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Sagittarius A*

Coordinates: Sky map 17h 45m 40.0409s, −29° 0′ 28.118″
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Sagittarius A*

Sagittarius A* imaged by the Event Horizon Telescope in 2017, released in 2022
Observation data
Epoch J2000      Equinox J2000
Constellation Sagittarius
Right ascension 17h 45m 40.0409s
Declination −29° 0′ 28.118″[1]
Details
Mass8.54×1036 kg
4.297×106[2] M
Astrometry
Distance26996±29[2] ly
(8277±9[2] pc)
Database references
SIMBADdata

Sagittarius A*, abbreviated as Sgr A* (/ˈsæ ˈ stɑːr/ SADGE-AY-star[3]), is the supermassive black hole[4][5][6] at the Galactic Center of the Milky Way. Viewed from Earth, it is located near the border of the constellations Sagittarius and Scorpius, about 5.6° south of the ecliptic,[7] visually close to the Butterfly Cluster (M6) and Lambda Scorpii.

The object is a bright and very compact astronomical radio source. The name Sagittarius A* distinguishes the compact source from the larger (and much brighter) Sagittarius A (Sgr A) region in which it is embedded. Sgr A* was discovered in 1974 by Bruce Balick [de] and Robert L. Brown,[8][9] and the asterisk * was assigned in 1982 by Brown,[10] who understood that the strongest radio emission from the center of the galaxy appeared to be due to a compact non-thermal radio object.

The observations of several stars orbiting Sagittarius A*, particularly star S2, have been used to determine the mass and upper limits on the radius of the object. Based on mass and increasingly precise radius limits, astronomers have concluded that Sagittarius A* must be the central supermassive black hole of the Milky Way galaxy.[11] The current best estimate of its mass is 4.297±0.012 million solar masses.[2]

Reinhard Genzel and Andrea Ghez were awarded the 2020 Nobel Prize in Physics for their discovery that Sagittarius A* is a supermassive compact object, for which a black hole was the only plausible explanation at the time.[12]

In May 2022, astronomers released the first image of the accretion disk around the horizon of Sagittarius A*, confirming it to be a black hole, using the Event Horizon Telescope, a world-wide network of radio observatories.[13] This is the second confirmed image of a black hole, after Messier 87's supermassive black hole in 2019.[14][15] The black hole itself is not seen; as light is incapable of escaping the immense gravitational force of a black hole, only nearby objects whose behavior is influenced by the black hole can be observed. The observed radio and infrared energy emanates from gas and dust heated to millions of degrees while falling into the black hole.[16]

Observation and description

[edit]
Sagittarius A* in the constellation of Sagittarius. The black hole is marked with a red circle within the constellation of Sagittarius (The Archer). This map shows most of the stars visible to the unaided eye under good conditions.
Size comparison between Sagittarius A* and M87*. The diameter of Sagittarius A* is smaller than the orbit of Mercury.

On May 12, 2022, the first image of Sagittarius A* was released by the Event Horizon Telescope Collaboration. The image, which is based on radio interferometer data taken in 2017, confirms that the object contains a black hole. This is the second image of a black hole.[14][17] This image took five years of calculations to process.[18] The data was collected by eight radio observatories at six geographical sites. Radio images are produced from data by aperture synthesis, usually from night-long observations of stable sources. The radio emission from Sgr A* varies on the order of minutes, complicating the analysis.[19]

Their result gives an overall angular size for the source of 51.8±2.3 μas.[17] At a distance of 26,000 light-years (8,000 parsecs), this yields a diameter of 51.8 million kilometres (32.2 million miles).[a] For comparison, Earth is 150 million kilometres (1.0 astronomical unit; 93 million miles) from the Sun, and Mercury is 46 million km (0.31 AU; 29 million mi) from the Sun at perihelion. The proper motion of Sgr A* is approximately −2.70 mas per year for the right ascension and −5.6 mas per year for the declination.[20][21][22] The telescope's measurement of these black holes tested Einstein's theory of relativity more rigorously than has previously been done, and the results match perfectly.[15]

In 2019, measurements made with the High-resolution Airborne Wideband Camera-Plus (HAWC+) mounted in the SOFIA aircraft[23] revealed that magnetic fields cause the surrounding ring of gas and dust, temperatures of which range from −280 to 17,500 °F (99.8 to 9,977.6 K; −173.3 to 9,704.4 °C),[24] to flow into an orbit around Sagittarius A*, keeping black hole emissions low.[25]

Astronomers have been unable to observe Sgr A* in the optical spectrum because of the effect of 25 magnitudes of extinction (absorption and scattering) by dust and gas between the source and Earth.[26]

History

[edit]

In April 1933, Karl Jansky, considered one of the fathers of radio astronomy, discovered that a radio signal was coming from a location in the direction of the constellation of Sagittarius, towards the center of the Milky Way.[27] The radio source later became known as Sagittarius A. His observations did not extend quite as far south as we now know to be the Galactic Center.[28] Observations by Jack Piddington and Harry Minnett using the CSIRO radio telescope at Potts Hill Reservoir, in Sydney discovered a discrete and bright "Sagittarius-Scorpius" radio source,[29] which after further observation with the 80-foot (24-metre) CSIRO radio telescope at Dover Heights was identified in a letter to Nature as the probable Galactic Center.[30]

Later observations showed that Sagittarius A actually consists of several overlapping sub-components; a bright and very compact component, Sgr A*, was discovered on February 13 and 15, 1974, by Balick and Robert L Brown using the baseline interferometer of the National Radio Astronomy Observatory.[31][32] The name Sgr A* was coined by Brown in a 1982 paper because the radio source was "exciting", and excited states of atoms are denoted with asterisks.[33][34]

Since the 1980s, it has been evident that the central component of Sgr A* is likely a black hole. In 1994, infrared and sub-millimetre spectroscopy studies by a Berkeley team involving Nobel Laureate Charles H. Townes and future Nobel Prize Winner Reinhard Genzel showed that the mass of Sgr A* was tightly concentrated and on the order of 3 million Suns.[35]

