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LOFAR and APERTIF Surveys of the radio sky: probing shocks and magnetic fields in galaxy clusters

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  • Institute of Astrophysics and Space Sciences & University of Lisbon

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At very low frequencies, the new pan-European radio telescope LOFAR is opening the last unexplored window of the electromagnetic spectrum for astrophysical studies. The revolutionary APERTIFphased arrays that are about to be installed on the Westerbork radio telescope (WSRT) will dramatically increase the survey speed for the WSRT. Combined surveys with these two facilities will deeply chart the northern sky over almost two decades in radio frequency from $sim$15 up to 1400 MHz. Here we briefly describe some of the capabilities of these new facilities and what radio surveys are planned to study fun-damental issues related to the formation and evolution of galaxies and clusters of galaxies. In the second part we briefly review some recent observational results directly showing that diffuse radio emission in clusters traces shocks due to cluster mergers. As these diffuse radio sources are relatively bright at low frequencies, LOFAR should be able to detect thousands of such sources up to the epoch of cluster formation. This will allow addressing many question about the origin and evolution of shocks and magnetic fields in clusters. At the end we briefly review some of the first and very preliminary LOFAR results on clusters.
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J. Astrophys. Astr. (xxxx) xx, 000–000
LOFAR and APERTIF surveys of the radio sky:
probing shocks and magnetic fields in galaxy
clusters
Huub ottgering
1
,Jose Afonso
2
,Peter Barthel
3
,
Fabien Batejat
4
,Philip Best
5
,Annalisa Bonafede
6
,
Marcus Br¨uggen
6
,Gianfranco Brunetti
7
,Krzysztof Chy˙zy
8
,
John Conway
9
,Francesco De Gasperin
10
,Chiara Ferrari
11
,
Marijke Haverkorn
1,12,17
,George Heald
12
,Matthias Hoeft
13
,
Neal Jackson
14
,Matt Jarvis
15
,Louise Ker
5
,
Matt Lehnert
16
,Giulia Macario
7
,John McKean
12
,
George Miley
1
,Raffaella Morganti
3,12
,Tom Oosterloo
3,12
,
Emanuela Orr`u
17
,Roberto Pizzo
12
,David Rafferty
1
,
Alexander Shulevski
3
,Cyril Tasse
16
,Ilse van Bemmel
12
,
Bas van der Tol
1
,Reinout van Weeren
1
,Marc Verheijen
3
,
Glenn White
18
, Michael Wise
12
, on behalf of the LOFAR collaboration
1
Leiden Observatory, Leiden University, PO Box 9513, 2300 RA Leiden, The Netherlands
2
Observat´orio Astron´omico de Lisboa, Faculdade de Ciˆencias,
Universidade de Lisboa, Tapada da Ajuda, 1349-018 Lisbon, Portugal
3
Kapteyn Instituut, Landleven 12, 9747 AD Groningen, The Netherlands
4
Chalmers University of Technology, Onsala Space Observatory, SE 439 92 Onsala, Sweden
5
Royal Observatory, Blackford Hill, Edinburgh EH9 3HJ, UK
6
Jacobs University Bremen, Campus Ring 1, 28759 Bremen, Germany
7
INAF, Istituto di Radioastronomia, Via P Gobetti 101, IT 40129, Bologna, Italy
8
Jagiellonian University, ul. Orla 171 30-244 Krak´ow POLAND
9
Chalmers University of Technology, Onsala Space Observatory, SE 439 92 Onsala, Sweden
10
Max-Planck-Institut f¨ur Astrophysik, Karl-Schwarzschildstraße 1, 85741 Garching, Germany
11
UNS, CNRS UMR 6202 Cassiop´ee, Observatoire de la Cote d’Azur, Nice, France
12
ASTRON, PO Box 2, 7990 AA Dwingeloo, The Netherlands
13
Th¨uringer Landessternwarte, Tautenburg
14
Jodrell Bank Centre for Astrophysics, University of Manchester,
Turing Building, Oxford Road, Manchester M13 9PL, UK
15
Centre for Astrophysics, University of Hertfordshire, Hatfield, Herts, UK
16
Observatoire de Paris, 5 Place Jules Janssen, 92195 Meudon, France
17
Radboud University Nijmegen, Heijendaalseweg 135, 6525 AJ Nijmegen, The Netherlands
18
Department of Physics and Astronomy, The Open University, Milton Keynes, MK7 6AA,
Space Science and Technology Department,
STFC Rutherford Appleton Laboratory, Chilton, OX11 0QX, UK
Received xxx; accepted xxx
1
arXiv:1107.1606v1 [astro-ph.CO] 8 Jul 2011
2 Huub ottgering
Abstract. At very low frequencies, the new pan-European
radio telescope LOFAR is opening the last unexplored window
of the electromagnetic spectrum for astrophysical studies. The
revolutionary APERTIF phased arrays that are about to be in-
stalled on the Westerbork radio telescope (WSRT) will dramati-
cally increase the survey speed for the WSRT. Combined surveys
with these two facilities will deeply chart the northern sky over
almost two decades in radio frequency from 15 up to 1400
MHz. Here we briefly describe some of the capabilities of these
new facilities and what radio surveys are planned to study fun-
damental issues related the formation and evolution of galaxies
and clusters of galaxies. In the second part we briefly review
some recent observational results directly showing that diffuse
radio emission in clusters traces shocks due to cluster mergers.
As these diffuse radio sources are relatively bright at low frequen-
cies, LOFAR should be able to detect thousands of such sources
up to the epoch of cluster formation. This will allow address-
ing many question about the origin and evolution of shocks and
magnetic fields in clusters. At the end we briefly review some of
the first and very preliminary LOFAR results on clusters.
Key words: Galaxies: clusters: general, intracluster medium;
Radio continuum: galaxies; Radio telescopes
1. Introduction
At low frequencies, the new pan-European radio telescope LOFAR is opening
the last unexplored window of the electromagnetic spectrum for astrophys-
ical studies. The revolutionary APERTIF phased arrays that are about to
be installed on the Westerbork radio telescope (WSRT) will dramatically
increase the survey speed for the WSRT. The resulting vast area of new ob-
servational parameter space will be fully exploited for many studies directly
related to the formation of massive black holes, galaxies, and clusters. Par-
ticularly important are three research areas that are driving the design of
several surveys that are planned to be carried out with these new facilities.
