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.

A detailed gravitational lens model based on Submillimeter Array and Keck adaptive optics imaging of a Herschel-atlas submillimeter galaxy at z = 4.243

Astrophysical Journal 756:2 (2012)

Authors:

RS Bussmann, MA Gurwell, H Fu, DJB Smith, S Dye, R Auld, M Baes, AJ Baker, D Bonfield, A Cava, DL Clements, A Cooray, K Coppin, H Dannerbauer, A Dariush, G De Zotti, L Dunne, S Eales, J Fritz, R Hopwood, E Ibar, RJ Ivison, MJ Jarvis, S Kim, LL Leeuw, S Maddox, MJ Michałowski, M Negrello, E Pascale, M Pohlen, DA Riechers, E Rigby, D Scott, P Temi, PP Van Der Werf, J Wardlow, D Wilner, A Verma

Abstract:

We present high-spatial resolution imaging obtained with the Submillimeter Array (SMA) at 880 μm and the Keck adaptive optics (AO) system at the K S-band of a gravitationally lensed submillimeter galaxy (SMG) at z = 4.243 discovered in the Herschel Astrophysical Terahertz Large Area Survey. The SMA data (angular resolution 06) resolve the dust emission into multiple lensed images, while the Keck AO K S-band data (angular resolution 01) resolve the lens into a pair of galaxies separated by 03. We present an optical spectrum of the foreground lens obtained with the Gemini-South telescope that provides a lens redshift of z lens = 0.595 ± 0.005. We develop and apply a new lens modeling technique in the visibility plane that shows that the SMG is magnified by a factor of μ = 4.1 ± 0.2 and has an intrinsic infrared (IR) luminosity of L IR = (2.1 ± 0.2) × 1013 L ⊙. We measure a half-light radius of the background source of r s = 4.4 ± 0.5kpc which implies an IR luminosity surface density of ΣIR = (3.4 ± 0.9) × 1011 L ⊙kpc-2, a value that is typical of z > 2 SMGs but significantly lower than IR luminous galaxies at z 0. The two lens galaxies are compact (r lens 0.9kpc) early-types with Einstein radii of θE1 = 0.57 ± 0.01 and θE2 = 0.40 ± 0.01 that imply masses of M lens1 = (7.4 ± 0.5) × 1010 M ⊙ and M lens2 = (3.7 ± 0.3) × 10 10 M ⊙. The two lensing galaxies are likely about to undergo a dissipationless merger, and the mass and size of the resultant system should be similar to other early-type galaxies at z 0.6. This work highlights the importance of high spatial resolution imaging in developing models of strongly lensed galaxies discovered by Herschel. © 2012. The American Astronomical Society. All rights reserved.

The coordinated radio and infrared survey for High-mass star formation (The CORNISH Survey). I. Survey design

Publications of the Astronomical Society of the Pacific 124:919 (2012) 939-955

Authors:

MG Hoare, CR Purcell, EB Churchwell, P Diamond, WD Cotton, CJ Chandler, S Smethurst, SE Kurtz, LG Mundy, SM Dougherty, RP Fender, GA Fuller, JM Jackson, ST Garrington, TR Gledhill, PF Goldsmith, SL Lumsden, J Martí, TJT Moore, TWB Muxlow, RD Oudmaijer, JD Pandian, JM Paredes, DS Shepherd, RE Spencer, MA Thompson, G Umana, JS Urquhart, AA Zijlstra

Abstract:

We describe the motivation, design, and implementation of the CORNISH survey, an arcsecondresolution radio continuum survey of the inner galactic plane at 5 GHz using the Very Large Array (VLA). It is a blind survey coordinated with the northern Spitzer GLIMPSE I region covering 10° < l < 65° and |b| < 1° at similar resolution. We discuss in detail the strategy that we employed to control the shape of the synthesised beam across this survey, which covers a wide range of fairly low declinations. Two snapshots separated by 4h kept the beam elongation to less that 1.5 over 75% of the survey area and less than 2 over 98% of the survey. The prime scientific motivation is to provide an unbiased survey for ultra-compact H II regions to study this key phase in massive star formation. A sensitivity around 2 mJy will allow the automatic distinction between radio-loud and radio-quiet mid- IR sources found in the Spitzer surveys. This survey has many legacy applications beyond star formation, including evolved stars, active stars and binaries, and extragalactic sources. The CORNISH survey for compact ionized sources complements other Galactic plane surveys that target diffuse and nonthermal sources, as well as atomic and molecular phases to build up a complete picture of the interstellar medium in the Galaxy. © 2012. The Astronomical Society of the Pacific.