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'''Dark energy''' is the unknown form of energy that is causing the expansion of the [[Universe]] to accelerate. It is the largest single ingredient of the universe: in the standard model of cosmology, dark energy makes up about 68% of the total mass–energy content, while [[dark matter]] accounts for about 27% and ordinary (baryonic) matter and energy for about 5%.<ref>{{#cite:Q1232}}</ref>
'''Dark energy''' is a theorised form of energy that explains the accelerating expansion of the [[Universe]]. According to [[the standard model of cosmology]], it is the largest single ingredient of the universe, making up about 68% of the total mass–energy content of the universe.<ref>{{#cite:Q1232}}</ref>


Dark energy differs from matter in two essential ways. It is spread almost uniformly through space, rather than being gathered into galaxies and clusters by gravity, and its density changes very slowly as the universe expands. Because matter and radiation are diluted by the expansion while dark energy is not, the fraction of the universe made of dark energy has grown over time; it has come to dominate the dynamics of the cosmos only in the recent cosmic past, and it is what now drives the expansion to accelerate.
[[File:Universe composition (NOIRLab).jpg|thumb|upright=1.5|Artist's illustration of the composition of the universe: roughly 68% dark energy, 27% dark matter and 5% ordinary matter. Credit: NOIRLab/NSF/AURA/P. Marenfeld (CC BY 4.0).]]


== History ==
Dark energy, unlike ordinary matter and energy, is not gathered into galaxies and clusters by gravity but spread almost uniformly throughout space. Furthermore, while ordinary matter and energy are diluted by the expansion of the universe, the density of dark energy in space changes very slowly as the universe expands.<ref>{{#cite:Q1542}}</ref> As such, the fraction of dark energy in the content of the universe has grown over time, causing it to increasingly dominate the dynamics of the cosmos.


=== The cosmological constant and the expanding universe ===
=== Type Ia supernovae and the return of the cosmological constant ===


The first theoretical ancestor of dark energy was introduced by Albert Einstein in 1917: the '''cosmological constant''', usually written Λ, a term in his field equations of general relativity representing an energy that is uniform in space and constant in time, which he added to allow a static universe. After the expansion of the universe was established, from Georges Lemaître's 1927 expanding-universe solution<ref>{{#cite:Q1526}}</ref> to Edwin Hubble's 1929 distance–velocity relation,<ref>{{#cite:Q1527}}</ref> the cosmological constant was no longer needed for its original purpose, but it remained available as an ingredient of cosmological models.
The story of the cosmological constant, however, was not over:


In the simplest Big Bang models, the expansion of a matter-filled universe should decelerate: gravity pulls every galaxy towards every other, slowing the expansion set going by the Big Bang. Measuring whether the expansion was slowing exactly as predicted required objects whose intrinsic brightness is known well enough that their apparent brightness reveals their distance, so-called standard candles.
With the cosmological constant set to zero, the standard Big Bang models predict that the expansion of the universe must decelerate: gravity pulls every galaxy towards every other, slowing down the expansion initiated by the Big Bang.


=== The discovery of the accelerating universe ===
For decades, scientists were however unable to measure experimentally the rate of cosmic expansion. This changed in the 1990s, when scientists sufficiently mastered the so-called "'''standard candles'''" method, which measures the expansion history of the universe via objects whose intrinsic brightness is known well enough that their apparent brightness reveals their distance, hence nicknamed "standard candles". A reliable "standard candle" class, it turned out, was Ia supernovae, the explosions of white dwarfs that have accreted matter beyond a critical mass, emitting a remarkably uniform peak brightness. Small remaining differences can be corrected by the width–luminosity relation, which links how fast the supernova fades to how bright it is at its peak.


During the 1990s, two teams, the High-Z Supernova Search Team and the Supernova Cosmology Project, used type Ia supernovae as standard candles to trace the expansion history of the universe over the last several billion years.
[[File:SN1994D type Ia supernova.jpg|thumb|The type Ia supernova SN 1994D (bright spot, lower left) in the galaxy NGC 4526, imaged by the Hubble Space Telescope. Credit: NASA/ESA, the Hubble Key Project Team and the High-Z Supernova Search Team (public domain).]]


