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Scientific Highlights Astronomical
discoveries following from observations SOLAR SYSTEM | GALAXY | EXTRAGALACTIC | OBSERVATIONAL COSMOLOGY | OTHER SCIENTIFIC HIGHLIGHTS BRIEFLY |
THE BEST CANDIDATE TO UNDERGO A SUPERNOVA EXPLOSION WHT+UES The Utrecht Echelle Spectrograph (UES) on the William Herschel Telescope has allowed astronomers to monitor Rho Cassiopeiae (ρ Cas or HD 224014) in detail from 1993 to 2002. The observations were aimed at investigating the processes occurring when yellow hypergiants approach and bounce against the Yellow Evolutionary Void, and the results revealed almost regular variations of temperature within a few hundred degrees. However, what happened with ρ Cas during the summer of 2000 went beyond anybody's expectations. The star suddenly cooled down from 7,000 to 4,000 degrees within a few months. Astronomers discovered molecular absorption bands of titanium-oxide (TiO) formed in the slowly expanding atmosphere, suggesting that they had witnessed the formation of a cool and extended shell which was detached from the star by a shock wave carrying a mass equal to 10% of our Sun or 10,000 times the mass of the Earth. This is the highest amount of ejected material astronomers have ever witnessed in a single stellar eruption.
ρ Cas experienced periods of excessive mass loss in 1893 and around 1945, that appeared to be associated with a decrease in effective temperature and the formation of a dense envelope. The results suggest that ρ Cas goes through these events every 50 years approximately. The recurrent eruptions of ρ Cas recorded over the past century are the hallmark of the exceptional atmospheric physics manifested by the yellow hypergiants. These cool luminous stars are thought to be post-red supergiants, rapidly evolving toward the blue supergiant phase. They are rare enigmatic objects, and continuous high-resolution spectroscopic investigations are limited to a small sample of bright stars (only seven of them are known in our Galaxy), often showing dissimilar spectra, but with very peculiar spectral properties. Yellow hypergiants are the candidates "par excellence" among the cool luminous stars to investigate the physical causes for the luminosity limit of evolved stars. They are peculiar stars because they display an uncommon combination of brightness and temperature, which places them in a so-called Yellow Evolutionary Void. When approaching the Void these stars may show signs of peculiar instability. Theoretically, they cannot cross the Void unless they have lost sufficient mass. During this process these stars end up in a supernova explosion: their ultimate and violent fate. The process of approaching the Void however, has not yet been studied observationally in sufficient detail as these events are very rare. Since the event in the year 2000, ρ Cas' atmosphere has been pulsating in a strange manner. Its outer layer now seems to be collapsing again, an event that looks similar to one that preceded the last outburst. The researchers think ρ Cas, at a distance of 10,000 light-years away from the Earth, could end up in a supernova explosion at any time as it has almost consumed the nuclear fuel at its core. It is perhaps the best candidate for a supernova in our Galaxy and the monitoring of this and other unstable evolved stars may help astronomers to shed some light on the very complicated evolutionary episodes that precede supernova explosions.
