M87 at metre wavelengths: the LOFAR picture

ArXiv 1210.1346 (2012)

Authors:

F de Gasperin, E Orru', M Murgia, A Merloni, H Falcke, R Beck, R Beswick, L Birzan, A Bonafede, M Bruggen, G Brunetti, K Chyzy, J Conway, JH Croston, T Ensslin, C Ferrari, G Heald, S Heidenreich, N Jackson, G Macario, J McKean, G Miley, R Morganti, A Offringa, R Pizzo, D Rafferty, H Roettgering, A Shulevski, M Steinmetz, C Tasse, S van der Tol, W van Driel, RJ van Weeren, JE van Zwieten, A Alexov, J Anderson, A Asgekar, M Avruch, M Bell, MR Bell, M Bentum, G Bernardi, P Best, F Breitling, JW Broderick, A Butcher, B Ciardi, RJ Dettmar, J Eisloeffel, W Frieswijk, H Gankema, M Garrett, M Gerbers, JM Griessmeier, AW Gunst, TE Hassall, J Hessels, M Hoeft, A Horneffer, A Karastergiou, J Koehler, Y Koopman, G Kuper, P Maat, G Mann, M Mevius, DD Mulcahy, H Munk, R Nijboer, M Kuniyoshi, J Noordam, H Paas, M Pandey, VN Pandey, A Polatidis, W Reich, AP Schoenmakers, J Sluman, O Smirnov, C Sobey, B Stappers, J Swinbank, M Tagger, Y Tang, I van Bemmel, W van Cappellen, AP van Duin, M van Haarlem, J van Leeuwen, R Vermeulen, C Vocks, S White, M Wise, O Wucknitz, P Zarka

Abstract:

M87 is a giant elliptical galaxy located in the centre of the Virgo cluster, which harbours a supermassive black hole of mass 6.4x10^9 M_sun, whose activity is responsible for the extended (80 kpc) radio lobes that surround the galaxy. The energy generated by matter falling onto the central black hole is ejected and transferred to the intra-cluster medium via a relativistic jet and morphologically complex systems of buoyant bubbles, which rise towards the edges of the extended halo. Here we present the first observations made with the new Low-Frequency Array (LOFAR) of M87 at frequencies down to 20 MHz. Images of M87 were produced at low radio frequencies never explored before at these high spatial resolution and dynamic range. To disentangle different synchrotron models and place constraints on source magnetic field, age and energetics, we also performed a detailed spectral analysis of M87 extended radio-halo using these observations together with archival data. We do not find any sign of new extended emissions; on the contrary the source appears well confined by the high pressure of the intra-cluster medium. A continuous injection of relativistic electrons is the model that best fits our data, and provides a scenario in which the lobes are still supplied by fresh relativistic particles from the active galactic nuclei. We suggest that the discrepancy between the low-frequency radio-spectral slope in the core and in the halo implies a strong adiabatic expansion of the plasma as soon as it leaves the core area. The extended halo has an equipartition magnetic field strength of ~10 uG, which increases to ~13 uG in the zones where the particle flows are more active. The continuous injection model for synchrotron ageing provides an age for the halo of ~40 Myr, which in turn provides a jet kinetic power of 6-10x10^44 erg/s.

The LOFAR radio environment

ArXiv 1210.0393 (2012)

Authors:

AR Offringa, AG de Bruyn, S Zaroubi, G van Diepen, O Martinez-Ruby, P Labropoulos, MA Brentjens, B Ciardi, S Daiboo, G Harker, V Jelic, S Kazemi, LVE Koopmans, G Mellema, VN Pandey, RF Pizzo, J Schaye, H Vedantham, V Veligatla, SJ Wijnholds, S Yatawatta, P Zarka, A Alexov, J Anderson, A Asgekar, M Avruch, R Beck, M Bell, MR Bell, M Bentum, G Bernardi, P Best, L Birzan, A Bonafede, F Breitling, JW Broderick, M Bruggen, H Butcher, J Conway, M de Vos, RJ Dettmar, J Eisloeffel, H Falcke, R Fender, W Frieswijk, M Gerbers, JM Griessmeier, AW Gunst, TE Hassall, G Heald, J Hessels, M Hoeft, A Horneffer, A Karastergiou, V Kondratiev, Y Koopman, M Kuniyoshi, G Kuper, P Maat, G Mann, J McKean, H Meulman, M Mevius, JD Mol, R Nijboer, J Noordam, M Norden, H Paas, M Pandey, R Pizzo, A Polatidis, D Rafferty, S Rawlings, W Reich, HJA Rottgering, AP Schoenmakers, J Sluman, O Smirnov, C Sobey, B Stappers, M Steinmetz, J Swinbank, M Tagger, Y Tang, C Tasse, A van Ardenne, W van Cappellen, AP van Duin, M van Haarlem, J van Leeuwen, RJ van Weeren, R Vermeulen, C Vocks, RAMJ Wijers, M Wise, O Wucknitz

Abstract:

Aims: This paper discusses the spectral occupancy for performing radio astronomy with the Low-Frequency Array (LOFAR), with a focus on imaging observations. Methods: We have analysed the radio-frequency interference (RFI) situation in two 24-h surveys with Dutch LOFAR stations, covering 30-78 MHz with low-band antennas and 115-163 MHz with high-band antennas. This is a subset of the full frequency range of LOFAR. The surveys have been observed with a 0.76 kHz / 1 s resolution. Results: We measured the RFI occupancy in the low and high frequency sets to be 1.8% and 3.2% respectively. These values are found to be representative values for the LOFAR radio environment. Between day and night, there is no significant difference in the radio environment. We find that lowering the current observational time and frequency resolutions of LOFAR results in a slight loss of flagging accuracy. At LOFAR's nominal resolution of 0.76 kHz and 1 s, the false-positives rate is about 0.5%. This rate increases approximately linearly when decreasing the data frequency resolution. Conclusions: Currently, by using an automated RFI detection strategy, the LOFAR radio environment poses no perceivable problems for sensitive observing. It remains to be seen if this is still true for very deep observations that integrate over tens of nights, but the situation looks promising. Reasons for the low impact of RFI are the high spectral and time resolution of LOFAR; accurate detection methods; strong filters and high receiver linearity; and the proximity of the antennas to the ground. We discuss some strategies that can be used once low-level RFI starts to become apparent. It is important that the frequency range of LOFAR remains free of broadband interference, such as DAB stations and windmills.