In 1998, the High-Z team, led by [[Person:Adam Riess|Adam Riess]] and [[Person:Brian Schmidt|Brian Schmidt]], reported the analysis of 16 high-redshift type Ia supernovae together with 34 nearby ones. The high-redshift supernovae were on average 10–15% farther away than expected in a low-density universe without a cosmological constant, and the data unanimously favoured eternally expanding models with a positive cosmological constant, ΩΛ > 0, and a currently accelerating expansion.<ref>{{#cite:Q1540}}</ref>
Two independent teams set out to measure the rate of cosmic expansion in the 1990s with Ia supernovae as standard candles: the High-Z Supernova Search Team, led by [[Person:Adam Riess|Adam Riess]] and [[Person:Brian Schmidt|Brian Schmidt]], and the Supernova Cosmology Project, led by [[Person:Saul Perlmutter|Saul Perlmutter]]. Both expected to observe a deceleration caused by gravity as predicted by standard Big Bang models.


One year later, the Supernova Cosmology Project, led by [[Person:Saul Perlmutter|Saul Perlmutter]], published its analysis of 42 type Ia supernovae at redshifts between 0.18 and 0.83. The data indicated that the cosmological constant is non-zero and positive, with 99% confidence.<ref>{{#cite:Q1541}}</ref>
In 1998, the High-Z team reported the analysis of 16 high-redshift type Ia supernovae together with 34 nearby ones. The high-redshift supernovae were on average 10–15% farther away than expected in a low-density universe without a cosmological constant, and the data unanimously favoured eternally expanding models with a currently accelerating cosmic expansion, consistent with a positive cosmological constant (ΩΛ > 0).<ref>{{#cite:Q1540}}</ref>  


[[Person:Saul Perlmutter|Saul Perlmutter]], [[Person:Brian Schmidt|Brian Schmidt]] and [[Person:Adam Riess|Adam Riess]] shared the 2011 Nobel Prize in Physics for the discovery of the accelerating expansion of the universe through observations of distant supernovae.
One year later, in 1999, the Supernova Cosmology Project published the analysis of 42 type Ia supernovae at redshifts between 0.18 and 0.83, and the data similarly favoured a positive cosmological constant, with 99% confidence.<ref>{{#cite:Q1541}}</ref>
 
The discovery of an accelerating cosmic expansion was ground-breaking. According to general relativity, ordinary matter and energy cannot provide such a positive cosmological constant. There must exist in this universe, therefore, something beyond ordinary matter and energy. Since scientists were (and are) uncertain of their nature, they decided to call it "'''dark-energy'''".
 
<blockquote>
[[Person:Saul Perlmutter|Saul Perlmutter]], [[Person:Brian Schmidt|Brian Schmidt]] and [[Person:Adam Riess|Adam Riess]] shared the 2011 Nobel Prize in Physics.
</blockquote>


[[File:Universe-timeline.jpg|thumb|upright=1.8|The history of the universe, from the Big Bang to the present day. The expansion first slowed under the pull of matter and radiation, then accelerated as dark energy came to dominate. Credit: NASA/WMAP Science Team (public domain).]]
[[File:Universe-timeline.jpg|thumb|upright=1.8|The history of the universe, from the Big Bang to the present day. The expansion first slowed under the pull of matter and radiation, then accelerated as dark energy came to dominate. Credit: NASA/WMAP Science Team (public domain).]]


The term dark energy was coined in analogy with dark matter: like that component it is invisible, and the name is intended to leave open what the new ingredient actually is.
== The physics of dark energy ==
 
Under the assumptions of homogeneity and isotropy on large scales, the expansion of the universe is described by the Friedmann equations, which follow from general relativity:
 
{{#content:Q1543}}
 
{{#content:Q1544}}
 
Here ''a'' is the scale factor (the Hubble parameter is H = ȧ/''a''), ''k'' the spatial curvature, ρ the total mass density, ''p'' the pressure, G the gravitational constant, ''c'' the speed of light, and Λ the cosmological constant.
 