These areas are: (i) forming massive galaxies at the epoch of reionisation, (ii)
magnetic fields and shocked hot gas associated with the first bound clusters
of galaxies, and (iii) star formation processes in distant galaxies. Further-
more, a most exciting aspect of LOFAR is that its enormous instantaneous
field of view coupled with its unprecedented sensitivity at low frequencies
e-mail:rottgering@strw.leidenuniv.nl
Northern radio surveys and shocks and magnetic fields in clusters 3
equips LOFAR for the discovery of new classes of rare extreme-spectrum
sources.
In this contribution, we will first briefly describe LOFAR and APERTIF.
For a more extended description of LOFAR we refer to the contribution of
George Heald that extensively describes LOFAR and the way the data will
be handled to form deep images at low frequencies. Second, we will discuss
how the prime science drivers led to the definition of the planned contin-
uum surveys with LOFAR and APERTIF. Third, we briefly review some
of the work we have been carrying out to understand diffuse radio emis-
sion associated with merging clusters. We will mainly concentrate on some
of the statistical results obtained for a partly new sample of relics showing
correlations between their sizes, spectral indices and distances from the clus-
ters centres. In the contribution of Reinout van Weeren, he will high-light
recent results for newly discovered individual relics, including the recently
discovered spectacular double relics in the cluster CIZA J2252.8+5301 (van
Weeren et al. 2010). Finally, a few preliminary results from LOFAR obser-
vations mainly related to clusters are briefly presented. These results show
the enormous potential that LOFAR has for studying shocks and magnetic
fields in clusters.
2. LOFAR
LOFAR, the Low Frequency Radio Array, is a pan-European radio telescope
that is currently being commissioned. Its revolutionary design makes use of
phased array technology. This replaces the traditional and expensive me-
chanical dishes by a combination of simple receivers and modern computing
equipment. LOFAR has two types of antennas, one optimised for the 30 - 80
MHz range and one for the 110 - 240 MHz range. The antennas are grouped
together in stations the size of soccer fields. The signals from the antennas
will be digitised so that many beams on the sky can be formed. This makes
LOFAR an extremely efficient instrument to survey large areas of sky. The
Dutch part of the array will be finished in 2011 and will comprise 40 stations
distributed over an area of diameter of 100 km. In addition, in 2011 eight
stations in a number of European countries (Germany, UK, Sweden, and
France) are planned to be operational. Currently many functional elements
of the LOFAR imaging system are in place. These elements include: (i) sta-
tion beam formation, (ii) high speed data transport, (iii) software correlator
to produce visibilities, (iv) calibration algorithms, and (v) wide field map
making. Although a significant amount of both continued commissioning
and technical research will be needed to obtain maps with the theoretical
noise levels, the maps that are currently produced already are the deepest
ever at these low frequencies.
4 Huub ottgering
With its unique design, LOFAR will provide enormous improvements
over previous facilities in the following three regions of parameter space:
Very Low Frequencies, with 2 - 3 orders of magnitude improvement in
both sensitivity and angular resolution. This is a mostly unexplored
spectral region that is uniquely sensitive to ultra-steep spectrum z > 6
radio galaxies, diffuse emission from clusters and the oldest ‘fossil’
synchrotron electrons.
Size of the Instantaneous Field of View, of many tens of square de-
grees. This will deliver a transformational increase in speed to survey
the radio sky, crucially important for the quest for rare objects such
as distant clusters, proto-clusters and z > 6 radio galaxies and rare
transient phenomena.
Low-Frequency Radio Spectroscopy, enabling studies of redshifted neu-
tral hydrogen at the Epoch of Reionisation.
The design of LOFAR is very versatile and has led to the development of 6
key science projects, related to cosmic rays, epoch of reionisation, transients
and pulsars, cosmic magnetism, the Sun, and extragalactic surveys. In this
contribution, we will focus on LOFAR and APERTIF surveys to probe the
extragalactic sky.
3. APERTIF
APERTIF, the new Phased Array Feed receiver system for the Westerbork
Synthesis Radio Telescope (WSRT) will dramatically enlarge the instanta-
neous Field-of-View of the WSRT (see Oosterloo et al 2010 for a detailed
description). This is done by replacing the current single Frontend Feeds
with Phased Array Feeds (PAFS). Each of the PAFs consists of 121 Vivaldi
elements and will detect the radiation field (in dual polarisation) in the focal
plane of each dish over an area of about one square meter. Because of this,
many beams can be formed simultaneously for each dish making it possible
to image an area of about 8 square degree on the sky, which is an increase
of about a factor 30 compared to the current WSRT. Its large 300 MHz
bandwidth will not only cater for sensitive continuum imaging, but is also
crucial for efficient HI and OH emission surveys and for studies of polarised
emission from large areas.
4. Transformational radio surveys
4.1 LOFAR
The three fundamental areas of astrophysics that have driven the design of
the planned LOFAR surveys are: (i) forming massive galaxies at the epoch
Northern radio surveys and shocks and magnetic fields in clusters 5
of reionisation, (ii) magnetic fields and shocked hot gas associated with the
first bound clusters of galaxies, and (iii) star formation processes in distant
galaxies. The areas, depths and frequencies of the surveys have been chosen
so that they would contain: (i) 100 powerful radio galaxies close to or at
the epoch of reionisation, (ii) 100 radio halos at the epoch when the first
massive bound galaxy clusters appeared, and (iii) 100 proto-clusters. The
resulting survey parameters are based on estimates of luminosity functions
for powerful radio galaxies by Wilman et al. 2008, for radio halos by Enßlin &
ottgering 2002 and Cassano et al. 2010, and for proto-clusters by Venemans
et al. 2007. To achieve the goals of the LOFAR surveys, a three-tiered
approach has been adopted (for details see ottgering et al. 2010). Tier-1
represents the all sky survey at frequencies 15, 30, 60 and 120 MHz. Tier-
2 are the medium deep surveys over 1000 sqr deg at 30, 60, 120 and 200
MHz, while Tier-3 encompasses about 100 sqr degrees down to an extreme
depth of 6 µJy rms at 150 MHz. The resulting depth versus frequency is
given in Fig. 1. In addition, very deep data will be taken on a selected
sample of 60 nearby clusters. Another important motivation of LOFAR
is to provide the entire international astronomical community with unique
surveys of the radio sky that have a long-lasting legacy value for a broad
range of astrophysical research. The international LOFAR survey team has
identified a range of fundamental astrophysical research topics on which
LOFAR surveys will have an important impact. These topics include (i)
the formation and evolution of large scale structure of the Universe, (ii)
the physics of the origin, evolution and end-stages of radio sources, (iii) the
magnetic field and interstellar medium in nearby galaxies, and (iv) Galactic
sources such as supernova remnants, HII regions, exoplanets and pulsars.
