Synchronous x-ray and radio mode switches: a rapid global transformation of the pulsar magnetosphere.

Science 339:6118 (2013) 436-439

Authors:

W Hermsen, JWT Hessels, L Kuiper, J van Leeuwen, D Mitra, J de Plaa, JM Rankin, BW Stappers, GAE Wright, R Basu, A Alexov, T Coenen, J-M Grießmeier, TE Hassall, A Karastergiou, E Keane, VI Kondratiev, M Kramer, M Kuniyoshi, A Noutsos, M Serylak, M Pilia, C Sobey, P Weltevrede, K Zagkouris, A Asgekar, IM Avruch, F Batejat, ME Bell, MR Bell, MJ Bentum, G Bernardi, P Best, L Bîrzan, A Bonafede, F Breitling, J Broderick, M Brüggen, HR Butcher, B Ciardi, S Duscha, J Eislöffel, H Falcke, R Fender, C Ferrari, W Frieswijk, MA Garrett, F de Gasperin, E de Geus, AW Gunst, G Heald, M Hoeft, A Horneffer, M Iacobelli, G Kuper, P Maat, G Macario, S Markoff, JP McKean, M Mevius, JCA Miller-Jones, R Morganti, H Munk, E Orrú, H Paas, M Pandey-Pommier, VN Pandey, R Pizzo, AG Polatidis, S Rawlings, W Reich, H Röttgering, AMM Scaife, A Schoenmakers, A Shulevski, J Sluman, M Steinmetz, M Tagger, Y Tang, C Tasse, S ter Veen, R Vermeulen, RH van de Brink, RJ van Weeren, RAMJ Wijers, MW Wise, O Wucknitz, S Yatawatta, P Zarka

Abstract:

Pulsars emit from low-frequency radio waves up to high-energy gamma-rays, generated anywhere from the stellar surface out to the edge of the magnetosphere. Detecting correlated mode changes across the electromagnetic spectrum is therefore key to understanding the physical relationship among the emission sites. Through simultaneous observations, we detected synchronous switching in the radio and x-ray emission properties of PSR B0943+10. When the pulsar is in a sustained radio-"bright" mode, the x-rays show only an unpulsed, nonthermal component. Conversely, when the pulsar is in a radio-"quiet" mode, the x-ray luminosity more than doubles and a 100% pulsed thermal component is observed along with the nonthermal component. This indicates rapid, global changes to the conditions in the magnetosphere, which challenge all proposed pulsar emission theories.

Bright radio emission from an ultraluminous stellar-mass microquasar in M 31

Nature 493:7431 (2013) 187-190

Authors:

MJ Middleton, JCA Miller-Jones, S Markoff, R Fender, M Henze, N Hurley-Walker, AMM Scaife, TP Roberts, D Walton, J Carpenter, JP MacQuart, GC Bower, M Gurwell, W Pietsch, F Haberl, J Harris, M Daniel, J Miah, C Done, JS Morgan, H Dickinson, P Charles, V Burwitz, MD Valle, M Freyberg, J Greiner, M Hernanz, DH Hartmann, D Hatzidimitriou, A Riffeser, G Sala, S Seitz, P Reig, A Rau, M Orio, D Titterington, K Grainge

Abstract:

A subset of ultraluminous X-ray sources (those with luminosities of less than 10 40 erg s -1; ref. 1) are thought to be powered by the accretion of gas onto black holes with masses of ∼5-20, probably by means of an accretion disk. The X-ray and radio emission are coupled in such Galactic sources; the radio emission originates in a relativistic jet thought to be launched from the innermost regions near the black hole, with the most powerful emission occurring when the rate of infalling matter approaches a theoretical maximum (the Eddington limit). Only four such maximal sources are known in the Milky Way, and the absorption of soft X-rays in the interstellar medium hinders the determination of the causal sequence of events that leads to the ejection of the jet. Here we report radio and X-ray observations of a bright new X-ray source in the nearby galaxy M 31, whose peak luminosity exceeded 10 39 erg s -1. The radio luminosity is extremely high and shows variability on a timescale of tens of minutes, arguing that the source is highly compact and powered by accretion close to the Eddington limit onto a black hole of stellar mass. Continued radio and X-ray monitoring of such sources should reveal the causal relationship between the accretion flow and the powerful jet emission. © 2013 Macmillan Publishers Limited. All rights reserved.