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| ONE RING TO ENCOMPASS THEM ALL INT+WFC, WFS archive A vast, but previously unknown structure was discovered around our own Milky Way galaxy by an international team of astronomers. Their observations suggest that there is a giant ring of several hundred million stars surrounding the main disk of the Milky Way. Despite its size, the ring has not been clearly seen before since the stars are spread around the whole sky, and are far fewer in number than the tens of billions of stars making up the rest of the Galaxy. Although known to be warped, probably from encounters
with its orbiting satellite galaxies, the disk of the Milky Way was
otherwise thought to be a relatively simple structure. The disk is roughly
100,000 light years across, with the Sun embedded in it and offset some
30,000 light years from the centre. From this vantage point, the nearest
edge of the ring is about 30,000 light years away, in the direction of the
constellation Monoceros, opposite the centre of the Galaxy. This region
of sky is where traces of the ring were first discovered. The data, taken with the Isaac Newton Telescope
Wide Field Camera, show a population narrowly aligned along the line
of sight, but with a galactocentric distance that changes from
Owing to our location within the disc of the Milky
Way, studies of the global structure of this Galactic component are hampered
by projection problems, crowding, dust, and the presence of intervening
populations (such as the bulge). Nowhere is this so problematic as in the
study of the very outer edge of the disc. The advent of the recent wide-area
infrared surveys (e.g. 2MASS and DENIS) have alleviated the extinction problem,
but the other problems remain, with the distance ambiguity being particularly
limiting. Even the future astrometric mission GAIA is unlikely to give
us a full picture of the Galactic disc, owing to telemetry limits in regions
of high stellar density. The INT WFS devotes a large fraction of observing
time to deep and wide-field surveys. Many fields have now been observed
since 1998. In examining INT WFC survey fields, the discovery team of astronomers
has been able to detect the presence of this unexpected feature in several
distant fields. However, the resulting coverage at the present time is
patchy, with most time having been spent in large extragalactic surveys
towards the Galactic polar caps. In the following figure an example of
one of these fields is displayed, the Elais field N1, located at l=
85°, b=+44°, which shows the normal Galactic stellar
population sequences. The Galactic disc dwarfs contribute to the well-populated
red vertical structure at ( g - r )0
Next figure displays the colour-magnitude diagram of the INT WFC field WFS-0801 (located at l=180°, b=+30°); a population that follows a track similar to a narrow main sequence is seen in addition to the usual Galactic components. This sequence is shown more clearly in the right-hand panel of the following figure, in which the Elais-N1 field has been used as a background to subtract the normal Galactic components.
It is clear that this structure cannot be related
to the normal thin disc, as it lies several magnitudes below the expected
thin disc sequence. The rapid decline in the density of the feature away
from the Galactic plane also rules out a direct connection to the halo.
This leaves the thick disc as the only normal Galactic option. However,
its nature remains a puzzle, and it is difficult to ascertain whether it
is a Galactic ring, an inhomogeneous mess arising from ancient warps and
disturbances, or part of a disrupted satellite stream. Ultimately, detailed studies of this kind of the
structure of the Milky Way and other galaxies, reveal how they came
into being and have evolved over the lifetime of the universe. If
this manifestly old population turns out to be the outer stellar disc,
it will pose a very interesting challenge to galaxy formation models that
predict inside-out assembly. Alternatively, if it transpires that the structure
is due to a disrupted satellite whose orbit has been circularized and accreted
along with its cargo of dark matter on to the disc, it will provide a unique
first-hand opportunity to understand the effect of massive accretions on
to the inner regions of galaxies. |
A DEARTH OF DARK MATTER IN ORDINARY ELLIPTICAL GALAXIES WHT+PN.S Over the past 25 years, astronomers have progressed from being surprised by the existence of dark matter to understanding that most of the universe is dominated by exotic nonluminous material. In the prevailing paradigm, the gravitational influence of cold dark matter (CDM) is crucial to the formation of structure, seeding the collapse and aggregation of luminous systems. An inherent consequence of CDM's role in these processes is that galaxies have massive, extended CDM halos. Indeed, such halos are evident around spiral galaxies, in which the rotational speeds in the extended cold-gas disks do not decrease outside the visible stars—a gravitational signature of dark matter. The evidence for dark matter in elliptical galaxies is still circumstantial. Assessments of the total masses of individual elliptical systems have generally been confined to the very brightest systems, for which the gravitational potential can be measured using X-ray emission or strong gravitational lensing, and to nearby dwarfs, for which the kinematics of individual stars offer a probe of the mass distribution. More "ordinary" elliptical galaxies are more difficult to study because in general they