A re-establishing jet during an X-ray re-brightening of the Be/X-ray binary Swift J0243.6+6124

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 483:4 (2019) 4628-4638

Authors:

J van den Eijnden, N Degenaar, TD Russell, JV Hernández Santisteban, R Wijnands, JCA Miller-Jones, A Rouco Escorial, GR Sivakoff

A systematic study of the phase difference between QPO harmonics in black hole X-ray binaries

ArXiv 1903.03135 (2019)

Authors:

Iris de Ruiter, Jakob van den Eijnden, Adam Ingram, Phil Uttley

The performance and calibration of the CRAFT fly’s eye fast radio burst survey

Publications of the Astronomical Society of Australia Cambridge University Press 36 (2019) e009

Authors:

CW James, KW Bannister, J-P Macquart, RD Ekers, S Oslowski, RM Shannon, James Allison, AP Chippendale, JD Collier, T Franzen, AW Hotan, M Leach, D McConnell, MA Pilawa, MA Voronkov, MT Whiting

Abstract:

The Commensal Real-time Australian Square Kilometre Array Pathfinder Fast Transients survey is the first extensive astronomical survey using phased array feeds. Since January 2017, it has been searching for fast radio bursts in fly’s eye mode. Here, we present a calculation of the sensitivity and total exposure of the survey that detected the first 20 of these bursts, using the pulsars B1641-45 and B0833-45 as calibrators. The beamshape, antenna-dependent system noise, and the effects of radio-frequency interference and fluctuations during commissioning are quantified. Effective survey exposures and sensitivities are calculated as a function of the source counts distribution. Statistical ‘stat’ and systematics ‘sys’ effects are treated separately. The implied fast radio burst rate is significantly lower than the 37 sky−1 day−1 calculated using nominal exposures and sensitivities for this same sample by Shannon et al. (2018). At the Euclidean (best-fit) power-law index of −1.5 (−2.2), the rate is (sys) ± 3.6 (stat) sky−1 day−1 ( (sys) ± 2.8 (stat) sky−1 day−1) above a threshold of 56.6 ± 6.6(sys) Jy ms (40.4 ± 1.2(sys) Jy ms). This strongly suggests that these calculations be performed for other FRB-hunting experiments, allowing meaningful comparisons to be made between them.

The First Tidal Disruption Flare in ZTF: From Photometric Selection to Multi-wavelength Characterization

The Astrophysical Journal American Astronomical Society 872:2 (2019) 198

Authors:

Sjoert van Velzen, Suvi Gezari, S Bradley Cenko, Erin Kara, James CA Miller-Jones, Tiara Hung, Joe Bright, Nathaniel Roth, Nadejda Blagorodnova, Daniela Huppenkothen, Lin Yan, Eran Ofek, Jesper Sollerman, Sara Frederick, Charlotte Ward, Matthew J Graham, Rob Fender, Mansi M Kasliwal, Chris Canella, Robert Stein, Matteo Giomi, Valery Brinnel, Jakob van Santen, Jakob Nordin, Eric C Bellm, Richard Dekany, Christoffer Fremling, V Zach Golkhou, Thomas Kupfer, Shrinivas R Kulkarni, Russ R Laher, Ashish Mahabal, Frank J Masci, Adam A Miller, James D Neill, Reed Riddle, Mickael Rigault, Ben Rusholme, Maayane T Soumagnac, Yutaro Tachibana

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.