Measuring the expansion velocity of the outflows of LS I +61 303 through low-frequency radio observations

AIP Conference Proceedings AIP Publishing 1792:1 (2017) 040018

Authors:

B Marcote, M Ribó, JM Paredes, CH Ishwara-Chandra, JD Swinbank, JW Broderick, S Markoff, R Fender, RAMJ Wijers, GG Pooley, AJ Stewart, ME Bell, RP Breton, D Carbone, S Corbel, J Eislöffel, H Falcke, J-M Grießmeier, M Kuniyoshi, M Pietka, A Rowlinson, M Serylak, AJ van der Horst, J van Leeuwen, MW Wise, P Zarka

Redshift measurement of Fermi blazars for the Cherenkov telescope array

AIP Conference Proceedings AIP Publishing 1792:1 (2017) 050025

Authors:

Santiago Pita, Paolo Goldoni, Catherine Boisson, Garret Cotter, Julien Lefaucheur, Jean-Philippe Lenain, Elina Lindfors, David A Williams

Inauguration and first light of the GCT-M prototype for the Cherenkov Telescope Array

6th International Symposium on High-Energy Gamma-Ray Astronomy (Gamma2016), Institute of Physics (2017)

Authors:

Jason J Watson, Andrea De Franco, A Abchiche, D Allan, J-P Amans, TP Armstrong, A Balzer, D Berge, C Boisson, J-J Bousquet, AM Brown, M Bryan, G Buchholtz, PM Chadwick, H Costantini, Garret Cotter, MK Daniel, F De Frondat, J-L Dournaux, D Dumas, J-P Ernenwein, G Fasola, S Funk, J Gironnet, JA Graham, T Greenshaw, O Hervet, N Hidaka, JA Hinton, J-M Huet, I Jegouzo, T Jogler, M Kraus, JS Lapington, P Laporte, J Lefaucheur, S Markoff, T Melse, L Mohrmann, P Molyneux, SJ Nolan, A Okumura, JP Osborne, RD Parsons, S Rosen, D Ross, G Rowell, CB Rulten, Y Sato, F Sayede

Abstract:

The Gamma-ray Cherenkov Telescope (GCT) is a candidate for the Small Size Telescopes (SSTs) of the Cherenkov Telescope Array (CTA). Its purpose is to extend the sensitivity of CTA to gamma-ray energies reaching 300 TeV. Its dual-mirror optical design and curved focal plane enables the use of a compact camera of 0.4 m diameter, while achieving a field of view of above 8 degrees. Through the use of the digitising TARGET ASICs, the Cherenkov flash is sampled once per nanosecond contin-uously and then digitised when triggering conditions are met within the analogue outputs of the photosensors. Entire waveforms (typically covering 96 ns) for all 2048 pixels are then stored for analysis, allowing for a broad spectrum of investigations to be performed on the data. Two prototypes of the GCT camera are under development, with differing photosensors: Multi-Anode Photomultipliers (MAPMs) and Silicon Photomultipliers (SiPMs). During November 2015, the GCT MAPM (GCT-M) prototype camera was integrated onto the GCT structure at the Observatoire de Paris-Meudon, where it observed the first Cherenkov light detected by a prototype instrument for CTA.

Rapid radio flaring during an anomalous outburst of SS Cyg

Monthly Notices of the Royal Astronomical Society: Letters Oxford University Press 467:1 (2017) L31-L35

Authors:

Kunal P Mooley, James CA Miller-Jones, Robert Fender, Gregory R Sivakoff, Clare Rumsey, Yvette Perrott, David Titterington, Keith Grainge, Thomas D Russell, Steven H Carey, Jack Hickish, Nima Razavi-Ghods, Anna Scaife, Paul Scott, Elisabeth O Waagen

Abstract:

The connection between accretion and jet production in accreting white dwarf binary systems, especially dwarf novae, is not well understood. Radio wavelengths provide key insights into the mechanisms responsible for accelerating electrons, including jets and outflows. Here we present densely-sampled radio coverage, obtained with the Arcminute MicroKelvin Imager Large Array, of the dwarf nova SS Cyg during its February 2016 anomalous outburst. The outburst displayed a slower rise (3 days mag^-1) in the optical than typical ones, and lasted for more than 3 weeks. Rapid radio flaring on timescales <1 hour was seen throughout the outburst. The most intriguing behavior in the radio was towards the end of the outburst where a fast, luminous (“giant”), flare peaking at ~20 mJy and lasting for 15 minutes was observed. This is the first time that such a flare has been observed in SS Cyg, and insufficient coverage could explain its non-detection in previous outbursts. These data, together with past radio observations, are consistent with synchrotron emission from plasma ejection events as being the origin of the radio flares. However, the production of the giant flare during the declining accretion rate phase remains unexplained within the standard accretion-jet framework and appears to be markedly different to similar patterns of behavior in X-ray binaries.

The LOFAR Two-metre Sky Survey. I. Survey description and preliminary data release

Astronomy & Astrophysics EDP Sciences 598 (2017) A104

Authors:

TW Shimwell, HJA Röttgering, PN Best, Matthew J Jarvis, Et Et al.

Abstract:

The LOFAR Two-metre Sky Survey (LoTSS) is a deep 120–168 MHz imaging survey that will eventually cover the entire northern sky. Each of the 3170 pointings will be observed for 8 h, which, at most declinations, is sufficient to produce ~5″ resolution images with a sensitivity of ~100 μJy/beam and accomplish the main scientific aims of the survey, which are to explore the formation and evolution of massive black holes, galaxies, clusters of galaxies and large-scale structure. Owing to the compact core and long baselines of LOFAR, the images provide excellent sensitivity to both highly extended and compact emission. For legacy value, the data are archived at high spectral and time resolution to facilitate subarcsecond imaging and spectral line studies. In this paper we provide an overview of the LoTSS. We outline the survey strategy, the observational status, the current calibration techniques, a preliminary data release, and the anticipated scientific impact. The preliminary images that we have released were created using a fully automated but direction-independent calibration strategy and are significantly more sensitive than those produced by any existing large-area low-frequency survey. In excess of 44 000 sources are detected in the images that have a resolution of 25″, typical noise levels of less than 0.5 mJy/beam, and cover an area of over 350 square degrees in the region of the HETDEX Spring Field (right ascension 10h45m00s to 15h30m00s and declination 45°00′00″ to 57°00′00″).