The Event Horizon Telescope (EHT) is a large telescope array consisting of a global network of radio telescopes. The EHT project combines data from several very-long-baseline interferometry (VLBI) stations around Earth, which form a combined array with an angular resolution sufficient to observe objects the size of a supermassive black hole's event horizon. The project's observational targets include the two black holes with the largest angular diameter as observed from Earth: the black hole at the center of the supergiant elliptical galaxyMessier 87 (M87*, pronounced "M87-Star"), and Sagittarius A* (Sgr A*, pronounced "Sagittarius A-Star") at the center of the Milky Way.[1][2][3]
The Event Horizon Telescope project is an international collaboration that was launched in 2009[1] after a long period of theoretical and technical developments. On the theory side, work on the photon orbit[4] and first simulations of what a black hole would look like[5] progressed to predictions of VLBI imaging for the Galactic Center black hole, Sgr A*.[6][7] Technical advances in radio observing moved from the first detection of Sgr A*,[8] through VLBI at progressively shorter wavelengths, ultimately leading to detection of horizon scale structure in both Sgr A* and M87.[9][10] The collaboration now comprises over 300[11] members, 60 institutions, working in over 20 countries and regions.[3]
The first image of a black hole, at the center of galaxy Messier 87, was published by the EHT Collaboration on April 10, 2019, in a series of six scientific publications.[12] The array made this observation at a wavelength of 1.3mm and with a theoretical diffraction-limited resolution of 25 microarcseconds. In March 2021, the Collaboration presented, for the first time, a polarized-based image of the black hole which may help better reveal the forces giving rise to quasars.[13] Future plans involve improving the array's resolution by adding new telescopes and by taking shorter-wavelength observations.[2][14] On 12 May 2022, astronomers unveiled the first image of the supermassive black hole at the center of the Milky Way, Sagittarius A*.[15]
Telescope array
A schematic diagram of the VLBI mechanism of EHT. Each antenna, spread out over vast distances, has an extremely precise atomic clock. Analogue signals collected by the antenna are converted to digital signals and stored on hard drives together with the time signals provided by the atomic clock. The hard drives are then shipped to a central location to be synchronized. An astronomical observation image is obtained by processing the data gathered from multiple locations.EHT observations during its 2017 M87 multiwavelength campaign decomposed by instrument from lower (EHT/ALMA/SMA) to higher (VERITAS) frequency. (Fermi-LAT in continuous survey mode) (dates also in Modified Julian days)Soft X-ray image of Sagittarius A* (center) and two light echoes from a recent explosion (circled)
The EHT is composed of many radio observatories or radio-telescope facilities around the world, working together to produce a high-sensitivity, high-angular-resolution telescope. Through the technique of very-long-baseline interferometry (VLBI), many independent radio antennas separated by hundreds or thousands of kilometres can act as a phased array, a virtual telescope which can be pointed electronically, with an effective aperture which is the diameter of the entire planet, substantially improving its angular resolution.[16] The effort includes development and deployment of submillimeter dual polarization receivers, highly stable frequency standards to enable very-long-baseline interferometry at 230–450GHz, higher-bandwidth VLBI backends and recorders, as well as commissioning of new submillimeter VLBI sites.[17]
Each year since its first data capture in 2006, the EHT array has moved to add more observatories to its global network of radio telescopes. The first image of the Milky Way's supermassive black hole, Sagittarius A*, was expected to be produced from data taken in April 2017,[18][19] but because there are no flights in or out of the South Pole during austral winter (April to October), the full data set could not be processed until December 2017, when the shipment of data from the South Pole Telescope arrived.[20]
Data collected on hard drives are transported by commercial freight airplanes[21] (a so-called sneakernet) from the various telescopes to the MIT Haystack Observatory and the Max Planck Institute for Radio Astronomy, where the data are cross-correlated and analyzed on a grid computer made from about 800 CPUs all connected through a 40 Gbit/s network.[22]
Because of the COVID-19 pandemic, weather patterns, and celestial mechanics, the 2020 observational campaign was postponed to March 2021.[23]
Messier 87*