lack a simple kinematical probe at the larger radii, where dark matter is expected to dominate. The velocity distribution of the diffuse stellar light is the natural candidate, but studies have been limited by the faintness of galaxies' outer parts to radii that are 2 Reff, where Reff is the galaxy's effective radius, which encloses half of its projected light. A powerful alternative is offered by Planetary Nebulas (PNs), which are detectable even in distant galaxies through their characteristic strong emission lines. Once found, their line-of-sight velocities can be readily determined by the Doppler shift in these emission lines. These objects have been used in the past as tracers of the stellar kinematics of galaxies, but the procedure of locating them with narrow-band imaging surveys and then blindly obtaining spectra at the identified positions has proven difficult to implement efficiently on a large scale. A specialized instrument, the Planetary Nebula Spectrograph (PN.S), was developed specifically to study the kinematics of PNs in elliptical galaxies. The PN.S uses counterdispersed imaging (a type of slitless spectroscopy) over a wide field to detect and measure velocities for PNs simultaneously by using their [O III] emissions at 500.7 nm. Because it is optimized for this purpose, the PN.S is far more efficient for extragalactic PN studies than any other existing instrumentation. Observations with the PN.S on the William Herschel Telescope allowed astronomers to extend stellar kinematic studies to the outer parts of three intermediate-luminosity elliptical galaxies: NGC 821, NGC 3379, and NGC 4494. In each of these systems, they measured 100 PN velocities with uncertainties of 20 km s–1 out to radii of 4 to 6 Reff. The line-of-sight velocities in the outer parts of all of these galaxies show a clear decline in dispersion with the radius. A decrease in random velocities with the radius has been indicated by small samples of PNs around NGC 3379, but the more extensive data set presented here provides a more definitive measurement of this decline, and reveals that it also occurs in other similar galaxies. The new data are inconsistent with simple dark halo models and thus different from kinematical results for brighter ellipticals.
More unexpectedly, the velocity dispersion data are consistent with simple models containing no dark matter, showing the nearly Keplerian decline with the radius outside 2 Reff that such models predict and suggesting that these systems are not embedded in massive dark halos.
This result clashes with conventional conceptions of galaxy formation. In particular, if ellipticals are built up by mergers of smaller galaxies, it is puzzling that the resulting systems show little trace of their precursors' dark matter halos. And it is also apparent that some important physics is still missing from the recipes for galaxy formation. For example, substantial portions of these galaxies' dark matter halos could have been shed through interactions with other galaxies. Such stripping has been inferred for ellipticals near the centers of dense galaxy clusters, but the galaxies studied here are in much sparser environments, in which substantial stripping is not expected to be an important process. Crucial to understanding the incidence and origin of this low–dark matter phenomenon will be the results for a large sample of ellipticals with a broad range of properties, including differing environmental densities, which could be a key factor in determining halo outcomes; the continuing PN.S observing program will provide this sample. Some references:
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EXTENDING COSMIC
SHEAR MEASUREMENTS WITH THE WILLIAM HERSCHEL TELESCOPE Astronomers extended the original detection of the cosmic shear on
the William Herschel Telescope by increasing the number of observed fields,
with a further increase in area as a result of the larger 16×16 arcmin2
size of field with the new prime focus mosaic camera. The aim
of the survey was to acquire deep (z The cosmic shear with both Keck and WHT was measured at a signal-to-noise
of 5.1, finding an amplitude of the matter power spectrum of σ 8
(Ωm/0.3)0.68= 0.97 ± 0.13, with 0.14 <Ωm<
0.65, including all contributions to the 68 per cent confidence level uncertainty:
statistical noise, sample variance, covariance between angular bins, systematic
effects and redshift uncertainty. A measurement of this quantity from cosmic
shear is cosmologically valuable, as it represents a direct measure of the
amplitude of mass fluctuations.
These results for Keck and WHT are consistent with each other, strengthening
confidence in control of systematics. The joint results are also consistent
with other recent cosmic shear measurements. They also agree with the old
cluster abundance normalization. However, they can not rule out lower cluster-abundance
normalization which has been derived recently. This discrepancy, if confirmed,
could arise from unknown systematics in either the cluster or cosmic shear
methods. For the cluster method, further studies would be needed to understand
the difference between the observed mass-temperature relation and that found
in numerical simulations. It is important to understand the origin of the
discrepancy between cosmic shear and cluster abundance methods. If this is
not explained by such systematics, it could point towards a failure of the
standard ΛCDM paradigm, and therefore have important consequences for cosmology. Some references: |
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