---
title: Sagittarius A*
canonical_url: https://paxabyssi.com/wiki/Sagittarius_A*
markdown_url: https://paxabyssi.com/wiki/Sagittarius_A*.md
type: wiki-page
revision_id: 587
revision_view: stable
last_updated: 2026-09-28
license: CC BY-SA 4.0
license_url: https://creativecommons.org/licenses/by-sa/4.0/
science_status:
  - observed
  - model
  - sim
summary: The supermassive black hole at the centre of the Milky Way, 4.3 million times the mass of the Sun, weighed by the stars that orbit it and imaged by the Event Horizon Telescope in 2022.
categories:
  - Black holes
  - Supermassive black holes
  - Galactic Centre
  - Named objects
aliases:
  - Sgr A*
  - Sgr A star
  - Sagittarius A star
  - SgrA*
  - Galactic Centre black hole
  - Milky Way black hole
infobox:
  type: black_hole
  jet: none confirmed
  class: supermassive
  image: File:Sagittarius_A_star_EHT_2022.jpg
  isco_km:
    non_spinning: 38100000
    prograde_a_0.9: 14700000
  evidence:
    - stellar orbits
    - horizon-scale imaging
  sim_stop: yes
  mass_msun:
    error: 0.012e6 statistical, about 0.04e6 systematic
    value: 4297000
    source: GRAVITY Collaboration 2022; 4.2996e6 in GRAVITY Collaboration 2024
  distance_ly: 27000
  distance_pc:
    error: 9 statistical, 33 systematic
    value: 8277
    source: GRAVITY Collaboration 2022
  spin_a_star: not measured; image models disfavour a non-spinning hole and a retrograde flow
  constellation: Sagittarius
  image_caption: "Observation: the Event Horizon Telescope's image of Sagittarius A*, 2022"
  discovery_year: 1974
  position_j2000: RA 17h 45m 40.04s, Dec -29 deg 00 min 28.2 s
  accretion_state: starved; hot, radiatively inefficient flow; about 1e-9 of the Eddington luminosity
  photon_sphere_km: 19000000
  schwarzschild_radius_au: 0.085
  schwarzschild_radius_km: 12700000
  nearest_well_studied_star: "S2: period 16.05 yr, eccentricity 0.88, pericentre 120 AU"
  accretion_rate_msun_per_yr: about 5e-9 to 1e-8 (models); 2e-9 to 2e-7 (Faraday rotation limits)
  bolometric_luminosity_erg_s: about 7e35 to 9e35 (favoured models), about 200 times the Sun
  shadow_angular_diameter_uas:
    measured_ring: 51.8 +/- 2.3
    measured_shadow: 48.7 +/- 7.0
    predicted_non_spinning: 53
  tidal_disruption_radius_sun_like_star_au: 0.76
related:
  - https://paxabyssi.com/wiki/Black_hole.md
  - https://paxabyssi.com/wiki/Milky_Way.md
  - https://paxabyssi.com/wiki/Neutron_star.md
  - https://paxabyssi.com/wiki/Orbit.md
  - https://paxabyssi.com/wiki/Star_catalogue.md
---

# Sagittarius A\*

> Source: https://paxabyssi.com/wiki/Sagittarius_A*
>
> Licence: [CC BY-SA 4.0](https://creativecommons.org/licenses/by-sa/4.0/). Text by Pax Abyssi Wiki contributors; history at https://paxabyssi.com/wiki/Sagittarius_A*/history
>
> Revision 587, 28 September 2026

**Sagittarius A\***, usually written **Sgr A\***, is the supermassive black hole at the centre of the Milky Way. It holds about 4.3 million times the mass of the Sun in a region smaller than the orbit of Mercury, and it lies about 8.3 kiloparsecs (27,000 light years) away in the direction of the constellation Sagittarius. It is the nearest supermassive black hole to Earth, which makes it the one astronomers can study in the most detail: its mass is known to better than one per cent from the orbits of individual stars, and in 2022 it became the second black hole ever imaged [1] [2].

In Pax Abyssi, Sagittarius A\* is a place you can fly to. The game draws it as the science says it would look from close by: a black shadow about ten degrees across, with no bright disk, because the real hole has almost nothing to eat, hung in the densest star field in the Galaxy, whose light the hole bends round its edge. The star S2 swings round it on its measured 16-year orbit.