The second equation demonstrates that any fluid with a non-negative pressure, such as ordinary matter (''p'' = 0) or radiation (''p'' = ρ''c''²/3), results in a more negative right-hand side, decelerating the expansion of the universe. The observed acceleration in the rate of expansion of the universe can only be explained by a dominant component with negative pressure satisfying ρ + 3''p''/''c''² < 0.
 
Cosmologists characterise each component by its dimensionless equation-of-state parameter
 
{{#content:Q1545}}
 
with ''w'' = 0 for non-relativistic matter, ''w'' = 1/3 for radiation, and ''w'' = −1 for a cosmological constant.
 
Mathematically, any component with ''w'' < −1/3 contributes to the acceleration of the rate of expansion of the universe. For this component to dominate the energy budget, it must also dilute more slowly than matter.
 
The simplest component satisfying ''w'' < −1/3 is the cosmological constant itself, which behaves exactly as a fluid of constant energy density
 
{{#content:Q1546}}
 
with a constant negative pressure
 
{{#content:Q1547}}
 
so that its equation-of-state parameter is exactly


== Observational evidence ==
{{#content:Q1548}}


=== Type Ia supernovae ===
As the universe expands and matter is diluted, such a constant-density component becomes steadily more dominant, explaining why the acceleration of the cosmic expansion began only when the universe was already several billion years old, as dark energy had overtaken matter.<ref>{{#cite:Q1542}}</ref>


Type Ia supernovae are the explosions of white dwarfs that have accreted matter beyond a critical mass, which makes their peak brightness remarkably uniform; after correction by the width–luminosity relation, they act as standardisable candles whose apparent brightness measures cosmic distances out to redshifts of the order of one. Comparing those distances with redshifts shows that distant supernovae are dimmer, and therefore farther, than the decelerating models of the time predicted, which is the direct evidence for accelerated expansion.<ref>{{#cite:Q1540}}</ref><ref>{{#cite:Q1541}}</ref>
== Additional observational evidence ==


=== The cosmic microwave background ===
=== The cosmic microwave background ===
[[File:WMAP nine-year CMB map.png|thumb|All-sky map of the cosmic microwave background from nine years of NASA's WMAP data; the colour differences are temperature fluctuations of ±200 microkelvin. Credit: NASA/WMAP Science Team (public domain).]]


The cosmic microwave background (CMB) offers an independent measurement of the geometry and content of the universe. The final full-mission Planck measurements, published in 2020, are consistent with a spatially flat universe whose total density is close to the critical density, but in which ordinary and dark matter together contribute only about 31% of that density.<ref>{{#cite:Q1232}}</ref> The remaining roughly 68% must be a smooth component that does not cluster like matter, in agreement with the supernova result: dark energy.<ref>{{#cite:Q1232}}</ref>
The cosmic microwave background (CMB) offers an independent measurement of the geometry and content of the universe. The final full-mission Planck measurements, published in 2020, are consistent with a spatially flat universe whose total density is close to the critical density, but in which ordinary and dark matter together contribute only about 31% of that density.<ref>{{#cite:Q1232}}</ref> The remaining roughly 68% must be a smooth component that does not cluster like matter, in agreement with the supernova result: dark energy.<ref>{{#cite:Q1232}}</ref>
Line 37: Line 73:
=== Large-scale structure and baryon acoustic oscillations ===
=== Large-scale structure and baryon acoustic oscillations ===


A third, independent class of evidence comes from the growth of large-scale structure. In the early universe, pressure waves travelled through the hot plasma until recombination, leaving a characteristic scale, the baryon acoustic oscillation (BAO) scale, imprinted in the clustering of galaxies; measuring this standard ruler at different cosmic epochs, together with the growth of structure itself, traces the expansion history and the competition between the pull of matter and the push of dark energy. Combined with the CMB, these measurements confirm the energy budget inferred from supernovae and pin down the equation of state of dark energy.<ref>{{#cite:Q1232}}</ref>
Another independent class of evidence comes from the way galaxies are distributed in space. In the hot early universe, matter and light were tightly coupled, and pressure waves, in effect sound waves, rippled outward from every overdense region. When the universe cooled enough for atoms to form, matter and light decoupled, and those ripples froze into the distribution of matter. The consequence is visible today in galaxy surveys: two galaxies are slightly more likely to be separated by one particular distance, about 150 megaparsecs (roughly 500 million light-years), than by any other. Cosmologists call this preferred spacing the baryon acoustic oscillation (BAO) scale. Because its true length is known from the CMB, it acts as a cosmic standard ruler: measuring how this ruler appears in surveys at different distances, and therefore at different times in cosmic history, traces the expansion history of the universe and the competition between the pull of matter and the push of dark energy. Combined with the CMB, these measurements confirm the energy budget inferred from supernovae and pin down the equation of state of dark energy.<ref>{{#cite:Q1232}}</ref>