4.2 WODAN
The extremely large field of view of APERTIF would enable the WODAN
(Westerbork Observations of the Deep APERTIF Northern-Sky) project.
This project aims to chart the entire accessible northern sky at 1400 MHz
down to 10 µJy rms and about 1000 deg
2
down to 5 µJy. WODAN will be
an important compliment to the EMU (Evolutionary Map of the Universe)
project. EMU will use the phased-array feed (PAF) mounted on the Aus-
tralian SKA Pathfinder (ASKAP, De-boer et al. 2009) to chart the entire sky
south of δ = 30
to a similar depth as WODAN. For a detailed description
of EMU we will refer to the contribution of Ray Norris to this conference.
WODAN and EMU have an enormous synergy with the LOFAR surveys:
virtually all the 5 × 10
7
radio sources from the LOFAR all sky surveys will
have their flux density at 1400 MHz measured. It will yield radio data
for all radio loud AGN, and most luminous starbursts up to z = 2. The
resulting densely populated radio color-color diagrams will be a powerful
tool to spectrally discriminate between very rare radio sources with extreme
6 Huub ottgering
Figure 1. Flux limits (5 sigma) of the proposed LOFAR and APERTIF surveys
compared to other existing radio surveys. The triangle represent existing surveys:
HDF (VLA Richards et al. 2000; WSRT Garrett et al. 2000), WENSS, NVSS, 6C,
VLSS and 8C. The lines represent different power-laws (S ν
α
, with α = 1.6
and 0.8) to illustrate how, depending on the spectral indices of the sources, the
LOFAR surveys will compare to other surveys.
radio spectra such as diffuse emission from clusters and very distant radio
galaxies. For nearby resolved sources it will instantly yield spectral index
and spectral curvature maps, a very rich source of information to constrain
many physical parameters. As the combined surveys will cover the entire sky,
measurements of the Integrated Sachs-Wolfe effect, galaxy auto-correlation
functions and cosmic magnification will significantly tighten cosmological
model parameters (Raccanelli et al. submitted).
5. LOFAR and diffuse radio emission from clusters of galax-
ies
Clusters of galaxies are large ensembles of hundreds of galaxies embedded in
hot gas and held together by gravity. Besides the hot thermal gas observed
in X-rays, the intra-cluster-medium (ICM) contains relativistic electrons (E
Gev) and magnetic fields (1 10µG), which have been detected via syn-
chrotron emission in the radio band. LOFAR is uniquely suited to probe
Northern radio surveys and shocks and magnetic fields in clusters 7
these synchrotron emitting regions and will address many questions related
to the large-scale magnetic fields and relativistic particles mixed with the
thermal ICM. These questions include: What are the strengths and topolo-
gies of the magnetic fields? When and how were the first magnetic fields gen-
erated? How were magnetic fields subsequently amplified and maintained?
Furthermore, diffuse radio sources in galaxy clusters are likely to be di-
rect signatures of huge shock waves caused by massive cluster mergers. These
shocks have a crucial impact on the energetics and detailed temperature dis-
tribution of the cluster gas. LOFAR observations are therefore very relevant
for studies of the evolution of the energy content of both the thermal and
non-thermal gas in the cluster. Some of the most prominent nearby clusters
of galaxies host such diffuse synchrotron emitting radio sources. Classical
examples of spectacularly large ( 1 Mpc) diffuse cluster emission have
been found for the Coma cluster, Abell 2256 and Abell 3667. The proper-
ties of the associated clusters are extreme: they are very X-ray luminous,
have high temperatures (kT > 7 keV), large masses (> 10
15
M
), and high
galaxy velocity dispersions. The overall properties are indicative of the vio-
lent merging of sub-clusters, an important process in the assembly of massive
clusters. Diffuse radio emission associated with clusters of galaxies has been
classified into three groups: relics, halos and phoenixes (e.g. Giovannini &
Feretti 2004).
Cluster relics are large elongated diffuse structures at the periphery of
clusters. Recently we have discovered a spectacularly long and narrow relic
with a size of 2.0 Mpc × 50 kpc, located at a distance of 1 Mpc from the
centre of the merging cluster CIZA J2242.8+5301 (van Weeren et al. 2010).
The relic displays highly aligned magnetic fields and a strong spectral index
gradient due to cooling of the synchrotron emitting particles in the post
shock region. We have argued that these observations provide conclusive
evidence that shocks in merging clusters produce extremely energetic cosmic
rays. Detailed modelling of the morphology, polarization properties and
variations of the radio spectrum, allowed us to determine the strength of
the magnetic field (5 µG) and the Mach number (4.6
+1.3
0.9
) of the shock. Our
numerical simulations indicated that the impact parameter of the cluster
collision was about zero and the mass ratio of the colliding clusters was
roughly 2:1 (van Weeren et al. in prep.).
Cluster radio halos are located at the centres of clusters, their diffuse
morphologies following that of the X-ray emission. The origin of the halos
is not understood. Especially their enormous 1 Mpc sizes pose problems.
The radiative lifetimes of the synchrotron emitting electrons are so short
that the electrons need to have been accelerated to relativistic speeds close
to the place where they radiate. Although many explanations have been put
forward, a currently favoured one is that turbulence due to cluster mergers
is capable of accelerating electrons to relativistic speeds (e.g. Brunetti et al.
2001). Alternatively, relative electrons could be produced when relativistic
8 Huub ottgering
protons from AGNs in the cluster collide with thermal protons within the
cluster gas (Dennison, 1980). A second important issue relates to the origin
of the magnetic fields (e.g. Dolag 2006). Are they primordial in origin and
have turbulent processes subsequently amplified the fields? Or have outflows
from active galaxies or starburst galaxies transported magnetic fields into
the inter-galactic medium?
Radio phoenixes are suggested to be due to shocks in the cluster gas
that would adiabatically compress old radio plasma ejected by former active
galaxies. The resulting diffuse objects would have an extremely steep radio
spectrum making them relatively bright at low radio frequencies (Enßlin and
Kopal-Krishna 2001). Simply considering the timescales related to the AGN
activity, synchrotron losses, and the presence of shocks we recently argued
that such sources could determine the general appearance of clusters in low
frequency LOFAR maps (van Weeren, et al. 2009a).
