A simple disc wind model for broad absorption line quasars

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 436:2 (2013) 1390-1407

Authors:

N Higginbottom, C Knigge, KS Long, SA Sim, JH Matthews

Detecting cosmic rays with the LOFAR radio telescope

Astronomy and Astrophysics 560 (2013)

Authors:

P Schellart, A Nelles, S Buitink, A Corstanje, JE Enriquez, H Falcke, W Frieswijk, JR Horandel, A Horneffer, CW James, M Krause, M Mevius, O Scholten, S Ter Veen, S Thoudam, M Van Den Akker, A Alexov, J Anderson, IM Avruch, L Bahren, R Beck, ME Bell, P Bennema, MJ Bentum, G Bernardi, P Best, J Bregman, F Breitling, M Brentjens, J Broderick, M Bruggen, B Ciardi, A Coolen, F De Gasperin, E De Geus, A De Jong, M De Vos, S Duscha, J Eisloffel, RA Fallows, C Ferrari, MA Garrett, J Grießmeier, T Grit, JP Hamaker, TE Hassall, G Heald, JWT Hessels, M Hoeft, HA Holties, M Iacobelli, E Juette, A Karastergiou, W Klijn, J Kohler, VI Kondratiev, M Kramer, M Kuniyoshi, G Kuper, P Maat, G Macario, G Mann, S Markoff, D McKay-Bukowski, JP McKean, JCA Miller-Jones, JD Mol, DD Mulcahy, H Munk, R Nijboer, MJ Norden, E Orru, R Overeem, H Paas, M Pandey-Pommier, R Pizzo, AG Polatidis, A Renting, JW Romein, H Rottgering, A Schoenmakers, D Schwarz, J Sluman, O Smirnov, C Sobey, BW Stappers, M Steinmetz, J Swinbank, Y Tang, C Tasse, C Toribio, J Van Leeuwen, R Van Nieuwpoort, RJ Van Weeren, N Vermaas, R Vermeulen, C Vocks, C Vogt, RAMJ Wijers, SJ Wijnholds

Abstract:

The low frequency array (LOFAR), is the first radio telescope designed with the capability to measure radio emission from cosmic-ray induced air showers in parallel with interferometric observations. In the first ~2 years of observing, 405 cosmic-ray events in the energy range of 1016-1018 eV have been detected in the band from 30-80 MHz. Each of these air showers is registered with up to ~1000 independent antennas resulting in measurements of the radio emission with unprecedented detail. This article describes the dataset, as well as the analysis pipeline, and serves as a reference for future papers based on these data. All steps necessary to achieve a full reconstruction of the electric field at every antenna position are explained, including removal of radio frequency interference, correcting for the antenna response and identification of the pulsed signal. © ESO, 2013.

Radio Detections During Two State Transitions of the Intermediate Mass Black Hole HLX-1

(2013)

Authors:

Natalie Webb, David Cseh, Emil Lenc, Olivier Godet, Didier Barret, Stephane Corbel, Sean Farrell, Rob Fender, Neil Gehrels, Ian Heywood

New constraints on the cooling of the Central Compact Object in Cas A

(2013)

Authors:

B Posselt, GG Pavlov, V Suleimanov, O Kargaltsev

H-ATLAS: Estimating redshifts of herschel sources from sub-mm fluxes

Monthly Notices of the Royal Astronomical Society 435:4 (2013) 2753-2763

Authors:

EA Pearson, S Eales, L Dunne, J Gonzalez-Nuevo, S Maddox, JE Aguirre, M Baes, AJ Baker, N Bourne, CM Bradford, CJR Clark, A Cooray, A Dariush, G De Zotti, S Dye, D Frayer, HL Gomez, AI Harris, R Hopwood, E Ibar, RJ Ivison, M Jarvis, M Krips, A Lapi, RE Lupu, MJ Michałowski, M Rosenman, D Scott, E Valiante, I Valtchanov, P van der Werf, JD Vieira

Abstract:

Upon its completion, the Herschel Astrophysics Terahertz Large Area Survey (H-ATLAS) will be the largest sub-millimetre survey to date, detecting close to half-a-million sources. It will only be possible to measure spectroscopic redshifts for a small fraction of these sources. However, if the rest-frame spectral energy distribution (SED) of a typical H-ATLAS source is known, this SED and the observed Herschel fluxes can be used to estimate the redshifts of the H-ATLAS sources without spectroscopic redshifts. In this paper, we use a sub-set of 40 H-ATLAS sources with previously measured redshifts in the range 0.5 < z < 4.2 to derive a suitable average template for high-redshift H-ATLAS sources. We find that a template with two dust components (Tc= 23.9K, Th= 46.9K and ratio of mass of cold dust to mass of warm dust of 30.1) provides a good fit to the rest-frame fluxes of the sources in our calibration sample. We use a jackknife technique to estimate the accuracy of the redshifts estimated with this template, finding a root mean square of Δz/(1 + z) = 0.26. For sources for which there is prior information that they lie at z > 1, we estimate that the rms of Δz/(1 + z) = 0.12. We have used this template to estimate the redshift distribution for the sources detected in the H-ATLAS equatorial fields, finding a bimodal distribution with a mean redshift of 1.2, 1.9 and 2.5 for 250, 350 and 500 μm selected sources, respectively. © 2013 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society.