On October 16, 2002, an international team led by Reinhard Genzel at the Max Planck Institute for Extraterrestrial Physics reported the observation of the motion of the star S2 near Sagittarius A* throughout a period of ten years. According to the team's analysis, the data ruled out the possibility that Sgr A* contains a cluster of dark stellar objects or a mass of degenerate fermions, strengthening the evidence for a massive black hole. The observations of S2 used near-infrared (NIR) interferometry (in the Ks-band, i.e. 2.1 μm) because of reduced interstellar extinction in this band. SiO masers were used to align NIR images with radio observations, as they can be observed in both NIR and radio bands. The rapid motion of S2 (and other nearby stars) easily stood out against slower-moving stars along the line-of-sight so these could be subtracted from the images.[36][37]

Dusty cloud G2 passes the supermassive black hole at the center of the Milky Way.[38] Composition of images taken at different times to show motion; colored blue when approaching the viewer, red when receding; time is left to right. Red cross marks the black hole.

The VLBI radio observations of Sagittarius A* could also be aligned centrally with the NIR images, so the focus of S2's elliptical orbit was found to coincide with the position of Sagittarius A*. From examining the Keplerian orbit of S2, they determined the mass of Sagittarius A* to be 4.1±0.6 million solar masses, confined in a volume with a radius no more than 17 light-hours (120 AU [18 billion km; 11 billion mi]).[39] Later observations of the star S14 showed the mass of the object to be about 4.1 million solar masses within a volume with radius no larger than 6.25 light-hours (45 AU [6.7 billion km; 4.2 billion mi]).[40] S175 passed within a similar distance.[41] For comparison, the Schwarzschild radius is 0.08 AU (12 million km; 7.4 million mi). They also determined the distance from Earth to the Galactic Center (the rotational center of the Milky Way), which is important in calibrating astronomical distance scales, as 8,000 ± 600 parsecs (30,000 ± 2,000 light-years). In November 2004, a team of astronomers reported the discovery of a potential intermediate-mass black hole, referred to as GCIRS 13E, orbiting 3 light-years from Sagittarius A*. This black hole of 1,300 solar masses is within a cluster of seven stars. This observation may add support to the idea that supermassive black holes grow by absorbing nearby smaller black holes and stars.[citation needed]

After monitoring stellar orbits around Sagittarius A* for 16 years, Gillessen et al. estimated the object's mass at 4.31±0.38 million solar masses. The result was announced in 2008 and published in The Astrophysical Journal in 2009.[42] Reinhard Genzel, team leader of the research, said the study has delivered "what is now considered to be the best empirical evidence that supermassive black holes do really exist. The stellar orbits in the Galactic Center show that the central mass concentration of four million solar masses must be a black hole, beyond any reasonable doubt."[43]

On January 5, 2015, NASA reported observing an X-ray flare 400 times brighter than usual, a record-breaker, from Sgr A*. The unusual event may have been caused by the breaking apart of an asteroid falling into the black hole or by the entanglement of magnetic field lines within gas flowing into Sgr A*, according to astronomers.[44]

On 13 May 2019, astronomers using the Keck Observatory witnessed a sudden brightening of Sgr A*, which became 75 times brighter than usual, suggesting that the supermassive black hole may have encountered another object.[45]

In June 2023, unexplained filaments of radio energy were found associated with Sagittarius A*.[46]

Central black hole

[edit]
NuSTAR has captured these first, focused views of the supermassive black hole at the heart of the Milky Way in high-energy X-rays.

In a paper published on October 31, 2018, the discovery of conclusive evidence that Sagittarius A* is a black hole was announced. Using the GRAVITY interferometer and the four telescopes of the Very Large Telescope (VLT) to create a virtual telescope 130 metres (430 feet) in diameter, astronomers detected clumps of gas moving at about 30% of the speed of light. Emission from highly energetic electrons very close to the black hole was visible as three prominent bright flares. These exactly match theoretical predictions for hot spots orbiting close to a black hole of four million solar masses. The flares are thought to originate from magnetic interactions in the very hot gas orbiting very close to Sagittarius A*.[16][48]

In July 2018, it was reported that S2 orbiting Sgr A* had been recorded at 7,650 km/s (17.1 million mph), or 2.55% the speed of light, leading up to the pericenter approach, in May 2018, at about 120 AU (18 billion km; 11 billion mi) (approximately 1,400 Schwarzschild radii) from Sgr A*. At that close distance to the black hole, Einstein's theory of general relativity (GR) predicts that S2 would show a discernible gravitational redshift in addition to the usual velocity redshift; the gravitational redshift was detected, in agreement with the GR prediction within the 10 percent measurement precision.[49][50]

Assuming that general relativity is still a valid description of gravity near the event horizon, the Sagittarius A* radio emissions are not centered on the black hole, but arise from a bright spot in the region around the black hole, close to the event horizon, possibly in the accretion disc, or a relativistic jet of material ejected from the disc.[51] If the apparent position of Sagittarius A* were exactly centered on the black hole, it would be possible to see it magnified beyond its size, because of gravitational lensing of the black hole. According to general relativity, this would result in a ring-like structure, which has a diameter about 5.2 times the black hole's Schwarzschild radius (10 μas). For a black hole of around 4 million solar masses, this corresponds to a size of approximately 52 μas, which is consistent with the observed overall size of about 50 μas,[51] the size (apparent diameter) of the black hole Sgr A* itself being 20 μas.

