The ASKAP Variables and Slow Transients (VAST) Pilot Survey

Publications of the Astronomical Society of Australia Cambridge University Press 38 (2021) e054

Authors:

Tara Murphy, David L Kaplan, Adam J Stewart, Andrew O'Brien, Emil Lenc, Sergio Pintaldi, Joshua Pritchard, Dougal Dobie, Archibald Fox, James K Leung, Tao An, Martin E Bell, Jess W Broderick, Shami Chatterjee, Shi Dai, Daniele d'Antonio, J Gerry Doyle, BM Gaensler, George Heald, Assaf Horesh, Megan L Jones, David McConnell, Vanessa A Moss, Wasim Raja, Gavin Ramsay, Stuart Ryder, Elaine M Sadler, Gregory R Sivakoff, Yuanming Wang, Ziteng Wang, Michael S Wheatland, Matthew Whiting, James R Allison, CS Anderson, Lewis Ball, K Bannister, DC-J Bock, R Bolton, JD Bunton, R Chekkala, AP Chippendale, FR Cooray, N Gupta, DB Hayman, K Jeganathan, B Koribalski, K Lee-Waddell, Elizabeth K Mahony, J Marvil, NM McClure-Griffiths

Abstract:

The Variables and Slow Transients Survey (VAST) on the Australian Square Kilometre Array Pathfinder (ASKAP) is designed to detect highly variable and transient radio sources on timescales from 5 s to ~5 yr. In this paper, we present the survey description, observation strategy and initial results from the VAST Phase I Pilot Survey. This pilot survey consists of ~162 h of observations conducted at a central frequency of 888 MHz between 2019 August and 2020 August, with a typical rms sensitivity of 0.24 mJy beam-1 and angular resolution of 12 – 20 arcseconds. There are 113 fields, each of which was observed for 12 min integration time, with between 5 and 13 repeats, with cadences between 1 day and 8 months. The total area of the pilot survey footprint is 5 131 square degrees, covering six distinct regions of the sky. An initial search of two of these regions, totalling 1 646 square degrees, revealed 28 highly variable and/or transient sources. Seven of these are known pulsars, including the millisecond pulsar J2039–5617. Another seven are stars, four of which have no previously reported radio detection (SCR J0533–4257, LEHPM 2-783, UCAC3 89–412162 and 2MASS J22414436–6119311). Of the remaining 14 sources, two are active galactic nuclei, six are associated with galaxies and the other six have no multi-wavelength counterparts and are yet to be identified.

Radio and X-ray observations of the luminous Fast Blue Optical Transient AT2020xnd

ArXiv 2110.05514 (2021)

Authors:

Joe S Bright, Raffaella Margutti, David Matthews, Daniel Brethauer, Deanne Coppejans, Mark H Wieringa, Brian D Metzger, Lindsay DeMarchi, Tanmoy Laskar, Charles Romero, Kate D Alexander, Assaf Horesh, Giulia Migliori, Ryan Chornock, E Berger, Michael Bietenholz, Mark J Devlin, Simon R Dicker, WV Jacobson-Galán, Brian S Mason, Dan Milisavljevic, Sara E Motta, Tony Mroczkowski, Enrico Ramirez-Ruiz, Lauren Rhodes, Craig L Sarazin, Itai Sfaradi, Jonathan Sievers

The gaseous natal environments of GPS and CSS sources with ASKAP -- FLASH

ArXiv 2110.03046 (2021)

Authors:

James R Allison, Elaine M Sadler, Elizabeth K Mahony, Vanessa A Moss, Hyein Yoon

Abstract:

GPS and CSS sources are thought to represent a young and/or confined sub-population of radio-loud active galactic nuclei (AGN) that are yet to evacuate their surrounding ambient interstellar gas. By studying the gaseous environments of these objects we can gain an insight into the inter-dependent relationship between galaxies and their supermassive black holes (SMBHs). The First Large Absorption Survey in HI (FLASH) will build a census of the neutral atomic hydrogen (HI) gas in galaxies at intermediate cosmological redshifts. FLASH is expected to detect at least several hundred HI absorbers associated with GPS and CSS sources. These absorbers provide an important probe of the abundance and kinematics of line-of-sight neutral gas towards radio AGN, in some cases revealing gas associated with infalling clouds and outflows. Observations are now complete for the first phase of the FLASH Pilot Survey and early analysis has already yielded several detections, including the GPS source PKS2311$-$477. Optical imaging of this galaxy reveals an interacting system that could have supplied the neutral gas seen in absorption and triggered the radio-loud AGN. FLASH will provide a statistically significant sample with which the prevalence of such gas-rich interactions amongst compact radio galaxies can be investigated.

