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    Strategies for Finding Prompt Radio Counterparts to Gravitational Wave Transients with the Murchison Widefield Array

    Access Status
    Fulltext not available
    Authors
    Kaplan, D.
    Murphy, T.
    Rowlinson, A.
    Croft, S.
    Wayth, Randall
    Trott, C.
    Date
    2016
    Type
    Journal Article
    
    Metadata
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    Citation
    Kaplan, D. and Murphy, T. and Rowlinson, A. and Croft, S. and Wayth, R. and Trott, C. 2016. Strategies for Finding Prompt Radio Counterparts to Gravitational Wave Transients with the Murchison Widefield Array. Publications of the Astronomical Society of Australia. 33: e050.
    Source Title
    Publications of the Astronomical Society of Australia
    DOI
    10.1017/pasa.2016.43
    ISSN
    1323-3580
    School
    Department of Electrical and Computer Engineering
    Funding and Sponsorship
    http://purl.org/au-research/grants/arc/DE140100316
    URI
    http://hdl.handle.net/20.500.11937/27827
    Collection
    • Curtin Research Publications
    Abstract

    We present and evaluate several strategies to search for prompt, low-frequency radio emission associated with gravitational wave transients using the Murchison Widefield Array. As we are able to repoint the Murchison Widefield Array on timescales of tens of seconds, we can search for the dispersed radio signal that has been predicted to originate along with or shortly after a neutron star-neutron star merger. We find that given the large, 600 deg2 instantaneous field of view of the Murchison Widefield Array, we can cover a significant fraction of the predicted gravitational wave error region, although due to the complicated geometry of the latter, we only cover > 50% of the error region for approximately 5% of events, and roughly 15% of events will be located < 10° from the Murchison Widefield Array pointing centre such that they will be covered in the radio images. For optimal conditions, our limiting flux density for a 10-s long transient would be 0.1 Jy, increasing to about 1 Jy for a wider range of events. This corresponds to luminosity limits of 1038-39 erg s-1 based on expectations for the distances of the gravitational wave transients, which should be sufficient to detect or significantly constrain a range of models for prompt emission.

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