The LOFAR radio environment

(2012)

Authors:

AR Offringa, AG de Bruyn, S Zaroubi, G van Diepen, O Martinez-Ruby, P Labropoulos, MA Brentjens, B Ciardi, S Daiboo, G Harker, V Jelic, S Kazemi, LVE Koopmans, G Mellema, VN Pandey, RF Pizzo, J Schaye, H Vedantham, V Veligatla, SJ Wijnholds, S Yatawatta, P Zarka, A Alexov, J Anderson, A Asgekar, M Avruch, R Beck, M Bell, MR Bell, M Bentum, G Bernardi, P Best, L Birzan, A Bonafede, F Breitling, JW Broderick, M Bruggen, H Butcher, J Conway, M de Vos, RJ Dettmar, J Eisloeffel, H Falcke, R Fender, W Frieswijk, M Gerbers, JM Griessmeier, AW Gunst, TE Hassall, G Heald, J Hessels, M Hoeft, A Horneffer, A Karastergiou, V Kondratiev, Y Koopman, M Kuniyoshi, G Kuper, P Maat, G Mann, J McKean, H Meulman, M Mevius, JD Mol, R Nijboer, J Noordam, M Norden, H Paas, M Pandey, R Pizzo, A Polatidis, D Rafferty, S Rawlings, W Reich, HJA Rottgering, AP Schoenmakers, J Sluman, O Smirnov, C Sobey, B Stappers, M Steinmetz, J Swinbank, M Tagger, Y Tang, C Tasse, A van Ardenne, W van Cappellen, AP van Duin, M van Haarlem, J van Leeuwen, RJ van Weeren, R Vermeulen, C Vocks, RAMJ Wijers, M Wise, O Wucknitz

The Large Observatory for X-ray Timing (LOFT)

Experimental Astronomy 34:2 (2012) 415-444

Authors:

M Feroci, L Stella, M van der Klis, TJL Courvoisier, M Hernanz, R Hudec, A Santangelo, D Walton, A Zdziarski, D Barret, T Belloni, J Braga, S Brandt, C Budtz-Jørgensen, S Campana, JW den Herder, J Huovelin, GL Israel, M Pohl, P Ray, A Vacchi, S Zane, A Argan, P Attinà, G Bertuccio, E Bozzo, R Campana, D Chakrabarty, E Costa, A de Rosa, E Del Monte, S Di Cosimo, I Donnarumma, Y Evangelista, D Haas, P Jonker, S Korpela, C Labanti, P Malcovati, R Mignani, F Muleri, M Rapisarda, A Rashevsky, N Rea, A Rubini, C Tenzer, C Wilson-Hodge, B Winter, K Wood, G Zampa, N Zampa, MA Abramowicz, MA Alpar, D Altamirano, JM Alvarez, L Amati, C Amoros, LA Antonelli, R Artigue, P Azzarello, M Bachetti, G Baldazzi, M Barbera, C Barbieri, S Basa, A Baykal, R Belmont, L Boirin, V Bonvicini, L Burderi, M Bursa, C Cabanac, E Cackett, GA Caliandro, P Casella, S Chaty, J Chenevez, MJ Coe, A Collura, A Corongiu, S Covino, G Cusumano, F D'Amico, S Dall'Osso, D de Martino, G de Paris, G Di Persio, T Di Salvo, C Done, M Dovčiak, A Drago, U Ertan, S Fabiani, M Falanga, R Fender, P Ferrando, D della Monica Ferreira, G Fraser, F Frontera, F Fuschino

Abstract:

High-time-resolution X-ray observations of compact objects provide direct access to strong-field gravity, to the equation of state of ultradense matter and to black hole masses and spins. A 10 m 2-class instrument in combination with good spectral resolution is required to exploit the relevant diagnostics and answer two of the fundamental questions of the European Space Agency (ESA) Cosmic Vision Theme "Matter under extreme conditions", namely: does matter orbiting close to the event horizon follow the predictions of general relativity? What is the equation of state of matter in neutron stars? The Large Observatory For X-ray Timing (LOFT), selected by ESA as one of the four Cosmic Vision M3 candidate missions to undergo an assessment phase, will revolutionise the study of collapsed objects in our galaxy and of the brightest supermassive black holes in active galactic nuclei. Thanks to an innovative design and the development of large-area monolithic silicon drift detectors, the Large Area Detector (LAD) on board LOFT will achieve an effective area of ~12 m 2 (more than an order of magnitude larger than any spaceborne predecessor) in the 2-30 keV range (up to 50 keV in expanded mode), yet still fits a conventional platform and small/medium-class launcher. With this large area and a spectral resolution of <260 eV, LOFT will yield unprecedented information on strongly curved spacetimes and matter under extreme conditions of pressure and magnetic field strength. © 2011 Springer Science+Business Media B.V.

Infrared spectroscopy of nearby radio active elliptical galaxies

(2012)

Authors:

Jeremy Mould, Tristan Reynolds, Tony Readhead, David Floyd, Buell Jannuzi, Garret Cotter, Laura Ferrarese, Keith Matthews, David Atlee, Michael Brown