Because these radio sources associated with cluster wide shocks are dif-
fuse, have low luminosities and steep radio spectra, they are difficult to
detect with conventional radio observatories, such as Westerbork. As a re-
sult there are only about 50 cluster radio sources currently known. Due to
its extreme sensitivity at low radio frequencies, LOFAR will be the break-
through instrument for this field of research (Cassano et al. 2010). For the
first time, the occurrence and characteristics of diffuse cluster radio sources
will be measured as a function of cluster properties up to the epoch at which
the first massive clusters assembled (z 1). This will directly show the ef-
fects of shock waves on the evolution of the cluster gas and magnetic fields,
and test predictions that cluster merging is rampant at high redshift. De-
tailed LOFAR maps of rotation measures, polarization properties and radio
spectra of nearby halos will distinguish between the various physical models
for the origin of the diffuse radio emission. It also will probe radio AGN
activity over long time scales, important for studies of the radio feedback
processes in clusters. With the LOFAR observations, we will address the
following questions:
What are the properties of the cluster-wide shocks (rate of occurrence,
volume filling, geometry, Mach numbers)? How do they accelerate
particles?
What are the characteristics of the magnetic fields (strength, topol-
ogy)? And how do these relate to models of the origin of the fields?
What is the total energy input into the cluster medium by radio loud
AGN?
What are the properties of the merging clusters (mass ratios, impact
parameters) as can be directly deduced by the relic morphologies?
How do the properties of merging clusters evolve over cosmic time?
Northern radio surveys and shocks and magnetic fields in clusters 9
6. Towards a sample of relics, a prelude to LOFAR
As discussed, detailed radio observations of individual relics clearly suggest
that relics originate in shocks induced by merging clusters. This scenario
can be further tested by studying larger samples of relics. From GMRT,
WSRT and VLA observations of a sample of diffuse radio sources from the
74 MHz VLSS survey with spectral indices α < 1.7, 5 new relics were
discovered. A comparison of the NVSS and WENSS radio catalogues with
the ROSAT all sky catalogue, 5 additional relics were found. Combined
with 17 known relics from the literature, the resulting sample was large
enough for a statistical study. For details we refer to van Weeren et al.
2009b. For this sample, we found that larger relics are mostly located in the
cluster periphery, while smaller relics are found closer to the cluster center.
We also discovered an anti-correlation between the steepness of the spectral
index and the physical size of the relics. A likely explanation for these two
correlations is that the larger shock waves occur mainly in lower-density
regions. The larger shocks then have larger Mach numbers translating into
flatter radio spectra. As larger relics are also more luminous, this then also
explains that within this sample the more luminous radio relics have flatter
spectral indices. Finally, there is a tendency for the steep spectrum relics
to show more spectral curvature. This would provide evidence for spectral
ageing due to inverse compton and/or synchrotron losses. We note however
that some of the smallest relics might be due to the compression of fossil
AGN radio plasma. Their very steep and curved spectrum sources are also
consistent with this scenario.
6.1 LOFAR and cluster observations: the rich cluster of galaxies Abell 2256
Abell 2256 is a rich X-ray cluster at z = 0.058 that has undergone a merging
event estimated to have happened 0.3 Gyr ago (e.g. Miller et al 2003). Apart
from 9 tailed sources, it rather exceptionally contains three classes of diffuse
cluster radio sources: relics, halos and phoenixes. The northern relics have
been discovered a long time ago (Bridle and Fomalon 1976) and were studied
in detail by Clarke and Enßlin (2006). They also clearly showed that A2256
possesses a central halo with a luminosity following the X-ray - radio halo
luminosity relation (Liang et al. 2000). In very deep 325 MHz GMRT radio
maps van Weeren et al. (2009a) recently discovered three diffuse elongated
radio sources with extremely steep spectral indices located about 1 Mpc
from the cluster center. These properties indicate that these objects can be
classified as phoenixes.
As A2256 is one of the most luminous radio emitting clusters showing
so many intriguing characteristics, it was one of the prime candidates to be
observed during early commissioning of LOFAR (see also ottgering et al.
2010; Heald et al. 2010). It was observed in the HBA band in May 2010
10 Huub ottgering
for about 8 hours. The data were taken with 10 core stations and 5 remote
stations and the observed frequencies ranged from 115 to 165 MHz. An
image from 18 subbands covering a total of 4 MHz of bandwidth around 135
MHz was made (see Figure 2). The resolution of the image is 31 × 19 arcsec
and the noise is 5 mJy/beam. So far, the deepest images at low frequencies
have been obtained with the GMRT at 150 MHz (Intema 2009, Intema et
al. submitted, Kale and Dwarakanath 2010). The GMRT image clearly
shows the relic and several of the head tail galaxies that are also visible
on the LOFAR image. The GMRT image recovers the central part of the
halo emission. With LOFAR’s very sensitive central core, the full extent of
the halo is visible, showing LOFAR’s power to study diffuse steep spectrum
emission from clusters. Next steps in improving this image are reducing the
data from all the 256 sub-bands, and the application of more sophisticated
data reduction algorithms. These include proper wide-field imaging taking
the varying station beams into account, iteration of self-calibration/peeling
loops, and removal of ionospheric corrections following the “SPAM” method
(Intema et al. 2009). Finally, recently we have observed A2256 in the
lowband and produced images at 20, 30 and 49 MHz. A spectral map from a
combination of 49 MHz and the 350 MHz WSRT data (Brentjens et al. 2008)
very nicely spatially resolved the extremely streep spectrum central radio
halo from the flatter spectrum northern relics. We also recently obtained
data on Coma A and A2255. The commissioning team is working very hard
to obtain excellent images.
Acknowledgements C. Ferrari acknowledges financial support by the Agence
Nationale de la Recherche through grant ANR-09-JCJC-0001-01.
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... These limits are also far brighter than the astrometric magnitude limit of < 20 − 21 in both cases. Similarly, although the exquisite low-frequency continuum sensitivity of the LOFAR Surveys Key Science Project (Röttgering et al. 2011) observations in the LOFAR two-metre sky survey (LoTSS; e.g. Shimwell et al. 2017Shimwell et al. , 2019Shimwell et al. , 2022Tasse et al. 2021) enables the detection of extremely faint radio sources, the redshift (i.e. ...
