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Author

Mark J. Bentum

Other affiliations: University of Twente, ASTRON, Information Technology University  ...read more
Bio: Mark J. Bentum is an academic researcher from Eindhoven University of Technology. The author has contributed to research in topics: LOFAR & Radio telescope. The author has an hindex of 42, co-authored 226 publications receiving 8347 citations. Previous affiliations of Mark J. Bentum include University of Twente & ASTRON.


Papers
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Journal ArticleDOI
M. P. van Haarlem1, Michael W. Wise2, Michael W. Wise1, A. W. Gunst1  +219 moreInstitutions (27)
TL;DR: In dit artikel zullen the authors LOFAR beschrijven: van de astronomische mogelijkheden met de nieuwe telescoop tot aan een nadere technische beshrijving of het instrument.
Abstract: LOFAR, the LOw-Frequency ARray, is a new-generation radio interferometer constructed in the north of the Netherlands and across europe. Utilizing a novel phased-array design, LOFAR covers the largely unexplored low-frequency range from 10-240 MHz and provides a number of unique observing capabilities. Spreading out from a core located near the village of Exloo in the northeast of the Netherlands, a total of 40 LOFAR stations are nearing completion. A further five stations have been deployed throughout Germany, and one station has been built in each of France, Sweden, and the UK. Digital beam-forming techniques make the LOFAR system agile and allow for rapid repointing of the telescope as well as the potential for multiple simultaneous observations. With its dense core array and long interferometric baselines, LOFAR achieves unparalleled sensitivity and angular resolution in the low-frequency radio regime. The LOFAR facilities are jointly operated by the International LOFAR Telescope (ILT) foundation, as an observatory open to the global astronomical community. LOFAR is one of the first radio observatories to feature automated processing pipelines to deliver fully calibrated science products to its user community. LOFAR's new capabilities, techniques and modus operandi make it an important pathfinder for the Square Kilometre Array (SKA). We give an overview of the LOFAR instrument, its major hardware and software components, and the core science objectives that have driven its design. In addition, we present a selection of new results from the commissioning phase of this new radio observatory.

2,067 citations

Journal ArticleDOI
TL;DR: The International LOFAR Telescope (ILT) as mentioned in this paper is a new-generation radio interferometer constructed in the north of the Netherlands and across europe, which covers the largely unexplored low frequency range from 10-240 MHz and provides a number of unique observing capabilities.
Abstract: LOFAR, the LOw-Frequency ARray, is a new-generation radio interferometer constructed in the north of the Netherlands and across europe. Utilizing a novel phased-array design, LOFAR covers the largely unexplored low-frequency range from 10-240 MHz and provides a number of unique observing capabilities. Spreading out from a core located near the village of Exloo in the northeast of the Netherlands, a total of 40 LOFAR stations are nearing completion. A further five stations have been deployed throughout Germany, and one station has been built in each of France, Sweden, and the UK. Digital beam-forming techniques make the LOFAR system agile and allow for rapid repointing of the telescope as well as the potential for multiple simultaneous observations. With its dense core array and long interferometric baselines, LOFAR achieves unparalleled sensitivity and angular resolution in the low-frequency radio regime. The LOFAR facilities are jointly operated by the International LOFAR Telescope (ILT) foundation, as an observatory open to the global astronomical community. LOFAR is one of the first radio observatories to feature automated processing pipelines to deliver fully calibrated science products to its user community. LOFAR's new capabilities, techniques and modus operandi make it an important pathfinder for the Square Kilometre Array (SKA). We give an overview of the LOFAR instrument, its major hardware and software components, and the core science objectives that have driven its design. In addition, we present a selection of new results from the commissioning phase of this new radio observatory.