![A glowing orange ring with three brighter knots surrounding a dark centre, on a black background.](https://media.paxabyssi.com/public/372c24c62809ee4455648fc520296d649c5d11751650cce146fb5013a261fd1c/2560.webp "Observation: the first image of Sagittarius A*, made by the Event Horizon Telescope from observations in April 2017 at 1.3 mm wavelength. The dark centre is the black hole's shadow; the ring is hot gas whose light is bent around it. Credit: EHT Collaboration.")

*Figure 1.* Observation: the first image of Sagittarius A\*, made by the Event Horizon Telescope from observations in April 2017 at 1.3 mm wavelength. The dark centre is the black hole's shadow; the ring is hot gas whose light is bent around it. Credit: EHT Collaboration. Licence: CC BY 4.0.

## Discovery

In 1974 Bruce Balick and Robert Brown used a radio interferometer in West Virginia to find a bright, extremely compact radio source at the dynamical centre of the Galaxy [3]. It is the object now called Sgr A\*. A compact radio source alone did not prove a black hole: dust in the Galactic plane dims visible light from the centre by a factor of about a trillion, so nobody could see what surrounded it [4].

The proof came from infrared light, which passes through the dust. From the early 1990s two teams, one led by Reinhard Genzel in Germany and one by Andrea Ghez in the United States, tracked the stars closest to Sgr A\* year after year, using adaptive optics to undo the blurring of Earth's atmosphere. Their stars move on tight Keplerian orbits around an invisible point [5] [6]. The two leaders shared half of the 2020 Nobel Prize in Physics "for the discovery of a supermassive compact object at the centre of our galaxy" [7].

## Weighing a black hole with a star

The star S2 is the best clock around Sgr A\*. It is a young B-type star of about 14 solar masses [8] that circles the black hole every 16.05 years on an orbit with eccentricity 0.88. At its closest, in May 2018, it passed 120 AU from the hole, about 1,400 Schwarzschild radii, moving at about 7,650 km/s, or 2.5 per cent of the speed of light [9].

That orbit is enough to weigh the hole. Kepler's third law, written in solar-system units, says that the total mass in solar masses equals the cube of the semi-major axis in astronomical units divided by the square of the period in years:

$$
M \approx \frac{a^3}{P^2} = \frac{(1{,}035\ \mathrm{AU})^3}{(16.05\ \mathrm{yr})^2} \approx 4.3 \times 10^{6}\ M_\odot .
$$

Fitting the orbits of S2 and three other stars measured with the GRAVITY instrument, which combines the four 8-metre telescopes of ESO's Very Large Telescope, gives $M = 4.297 \times 10^6$ solar masses with a statistical uncertainty of about 0.3 per cent, and a distance of $R_0 = 8{,}277$ parsecs [1]. Any extra matter spread through S2's orbit, such as a cloud of faint stars or dark matter, can add at most about 1,200 solar masses [10]. Nothing but a black hole can pack so much mass into so small a space for long.

### General relativity in the orbit of a star

S2 is also a test of Einstein's theory. Near pericentre its light is shifted to the red by about 200 km/s more than Newton's gravity predicts, the combined effect of the hole's gravitational redshift and the star's time dilation, exactly as general relativity requires [9]. Its orbit also turns slowly in its own plane. General relativity predicts a periapsis shift per orbit of

$$
\Delta\phi = \frac{6\pi G M}{c^2 a (1 - e^2)},
$$

which for S2 is about 12 arcminutes per orbit. GRAVITY measured it in 2020 [11]. For comparison, the same formula gives Mercury's famous relativistic precession of 43 arcseconds per century, about a tenth of an arcsecond per Mercury orbit: S2's orbit swings about seven thousand times further each lap.

## The image of the shadow

A black hole of this mass has a Schwarzschild radius of about 12.7 million km (0.085 AU, some 18 times the Sun's radius). General relativity predicts that its shadow, seen from Earth, spans about 53 microarcseconds. That is the width of a 10 cm doughnut lying on the Moon, seen from Earth.

The Event Horizon Telescope reached that resolution by linking eight radio telescopes at six sites, from Hawaii to the South Pole, observing at a wavelength of 1.3 mm in April 2017. The team found a bright, thick ring 51.8 ± 2.3 microarcseconds across around a dimmer centre [2]. The ring's size matches the prediction for a Kerr black hole of the mass measured from the stars to within about 10 per cent, and a star-like object with a hot surface is ruled out [12]. The image took five years longer than that of M87\* partly because Sgr A\* changes within the hour: gas near its inner edge orbits in about half an hour, while the matching timescale for M87\*, 1,500 times heavier, is weeks.

