Issue |
A&A
Volume 550, February 2013
|
|
---|---|---|
Article Number | A136 | |
Number of page(s) | 17 | |
Section | Astronomical instrumentation | |
DOI | https://doi.org/10.1051/0004-6361/201220874 | |
Published online | 07 February 2013 |
Initial deep LOFAR observations of epoch of reionization windows
I. The north celestial pole
1
University of Groningen, Kapteyn Astronomical
Institute, PO Box
800, 9700 AV
Groningen, The
Netherlands
2
ASTRON, PO Box
2, 7990 AA
Dwingeloo, The
Netherlands
e-mail: yatawatta@astron.nl
3
Max-Planck Institute for Astrophysics,
Karl-Schwarzschild-Strasse 1,
85748
Garching bei München,
Germany
4
Center for Astrophysics and Space Astronomy, University of
Colorado, 389
UCB, Boulder,
Colorado
80309-0389,
USA
5
Department of Astronomy & Oskar Klein Centre, AlbaNova,
Stockholm University, 10691
Stockholm,
Sweden
6
Leiden Observatory, Leiden University,
PO Box 9513, 2300 RA
Leiden, The
Netherlands
7
Observatoire de Paris, 92195
Meudon,
France
8
University of Amsterdam, Astronomical Institute Anton
Pannekoek, PO Box
94249, 1090 GE
Amsterdam, The
Netherlands
9
Max-Planck Institute for Astrophysics,
PO Box 20 24, 53010
Bonn,
Germany
10
SRON Netherlands Institute for Space Research,
PO Box 800, 9700 AV
Groningen, The
Netherlands
11 Sydney Institute for Astronomy, School of Physics A28,
University of Sydney, NSW 2006, Australia
12
Harvard-Smithsonian Center for Astrophysics, 60 Garden
Street, Cambridge,
MA
02138,
USA
13
Royal Observatory Edinburgh, Blackford Hill, Edinburgh, EH9 3HJ, UK
14
Jacobs University Bremen, Campus Ring 1, 28759
Bremen,
Germany
15
Astrophysical Institute Potsdam, An der Sternwarte 16, 14482
Potsdam,
Germany
16
University of Southampton, University Road,
Southampton
SO17 1BJ,
UK
17
University of Hamburg, Gojenbergsweg 112, 21029
Hamburg,
Germany
18
Astronomisches Institut der Ruhr-Universität Bochum,
Universitaetsstrasse 150, 44780
Bochum,
Germany
19
Thüringer Landessternwarte, Tautenburg Observatory,
Sternwarte 5, 07778
Tautenburg,
Germany
20
Radboud University Nijmegen, Faculty of NWI,
PO Box 9010, 6500 GL
Nijmegen, The
Netherlands
21
Centre national de la recherche scientifique, 3 rue
Michel-Ange, 75794
Paris Cedex 16,
France
22
Jodrell Bank Center for Astrophysics, School of Physics and
Astronomy, The University of Manchester, Manchester
M13 9PL,
UK
23
University of Oxford, Wellington Square, Oxford
OX1 2JD,
UK
24
Centre de Recherche Astrophysique de Lyon, Observatoire de
Lyon, 9 Av. Charles
André, 69561
Saint Genis Laval Cedex,
France
25
Rhodes University, RATT, Dep. Physics and Electronics, PO Box 94,
6140
Grahamstown, South
Africa
26
Argelander-Institut für Astronomie, Auf dem Hügel 71, 53121
Bonn,
Germany
27
UCL, Department of Physics & Astronomy, University
College London, Gower
Street, London,
WC1E 6BT,
UK
28
Space Telescope Science Institute, 3700 San Martin Drive, Baltimore, MD
21218,
USA
29
Onsala Space Observatory, Dept. of Earth and Space Sciences,
Chalmers University of Technology, 43992
Onsala,
Sweden
30
Laboratoire Lagrange, UMR7293, Universitè de Nice
Sophia-Antipolis, CNRS, Observatoire de la Cóte d’Azur, 06300
Nice,
France
31
Astro Space Center of the Lebedev Physical
Institute, Profsoyuznaya str.
84/32, 117997
Moscow,
Russia
32 Center for Information Technology (CIT), University of
Groningen, The Netherlands
33
Mount Stromlo Observatory, RSAA, Cotter Road, Weston Creek, ACT
2611,
Australia
Received:
7
December
2012
Accepted:
8
January
2013
Aims. The aim of the LOFAR epoch of reionization (EoR) project is to detect the spectral fluctuations of the redshifted HI 21 cm 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.
Methods. 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. The data was processed using a dedicated processing pipeline which is an enhanced version of the standard LOFAR processing pipeline.
Results. With about 3 nights, of 6 h each, effective integration we have achieved a noise level of about 100 μJy/PSF in the NCP window. Close to the NCP, the noise level increases to about 180 μJy/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. We present some details of the data processing challenges and how we solved them.
Conclusions. Although many LOFAR stations were, at the time of the observations, in a still poorly calibrated state we have seen no artefacts in our images which would prevent us from producing deeper images in much longer integrations on the NCP window which are about to commence. The limitations present in our current results are mainly due to sidelobe noise from the large number of distant sources, as well as errors related to station beam variations and rapid ionospheric phase fluctuations acting on bright sources. We are confident that we can improve our results with refined processing.
Key words: dark ages, reionization, first stars / instrumentation: interferometers / techniques: interferometric / methods: data analysis
© ESO, 2013
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