Dark energy, ![Type Ia supernova [Credit: Photo AURA/STScI/NASA/JPL (NASA photo # STScI-PRC98-02a-js)]](https://lh3.googleusercontent.com/blogger_img_proxy/AEn0k_sOSV-K6qR67ynjccoK6gsMHZnNsm0EN79cOwIqJhGSCfLVtSUW-gxM3CWjQ14aE49JoHXS9XVuehPd-YUIefbGdM6-FSfFPUt6YtdpgkXq6e5sl7hO1vPEH342k6NRZrIypaTr2zvs=s0-d)
repulsive force that is the dominant component (73 percent) of the
universe. The remaining portion of the
universe consists of ordinary
matter and
dark matter. Dark energy, in contrast to both forms of
matter,
is relatively uniform in time and space and is gravitationally
repulsive, not attractive, within the volume it occupies. The nature of
dark energy is still not well understood.
A kind of cosmic repulsive force was first hypothesized by
Albert Einstein
in 1917 and was represented by a term, the “cosmological constant,”
that Einstein reluctantly introduced into his theory of general
relativity in order to counteract the attractive force of
gravity
and account for a universe that was assumed to be static (neither
expanding nor contracting). After the discovery in the 1920s by American
astronomer
Edwin Hubble that the
universe
is not static but is in fact expanding, Einstein referred to the
addition of this constant as his “greatest blunder.” However, the
measured amount of matter in the mass-energy budget of the universe was
improbably low, and thus some unknown “missing component,” much like the
cosmological constant,
was required to make up the deficit. Direct evidence for the existence
of this component, which was dubbed dark energy, was first presented in
1998.
Dark energy is detected by its effect on the rate at which
the universe expands and its effect on the rate at which large-scale
structures such as
galaxies and clusters of galaxies form through gravitational instabilities. The measurement of the expansion rate requires the use of
telescopes to measure the distance (or light travel time) of objects seen at different size scales (or
redshifts)
in the history of the universe. These efforts are generally limited by
the difficulty in accurately measuring astronomical distances. Since
dark energy works against gravity, more dark energy accelerates the
universe’s expansion and retards the formation of large-scale structure.
One technique for measuring the expansion rate is to observe the
apparent brightness of objects of known luminosity like
Type Ia supernovas. Dark energy was discovered in 1998 with this method by two international teams that included American astronomers
Adam Riess (the author of this article) and
Saul Perlmutter and Australian astronomer
Brian Schmidt. The two teams used eight telescopes including those of the
Keck Observatory and the
MMT Observatory.
Type Ia supernovas that exploded when the universe was only two-thirds
of its present size were fainter and thus farther away than they would
be in a universe without dark
energy.
This implied the expansion rate of the universe is faster now than it
was in the past, a result of the current dominance of dark energy. (Dark
energy was negligible in the early universe.)
![Wilkinson Microwave Anisotropy Probe [Credit: NASA/WMAP Science Team]](https://lh3.googleusercontent.com/blogger_img_proxy/AEn0k_tO3ocNgxj-fhPhyXCS1oNdUxtemrOoS4SArbPUCiAy3i63aVLCn96-PLAQMRI98AygRYZ_oWhgRWTXM4pDco0KxvH8g0LG5mhyWDV2zkZBUDZrlPg0ZxcFVShGCG27scK42pfJKSJl=s0-d)
Studying
the effect of dark energy on large-scale structure involves measuring
subtle distortions in the shapes of galaxies arising from the bending of
space by intervening matter, a phenomenon known as “
weak lensing.”
At some point in the last few billion years, dark energy became
dominant in the universe and thus prevented more galaxies and clusters
of galaxies from forming. This change in the structure of the universe
is revealed by weak lensing. Another measure comes from counting the
number of clusters of galaxies in the universe to measure the volume of
space and the rate at which that volume is increasing. The goals of most
observational studies of dark energy are to measure its
equation of state
(the ratio of its pressure to its energy density), variations in its
properties, and the degree to which dark energy provides a complete
description of gravitational physics.