A series of images representing the magnification achieved (as though trying to see a tennis ball on the moon). Starts at top left corner and moves counter−clockwise to eventually end at the top right corner.Image of M87* generated from data gathered by the Event Horizon Telescope[24][25]A view of M87* black hole in polarised light
The Event Horizon Telescope Collaboration announced its first results in six simultaneous press conferences worldwide on April 10, 2019.[24][25][26] The announcement featured the first direct image of a black hole, which showed the supermassive black hole at the center of Messier 87, designated M87*.[2][27][28] The scientific results were presented in a series of six papers published in The Astrophysical Journal Letters.[29] Clockwise rotating black hole was observed in the 6σ region.[30]
The image provided a test for Albert Einstein's general theory of relativity under extreme conditions.[16][19] Studies have previously tested general relativity by looking at the motions of stars and gas clouds near the edge of a black hole. However, an image of a black hole brings observations even closer to the event horizon.[31] Relativity predicts a dark shadow-like region, caused by gravitational bending and capture of light,[6][7] which matches the observed image. The published paper states: "Overall, the observed image is consistent with expectations for the shadow of a spinning Kerr black hole as predicted by general relativity."[32] Paul T.P. Ho, EHT Board member, said: "Once we were sure we had imaged the shadow, we could compare our observations to extensive computer models that include the physics of warped space, superheated matter, and strong magnetic fields. Many of the features of the observed image match our theoretical understanding surprisingly well."[29]
The image also provided new measurements for the mass and diameter of M87*. EHT measured the black hole's mass to be 6.5±0.7billion solar masses and measured the diameter of its event horizon to be approximately 40billion kilometres (270AU; 0.0013pc; 0.0042ly), roughly 2.5 times smaller than the shadow that it casts, seen at the center of the image.[29][31] Previous observations of M87 showed that the large-scale jet is inclined at an angle of 17° relative to the observer's line of sight and oriented on the plane of the sky at a position angle of −72°.[2][33] From the enhanced brightness of the southern part of the ring due to relativistic beaming of approaching funnel wall jet emission, EHT concluded the black hole, which anchors the jet, spins clockwise, as seen from Earth.[2][14] EHT simulations allow for both prograde and retrograde inner disk rotation with respect to the black hole, while excluding zero black hole spin using a conservative minimum jet power of 1042 erg/s via the Blandford–Znajek process.[2][34]
Producing an image from data from an array of radio telescopes requires much mathematical work. Four independent teams created images to assess the reliability of the results.[35] These methods included both an established algorithm in radio astronomy for image reconstruction known as CLEAN, invented by Jan Högbom,[36] as well as self-calibrating image processing methods[37] for astronomy such as the CHIRP algorithm created by Katherine Bouman and others.[35][38] The algorithms that were ultimately used were a regularized maximum likelihood (RML)[39] algorithm and the CLEAN algorithm.[35]
In March 2020, astronomers proposed an improved way of seeing more of the rings in the first black hole image.[40][41] In March 2021, a new photo was revealed, showing how the M87 black hole looks in polarised light. This is the first time astronomers have been able to measure polarisation so close to the edge of a black hole. The lines on the photo mark the orientation of polarisation, which is related to the magnetic field around the shadow of the black hole.[42]
In August 2022, a team led by University of Waterloo researcher Avery Broderick released a "remaster[ed]" version of original image generated from the data collected by the EHT. This image "resolve[d] a fundamental signature of gravity around a black hole," with it showing a displaying photon ring around M87*[43][44].The claim has been subsequently disputed[45]
3C 279
EHT image of the archetypal blazar 3C 279 showing a relativistic jet down to the AGN core surrounding the supermassive black hole.
In April 2020, the EHT released the first 20 microarcsecond resolution images of the archetypal blazar 3C 279 it observed in April 2017.[46] These images, generated from observations over 4 nights in April 2017, reveal bright components of a jet whose projection on the observer plane exhibit apparent superluminal motions with speeds up to 20 c.[47] Such apparent superluminal motion from relativistic emitters such as an approaching jet is explained by emission originating closer to the observer (downstream along the jet) catching up with emission originating further from the observer (at the jet base) as the jet propagates close to the speed of light at small angles to the line of sight.