... Since its inception, an important driver for LOFAR has been to carry out a series of surveys of the sky at low radio frequencies, in particular to advance our understanding of the formation and evolution of galaxies, galaxy clusters, and active galactic nuclei (AGN). The LOFAR Surveys Key Science Project (LSKSP; Röttgering et al. 2011) is carrying out this aim, using a suite of related surveys. ...
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WEAVE, the new wide-field, massively multiplexed spectroscopic survey facility for the William Herschel Telescope, will see first light in late 2022. WEAVE comprises a new 2-degree field-of-view prime-focus corrector system, a nearly 1000-multiplex fibre positioner, 20 individually deployable 'mini' integral field units (IFUs), and a single large IFU. These fibre systems feed a dual-beam spectrograph covering the wavelength range 366$-$959\,nm at $R\sim5000$, or two shorter ranges at $R\sim20\,000$. After summarising the design and implementation of WEAVE and its data systems, we present the organisation, science drivers and design of a five- to seven-year programme of eight individual surveys to: (i) study our Galaxy's origins by completing Gaia's phase-space information, providing metallicities to its limiting magnitude for $\sim$3 million stars and detailed abundances for $\sim1.5$ million brighter field and open-cluster stars; (ii) survey $\sim0.4$ million Galactic-plane OBA stars, young stellar objects and nearby gas to understand the evolution of young stars and their environments; (iii) perform an extensive spectral survey of white dwarfs; (iv) survey $\sim400$ neutral-hydrogen-selected galaxies with the IFUs; (v) study properties and kinematics of stellar populations and ionised gas in $z<0.5$ cluster galaxies; (vi) survey stellar populations and kinematics in $\sim25\,000$ field galaxies at $0.3\lesssim z \lesssim 0.7$; (vii) study the cosmic evolution of accretion and star formation using $>1$ million spectra of LOFAR-selected radio sources; (viii) trace structures using intergalactic/circumgalactic gas at $z>2$. Finally, we describe the WEAVE Operational Rehearsals using the WEAVE Simulator.
... Particularly, lowfrequency radio telescopes such as the Low Frequency Array (LOFAR, van Haarlem et al. 2013) open a new observational spectral window to study the evolution of quasar activity. The LOFAR Surveys Key Science Project (LSKSP, Röttgering et al. 2011) aims to map the entire Northern Sky down to 100 µJy, while for extragalatic fields, greater than a few square degrees in size and with extensive multiwavelength data, the target rms noise is of a few tens of µ Jy. In this paper, we investigate the evolution of the luminosity function of RSQs. ...
... Our work demonstrates the feasibility of studying the evolution of RSQs using samples of quasars compiled with ML algorithms trained with optical and infrared photome-try combined with LOFAR data. Future studies of the luminosity function of RSQs will benefit from the advent of the new generation of wide-field radio (LOTSS: Röttgering et al. 2011;Shimwell et al. 2017Shimwell et al. , 2019EMU: Norris et al. 2011), optical (LSST: Tyson 2002LSST Science Collaboration et al. 2009;DES: Flaugher 2005), infrared (WFIRST: Spergel et al. 2013;Euclid: Laureijs et al. 2011), and spectroscopic surveys (EBOSS: Dawson et al. 2016;DESI: DESI Collaboration et al. 2016). ...
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We present an estimate of the optical luminosity function (OLF) of LOFAR radio-selected quasars (RSQs) at $1.4<z<5.0$ in the $9.3\:\textrm{deg}^{2}$ NOAO Deep Wide-field survey (NDWFS) of the Bo\"otes field. The selection was based on optical/mid-ir photometry used to train three different machine learning (ML) algorithms. Objects taken as quasars by the ML algorithms are required to be detected at $5\sigma$ significance in deep radio maps to be classified as candidate quasars. The optical imaging came from the SDSS and the PS1 $3\pi$ survey; mid-ir photometry was taken from the SDWFS survey; and radio data was obtained from deep LOFAR imaging of the NDWFS-Bo\"otes field. The requirement of a $5\sigma$ LOFAR detection allowed us to reduce the stellar contamination in our sample by two orders of magnitude. The sample comprises 134 objects, including both photometrically selected candidate quasars (47) and spectroscopically confirmed quasars (83). The depth of our LOFAR observations allowed us to detect the radio-emission of quasars that would be otherwise classified as radio-quiet. Around $65\%$ of the quasars in the sample are fainter than $M_{\textrm{1450}}<-24.0$, a regime where the OLF of quasars selected through their radio emission, has not been investigated in detail. It has been demonstrated that in cases where mid-ir wedge-based AGN selection is not possible due to a lack of appropriate data, the selection of quasars using ML algorithms trained with optical/mid-ir photometry in combination with LOFAR data provides an excellent approach for obtaining samples of quasars. We demonstrate that RSQs show an evolution similar to the exhibited by faint quasars $(M_{\textrm{1450}}<-22.0)$. Finally, we find that RSQs may compose up to $\sim20\%$ of the whole faint quasar population (radio-detected plus radio-undetected).
... The LOFAR two-metre Sky Survey has published two data releases (LoTSS DR1, DR2; [471]), and there is the additional LOFAR Low-Band Antenna (LBA) Sky Survey (LoLSS; [466]), which aims to cover the entire northern sky and providing ultra-low-frequency information for ∼ 10 5 radio sources. In the future, there are plans for an evolutionary map of the Universe (EMU; [472]) that will almost cover the whole southern sky, the precursor of which is the EMU pilot [473] which released data 2022, as well as the Westerbork Observations of the Deep Apertif Northern Sky Survey (WODAN; [474]), which covers the northern sky. Together they will cover the whole sky, thus aiding large-scale structure studies. ...
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The current standard cosmological model is constructed within the framework of general relativity with a cosmological constant Λ, which is often associated with dark energy, and phenomenologically explains the accelerated cosmic expansion. Understanding the nature of dark energy is one of the most appealing questions in achieving a self-consistent physical model at cosmological scales. Modification of general relativity could potentially provide a more natural and physical solution to the accelerated expansion. The growth of the cosmic structure is sensitive in constraining gravity models. In this paper, we aim to provide a concise introductory review of modified gravity models from an observational point of view. We will discuss various mainstream cosmological observables, and their potential advantages and limitations as probes of gravity models.