<uml>
<uml>
Line 60: Line 96:
</uml>
</uml>


== The physics of dark energy ==
== Multiple hypotheses on the nature of dark energy ==
 
Under the assumptions of homogeneity and isotropy on large scales, the expansion of the universe is described by the Friedmann equations, which follow from general relativity:
 
{{#content:Q1543}}
 
{{#content:Q1544}}
 
Here ''a'' is the scale factor (the Hubble parameter is H = ȧ/''a''), ''k'' the spatial curvature, ρ the total mass density, ''p'' the pressure, G the gravitational constant, ''c'' the speed of light, and Λ the cosmological constant.
 
The second equation shows why the 1998 result was so surprising: any fluid with a non-negative pressure, such as ordinary matter (''p'' = 0) or radiation (''p'' = ρ''c''²/3), makes the right-hand side more negative, so it can only decelerate the expansion. Acceleration requires a dominant component with negative pressure satisfying ρ + 3''p''/''c''² < 0. Cosmologists characterise each component by its dimensionless equation-of-state parameter
 
{{#content:Q1545}}
 
with ''w'' = 0 for non-relativistic matter, ''w'' = 1/3 for radiation, and ''w'' = −1 for a cosmological constant. Any component with ''w'' < −1/3 acts as dark energy; acceleration requires such a component, and for dark energy to dominate the energy budget it must also dilute more slowly than matter.
 
The simplest candidate is the cosmological constant itself. It behaves exactly as a fluid of constant energy density
 
{{#content:Q1546}}
 
with pressure ''p'' = −ρ''c''², that is, with an equation-of-state parameter ''w'' = −1 exactly. As the universe expands and matter is diluted, such a constant-density component becomes steadily more dominant, which naturally explains why the acceleration began only when the universe was already several billion years old and dark energy had overtaken matter.<ref>{{#cite:Q1542}}</ref>
 
== What could dark energy be? ==


<uml>
<uml>
@startuml
@startuml
!theme bluegray
!theme bluegray
title What could dark energy be?
title Three hypotheses on the nature of dark energy


rectangle "Dark energy" as DE
rectangle "Dark energy" as DE
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=== The cosmological constant and the vacuum ===
=== The cosmological constant and the vacuum ===


If dark energy is the cosmological constant, it can be interpreted as the energy of the vacuum: quantum field theory predicts that empty space should carry a vacuum energy that behaves exactly like a cosmological constant. The trouble is its magnitude: naive estimates of the vacuum energy exceed the observed value of Λ by some 120 orders of magnitude, one of the largest discrepancies between theory and observation in physics, a difficulty known as the cosmological constant problem.<ref>{{#cite:Q1542}}</ref> Because of this problem, many cosmologists suspect that dark energy is something more subtle than a bare constant.<ref>{{#cite:Q1542}}</ref>
If dark energy is the cosmological constant, it can be interpreted as the energy of the vacuum: quantum field theory predicts that empty space should carry a vacuum energy that behaves exactly like a cosmological constant. The trouble is its magnitude: naive estimates of the vacuum energy exceed the observed value of Λ by some 120 orders of magnitude, one of the largest discrepancies between theory and observation in physics. This difficulty is known as the cosmological constant problem.<ref>{{#cite:Q1542}}</ref> Because of this problem, many cosmologists suspect that dark energy is more subtle than a bare cosmological constant.<ref>{{#cite:Q1542}}</ref>


=== Quintessence and modified gravity ===
=== Quintessence ===


Alternatives propose a dynamical dark energy, in which the acceleration is driven by a slowly-evolving scalar field, called quintessence, whose density declines with time, so that its equation-of-state parameter can differ from −1 and vary over cosmic history. Others argue that no new ingredient is needed at all, and that the acceleration signals a breakdown of general relativity on cosmological scales, which would require a modified theory of gravity.
Alternatives propose a dynamical dark energy, in which the acceleration is driven by a slowly-evolving scalar field, called quintessence, whose density declines with time, so that its equation-of-state parameter can differ from −1 and vary over cosmic history.
 
