Mining the Herschel-astrophysical terahertz large area survey: Submillimetre-selected blazars in equatorial fields

Monthly Notices of the Royal Astronomical Society 430:3 (2013) 1566-1577

Authors:

M López-Caniego, J González-Nuevo, M Massardi, L Bonavera, D Herranz, M Negrello, G De Zotti, FJ Carrera, L Danese, S Fleuren, M Hardcastle, MJ Jarvis, HR Klöckner, T Mauch, P Procopio, S Righini, W Sutherland, R Auld, M Baes, S Buttiglione, CJR Clark, A Cooray, A Dariush, L Dunne, S Dye, S Eales, R Hopwood, C Hoyos, E Ibar, RJ Ivison, S Maddox, E Valiante

Abstract:

The Herschel-Astrophysical Terahertz Large Area Survey (H-ATLAS) provides an unprecedented opportunity to search for blazars at sub-mm wavelengths. We cross-matched the Faint Images of the Radio Sky at Twenty-cm (FIRST) radio source catalogue with the 11 655 sources brighter than 35 mJy at 500 μm in the ∼135 deg2 of the sky covered by the H-ATLAS equatorial fields at 9h and 15h, plus half of the field at 12h. We found that 379 of the H-ATLAS sources have a FIRST counterpart within 10 arcsec, including eight catalogued blazars (plus one known blazar that was found at the edge of one of the H-ATLAS maps). To search for additional blazar candidates we have devised new diagnostic diagrams and found that known blazars occupy a region of the log(S500μm/S350μm) versus log(S500μm/S1.4 GHz) plane separated from that of sub-mm sources with radio emission powered by star formation, but shared with radio galaxies and steep-spectrum radio quasars. Using this diagnostic we have selected 12 further possible candidates that turn out to be scattered in the (r-z) versus (u-r) plane or in the Wide-Field Infrared Survey Explorer colour-colour diagram, where known blazars are concentrated in well defined strips. This suggests that the majority of them are not blazars. Based on an inspection of all the available photometric data, including unpublished VISTA Kilo-degree Infrared Galaxy survey photometry and new radio observations, we found that the spectral energy distributions (SEDs) of only one out of the 12 newly selected sources are compatible with being synchrotron dominated at least up to 500 μm, i.e. with being a blazar. Another object may consist of a faint blazar nucleus inside a bright star-forming galaxy. The possibility that some blazar hosts are endowed with active star formation is supported by our analysis of the SEDs of Planck Early Release Compact Source Catalogue blazars detected at both 545 and 857 GHz. The estimated rest-frame synchrotron peak frequencies of H-ATLAS blazars are in the range 11.5 ≤ log (νpeak, Hz) ≤ 13.7, implying that these objects are low synchrotron peak. Six of them also show evidence of an ultraviolet excess that can be attributed to emission from the accretion disc. Allowing for the possibility of misidentifications and of contamination of the 500 μm flux density by the dusty torus or by the host galaxy, we estimate that there are seven or eight pure synchrotron sources brighter than S500μm = 35 mJy over the studied area, a result that sets important constraints on blazar evolutionary models. © 2013 The Author. Published by Oxford University Press on behalf of the Royal Astronomical Society.

The closest black holes

Monthly Notices of the Royal Astronomical Society 430:3 (2013) 1538-1547

Authors:

RP Fender, TJ Maccarone, I Heywood

Abstract:

Starting from the assumption that there is a large population (≥108) of stellar-mass isolated black holes (IBH) distributed throughout our Galaxy, we consider the detectable signatures of accretion from the interstellar medium (ISM) that may be associated with such a population. We simulate the nearby (radius 250 pc) part of this population, corresponding to the closest ~35 000 black holes, using current best estimates of the mass distribution of stellar-mass black holes combined with two models for the velocity distribution of stellar-mass IBH which bracket likely possibilities. We distribute this population of objects appropriately within the different phases of the ISM and calculate the Bondi-Hoyle accretion rate, modified by a further dimensionless efficiency parameter λ. Assuming a simple prescription for radiatively inefficient accretion at low Eddington ratios, we calculate the X-ray luminosity of these objects, and similarly estimate the radio luminosity from relations found empirically for black holes accreting at low rates. The latter assumption depends crucially on whether or not the IBH accrete from the ISM in a manner which is axisymmetric enough to produce jets. Comparing the predicted X-ray fluxes with limits from hard X-ray surveys, we conclude that either the Bondi-Hoyle efficiency parameter λ is rather small (=0.01), the velocities of the IBH are rather high, or some combination of both. The predicted radio flux densities correspond to a population of objects which, while below current survey limits, should be detectable with the Square Kilometre Array (SKA). Converting the simulated space velocities into proper motions, we further demonstrate that such IBH could be identified as faint high proper motion radio sources in SKA surveys. © 2013 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society.