1,818 citations

Journal ArticleDOI
B. W. Stappers1, Jason W. T. Hessels2, Jason W. T. Hessels3, A. Alexov3, Kenneth C. Anderson3, T. Coenen3, T. E. Hassall1, Aris Karastergiou4, V. I. Kondratiev2, Michael Kramer1, Michael Kramer5, J. van Leeuwen3, J. van Leeuwen2, J. D. Mol2, A. Noutsos5, John W. Romein2, Patrick Weltevrede1, Rob Fender6, Ralph A. M. J. Wijers3, L. Bähren3, Martin Bell6, J. W. Broderick6, E. J. Daw7, V. S. Dhillon7, Jochen Eislöffel, Heino Falcke2, Heino Falcke8, J. M. Griessmeier2, J. M. Griessmeier9, Casey J. Law3, Casey J. Law10, Sera Markoff3, James Miller-Jones3, James Miller-Jones11, Bart Scheers3, H. Spreeuw3, John D. Swinbank3, S. ter Veen8, Michael W. Wise2, Michael W. Wise3, Olaf Wucknitz12, Philippe Zarka13, J. M. Anderson5, Ashish Asgekar2, I. M. Avruch2, I. M. Avruch14, Rainer Beck5, P. Bennema2, Mark J. Bentum2, Philip Best15, Joel N. Bregman2, Michiel A. Brentjens2, R. H. van de Brink2, P. C. Broekema2, W. N. Brouw14, Marcus Brüggen16, A. G. de Bruyn2, A. G. de Bruyn14, Harvey Butcher2, Harvey Butcher17, B. Ciardi5, John Conway18, R.-J. Dettmar19, A. van Duin2, J. van Enst2, M. A. Garrett20, M. A. Garrett2, M. Gerbers2, T. Grit2, A. W. Gunst2, M. P. van Haarlem2, J. P. Hamaker2, George Heald2, Matthias Hoeft, H. A. Holties2, A. Horneffer5, A. Horneffer8, Léon V. E. Koopmans14, Gerard H. Kuper2, M. Loose2, P. Maat2, D. McKay-Bukowski21, John McKean2, George K. Miley20, Raffaella Morganti14, Raffaella Morganti2, R. Nijboer2, J. Noordam2, M. J. Norden2, Hans Olofsson18, M. Pandey-Pommier20, A. G. Polatidis2, Wolfgang Reich5, H. J. A. Röttgering20, A. Schoenmakers2, J. Sluman2, Oleg Smirnov2, Matthias Steinmetz22, C. G. M. Sterks23, Michel Tagger9, Y. Tang2, R. Vermeulen2, N. J. Vermaas2, C. Vogt2, M. de Vos2, Stefan J. Wijnholds2, Sarod Yatawatta14, A. Zensus5 
TL;DR: The LOw Frequency ARray (LOFAR) as mentioned in this paper is a radio interferometer operating in the lowest 4 octaves of the ionospheric "radio window": 10-240 MHz, that will greatly facilitate observing pulsars at low radio frequencies.
Abstract: Low frequency radio waves, while challenging to observe, are a rich source of information about pulsars. The LOw Frequency ARray (LOFAR) is a new radio interferometer operating in the lowest 4 octaves of the ionospheric "radio window": 10-240 MHz, that will greatly facilitate observing pulsars at low radio frequencies. Through the huge collecting area, long baselines, and flexible digital hardware, it is expected that LOFAR will revolutionize radio astronomy at the lowest frequencies visible from Earth. LOFAR is a next-generation radio telescope and a pathfinder to the Square Kilometre Array (SKA), in that it incorporates advanced multi-beaming techniques between thousands of individual elements. We discuss the motivation for low-frequency pulsar observations in general and the potential of LOFAR in addressing these science goals. We present LOFAR as it is designed to perform high-time-resolution observations of pulsars and other fast transients, and outline the various relevant observing modes and data reduction pipelines that are already or will soon be implemented to facilitate these observations. A number of results obtained from commissioning observations are presented to demonstrate the exciting potential of the telescope. This paper outlines the case for low frequency pulsar observations and is also intended to serve as a reference for upcoming pulsar/fast transient science papers with LOFAR.

284 citations

Journal ArticleDOI
TL;DR: In this paper, a novel optical beamformer concept is introduced that can be used for seamless control of the reception angle in broadband wireless receivers employing a large phased array antenna (PAA).
Abstract: A novel optical beamformer concept is introduced that can be used for seamless control of the reception angle in broadband wireless receivers employing a large phased array antenna (PAA). The core of this beamformer is an optical beamforming network (OBFN), using ring resonator-based broadband delays, and coherent optical combining. The electro-optical conversion is performed by means of single-sideband suppressed carrier modulation, employing a common laser, Mach-Zehnder modulators, and a common optical sideband filter after the OBFN. The unmodulated laser signal is then re-injected in order to perform balanced coherent optical detection, for the opto-electrical conversion. This scheme minimizes the requirements on the complexity of the OBFN, and has potential for compact realization by means of full integration on chip. The impact of the optical beamformer concept on the performance of the full receiver system is analyzed, by modeling the combination of the PAA and the beamformer as an equivalent two-port RF system. The results are illustrated by a numerical example of a PAA receiver for satellite TV reception, showing that - when properly designed - the beamformer hardly affects the sensitivity of the receiver.

