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Physical cosmology is a branch of cosmology concerned with the study of cosmological models. A cosmological model, or simply cosmology, provides a description of the largest-scale structures and dynamics of the universe and allows study of fundamental questions about its origin, structure, evolution, and ultimate fate.^[1] Cosmology as a science originated with the Copernican principle, which implies that celestial bodies obey identical physical laws to those on Earth, and Newtonian mechanics, which first allowed those physical laws to be understood.

Physical cosmology, as it is now understood, began in 1915 with the development of Albert Einstein's general theory of relativity, followed by major observational discoveries in the 1920s: first, Edwin Hubble discovered that the universe contains a huge number of external galaxies beyond the Milky Way; then, work by Vesto Slipher and others showed that the universe is expanding. These advances made it possible to speculate about the origin of the universe, and allowed the establishment of the Big Bang theory, by Georges Lemaître, as the leading cosmological model. A few researchers still advocate a handful of alternative cosmologies;^[2] however, most cosmologists agree that the Big Bang theory best explains the observations.

Dramatic advances in observational cosmology since the 1990s, including the cosmic microwave background, distant supernovae and galaxy redshift surveys, have led to the development of a standard model of cosmology. This model requires the universe to contain large amounts of dark matter and dark energy whose nature is currently not well understood, but the model gives detailed predictions that are in excellent agreement with many diverse observations.^[3]

Cosmology draws heavily on the work of many disparate areas of research in theoretical and applied physics. Areas relevant to cosmology include particle physics experiments and theory, theoretical and observational astrophysics, general relativity, quantum mechanics, and plasma physics.

Subject history

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Modern cosmology developed along tandem tracks of theory and observation. In 1916, Albert Einstein published his theory of general relativity, which provided a unified description of gravity as a geometric property of space and time.^[4] At the time, Einstein believed in a static universe, but found that his original formulation of the theory did not permit it.^[5] This is because masses distributed throughout the universe gravitationally attract, and move toward each other over time.^[6] However, he realized that his equations permitted the introduction of a constant term which could counteract the attractive force of gravity on the cosmic scale. Einstein published his first paper on relativistic cosmology in 1917, in which he added this cosmological constant to his field equations in order to force them to model a static universe.^[7] The Einstein model describes a static universe; space is finite and unbounded (analogous to the surface of a sphere, which has a finite area but no edges). However, this so-called Einstein model is unstable to small perturbations—it will eventually start to expand or contract.^[5] It was later realized that Einstein's model was just one of a larger set of possibilities, all of which were consistent with general relativity and the cosmological principle. The cosmological solutions of general relativity were found by Alexander Friedmann in the early 1920s.^[8] His equations describe the Friedmann–Lemaître–Robertson–Walker universe, which may expand or contract, and whose geometry may be open, flat, or closed.

In the 1910s, Vesto Slipher (and later Carl Wilhelm Wirtz) interpreted the red shift of spiral nebulae as a Doppler shift that indicated they were receding from Earth.^[12]^[13] However, it is difficult to determine the distance to astronomical objects. One way is to compare the physical size of an object to its angular size, but a physical size must be assumed in order to do this. Another method is to measure the brightness of an object and assume an intrinsic luminosity, from which the distance may be determined using the inverse-square law. Due to the difficulty of using these methods, they did not realize that the nebulae were actually galaxies outside our own Milky Way, nor did they speculate about the cosmological implications. In 1927, the Belgian Roman Catholic priest Georges Lemaître independently derived the Friedmann–Lemaître–Robertson–Walker equations and proposed, on the basis of the recession of spiral nebulae, that the universe began with the "explosion" of a "primeval atom"^[14]—which was later called the Big Bang. In 1929, Edwin Hubble provided an observational basis for Lemaître's theory. Hubble showed that the spiral nebulae were galaxies by determining their distances using measurements of the brightness of Cepheid variable stars. He discovered a relationship between the redshift of a galaxy and its distance. He interpreted this as evidence that the galaxies are receding from Earth in every direction at speeds proportional to their distance from Earth.^[15] This fact is now known as Hubble's law, though the numerical factor Hubble found relating recessional velocity and distance was off by a factor of ten, due to not knowing about the types of Cepheid variables.

Given the cosmological principle, Hubble's law suggested that the universe was expanding. Two primary explanations were proposed for the expansion. One was Lemaître's Big Bang theory, advocated and developed by George Gamow. The other explanation was Fred Hoyle's steady state model in which new matter is created as the galaxies move away from each other. In this model, the universe is roughly the same at any point in time.^[16]^[17]

For a number of years, support for these theories was evenly divided. However, the observational evidence began to support the idea that the universe evolved from a hot dense state. The discovery of the cosmic microwave background in 1965 lent strong support to the Big Bang model,^[17] and since the precise measurements of the cosmic microwave background by the Cosmic Background Explorer in the early 1990s, few cosmologists have seriously proposed other theories of the origin and evolution of the cosmos. One consequence of this is that in standard general relativity, the universe began with a singularity, as demonstrated by Roger Penrose and Stephen Hawking in the 1960s.^[18]

An alternative view to extend the Big Bang model, suggesting the universe had no beginning or singularity and the age of the universe is infinite, has been presented.^[19]^[20]^[21]

In September 2023, astrophysicists questioned the overall current view of the universe, in the form of the Standard Model of Cosmology, based on the latest James Webb Space Telescope studies.^[22]

Energy of the cosmos

The lightest chemical elements, primarily hydrogen and helium, were created during the Big Bang through the process of nucleosynthesis.^[23] In a sequence of stellar nucleosynthesis reactions, smaller atomic nuclei are then combined into larger atomic nuclei, ultimately forming stable iron group elements such as iron and nickel, which have the highest nuclear binding energies.^[24] The net process results in a later energy release, meaning subsequent to the Big Bang.^[25] Such reactions of nuclear particles can lead to sudden energy releases from cataclysmic variable stars such as novae. Gravitational collapse of matter into black holes also powers the most energetic processes, generally seen in the nuclear regions of galaxies, forming quasars and active galaxies.