The Thousand-Pulsar-Array programme on MeerKAT - VI. Pulse widths of a large and diverse sample of radio pulsars

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY Oxford University Press (OUP) 508:3 (2021) 4249-4268

Authors:

B Posselt, A Karastergiou, S Johnston, A Parthasarathy, Mj Keith, Ls Oswald, X Song, P Weltevrede, Ed Barr, S Buchner, M Geyer, M Kramer, Dj Reardon, M Serylak, Rm Shannon, R Spiewak, V Venkatraman Krishnan

Abstract:

We present pulse width measurements for a sample of radio pulsars observed with the MeerKAT telescope as part of the Thousand-Pulsar-Array (TPA) programme in the MeerTime project. For a centre frequency of 1284 MHz, we obtain 762 W10 measurements across the total bandwidth of 775 MHz, where W10 is the width at the 10 per cent level of the pulse peak. We also measure about 400 W10 values in each of the four or eight frequency sub-bands. Assuming, the width is a function of the rotation period P, this relationship can be described with a power law with power law index μ = -0.29 ± 0.03. However, using orthogonal distance regression, we determine a steeper power law with μ = -0.63 ± 0.06. A density plot of the period-width data reveals such a fit to align well with the contours of highest density. Building on a previous population synthesis model, we obtain population-based estimates of the obliquity of the magnetic axis with respect to the rotation axis for our pulsars. Investigating the width changes over frequency, we unambiguously identify a group of pulsars that have width broadening at higher frequencies. The measured width changes show a monotonic behaviour with frequency for the whole TPA pulsar population, whether the pulses are becoming narrower or broader with increasing frequency. We exclude a sensitivity bias, scattering and noticeable differences in the pulse component numbers as explanations for these width changes, and attempt an explanation using a qualitative model of five contributing Gaussian pulse components with flux density spectra that depend on their rotational phase.

The Thousand-Pulsar-Array programme on MeerKAT – VI. Pulse widths of a large and diverse sample of radio pulsars

Monthly Notices of the Royal Astronomical Society Oxford University Press 508:3 (2021) 4249-4268

Authors:

B Posselt, A Karastergiou, S Johnston, A Parthasarathy, Mj Keith, Ls Oswald, X Song, P Weltevrede, Ed Barr, S Buchner, M Geyer, M Kramer, Dj Reardon, M Serylak, Rm Shannon, R Spiewak, V Venkatraman Krishnan

Abstract:

We present pulse width measurements for a sample of radio pulsars observed with the MeerKAT telescope as part of the Thousand-Pulsar-Array (TPA) programme in the MeerTime project. For a centre frequency of 1284 MHz, we obtain 762 W10 measurements across the total bandwidth of 775 MHz, where W10 is the width at the 10 per cent level of the pulse peak. We also measure about 400 W10 values in each of the four or eight frequency sub-bands. Assuming, the width is a function of the rotation period P, this relationship can be described with a power law with power law index μ = −0.29 ± 0.03. However, using orthogonal distance regression, we determine a steeper power law with μ = −0.63 ± 0.06. A density plot of the period-width data reveals such a fit to align well with the contours of highest density. Building on a previous population synthesis model, we obtain population-based estimates of the obliquity of the magnetic axis with respect to the rotation axis for our pulsars. Investigating the width changes over frequency, we unambiguously identify a group of pulsars that have width broadening at higher frequencies. The measured width changes show a monotonic behaviour with frequency for the whole TPA pulsar population, whether the pulses are becoming narrower or broader with increasing frequency. We exclude a sensitivity bias, scattering and noticeable differences in the pulse component numbers as explanations for these width changes, and attempt an explanation using a qualitative model of five contributing Gaussian pulse components with flux density spectra that depend on their rotational phase.