The radio source count at 93.2 GHz from observations of 9C sources using AMI and CARMA

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 430:3 (2013) 1961-1969

Authors:

Matthew L Davies, Irina I Stefan, Rosie C Bolton, John M Carpenter, Thomas MO Franzen, Keith JB Grainge, David A Green, Michael P Hobson, Natasha Hurley-Walker, Anthony N Lasenby, Malak Olamaie, Yvette C Perrott, Guy G Pooley, Julia M Riley, Carmen Rodríguez-Gonzálvez, Richard DE Saunders, Anna MM Scaife, Michel P Schammel, Paul F Scott, Timothy W Shimwell, David J Titterington, Elizabeth M Waldram, Imogen H Whittam

The Q/U imaging experiment instrument

Astrophysical Journal American Astronomical Society 768:1 (2013) 1-28

Authors:

C Bischoff, A Brizius, I Buder, Y Chinone, K Cleary, RN Dumoulin, A Kusaka, R Monsalve, SK Naess, LB Newburgh, G Nixon, R Reeves, KM Smith, K Vanderlinde, IK Wehus, M Bogdan, R Bustos, Church, R Davis, C Dickinson, HK Eriksen, T Gaier, JO Gundersen, M Hasegawa, M Hazumi, C Holler, KM Huffenberger, WA Imbriale, K Ishidoshiro, Michael Jones, P Kangaslahti, DJ Kapner, CR Lawrence, EM Leitch, M Limon, JJ McMahon, AD Miller, M Nagai, H Nguyen, TJ Pearson, L Piccirillo, SJE Radford, ACS Readhead, JL Richards, D Samtleben, M Seiffert, MC Shepherd, ST Staggs, O Tajima

Abstract:

The Q/U Imaging ExperimenT (QUIET) is designed to measure polarization in the cosmic microwave background, targeting the imprint of inflationary gravitational waves at large angular scales(~1°). Between 2008 October and 2010 December, two independent receiver arrays were deployed sequentially on a 1.4 m side-fed Dragonian telescope. The polarimeters that form the focal planes use a compact design based on high electron mobility transistors (HEMTs) that provides simultaneous measurements of the Stokes parameters Q, U, and I in a single module. The 17-element Q-band polarimeter array, with a central frequency of 43.1 GHz, has the best sensitivity (69 μKs1/2) and the lowest instrumental systematic errors ever achieved in this band, contributing to the tensor-to-scalar ratio at r < 0.1. The 84-element W-band polarimeter array has a sensitivity of 87 μKs1/2 at a central frequency of 94.5 GHz. It has the lowest systematic errors to date, contributing at r < 0.01. The two arrays together cover multipoles in the range ℓ ~ 25-975. These are the largest HEMT-based arrays deployed to date. This article describes the design, calibration, performance, and sources of systematic error of the instrument.

Differential frequency-dependent delay from the pulsar magnetosphere

Astronomy and Astrophysics 552 (2013)

Authors:

TE Hassall, BW Stappers, P Weltevrede, JWT Hessels, A Alexov, T Coenen, A Karastergiou, M Kramer, EF Keane, VI Kondratiev, J Van Leeuwen, A Noutsos, M Pilia, M Serylak, C Sobey, K Zagkouris, R Fender, ME Bell, J Broderick, J Eislöffel, H Falcke, JM Grießmeier, M Kuniyoshi, JCA Miller-Jones, MW Wise, O Wucknitz, P Zarka, A Asgekar, F Batejat, MJ Bentum, G Bernardi, P Best, A Bonafede, F Breitling, M Brüggen, HR Butcher, B Ciardi, F De Gasperin, JP De Reijer, S Duscha, RA Fallows, C Ferrari, W Frieswijk, MA Garrett, AW Gunst, G Heald, M Hoeft, E Juette, P Maat, JP McKean, MJ Norden, M Pandey-Pommier, R Pizzo, AG Polatidis, W Reich, H Röttgering, J Sluman, Y Tang, C Tasse, R Vermeulen, RJ Van Weeren, SJ Wijnholds, S Yatawatta

Abstract:

Some radio pulsars show clear "drifting subpulses", in which subpulses are seen to drift in pulse longitude in a systematic pattern. Here we examine how the drifting subpulses of PSR B0809+74 evolve with time and observing frequency. We show that the subpulse period (P3) is constant on timescales of days, months and years, and between 14-5100 MHz. Despite this, the shapes of the driftbands change radically with frequency. Previous studies have concluded that, while the subpulses appear to move through the pulse window approximately linearly at low frequencies (<500 MHz), a discrete step of ~180 in subpulse phase is observed at higher frequencies (>820 MHz) near to the peak of the average pulse profile. We use LOFAR, GMRT, GBT, WSRT and Effelsberg 100-m data to explore the frequency-dependence of this phase step. We show that the size of the subpulse phase step increases gradually, and is observable even at low frequencies. We attribute the subpulse phase step to the presence of two separate driftbands, whose relative arrival times vary with frequency - one driftband arriving 30 pulses earlier at 20 MHz than it does at 1380 MHz, whilst the other arrives simultaneously at all frequencies. The drifting pattern which is observed here cannot be explained by either the rotating carousel model or the surface oscillation model, and could provide new insight into the physical processes happening within the pulsar magnetosphere. © ESO, 2013.