Cosmologists cannot explain all cosmic phenomena exactly, such as those related to the accelerating expansion of the universe, using conventional forms of energy. Instead, cosmologists propose a new form of energy called dark energy that permeates all space.^[26] One hypothesis is that dark energy is just the vacuum energy, a component of empty space that is associated with the virtual particles that exist due to the uncertainty principle.^[27]

There is no clear way to define the total energy in the universe using the most widely accepted theory of gravity, general relativity. Therefore, it remains controversial whether the total energy is conserved in an expanding universe. For instance, each photon that travels through intergalactic space loses energy due to the redshift effect. This energy is not transferred to any other system, so seems to be permanently lost. On the other hand, some cosmologists insist that energy is conserved in some sense; this follows the law of conservation of energy.^[28]

Different forms of energy may dominate the cosmos—relativistic particles which are referred to as radiation, or non-relativistic particles referred to as matter. Relativistic particles are particles whose rest mass is zero or negligible compared to their kinetic energy, and so move at the speed of light or very close to it; non-relativistic particles have much higher rest mass than their energy and so move much slower than the speed of light.

As the universe expands, both matter and radiation become diluted. However, the energy densities of radiation and matter dilute at different rates. As a particular volume expands, mass-energy density is changed only by the increase in volume, but the energy density of radiation is changed both by the increase in volume and by the increase in the wavelength of the photons that make it up. Thus the energy of radiation becomes a smaller part of the universe's total energy than that of matter as it expands. The very early universe is said to have been 'radiation dominated' and radiation controlled the deceleration of expansion. Later, as the average energy per photon becomes roughly 10 eV and lower, matter dictates the rate of deceleration and the universe is said to be 'matter dominated'. The intermediate case is not treated well analytically. As the expansion of the universe continues, matter dilutes even further and the cosmological constant becomes dominant, leading to an acceleration in the universe's expansion.

History of the universe

The history of the universe is a central issue in cosmology. The history of the universe is divided into different periods called epochs, according to the dominant forces and processes in each period. The standard cosmological model is known as the Lambda-CDM model.

Equations of motion

Within the standard cosmological model, the equations of motion governing the universe as a whole are derived from general relativity with a small, positive cosmological constant.^[29] The solution is an expanding universe; due to this expansion, the radiation and matter in the universe cool and become diluted. At first, the expansion is slowed down by gravitation attracting the radiation and matter in the universe. However, as these become diluted, the cosmological constant becomes more dominant and the expansion of the universe starts to accelerate rather than decelerate. In our universe this happened billions of years ago.^[30]

Particle physics in cosmology

During the earliest moments of the universe, the average energy density was very high, making knowledge of particle physics critical to understanding this environment. Hence, scattering processes and decay of unstable elementary particles are important for cosmological models of this period.

As a rule of thumb, a scattering or a decay process is cosmologically important in a certain epoch if the time scale describing that process is smaller than, or comparable to, the time scale of the expansion of the universe.^{[clarification needed]} The time scale that describes the expansion of the universe is $1/H$ with $H$ being the Hubble parameter, which varies with time. The expansion timescale $1/H$ is roughly equal to the age of the universe at each point in time.

Timeline of the Big Bang

Observations suggest that the universe began around 13.8 billion years ago.^[31] Since then, the evolution of the universe has passed through three phases. The very early universe, which is still poorly understood, was the split second in which the universe was so hot that particles had energies higher than those currently accessible in particle accelerators on Earth. Therefore, while the basic features of this epoch have been worked out in the Big Bang theory, the details are largely based on educated guesses.

Following this, in the early universe, the evolution of the universe proceeded according to known high energy physics. This is when the first protons, electrons and neutrons formed, then nuclei and finally atoms. With the formation of neutral hydrogen, the cosmic microwave background was emitted. Finally, the epoch of structure formation began, when matter started to aggregate into the first stars and quasars, and ultimately galaxies, clusters of galaxies and superclusters formed. The future of the universe is not yet firmly known, but according to the ΛCDM model it will continue expanding forever.

Areas of study

Below, some of the most active areas of inquiry in cosmology are described, in roughly chronological order. This does not include all of the Big Bang cosmology, which is presented in Timeline of the Big Bang.

Very early universe

The early, hot universe appears to be well explained by the Big Bang from roughly 10⁻³³ seconds onwards, but there are several problems. One is that there is no compelling reason, using current particle physics, for the universe to be flat, homogeneous, and isotropic (see the cosmological principle). Moreover, grand unified theories of particle physics suggest that there should be magnetic monopoles in the universe, which have not been found. These problems are resolved by a brief period of cosmic inflation, which drives the universe to flatness, smooths out anisotropies and inhomogeneities to the observed level, and exponentially dilutes the monopoles.^[32] The physical model behind cosmic inflation is extremely simple, but it has not yet been confirmed by particle physics, and there are difficult problems reconciling inflation and quantum field theory.^[vague] Some cosmologists think that string theory and brane cosmology will provide an alternative to inflation.^[33]

Another major problem in cosmology is what caused the universe to contain far more matter than antimatter. Cosmologists can observationally deduce that the universe is not split into regions of matter and antimatter. If it were, there would be X-rays and gamma rays produced as a result of annihilation, but this is not observed. Therefore, some process in the early universe must have created a small excess of matter over antimatter, and this (currently not understood) process is called baryogenesis. Three required conditions for baryogenesis were derived by Andrei Sakharov in 1967, and requires a violation of the particle physics symmetry, called CP-symmetry, between matter and antimatter.^[34] However, particle accelerators measure too small a violation of CP-symmetry to account for the baryon asymmetry. Cosmologists and particle physicists look for additional violations of the CP-symmetry in the early universe that might account for the baryon asymmetry.^[35]

Both the problems of baryogenesis and cosmic inflation are very closely related to particle physics, and their resolution might come from high energy theory and experiment, rather than through observations of the universe.^{[speculation?]}

