M. F. Morales
University of Washington
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Publications of the Astronomical Society of Australia | 2013
S. J. Tingay; R. Goeke; Judd D. Bowman; D. Emrich; S. M. Ord; D. A. Mitchell; M. F. Morales; T. Booler; B. Crosse; R. B. Wayth; C. J. Lonsdale; S. E. Tremblay; D. Pallot; T. Colegate; Andreas Wicenec; N. Kudryavtseva; W. Arcus; David G. Barnes; G. Bernardi; F. Briggs; S. Burns; John D. Bunton; R. J. Cappallo; B. E. Corey; Avinash A. Deshpande; L. deSouza; B. M. Gaensler; L. J. Greenhill; Peter Hall; B. J. Hazelton
The Murchison Widefield Array (MWA) is one of three Square Kilometre Array Precursor telescopes and is located at the Murchison Radio-astronomy Observatory in the Murchison Shire of the mid-west of Western Australia, a location chosen for its extremely low levels of radio frequency interference. The MWA operates at low radio frequencies, 80–300 MHz, with a processed bandwidth of 30.72 MHz for both linear polarisations, and consists of 128 aperture arrays (known as tiles) distributed over a ~3-km diameter area. Novel hybrid hardware/software correlation and a real-time imaging and calibration systems comprise the MWA signal processing backend. In this paper, the as-built MWA is described both at a system and sub-system level, the expected performance of the array is presented, and the science goals of the instrument are summarised.
Annual Review of Astronomy and Astrophysics | 2010
M. F. Morales; J. Stuart B. Wyithe
Measurement of the spatial distribution of neutral hydrogen via the redshifted 21-cm line promises to revolutionize our knowledge of the epoch of reionization and the first galaxies, and may provide a powerful new tool for observational cosmology from redshifts 1<z<4. In this review we discuss recent advances in our theoretical understanding of the epoch of reionization (EoR), the application of 21-cm tomography to cosmology and measurements of the dark energy equation of state after reionization, and the instrumentation and observational techniques shared by 21-cm EoR and postreionization cosmology machines. We place particular emphasis on the expected signal and observational capabilities of first generation 21-cm fluctuation instruments.
Publications of the Astronomical Society of Australia | 2013
Judd D. Bowman; Iver H. Cairns; David L. Kaplan; Tara Murphy; Divya Oberoi; Lister Staveley-Smith; W. Arcus; David G. Barnes; G. Bernardi; F. Briggs; Shea Brown; John D. Bunton; Adam J. Burgasser; R. J. Cappallo; Shami Chatterjee; B. E. Corey; Anthea J. Coster; Avinash A. Deshpande; L. deSouza; D. Emrich; Philip J. Erickson; R. Goeke; B. M. Gaensler; L. J. Greenhill; L. Harvey-Smith; B. J. Hazelton; David Herne; Jacqueline N. Hewitt; M. Johnston-Hollitt; J. Kasper
Significant new opportunities for astrophysics and cosmology have been identified at low radio frequencies. The Murchison Widefield Array is the first telescope in the southern hemisphere designed specifically to explore the low-frequency astronomical sky between 80 and 300 MHz with arcminute angular resolution and high survey efficiency. The telescope will enable new advances along four key science themes, including searching for redshifted 21-cm emission from the EoR in the early Universe; Galactic and extragalactic all-sky southern hemisphere surveys; time-domain astrophysics; and solar, heliospheric, and ionospheric science and space weather. The Murchison Widefield Array is located in Western Australia at the site of the planned Square Kilometre Array (SKA) low-band telescope and is the only low-frequency SKA precursor facility. In this paper, we review the performance properties of the Murchison Widefield Array and describe its primary scientific objectives.
The Astrophysical Journal | 2009
Judd D. Bowman; M. F. Morales; Jacqueline N. Hewitt
Subtraction of astrophysical foreground contamination from “dirty” sky maps produced by simulated measurements of the Murchison Widefield Array (MWA) has been performed by fitting a third-order polynomial along the spectral dimension of each pixel in the data cubes. The simulations are the first to include the unavoidable instrumental effects of the frequency-dependent primary antenna beams and synthesized array beams. They recover the onedimensional spherically binned input redshifted 21 cm power spectrum within ∼ 1% over the scales probed most sensitively by the MWA (0.01 k 1M pc −1 ) and demonstrate that realistic instrumental effects will not mask the epoch of reionization signal. We find that the weighting function used to produce the dirty sky maps from the gridded visibility measurements is important to the success of the technique. Uniform weighting of the visibility measurements produces the best results, whereas natural weighting significantly worsens the foreground subtraction by coupling structure in the density of the visibility measurements to spectral structure in the dirty sky map data cube. The extremely dense uv-coverage of the MWA was found to be advantageous for this technique and produced very good results on scales corresponding to |u| 500λ in the uv-plane without any selective editing of the uv-coverage.
