224 research outputs found
Absolute Wavelength Shifts - A new diagnostic for rapidly rotating stars
Accuracies reached in space astrometry now permit the accurate determination of astrometric radial velocities, without any use of spectroscopy. Knowing this true stellar motion, spectral shifts intrinsic to stellar atmospheres can be identified, for instance gravitational redshifts and those caused by velocity fields on stellar surfaces. The astrometric accuracy is independent of any spectral complexity, such as the smeared-out line profiles of rapidly rotating stars. Besides a better determination of stellar velocities, this permits more precise studies of atmospheric dynamics, such as possible modifications of stellar surface convection (granulation) by rotation-induced forces, as well as a potential for observing meridional flows across stellar surfaces
Exoplanet Transit Parallax
The timing and duration of exoplanet transits has a dependency on observer
position due to parallax. In the case of an Earth-bound observer with a 2 AU
baseline the dependency is typically small and slightly beyond the limits of
current timing precision capabilities. However, it can become an important
systematic effect in high-precision repeated transit measurements for long
period systems due to its relationship to secular perspective acceleration
phenomena. In this short paper we evaluate the magnitude and characteristics of
transit parallax in the case of exoplanets using simplified geometric examples.
We also discuss further implications of the effect, including its possible
exploitation to provide immediate confirmation of planetary transits and/or
unique constraints on orbital parameters and orientations.Comment: 12 Pages, 3 Figures, Accepted for publication in Ap
Stellar intensity interferometry: Optimizing air Cherenkov telescope array layouts
Kilometric-scale optical imagers seem feasible to realize by intensity
interferometry, using telescopes primarily erected for measuring Cherenkov
light induced by gamma rays. Planned arrays envision 50--100 telescopes,
distributed over some 1--4 km. Although array layouts and telescope sizes
will primarily be chosen for gamma-ray observations, also their interferometric
performance may be optimized. Observations of stellar objects were numerically
simulated for different array geometries, yielding signal-to-noise ratios for
different Fourier components of the source images in the interferometric
-plane. Simulations were made for layouts actually proposed for future
Cherenkov telescope arrays, and for subsets with only a fraction of the
telescopes. All large arrays provide dense sampling of the -plane due to
the sheer number of telescopes, irrespective of their geographic orientation or
stellar coordinates. However, for improved coverage of the -plane and a
wider variety of baselines (enabling better image reconstruction), an exact
east-west grid should be avoided for the numerous smaller telescopes, and
repetitive geometric patterns avoided for the few large ones. Sparse arrays
become severely limited by a lack of short baselines, and to cover
astrophysically relevant dimensions between 0.1--3 milliarcseconds in visible
wavelengths, baselines between pairs of telescopes should cover the whole
interval 30--2000 m.Comment: 12 pages, 10 figures; presented at the SPIE conference "Optical and
Infrared Interferometry II", San Diego, CA, USA (June 2010
Long-baseline optical intensity interferometry: Laboratory demonstration of diffraction-limited imaging
A long-held vision has been to realize diffraction-limited optical aperture
synthesis over kilometer baselines. This will enable imaging of stellar
surfaces and their environments, and reveal interacting gas flows in binary
systems. An opportunity is now opening up with the large telescope arrays
primarily erected for measuring Cherenkov light in air induced by gamma rays.
With suitable software, such telescopes could be electronically connected and
also used for intensity interferometry. Second-order spatial coherence of light
is obtained by cross correlating intensity fluctuations measured in different
pairs of telescopes. With no optical links between them, the error budget is
set by the electronic time resolution of a few nanoseconds. Corresponding
light-travel distances are approximately one meter, making the method
practically immune to atmospheric turbulence or optical imperfections,
permitting both very long baselines and observing at short optical wavelengths.
Previous theoretical modeling has shown that full images should be possible to
retrieve from observations with such telescope arrays. This project aims at
verifying diffraction-limited imaging experimentally with groups of detached
and independent optical telescopes. In a large optics laboratory, artificial
stars were observed by an array of small telescopes. Using high-speed
photon-counting solid-state detectors, intensity fluctuations were
cross-correlated over up to 180 baselines between pairs of telescopes,
producing coherence maps across the interferometric Fourier-transform plane.
These measurements were used to extract parameters about the simulated stars,
and to reconstruct their two-dimensional images. As far as we are aware, these
are the first diffraction-limited images obtained from an optical array only
linked by electronic software, with no optical connections between the
telescopes.Comment: 13 pages, 9 figures, Astronomy & Astrophysics, in press. arXiv admin
note: substantial text overlap with arXiv:1407.599
The fundamental definition of 'radial velocity'
Accuracy levels of metres per second require the fundamental concept of 'radial velocity' for stars and other distant objects to be examined, both as a physical velocity, and as measured by spectroscopic and astrometric techniques. Aiming at definitions that are unambiguous at accuracy levels of 1 m/s, we analyse different concepts of radial velocity and their interrelations. We distinguish between the geometrically defined 'kinematic radial velocity' and 'astrometric radial velocity' on one hand, and the spectroscopically defined 'barycentric radial-velocity measure' on the other. The last two concepts are defined by recent resolutions adopted by the International Astronomical Union (IAU), the motives and consequences of which are explained in this paper
Stellar Intensity Interferometry: Astrophysical targets for sub-milliarcsecond imaging
Intensity interferometry permits very long optical baselines and the
observation of sub-milliarcsecond structures. Using planned kilometric arrays
of air Cherenkov telescopes at short wavelengths, intensity interferometry may
increase the spatial resolution achieved in optical astronomy by an order of
magnitude, inviting detailed studies of the shapes of rapidly rotating hot
stars with structures in their circumstellar disks and winds, or mapping out
patterns of nonradial pulsations across stellar surfaces. Signal-to-noise in
intensity interferometry favors high-temperature sources and emission-line
structures, and is independent of the optical passband, be it a single spectral
line or the broad spectral continuum. Prime candidate sources have been
identified among classes of bright and hot stars. Observations are simulated
for telescope configurations envisioned for large Cherenkov facilities,
synthesizing numerous optical baselines in software, confirming that
resolutions of tens of microarcseconds are feasible for numerous astrophysical
targets.Comment: 12 pages, 4 figures; presented at the SPIE conference "Optical and
Infrared Interferometry II", San Diego, CA, USA (June 2010
The statistics of the photometric accuracy based on MASS data and the evaluation of high-altitude wind
The effect of stellar scintillation on the accuracy of photometric
measurements is analyzed. We obtain a convenient form of estimaton of this
effect in the long exposure regime, when the turbulence shift produced by the
wind is much larger than the aperture of the telescope. A simple method is
proposed to determine index introduced by perture of the Kenyon et al.