Big Bang Theory

Big Bang nucleosynthesis is the theory of the formation of the elements in the early universe. It finished when the universe was about three minutes old and its temperature dropped below that at which nuclear fusion could occur. Big Bang nucleosynthesis had a brief period during which it could operate, so only the very lightest elements were produced. Starting from hydrogen ions (protons), it principally produced deuterium, helium-4, and lithium. Other elements were produced in only trace abundances. The basic theory of nucleosynthesis was developed in 1948 by George Gamow, Ralph Asher Alpher, and Robert Herman.^[36] It was used for many years as a probe of physics at the time of the Big Bang, as the theory of Big Bang nucleosynthesis connects the abundances of primordial light elements with the features of the early universe.^[23] Specifically, it can be used to test the equivalence principle,^[37] to probe dark matter, and test neutrino physics.^[38] Some cosmologists have proposed that Big Bang nucleosynthesis suggests there is a fourth "sterile" species of neutrino.^[39]

Standard model of Big Bang cosmology

The ΛCDM (Lambda cold dark matter) or Lambda-CDM model is a parametrization of the Big Bang cosmological model in which the universe contains a cosmological constant, denoted by Lambda (Greek Λ), associated with dark energy, and cold dark matter (abbreviated CDM). It is frequently referred to as the standard model of Big Bang cosmology.^[40]^[41]

Cosmic microwave background

The cosmic microwave background is radiation left over from decoupling after the epoch of recombination when neutral atoms first formed. At this point, radiation produced in the Big Bang stopped Thomson scattering from charged ions. The radiation, first observed in 1965 by Arno Penzias and Robert Woodrow Wilson, has a perfect thermal black-body spectrum. It has a temperature of 2.7 kelvins today and is isotropic to one part in 10⁵. Cosmological perturbation theory, which describes the evolution of slight inhomogeneities in the early universe, has allowed cosmologists to precisely calculate the angular power spectrum of the radiation, and it has been measured by the recent satellite experiments (COBE and WMAP)^[42] and many ground and balloon-based experiments (such as Degree Angular Scale Interferometer, Cosmic Background Imager, and Boomerang).^[43] One of the goals of these efforts is to measure the basic parameters of the Lambda-CDM model with increasing accuracy, as well as to test the predictions of the Big Bang model and look for new physics. The results of measurements made by WMAP, for example, have placed limits on the neutrino masses.^[44]

Newer experiments, such as QUIET and the Atacama Cosmology Telescope, are trying to measure the polarization of the cosmic microwave background.^[45] These measurements are expected to provide further confirmation of the theory as well as information about cosmic inflation, and the so-called secondary anisotropies,^[46] such as the Sunyaev-Zel'dovich effect and Sachs-Wolfe effect, which are caused by interaction between galaxies and clusters with the cosmic microwave background.^[47]^[48]

On 17 March 2014, astronomers of the BICEP2 Collaboration announced the apparent detection of B-mode polarization of the CMB, considered to be evidence of primordial gravitational waves that are predicted by the theory of inflation to occur during the earliest phase of the Big Bang.^[9]^[10]^[11]^[49] However, later that year the Planck collaboration provided a more accurate measurement of cosmic dust, concluding that the B-mode signal from dust is the same strength as that reported from BICEP2.^[50]^[51] On 30 January 2015, a joint analysis of BICEP2 and Planck data was published and the European Space Agency announced that the signal can be entirely attributed to interstellar dust in the Milky Way.^[52]

Formation and evolution of large-scale structure

Understanding the formation and evolution of the largest and earliest structures (i.e., quasars, galaxies, clusters and superclusters) is one of the largest efforts in cosmology. Cosmologists study a model of hierarchical structure formation in which structures form from the bottom up, with smaller objects forming first, while the largest objects, such as superclusters, are still assembling.^[53] One way to study structure in the universe is to survey the visible galaxies, in order to construct a three-dimensional picture of the galaxies in the universe and measure the matter power spectrum. This is the approach of the Sloan Digital Sky Survey and the 2dF Galaxy Redshift Survey.^[54]^[55]

Another tool for understanding structure formation is simulations, which cosmologists use to study the gravitational aggregation of matter in the universe, as it clusters into filaments, superclusters and voids. Most simulations contain only non-baryonic cold dark matter, which should suffice to understand the universe on the largest scales, as there is much more dark matter in the universe than visible, baryonic matter. More advanced simulations are starting to include baryons and study the formation of individual galaxies. Cosmologists study these simulations to see if they agree with the galaxy surveys, and to understand any discrepancy.^[56]

Other, complementary observations to measure the distribution of matter in the distant universe and to probe reionization include:

The Lyman-alpha forest, which allows cosmologists to measure the distribution of neutral atomic hydrogen gas in the early universe, by measuring the absorption of light from distant quasars by the gas.^[57]
The 21-centimeter absorption line of neutral atomic hydrogen also provides a sensitive test of cosmology.^[58]
Weak lensing, the distortion of a distant image by gravitational lensing due to dark matter.^[59]

These will help cosmologists settle the question of when and how structure formed in the universe.

Dark matter

Evidence from Big Bang nucleosynthesis, the cosmic microwave background, structure formation, and galaxy rotation curves suggests that about 23% of the mass of the universe consists of non-baryonic dark matter, whereas only 4% consists of visible, baryonic matter. The gravitational effects of dark matter are well understood, as it behaves like a cold, non-radiative fluid that forms haloes around galaxies. Dark matter has never been detected in the laboratory, and the particle physics nature of dark matter remains completely unknown. Without observational constraints, there are a number of candidates, such as a stable supersymmetric particle, a weakly interacting massive particle, a gravitationally-interacting massive particle, an axion, and a massive compact halo object. Alternatives to the dark matter hypothesis include a modification of gravity at small accelerations (MOND) or an effect from brane cosmology. TeVeS is a version of MOND that can explain gravitational lensing.^[60]

Dark energy

If the universe is flat, there must be an additional component making up 73% (in addition to the 23% dark matter and 4% baryons) of the energy density of the universe. This is called dark energy. In order not to interfere with Big Bang nucleosynthesis and the cosmic microwave background, it must not cluster in haloes like baryons and dark matter. There is strong observational evidence for dark energy, as the total energy density of the universe is known through constraints on the flatness of the universe, but the amount of clustering matter is tightly measured, and is much less than this. The case for dark energy was strengthened in 1999, when measurements demonstrated that the expansion of the universe has begun to gradually accelerate.^[61]

Apart from its density and its clustering properties, nothing is known about dark energy. Quantum field theory predicts a cosmological constant (CC) much like dark energy, but 120 orders of magnitude larger than that observed.^[62] Steven Weinberg and a number of string theorists (see string landscape) have invoked the 'weak anthropic principle': i.e. the reason that physicists observe a universe with such a small cosmological constant is that no physicists (or any life) could exist in a universe with a larger cosmological constant. Many cosmologists find this an unsatisfying explanation: perhaps because while the weak anthropic principle is self-evident (given that living observers exist, there must be at least one universe with a cosmological constant (CC) which allows for life to exist) it does not attempt to explain the context of that universe.^[63] For example, the weak anthropic principle alone does not distinguish between:

Only one universe will ever exist and there is some underlying principle that constrains the CC to the value we observe.
Only one universe will ever exist and although there is no underlying principle fixing the CC, we got lucky.
Lots of universes exist (simultaneously or serially) with a range of CC values, and of course ours is one of the life-supporting ones.