Initial deep LOFAR observations of Epoch of Reionization windows: I. The North Celestial Pole

ArXiv 1301.163 (2013)

Authors:

S Yatawatta, AG de Bruyn, MA Brentjens, P Labropoulos, VN Pandey, S Kazemi, S Zaroubi, LVE Koopmans, AR Offringa, V Jelic, O Martinez Rubi, V Veligatla, SJ Wijnholds, WN Brouw, G Bernardi, B Ciardi, S Daiboo, G Harker, G Mellema, J Schaye, R Thomas, H Vedantham, E Chapman, FB Abdalla, A Alexov, J Anderson, IM Avruch, F Batejat, ME Bell, MR Bell, M Bentum, P Best, A Bonafede, J Bregman, F Breitling, RH van de Brink, JW Broderick, M Bruggen, J Conway, F de Gasperin, E de Geus, S Duscha, H Falcke, RA Fallows, C Ferrari, W Frieswijk, MA Garrett, JM Griessmeier, AW Gunst, TE Hassall, JWT Hessels, M Hoeft, M Iacobelli, E Juette, A Karastergiou, VI Kondratiev, M Kramer, M Kuniyoshi, G Kuper, J van Leeuwen, P Maat, G Mann, JP McKean, M Mevius, JD Mol, H Munk, R Nijboer, JE Noordam, MJ Norden, E Orru, H Paas, M Pandey-Pommier, R Pizzo, AG Polatidis, W Reich, HJA Rottgering, J Sluman, O Smirnov, B Stappers, M Steinmetz, M Tagger, Y Tang, C Tasse, S ter Veen, R Vermeulen, RJ van Weeren, M Wise, O Wucknitz, P Zarka

Abstract:

The aim of the LOFAR Epoch of Reionization (EoR) project is to detect the spectral fluctuations of the redshifted HI 21cm signal. This signal is weaker by several orders of magnitude than the astrophysical foreground signals and hence, in order to achieve this, very long integrations, accurate calibration for stations and ionosphere and reliable foreground removal are essential. One of the prospective observing windows for the LOFAR EoR project will be centered at the North Celestial Pole (NCP). We present results from observations of the NCP window using the LOFAR highband antenna (HBA) array in the frequency range 115 MHz to 163 MHz. The data were obtained in April 2011 during the commissioning phase of LOFAR. We used baselines up to about 30 km. With about 3 nights, of 6 hours each, effective integration we have achieved a noise level of about 100 microJy/PSF in the NCP window. Close to the NCP, the noise level increases to about 180 microJy/PSF, mainly due to additional contamination from unsubtracted nearby sources. We estimate that in our best night, we have reached a noise level only a factor of 1.4 above the thermal limit set by the noise from our Galaxy and the receivers. Our continuum images are several times deeper than have been achieved previously using the WSRT and GMRT arrays. We derive an analytical explanation for the excess noise that we believe to be mainly due to sources at large angular separation from the NCP.

The closest black holes

(2013)

Authors:

Rob Fender, Tom Maccarone, Ian Heywood

Active galactic nucleus torus models and the puzzling infrared spectrum of IRAS F10214+4724

Monthly Notices of the Royal Astronomical Society 436:2 (2013) 1873-1882

Authors:

A Efstathiou, N Christopher, A Verma, R Siebenmorgen

Abstract:

We present a revised model for the infrared emission of the hyperluminous infrared galaxy IRAS F10214+4724 which takes into account recent photometric data from Spitzer and Herschel that sample the peak of its spectral energy distribution. We first present and discuss a grid of smooth active galactic nucleus (AGN) torus models computed with the method of Efstathiou & Rowan-Robinson and demonstrate that the combination of these models and the starburst models of Efstathiou and coworkers, while able to give an excellent fit to the average spectrum of Seyfert 2s and spectra of individual type 2 quasars measured by Spitzer, fails to match the spectral energy distribution of IRAS F10214+4724. This is mainly due to the fact that the νSν distribution of the galaxy falls very steeply with increasing frequency (a characteristic that is usually indicative of heavy absorption by dust) but shows a silicate feature in emission. Such emission features are not expected in sources with optical/near-infrared type 2 AGN spectral signatures. The Herschel data show that there is more power emitted in the rest-frame 20-50 μm wavelength range compared with the model presented by Efstathiou which assumes three components of emission: an edge-on torus, clouds (at a temperature of 610 and 200 K) that are associated with the narrow-line region (NLR) and a highly obscured starburst that dominates in the submillimetre. We present a revised version of that model that assumes an additional component of emission which we associate with NLR clouds at a temperature of 100 K. The 100 K dust component could also be explained by a highly obscured hot starburst. The model suggests that the NLR of IRAS F10214+4724 has an unusually high covering factor (≥17 per cent) or more likely the magnification of the emission from the NLR clouds is significantly higher than that of the emission from the torus. © 2013 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society.