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Design and Development of a Ka-band Interferometer for Cryospheric Applications
Topographic maps of the earth are essential to geographic and earth science studies. In particular, mapping and estimating physical parameters of the earth’s water and ice cover are critical to global climate studies. Among these, snow, ocean and fresh water topography, snow wetness and water equivalent are of immediate interest to the scientific community.
Challenges in the instrument development and deployment posed by these required measurements are twofold. Firstly, these measurements are required to have global coverage, yet maintain stringent spatial resolution and accuracy margins. Secondly, snow topography measurement requires minimal electromagnetic wave penetration through snow, hence requiring the use of millimeter-wave frequency radars. While having the advantage of smaller and lighter structures, instruments at millimeter-wave frequencies are difficult to design, evaluate and deploy due to their mechanical and electric precision requirements.
This thesis presents the design, development, detailed evaluation and first deployment of a Ka-band interferometer. An overview of the theory of interferometric mapping is presented including a discussion on instrument sensitivity and accuracy. Based in this theory, a geometric and hardware configuration for a rooftop deployment is arrived at. Detailed design and evaluation of the radar receiver is documented. Lastly first results from a rooftop and ground-based deployment are presented
All-sky signals from recombination to reionization with the SKA
Cosmic evolution in the hydrogen content of the Universe through
recombination and up to the end of reionization is expected to be revealed as
subtle spectral features in the uniform extragalactic cosmic radio background.
The redshift evolution in the excitation temperature of the 21-cm spin flip
transition of neutral hydrogen appears as redshifted emission and absorption
against the cosmic microwave background. The precise signature of the spectral
trace from cosmic dawn and the epoch of reionization are dependent on the
spectral radiance, abundance and distribution of the first bound systems of
stars and early galaxies, which govern the evolution in the spin-flip level
populations. Redshifted 21 cm from these epochs when the spin temperature
deviates from the temperature of the ambient relic cosmic microwave background
results in an all-sky spectral structure in the 40-200 MHz range, almost wholly
within the band of SKA-Low. Another spectral structure from gas evolution is
redshifted recombination lines from epoch of recombination of hydrogen and
helium; the weak all-sky spectral structure arising from this event is best
detected at the upper end of the 350-3050 MHz band of SKA-mid. Total power
spectra of SKA interferometer elements form the measurement set for these faint
signals from recombination and reionization; the inter-element interferometer
visibilities form a calibration set. The challenge is in precision polarimetric
calibration of the element spectral response and solving for additives and
unwanted confusing leakages of sky angular structure modes into spectral modes.
Herein we discuss observing methods and design requirements that make possible
these all-sky SKA measurements of the cosmic evolution of hydrogen.Comment: Accepted for publication in the SKA Science Book 'Advancing
Astrophysics with the Square Kilometre Array', to appear in 201
Hunting for exoplanets via magnetic star-planet interactions: geometrical considerations for radio emission
Recent low-frequency radio observations suggest that some nearby M dwarfs
could be interacting magnetically with undetected close-in planets, powering
the emission via the electron cyclotron maser (ECM) instability. Confirmation
of such a scenario could reveal the presence of close-in planets around M
dwarfs, which are typically difficult to detect via other methods. ECM emission
is beamed, and is generally only visible for brief windows depending on the
underlying system geometry. Due to this, detection may be favoured at certain
orbital phases, or from systems with specific geometric configurations. In this
work, we develop a geometric model to explore these two ideas. Our model
produces the visibility of the induced emission as a function of time, based on
a set of key parameters that characterise magnetic star-planet interactions.
Utilising our model, we find that the orbital phases where emission appears are
highly dependent on the underlying parameters, and does not generally appear at
the quadrature points in the orbit as is seen for the Jupiter-Io interaction.