... Carilli & Rawlings 2004;Dewdney et al. 2009), radio observations are undergoing an explosion of capabilities, including huge increases in survey speed, spatial resolution and sensitivity. The Low Fre-quency Array (LOFAR; van Haarlem et al. 2013) is already revolutionising our understanding of the low-frequency radio sky, and the LOFAR Surveys Key Science Project (LSKSP; Röttgering et al. 2011) aims to survey the entire northern sky with an unprecedented combination of sensitivity and angular resolution. Huge progress has already been made; the first data release of the LOFAR Two-metre Sky Survey (LoTSS: Shimwell et al. 2017Shimwell et al. , 2019Duncan et al. 2019;Williams et al. 2019) covered an area of 424 deg 2 with a median sensitivity of 71 µJy at 150 MHz and with 6 arcsec resolution, while the forthcoming second data re-Article number, page 1 of 17 arXiv:2011.08196v1 ...
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In this paper, we investigate the relationship between 150MHz luminosity and star formation rate (the SFR-L150 relation) using 150MHz measurements for a near-infrared selected sample of 118,517 $z<1$ galaxies. New radio survey data offer compelling advantages for studying star formation in galaxies, with huge increases in sensitivity, survey speed and resolution over previous generation surveys, and remaining impervious to extinction. The LOFAR Surveys Key Science Project is transforming our understanding of the low-frequency radio sky, with the 150MHz data over the ELAIS-N1 field reaching an RMS sensitivity of 20uJy/beam over 10 deg$^2$ at 6" resolution. All of the galaxies studied have SFR and stellar mass estimates derived from energy balance SED fitting, using redshifts and aperture-matched forced photometry from the LOFAR Two-metre Sky Survey (LoTSS) deep fields data release. The impact of active galactic nuclei is minimised by leveraging the deep ancillary data alongside outlier-resistant median-likelihood methods. We find a linear and non-evolving SFR-L150 relation, apparently consistent with expectations based on calorimetric arguments, down to the lowest SFRs. However, we also recover compelling evidence for stellar mass dependence in line with previous work on this topic, in the sense that higher mass galaxies have a larger 150MHz luminosity at a given SFR, suggesting that the overall agreement with calorimetric arguments may be a coincidence. We conclude that in the absence of AGN, 150MHz observations can be used to measure accurate galaxy SFRs out to $z=1$ at least, but it is necessary to account for stellar mass in order to obtain 150MHz-derived SFRs accurate to <0.5 dex. Our best-fit relation is $\log_{10} (L_\mathrm{150 MHz} / W\,Hz^{-1}) = (0.90\pm 0.01) \log_{10}(\psi/M_\odot\,\mathrm{yr}^{-1}) + (0.33 \pm 0.04) \log_{10} (M/10^{10}M_\odot) + 22.22 \pm 0.02$. (Abridged)
... VLASS, combined with radio observations at other frequencies and infrared observations, will provide an expanded sample of H II regions and PNe throughout 75% of the Galactic disk, allowing a fuller census of these phenomena. (Gaensler et al. 2010)); the Westerbork Synthesis Radio Telescope (WSRT/Apertif; in particular the WODAN survey, Röttgering et al. 2011), and the ongoing LoFAR Two Metre Sky Survey (Shimwell et al. 2017), leading to Phase 1 science operations of the SKA that will commence in the late 2020 s. Each of these facilities includes dedicated surveys at ≈1.4 GHz as a prime component of their science programs (Norris 2017). ...
... With the advent of the LOw Frequency ARray (LOFAR; Röttgering et al. 2011;van Haarlem et al. 2013) which combines a large field of view with high sensitivity on both small and large angular scales, we can now study the FIRC at lower frequencies where the contribution from thermal free-free emission is even less important than at 1.4 GHz. Operating between 30 and 230 MHz, LOFAR offers complementary information to the wealth of data collected at higher frequencies. ...
Preprint
Aims. We aim to study the far-infrared radio correlation (FIRC) at 150 MHz in the local Universe (at a median redshift z~0:05) and improve the use of the rest-frame 150-MHz luminosity, L150, as a star-formation rate (SFR) tracer, which is unaffected by dust extinction. Methods. We cross-match the 60-um selected Revised IRAS Faint Source Survey Redshift (RIFSCz) catalogue and the 150-MHz selected LOFAR value-added source catalogue in the Hobby-Eberly Telescope Dark Energy Experiment (HETDEX) Spring Field. We estimate L150 for the cross-matched sources and compare it with the total infrared (IR) luminosity, LIR, and various SFR tracers. Results. We find a tight linear correlation between log L150 and log LIR for star-forming galaxies, with a slope of 1.37. The median qIR value (defined as the logarithm of the LIR to L150 ratio) and its rms scatter of our main sample are 2.14 and 0.34, respectively. We also find that log L150 correlates tightly with the logarithm of SFR derived from three different tracers, i.e., SFR_Halpha based on the Halpha line luminosity, SFR_60 based on the rest-frame 60-um luminosity and SFR_IR based on LIR, with a scatter of 0.3 dex. Our best-fit relations between L150 and these SFR tracers are, log L150 (Lsun) = 1.35(0.06) x log SFR_Halpha (Msun/yr) + 3.20(0.06), log L150 (Lsun) = 1.31(0.05) x log SFR_60 (Msun/yr) + 3.14(0.06), and log L150 (Lsun) = 1.37(0.05) x log SFR_IR (Msun/yr) + 3.09(0.05), which show excellent agreement with each other.
... VLASS, combined with radio observations at other frequencies and infrared observations, will provide an expanded sample of H ii regions and PNe throughout 75% of the Galactic disk, allowing a fuller census of these phenomena. Röttgering et al. (2011)], and the ongoing LoFAR Two Metre Sky Survey (Shimwell et al. 2017), leading to Phase 1 science operations of the Square Kilometre Array (SKA) that will commence in the late 2020s. Each of these facilities includes dedicated surveys at ≈1.4 GHz as a prime component of their science programs (Norris 2017). ...
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The Very Large Array Sky Survey (VLASS) is a synoptic, all-sky radio sky survey with a unique combination of high angular resolution (≈2.5"), sensitivity (a 1σ goal of 70 μJy/beam in the coadded data), full linear Stokes polarimetry, time domain coverage, and wide bandwidth (2-4 GHz). The first observations began in September 2017, and observing for the survey will finish in 2024. VLASS will use approximately 5500 hours of time on the Karl G. Jansky Very Large Array (VLA) to cover the whole sky visible to the VLA (Declination > −40∘), a total of 33,885 deg^2. The data will be taken in three epochs to allow the discovery of variable and transient radio sources. The survey is designed to engage radio astronomy experts, multi-wavelength astronomers, and citizen scientists alike. By utilizing an "on the fly" interferometry mode, the observing overheads are much reduced compared to a conventional pointed survey. In this paper, we present the science case and observational strategy for the survey, and also results from early survey observations.