Other possible explanations for dark energy include quintessence^[64] or a modification of gravity on the largest scales.^[65] The effect on cosmology of the dark energy that these models describe is given by the dark energy's equation of state, which varies depending upon the theory. The nature of dark energy is one of the most challenging problems in cosmology.

A better understanding of dark energy is likely to solve the problem of the ultimate fate of the universe. In the current cosmological epoch, the accelerated expansion due to dark energy is preventing structures larger than superclusters from forming. It is not known whether the acceleration will continue indefinitely, perhaps even increasing until a big rip, or whether it will eventually reverse, lead to a Big Freeze, or follow some other scenario.^[66]

Gravitational waves

Gravitational waves are ripples in the curvature of spacetime that propagate as waves at the speed of light, generated in certain gravitational interactions that propagate outward from their source. Gravitational-wave astronomy is an emerging branch of observational astronomy which aims to use gravitational waves to collect observational data about sources of detectable gravitational waves such as binary star systems composed of white dwarfs, neutron stars, and black holes; and events such as supernovae, and the formation of the early universe shortly after the Big Bang.^[67]

In 2016, the LIGO Scientific Collaboration and Virgo Collaboration teams announced that they had made the first observation of gravitational waves, originating from a pair of merging black holes using the Advanced LIGO detectors.^[68]^[69]^[70] On 15 June 2016, a second detection of gravitational waves from coalescing black holes was announced.^[71] Besides LIGO, many other gravitational-wave observatories (detectors) are under construction.^[72]

Other areas of inquiry

Cosmologists also study:

Whether primordial black holes were formed in our universe, and what happened to them.^[73]
Detection of cosmic rays with energies above the GZK cutoff,^[74] and whether it signals a failure of special relativity at high energies.
The equivalence principle,^[37] whether or not Einstein's general theory of relativity is the correct theory of gravitation,^[75] and if the fundamental laws of physics are the same everywhere in the universe.^[76]
Biophysical cosmology: a type of physical cosmology that studies and understands life as part or an inherent part of physical cosmology. It stresses that life is inherent to the universe and therefore frequent.^[77]

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External links

From groups

Cambridge Cosmology – from Cambridge University (public home page)
Cosmology 101 – from the NASA WMAP group
Center for Cosmological Physics. University of Chicago, Chicago, Illinois
Origins, Nova Online – Provided by PBS

From individuals

Gale, George, "Cosmology: Methodological Debates in the 1930s and 1940s", The Stanford Encyclopedia of Philosophy, Edward N. Zalta (ed.)
Madore, Barry F., "Level 5 : A Knowledgebase for Extragalactic Astronomy and Cosmology". Caltech and Carnegie. Pasadena, California.
Tyler, Pat, and Newman, Phil, "Beyond Einstein". Laboratory for High Energy Astrophysics (LHEA) NASA Goddard Space Flight Center.
Wright, Ned. "Cosmology tutorial and FAQ". Division of Astronomy & Astrophysics, UCLA.
Musser, George (February 2004). "Four Keys to Cosmology". Scientific American. Retrieved 22 March 2015.
Burgess, Cliff; Quevedo, Fernando (November 2007). "The Great Cosmic Roller-Coaster Ride". Scientific American (print). pp. 52–59. (subtitle) Could cosmic inflation be a sign that our universe is embedded in a far vaster realm?