Recent lower resolution observations revealed that the radio source of Sagittarius A* is symmetrical.[52] Simulations of alternative theories of gravity depict results that may be difficult to distinguish from GR.[53] However, a 2018 paper predicts an image of Sagittarius A* that is in agreement with recent observations; in particular, it explains the small angular size and the symmetrical morphology of the source.[54]

The mass of Sagittarius A* has been estimated in two different ways:

  1. Two groups—in Germany and the U.S.—monitored the orbits of individual stars very near to the black hole and used Kepler's laws to infer the enclosed mass. The German group found a mass of 4.31±0.38 million solar masses,[42] whereas the American group found 4.1±0.6 million solar masses.[40] Given that this mass is confined inside a 44-million-kilometre-diameter sphere, this yields a density ten times higher than previous estimates.[citation needed]
  2. More recently, measurement of the proper motions of a sample of several thousand stars within approximately one parsec from the black hole, combined with a statistical technique, has yielded both an estimate of the black hole's mass at 3.6+0.2
    −0.4
    ×106
    M, plus a distributed mass in the central parsec amounting to (1±0.5)×106 M.[55] The latter is thought to be composed of stars and stellar remnants.[citation needed]
Magnetar found very close to the supermassive black hole, Sagittarius A*, at the center of the Milky Way galaxy

The comparatively small mass of this supermassive black hole, along with the low luminosity of the radio and infrared emission lines, imply that the Milky Way is not a Seyfert galaxy.[26]

Ultimately, what is seen is not the black hole itself, but observations that are consistent only if there is a black hole present near Sgr A*. In the case of such a black hole, the observed radio and infrared energy emanates from gas and dust heated to millions of degrees while falling into the black hole.[16] The black hole itself is thought to emit only Hawking radiation at a negligible temperature, on the order of 10−14 kelvin.[citation needed]

The European Space Agency's gamma-ray observatory INTEGRAL observed gamma rays interacting with the nearby giant molecular cloud Sagittarius B2, causing X-ray emission from the cloud. The total luminosity from this outburst (L≈1,5×1039 erg/s) is estimated to be a million times stronger than the current output from Sgr A* and is comparable with a typical active galactic nucleus.[56][57] In 2011 this conclusion was supported by Japanese astronomers observing the Milky Way's center with the Suzaku satellite.[58]

In July 2019, astronomers reported finding a star, S5-HVS1, traveling 1,755 km/s (3.93 million mph) or 0.006 c. The star is in the Grus (or Crane) constellation in the southern sky, and about 29,000 light-years from Earth, and may have been propelled out of the Milky Way galaxy after interacting with Sagittarius A*.[59][60]

Several values[61][62] have been given for its spin parameter ; some examples are Fragione & Loeb (2020) [63], Belanger et al. (2006) ,[64] Meyer et al. (2006) ,[65] Genzel et al. (2003) [66] and Daly et al. (2023) .[62] Daly et al. (2023) also found that the ratio of the black hole rotational mass component to the irreducible mass component of Sgr A* is , which indicates that the black hole is rotating with an angular velocity that is of the maximum possible value, set by the speed of light.[62] [67]



Orbiting stars

[edit]
Inferred orbits of six stars around supermassive black hole candidate Sagittarius A* at the Milky Way's center[68]
Stars moving around Sagittarius A*, 20-year timelapse, ending in 2018[69][70]
Stars moving around Sagittarius A* as seen in 2021[71][72][73]

There are a number of stars in close orbit around Sagittarius A*, which are collectively known as "S stars".[74] These stars are observed primarily in K band infrared wavelengths, as interstellar dust drastically limits visibility in visible wavelengths. This is a rapidly changing field—in 2011, the orbits of the most prominent stars then known were plotted in the diagram at left, showing a comparison between their orbits and various orbits in the solar system.[70] Since then, S62 has been found to approach even more closely than those stars.[75]

The high velocities and close approaches to the supermassive black hole makes these stars useful to establish limits on the physical dimensions of Sagittarius A*, as well as to observe general-relativity associated effects like periapse shift of their orbits. An active watch is maintained for the possibility of stars approaching the event horizon close enough to be disrupted, but none of these stars are expected to suffer that fate.

As of 2020, S4714 is the current record holder of closest approach to Sagittarius A*, at about 12.6 AU (1.88 billion km), almost as close as Saturn gets to the Sun, traveling at about 8% of the speed of light. These figures given are approximate, the formal uncertainties being 12.6±9.3 AU and 23,928±8,840 km/s. Its orbital period is 12 years, but an extreme eccentricity of 0.985 gives it the close approach and high velocity.[76]

An excerpt from a table of this cluster (see Sagittarius A* cluster), featuring the most prominent members. In the below table, id1 is the star's name in the Gillessen catalog and id2 in the catalog of the University of California, Los Angeles. a, e, i, Ω and ω are standard orbital elements, with a measured in arcseconds. Tp is the epoch of pericenter passage, P is the orbital period in years and Kmag is the infrared K-band apparent magnitude of the star. q and v are the pericenter distance in AU and pericenter speed in percent of the speed of light.[77]

id1 id2 a e i (°) Ω (°) ω (°) Tp (yr) P (yr) Kmag q (AU) v (%c)
S1 S0-1 0.5950 0.5560 119.14 342.04 122.30 2001.800 166.0 14.70 2160.7 0.55
S2 S0-2 0.1251 0.8843 133.91 228.07 66.25 2018.379 16.1 13.95 118.4 2.56
S8 S0-4 0.4047 0.8031 74.37 315.43 346.70 1983.640 92.9 14.50 651.7 1.07
S12 S0-19 0.2987 0.8883 33.56 230.10 317.90 1995.590 58.9 15.50 272.9 1.69
S13 S0-20 0.2641 0.4250 24.70 74.50 245.20 2004.860 49.0 15.80 1242.0 0.69
S14 S0-16 0.2863 0.9761 100.59 226.38 334.59 2000.120 55.3 15.70 56.0 3.83
S62 0.0905 0.9760 72.76 122.61 42.62 2003.330 9.9 16.10 16.4 7.03
S4714 0.102 0.985 127.7 129.28 357.25 2017.29 12.0 17.7 12.6 8.0

Discovery of G2 gas cloud on an accretion course

[edit]