In 2024 the collaboration published the ring in polarised light. It is strongly polarised, up to about 40 per cent, in a spiral pattern that traces an ordered magnetic field threading the hot gas [13].

![The orange ring of Sagittarius A\* overlaid with fine curved lines that spiral around the dark centre.](https://media.paxabyssi.com/public/3b0a4b53194adbbae75f93b4fe105d489b83fd62a37340b91a7d3a6d744ed661/2560.webp "Observation: Sagittarius A* in polarised light. The lines show the orientation of the polarisation, which follows the magnetic field around the black hole. Credit: EHT Collaboration.")

*Figure 2.* Observation: Sagittarius A\* in polarised light. The lines show the orientation of the polarisation, which follows the magnetic field around the black hole. Credit: EHT Collaboration. Licence: CC BY 4.0.

### What the image says about spin

Sgr A\*'s spin is **not measured**. The collaboration compared its images and light curves with a large library of computer simulations. Models of a non-spinning hole, of gas orbiting against the hole's spin, and of a hole seen at more than about 50 degrees from its axis all fit poorly [2]. The most promising cluster of models has a strongly magnetised flow seen within 30 degrees of face-on, but every model fails at least one of the eleven tests, most often the observed variability [14]. Any single spin value quoted for Sgr A\* is a model preference.

## A starving black hole

Sgr A\* is astonishingly faint for its size. The favoured models have it swallowing about 5 to 10 billionths of a solar mass a year, one Moon's worth of gas every four to seven years, and shining at under $10^{36}$ erg/s, about 200 times the Sun's output [14]. Measurements of how the polarised radio light is twisted on its way out limit the inflow near the hole to between about $2 \times 10^{-9}$ and $2 \times 10^{-7}$ solar masses a year [15]. That is a billion times below the Eddington limit, the brightness at which radiation pressure would halt the inflow. The gas forms a hot, tenuous, puffed-up flow that radiates mainly in radio and submillimetre waves. No jet has been confirmed.

It is not quiet. X-ray flares, in which the source brightens by tens of times within an hour, were discovered in 2000 and recur often [16]. In the near infrared, GRAVITY has watched flares whose light moves in a loop on the sky with a period of about 45 minutes, as a hot spot orbiting at six to ten gravitational radii, just outside the innermost stable orbit, would [17].

## Neighbourhood

Sgr A\* sits at the heart of the Galaxy's nuclear star cluster, the densest stellar system in the Milky Way, with millions of stars within a few parsecs. The S-stars, S2 among them, crowd within a few hundredths of a parsec; a disk of young, massive stars circles further out; streamers of ionised gas called the minispiral fall towards the centre, and a ring of molecular gas lies beyond, a few parsecs from the hole [4].

A Sun-like star that strayed too close would be torn apart. For Sgr A\* the tidal disruption radius, $R_\star (M_\mathrm{BH}/M_\star)^{1/3}$, is about 160 solar radii or 0.76 AU, nine times the Schwarzschild radius, so the star would be shredded well outside the horizon and part of its gas would light up as a flare lasting months [18]. No such event has been seen from Sgr A\*.

![A star traces a sequence of overlapping elliptical loops that form a rosette around a central point.](https://media.paxabyssi.com/public/a528e685b4bd5c5c787f088cde1a67e4a9d5b9a5518688b69a43b59acf07fca1/2560.webp "Artist's impression: the orbit of S2 turns a little each time around Sagittarius A*, tracing a rosette. The effect is exaggerated here; the real shift is about 12 arcminutes per orbit. Credit: ESO/L. Calçada.")

*Figure 3.* Artist's impression: the orbit of S2 turns a little each time around Sagittarius A\*, tracing a rosette. The effect is exaggerated here; the real shift is about 12 arcminutes per orbit. Credit: ESO/L. Calçada. Licence: CC BY 4.0.

> **Numbers at a glance**
>
> - Mass: 4.30 million solar masses. Distance: 8.28 kpc.
> - Schwarzschild radius: 12.7 million km. Mercury's orbit is more than four times as wide as the horizon.
> - Light orbiting at the photon sphere takes about 11.5 minutes per lap; a particle at the innermost stable orbit of a non-spinning hole of this mass takes about 33 minutes.
> - Its shadow on our sky: about 50 microarcseconds.