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@@ Line 3: / Line 3: @@
 {{Use dmy dates|date=July 2019}}
-[[File:CMB Timeline300 no WMAP.jpg|upright=1.5|thumb|Artist conception of the [[Big Bang]] cosmological model, the most widely accepted out of all in physical cosmology (neither time nor size to scale)]]
+[[File:CMB Timeline300 no WMAP.jpg|upright=1.6|thumb|Artist conception of the [[Big Bang]] cosmological model, the most widely accepted out of all in physical cosmology (neither time nor size to scale)]]
 {{Cosmology}}
-'''Physical cosmology''' is a branch of [[cosmology]] concerned with the study of cosmological models.  A '''cosmological model''', or simply '''cosmology''', provides a description of the largest-scale structures and dynamics of the [[universe]] and allows study of fundamental questions about its [[Cosmogony|origin]], structure, [[Chronology of the universe|evolution]], and [[ultimate fate]].<ref name=GFR_Ellis>For an overview, see {{cite book |chapter=Issues in the Philosophy of Cosmology |author=George FR Ellis |arxiv=astro-ph/0602280 |isbn=978-0-444-51560-5 |publisher=North Holland |title=Philosophy of Physics (Handbook of the Philosophy of Science) 3 volume set |editor=Jeremy Butterfield & John Earman|bibcode = 2006astro.ph..2280E |year=2006 }}</ref>  Cosmology as a [[science]] originated with the [[Copernican principle]], which implies that [[astronomical object|celestial bodies]] obey identical [[physical law]]s to those on Earth, and [[Newtonian mechanics]], which first allowed those physical laws to be understood.
+'''Physical cosmology''' is a branch of [[cosmology]] concerned with the study of cosmological models. A '''cosmological model''', or simply '''cosmology''', provides a description of the largest-scale structures and dynamics of the [[universe]] and allows study of fundamental questions about its [[Cosmogony|origin]], structure, [[Chronology of the universe|evolution]], and [[ultimate fate]].<ref name=GFR_Ellis>For an overview, see {{cite book |chapter=Issues in the Philosophy of Cosmology |author=George FR Ellis |arxiv=astro-ph/0602280 |isbn=978-0-444-51560-5 |publisher=North Holland |title=Philosophy of Physics (Handbook of the Philosophy of Science) 3 volume set |editor=Jeremy Butterfield & John Earman|bibcode = 2006astro.ph..2280E |year=2006 }}</ref> Cosmology as a [[science]] originated with the [[Copernican principle]], which implies that [[astronomical object|celestial bodies]] obey identical [[physical law]]s to those on Earth, and [[Newtonian mechanics]], which first allowed those physical laws to be understood.
-Physical cosmology, as it is now understood, began with the development in 1915 of [[Albert Einstein]]'s [[general relativity|general theory of relativity]], followed by major observational discoveries in the 1920s: first, [[Edwin Hubble]] discovered that the universe contains a huge number of external [[Galaxy|galaxies]] beyond the [[Milky Way]]; then, work by [[Vesto Slipher]] and others showed that the universe is [[expanding universe|expanding]]. These advances made it possible to speculate about the origin of the universe, and allowed the establishment of the [[Big Bang]] theory, by [[Georges Lemaître]], as the leading cosmological model. A few researchers still advocate a handful of [[Non-standard cosmology|alternative cosmologies]];<ref>{{Cite web|url=http://cosmologystatement.org/|archive-url=https://web.archive.org/web/20140401081546/http://cosmologystatement.org/|title=An Open Letter to the Scientific Community as published in New Scientist, May 22, 2004|date=2014-04-01|website=cosmologystatement.org|archive-date=1 April 2014|url-status=dead|access-date=2017-09-27}}</ref> however, most cosmologists agree that the Big Bang theory best explains the observations.
+Physical cosmology, as it is now understood, began in 1915 with the development of [[Albert Einstein]]'s [[general relativity|general theory of relativity]], followed by major observational discoveries in the 1920s: first, [[Edwin Hubble]] discovered that the universe contains a huge number of external [[Galaxy|galaxies]] beyond the [[Milky Way]]; then, work by [[Vesto Slipher]] and others showed that the universe is [[expanding universe|expanding]]. These advances made it possible to speculate about the origin of the universe, and allowed the establishment of the [[Big Bang]] theory, by [[Georges Lemaître]], as the leading cosmological model. A few researchers still advocate a handful of [[Non-standard cosmology|alternative cosmologies]];<ref>{{Cite web|url=http://cosmologystatement.org/|archive-url=https://web.archive.org/web/20140401081546/http://cosmologystatement.org/|title=An Open Letter to the Scientific Community as published in New Scientist, May 22, 2004|date=2014-04-01|website=cosmologystatement.org|archive-date=1 April 2014|url-status=dead|access-date=2017-09-27}}</ref> however, most cosmologists agree that the Big Bang theory best explains the observations.
 Dramatic advances in observational cosmology since the 1990s, including the [[cosmic microwave background]], distant [[supernovae]] and galaxy [[redshift survey]]s, have led to the development of a [[Lambda-CDM model|standard model of cosmology]]. This model requires the universe to contain large amounts of [[dark matter]] and [[dark energy]] whose nature is currently not well understood, but the model gives detailed predictions that are in excellent agreement with many diverse observations.<ref name="PDG">{{cite journal | url=http://pdg.ge.infn.it/2011/reviews/rpp2011-rev-cosmological-parameters.pdf |archive-url=https://ghostarchive.org/archive/20221009/http://pdg.ge.infn.it/2011/reviews/rpp2011-rev-cosmological-parameters.pdf |archive-date=2022-10-09 |url-status=live | title=2013 Review of Particle Physics | author=Beringer, J. | author2=et al. (Particle Data Group) | journal=Phys. Rev. D | date=2012 | volume=86 | issue=1 | page=010001|doi=10.1103/PhysRevD.86.010001|bibcode = 2012PhRvD..86a0001B | doi-access=free }}</ref>
@@ Line 16: / Line 16: @@
 == Subject history ==
 <!--[[History of physical cosmology]] redirects here.-->
-{{Nature timeline}}
+{{Nature timeline|upright=0.6}}
 {{see also|Timeline of cosmology|List of cosmologists}}