First noticed as something unusual in images of the center of the Milky Way in 2002,[78] the gas cloud G2, which has a mass about three times that of Earth, was confirmed to be likely on a course taking it into the accretion zone of Sgr A* in a paper published in Nature in 2012.[79] Predictions of its orbit suggested it would make its closest approach to the black hole (a perinigricon) in early 2014, when the cloud was at a distance of just over 3,000 times the radius of the event horizon (or ≈260 AU, 36 light-hours) from the black hole. G2 has been observed to be disrupting since 2009,[79] and was predicted by some to be completely destroyed by the encounter, which could have led to a significant brightening of X-ray and other emission from the black hole. Other astronomers suggested the gas cloud could be hiding a dim star, or a binary star merger product, which would hold it together against the tidal forces of Sgr A*, allowing the ensemble to pass by without any effect.[80] In addition to the tidal effects on the cloud itself, it was proposed in May 2013[81] that, prior to its perinigricon, G2 might experience multiple close encounters with members of the black-hole and neutron-star populations thought to orbit near the Galactic Center, offering some insight to the region surrounding the supermassive black hole at the center of the Milky Way.[82]

The average rate of accretion onto Sgr A* is unusually small for a black hole of its mass[83] and is only detectable because it is so close to Earth. It was thought that the passage of G2 in 2013 might offer astronomers the chance to learn much more about how material accretes onto supermassive black holes. Several astronomical facilities observed this closest approach, with observations confirmed with Chandra, XMM, VLA, INTEGRAL, Swift, Fermi and requested at VLT and Keck.[84]

Simulations of the passage were made before it happened by groups at ESO[85] and Lawrence Livermore National Laboratory (LLNL).[86]

As the cloud approached the black hole, Daryl Haggard said, "It's exciting to have something that feels more like an experiment", and hoped that the interaction would produce effects that would provide new information and insights.[87]

Nothing was observed during and after the closest approach of the cloud to the black hole, which was described as a lack of "fireworks" and a "flop".[88] Astronomers from the UCLA Galactic Center Group published observations obtained on March 19 and 20, 2014, concluding that G2 was still intact (in contrast to predictions for a simple gas cloud hypothesis) and that the cloud was likely to have a central star.[80]

An analysis published on July 21, 2014, based on observations by the ESO's Very Large Telescope in Chile, concluded alternatively that the cloud, rather than being isolated, might be a dense clump within a continuous but thinner stream of matter, and would act as a constant breeze on the disk of matter orbiting the black hole, rather than sudden gusts that would have caused high brightness as they hit, as originally expected. Supporting this hypothesis, G1, a cloud that passed near the black hole 13 years ago, had an orbit almost identical to G2, consistent with both clouds, and a gas tail thought to be trailing G2, all being denser clumps within a large single gas stream.[88][89]

Andrea Ghez et al. suggested in 2014 that G2 is not a gas cloud but rather a pair of binary stars that had been orbiting the black hole in tandem and merged into an extremely large star.[80][90]

Artist impression of the accretion of gas cloud G2 onto Sgr A*. Credit: ESO[91]
This simulation shows a gas cloud, discovered in 2011, as it passes close to the supermassive black hole at the center of the Milky Way.
This video sequence shows the motion of the dusty cloud G2 as it closes in on, and then passes, the supermassive black hole at the center of the Milky Way.

See also

[edit]

Notes

[edit]
  1. ^ This roughly equates to around 37 times the diameter of the Sun at ~1,400,000 kilometers (~865,000 miles).