Then using non-informative priors on the system geometry, we show that
untargeted radio surveys are biased towards detecting emission from systems
with planets in near face-on orbits. While transiting exoplanets are still
likely to be detectable, they are less likely to be seen than those in near
face-on orbits. Our forward model serves to be a powerful tool for both
interpreting and appropriately scheduling radio observations of exoplanetary
systems, as well as inverting the system geometry from observations.Comment: 19 pages, 16 figures. Accepted for publication in MNRA
Radio emission as a stellar activity indicator
Radio observations of stars trace the plasma conditions and magnetic field
properties of stellar magnetospheres and coronae. Depending on the plasma
conditions at the emitter site, radio emission in the metre- and decimetre-wave
bands is generated via different mechanisms such as gyrosynchrotron, electron
cyclotron maser instability, and plasma radiation processes. The ongoing LOFAR
Two-metre Sky Survey (LoTSS) and VLA Sky Survey (VLASS) are currently the most
sensitive wide-field radio sky surveys ever conducted. Because these surveys
are untargeted, they provide an opportunity to study the statistical properties
of the radio-emitting stellar population in an unbiased manner. Here, we
perform an untargeted search for stellar radio sources down to sub-mJy level
using these radio surveys. We find that the population of radio-emitting
stellar systems is mainly composed of two distinct categories:
chromospherically active stellar (CAS) systems and M dwarfs. We also seek to
identify signatures of a gradual transition within the M-dwarf population from
chromospheric/coronal acceleration close to the stellar surface similar to that
observed on the Sun, to magnetospheric acceleration occurring far from the
stellar surface similar to that observed on Jupiter. We determine that radio
detectability evolves with spectral type, and we identify a transition in radio
detectability around spectral type M4, where stars become fully convective.
Furthermore, we compare the radio detectability vs spectra type with X-ray and
optical flare (observed by TESS) incidence statistics. We find that the radio
efficiency of X-ray/optical flares, which is the fraction of flare energy
channelled into radio-emitting charges, increases with spectral type. These
results motivate us to conjecture that the emergence of large-scale magnetic
fields in CAS systems and later M dwarfs leads to an increase in radio
efficiency.Comment: 29 pages, 14 figures, 5 tables. Accepted for publication in A&
Radio masers on WX UMa : hints of a Neptune-sized planet, or magnetospheric reconnection?
RDK acknowledges funding received from the Irish Research Council (IRC) through the Government of Ireland Postgraduate Scholarship Programme. RDK and AAV acknowledges funding from the European Research Council (ERC) under the European Union’s Horizon 2020 research and innovation programme (grant agreement No 817540, ASTROFLOW). We acknowledge the provisions of the Space Weather Modelling Framework (SWMF) code from the Center for Space Environment Modeling (CSEM) at the University of Michigan, and the computational resources of the Irish Centre for High End Computing (ICHEC), both of which were utilised in this work.The nearby M dwarf WX UMa has recently been detected at radio wavelengths with LOFAR. The combination of its observed brightness temperature and circular polarisation fraction suggests that the emission is generated via the electron-cyclotron maser instability. Two distinct mechanisms have been proposed to power such emission from low-mass stars: either a sub-Alfvénic interaction between the stellar magnetic field and an orbiting planet, or reconnection at the edge of the stellar magnetosphere. In this paper, we investigate the feasibility of both mechanisms, utilising the information about the star’s surrounding plasma environment obtained from modelling its stellar wind. Using this information, we show that a Neptune-sized exoplanet with a magnetic field strength of 10 – 100 G orbiting at ∼0.034 au can accurately reproduce the observed radio emission from the star, with corresponding orbital periods of 7.4 days. Due to the stellar inclination, a planet in an equatorial orbit is unlikely to transit the star. While such a planet could induce radial velocity semi-amplitudes from 7 to 396 m s−1, it is unlikely that this signal could be detected with current techniques due to the activity of the host star. The application of our planet-induced radio emission model here illustrates its exciting potential as a new tool for identifying planet-hosting candidates from long-term radio monitoring. We also develop a model to investigate the reconnection-powered emission scenario. While this approach produces less favourable results than the planet-induced scenario, it nevertheless serves as a potential alternative emission mechanism which is worth exploring further.PostprintPeer reviewe
A simultaneous search for prompt radio emission associated with the short GRB 170112A using the all-sky imaging capability of the OVRO-LWA
We have conducted the most sensitive low frequency (below 100 MHz) search to
date for prompt, low-frequency radio emission associated with short-duration
gamma-ray bursts (GRBs), using the Owens Valley Radio Observatory Long
Wavelength Array (OVRO-LWA). The OVRO-LWA's nearly full-hemisphere