> **In Pax Abyssi**
>
> Sagittarius A\* is one of the game's five black-hole stops. Its mass (4,297,000 solar masses) and distance (8,277 pc) come from the game's catalogue of known black holes, citing the GRAVITY measurement. The star S2 is placed with it, at 13.6 solar masses on its 16.05-year orbit, whose semi-major axis of about 1,034 AU follows from Kepler's law and the hole's mass. The ship arrives 30 Schwarzschild radii out, about 2.5 AU, where the shadow spans about 10 degrees of sky.
>
> No thin disk is drawn, because the real hole has none: its hot, thin flow is all but invisible to the eye. The sky round it is rebuilt from the hole's own position, from inside the nuclear star cluster, and every ray of it is bent through the Kerr geometry at a spin of 0.9, a ruled choice inside the range the image models allow. Like every black hole in the game, Sagittarius A\* is getting the artist's vision as its default look, with the scientific setting one step back (see [Black hole](https://paxabyssi.com/wiki/Black_hole.md)).

## Things we haven't modelled yet

Our aim at the centre of the Galaxy is the same as everywhere: full scientific realism, always available as an option. Next:

- **The flares.** Sagittarius A\* brightens tens of times in X-rays within an hour [16], and in the near infrared a hot spot circles it about every 45 minutes [17]. We want you to watch one go round.
- **The S-stars in motion.** S2 and its neighbours swinging round the hole on their measured orbits, S2 passing within 120 AU of it every 16 years [9].
- **The glow of the hot flow**, the faint ring the Event Horizon Telescope saw, as an option for eyes that see beyond visible light.
- **Stars torn apart.** A star strayed inside 0.76 AU, shredded, and the months-long flare that follows [18].

## See also

- [Black hole](https://paxabyssi.com/wiki/Black_hole.md)
- [Milky Way](https://paxabyssi.com/wiki/Milky_Way.md)
- [Orbit](https://paxabyssi.com/wiki/Orbit.md)
- [Neutron star](https://paxabyssi.com/wiki/Neutron_star.md)
- [Star catalogue](https://paxabyssi.com/wiki/Star_catalogue.md)

## References

1. GRAVITY Collaboration (2022). Mass distribution in the Galactic Center based on interferometric astrometry of multiple stellar orbits. Astronomy & Astrophysics 657, L12. <https://doi.org/10.1051/0004-6361/202142465>
2. Event Horizon Telescope Collaboration (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, L12. <https://doi.org/10.3847/2041-8213/ac6674>
3. Balick, B. and Brown, R. L. (1974). Intense sub-arcsecond structure in the galactic center. The Astrophysical Journal 194, 265. <https://doi.org/10.1086/153242>
4. Genzel, R., Eisenhauer, F. and Gillessen, S. (2010). The Galactic Center massive black hole and nuclear star cluster. Reviews of Modern Physics 82, 3121-3195. <https://doi.org/10.1103/RevModPhys.82.3121>
5. Schödel, R. and et al. (2002). A star in a 15.2-year orbit around the supermassive black hole at the centre of the Milky Way. Nature 419, 694-696. <https://doi.org/10.1038/nature01121>
6. Ghez, A. M. and et al. (2008). Measuring Distance and Properties of the Milky Way's Central Supermassive Black Hole with Stellar Orbits. The Astrophysical Journal 689, 1044-1062. <https://doi.org/10.1086/592738>
7. Nobel Prize Outreach (2020). The Nobel Prize in Physics 2020: summary. NobelPrize.org. <https://www.nobelprize.org/prizes/physics/2020/summary/>
8. Habibi, M. and et al. (2017). Twelve Years of Spectroscopic Monitoring in the Galactic Center: The Closest Look at S-stars near the Black Hole. The Astrophysical Journal 847, 120. <https://doi.org/10.3847/1538-4357/aa876f>
9. GRAVITY Collaboration (2018). Detection of the gravitational redshift in the orbit of the star S2 near the Galactic centre massive black hole. Astronomy & Astrophysics 615, L15. <https://doi.org/10.1051/0004-6361/201833718>
10. GRAVITY Collaboration (2024). Improving constraints on the extended mass distribution in the Galactic Center with stellar orbits. Astronomy & Astrophysics 692, A242. <https://doi.org/10.1051/0004-6361/202452274>
11. GRAVITY Collaboration (2020). Detection of the Schwarzschild precession in the orbit of the star S2 near the Galactic centre massive black hole. Astronomy & Astrophysics 636, L5. <https://doi.org/10.1051/0004-6361/202037813>
12. Event Horizon Telescope Collaboration (2022). First Sagittarius A\* Event Horizon Telescope Results. VI. Testing the Black Hole Metric. The Astrophysical Journal Letters 930, L17. <https://doi.org/10.3847/2041-8213/ac6756>
13. Event Horizon Telescope Collaboration (2024). First Sagittarius A\* Event Horizon Telescope Results. VII. Polarization of the Ring. The Astrophysical Journal Letters 964, L25. <https://doi.org/10.3847/2041-8213/ad2df0>
14. Event Horizon Telescope Collaboration (2022). First Sagittarius A\* Event Horizon Telescope Results. V. Testing Astrophysical Models of the Galactic Center Black Hole. The Astrophysical Journal Letters 930, L16. <https://doi.org/10.3847/2041-8213/ac6672>
15. Marrone, D. P. et al. (2007). An Unambiguous Detection of Faraday Rotation in Sagittarius A\*. The Astrophysical Journal 654, L57-L60. <https://doi.org/10.1086/510850>
16. Baganoff, F. K. and et al. (2001). Rapid X-ray flaring from the direction of the supermassive black hole at the Galactic Centre. Nature 413, 45-48. <https://doi.org/10.1038/35092510>
17. GRAVITY Collaboration (2018). Detection of orbital motions near the last stable circular orbit of the massive black hole SgrA\*. Astronomy & Astrophysics 618, L10. <https://doi.org/10.1051/0004-6361/201834294>
18. Rees, M. J. (1988). Tidal disruption of stars by black holes of 10^6-10^8 solar masses in nearby galaxies. Nature 333, 523-528. <https://doi.org/10.1038/333523a0>