188 citations

Journal ArticleDOI
Sarod Yatawatta1, de Antonius Bruyn1, de Antonius Bruyn2, Michiel A. Brentjens1, Panagiotis Labropoulos1, V. N. Pandey1, S. Kazemi2, Saleem Zaroubi2, Léon V. E. Koopmans2, A. R. Offringa2, A. R. Offringa3, Vibor Jelić2, O. Martinez Rubi2, V. Veligatla2, Stefan J. Wijnholds1, W. N. Brouw1, Gianni Bernardi4, Gianni Bernardi2, B. Ciardi5, S. Daiboo2, Geraint Harker6, Garrelt Mellema7, Joop Schaye8, Rajat M. Thomas2, Harish Vedantham2, Emma Chapman9, F. B. Abdalla9, A. Alexov10, J. M. Anderson5, I. M. Avruch2, I. M. Avruch11, F. Batejat12, Martin Bell13, Martin Bell14, Michael R. Bell5, Mark J. Bentum1, Philip Best, Annalisa Bonafede15, Joel N. Bregman1, F. Breitling, R. H. van de Brink1, J. W. Broderick13, Marcus Brüggen15, Marcus Brüggen16, John Conway12, F. de Gasperin16, E. de Geus1, S. Duscha1, Heino Falcke17, Richard Fallows1, Chiara Ferrari18, W. Frieswijk1, M. A. Garrett1, M. A. Garrett8, J. M. Griessmeier1, J. M. Griessmeier19, A. W. Gunst1, T. E. Hassall13, T. E. Hassall20, Jason W. T. Hessels1, Jason W. T. Hessels21, Matthias Hoeft, Marco Iacobelli8, E. Juette22, Aris Karastergiou23, V. I. Kondratiev1, V. I. Kondratiev24, Michael Kramer20, Michael Kramer5, M. Kuniyoshi5, Gerard H. Kuper1, J. van Leeuwen1, J. van Leeuwen21, P. Maat1, Gottfried Mann, John McKean1, M. Mevius1, M. Mevius2, J. D. Mol1, H. Munk1, R. Nijboer1, J. Noordam1, M. J. Norden1, Emanuela Orru1, Emanuela Orru17, H. Paas25, M. Pandey-Pommier8, R. Pizzo1, A. G. Polatidis1, Wolfgang Reich5, H. J. A. Röttgering8, J. Sluman1, Oleg Smirnov26, Ben Stappers20, Matthias Steinmetz, Michel Tagger19, Y. Tang1, Cyril Tasse, S. ter Veen17, R. Vermeulen1, R. J. van Weeren1, R. J. van Weeren8, R. J. van Weeren4, Michael W. Wise1, Olaf Wucknitz5, Ph. Zarka 
TL;DR: In this article, the authors present results from observations of the NCP window using the LOFAR highband antenna (HBA) array in the frequency range 115 MHz to 163 MHz.
Abstract: The aim of the LOFAR Epoch of Reionization (EoR) project is to detect the spectral fluctuations of the redshifted HI 21cm 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. 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. With about 3 nights, of 6 hours each, effective integration we have achieved a noise level of about 100 microJy/PSF in the NCP window. Close to the NCP, the noise level increases to about 180 microJy/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.

159 citations


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[...]

08 Dec 2001-BMJ
TL;DR: There is, I think, something ethereal about i —the square root of minus one, which seems an odd beast at that time—an intruder hovering on the edge of reality.
Abstract: There is, I think, something ethereal about i —the square root of minus one. I remember first hearing about it at school. It seemed an odd beast at that time—an intruder hovering on the edge of reality. Usually familiarity dulls this sense of the bizarre, but in the case of i it was the reverse: over the years the sense of its surreal nature intensified. It seemed that it was impossible to write mathematics that described the real world in …

33,785 citations

Journal ArticleDOI
TL;DR: A binary neutron star coalescence candidate (later designated GW170817) with merger time 12:41:04 UTC was observed through gravitational waves by the Advanced LIGO and Advanced Virgo detectors.
Abstract: On 2017 August 17 a binary neutron star coalescence candidate (later designated GW170817) with merger time 12:41:04 UTC was observed through gravitational waves by the Advanced LIGO and Advanced Virgo detectors. The Fermi Gamma-ray Burst Monitor independently detected a gamma-ray burst (GRB 170817A) with a time delay of $\sim 1.7\,{\rm{s}}$ with respect to the merger time. From the gravitational-wave signal, the source was initially localized to a sky region of 31 deg2 at a luminosity distance of ${40}_{-8}^{+8}$ Mpc and with component masses consistent with neutron stars. The component masses were later measured to be in the range 0.86 to 2.26 $\,{M}_{\odot }$. An extensive observing campaign was launched across the electromagnetic spectrum leading to the discovery of a bright optical transient (SSS17a, now with the IAU identification of AT 2017gfo) in NGC 4993 (at $\sim 40\,{\rm{Mpc}}$) less than 11 hours after the merger by the One-Meter, Two Hemisphere (1M2H) team using the 1 m Swope Telescope. The optical transient was independently detected by multiple teams within an hour. Subsequent observations targeted the object and its environment. Early ultraviolet observations revealed a blue transient that faded within 48 hours. Optical and infrared observations showed a redward evolution over ~10 days. Following early non-detections, X-ray and radio emission were discovered at the transient's position $\sim 9$ and $\sim 16$ days, respectively, after the merger. Both the X-ray and radio emission likely arise from a physical process that is distinct from the one that generates the UV/optical/near-infrared emission. No ultra-high-energy gamma-rays and no neutrino candidates consistent with the source were found in follow-up searches. These observations support the hypothesis that GW170817 was produced by the merger of two neutron stars in NGC 4993 followed by a short gamma-ray burst (GRB 170817A) and a kilonova/macronova powered by the radioactive decay of r-process nuclei synthesized in the ejecta.