=== Modified gravity ===
 
Instead of introducing a new energy component, other physicists argue that the accelerating cosmic expansion signals a breakdown of general relativity on cosmological scales, which would require a modified theory of gravity.


== Current and future probes ==
== Current and future probes ==


As of September 2026, distinguishing these possibilities is a major goal of observational cosmology. The Dark Energy Spectroscopic Instrument (DESI) and the European Space Agency's Euclid space telescope are measuring the expansion history and the growth of cosmic structure over most of cosmic history, and the Nancy Grace Roman Space Telescope, launched in August 2026, is extending the supernova and weak-lensing measurements to much larger samples. The key observable is the equation-of-state parameter ''w'' and its possible variation with time: any deviation from −1 would rule out a pure cosmological constant and point to one of the dynamical alternatives.
[[File:DESI on the Mayall 4-meter Telescope.jpg|thumb|The Dark Energy Spectroscopic Instrument (DESI) installed on the Nicholas U. Mayall 4-metre Telescope at Kitt Peak National Observatory. Credit: NOIRLab/KPNO/NSF/AURA/P. Marenfeld (CC BY 4.0).]]
 
[[File:Euclid spacecraft (ESA artist impression).jpg|thumb|left|Artist's impression of ESA's Euclid space telescope in orbit. Credit: ESA (CC BY-SA 3.0 IGO).]]
 
As of September 2026, the nature of dark energy remains a core objective of observational cosmology. The Dark Energy Spectroscopic Instrument (DESI) and the European Space Agency's Euclid space telescope are measuring the expansion history of the universe and the growth of cosmic structure over most of cosmic history, and the Nancy Grace Roman Space Telescope, launched in August 2026, is extending the supernova and weak-lensing measurements to much larger samples. The key observable is the equation-of-state parameter ''w'' and its possible variation with time: any deviation from −1 would rule out a pure cosmological constant and point to one of the dynamical alternatives.


== References ==
== References ==

Latest revision as of 07:49, 3 September 2026

Dark energy is a theorised form of energy that explains the accelerating expansion of the Universe. According to the standard model of cosmology, it is the largest single ingredient of the universe, making up about 68% of the total mass–energy content of the universe.[1]

Artist's illustration of the composition of the universe: roughly 68% dark energy, 27% dark matter and 5% ordinary matter. Credit: NOIRLab/NSF/AURA/P. Marenfeld (CC BY 4.0).

Dark energy, unlike ordinary matter and energy, is not gathered into galaxies and clusters by gravity but spread almost uniformly throughout space. Furthermore, while ordinary matter and energy are diluted by the expansion of the universe, the density of dark energy in space changes very slowly as the universe expands.[2] As such, the fraction of dark energy in the content of the universe has grown over time, causing it to increasingly dominate the dynamics of the cosmos.

Type Ia supernovae and the return of the cosmological constant

The story of the cosmological constant, however, was not over:

With the cosmological constant set to zero, the standard Big Bang models predict that the expansion of the universe must decelerate: gravity pulls every galaxy towards every other, slowing down the expansion initiated by the Big Bang.

For decades, scientists were however unable to measure experimentally the rate of cosmic expansion. This changed in the 1990s, when scientists sufficiently mastered the so-called "standard candles" method, which measures the expansion history of the universe via objects whose intrinsic brightness is known well enough that their apparent brightness reveals their distance, hence nicknamed "standard candles". A reliable "standard candle" class, it turned out, was Ia supernovae, the explosions of white dwarfs that have accreted matter beyond a critical mass, emitting a remarkably uniform peak brightness. Small remaining differences can be corrected by the width–luminosity relation, which links how fast the supernova fades to how bright it is at its peak.

