Radio halo

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Halo of the Abell 1758 cluster shown in pink from the GMRT, overlaid with Chandra data shown in blue. Cluster Collisions Switch on Radio Halos - Copy.jpg
Halo of the Abell 1758 cluster shown in pink from the GMRT, overlaid with Chandra data shown in blue.

Radio halos are large-scale sources of diffuse radio emission found in the center of some, but not all, galaxy clusters. [1] [2] There are two classes of radio halos: mini-halos and giant radio halos. The linear size of giant radio halos is about 700kpc-1Mpc, whereas mini-halos are typically less than 500kpc. Giant radio halos are more often observed in highly X-ray luminous cluster samples than less luminous X-ray clusters () in complete samples. [1] They have a very low surface brightness and do not have obvious galaxy counterparts [2] (in contrast to radio galaxies which have AGN counterparts). However, their morphologies typically follow the distribution of gas in the intra-cluster medium. Mini-halos however, while similar to giant halos, are found at the center of cooling core clusters but around a radio galaxy.

The cause of radio haloes is still debated, but they may be caused by reacceleration of mildly relativistic electrons during a merger event between galaxy clusters. The generated turbulent motions of the intra-cluster plasma drive Magneto-Hydrodynamical Waves, which couples with mildly relativistic particles (i.e. of energy on the level of 100 MeV) and accelerate them up to energy of 10 GeV or more. An alternative model suggests they are caused by secondary electrons generated by collisions between cosmic ray protons (CRp) and intra-cluster medium (ICM) protons. [3]

Radio relics resemble haloes but are found at the edge of clusters. They are likely to result from synchrotron radiation originating from electrons accelerated by shock waves, moving in the intracluster magnetic field of around 0.1 - 3 μG. [4]

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<span class="mw-page-title-main">Galaxy formation and evolution</span>

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<span class="mw-page-title-main">Synchrotron radiation</span> Electromagnetic radiation emitted by charged particles accelerated perpendicular to their velocity

Synchrotron radiation is the electromagnetic radiation emitted when relativistic charged particles are subject to an acceleration perpendicular to their velocity. It is produced artificially in some types of particle accelerators or naturally by fast electrons moving through magnetic fields. The radiation produced in this way has a characteristic polarization, and the frequencies generated can range over a large portion of the electromagnetic spectrum.

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<span class="mw-page-title-main">Seyfert galaxy</span> Class of active galaxies with very bright nuclei

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<span class="mw-page-title-main">Radio galaxy</span> Type of active galaxy that is very luminous at radio wavelengths

A radio galaxy is a galaxy with giant regions of radio emission extending well beyond its visible structure. These energetic radio lobes are powered by jets from its active galactic nucleus. They have luminosities up to 1039 W at radio wavelengths between 10 MHz and 100 GHz. The radio emission is due to the synchrotron process. The observed structure in radio emission is determined by the interaction between twin jets and the external medium, modified by the effects of relativistic beaming. The host galaxies are almost exclusively large elliptical galaxies. Radio-loud active galaxies can be detected at large distances, making them valuable tools for observational cosmology. Recently, much work has been done on the effects of these objects on the intergalactic medium, particularly in galaxy groups and clusters.

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<span class="mw-page-title-main">BL Lacertae object</span> Type of active galactic nucleus

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In astroparticle physics, an ultra-high-energy cosmic ray (UHECR) is a cosmic ray with an energy greater than 1 EeV (1018 electronvolts, approximately 0.16 joules), far beyond both the rest mass and energies typical of other cosmic ray particles.

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<span class="mw-page-title-main">Extragalactic cosmic ray</span>

Extragalactic cosmic rays are very-high-energy particles that flow into the Solar System from beyond the Milky Way galaxy. While at low energies, the majority of cosmic rays originate within the Galaxy (such as from supernova remnants), at high energies the cosmic ray spectrum is dominated by these extragalactic cosmic rays. The exact energy at which the transition from galactic to extragalactic cosmic rays occurs is not clear, but it is in the range 1017 to 1018 eV.

<span class="mw-page-title-main">Radio relics</span>

Radio relics are diffuse synchrotron radio sources found in the peripheral regions of galaxy clusters. As in the case of radio halos, they do not have any obvious galaxy counterpart, but their shapes are much more elongated and irregular compared to those of radio halos. Their energy distribution is steep, with hints of a distribution of different ages for the emitting electrons across the whole dimension of the emitting region.

<span class="mw-page-title-main">Swift J1644+57</span> Tidal disruption event in the constellation Draco

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Centrifugal acceleration of astroparticles to relativistic energies might take place in rotating astrophysical objects. It is strongly believed that active galactic nuclei and pulsars have rotating magnetospheres, therefore, they potentially can drive charged particles to high and ultra-high energies. It is a proposed explanation for ultra-high-energy cosmic rays (UHECRs) and extreme-energy cosmic rays (EECRs) exceeding the Greisen–Zatsepin–Kuzmin limit.

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<span class="mw-page-title-main">IC 1459</span> Elliptical galaxy in the constellation of Grus

IC 1459 is an elliptical galaxy located in the constellation Grus. It is located at a distance of circa 85 million light-years from Earth, which, given its apparent dimensions, means that IC 1459 is about 130,000 light-years across. It was discovered by Edward Emerson Barnard in 1892.

<span class="mw-page-title-main">IC 310</span> Lenticular galaxy in the constellation Perseus

IC 310 is a lenticular galaxy located in the constellation Perseus. It is located 265 million light-years from Earth, which means, given its apparent dimensions, it is about 117,000 light-years across. The galaxy was discovered by Edward D. Swift on November 3, 1888.

<span class="mw-page-title-main">Abell 2219 BCG</span>

Abell 2219 BCG, also known as PGC 2285869, is a massive type-cD elliptical galaxy residing as the brightest cluster galaxy (BCG) in the Abell 2219 galaxy cluster located in constellation Hercules. At the redshift of 0.224, the galaxy is around 2.7 billion light-years from Earth.

References

  1. 1 2 Giovannini, G.; Tordi, M.; Feretti, L. (1999). "Radio Halo and Relic Candidates from the NRAO VLA Sky Survey". New Astronomy. 4 (2): 141–155. arXiv: astro-ph/9904210 . Bibcode:1999NewA....4..141G. doi:10.1016/S1384-1076(99)00018-4. ISSN   1384-1076. S2CID   19610561.
  2. 1 2 Feretti, L., and G. Swarup. "The Universe at Low Radio Frequencies." Proceedings of IAU Symposium. Vol. 199. 2002.
  3. Brunetti, G.; Blasi, P. (November 2005). "Alfvénic reacceleration of relativistic particles in galaxy clusters in the presence of secondary electrons and positrons". Monthly Notices of the Royal Astronomical Society. 363 (4): 1173–1187. arXiv: astro-ph/0508100 . Bibcode:2005MNRAS.363.1173B. doi:10.1111/j.1365-2966.2005.09511.x. S2CID   16726839 . Retrieved 16 May 2022.
  4. Ferrari, C.; Govoni, F.; Schindler, S.; Bykov, A. M.; Rephaeli, Y. (2008). "Observations of Extended Radio Emission in Clusters". Clusters of Galaxies. pp. 93–118. arXiv: 0801.0985 . doi:10.1007/978-0-387-78875-3_6. ISBN   978-0-387-78874-6.