Monthly Notices of the Royal Astronomical Society | 2014
A. R. Offringa; B. McKinley; Natasha Hurley-Walker; F. Briggs; R. B. Wayth; David L. Kaplan; M. E. Bell; L. Feng; A. R. Neben; J. D. Hughes; Jonghwan Rhee; Tara Murphy; N. D. R. Bhat; G. Bernardi; Judd D. Bowman; R. J. Cappallo; B. E. Corey; Avinash A. Deshpande; D. Emrich; A. Ewall-Wice; B. M. Gaensler; R. Goeke; L. J. Greenhill; B. J. Hazelton; L. Hindson; M. Johnston-Hollitt; Daniel C. Jacobs; J. Kasper; E. Kratzenberg; E. Lenc
Astronomical widefield imaging of interferometric radio data is computationally expensive, especially for the large data volumes created by modern non-coplanar many-element arrays. We present a new widefield interferometric imager that uses the w-stacking algorithm and can make use of the w-snapshot algorithm. The performance dependencies of CASAs w-projection and our new imager are analysed and analytical functions are derived that describe the required computing cost for both imagers. On data from the Murchison Widefield Array, we find our new method to be an order of magnitude faster than w-projection, as well as being capable of full-sky imaging at full resolution and with correct polarisation correction. We predict the computing costs for several other arrays and estimate that our imager is a factor of 2-12 faster, depending on the array configuration. We estimate the computing cost for imaging the low-frequency Square-Kilometre Array observations to be 60 PetaFLOPS with current techniques. We find that combining w-stacking with the w-snapshot algorithm does not significantly improve computing requirements over pure w-stacking. The source code of our new imager is publicly released.
Monthly Notices of the Royal Astronomical Society | 2017
Natasha Hurley-Walker; J. R. Callingham; Paul Hancock; Thomas M. O. Franzen; L. Hindson; A. D. Kapińska; J. Morgan; A. R. Offringa; R. B. Wayth; C. Wu; Q. Zheng; Tara Murphy; M. E. Bell; K. S. Dwarakanath; Bi-Qing For; B. M. Gaensler; M. Johnston-Hollitt; E. Lenc; P. Procopio; Lister Staveley-Smith; Ron D. Ekers; Judd D. Bowman; F. Briggs; R. J. Cappallo; Avinash A. Deshpande; L. J. Greenhill; Brynah J. Hazelton; David L. Kaplan; Colin J. Lonsdale; S. R. McWhirter
Using the Murchison Widefield Array (MWA), the low-frequency Square Kilometre Array precursor located in Western Australia, we have completed the GaLactic and Extragalactic All-sky MWA (GLEAM) survey and present the resulting extragalactic catalogue, utilizing the first year of observations. The catalogue covers 24 831 square degrees, over declinations south of +30° and Galactic latitudes outside 10° of the Galactic plane, excluding some areas such as the Magellanic Clouds. It contains 307 455 radio sources with 20 separate flux density measurements across 72–231 MHz, selected from a time- and frequency-integrated image centred at 200 MHz, with a resolution of ≈ 2 arcmin. Over the catalogued region, we estimate that the catalogue is 90 per cent complete at 170 mJy and 50 per cent complete at 55 mJy and large areas are complete at even lower flux density levels. Its reliability is 99.97 per cent above the detection threshold of 5σ, which itself is typically 50 mJy. These observations constitute the widest fractional bandwidth and largest sky area survey at radio frequencies to date and calibrate the low-frequency flux density scale of the southern sky to better than 10 per cent. This paper presents details of the flagging, imaging, mosaicking and source extraction/characterization, as well as estimates of the completeness and reliability. All source measurements and images are available online. 1 This is the first in a series of publications describing the GLEAM survey results.
