First LOFAR Observations of Gamma-Ray Binaries

(2012)

Authors:

Benito Marcote, Marc Ribó, Josep M Paredes, John Swinbank, Jess Broderick, Rob Fender, Sera Markoff, Ralf Wijers

Observations of transients and pulsars with LOFAR international stations and the ARTEMIS backend

ArXiv 1210.4318 (2012)

Authors:

Maciej Serylak, Aris Karastergiou, Chris Williams, Wesley Armour, Michael Giles, the LOFAR Pulsar Working Group

Abstract:

The LOw Frequency ARray - LOFAR - is a new radio interferometer designed with emphasis on flexible digital hardware instead of mechanical solutions. The array elements, so-called stations, are located in the Netherlands and in neighbouring countries. The design of LOFAR allows independent use of its international stations, which, coupled with a dedicated backend, makes them very powerful telescopes in their own right. This backend is called the Advanced Radio Transient Event Monitor and Identification System (ARTEMIS). It is a combined software/hardware solution for both targeted observations and real-time searches for millisecond radio transients which uses Graphical Processing Unit (GPU) technology to remove interstellar dispersion and detect millisecond radio bursts from astronomical sources in real-time.

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.

Measurements of CO redshifts with Z-spec for lensed submillimeter galaxies discovered in the H-atlas survey

Astrophysical Journal 757:2 (2012)

Authors:

RE Lupu, KS Scott, JE Aguirre, I Aretxaga, R Auld, E Barton, A Beelen, F Bertoldi, JJ Bock, D Bonfield, CM Bradford, S Buttiglione, A Cava, DL Clements, J Cooke, A Cooray, H Dannerbauer, A Dariush, G De Zotti, L Dunne, S Dye, S Eales, D Frayer, J Fritz, J Glenn, DH Hughes, E Ibar, RJ Ivison, MJ Jarvis, J Kamenetzky, S Kim, G Lagache, L Leeuw, S Maddox, PR Maloney, H Matsuhara, EJ Murphy, BJ Naylor, M Negrello, H Nguyen, A Omont, E Pascale, M Pohlen, E Rigby, G Rodighiero, S Serjeant, D Smith, P Temi, M Thompson, I Valtchanov, A Verma, JD Vieira, J Zmuidzinas

Abstract:

We present new observations from Z-Spec, a broadband 185-305GHz spectrometer, of five submillimeter bright lensed sources selected from the Herschel-Astrophysical Terahertz Large Area Survey science demonstration phase catalog. We construct a redshift-finding algorithm using combinations of the signal to noise of all the lines falling in the Z-Spec bandpass to determine redshifts with high confidence, even in cases where the signal to noise in individual lines is low. We measure the dust continuum in all sources and secure CO redshifts for four out of five (z 1.5-3). In one source, SDP.17, we tentatively identify two independent redshifts and a water line, confirmed at z = 2.308. Our sources have properties characteristic of dusty starburst galaxies, with magnification-corrected star formation rates of 102-3 M ⊙ yr-1. Lower limits for the dust masses (∼a few 108 M ⊙) and spatial extents (1kpc equivalent radius) are derived from the continuum spectral energy distributions, corresponding to dust temperatures between 54 and 69K. In the local thermodynamic equilibrium (LTE) approximation, we derive relatively low CO excitation temperatures (≲ 100 K) and optical depths (τ ≲ 1). Performing a non-LTE excitation analysis using RADEX, we find that the CO lines measured by Z-Spec (from J = 4 → 3 to 10 → 9, depending on the galaxy) localize the best solutions to either a high-temperature/low-density region or a low/temperature/high-density region near the LTE solution, with the optical depth varying accordingly. Observations of additional CO lines, CO(1-0) in particular, are needed to constrain the non-LTE models. © 2012. The American Astronomical Society. All rights reserved.

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.