Artist concept of a SMBH consuming matter from a nearby star
A supermassive black hole (SMBH or sometimes SBH) is the largest type of black hole, containing a mass of the order of hundreds of thousands, to billions times, the mass of the Sun (M☉). This is a class of astronomical objects that has undergone gravitational collapse, leaving behind a spheroidal region of space from which nothing can escape; not even light. Observational evidence indicates that all, or nearly all, massive galaxies contain a supermassive black hole, located at the galaxy's center. In the case of the Milky Way, the supermassive black hole corresponds to the location of Sagittarius A* at the Galactic Core. Accretion of interstellar gas onto supermassive black holes is the process responsible for powering quasars and other types of active galactic nuclei.
Description
Supermassive black holes have properties that distinguish them from lower-mass classifications. First, the average density of a SMBH (defined as the mass of the black hole divided by the volume within its Schwarzschild radius) can be less than the density of water in the case of some SMBHs. This is because the Schwarzschild radius is directly proportional to its mass. Since the volume of a spherical object (such as the event horizon
of a non-rotating black hole) is directly proportional to the cube of
the radius, the density of a black hole is inversely proportional to the
square of the mass, and thus higher mass black holes have lower average density. In addition, the tidal forces in the vicinity of the event horizon
are significantly weaker for supermassive black holes. The tidal force
on a body at the event horizon is likewise inversely proportional to the
square of the mass: a person on the surface of the Earth and one at the event horizon of a 10 million M☉ black hole experience about the same tidal force between their head and feet. Unlike with stellar mass black holes, one would not experience significant tidal force until very deep into the black hole.
History of research
The story of how supermassive black holes were found began with the investigation by Maarten Schmidt of the radio source 3C 273
in 1963. Initially this was thought to be a star, but the spectrum
proved puzzling. It was determined to be hydrogen emission lines that
had been red shifted, indicating the object was moving away from the Earth. Hubble's law
showed that the object was located several billion light-years away,
and thus must be emitting the energy equivalent of hundreds of galaxies.
The rate of light variations of the source, dubbed a quasi-stellar object, or quasar, suggested the emitting region had a diameter of one parsec or less. Four such sources had been identified by 1964.
In 1963, Fred Hoyle and W. A. Fowler
proposed the existence of hydrogen burning supermassive stars (SMS) as
an explanation for the compact dimensions and high energy output of
quasars. These would have a mass of about 105 – 109 M☉. However, Richard Feynman
noted stars above a certain critical mass are dynamically unstable and
would collapse into a black hole, at least if they were non-rotating.
Fowler then proposed that these supermassive stars would undergo a
series of collapse and explosion oscillations, thereby explaining the
energy output pattern. Appenzeller and Fricke (1972) built models of
this behavior, but found that the resulting star would still undergo
collapse, concluding that a non-rotating 0.75×106 M☉ SMS "cannot escape collapse to a black hole by burning its hydrogen through the CNO cycle".
Edwin E. Salpeter and Yakov B. Zel'dovich
made the proposal in 1964 that matter falling onto a massive compact
object would explain the properties of quasars. It would require a mass
of around 108 M☉ to match the output of these objects. Donald Lynden-Bell noted in 1969 that the infalling gas would form a flat disk that spirals into the central "Schwarzschild throat". He noted that the relatively low output of nearby galactic cores implied these were old, inactive quasars. Meanwhile, in 1967, Martin Ryle and Malcolm Longair
suggested that nearly all sources of extra-galactic radio emission
could be explained by a model in which particles are ejected from
galaxies at relativistic velocities; meaning they are moving near the speed of light. Martin Ryle, Malcolm Longair, and Peter Scheuer then proposed in 1973 that the compact central nucleus could be the original energy source for these relativistic jets.
Arthur M. Wolfe and Geoffrey Burbidge noted in 1970 that the large velocity dispersion of the stars in the nuclear region of elliptical galaxies
could only be explained by a large mass concentration at the nucleus;
larger than could be explained by ordinary stars. They showed that the
behavior could be explained by a massive black hole with up to 1010 M☉, or a large number of smaller black holes with masses below 103 M☉. Dynamical evidence for a massive dark object was found at the core of the active elliptical galaxy Messier 87 in 1978, initially estimated at 5×109 M☉. Discovery of similar behavior in other galaxies soon followed, including the Andromeda Galaxy in 1984 and the Sombrero Galaxy in 1988.
Donald Lynden-Bell and Martin Rees hypothesized in 1971 that the center of the Milky Way galaxy would contain a massive black hole. Sagittarius A* was discovered and named on February 13 and 15, 1974, by astronomers Bruce Balick and Robert Brown using the Green Bank Interferometer of the National Radio Astronomy Observatory. They discovered a radio source that emits synchrotron radiation;
it was found to be dense and immobile because of its gravitation. This
was, therefore, the first indication that a supermassive black hole
exists in the center of the Milky Way.