field-of-view (, square degrees) allows us to search for
low-frequency (sub- MHz) counterparts for a large sample of the subset of
GRB events for which prompt radio emission has been predicted. Following the
detection of short GRB 170112A by Swift, we used all-sky OVRO-LWA images
spanning one hour prior to and two hours following the GRB event to search for
a transient source coincident with the position of GRB 170112A. We detect no
transient source, with our most constraining flux density limit of
for frequencies spanning . We
place constraints on a number of models predicting prompt, low-frequency radio
emission accompanying short GRBs and their potential binary neutron star merger
progenitors, and place an upper limit of on the fraction of energy released in the prompt radio
emission. These observations serve as a pilot effort for a program targeting a
wider sample of both short and long GRBs with the OVRO-LWA, including bursts
with confirmed redshift measurements which are critical to placing the most
constraining limits on prompt radio emission models, as well as a program for
the follow-up of gravitational wave compact binary coalescence events detected
by advanced LIGO and Virgo.Comment: 14 pages, 5 figures, ApJ submitte
No Massive Companion to the Coherent Radio-Emitting M Dwarf GJ 1151
The recent detection of circularly polarized, long-duration (>8 hr)
low-frequency (~150 MHz) radio emission from the M4.5 dwarf GJ 1151 has been
interpreted as arising from a star-planet interaction via the electron
cyclotron maser instability. The existence or parameters of the proposed
planets have not been determined. Using 20 new HARPS-N observations, we put
99th-percentile upper limits on the mass of any close companion to GJ 1151 at
Msini < 5.6 M earth. With no stellar, brown dwarf, or giant planet companion
likely in a close orbit, our data are consistent with detected radio emission
emerging from a magnetic interaction between a short-period terrestrial-mass
planet and GJ 1151
The Radio Sky at Meter Wavelengths: m-Mode Analysis Imaging with the Owens Valley Long Wavelength Array
A host of new low-frequency radio telescopes seek to measure the 21-cm
transition of neutral hydrogen from the early universe. These telescopes have
the potential to directly probe star and galaxy formation at redshifts , but are limited by the dynamic range they can achieve
against foreground sources of low-frequency radio emission. Consequently, there
is a growing demand for modern, high-fidelity maps of the sky at frequencies
below 200 MHz for use in foreground modeling and removal. We describe a new
widefield imaging technique for drift-scanning interferometers,
Tikhonov-regularized -mode analysis imaging. This technique constructs
images of the entire sky in a single synthesis imaging step with exact
treatment of widefield effects. We describe how the CLEAN algorithm can be
adapted to deconvolve maps generated by -mode analysis imaging. We
demonstrate Tikhonov-regularized -mode analysis imaging using the Owens
Valley Long Wavelength Array (OVRO-LWA) by generating 8 new maps of the sky
north of with 15 arcmin angular resolution, at frequencies
evenly spaced between 36.528 MHz and 73.152 MHz, and 800 mJy/beam thermal
noise. These maps are a 10-fold improvement in angular resolution over existing
full-sky maps at comparable frequencies, which have angular resolutions . Each map is constructed exclusively from interferometric observations
and does not represent the globally averaged sky brightness. Future
improvements will incorporate total power radiometry, improved thermal noise,
and improved angular resolution -- due to the planned expansion of the OVRO-LWA
to 2.6 km baselines. These maps serve as a first step on the path to the use of
more sophisticated foreground filters in 21-cm cosmology incorporating the
measured angular and frequency structure of all foreground contaminants.Comment: 27 pages, 18 figure
Evidence for Cold Plasma in Planetary Nebulae From Radio Observations With the LOw Frequency ARray (LOFAR)
We present observations of planetary nebulae with the LOw Frequency ARray (LOFAR) between 120 and 168 MHz. The images show thermal free–free emission from the nebular shells. We have determined the electron temperatures for spatially resolved, optically thick nebulae. These temperatures are 20%–60% lower than those estimated from collisionally excited optical emission lines. This strongly supports the existence of a cold plasma component, which co-exists with hot plasma in planetary nebulae. This cold plasma does not contribute to the collisionally excited lines, but does contribute to recombination lines and radio flux. Neither of the plasma components are spatially resolved in our images, although we infer that the cold plasma extends to the outer radii of planetary nebulae. However, more cold plasma appears to exist at smaller radii. The presence of cold plasma should be taken into account in modeling of radio emission of planetary nebulae. Modelling of radio emission usually uses electron temperatures calculated from collisionally excited optical and/or infrared lines. This may lead to an underestimate of the ionized mass and an overestimate of the extinction correction from planetary nebulae when derived from the radio flux alone. The correction improves the consistency of extinction derived from the radio fluxes when compared to estimates from the Balmer decrement flux ratios