2,746 citations

Journal ArticleDOI
Kazunori Akiyama, Antxon Alberdi1, Walter Alef2, Keiichi Asada3  +403 moreInstitutions (82)
TL;DR: In this article, the Event Horizon Telescope was used to reconstruct event-horizon-scale images of the supermassive black hole candidate in the center of the giant elliptical galaxy M87.
Abstract: When surrounded by a transparent emission region, black holes are expected to reveal a dark shadow caused by gravitational light bending and photon capture at the event horizon. To image and study this phenomenon, we have assembled the Event Horizon Telescope, a global very long baseline interferometry array observing at a wavelength of 1.3 mm. This allows us to reconstruct event-horizon-scale images of the supermassive black hole candidate in the center of the giant elliptical galaxy M87. We have resolved the central compact radio source as an asymmetric bright emission ring with a diameter of 42 +/- 3 mu as, which is circular and encompasses a central depression in brightness with a flux ratio greater than or similar to 10: 1. The emission ring is recovered using different calibration and imaging schemes, with its diameter and width remaining stable over four different observations carried out in different days. Overall, the observed image is consistent with expectations for the shadow of a Kerr black hole as predicted by general relativity. The asymmetry in brightness in the ring can be explained in terms of relativistic beaming of the emission from a plasma rotating close to the speed of light around a black hole. We compare our images to an extensive library of ray-traced general-relativistic magnetohydrodynamic simulations of black holes and derive a central mass of M = (6.5 +/- 0.7) x 10(9) M-circle dot. Our radio-wave observations thus provide powerful evidence for the presence of supermassive black holes in centers of galaxies and as the central engines of active galactic nuclei. They also present a new tool to explore gravity in its most extreme limit and on a mass scale that was so far not accessible.

2,589 citations

Journal ArticleDOI
TL;DR: The third generation of the Sloan Digital Sky Survey (SDSS-III) took data from 2008 to 2014 using the original SDSS wide-field imager, the original and an upgraded multi-object fiber-fed optical spectrograph, a new near-infrared high-resolution spectrogram, and a novel optical interferometer.
Abstract: The third generation of the Sloan Digital Sky Survey (SDSS-III) took data from 2008 to 2014 using the original SDSS wide-field imager, the original and an upgraded multi-object fiber-fed optical spectrograph, a new near-infrared high-resolution spectrograph, and a novel optical interferometer. All the data from SDSS-III are now made public. In particular, this paper describes Data Release 11 (DR11) including all data acquired through 2013 July, and Data Release 12 (DR12) adding data acquired through 2014 July (including all data included in previous data releases), marking the end of SDSS-III observing. Relative to our previous public release (DR10), DR12 adds one million new spectra of galaxies and quasars from the Baryon Oscillation Spectroscopic Survey (BOSS) over an additional 3000 sq. deg of sky, more than triples the number of H-band spectra of stars as part of the Apache Point Observatory (APO) Galactic Evolution Experiment (APOGEE), and includes repeated accurate radial velocity measurements of 5500 stars from the Multi-Object APO Radial Velocity Exoplanet Large-area Survey (MARVELS). The APOGEE outputs now include measured abundances of 15 different elements for each star. In total, SDSS-III added 2350 sq. deg of ugriz imaging; 155,520 spectra of 138,099 stars as part of the Sloan Exploration of Galactic Understanding and Evolution 2 (SEGUE-2) survey; 2,497,484 BOSS spectra of 1,372,737 galaxies, 294,512 quasars, and 247,216 stars over 9376 sq. deg; 618,080 APOGEE spectra of 156,593 stars; and 197,040 MARVELS spectra of 5,513 stars. Since its first light in 1998, SDSS has imaged over 1/3 of the Celestial sphere in five bands and obtained over five million astronomical spectra.

2,471 citations

01 Jan 2005
TL;DR: The Monthly Notices as mentioned in this paper is one of the three largest general primary astronomical research publications in the world, published by the Royal Astronomical Society (RAE), and it is the most widely cited journal in astronomy.
Abstract: Monthly Notices is one of the three largest general primary astronomical research publications. It is an international journal, published by the Royal Astronomical Society. This article 1 describes its publication policy and practice.

2,091 citations