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WEAVE, the new wide-field, massively multiplexed spectroscopic survey facility for the William Herschel Telescope, will see first light in late 2022. WEAVE comprises a new 2-degree field-of-view prime-focus corrector system, a nearly 1000-multiplex fibre positioner, 20 individually deployable ‘mini’ integral field units (IFUs), and a single large IFU. These fibre systems feed a dual-beam spectrograph covering the wavelength range 366−959 nm at R ∼ 5000, or two shorter ranges at R ∼ 20 000. After summarising the design and implementation of WEAVE and its data systems, we present the organisation, science drivers and design of a five- to seven-year programme of eight individual surveys to: (i) study our Galaxy’s origins by completing Gaia’s phase-space information, providing metallicities to its limiting magnitude for ∼3 million stars and detailed abundances for ∼1.5 million brighter field and open-cluster stars; (ii) survey ∼0.4 million Galactic-plane OBA stars, young stellar objects and nearby gas to understand the evolution of young stars and their environments; (iii) perform an extensive spectral survey of white dwarfs; (iv) survey ∼400 neutral-hydrogen-selected galaxies with the IFUs; (v) study properties and kinematics of stellar populations and ionised gas in z < 0.5 cluster galaxies; (vi) survey stellar populations and kinematics in ∼25 000 field galaxies at 0.3 ≲ z ≲ 0.7; (vii) study the cosmic evolution of accretion and star formation using >1 million spectra of LOFAR-selected radio sources; (viii) trace structures using intergalactic/circumgalactic gas at z > 2. Finally, we describe the WEAVE Operational Rehearsals using the WEAVE Simulator.
Preprint
With the advent of new generation low-frequency telescopes, such as the LOw Frequency ARray (LOFAR), and improved calibration techniques, we have now started to unveil the sub GHz radio sky with unprecedented depth and sensitivity. The LOFAR Two Meter Sky Survey (LoTSS) is an ongoing project in which the whole northern radio sky will be observed at 150 MHz with a sensitivity better than 100 $\mu$Jy beam$^{-1}$ at a resolution of 6". Additionally, deeper observations are planned to cover smaller areas with higher sensitivity. The Lockman Hole, the Bo\"otes and the Elais-N1 regions are among the most well known northern extra-galactic fields, and the deepest of the LoTSS Deep Fields so far. We exploit these deep observations to derive the deepest radio source counts at 150 MHz to date. Our counts are in broad agreement with those from the literature, and show the well known upturn at $\leq$ few mJy, mainly associated with the emergence of the star-forming galaxy population. More interestingly, our counts show for the first time a very pronounced drop around S$\sim$2 mJy, which results in a prominent `bump' at sub-mJy flux densities. Such a feature was not observed in previous counts' determinations (neither at 150 MHz nor at higher frequency), and we believe this is the result of a careful analysis aimed at deblending confused sources and removing spurious sources and artifacts from the radio catalogues. This bump cannot be reproduced by any of the existing state-of-the-art evolutionary models and appears to be associated with a low-redshift population of galaxies and/or AGN.
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Aims. We aim to study the far-infrared radio correlation (FIRC) at 150 MHz in the local Universe (at a median redshift ⟨ z ⟩∼0.05) and improve the use of the rest-frame 150 MHz luminosity, L150 , as a star-formation rate (SFR) tracer, which is unaffected by dust extinction. Methods. We cross-match the 60 μ m selected Revised IRAS Faint Source Survey Redshift (RIFSCz) catalogue and the 150 MHz selected LOFAR value-added source catalogue in the Hobby-Eberly Telescope Dark Energy Experiment (HETDEX) Spring Field. We estimate L150 for the cross-matched sources and compare it with the total infrared (IR) luminosity, LIR , and various SFR tracers. Results. We find a tight linear correlation between log L150 and log LIR for star-forming galaxies, with a slope of 1.37. The median qIR value (defined as the logarithm of the LIR to L150 ratio) and its rms scatter of our main sample are 2.14 and 0.34, respectively. We also find that log L150 correlates tightly with the logarithm of SFR derived from three different tracers, i.e., SFR Hα based on the H α line luminosity, SFR 60 based on the rest-frame 60 μ m luminosity and SFR IR based on LIR , with a scatter of 0.3 dex. Our best-fit relations between L150 and these SFR tracers are, log L150 ( L⊙ ) = 1.35(±0.06) × log SFR H α ( M⊙ yr ⁻¹ ) + 3.20(±0.06), log L150 ( L⊙ ) = 1.31(±0.05) × log SFR 60 ( M⊙ yr ⁻¹ ) + 3.14(±0.06), and log L150 ( L⊙ ) = 1.37 (±0.05) × log SFR IR ( M⊙ yr ⁻¹ ) + 3.09(±0.05), which show excellent agreement with each other.
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We report the detection of a diffuse radio halo source in the hottest known cluster of galaxies 1E 0657-56 (RX J0658-5557). The radio halo has a morphology similar to the X-ray emission from the hot intracluster medium. The presence of a luminous radio halo in such a hot cluster is further evidence for a steep correlation between the radio halo power and the X-ray temperature. We favor models for the origin of radio halo sources involving a direct connection between the X-ray emitting thermal particles and the radio emitting relativistic particles.
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The Australia SKA Pathfinder (ASKAP) is a new telescope under development as a world-class high-dynamic-range wide-field-of-view survey instrument. It will utilize focal plane phased array feeds on the 36 12-m antennas that will compose the array. The large amounts of data present a huge computing challenge, and ASKAP will store data products in an archive after near real-time pipeline processing. This powerful instrument will be deployed at a new radio-quiet observatory, the Murchison Radio-astronomy Observatory in the midwest region of Western Australia, to enable sensitive surveys of the entire sky to address some of the big questions in contemporary physics. As a pathfinder for the SKA, ASKAP will demonstrate field of view enhancement and computing/processing technology as well as the operation of a large-scale radio array in a remote and radio-quiet region of Australia.
