132 research outputs found
Weak G-band stars on the H-R Diagram: Clues to the origin of Li anomaly
Weak G-band (WGB) stars are a rare class of cool luminous stars that present
a strong depletion in carbon, but also lithium abundance anomalies that have
been little explored in the literature since the first discovery of these
peculiar objects in the early 50's. Here we focus on the Li-rich WGB stars and
report on their evolutionary status. We explore different paths to propose a
tentative explanation for the lithium anomaly. Using archive data, we derive
the fundamental parameters of WGB (Teff, log g, log(L/Lsun)) using Hipparcos
parallaxes and recent temperature scales. From the equivalent widths of Li
resonance line at 6707 {\AA}, we uniformly derive the lithium abundances and
apply when possible NLTE corrections following the procedure described by Lind
et al. (2009). We also compute dedicated stellar evolution models in the mass
range 3.0 to 4.5 Msun, exploring the effects of rotation-induced and
thermohaline mixing. These models are used to locate the WGB stars in the H-R
diagram and to explore the origin of the abundance anomalies. The location of
WGB stars in the H-R diagram shows that these are intermediate mass stars of
masses ranging from 3.0 to 4.5 Msun located at the clump, which implies a
degeneracy of their evolutionary status between subgiant/red giant branch and
core helium burning phases. The atmospheres of a large proportion of WGB stars
(more than 50%) exhibit lithium abundances A(Li) \geq 1.4 dex similar to
Li-rich K giants. The position of WGB stars along with the Li-rich K giants in
the H-R diagram however indicates that both are well separated groups. The
combined and tentatively consistent analysis of the abundance pattern for
lithium, carbon and nitrogen of WGB stars seems to indicate that carbon
underabundance could be decorrelated from the lithium and nitrogen
overabundances.Comment: 13 pages, 3 figures, Accepted for publication in Astronomy and
Astrophysic
Searching for links between magnetic fields and stellar evolution. II. The evolution of magnetic fields as revealed by observations of Ap stars in open clusters and associations
The evolution of magnetic fields in Ap stars during the main sequence phase
is presently mostly unconstrained by observation because of the difficulty of
assigning accurate ages to known field Ap stars.
We are carrying out a large survey of magnetic fields in cluster Ap stars
with the goal of obtaining a sample of these stars with well-determined ages.
In this paper we analyse the information available from the survey as it
currently stands.
We select from the available observational sample the stars that are probably
(1) cluster or association members and (2) magnetic Ap stars. For the stars in
this subsample we determine the fundamental parameters T_eff, log(L/L_o), and
M/M_o. With these data and the cluster ages we assign both absolute age and
fractional age (the fraction of the main sequence lifetime completed). For this
purpose we have derived new bolometric corrections for Ap stars.
Magnetic fields are present at the surfaces of Ap stars from the ZAMS to the
TAMS. Statistically for the stars with M > 3 M_o the fields decline with
advancing age approximately as expected from flux conservation together with
increased stellar radius, or perhaps even faster than this rate, on a time
scale of about 3 10^7 yr. In contrast, lower mass stars show no compelling
evidence for field decrease even on a timescale of several times 10^8 yr.
