages, 2 figures. (V2: Minor typo corrected
The Geometry and Ionization Structure of the Wind in the Eclipsing Nova-like Variables RW Tri and UX UMa
The UV spectra of nova-like variables are dominated by emission from the
accretion disk, modified by scattering in a wind emanating from the disk. Here
we model the spectra of RW Tri and UX UMa, the only two eclipsing nova-likes
which have been observed with the Hubble Space Telescope in the
far-ultraviolet, in an attempt to constrain the geometry and the ionization
structure of their winds. Using our Monte Carlo radiative transfer code we
computed spectra for simply-parameterized axisymmetric biconical outflow models
and were able to find plausible models for both systems. These reproduce the
primary UV resonance lines - N V, Si IV, and C IV - in the observed spectra in
and out of eclipse. The distribution of these ions in the wind models is
similar in both cases as is the extent of the primary scattering regions in
which these lines are formed. The inferred mass loss rates are 6% to 8% of the
mass accretion rates for the systems. We discuss the implication of our point
models for our understanding of accretion disk winds in cataclysmic variables.Comment: 13 pages, 15 figures and 4 tables. Published in Ap
The Impact of Accretion Disk Winds on the Optical Spectra of Cataclysmic Variables
Many high-state non-magnetic cataclysmic variables (CVs) exhibit blue-shifted
absorption or P-Cygni profiles associated with ultraviolet (UV) resonance
lines. These features imply the existence of powerful accretion disk winds in
CVs. Here, we use our Monte Carlo ionization and radiative transfer code to
investigate whether disk wind models that produce realistic UV line profiles
are also likely to generate observationally significant recombination line and
continuum emission in the optical waveband. We also test whether outflows may
be responsible for the single-peaked emission line profiles often seen in
high-state CVs and for the weakness of the Balmer absorption edge (relative to
simple models of optically thick accretion disks). We find that a standard disk
wind model that is successful in reproducing the UV spectra of CVs also leaves
a noticeable imprint on the optical spectrum, particularly for systems viewed
at high inclination. The strongest optical wind-formed recombination lines are
H and He II . We demonstrate that a higher-density outflow
model produces all the expected H and He lines and produces a recombination
continuum that can fill in the Balmer jump at high inclinations. This model
displays reasonable verisimilitude with the optical spectrum of RW Trianguli.
No single-peaked emission is seen, although we observe a narrowing of the
double-peaked emission lines from the base of the wind. Finally, we show that
even denser models can produce a single-peaked H line. On the basis of
our results, we suggest that winds can modify, and perhaps even dominate, the
line and continuum emission from CVs.Comment: 15 pages, 13 figures. Accepted to MNRA
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