References

[edit]
  1. ^ Reid and Brunthaler 2004
  2. ^ a b c d The GRAVITY collaboration (September 2023). "Polarimetry and astrometry of NIR flares as event horizon scale, dynamical probes for the mass of Sgr A*". Astronomy & Astrophysics. 677: L10. arXiv:2307.11821. Bibcode:2023A&A...677L..10G. doi:10.1051/0004-6361/202347416.
  3. ^ "Astronomers reveal first image of the black hole at the heart of our galaxy". Event Horizon Telescope. May 12, 2022. Archived from the original on May 12, 2022. Retrieved May 12, 2022.
  4. ^ Parsons, Jeff (October 31, 2018). "Scientists find proof a supermassive black hole is lurking at the centre of the Milky Way". Metro. Archived from the original on October 31, 2018. Retrieved October 31, 2018.
  5. ^ Mosher, Dave (October 31, 2018). "A 'mind-boggling' telescope observation has revealed the point of no return for our galaxy's monster black hole". The Middletown Press. Business Insider. Archived from the original on October 31, 2018. Retrieved May 16, 2022.
  6. ^ Plait, Phil (November 7, 2018). "Astronomers See Material Orbiting a Black Hole *Right* at the Edge of Forever". Bad Astronomy. Syfy Wire. Archived from the original on November 10, 2018. Retrieved November 12, 2018.
  7. ^ Calculated using Equatorial and Ecliptic Coordinates Archived July 21, 2019, at the Wayback Machine calculator
  8. ^ Balick, B.; Brown, R. L. (December 1, 1974). "Intense sub-arcsecond structure in the galactic center". Astrophysical Journal. 194 (1): 265–270. Bibcode:1974ApJ...194..265B. doi:10.1086/153242. S2CID 121802758.
  9. ^ Melia 2007, p. 7
  10. ^ Brown, Robert L. (November 1, 1982). "Precessing Jets in Sagittarius A: Gas Dynamics in the Central Parsec of the Galaxy". The Astrophysical Journal. 262: 110–119. Bibcode:1982ApJ...262..110B. doi:10.1086/160401.
  11. ^ Henderson, Mark (December 9, 2009). "Astronomers confirm black hole at the heart of the Milky Way". Times Online. Archived from the original on December 16, 2008. Retrieved June 6, 2019.
  12. ^ "The Nobel Prize in Physics 2020". October 6, 2020. Archived from the original on April 24, 2021. Retrieved October 7, 2020.
  13. ^ Bower, Geoffrey C. (May 2022). "Focus on First Sgr A* Results from the Event Horizon Telescope". The Astrophysical Journal. Archived from the original on July 19, 2022. Retrieved May 12, 2022.
  14. ^ a b "Astronomers reveal first image of the black hole at the heart of our galaxy". eso.org. May 12, 2022. Archived from the original on May 12, 2022. Retrieved May 12, 2022.
  15. ^ a b Overbye, Dennis (May 12, 2022). "The Milky Way's Black Hole Comes to Light". The New York Times. ISSN 0362-4331. Archived from the original on May 12, 2022. Retrieved May 12, 2022.
  16. ^ a b c Abuter, R.; Amorim, A.; Bauböck, M.; Berger, J. P.; Bonnet, H.; Brandner, W.; Clénet, Y.; Coudé Du Foresto, V.; De Zeeuw, P. T.; Deen, C.; Dexter, J.; Duvert, G.; Eckart, A.; Eisenhauer, F.; Förster Schreiber, N. M.; Garcia, P.; Gao, F.; Gendron, E.; Genzel, R.; Gillessen, S.; Guajardo, P.; Habibi, M.; Haubois, X.; Henning, T.; Hippler, S.; Horrobin, M.; Huber, A.; Jiménez Rosales, A.; Jocou, L.; et al. (2018). "Detection of orbital motions near the last stable circular orbit of the massive black hole SgrA". Astronomy & Astrophysics. 618: L10. arXiv:1810.12641. Bibcode:2018A&A...618L..10G. doi:10.1051/0004-6361/201834294. S2CID 53613305.
  17. ^ a b The Event Horizon Telescope Collaboration (May 1, 2022). "First Sagittarius A* Event Horizon Telescope Results. I. The Shadow of the Supermassive Black Hole in the Center of the Milky Way". The Astrophysical Journal Letters. 930 (2): L12. Bibcode:2022ApJ...930L..12E. doi:10.3847/2041-8213/ac6674. eISSN 2041-8213. hdl:10261/278882. ISSN 2041-8205. S2CID 248744791.
  18. ^ Hensley, Kerry (May 12, 2022). "First Image of the Milky Way's Supermassive Black Hole". AAS Nova. Archived from the original on August 2, 2022. Retrieved May 13, 2022.
  19. ^ The Event Horizon Telescope Collaboration (May 1, 2022). "First Sagittarius A* Event Horizon Telescope Results. III. Imaging of the Galactic Center Supermassive Black Hole". The Astrophysical Journal Letters. 930 (2): L14. arXiv:2311.09479. Bibcode:2022ApJ...930L..14E. doi:10.3847/2041-8213/ac6429. eISSN 2041-8213. ISSN 2041-8205. S2CID 248744704.
  20. ^ Backer and Sramek 1999, § 3
  21. ^ "Focus on the First Event Horizon Telescope Results – The Astrophysical Journal Letters – IOPscience". iopscience.iop.org. Archived from the original on May 14, 2019. Retrieved April 10, 2019.
  22. ^ Overbye, Dennis (April 10, 2019). "Black Hole Picture Revealed for the First Time". The New York Times. ISSN 0362-4331. Archived from the original on May 21, 2019. Retrieved April 10, 2019.
  23. ^ "HAWC+, the Far-Infrared Camera and Polarimeter for SOFIA". 2018. Archived from the original on August 3, 2021. Retrieved August 3, 2021.
  24. ^ "The Milky Way's Monster Black Hole Has a Cool Gas Halo – Literally". Space.com. June 5, 2019. Archived from the original on June 19, 2019. Retrieved June 19, 2019.
  25. ^ "Magnetic Fields May Muzzle Milky Way's Monster Black Hole". Space.com. June 14, 2019. Archived from the original on June 18, 2019. Retrieved June 19, 2019.
  26. ^ a b Osterbrock and Ferland 2006, p. 390
  27. ^ "Karl Jansky: The Father of Radio Astronomy". August 29, 2012. Archived from the original on June 28, 2019. Retrieved January 27, 2019.