The Hubble Space Telescope, launched in 1990, provided the resolution needed to perform more refined observations of galactic nuclei. In 1994 the Faint Object Spectrograph
on the Hubble was used to observe Messier 87, finding that ionized gas
was orbiting the central part of the nucleus at a velocity of ±500 km/s.
The data indicated a concentrated mass of (2.4±0.7)×109 M☉ lay within a 0.25″ span, providing strong evidence of a supermassive black hole. Using the Very Long Baseline Array to observe Messier 106 , Miyoshi et al. (1995) were able to demonstrate that the emission from an H2O maser in this galaxy came from a gaseous disk in the nucleus that orbited a concentrated mass of 3.6×107 M☉, which was constrained to a radius of 0.13 parsecs.
They noted that a swarm of solar mass black holes within a radius this
small would not survive for long without undergoing collisions, making a
supermassive black hole the sole viable candidate.
Formation
An artist's conception of a supermassive black hole and accretion disk
The origin of supermassive black holes remains an open field of
research. Astrophysicists agree that once a black hole is in place in
the center of a galaxy, it can grow by accretion
of matter and by merging with other black holes. There are, however,
several hypotheses for the formation mechanisms and initial masses of
the progenitors, or "seeds", of supermassive black holes.
One hypothesis is that the seeds are black holes of tens or
perhaps hundreds of solar masses that are left behind by the explosions
of massive stars and grow by accretion of matter. Another model
hypothesizes that before the first stars, large gas clouds could
collapse into a "quasi-star", which would in turn collapse into a black hole of around 20 M☉.
The "quasi-star" becomes unstable to radial perturbations because of
electron-positron pair production in its core and could collapse
directly into a black hole without a supernova
explosion (which would eject most of its mass, preventing the black
hole from growing as fast). Given sufficient mass nearby, the black hole
could accrete to become intermediate-mass black hole and possibly a SMBH if the accretion rate persists.
Artist's illustration of galaxy with jets from a supermassive black hole.
Another model involves a dense stellar cluster undergoing core-collapse as the negative heat capacity of the system drives the velocity dispersion in the core to relativistic speeds. Finally, primordial black holes could have been produced directly from external pressure in the first moments after the Big Bang.
These primordial black holes would then have more time than any of the
above models to accrete, allowing them sufficient time to reach
supermassive sizes. Formation of black holes from the deaths of the
first stars has been extensively studied and corroborated by
observations. The other models for black hole formation listed above are
theoretical.
The difficulty in forming a supermassive black hole resides in
the need for enough matter to be in a small enough volume. This matter
needs to have very little angular momentum in order for this to happen.
Normally, the process of accretion involves transporting a large initial
endowment of angular momentum outwards, and this appears to be the
limiting factor in black hole growth. This is a major component of the
theory of accretion disks.
Gas accretion is the most efficient and also the most conspicuous way
in which black holes grow. The majority of the mass growth of
supermassive black holes is thought to occur through episodes of rapid
gas accretion, which are observable as active galactic nuclei
or quasars. Observations reveal that quasars were much more frequent
when the Universe was younger, indicating that supermassive black holes
formed and grew early. A major constraining factor for theories of
supermassive black hole formation is the observation of distant luminous
quasars, which indicate that supermassive black holes of billions of
solar masses had already formed when the Universe was less than one
billion years old. This suggests that supermassive black holes arose
very early in the Universe, inside the first massive galaxies.
Artist’s impression of stars born in winds from supermassive black holes.
A vacancy exists in the observed mass distribution of black holes. Black holes that spawn from dying stars have masses 5–80 M☉.
The minimal supermassive black hole is approximately a hundred thousand
solar masses. Mass scales between these ranges are dubbed
intermediate-mass black holes. Such a gap suggests a different formation
process. However, some models suggest that ultraluminous X-ray sources (ULXs) may be black holes from this missing group.
There is, however, an upper limit to how large supermassive black holes can grow. So-called ultramassive black holes
(UMBHs), which are at least ten times the size of supermassive black
holes, appear to have a theoretical upper limit of around 50 billion
solar masses, as anything above this slows growth down to a crawl (the
slowdown tends to start around 10 billion solar masses) and causes the
unstable accretion disk surrounding the black hole to coalesce into
stars that orbit it.
A small minority of sources argue that distant supermassive black
holes whose large size is hard to explain so soon after the Big Bang,
such as ULAS J1342+0928, may be evidence that our universe is the result of a Big Bounce, instead of a Big Bang, with these supermassive black holes being formed before the Big Bounce.