 Modern cosmology developed along tandem tracks of theory and observation. In 1916, Albert Einstein published his theory of [[general relativity]], which provided a unified description of gravity as a geometric property of space and time.<ref>{{cite web|title=Nobel Prize Biography|url=http://nobelprize.org/nobel_prizes/physics/laureates/1921/einstein-bio.html|publisher=Nobel Prize|access-date=25 February 2011}}</ref> At the time, Einstein believed in a [[static universe]], but found that his original formulation of the theory did not permit it.<ref name="Liddle, A. 51">{{cite book | author = Liddle, A. | title = An Introduction to Modern Cosmology | url = https://archive.org/details/introductiontomo00lidd_717 | url-access = limited | publisher = Wiley | page=[https://archive.org/details/introductiontomo00lidd_717/page/n67 51] | isbn =978-0-470-84835-7 | date = 2003 }}</ref> This is because masses distributed throughout the universe gravitationally attract, and move toward each other over time.<ref>{{cite book | last = Vilenkin | first = Alex | title = Many worlds in one: the search for other universes | publisher = Hill and Wang, A division of Farrar, Straus and Giroux | location = New York | date = 2007 | isbn = 978-0-8090-6722-0 | page=19}}</ref> However, he realized that his equations permitted the introduction of a constant term which could counteract the attractive force of gravity on the cosmic scale. Einstein published his first paper on relativistic cosmology in 1917, in which he added this ''[[cosmological constant]]'' to his field equations in order to force them to model a static universe.<ref>{{cite book |last1=Jones |first1=Mark |last2=Lambourne |first2=Robert | title = An introduction to galaxies and cosmology | publisher = Open University Cambridge University Press | location = Milton Keynes Cambridge, UK; New York | date = 2004 | isbn = 978-0-521-54623-2 | page= 228}}</ref> The Einstein model describes a static universe; space is finite and unbounded (analogous to the surface of a sphere, which has a finite area but no edges). However, this so-called Einstein model is unstable to small perturbations—it will eventually start to [[metric expansion of space|expand]] or contract.<ref name="Liddle, A. 51"/> It was later realized that Einstein's model was just one of a larger set of possibilities, all of which were consistent with general relativity and the [[cosmological principle]]. The cosmological solutions of general relativity were found by [[Alexander Friedmann]] in the early 1920s.<ref>{{cite book |last1=Jones |first1=Mark |last2=Lambourne |first2=Robert | title = An introduction to galaxies and cosmology | publisher = Open University Cambridge University Press | location = Milton Keynes Cambridge, UK; New York | date = 2004 | isbn = 978-0-521-54623-2 |page=232 }}</ref> His equations describe the [[Friedmann–Lemaître–Robertson–Walker]] universe, which may expand or contract, and whose geometry may be open, flat, or closed.
-[[File:History of the Universe.svg|thumb|left|350px|History of the [[Universe]] – [[gravitational wave]]s are hypothesized to arise from [[Inflation (cosmology)|cosmic inflation]], a rapidly accelerated expansion just after the [[Big Bang]]<ref name="BICEP2-2014" /><ref name="NASA-20140317" /><ref name="NYT-20140317" />]]
+[[File:History of the Universe.svg|thumb|upright=1.9|History of the [[Universe]] – [[gravitational wave]]s are hypothesized to arise from [[Inflation (cosmology)|cosmic inflation]], a rapidly accelerated expansion just after the [[Big Bang]]<ref name="BICEP2-2014" /><ref name="NASA-20140317" /><ref name="NYT-20140317" />]]
-In the 1910s, [[Vesto Melvin Slipher|Vesto Slipher]] (and later [[Carl Wilhelm Wirtz]]) interpreted the [[red shift]] of [[nebula|spiral nebulae]] as a [[Doppler shift]] that indicated they were receding from Earth.<ref>{{cite journal | last1=Slipher | first1=V. M. | title=Further Notes on Spectrographic Observations of Nebulae and Clusters | journal=Publications of the American Astronomical Society| volume=4| date=1922 | pages=284–286 | bibcode=1922PAAS....4..284S }}</ref><ref>{{cite journal | last1=Seitter | first1=Waltraut C. | last2=Duerbeck | first2=Hilmar W. | title=Carl Wilhelm Wirtz – Pioneer in Cosmic Dimensions  | journal=Harmonizing Cosmic Distance Scales in a Post-Hipparcos Era | series=ASP Conference Series | volume=167 | editor1-first=Daniel | editor1-last=Egret | editor2-first=Andre | editor2-last=Heck | isbn=978-1-886733-88-6 | date=1999 | pages=237–242 | bibcode=1999ASPC..167..237S }}</ref> However, it is difficult to determine the distance to astronomical objects. One way is to compare the physical size of an object to its [[angular size]], but a physical size must be assumed to do this. Another method is to measure the [[brightness]] of an object and assume an intrinsic [[luminosity]], from which the distance may be determined using the [[inverse-square law]]. Due to the difficulty of using these methods, they did not realize that the nebulae were actually galaxies outside our own [[Milky Way]], nor did they speculate about the cosmological implications. In 1927, the [[Belgium|Belgian]] [[Roman Catholic]] [[priest]] [[Georges Lemaître]] independently derived the Friedmann–Lemaître–Robertson–Walker equations and proposed, on the basis of the recession of spiral nebulae, that the universe began with the "explosion" of a "primeval [[atom]]"<ref>{{cite journal | last1=Lemaître | first1=G. | title=Un Univers homogène de masse constante et de rayon croissant rendant compte de la vitesse radiale des nébuleuses extra-galactiques | journal=Annales de la Société Scientifique de Bruxelles | volume=A47 | pages=49–59 | date=1927 | language=fr | bibcode=1927ASSB...47...49L }}</ref>—which was later called the Big Bang. In 1929, [[Edwin Hubble]] provided an observational basis for Lemaître's theory. Hubble showed that the spiral nebulae were galaxies by determining their distances using measurements of the brightness of [[Cepheid variable]] stars. He discovered a relationship between the redshift of a galaxy and its distance. He interpreted this as evidence that the galaxies are receding from Earth in every direction at speeds proportional to their distance.<ref>{{cite journal | last1=Hubble | first1=Edwin  | title=A Relation between Distance and Radial Velocity among Extra-Galactic Nebulae | journal=Proceedings of the National Academy of Sciences of the United States of America | volume=15 | issue=3 | pages=168–173 | date=March 1929 | doi=10.1073/pnas.15.3.168  | bibcode=1929PNAS...15..168H | pmid=16577160 | pmc=522427| doi-access=free }}</ref> This fact is now known as [[Hubble's law]], though the numerical factor Hubble found relating recessional velocity and distance was off by a factor of ten, due to not knowing about the types of Cepheid variables.