Publications of the Astronomical Society of Australia | 2015
R. B. Wayth; E. Lenc; M. E. Bell; J. R. Callingham; K. S. Dwarakanath; Thomas M. O. Franzen; Bi Qing For; B. M. Gaensler; Paul Hancock; L. Hindson; Natasha Hurley-Walker; C. A. Jackson; M. Johnston-Hollitt; A. D. Kapińska; B. McKinley; J. Morgan; A. R. Offringa; P. Procopio; Lister Staveley-Smith; C. Wu; Q. Zheng; Cathryn M. Trott; G. Bernardi; Judd D. Bowman; F. Briggs; R. J. Cappallo; B. E. Corey; Avinash A. Deshpande; D. Emrich; R. Goeke
© Astronomical Society of Australia 2015; published by Cambridge University Press. This is an Open Access article distributed in accordance with the terms of the Creative Commons Attribution (CC BY 4.0) license, which permits others to distribute, remix, adapt and build upon this work, for commercial use, provided the original work is properly cited. See: http://creativecommons.org/licenses/by/4.0/
The Astrophysical Journal | 2013
Nithyanandan Thyagarajan; N. Udaya Shankar; Ravi Subrahmanyan; W. Arcus; G. Bernardi; Judd D. Bowman; F. Briggs; John D. Bunton; R. J. Cappallo; B. E. Corey; L. deSouza; D. Emrich; B. M. Gaensler; R. Goeke; L. J. Greenhill; B. J. Hazelton; David Herne; Jacqueline N. Hewitt; M. Johnston-Hollitt; David L. Kaplan; J. Kasper; B. B. Kincaid; R. Koenig; E. Kratzenberg; Colin J. Lonsdale; M. J. Lynch; S. Russell McWhirter; D. A. Mitchell; M. F. Morales; E. Morgan
In this paper, we explore for the first time the relative magnitudes of three fundamental sources of uncertainty, namely, foreground contamination, thermal noise, and sample variance, in detecting the H I power spectrum from the epoch of reionization (EoR). We derive limits on the sensitivity of a Fourier synthesis telescope to detect EoR based on its array configuration and a statistical representation of images made by the instrument. We use the Murchison Widefield Array (MWA) configuration for our studies. Using a unified framework for estimating signal and noise components in the H I power spectrum, we derive an expression for and estimate the contamination from extragalactic point-like sources in three-dimensional k -space. Sensitivity for EoR H I power spectrum detection is estimated for different observing modes with MWA. With 1000 hr of observing on a single field using the 128 tile MWA, EoR detection is feasible (S/N >1 for k ≲ 0.8 Mpc -1 ). Bandpass shaping and refinements to the EoR window are found to be effective in containing foreground contamination, which makes the instrument tolerant to imaging errors. We find that for a given observing time, observing many independent fields of view does not offer an advantage over a single field observation when thermal noise dominates over other uncertainties in the derived power spectrum.
Publications of the Astronomical Society of the Pacific | 2017
David R. DeBoer; Aaron R. Parsons; James E. Aguirre; Paul Alexander; Zaki S. Ali; Adam P. Beardsley; G. Bernardi; Judd D. Bowman; Richard Bradley; C. L. Carilli; Carina Cheng; Eloy de Lera Acedo; Joshua S. Dillon; A. Ewall-Wice; Gcobisa Fadana; Nicolas Fagnoni; Randall Fritz; Steve Furlanetto; Brian Glendenning; Bradley Greig; Jasper Grobbelaar; B. J. Hazelton; Jacqueline N. Hewitt; Jack Hickish; Daniel C. Jacobs; Austin Julius; MacCalvin Kariseb; Saul A. Kohn; Telalo Lekalake; Adrian Liu
The Hydrogen Epoch of Reionization Array (HERA http://reionization.org) is a staged experiment that uses the unique properties of the 21-cm line from neutral hydrogen to probe the Epoch of Reionization (EOR). During this epoch, roughly 0.3-1 billion years after the Big Bang, the first galaxies and black holes heated and reionized the early Universe. Direct observation of the large scale structure of reionization and its evolution with time will have a profound impact on our understanding of the birth of the first galaxies and black holes, their influence on the intergalactic medium (IGM), and cosmology. This paper will provide an overview of the project and describe the design of the HERA receiving element.
The Astrophysical Journal | 2015
Nithyanandan Thyagarajan; Daniel C. Jacobs; Judd D. Bowman; N. Barry; A. P. Beardsley; G. Bernardi; F. Briggs; R. J. Cappallo; P. Carroll; B. E. Corey; A. de Oliveira-Costa; Joshua S. Dillon; D. Emrich; A. Ewall-Wice; L. Feng; R. Goeke; L. J. Greenhill; B. J. Hazelton; Jacqueline N. Hewitt; Natasha Hurley-Walker; M. Johnston-Hollitt; David L. Kaplan; J. Kasper; Han-Seek Kim; P. Kittiwisit; E. Kratzenberg; E. Lenc; J. Line; Abraham Loeb; Colin J. Lonsdale
Detection of 21 cm emission of H I from the epoch of reionization, at redshifts > z 6, is limited primarily by foreground emission. We investigate the signatures of wide-field measurements and an all-sky foreground model using the delay spectrum technique that maps the measurements to foreground object locations through signal delays between antenna pairs. We demonstrate interferometric measurements are inherently sensitive to all scales, including the largest angular scales, owing to the nature of wide-field measurements. These wide-field effects are generic to all observations but antenna shapes impact their amplitudes substantially. A dish-shaped antenna yields the most desirable features from a foreground contamination viewpoint, relative to a dipole or a phased array. Comparing data from recent Murchison Widefield Array observations, we demonstrate that the foreground signatures that have the largest impact on the H I signal arise from power received far away from the primary field of view. We identify diffuse emission near the horizon as a significant contributing factor, even on wide antenna spacings that usually represent structures on small scales. For signals entering through the primary field of view, compact emission dominates the foreground contamination. These two mechanisms imprint a characteristic pitchfork signature on the “foreground wedge” in Fourier delay space. Based on these results, we propose that selective down-weighting of data based on antenna spacing and time can mitigate foreground contamination substantially by a factor of ∼100 with negligible loss of sensitivity.