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sky and dish

Aris Karastergiou

Professor of Astrophysics and Fellow at St Edmund Hall

Research theme

  • Astronomy and astrophysics

Sub department

  • Astrophysics

Research groups

  • MeerKAT
  • Pulsars, transients and relativistic astrophysics
  • The Square Kilometre Array (SKA)
  • Gamma-ray astronomy
Aris.Karastergiou@physics.ox.ac.uk
Telephone: 01865 (2)73642
Denys Wilkinson Building, room 603C
  • About
  • Publications

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.
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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.
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Long timescale radio emission variability and spin-down changes in PSR J0738-4042

Proceedings of the International Astronomical Union Cambridge University Press (CUP) 8:S291 (2012) 161-161

Authors:

Aris Karastergiou, Paul Brook, Steve Roberts, Sarah Buchner, Simon Johnston
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Observations of transients and pulsars with LOFAR international stations

ArXiv 1207.0354 (2012)

Authors:

Maciej Serylak, Aris Karastergiou, Chris Williams, Wes Armour, LOFAR Pulsar Working Group

Abstract:

The LOw FRequency ARray - LOFAR is a new radio telescope that is moving the science of radio pulsars and transients into a new phase. Its design places emphasis on digital hardware and flexible software instead of mechanical solutions. LOFAR observes at radio frequencies between 10 and 240 MHz where radio pulsars and many transients are expected to be brightest. Radio frequency signals emitted from these objects allow us to study the intrinsic pulsar emission and phenomena such as propagation effects through the interstellar medium. The design of LOFAR allows independent use of its stations to conduct observations of known bright objects, or wide field monitoring of transient events. One such combined software/hardware solution is called the Advanced Radio Transient Event Monitor and Identification System (ARTEMIS). It is a backend 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 using a single LOFAR station.
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Wide-band Simultaneous Observations of Pulsars: Disentangling Dispersion Measure and Profile Variations

ArXiv 1204.3864 (2012)

Authors:

TE Hassall, BW Stappers, JWT Hessels, M Kramer, A Alexov, K Anderson, T Coenen, A Karastergiou, EF Keane, VI Kondratiev, K Lazaridis, J van Leeuwen, A Noutsos, M Serylak, C Sobey, JPW Verbiest, P Weltevrede, K Zagkouris, R Fender, RAMJ Wijers, L Bahren, ME Bell, JW Broderick, S Corbel, EJ Daw, VS Dhillon, J Eisloffel, H Falcke, J-M Griessmeier, P Jonker, C Law, S Markoff, JCA Miller-Jones, R Osten, E Rol, AMM Scaife, B Scheers, P Schellart, H Spreeuw, J Swinbank, S ter Veen, MW Wise, R Wijnands, O Wucknitz, P Zarka, A Asgekar, MR Bell, MJ Bentum, G Bernardi, P Best, A Bonafede, AJ Boonstra, M Brentjens, WN Brouw, M Bruggen, HR Butcher, B Ciardi, MA Garrett, M Gerbers, AW Gunst, MP van Haarlem, G Heald, M Hoeft, H Holties, A de Jong, LVE Koopmans, M Kuniyoshi, G Kuper, GM Loose, P Maat, J Masters, JP McKean, H Meulman, M Mevius, H Munk, JE Noordam, E Orru, H Paas, M Pandey-Pommier, VN Pandey, R Pizzo, A Polatidis, W Reich, H Rottgering, J Sluman, M Steinmetz, CGM Sterks, M Tagger, Y Tang, C Tasse, R Vermeulen, RJ van Weeren, SJ Wijnholds, S Yatawatta

Abstract:

Dispersion in the interstellar medium is a well known phenomenon that follows a simple relationship, which has been used to predict the time delay of dispersed radio pulses since the late 1960s. We performed wide-band simultaneous observations of four pulsars with LOFAR (at 40-190 MHz), the 76-m Lovell Telescope (at 1400 MHz) and the Effelsberg 100-m Telescope (at 8000 MHz) to test the accuracy of the dispersion law over a broad frequency range. In this paper we present the results of these observations which show that the dispersion law is accurate to better than 1 part in 100000 across our observing band. We use this fact to constrain some of the properties of the ISM along the line-of-sight and use the lack of any aberration or retardation effects to determine upper limits on emission heights in the pulsar magnetosphere. We also discuss the effect of pulse profile evolution on our observations, and the implications that it could have for precision pulsar timing projects such as the detection of gravitational waves with pulsar timing arrays.
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