  28. ^ Goss, W. M.; McGee, R. X. (1996). "The Discovery of the Radio Source Sagittarius A (Sgr A)". The Galactic Center, Astronomical Society of the Pacific Conference Series. 102: 369. Bibcode:1996ASPC..102..369G. Archived from the original on March 3, 2021. Retrieved February 25, 2021.
  29. ^ Piddington, J. H.; Minnett, H. C. (December 1, 1951). "Observations of Galactic Radiation at Frequencies of 1200 and 3000 Mc/s". Australian Journal of Scientific Research A. 4 (4): 459. Bibcode:1951AuSRA...4..459P. doi:10.1071/CH9510459. Archived from the original on April 13, 2021. Retrieved February 25, 2021.
  30. ^ McGee, R. X.; Bolton, J. G. (May 1, 1954). "Probable observation of the galactic nucleus at 400 Mc./s". Nature. 173 (4412): 985–987. Bibcode:1954Natur.173..985M. doi:10.1038/173985b0. ISSN 0028-0836. S2CID 4188235. Archived from the original on January 30, 2022. Retrieved February 25, 2021.
  31. ^ Balick, B.; Brown, R. L. (December 1, 1974). "Intense sub-arcsecond structure in the galactic center". Astrophysical Journal. 194 (1): 265–270. Bibcode:1974ApJ...194..265B. doi:10.1086/153242. S2CID 121802758.
  32. ^ Melia 2007, p. 7
  33. ^ Goss, W. M.; Brown, Robert L.; Lo, K. Y. (May 6, 2003). "The Discovery of Sgr A*". Astronomische Nachrichten. 324 (1): 497. arXiv:astro-ph/0305074. Bibcode:2003ANS...324..497G. doi:10.1002/asna.200385047.
  34. ^ Brown, R. L. (November 1, 1982). "Precessing jets in Sagittarius A – Gas dynamics in the central parsec of the galaxy". Astrophysical Journal, Part 1. 262: 110–119. Bibcode:1982ApJ...262..110B. doi:10.1086/160401.
  35. ^ Genzel, R; Hollenbach, D; Townes, C H (1994). "The nucleus of our Galaxy". Reports on Progress in Physics. 57 (5): 417–479. Bibcode:1994RPPh...57..417G. doi:10.1088/0034-4885/57/5/001. ISSN 0034-4885. S2CID 250900662.
  36. ^ Schödel et al. 2002
  37. ^ Sakai, Shoko; Lu, Jessica R.; Ghez, Andrea; Jia, Siyao; Do, Tuan; Witzel, Gunther; Gautam, Abhimat K.; Hees, Aurelien; Becklin, E.; Matthews, K.; Hosek, M. W. (March 5, 2019). "The Galactic Center: An Improved Astrometric Reference Frame for Stellar Orbits around the Supermassive Black Hole". The Astrophysical Journal. 873 (1): 65. arXiv:1901.08685. Bibcode:2019ApJ...873...65S. doi:10.3847/1538-4357/ab0361. ISSN 1538-4357. S2CID 119331998.
  38. ^ "Best View Yet of Dusty Cloud Passing Galactic Centre Black Hole". Archived from the original on April 7, 2015. Retrieved June 16, 2015.
  39. ^ Ghez et al. (2003) "The First Measurement of Spectral Lines in a Short-Period Star Bound to the Galaxy's Central Black Hole: A Paradox of Youth" Astrophysical Journal 586 L127
  40. ^ a b Ghez, A. M.; et al. (December 2008). "Measuring Distance and Properties of the Milky Way's Central Supermassive Black Hole with Stellar Orbits". Astrophysical Journal. 689 (2): 1044–1062. arXiv:0808.2870. Bibcode:2008ApJ...689.1044G. doi:10.1086/592738. S2CID 18335611.
  41. ^ Gillessen, S.; Plewa, P. M.; Eisenhauer, F.; Sari, R.; Waisberg, I.; Habibi, M.; Pfuhl, O.; George, E.; Dexter, J. (2017). "An Update on Monitoring Stellar Orbits in the Galactic Center". The Astrophysical Journal. 837 (1): 30. arXiv:1611.09144. Bibcode:2017ApJ...837...30G. doi:10.3847/1538-4357/aa5c41. ISSN 0004-637X. S2CID 119087402.
  42. ^ a b Gillessen et al. 2009
  43. ^ O'Neill 2008
  44. ^ a b Chou, Felicia; Anderson, Janet; Watzke, Megan (January 5, 2015). "NASA's Chandra Detects Record-Breaking Outburst from Milky Way's Black Hole". NASA. Archived from the original on January 6, 2015. Retrieved January 6, 2015.
  45. ^ "Our Galaxy's Supermassive Black Hole Has Emitted a Mysteriously Bright Flare". Science Alert. August 12, 2019. Archived from the original on August 12, 2019. Retrieved August 12, 2019.
  46. ^ Overbye, Dennis (June 8, 2023). "Our Local Black Hole Serves Up an 'Awe Moment' – Filaments of radio energy from Sagittarius A*, the black hole at the center of the Milky Way galaxy, are turning astronomers' heads". The New York Times. Archived from the original on June 8, 2023. Retrieved June 9, 2023.
  47. ^ "Cloudlets swarm around our local supermassive black hole". www.eso.org. Archived from the original on October 22, 2018. Retrieved October 22, 2018.
  48. ^ "Most Detailed Observations of Material Orbiting close to a Black Hole". European Southern Observatory (ESO). Archived from the original on November 1, 2018. Retrieved November 1, 2018.
  49. ^ Genzel; et al. (July 26, 2018). "Detection of the gravitational redshift in the orbit of the star S2 near the Galactic centre massive black hole". Astronomy & Astrophysics. 615: L15. arXiv:1807.09409. Bibcode:2018A&A...615L..15G. doi:10.1051/0004-6361/201833718. S2CID 118891445. Archived from the original on April 4, 2019. Retrieved July 27, 2018.
  50. ^ "Star spotted speeding near black hole at centre of Milky Way – Chile's Very Large Telescope tracks S2 star as it reaches mind-boggling speeds by supermassive black hole". The Guardian. July 26, 2017. Archived from the original on April 4, 2019. Retrieved July 27, 2018.
  51. ^ a b Lu, R.; et al. (2018). "Detection of intrinsic source structure at ~3 Schwarzschild radii with Millimeter-VLBI observations of Sgr A*". Astrophysical Journal. 859 (1): 60. arXiv:1805.09223. doi:10.3847/1538-4357/aabe2e. S2CID 51917277.
  52. ^ Issaoun, S. (January 18, 2019). "The Size, Shape, and Scattering of Sagittarius A* at 86 GHz: First VLBI with ALMA". The Astrophysical Journal. 871 (1): 30. arXiv:1901.06226. Bibcode:2019ApJ...871...30I. doi:10.3847/1538-4357/aaf732. S2CID 84180473.