## Infobox (black hole)

| Field | Value |
| --- | --- |
| Jet | none confirmed |
| Class | supermassive |
| Image | File:Sagittarius_A_star_EHT_2022.jpg |
| Evidence | stellar orbits, horizon-scale imaging |
| Sim stop | yes |
| Mass msun | 4297000 |
| Distance ly | 27000 |
| Distance pc | 8277 |
| Spin a star | not measured; image models disfavour a non-spinning hole and a retrograde flow |
| Constellation | Sagittarius |
| Image caption | Observation: the Event Horizon Telescope's image of Sagittarius A*, 2022 |
| Discovery year | 1974 |
| Position j2000 | RA 17h 45m 40.04s, Dec -29 deg 00 min 28.2 s |
| Accretion state | starved; hot, radiatively inefficient flow; about 1e-9 of the Eddington luminosity |
| Photon sphere km | 19000000 |
| Schwarzschild radius au | 0.085 |
| Schwarzschild radius km | 12700000 |
| Nearest well studied star | S2: period 16.05 yr, eccentricity 0.88, pericentre 120 AU |
| Accretion rate msun per yr | about 5e-9 to 1e-8 (models); 2e-9 to 2e-7 (Faraday rotation limits) |
| Bolometric luminosity erg s | about 7e35 to 9e35 (favoured models), about 200 times the Sun |
| Tidal disruption radius sun like star au | 0.76 |

## Related pages

- [Black hole](https://paxabyssi.com/wiki/Black_hole.md): A region of spacetime where gravity is so strong that nothing, light included, can climb back out; the collapsed remains of massive stars, and the giants at the centres of galaxies.
- [Milky Way](https://paxabyssi.com/wiki/Milky_Way.md): The barred spiral galaxy that contains the Sun, some 100 to 400 billion stars in a disk about 30 kiloparsecs across, and the setting of Pax Abyssi.
- [Neutron star](https://paxabyssi.com/wiki/Neutron_star.md): The collapsed core of a massive star, more massive than the Sun yet only about 24 km across; seen as radio pulsars, millisecond pulsars, magnetars and X-ray pulsars.
- [Orbit](https://paxabyssi.com/wiki/Orbit.md): The path one body follows around another under gravity. For two bodies alone it is an ellipse, fixed by Kepler's three laws and described by six orbital elements.
- [Star catalogue](https://paxabyssi.com/wiki/Star_catalogue.md): The 119,626 real stars at the heart of Pax Abyssi, built from the HYG database and corrected against Gaia DR3, Hipparcos, XHIP and the Washington Double Star Catalog, with every correction kept beside the original value.

Categories: [Black holes](https://paxabyssi.com/wiki/Category:Black_holes.md), [Supermassive black holes](https://paxabyssi.com/wiki/Category:Supermassive_black_holes.md), [Galactic Centre](https://paxabyssi.com/wiki/Category:Galactic_Centre.md), [Named objects](https://paxabyssi.com/wiki/Category:Named_objects.md)