Centaurus A
Image of Centaurus A showing its black hole jet at different scales
In July 2021, high resolution images of the jet produced by black hole sitting at the center of Centaurus A were released. With a mass around 5.5×107M☉, the black hole is not big enough to observe its ring as with Messier M87*, but its jet extends even beyond its host galaxy while staying as a highly collimated beam which is a point of study. Edge-brightening of the jet was also observed which would exclude models of particle acceleration that are unable to reproduce this effect. The image was 16 times sharper than previous observations and utilized a 1.3 mm wavelength.[48][49][50]
Sagittarius A*
Sagittarius A*, black hole in the center of the Milky Way
On May 12, 2022, the EHT Collaboration revealed an image of Sagittarius A*, the supermassive black hole at the center of the Milky Way galaxy. The black hole is 27,000 light-years away from Earth; it is thousands of times smaller than M87*. Sera Markoff, Co-Chair of the EHT Science Council, said: "We have two completely different types of galaxies and two very different black hole masses, but close to the edge of these black holes they look amazingly similar. This tells us that General Relativity governs these objects up close, and any differences we see further away must be due to differences in the material that surrounds the black holes."[51]
J1924-2914
A multifrequency view of the bent jet in Blazar J1924-2914.[52][53]
In August 2022, the EHT together with Global Millimeter VLBI Array and the Very Long Baseline Array imaged the distant blazar J1924-2914. They operated at 230 GHz, 86 GHz and 2.3+8.7 GHz, respectively, the highest angular resolution images of polarized emission from a quasar ever obtained. Observations reveal a helically bent jet and the polarization of its emission suggest a toroidal magnetic field structure. The object is used as calibrator for Sagittarius A* sharing strong optical variability and polarization with it.[52][53]
Collaborating institutes
The EHT Collaboration consists of 13 stakeholder institutes:[3]
the Academia Sinica Institute of Astronomy and Astrophysics
Institut de radioastronomie millimétrique (IRAM, itself a collaboration between the French CNRS, the German Max Planck Society, and the Spanish Instituto Geográfico Nacional),
National Sun Yat-Sen University, Physics Department
National Taiwan University, Department of Physics
Netherlands Organisation for Scientific Research
Peking University, Department of Astronomy, School of Physics / Kavli Institute for Astronomy and Astrophysics
Rhodes University, Centre for Radio Astronomy Techniques and Technologies, Department of Physics and Electronics
Seoul National University, Department of Physics and Astronomy
Tohoku University, Astronomy Institute / Frontier Research Institute for Interdisciplinary Sciences
Universidad de Concepción, Astronomy Department
Universidad Nacional Autónoma de México, Instituto de Astronomía / Instituto de Radioastronomía y Astrofísica
Universitat de València, Departament d'Astronomia i Astrofísica / Observatori Astronòmic
University College London, Mullard Space Science Laboratory
University of Amsterdam, Anton Pannekoek Institute & GRAPPA
University of Arizona
University of California Berkeley
University of California Santa Barbara
University of Chinese Academy of Sciences, School of Astronomy and Space Sciences
University of Illinois, Department of Astronomy / Department of Physics
University of Massachusetts Amherst, Department of Astronomy
University of Pretoria, Department of Physics
University of Science and Technology
University of Science and Technology of China, Astronomy Department
University of St. Petersburg, Astronomy Institute
University of Tokyo, Graduate School of Science, Department of Astronomy / Kavli Institute for Physics & Mathematics of the Universe
University of Toronto, Dunlap Institute for Astronomy and Astrophysics
University of Waterloo, Waterloo Center for Astrophysics / Department of Physics and Astronomy
Yonsei University, Department of Astronomy
References
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Falcke, Heino; Melia, Fulvio; Agol, Eric (January 1, 2000). "Viewing the Shadow of the Black Hole at the Galactic Center". The Astrophysical Journal Letters. 528 (1): L13–L16. arXiv:astro-ph/9912263. Bibcode:2000ApJ...528L..13F. doi:10.1086/312423. PMID10587484. S2CID119433133.
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Lu, Donna (April 12, 2019). "How do you name a black hole? It is actually pretty complicated". New Scientist. London. Retrieved April 12, 2019. “For the case of M87*, which is the designation of this black hole, a (very nice) name has been proposed, but it has not received an official IAU approval,” says Christensen.
Walker, R. Craig; Hardee, Philip E.; Davies, Frederick B.; Ly, Chun; Junor, William (2018). "The Structure and Dynamics of the Subparsec Jet in M87 Based on 50 VLBA Observations over 17 Years at 43 GHZ". The Astrophysical Journal. 855 (2): 128. arXiv:1802.06166. Bibcode:2018ApJ...855..128W. doi:10.3847/1538-4357/aaafcc. S2CID59322635.
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