![matter-energy content of the universe [Credit: Encyclopædia Britannica, Inc.]](https://lh3.googleusercontent.com/blogger_img_proxy/AEn0k_vtcrShHW6cT8-Y8-lee_Xv0_bxycwGwRKqgSxCwyMb5LDzl1Ro-zc0WMvdaQ8YU_59SpmYE_XoKt-QvPq556ihoxr9DmmduHmIqFfuycRMSW-vw_CN6C7jD5MuVkt4AwzguwJ7M2dsuA=s0-d)
In cosmological theory, dark energy is a general class of components in the stress-energy tensor of the field equations in
Einstein’s theory of
general relativity.
In this theory, there is a direct correspondence between the
matter-energy of the universe (expressed in the tensor) and the shape of
space-time. Both the matter (or energy)
density
(a positive quantity) and the internal pressure contribute to a
component’s gravitational field. While familiar components of the
stress-energy tensor such as matter and radiation provide attractive
gravity by bending
space-time,
dark energy causes repulsive gravity through negative internal
pressure. If the ratio of the pressure to the energy density is less
than −1/3, a possibility for a component with negative pressure, that
component will be gravitationally self-repulsive. If such a component
dominates the universe, it will accelerate the universe’s expansion.
![dark energy [Credit: © MinutePhysics (A Britannica Publishing Partner)]](https://lh3.googleusercontent.com/blogger_img_proxy/AEn0k_si9rN-loAHVuaR8xAG8k00grE1aZl_xyMtbuZulQjt0kSeFnxS__fREgMroCsMN5C0e3rIpWkLjElp_xvBdZiaFLBHXV_gMqOojbkjEvDIC4xHsF3PRVwfb13Q7_6GPrXfV9s6cQf8=s0-d)
The simplest and oldest explanation for dark energy is that it is an energy density inherent to empty space, or a “
vacuum
energy.” Mathematically, vacuum energy is equivalent to Einstein’s
cosmological constant. Despite the rejection of the cosmological
constant by Einstein and others, the modern understanding of the vacuum,
based on
quantum field theory,
is that vacuum energy arises naturally from the totality of quantum
fluctuations (i.e., virtual particle-antiparticle pairs that come into
existence and then annihilate each other shortly thereafter) in empty
space. However, the observed density of the cosmological vacuum energy
density is ~10
−10 ergs per cubic centimetre; the value predicted from
quantum field theory is ~10
110 ergs per cubic centimetre. This discrepancy of 10
120
was known even before the discovery of the far weaker dark energy.
While a fundamental solution to this problem has not yet been found,
probabilistic solutions have been posited, motivated by
string theory
and the possible existence of a large number of disconnected universes.
In this paradigm the unexpectedly low value of the constant is
understood as a result of an even greater number of opportunities (i.e.,
universes) for the occurrence of different values of the constant and
the random selection of a value small enough to allow for the formation
of galaxies (and thus stars and life).
Another popular theory for dark energy is that it is a transient vacuum energy resulting from the
potential energy of a dynamical field. Known as “
quintessence,”
this form of dark energy would vary in space and time, thus providing a
possible way to distinguish it from a cosmological constant. It is also
similar in mechanism (though vastly different in scale) to the scalar
field energy invoked in the inflationary theory of the
big bang.
Another
possible explanation for dark energy is topological defects in the
fabric of the universe. In the case of intrinsic defects in space-time
(e.g., cosmic strings or walls), the production of new defects as the
universe expands is mathematically similar to a cosmological constant,
although the value of the equation of state for the defects depends on
whether the defects are strings (one-dimensional) or walls
(two-dimensional).
There have also been attempts to modify gravity
to explain both cosmological and local observations without the need
for dark energy. These attempts invoke departures from
general relativity on scales of the entire observable universe.
A
major challenge to understanding accelerated expansion with or without
dark energy is to explain the relatively recent occurrence (in the past
few billion years) of near-equality between the density of dark energy
and
dark matter
even though they must have evolved differently. (For cosmic structures
to have formed in the early universe, dark energy must have been an
insignificant component.) This problem is known as the “
coincidence problem”
or the “fine-tuning problem.” Understanding the nature of dark energy
and its many related problems is one of the most formidable challenges
in modern physics.