Doppler measurements
Side view of black hole with transparent toroidal ring of ionised matter according to a proposed model for Sgr A*. This image shows the result of bending of light from behind the black hole, and it also shows the asymmetry arising by the Doppler effect from the extremely high orbital speed of the matter in the ring.
Some of the best evidence for the presence of black holes is provided by the Doppler effect
whereby light from nearby orbiting matter is red-shifted when receding
and blue-shifted when advancing. For matter very close to a black hole
the orbital speed must be comparable with the speed of light, so
receding matter will appear very faint compared with advancing matter,
which means that systems with intrinsically symmetric discs and rings
will acquire a highly asymmetric visual appearance. This effect has been
allowed for in modern computer generated images such as the example
presented here, based on a plausible model for the supermassive black hole in Sgr A*
at the centre of our own galaxy. However the resolution provided by
presently available telescope technology is still insufficient to
confirm such predictions directly.
What already has been observed directly in many systems are the
lower non-relativistic velocities of matter orbiting further out from
what are presumed to be black holes. Direct Doppler measures of water masers surrounding the nuclei of nearby galaxies have revealed a very fast Keplerian motion,
only possible with a high concentration of matter in the center.
Currently, the only known objects that can pack enough matter in such a
small space are black holes, or things that will evolve into black holes
within astrophysically short timescales. For active galaxies farther away, the width of broad spectral lines can be used to probe the gas orbiting near the event horizon. The technique of reverberation mapping uses variability of these lines to measure the mass and perhaps the spin of the black hole that powers active galaxies.
Gravitation from supermassive black holes in the center of many galaxies is thought to power active objects such as Seyfert galaxies and quasars.
An empirical correlation between the size of supermassive black holes and the stellar velocity dispersion of a galaxy bulge is called the M-sigma relation.
In the Milky Way
Inferred orbits of 6 stars around supermassive black hole candidate Sagittarius A* at the Milky Way galactic center
Astronomers are very confident that the Milky Way galaxy has a supermassive black hole at its center, 26,000 light-years from the Solar System, in a region called Sagittarius A* because:
- The star S2 follows an elliptical orbit with a period of 15.2 years and a pericenter (closest distance) of 17 light-hours (1.8×1013 m or 120 AU) from the center of the central object.
- From the motion of star S2, the object's mass can be estimated as 4.1 million M☉, or about 8.2×1036 kg.
- The radius of the central object must be less than 17 light-hours, because otherwise S2 would collide with it. Observations of the star S14 indicate that the radius is no more than 6.25 light-hours, about the diameter of Uranus' orbit.
- No known astronomical object other than a black hole can contain 4.1 million M☉ in this volume of space.
Infrared observations of bright flare activity near Sagittarius A* show orbital motion of plasma with a period of 45±15 min
at a separation of six to ten times the gravitational radius of the
candidate SMBH. This emission is consistent with a circularized orbit of
a polarized "hot spot" on an accretion disk in a strong magnetic field.
The radiating matter is orbiting at 30% of the speed of light just outside the innermost stable circular orbit.
On January 5, 2015, NASA reported observing an X-ray
flare 400 times brighter than usual, a record-breaker, from Sagittarius
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 Sagittarius A*, according to astronomers.
Detection of an unusually bright X-ray flare from Sagittarius A*, a supermassive black hole in the center of the Milky Way galaxy.
Outside the Milky Way
Artist's
impression of a supermassive black hole tearing apart a star. Below:
supermassive black hole devouring a star in galaxy RX J1242-11 – X-ray (left) and optical (right).
Unambiguous dynamical evidence for supermassive black holes exists only in a handful of galaxies; these include the Milky Way, the Local Group galaxies M31 and M32, and a few galaxies beyond the Local Group, e.g. NGC 4395. In these galaxies, the mean square (or rms) velocities of the stars or gas rises proportionally to 1/r
near the center, indicating a central point mass. In all other galaxies
observed to date, the rms velocities are flat, or even falling, toward
the center, making it impossible to state with certainty that a
supermassive black hole is present. Nevertheless, it is commonly accepted that the center of nearly every galaxy contains a supermassive black hole. The reason for this assumption is the M-sigma relation,
a tight (low scatter) relation between the mass of the hole in the 10
or so galaxies with secure detections, and the velocity dispersion of
the stars in the bulges of those galaxies.
This correlation, although based on just a handful of galaxies,
suggests to many astronomers a strong connection between the formation
of the black hole and the galaxy itself.