Study of magnetic cluster stars is now a powerful tool for obtaining
constraints on evolution of Ap stars through the main sequence. Enlarging the
sample of known cluster magnetic stars, and obtaining more precise RMS fields,
will help to clarify the results obtained so far. Further field observations
are in progress.Comment: Accepted by Astronomy & Astrophysic
Abundances of Vanadium and Bromine in 3 Cen A: Additional Odd-Z Anomalies
We report abundance excesses of 1.2 and 2.6 dex, respectively, for vanadium
and bromine in the hot, peculiar star 3 Cen A. Abundances for these two odd-Z
elements have not been previously reported for this star. Taken with previous
work, they strengthen the case of the origin of the abundance peculiarities by
diffusion.Comment: 4 Pages, 2 tables, 2 figures; accepted by Astronomy and Astrophysic
Doppler imaging of the helium-variable star a Cen
The helium-peculiar star a Cen exhibits line profile variations of elements
such as iron, nitrogen and oxygen in addition to its well-known extreme helium
variability. New high S/N, high-resolution spectra are used to perform a
quantitative measurement of the abundances of the star and determine the
relation of the concentrations of the heavier elements on the surface of the
star to the helium concentration and the magnetic field orientation. Doppler
images have been created using programs described in earlier papers by Rice and
others. An alternative surface abundance mapping code has been used to model
the helium line variations after our Doppler imaging of certain individual
helium lines produced mediocre results. We confirm the long-known existence of
helium-rich and helium-poor hemispheres on a Cen and we measure a difference of
more than two orders of magnitude in helium abundance from one side of the star
to the other. Helium is overabundant by a factor of about 5 over much of the
helium-rich hemisphere. Of particular note is our discovery that the
helium-poor hemisphere has a very high abundance of helium-3, approximately
equal to the helium-4 abundance. a Cen is therefore a new member of the small
group of helium-3 stars and the first well-established magnetic member of the
class. For the three metals investigated here, there are two strong
concentrations of abundance near the equator consistent with the positive
magnetic maximum and two somewhat weaker concentrations of abundance where the
helium concentration is centered and roughly where the negative peak of the
magnetic field would be found. Another strong concentration is found near the
equator and this is not explainable in terms of any simple symmetry with the
helium abundance or the apparent magnetic field main polar locations.Comment: 9 pages, 9 figure
The host-galaxy response to the afterglow of GRB 100901A
For Gamma-Ray Burst 100901A, we have obtained Gemini-North and Very Large
Telescope optical afterglow spectra at four epochs: one hour, one day, three
days and one week after the burst, thanks to the afterglow remaining unusually
bright at late times. Apart from a wealth of metal resonance lines, we also
detect lines arising from fine-structure levels of the ground state of Fe II,
and from metastable levels of Fe II and Ni II at the host redshift (z =
1.4084). These lines are found to vary significantly in time. The combination
of the data and modelling results shows that we detect the fall of the Ni II 4
F9/2 metastable level population, which to date has not been observed. Assuming
that the population of the excited states is due to the UV-radiation of the
afterglow, we estimate an absorber distance of a few hundred pc. This appears
to be a typical value when compared to similar studies. We detect two
intervening absorbers (z = 1.3147, 1.3179). Despite the wide temporal range of
the data, we do not see significant variation in the absorption lines of these
two intervening systems.Comment: 17 pages, 9 figures. Accepted by Monthly Notices of the Royal
Astronomical Society on Jan 11th 201
First VLT/X-shooter spectroscopy of early-type stars outside the Local Group
As part of the VLT/X-shooter science verification, we obtained the first
optical medium-resolution spectrum of a previously identified bright O-type
object in NGC55, an LMC-like galaxy at a distance of \sim2.0 Mpc. Based on the
stellar and nebular spectrum, we investigate the nature and evolutionary status
of the central object(s) and its influence on the surrounding interstellar
medium. We conclude that the source, NGC55_C1_31, is a composite object, likely
a stellar cluster, which contains one or several hot (T_eff \simeq 50000 K) WN
stars with a high mass-loss rate (\sim3 \times 10^{-5} M_\odot yr^{-1}) and a
helium-rich composition (N_He/N_H = 0.8). The visual flux is dominated by
OB-type (super)giant stars with T_eff \sim< 35000 K, solar helium abundance
(N_He/N_H = 0.1), and mass-loss rate \sim2 \times 10^{-6} M_\odot yr^{-1}. The
surrounding H II region has an electron density n_e < 10^2 cm^{-3} and an
