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Black Hole

Lensing of space time around a black hole. At Oxford we study black holes observationally and theoretically on all size and time scales - it is some of our core work.

Credit: ALAIN RIAZUELO, IAP/UPMC/CNRS. CLICK HERE TO VIEW MORE IMAGES.

Ian Heywood

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Research theme

  • Astronomy and astrophysics

Sub department

  • Astrophysics

Research groups

  • Galaxy formation and evolution
  • MeerKAT
  • Pulsars, transients and relativistic astrophysics
  • The Square Kilometre Array (SKA)
  • Breakthrough Listen
ian.heywood@physics.ox.ac.uk
  • About
  • Publications

LOFAR observations of the XMM-LSS field

Astronomy and Astrophysics EDP Sciences 622 (2019) A4

Authors:

Catherine L Hale, W Williams, Matthew Jarvis, MJ Hardcastle, Leah K Morabito, TW Shimwell, C Tasse, PN Best, JJ Harwood, Ian Heywood, I Prandoni, HJA Röttgering, J Sabater, DJB Smith, RJV Weeren

Abstract:

We present observations of the XMM Large-Scale Structure (XMM-LSS) field observed with the LOw Frequency ARray (LOFAR) at 120–168 MHz. Centred at a J2000 declination of −4.5°, this is a challenging field to observe with LOFAR because of its low elevation with respect to the array. The low elevation of this field reduces the effective collecting area of the telescope, thereby reducing sensitivity. This low elevation also causes the primary beam to be elongated in the north-south direction, which can introduce side lobes in the synthesised beam in this direction. However the XMM-LSS field is a key field to study because of the wealth of ancillary information, encompassing most of the electromagnetic spectrum. The field was observed for a total of 12 h from three four-hour LOFAR tracks using the Dutch array. The final image presented encompasses ∼27 deg2, which is the region of the observations with a >50% primary beam response. Once combined, the observations reach a central rms of 280 μJy beam−1 at 144 MHz and have an angular resolution of 7.5 × 8.5″. We present our catalogue of detected sources and investigate how our observations compare to previous radio observations. This includes investigating the flux scale calibration of these observations compared to previous measurements, the implied spectral indices of the sources, the observed source counts and corrections to obtain the true source counts, and finally the clustering of the observed radio sources.
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Towards the first detection of strongly lensed H i emission

Monthly Notices of the Royal Astronomical Society Oxford University Press 484:3 (2019) 3681-3690

Authors:

T Blecher, R Deane, Ian Heywood, D Obreschkow
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Molecular gas in two companion cluster galaxies at z = 1.2 (vol 617, A103, 2018)

ASTRONOMY & ASTROPHYSICS 620 (2018) ARTN C4

Authors:

G Castignani, F Combes, P Salome, S Andreon, M Pannella, I Heywood, G Trinchieri, C Cicone, LJM Davies, FN Owen, A Raichoor
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A Strong Jet Signature in the Late-time Light Curve of GW170817

ASTROPHYSICAL JOURNAL LETTERS 868:1 (2018) ARTN L11

Authors:

KP Mooley, DA Frail, D Dobie, E Lenc, A Corsi, K De, AJ Nayana, S Makhathini, I Heywood, T Murphy, DL Kaplan, P Chandra, O Smirnov, E Nakar, G Hallinan, F Camilo, R Fender, S Goedhart, P Groot, MM Kasliwal, SR Kulkarni, PA Woudt
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The relation between galaxy density and radio jet power for 1.4 GHz VLA selected AGNs in Stripe 82

Monthly Notices of the Royal Astronomical Society Oxford University Press 482:4 (2018) 5156-5166

Authors:

S Kolwa, Matthew J Jarvis, K McAlpine, Ian Heywood

Abstract:

Using a Karl G. Jansky Very Large Array (VLA) L-band (1-2 GHz) survey covering∼100 deg^2 of the Stripe 82 field, we have obtained a catalogue of 2716 radio AGNs. For these AGNs, we investigate the impact of galaxy density on 1.4 GHz radio luminosity (L1.4).We determine their close environment densities using the surface density parameter, ΣN, for N = 2 and N = 5, which we bin by redshift to obtain a pseudo-3D galaxy density measure. Matching the radio AGNs to sources without radio detections in terms of redshift, K-band magnitude and (g−K) colour index, we obtain samples of control galaxies and determine whether radio AGN environments differ from this general population. Our results indicate that the environmental density of radio AGNs and their radio luminosity are not correlated up to z ∼ 0.8, over the luminosity range 10^23 < (L1.4/W Hz−1) < 10^26.We also find that, when using a control sample matched in terms of redshift, K-band magnitude and colour, environments of radio AGNs are similar to those of the control sample but with an excess of overdense regions in which radio AGNs aremore prevalent. Our results suggest that the <1Mpc-scale galaxy environment plays some role in determining whether a galaxy produces a radio AGN. The jet power, however, does not correlate with environment. From this, we infer that secular processes, e.g. accretion flows of cold gas to the central black hole are more critical in fuelling radio AGN activity than radio jet power.
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