  53. ^ Rezzolla, Luciano (April 17, 2018). "Astrophysicists Test Theories of Gravity with Black Hole Shadows". SciTech Daily. Archived from the original on April 2, 2019. Retrieved April 2, 2019.
  54. ^ "Revealing the black hole at the heart of the galaxy". Netherlands Research School for Astronomy. January 22, 2019. Archived from the original on March 18, 2019. Retrieved April 2, 2019 – via Phys.org.
  55. ^ Schödel et al. 2009
  56. ^ "Integral rolls back history of Milky Way's super-massive black hole". Hubble News Desk. January 28, 2005. Archived from the original on October 16, 2012. Retrieved October 31, 2007.
  57. ^ Revnivtsev, M. G.; et al. (October 2004). "Hard X-ray view of the past activity of Sgr A$^{\star}$ in a natural Compton mirror". Astronomy & Astrophysics. 425 (3): L49–L52. arXiv:astro-ph/0408190. Bibcode:2004A&A...425L..49R. doi:10.1051/0004-6361:200400064. ISSN 0004-6361. S2CID 18872302.
  58. ^ Nobukawa, M.; et al. (September 8, 2011). "New Evidence for High Activity of the Supermassive Black Hole in our Galaxy". The Astrophysical Journal. 739 (2): L52. arXiv:1109.1950. Bibcode:2011ApJ...739L..52N. doi:10.1088/2041-8205/739/2/L52. ISSN 2041-8205. S2CID 119244398.
  59. ^ Overbye, Dennis (November 14, 2019). "A Black Hole Threw a Star Out of the Milky Way Galaxy – So long, S5-HVS1, we hardly knew you". The New York Times. Archived from the original on November 17, 2019. Retrieved November 18, 2019.
  60. ^ Koposov, Sergey E; et al. (January 11, 2020). "Discovery of a nearby 1700 km s−1 star ejected from the Milky Way by Sgr A*". Monthly Notices of the Royal Astronomical Society. 491 (2): 2465–2480. arXiv:1907.11725. doi:10.1093/mnras/stz3081. ISSN 0035-8711. S2CID 198968336.
  61. ^ Eckart, Andreas; Tursunov, A.A.; Zajacek, M.; Parsa, M.; Hosseini, E.; Subroweit, M.; Peissker, F.; Straubmeier, C.; Horrobin, M.; Karas, V. (February 1, 2019). "Mass, Distance, Spin, Charge, and Orientation of the super massive black hole SgrA*". Proceedings of Science. 342. Sissa Medialab: 048. doi:10.22323/1.342.0048. S2CID 189921901.
  62. ^ a b c Daly, Ruth A; Donahue, Megan; O'Dea, Christopher P; Sebastian, Biny; Haggard, Daryl; Lu, Anan (October 28, 2023). "New black hole spin values for Sagittarius A* obtained with the outflow method". Monthly Notices of the Royal Astronomical Society. 527 (1): 428–436. arXiv:2310.12108. doi:10.1093/mnras/stad3228. ISSN 0035-8711.
  63. ^ Fragione, Giacomo; Loeb, Abraham (October 1, 2020). "An Upper Limit on the Spin of SgrA* Based on Stellar Orbits in Its Vicinity". The Astrophysical Journal. 901 (2): L32. arXiv:2008.11734. Bibcode:2020ApJ...901L..32F. doi:10.3847/2041-8213/abb9b4. ISSN 2041-8213.
  64. ^ Bélanger, G; Terrier, R; Jager, O C de; Goldwurm, A; Melia, F (December 1, 2006). "Periodic Modulations in an X-ray Flare from Sagittarius A*". Journal of Physics: Conference Series. 54: 420–426. arXiv:astro-ph/0604337. Bibcode:2006JPhCS..54..420B. doi:10.1088/1742-6596/54/1/066. ISSN 1742-6588. S2CID 250670477.
  65. ^ Meyer, L.; Eckart, A.; Schödel, R.; Duschl, W. J.; Mužić, K.; Dovčiak, M.; Karas, V. (December 2006). "Near-infrared polarimetry setting constraints on the orbiting spot model for Sgr A* flares". Astronomy & Astrophysics. 460 (1): 15–21. arXiv:astro-ph/0610104. Bibcode:2006A&A...460...15M. doi:10.1051/0004-6361:20065925. ISSN 0004-6361. S2CID 15370123.
  66. ^ Genzel, R.; Schödel, R.; Ott, T.; Eckart, A.; Alexander, T.; Lacombe, F.; Rouan, D.; Aschenbach, B. (November 2003). "Near-infrared flares from accreting gas around the supermassive black hole at the Galactic Centre". Nature. 425 (6961): 934–937. arXiv:astro-ph/0310821. Bibcode:2003Natur.425..934G. doi:10.1038/nature02065. ISSN 0028-0836. PMID 14586462. S2CID 4325930.
  67. ^ Daly, Ruth A (October 20, 2022). "Robust supermassive black hole spin mass-energy characteristics: a new method and results". Monthly Notices of the Royal Astronomical Society. 517 (4): 5144–5159. arXiv:2210.07779. doi:10.1093/mnras/stac2976. ISSN 0035-8711.
  68. ^ Eisenhauer, F.; et al. (July 20, 2005). "SINFONI in the Galactic Center: Young Stars and Infrared Flares in the Central Light-Month". The Astrophysical Journal. 628 (1): 246–259. arXiv:astro-ph/0502129. Bibcode:2005ApJ...628..246E. doi:10.1086/430667. S2CID 122485461.
  69. ^ "First Successful Test of Einstein's General Relativity Near Supermassive Black Hole – Culmination of 26 years of ESO observations of the heart of the Milky Way". www.eso.org. Archived from the original on March 8, 2019. Retrieved December 15, 2021.
  70. ^ a b GRAVITY Collaboration; Abuter, R.; Amorim, A.; Anugu, N.; Bauböck, M.; Benisty, M.; Berger, J. P.; Blind, N.; Bonnet, H.; Brandner, W.; Buron, A. (July 2018). "Detection of the gravitational redshift in the orbit of the star S2 near the Galactic centre massive black hole". Astronomy & Astrophysics. 615: L15. arXiv:1807.09409. Bibcode:2018A&A...615L..15G. doi:10.1051/0004-6361/201833718. ISSN 0004-6361. S2CID 118891445. Archived from the original on July 27, 2020. Retrieved December 15, 2021.
  71. ^ "Watch stars move around the Milky Way's supermassive black hole in deepest images yet". www.eso.org. Archived from the original on December 14, 2021. Retrieved December 15, 2021.
