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    Building Models for Extended Radio Sources: Implications for Epoch of Reionisation Science

    Access Status
    Fulltext not available
    Authors
    Trott, Cathryn
    Wayth, Randall
    Date
    2017
    Type
    Journal Article
    
    Metadata
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    Citation
    Trott, C. and Wayth, R. 2017. Building Models for Extended Radio Sources: Implications for Epoch of Reionisation Science. Publications of the Astronomical Society of Australia. 34: e061.
    Source Title
    Publications of the Astronomical Society of Australia
    DOI
    10.1017/pasa.2017.57
    ISSN
    1323-3580
    School
    Curtin Institute of Radio Astronomy (Physics)
    Funding and Sponsorship
    http://purl.org/au-research/grants/arc/DE140100316
    URI
    http://hdl.handle.net/20.500.11937/63070
    Collection
    • Curtin Research Publications
    Abstract

    Copyright © Astronomical Society of Australia 2017. We test the hypothesis that limitations in the sky model used to calibrate an interferometric radio telescope, where the model contains extended radio sources, will generate bias in the Epoch of Reionisation power spectrum. The information contained in a calibration model about the spatial and spectral structure of an extended source is incomplete because a radio telescope cannot sample all Fourier components. Application of an incomplete sky model to calibration of Epoch of Reionisation data will imprint residual error in the data, which propagates forward to the Epoch of Reionisation power spectrum. This limited information is studied in the context of current and future planned instruments and surveys at Epoch of Reionisation frequencies, such as the Murchison Widefield Array (MWA), Giant Metrewave Radio Telescope and the Square Kilometre Array (SKA1-Low). For the MWA Epoch of Reionisation experiment, we find that both the additional short baseline uv-coverage of the compact Epoch of Reionisation array, and the additional long baselines provided by TGSS and planned MWA expansions, are required to obtain sufficient information on all relevant scales. For SKA1-Low, arrays with maximum baselines of 49 km and 65 km yield comparable performance at 50 MHz and 150 MHz, while 39 km, 14 km, and 4 km arrays yield degraded performance.

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