(2006), directly from the measurements with the Multi Aperture Scintillation
Sensor (MASS) without information on vertical profile of the wind. The
statistics resulting from our campaign of 2005 -- 2007 at Maidanak
observatory is presented. It is shown that these data can be used to estimate
high-altitude winds at pressure level 70 -- 100 mbar. Comparison with the wind
speed retrieved from the NCEP/NCAR global models shows a good agreement. Some
prospects for retrieval of the wind speed profile from the MASS measurements
are outlined.Comment: 11 pages, 9 figures, accepted for publication in Astronomy Letter
Spectroscopic Observations of Convective Patterns in the Atmospheres of Metal-Poor Stars
Convective line asymmetries in the optical spectrum of two metal-poor stars,
Gmb1830 and HD140283, are compared to those observed for solar metallicity
stars. The line bisectors of the most metal-poor star, the subgiant HD140283,
show a significantly larger velocity span that the expectations for a
solar-metallicity star of the same spectral type and luminosity class. The
enhanced line asymmetries are interpreted as the signature of the lower metal
content, and therefore opacity, in the convective photospheric patterns. These
findings point out the importance of three-dimensional convective velocity
fields in the interpretation of the observed line asymmetries in metal-poor
stars, and in particular, urge for caution when deriving isotopic ratios from
observed line shapes and shifts using one-dimensional model atmospheres.
The mean line bisector of the photospheric atomic lines is compared with
those measured for the strong Mg I b1 and b2 features. The upper part of the
bisectors are similar, and assuming they overlap, the bottom end of the
stronger lines, which are formed higher in the atmosphere, goes much further to
the red. This is in agreement with the expected decreasing of the convective
blue-shifts in upper atmospheric layers, and compatible with the high velocity
redshifts observed in the chromosphere, transition region, and corona of
late-type stars.Comment: 27 pages, LaTeX; 10 Figures (14 PostScript files); to be published in
The Astrophysical Journa
Stellar Intensity Interferometry: Imaging capabilities of air Cherenkov telescope arrays
Sub milli-arcsecond imaging in the visible band will provide a new
perspective in stellar astrophysics. Even though stellar intensity
interferometry was abandoned more than 40 years ago, it is capable of imaging
and thus accomplishing more than the measurement of stellar diameters as was
previously thought. Various phase retrieval techniques can be used to
reconstruct actual images provided a sufficient coverage of the interferometric
plane is available. Planned large arrays of Air Cherenkov telescopes will
provide thousands of simultaneously available baselines ranging from a few tens
of meters to over a kilometer, thus making imaging possible with unprecedented
angular resolution. Here we investigate the imaging capabilities of arrays such
as CTA or AGIS used as Stellar Intensity Interferometry receivers. The study
makes use of simulated data as could realistically be obtained from these
arrays. A Cauchy-Riemann based phase recovery allows the reconstruction of
images which can be compared to the pristine image for which the data were
simulated. This is first done for uniform disk stars with different radii and
corresponding to various exposure times, and we find that the uncertainty in
reconstructing radii is a few percent after a few hours of exposure time.
Finally, more complex images are considered, showing that imaging at the
sub-milli-arc-second scale is possible.Comment: 10 pages, 6 figures; presented at the SPIE conference "Optical and
Infrared Interferometry II", San Diego, CA, USA (June 2010
Granulation in K-type Dwarf Stars. II. Hydrodynamic simulations and 3D spectrum synthesis
We construct a 3D radiative-hydrodynamic model atmosphere of parameters Teff
= 4820 K, log g = 4.5, and solar chemical composition. The theoretical line
profiles computed with this model are asymmetric, with their bisectors having a
characteristic C-shape and their core wavelengths shifted with respect to their
laboratory values. The line bisectors span from about 10 to 250 m/s, depending
on line strength, with the stronger features showing larger span. The
corresponding core wavelength shifts range from about -200 m/s for the weak Fe
I lines to almost +100 m/s in the strong Fe I features. Based on observational
results for the Sun, we argue that there should be no core wavelength shift for
Fe I lines of EW > 100 mA. The cores of the strongest lines show contributions
from the uncertain top layers of the model, where non-LTE effects and the
presence of the chromosphere, which are important in real stars, are not
accounted for. The comparison of model predictions to observed Fe I line
bisectors and core wavelength shifts for a reference star, HIP86400, shows
excellent agreement, with the exception of the core wavelength shifts of the
strongest features, for which we suspect inaccurate theoretical values. Since
this limitation does not affect the predicted line equivalent widths
significantly, we consider our 3D model validated for photospheric abundance
work.Comment: A&A, in pres
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