Hubble Space Telescope photograph of the 4,400 light-year long relativistic jet of Messier 87, which is matter being ejected by the 6.4×109 M☉ supermassive black hole at the center of the galaxy
The nearby Andromeda Galaxy, 2.5 million light-years away, contains a (1.1–2.3)×108 (110–230 million) M☉ central black hole, significantly larger than the Milky Way's. The largest supermassive black hole in the Milky Way's vicinity appears to be that of M87, at a mass of (6.4±0.5)×109 (c. 6.4 billion) M☉ at a distance of 53.5 million light-years. The supergiant elliptical galaxy NGC 4889, at a distance of 336 million light-years away in the Coma Berenices constellation, contains a black hole measured to be 2.1×1010 (21 billion) M☉.
Masses of black holes in quasars can be estimated via indirect methods that are subject to substantial uncertainty. The quasar TON 618 is an example of an object with an extremely large black hole, estimated at 6.6×1010 (66 billion) M☉. Its redshift is 2.219. Other examples of quasars with large estimated black hole masses are the hyperluminous quasar APM 08279+5255, with an estimated mass of 2.3×1010 (23 billion) M☉, and the quasar S5 0014+81, with a mass of 4.0×1010 (40 billion) M☉, or 10,000 times the mass of the black hole at the Milky Way Galactic Center.
Some galaxies, such as the galaxy 4C +37.11, appear to have two supermassive black holes at their centers, forming a binary system. If they collided, the event would create strong gravitational waves. Binary supermassive black holes are believed to be a common consequence of galactic mergers. The binary pair in OJ 287, 3.5 billion light-years away, contains the most massive black hole in a pair, with a mass estimated at 18 billion M☉.
In 2011, a super-massive black hole was discovered in the dwarf galaxy Henize 2-10,
which has no bulge. The precise implications for this discovery on
black hole formation are unknown, but may indicate that black holes
formed before bulges.
On March 28, 2011, a supermassive black hole was seen tearing a mid-size star apart.
That is the only likely explanation of the observations that day of
sudden X-ray radiation and the follow-up broad-band observations.
The source was previously an inactive galactic nucleus, and from study
of the outburst the galactic nucleus is estimated to be a SMBH with mass
of the order of a million solar masses. This rare event is assumed to
be a relativistic outflow (material being emitted in a jet at a significant fraction of the speed of light) from a star tidally disrupted
by the SMBH. A significant fraction of a solar mass of material is
expected to have accreted onto the SMBH. Subsequent long-term
observation will allow this assumption to be confirmed if the emission
from the jet decays at the expected rate for mass accretion onto a SMBH.
In 2012, astronomers reported an unusually large mass of approximately 17 billion M☉ for the black hole in the compact, lenticular galaxy NGC 1277, which lies 220 million light-years away in the constellation Perseus.
The putative black hole has approximately 59 percent of the mass of the
bulge of this lenticular galaxy (14 percent of the total stellar mass
of the galaxy).
Another study reached a very different conclusion: this black hole is
not particularly overmassive, estimated at between 2 and 5 billion M☉ with 5 billion M☉ being the most likely value. On 28 February 2013 astronomers reported on the use of the NuSTAR satellite to accurately measure the spin of a supermassive black hole for the first time, in NGC 1365, reporting that the event horizon was spinning at almost the speed of light.
Hubble view of a supermassive black hole "burping".
In September 2014, data from different X-ray telescopes has shown that the extremely small, dense, ultracompact dwarf galaxy M60-UCD1
hosts a 20 million solar mass black hole at its center, accounting for
more than 10% of the total mass of the galaxy. The discovery is quite
surprising, since the black hole is five times more massive than the
Milky Way's black hole despite the galaxy being less than
five-thousandths the mass of the Milky Way.
Some galaxies, however, lack any supermassive black holes in
their centers. Although most galaxies with no supermassive black holes
are very small, dwarf galaxies, one discovery remains mysterious: The
supergiant elliptical cD galaxy A2261-BCG
has not been found to contain an active supermassive black hole,
despite the galaxy being one of the largest galaxies known; ten times
the size and one thousand times the mass of the Milky Way. Since a
supermassive black hole will only be visible while it is accreting, a
supermassive black hole can be nearly invisible, except in its effects
on stellar orbits.
In December 2017, astronomers reported the detection of the most distant quasar currently known, ULAS J1342+0928, containing the most distant supermassive black hole, at a reported redshift of z = 7.54, surpassing the redshift of 7 for the previously known most distant quasar ULAS J1120+0641.
Hawking evaporation
If black holes evaporate via Hawking radiation, a supermassive black hole with a mass of 1011 (100 billion) M☉ will evaporate in around 2×10100 years.
Some monster black holes in the universe are predicted to continue to grow up to perhaps 1014 M☉ during the collapse of superclusters of galaxies. Even these would evaporate over a timescale of up to 10106 years.