+In the 1910s, [[Vesto Melvin Slipher|Vesto Slipher]] (and later [[Carl Wilhelm Wirtz]]) interpreted the [[red shift]] of [[nebula|spiral nebulae]] as a [[Doppler shift]] that indicated they were receding from Earth.<ref>{{cite journal | last1=Slipher | first1=V. M. | title=Further Notes on Spectrographic Observations of Nebulae and Clusters | journal=Publications of the American Astronomical Society| volume=4| date=1922 | pages=284–286 | bibcode=1922PAAS....4..284S }}</ref><ref>{{cite journal | last1=Seitter | first1=Waltraut C. | last2=Duerbeck | first2=Hilmar W. | title=Carl Wilhelm Wirtz – Pioneer in Cosmic Dimensions  | journal=Harmonizing Cosmic Distance Scales in a Post-Hipparcos Era | series=ASP Conference Series | volume=167 | editor1-first=Daniel | editor1-last=Egret | editor2-first=Andre | editor2-last=Heck | isbn=978-1-886733-88-6 | date=1999 | pages=237–242 | bibcode=1999ASPC..167..237S }}</ref> However, it is difficult to determine the distance to astronomical objects. One way is to compare the physical size of an object to its [[angular size]], but a physical size must be assumed in order to do this. Another method is to measure the [[brightness]] of an object and assume an intrinsic [[luminosity]], from which the distance may be determined using the [[inverse-square law]]. Due to the difficulty of using these methods, they did not realize that the nebulae were actually galaxies outside our own [[Milky Way]], nor did they speculate about the cosmological implications. In 1927, the [[Belgium|Belgian]] [[Roman Catholic]] [[priest]] [[Georges Lemaître]] independently derived the Friedmann–Lemaître–Robertson–Walker equations and proposed, on the basis of the recession of spiral nebulae, that the universe began with the "explosion" of a "primeval [[atom]]"<ref>{{cite journal |last1=Lemaître |first1=Georges |date=1927 |title=Un Univers homogène de masse constante et de rayon croissant rendant compte de la vitesse radiale des nébuleuses extra-galactiques |journal=Annales de la Société Scientifique de Bruxelles |language=fr |volume=A47 |pages=49–59 |bibcode=1927ASSB...47...49L}}</ref>—which was later called the Big Bang. In 1929, [[Edwin Hubble]] provided an observational basis for Lemaître's theory. Hubble showed that the spiral nebulae were galaxies by determining their distances using measurements of the brightness of [[Cepheid variable]] stars. He discovered a relationship between the redshift of a galaxy and its distance. He interpreted this as evidence that the galaxies are receding from Earth in every direction at speeds proportional to their distance from Earth.<ref>{{cite journal | last1=Hubble | first1=Edwin  | title=A Relation between Distance and Radial Velocity among Extra-Galactic Nebulae | journal=Proceedings of the National Academy of Sciences of the United States of America | volume=15 | issue=3 | pages=168–173 | date=March 1929 | doi=10.1073/pnas.15.3.168  | bibcode=1929PNAS...15..168H | pmid=16577160 | pmc=522427| doi-access=free }}</ref> This fact is now known as [[Hubble's law]], though the numerical factor Hubble found relating recessional velocity and distance was off by a factor of ten, due to not knowing about the types of Cepheid variables.
-Given the cosmological principle, Hubble's law suggested that the universe was expanding. Two primary explanations were proposed for the expansion. One was Lemaître's Big Bang theory, advocated and developed by George Gamow. The other explanation was [[Fred Hoyle]]'s [[steady state model]] in which new matter is created as the galaxies move away from each other. In this model, the universe is roughly the same at any point in time.<ref>{{cite journal | last1=Hoyle | first1=F. | title=A New Model for the Expanding Universe | journal=Monthly Notices of the Royal Astronomical Society | volume=108 | issue=5 | pages=372–382 | date=1948 | bibcode=1948MNRAS.108..372H | doi=10.1093/mnras/108.5.372| doi-access=free }}</ref><ref name="aip">{{cite web | title=Big Bang or Steady State? | work=Ideas of Cosmology | publisher=American Institute of Physics | url=https://www.aip.org/history/cosmology/ideas/bigbang.htm | access-date=2015-07-29 | archive-date=12 June 2015 | archive-url=https://web.archive.org/web/20150612115523/http://www.aip.org/history/cosmology/ideas/bigbang.htm | url-status=dead }}</ref>
+Given the cosmological principle, Hubble's law suggested that the universe was expanding. Two primary explanations were proposed for the expansion. One was Lemaître's Big Bang theory, advocated and developed by [[George Gamow|George Gamow.]] The other explanation was [[Fred Hoyle]]'s [[steady state model]] in which new matter is created as the galaxies move away from each other. In this model, the universe is roughly the same at any point in time.<ref>{{cite journal |last1=Hoyle |first1=Fred |date=1948 |title=A New Model for the Expanding Universe |journal=Monthly Notices of the Royal Astronomical Society |volume=108 |issue=5 |pages=372–382 |bibcode=1948MNRAS.108..372H |doi=10.1093/mnras/108.5.372 |doi-access=free}}</ref><ref name="aip">{{cite web | title=Big Bang or Steady State? | work=Ideas of Cosmology | publisher=American Institute of Physics | url=https://www.aip.org/history/cosmology/ideas/bigbang.htm | access-date=2015-07-29 | archive-date=12 June 2015 | archive-url=https://web.archive.org/web/20150612115523/http://www.aip.org/history/cosmology/ideas/bigbang.htm | url-status=dead }}</ref>
-For a number of years, support for these theories was evenly divided. However, the observational evidence began to support the idea that the universe evolved from a hot dense state. The discovery of the cosmic microwave background in 1965 lent strong support to the Big Bang model,<ref name="aip"/> and since the precise measurements of the cosmic microwave background by the [[Cosmic Background Explorer]] in the early 1990s, few cosmologists have seriously proposed other theories of the origin and evolution of the cosmos. One consequence of this is that in standard general relativity, the universe began with a [[Gravitational singularity|singularity]], as demonstrated by [[Roger Penrose]] and [[Stephen Hawking]] in the 1960s.<ref name=Earman1999>{{cite book | last1=Earman | first1=John | title=The Penrose-Hawking Singularity Theorems: History and Implications – The expanding worlds of general relativity | journal=The Expanding Worlds of General Relativity | pages=235–267 | editor1-first=Hubert | editor1-last=Goenner | editor2-last=Jürgen | editor3-first=Jim | editor3-last=Ritter | editor4-first=Tilman | editor4-last=Sauer | series=Birk presentations of the fourth conference on the and gravitation | year=1999 | bibcode=1999ewgr.book..235E | doi=10.1007/978-1-4612-0639-2_7 | doi-broken-date=23 January 2024 | isbn=978-1-4612-6850-5 }}</ref>