  72. ^ GRAVITY Collaboration; Stadler, J.; Drescher, A. (December 14, 2021). "Deep images of the Galactic center with GRAVITY". Astronomy & Astrophysics. 657: A82. arXiv:2112.07477. doi:10.1051/0004-6361/202142459. ISSN 0004-6361. S2CID 245131155.
  73. ^ GRAVITY Collaboration; Abuter, R.; Aimar, N.; Amorim, A.; Ball, J.; Bauböck, M.; Gillessen, S.; Widmann, F.; Heissel, G. (December 14, 2021). "Mass distribution in the Galactic Center based on interferometric astrometry of multiple stellar orbits". Astronomy & Astrophysics. 657: L12. arXiv:2112.07478. doi:10.1051/0004-6361/202142465. ISSN 0004-6361. S2CID 245131377.
  74. ^ Eckart, A.; Genzel, R.; Ott, T.; Schödel, R. (April 11, 2002). "Stellar orbits near Sagittarius A*". Monthly Notices of the Royal Astronomical Society. 331 (4): 917–934. arXiv:astro-ph/0201031. Bibcode:2002MNRAS.331..917E. doi:10.1046/j.1365-8711.2002.05237.x. ISSN 0035-8711. S2CID 11167996.
  75. ^ Peissker, Florian; Eckart, Andreas; Parsa, Marzieh (January 2020). "S62 on a 9.9 year orbit around SgrA*". The Astrophysical Journal. 889 (1): 61. arXiv:2002.02341. Bibcode:2020ApJ...889...61P. doi:10.3847/1538-4357/ab5afd. S2CID 211043784.
  76. ^ Peißker, Florian; Eckart, Andreas; Zajaček, Michal; Basel, Ali; Parsa, Marzieh (August 2020). "S62 and S4711: Indications of a Population of Faint Fast-moving Stars inside the S2 Orbit—S4711 on a 7.6 yr Orbit around Sgr A*". The Astrophysical Journal. 889 (50): 5. arXiv:2008.04764. Bibcode:2020ApJ...899...50P. doi:10.3847/1538-4357/ab9c1c. S2CID 221095771.
  77. ^ Næss, S. (October 4, 2019). "Galactic center S-star orbital parameters".
  78. ^ Matson, John (October 22, 2012). "Gas Guzzler: Cloud Could Soon Meet Its Demise in Milky Way's Black Hole". Scientific American. Archived from the original on June 19, 2013. Retrieved October 30, 2012.
  79. ^ a b Gillessen, S.; Genzel, R.; Fritz, T. K.; Quataert, E.; Alig, C.; Burkert, A.; Cuadra, J.; Eisenhauer, F.; Pfuhl, O.; Dodds-Eden, K.; Gammie, C. F.; Ott, T. (January 2012). "A gas cloud on its way towards the supermassive black hole at the Galactic Centre". Nature. 481 (7379): 51–54. arXiv:1112.3264. Bibcode:2012Natur.481...51G. doi:10.1038/nature10652. ISSN 0028-0836. PMID 22170607. S2CID 4410915.
  80. ^ a b c Witzel, G.; Ghez, A. M.; Morris, M. R.; Sitarski, B. N.; Boehle, A.; Naoz, S.; Campbell, R.; Becklin, E. E.; G. Canalizo; Chappell, S.; Do, T.; Lu, J. R.; Matthews, K.; Meyer, L.; Stockton, A.; Wizinowich, P.; Yelda, S. (January 1, 2014). "Detection of Galactic Center Source G2 at 3.8 μm during Periapse Passage". Astrophysical Journal Letters. 796 (1): L8. arXiv:1410.1884. Bibcode:2014ApJ...796L...8W. doi:10.1088/2041-8205/796/1/L8. S2CID 36797915.
  81. ^ Bartos, Imre; Haiman, Zoltán; Kocsis, Bence; Márka, Szabolcs (May 2013). "Gas Cloud G2 Can Illuminate the Black Hole Population Near the Galactic Center". Physical Review Letters. 110 (22): 221102 (5 pages). arXiv:1302.3220. Bibcode:2013PhRvL.110v1102B. doi:10.1103/PhysRevLett.110.221102. PMID 23767710. S2CID 12284209.
  82. ^ de la Fuente Marcos, R.; de la Fuente Marcos, C. (August 2013). "Colliding with G2 near the Galactic Centre: a geometrical approach". Monthly Notices of the Royal Astronomical Society: Letters. 435 (1): L19–L23. arXiv:1306.4921. Bibcode:2013MNRAS.435L..19D. doi:10.1093/mnrasl/slt085. S2CID 119287777.
  83. ^ Morris, Mark (January 4, 2012). "Astrophysics: The Final Plunge". Nature. 481 (7379): 32–33. Bibcode:2012Natur.481...32M. doi:10.1038/nature10767. PMID 22170611. S2CID 664513.
  84. ^ Gillessen. "Wiki Page of Proposed Observations of G2 Passage". Archived from the original on February 1, 2014. Retrieved October 30, 2012.
  85. ^ "A Black Hole's Dinner is Fast Approaching". ESO. December 14, 2011. Archived from the original on February 13, 2012. Retrieved February 27, 2015.
  86. ^ H Hirschfeld, Robert (October 22, 2012). "Milky Way's black hole getting ready for snack". Lawrence Livermore National Laboratory. Archived from the original on June 19, 2013. Retrieved February 27, 2015.
  87. ^ Taylor Tillman, Nola (April 28, 2014). "Doomed Space Cloud Nears Milky Way's Black Hole as Scientists Watch". Space.com. Retrieved September 15, 2024. Cosmic encounter that might reveal new secrets on how such supermassive black holes evolve; We get to watch it unfolding in a human lifetime, which is very unusual and very exciting
  88. ^ a b Cowen, Ron (2014). "Why galactic black hole fireworks were a flop : Nature News & Comment". Nature. doi:10.1038/nature.2014.15591. S2CID 124346286. Archived from the original on February 19, 2015. Retrieved February 27, 2015.
  89. ^ Pfuhl, Oliver; Gillessen, Stefan; Eisenhauer, Frank; Genzel, Reinhard; Plewa, Philipp M.; Thomas Ott; Ballone, Alessandro; Schartmann, Marc; Burkert, Andreas (2015). "The Galactic Center Cloud G2 and its Gas Streamer". The Astrophysical Journal. 798 (2): 111. arXiv:1407.4354. Bibcode:2015ApJ...798..111P. doi:10.1088/0004-637x/798/2/111. ISSN 0004-637X. S2CID 118440030.
  90. ^ "How G2 survived the black hole at our Milky Way's heart - EarthSky.org". November 4, 2014. Archived from the original on February 5, 2016. Retrieved February 14, 2016.
  91. ^ "Simulation of gas cloud after close approach to the black hole at the centre of the Milky Way". ESO. Archived from the original on March 7, 2015. Retrieved February 27, 2015.

Further reading

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