The type Ia supernova SN 1994D (bright spot, lower left) in the galaxy NGC 4526, imaged by the Hubble Space Telescope. Credit: NASA/ESA, the Hubble Key Project Team and the High-Z Supernova Search Team (public domain).

Two independent teams set out to measure the rate of cosmic expansion in the 1990s with Ia supernovae as standard candles: the High-Z Supernova Search Team, led by Adam Riess and Brian Schmidt, and the Supernova Cosmology Project, led by Saul Perlmutter. Both expected to observe a deceleration caused by gravity as predicted by standard Big Bang models.

In 1998, the High-Z team reported the analysis of 16 high-redshift type Ia supernovae together with 34 nearby ones. The high-redshift supernovae were on average 10–15% farther away than expected in a low-density universe without a cosmological constant, and the data unanimously favoured eternally expanding models with a currently accelerating cosmic expansion, consistent with a positive cosmological constant (ΩΛ > 0).[3]

One year later, in 1999, the Supernova Cosmology Project published the analysis of 42 type Ia supernovae at redshifts between 0.18 and 0.83, and the data similarly favoured a positive cosmological constant, with 99% confidence.[4]

The discovery of an accelerating cosmic expansion was ground-breaking. According to general relativity, ordinary matter and energy cannot provide such a positive cosmological constant. There must exist in this universe, therefore, something beyond ordinary matter and energy. Since scientists were (and are) uncertain of their nature, they decided to call it "dark-energy".

Saul Perlmutter, Brian Schmidt and Adam Riess shared the 2011 Nobel Prize in Physics.

The history of the universe, from the Big Bang to the present day. The expansion first slowed under the pull of matter and radiation, then accelerated as dark energy came to dominate. Credit: NASA/WMAP Science Team (public domain).

The physics of dark energy

Under the assumptions of homogeneity and isotropy on large scales, the expansion of the universe is described by the Friedmann equations, which follow from general relativity:

H^2 = \frac{8\pi G}{3}\rho - \frac{k c^2}{a^2} + \frac{\Lambda c^2}{3}

\frac{\ddot a}{a} = -\frac{4\pi G}{3}\left(\rho + \frac{3p}{c^2}\right) + \frac{\Lambda c^2}{3}

Here a is the scale factor (the Hubble parameter is H = ȧ/a), k the spatial curvature, ρ the total mass density, p the pressure, G the gravitational constant, c the speed of light, and Λ the cosmological constant.

The second equation demonstrates that any fluid with a non-negative pressure, such as ordinary matter (p = 0) or radiation (p = ρc²/3), results in a more negative right-hand side, decelerating the expansion of the universe. The observed acceleration in the rate of expansion of the universe can only be explained by a dominant component with negative pressure satisfying ρ + 3p/c² < 0.

Cosmologists characterise each component by its dimensionless equation-of-state parameter

w = \frac{p}{\rho c^2}

with w = 0 for non-relativistic matter, w = 1/3 for radiation, and w = −1 for a cosmological constant.

Mathematically, any component with w < −1/3 contributes to the acceleration of the rate of expansion of the universe. For this component to dominate the energy budget, it must also dilute more slowly than matter.

The simplest component satisfying w < −1/3 is the cosmological constant itself, which behaves exactly as a fluid of constant energy density

\rho_{\Lambda} = \frac{\Lambda c^2}{8\pi G}

with a constant negative pressure

p = -\rho_\Lambda c^2

so that its equation-of-state parameter is exactly

w = -1

As the universe expands and matter is diluted, such a constant-density component becomes steadily more dominant, explaining why the acceleration of the cosmic expansion began only when the universe was already several billion years old, as dark energy had overtaken matter.[2]

Additional observational evidence

The cosmic microwave background

All-sky map of the cosmic microwave background from nine years of NASA's WMAP data; the colour differences are temperature fluctuations of ±200 microkelvin. Credit: NASA/WMAP Science Team (public domain).