electron temperature T(OIII) \simeq 11500 \pm 600 K. The oxygen abundance of
this region is [O/H] = 8.18 \pm 0.03 which corresponds to Z = 0.31 \pm 0.04
Z_\odot. We observed no significant gradients in T(OIII), n_e or [O/H] on a
scale of 73 pc extending in four directions from the ionising source. The
properties of the HII region can be reproduced by a CLOUDY model which uses the
central cluster as ionising source, thus providing a self-consistent
interpretation of the data. We also report on the serendipitous discovery of
HeII nebular emission associated with the nearby source NGC55_C2_35, a feature
usually associated with strong X-ray sources.Comment: 12 pages, 10 figures, accepted for publication in Monthly Notices of
the Royal Astronomical Society; the definitive version will be available at
wwww.blackwell-synergy.co
VLT/X-shooter spectroscopy of the afterglow of the Swift GRB 130606A: Chemical abundances and reionisation at
The reionisation of the Universe is thought to have ended around z~6, as
inferred from spectroscopy of distant bright background sources, such as
quasars (QSO) and gamma-ray burst (GRB) afterglows. Furthermore, spectroscopy
of a GRB afterglow provides insight in its host galaxy, which is often too dim
and distant to study otherwise. We present the high S/N VLT/X-shooter spectrum
of GRB130606A at z=5.913. We aim to measure the degree of ionisation of the IGM
between 5.02<z<5.84 and to study the chemical abundance pattern and dust
content of its host galaxy. We measured the flux decrement due to absorption at
Ly, and wavelength regions. The hydrogen and metal
absorption lines formed in the host galaxy were fitted with Voigt profiles to
obtain column densities. Our measurements of the Ly-forest optical
depth are consistent with previous measurements of QSOs, but have a much
smaller uncertainty. The analysis of the red damping wing yields a neutral
fraction (3). We obtain column density measurements of
several elements. The ionisation corrections due to the GRB is estimated to be
negligible (<0.03 dex), but larger corrections may apply due to the
pre-existing radiation field (up to 0.4 dex based on sub-DLA studies). Our
measurements confirm that the Universe is already predominantly ionised over
the redshift range probed in this work, but was slightly more neutral at z>5.6.
GRBs are useful probes of the ionisation state of the IGM in the early
Universe, but because of internal scatter we need a larger statistical sample
to draw robust conclusions. The high [Si/Fe] in the host can be due to dust
depletion, alpha-element enhancement, or a combination of both. The very high
value of [Al/Fe]=2.40+/-0.78 might connected to the stellar population history.
We estimate the host metallicity to be -1.7<[M/H]<-0.9 (2%-13% of solar).
(trunc.)Comment: 15 pages, 12 figure
New Rotation Periods in the Open Cluster NGC 1039 (M 34), and a Derivation of its Gyrochronology Age
Employing photometric rotation periods for solar-type stars in NGC 1039 [M
34], a young, nearby open cluster, we use its mass-dependent rotation period
distribution to derive the cluster's age in a distance independent way, i.e.,
the so-called gyrochronology method. We present an analysis of 55 new rotation
periods,using light curves derived from differential photometry, for solar type
stars in M 34. We also exploit the results of a recently-completed,
standardized, homogeneous BVIc CCD survey of the cluster in order to establish
photometric cluster membership and assign B-V colours to each photometric
variable. We describe a methodology for establishing the gyrochronology age for
an ensemble of solar-type stars. Empirical relations between rotation period,
photometric colour and stellar age (gyrochronology) are used to determine the
age of M 34. Based on its position in a colour-period diagram, each M 34 member
is designated as being either a solid-body rotator (interface or I-star), a
differentially rotating star (convective or C-star) or an object which is in
some transitory state in between the two (gap or g-star). Fitting the period
and photometric colour of each I-sequence star in the cluster, we derive the
cluster's mean gyrochronology age.
47/55 of the photometric variables lie along the loci of the cluster main
sequence in V/B-V and V/V-I space. We are further able to confirm kinematic
membership of the cluster for half of the periodic variables [21/55], employing
results from an on-going radial velocity survey of the cluster. For each
cluster member identified as an I-sequence object in the colour-period diagram,
we derive its individual gyrochronology age, where the mean gyro age of M 34 is
found to be 193 +/- 9 Myr, formally consistent (within the errors) with that
derived using several distance-dependent, photometric isochrone methods (250
+/- 67 Myr).Comment: accepted for publication in Astronomy & Astrophysic
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