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The Australian SKA Pathfinder (ASKAP) is a new radio-telescope being built in Western Australia. One of the key surveys for which it is being built is EMU (Evolutionary Map of the Universe), which will make a deep (~10 {\mu}Jy/bm rms) radio continuum survey covering the entire sky as far North as +30\circ. EMU may be compared to the NRAO VLA Sky Survey (NVSS), except that it will have about 45 times the sensitivity, and five times the resolution. EMU will also have much better sensitivity to diffuse emission than previous large surveys, and is expected to produce a large catalogue of relics, tailed galaxies, and haloes, and will increase the number of known clusters by a significant factor. Here we describe the EMU project and its impact on the astrophysics of clusters.
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We present a multi-wavelength analysis of the merging rich cluster of galaxies Abell 2256. We have observed A2256 at 150 MHz using the Giant Metrewave Radio Telescope and successfully detected the diffuse radio halo and the relic emission over an extent $\sim1.2$ Mpc$^2$. Using this 150 MHz image and the images made using archival observations from the VLA (1369 MHz) and the WSRT (350 MHz), we have produced spectral index images of the diffuse radio emission in A2256. These spectral index images show a distribution of flat spectral index (S$\propto\nu^\alpha$, $\alpha$ in the range -0.7 to -0.9) plasma in the NW of the cluster centre. Regions showing steep spectral indices ($\alpha$ in the range -1.0 to -2.3) are toward the SE of the cluster centre. These spectral indices indicate synchrotron life times for the relativistic plasmas in the range 0.08 - 0.4 Gyr. We interpret this spectral behaviour as resulting from a merger event along the direction SE to NW within the last 0.5 Gyr or so. A shock may be responsible for the NW relic in A2256 and the Mpc scale radio halo towards the SE is likely to be generated by the turbulence injected by mergers. Furthermore, the diffuse radio emission shows spectral steepening toward lower frequencies. This low frequency spectral steepening is consistent with a combination of spectra from two populations of relativistic electrons created at two epochs (two mergers) within the last $\sim$0.5 Gyr. Earlier interpretations of the X-ray and the optical data also suggested that there were two mergers in Abell 2256 in the last 0.5 Gyr, consistent with the current findings. Also highlighted in this study is the futility of correlating the average temperatures of thermal gas and the average spectral indices of diffuse radio emission in respective clusters. Comment: Accepted for publication in ApJ
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Giant radio halos are mega-parsec scale synchrotron sources detected in a fraction of massive and merging galaxy clusters. Radio halos provide one of the most important pieces of evidence for non-thermal components in large scale structure. Statistics of their properties can be used to discriminate among various models for their origin. Therefore, theoretical predictions of the occurrence of radio halos are important as several new radio telescopes are about to begin to survey the sky at low frequencies with unprecedented sensitivity. In this paper we carry out Monte Carlo simulations to model the formation and evolution of radio halos in a cosmological framework. We extend previous works on the statistical properties of radio halos in the context of the turbulent re-acceleration model. First we compute the fraction of galaxy clusters that show radio halos and derive the luminosity function of radio halos. Then, we derive differential and integrated number count distributions of radio halos at low radio frequencies with the main goal to explore the potential of the upcoming LOFAR surveys. By restricting to the case of clusters at redshifts
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We present deep Very Large Array observations of the merging galaxy cluster A2256. This cluster is known to possess diffuse steep-spectrum radio relic emission in the peripheral regions. Our new observations provide the first detailed image of the central diffuse radio halo emission in this cluster. The radio halo extends over more than 800 kpc in the cluster core, while the relic emission covers a region of ~1125 kpc × 520 kpc. A spectral index map of the radio relic shows a spectral steepening from the northwest toward the southeast edge of the emission, with an average spectral index between 1369 and 1703 MHz of α = -1.2 across the relic. Polarization maps reveal high fractional polarization of up to 45% in the relic region with an average polarization of 20% across the relic region. The observed Faraday rotation measure is consistent with the Galactic estimate, and the dispersion in the rotation measure is small, suggesting that there is very little contribution to the rotation measure of the relic from the intracluster medium. We use these Faraday properties of the relic to argue that it is located on the front side of the cluster.
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In the past, different works based on numerical simulations have been presented to explain magnetic fields (MFs) in the large scale structure and within galaxy clusters. In this review, I will summarize the main findings obtained by different authors and – even if many details are still unclear – I will try to construct a consistent picture of our interpretation of largescale magnetic fields based on numerical effort. I will also sketch how this is related to our understanding of radio emission and summarize some arguments where our theoretical understanding has to be improved to match the observations. (© 2006 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim)
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Shocking Radio Relic Radio relics are diffuse, elongated radio sources located on the outskirts of galaxy clusters thought to trace shocks generated by collisions between galaxy clusters. Particles may be accelerated within the shock waves by a diffusive shock acceleration mechanism, which also accelerates particles in shock waves produced by supernova explosions. Van Weeren et al. (p. 347 , published online 23 September) report the detection of a megaparsec-scale radio relic showing all the properties of diffusive shock acceleration expected at radio wavelengths. The results suggest that this acceleration mechanism operates on scales larger than those of supernova remnants and imply that merging clusters of galaxies can accelerate particles to energies much higher than those achieved in supernova remnants
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Context: Diffuse radio emission, in the form of radio halos and relics, traces regions in clusters with shocks or turbulence, probably produced by cluster mergers. Some models of diffuse radio emission in clusters indicate that virtually all clusters should contain diffuse radio sources with a steep spectrum. External accretion shocks associated with filamentary structures of galaxies could also accelerate electrons to relativistic energies and hence produce diffuse synchrotron emitting regions. Here we report on Giant Metrewave Radio Telescope (GMRT) observations of a sample of steep spectrum sources from the 74 MHz VLSS survey. These sources are diffuse and not associated with nearby galaxies. Aims: The main aim of the observations is to search for diffuse radio emission associated with galaxy clusters or the cosmic web. Methods: We carried out GMRT 610 MHz continuum observations of unidentified diffuse steep spectrum sources. Results: We have constructed a sample of diffuse steep spectrum sources, selected from the 74 MHz VLSS survey. We identified eight diffuse radio sources probably all located in clusters. We found five radio relics, one cluster with a giant radio halo and a radio relic, and one radio mini-halo. By complementing our observations with measurements from the literature we find correlations between the physical size of relics and the spectral index, in the sense that smaller relics have steeper spectra. Furthermore, larger relics are mostly located in the outskirts of clusters while smaller relics are located closer to the cluster center. Comment: 20 pages, 26 figures, accepted for publication in A&A on October 7, 2009