The cosmic microwave background (CMB) offers an independent measurement of the geometry and content of the universe. The final full-mission Planck measurements, published in 2020, are consistent with a spatially flat universe whose total density is close to the critical density, but in which ordinary and dark matter together contribute only about 31% of that density.[1] The remaining roughly 68% must be a smooth component that does not cluster like matter, in agreement with the supernova result: dark energy.[1]

Large-scale structure and baryon acoustic oscillations

Another independent class of evidence comes from the way galaxies are distributed in space. In the hot early universe, matter and light were tightly coupled, and pressure waves, in effect sound waves, rippled outward from every overdense region. When the universe cooled enough for atoms to form, matter and light decoupled, and those ripples froze into the distribution of matter. The consequence is visible today in galaxy surveys: two galaxies are slightly more likely to be separated by one particular distance, about 150 megaparsecs (roughly 500 million light-years), than by any other. Cosmologists call this preferred spacing the baryon acoustic oscillation (BAO) scale. Because its true length is known from the CMB, it acts as a cosmic standard ruler: measuring how this ruler appears in surveys at different distances, and therefore at different times in cosmic history, traces the expansion history of the universe and the competition between the pull of matter and the push of dark energy. Combined with the CMB, these measurements confirm the energy budget inferred from supernovae and pin down the equation of state of dark energy.[1]

Multiple hypotheses on the nature of dark energy

The cosmological constant and the vacuum

If dark energy is the cosmological constant, it can be interpreted as the energy of the vacuum: quantum field theory predicts that empty space should carry a vacuum energy that behaves exactly like a cosmological constant. The trouble is its magnitude: naive estimates of the vacuum energy exceed the observed value of Λ by some 120 orders of magnitude, one of the largest discrepancies between theory and observation in physics. This difficulty is known as the cosmological constant problem.[2] Because of this problem, many cosmologists suspect that dark energy is more subtle than a bare cosmological constant.[2]

Quintessence

Alternatives propose a dynamical dark energy, in which the acceleration is driven by a slowly-evolving scalar field, called quintessence, whose density declines with time, so that its equation-of-state parameter can differ from −1 and vary over cosmic history.

Modified gravity

Instead of introducing a new energy component, other physicists argue that the accelerating cosmic expansion signals a breakdown of general relativity on cosmological scales, which would require a modified theory of gravity.

Current and future probes

The Dark Energy Spectroscopic Instrument (DESI) installed on the Nicholas U. Mayall 4-metre Telescope at Kitt Peak National Observatory. Credit: NOIRLab/KPNO/NSF/AURA/P. Marenfeld (CC BY 4.0).
Artist's impression of ESA's Euclid space telescope in orbit. Credit: ESA (CC BY-SA 3.0 IGO).

As of September 2026, the nature of dark energy remains a core objective of observational cosmology. The Dark Energy Spectroscopic Instrument (DESI) and the European Space Agency's Euclid space telescope are measuring the expansion history of the universe and the growth of cosmic structure over most of cosmic history, and the Nancy Grace Roman Space Telescope, launched in August 2026, is extending the supernova and weak-lensing measurements to much larger samples. The key observable is the equation-of-state parameter w and its possible variation with time: any deviation from −1 would rule out a pure cosmological constant and point to one of the dynamical alternatives.

References

  1. Planck Collaboration. (2020). Planck 2018 results (Scholarly article). In Astronomy and Astrophysics (Vols. 641, p. A6). https://doi.org/10.1051/0004-6361/201833910
  2. Carroll, S. (2001). The Cosmological Constant (Scholarly article). In Living Reviews in Relativity (Vols. 4, p. 1). https://doi.org/10.12942/lrr-2001-1
  3. Riess, A. (1998). Observational Evidence from Supernovae for an Accelerating Universe and a Cosmological Constant (Scholarly article). In The Astronomical Journal (Vols. 116, Issues 3, pp. 1009–1038). https://doi.org/10.1086/300499
  4. Perlmutter, S. (1999). Measurements of Omega and Lambda from 42 High-Redshift Supernovae (Scholarly article). In The Astrophysical Journal (Vols. 517, Issues 2, pp. 565–586). https://doi.org/10.1086/307221

Further reading