Field sources near the southern-sky calibrator PKS B1934-638: effect on spectral line observations with SKA-MID and its precursors

Author:

Heywood I123ORCID,Lenc E4ORCID,Serra P5,Hugo B23,Bannister K W4,Bell M E6,Chippendale A4ORCID,Harvey-Smith L78ORCID,Marvil J9,McConnell D4,Voronkov M A4

Affiliation:

1. Astrophysics, Department of Physics, University of Oxford, Keble Road, Oxford OX1 3RH, UK

2. Department of Physics and Electronics, Rhodes University, PO Box 94, Makhanda 6140, South Africa

3. South African Radio Astronomy Observatory, 2 Fir Street, Black River Park, Observatory, Cape Town 7925, South Africa

4. CSIRO Astronomy and Space Science, PO Box 76, Epping, NSW 1710, Australia

5. INAF - Osservatorio Astronomico di Cagliari, Via della Scienza 5, I-09047 Selargius (CA), Italy

6. School of Mathematical and Physical Sciences, University of Technology Sydney, 15 Broadway, Ultimo, NSW 2007, Australia

7. School of Physics, University of New South Wales, Sydney, NSW 2052, Australia

8. Western Sydney University, Locked Bag 1797, Penrith, NSW 2751, Australia

9. National Radio Astronomy Observatory, PO Box 0, Soccoro, NM 87801, USA

Abstract

ABSTRACT Accurate instrumental bandpass corrections are essential for the reliable interpretation of spectral lines from targeted and survey-mode observations with radio interferometers. Bandpass correction is typically performed by comparing measurements of a strong calibrator source to an assumed model, typically an isolated point source. The wide field-of-view and high sensitivity of modern interferometers means that additional sources are often detected in observations of calibrators. This can introduce errors into bandpass corrections and subsequently the target data if not properly accounted for. Focusing on the standard calibrator PKS B1934-638, we perform simulations to asses this effect by constructing a wide-field sky model. The cases of ASKAP (0.7–1.9 GHz), MeerKAT (UHF: 0.58–1.05 GHz; L-band: 0.87–1.67 GHz) and Band 2 (0.95–1.76 GHz) of SKA-MID are examined. The use of a central point source model during bandpass calibration is found to impart amplitude errors into spectra measured by the precursor instruments at the ∼0.2–0.5 per cent level dropping to ∼0.01 per cent in the case of SKA-MID. This manifests itself as ripples in the source spectrum, the behaviour of which is coupled to the distribution of the array baselines, the solution interval, the primary beam size, the hour-angle of the calibration scan, as well as the weights used when imaging the target. Calibration pipelines should routinely employ complete field models for standard calibrators to remove this potentially destructive contaminant from the data, a recommendation we validate by comparing our simulation results to a MeerKAT scan of PKS B1934-638, calibrated with and without our expanded sky model.

Funder

European Research Council

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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