+For a number of years, support for these theories was evenly divided. However, the observational evidence began to support the idea that the universe evolved from a hot dense state. The discovery of the cosmic microwave background in 1965 lent strong support to the Big Bang model,<ref name="aip"/> and since the precise measurements of the cosmic microwave background by the [[Cosmic Background Explorer]] in the early 1990s, few cosmologists have seriously proposed other theories of the origin and evolution of the cosmos. One consequence of this is that in standard general relativity, the universe began with a [[Gravitational singularity|singularity]], as demonstrated by [[Roger Penrose]] and [[Stephen Hawking]] in the 1960s.<ref name=Earman1999>{{cite book | last1=Earman | first1=John | title=The Penrose-Hawking Singularity Theorems: History and Implications – The expanding worlds of general relativity | journal=The Expanding Worlds of General Relativity | pages=235–267 | editor1-first=Hubert | editor1-last=Goenner | editor2-last=Jürgen | editor3-first=Jim | editor3-last=Ritter | editor4-first=Tilman | editor4-last=Sauer | series=Birk presentations of the fourth conference on the and gravitation | year=1999 | bibcode=1999ewgr.book..235E | doi=10.1007/978-1-4612-0639-2_7 | doi-broken-date=1 November 2024 | isbn=978-1-4612-6850-5 }}</ref>
 An alternative view to extend the Big Bang model, suggesting the universe had no beginning or singularity and the age of the universe is infinite, has been presented.<ref name="LS-20150226">{{cite web |last=Ghose |first=Tia |title=Big Bang, Deflated? Universe May Have Had No Beginning |url=http://www.livescience.com/49958-theory-no-big-bang.html |date=26 February 2015 |website=[[Live Science]] |access-date=28 February 2015 }}</ref><ref name="PL-20150204">{{cite journal |last=Ali |first=Ahmed Faraq |title=Cosmology from quantum potential |journal=[[Physics Letters B]] |volume=741 |issue=2015 |pages=276–279 |doi=10.1016/j.physletb.2014.12.057 |date=4 February 2015 |arxiv=1404.3093 |bibcode=2015PhLB..741..276F |s2cid=55463396 }}</ref><ref name="AR-20141118">{{cite journal|last1=Das|first1=Saurya|last2=Bhaduri|first2=Rajat K|title=Dark matter and dark energy from a Bose–Einstein condensate|journal=Classical and Quantum Gravity|date=21 May 2015|volume=32|issue=10|pages=105003|doi=10.1088/0264-9381/32/10/105003|arxiv = 1411.0753 |bibcode = 2015CQGra..32j5003D |s2cid=119247745}}</ref>
@@ Line 49: / Line 49: @@
 Within the [[standard cosmological model]], the [[equations of motion]] governing the universe as a whole are derived from general relativity with a small, positive cosmological constant.<ref>
+{{cite journal |author=Ojeda |first1=P. |last2=Rosu |first2=H. |date=June 2006 |title=Supersymmetry of FRW barotropic cosmologies |journal=Int. J. Theor. Phys. |volume=45 |issue=6 |pages=1191–1196 |arxiv=gr-qc/0510004 |bibcode=2006IJTP...45.1152R |doi=10.1007/s10773-006-9123-2 |s2cid=119496918}}
-{{cite journal
+</ref> The solution is an expanding universe; due to this expansion, the radiation and matter in the universe cool and become diluted. At first, the expansion is slowed down by [[gravitation]] attracting the radiation and matter in the universe. However, as these become diluted, the cosmological constant becomes more dominant and the expansion of the universe starts to accelerate rather than decelerate. In our universe this happened billions of years ago.<ref name=Springel2006>{{cite journal | title=The large-scale structure of the Universe | last1=Springel | first1=Volker | last2=Frenk | first2=Carlos S. | last3=White | first3=Simon D.M. | journal=Nature | volume=440 | issue=7088 | pages=1137–1144 | year=2006 | doi=10.1038/nature04805 | pmid=16641985 | bibcode=2006Natur.440.1137S | arxiv=astro-ph/0604561 | citeseerx=10.1.1.255.8877 | s2cid=8900982 }}</ref>
-| title = Supersymmetry of FRW barotropic cosmologies
-| author = P. Ojeda
-| author2 = H. Rosu
-| journal = Int. J. Theor. Phys.
-|  volume = 45
-|  pages = 1191–1196
-|date=June 2006
-|  doi = 10.1007/s10773-006-9123-2
-|arxiv = gr-qc/0510004 |bibcode = 2006IJTP...45.1152R
-| issue = 6 | s2cid = 119496918
-}}
-</ref> The solution is an expanding universe; due to this expansion, the radiation and matter in the universe cool down and become diluted. At first, the expansion is slowed down by [[gravitation]] attracting the radiation and matter in the universe. However, as these become diluted, the cosmological constant becomes more dominant and the expansion of the universe starts to accelerate rather than decelerate. In our universe this happened billions of years ago.<ref name=Springel2006>{{cite journal | title=The large-scale structure of the Universe | last1=Springel | first1=Volker | last2=Frenk | first2=Carlos S. | last3=White | first3=Simon D.M. | journal=Nature | volume=440 | issue=7088 | pages=1137–1144 | year=2006 | doi=10.1038/nature04805 | pmid=16641985 | bibcode=2006Natur.440.1137S | arxiv=astro-ph/0604561 | citeseerx=10.1.1.255.8877 | s2cid=8900982 }}</ref>
 ===Particle physics in cosmology===
@@ Line 79: / Line 68: @@
 |access-date = 2013-04-25}}
 </ref> Since then, the evolution of the universe has passed through three phases. The very early universe, which is still poorly understood, was the split second in which the universe was so hot that [[subatomic particle|particles]] had energies higher than those currently accessible in [[particle accelerator]]s on Earth. Therefore, while the basic features of this epoch have been worked out in the Big Bang theory, the details are largely based on educated guesses.
 Following this, in the early universe, the evolution of the universe proceeded according to known [[high energy physics]]. This is when the first protons, electrons and neutrons formed, then nuclei and finally atoms. With the formation of neutral hydrogen, the [[cosmic microwave background]] was emitted. Finally, the epoch of structure formation began, when matter started to aggregate into the first [[star]]s and [[quasar]]s, and ultimately galaxies, [[clusters of galaxies]] and [[supercluster]]s formed. The future of the universe is not yet firmly known, but according to the [[ΛCDM]] model it will continue expanding forever.
@@ Line 85: / Line 75: @@
 ===Very early universe===
+[[File:Big bang inflation vs standard genericchart.png|thumb|upright=1.2|The inflationary theory as an augmentation to the Big Bang theory was first proposed by Alan Guth of MIT. Inflation solves the 'horizon problem' by making the early universe much more compact than was assumed in the standard model. Given such smaller size, causal contact (i.e., thermal communication) would have been possible among all regions of the early universe. The image was an adaptation from various generic charts depicting the growth of the size of the observable universe, for both the standard model and inflationary model respectively, of the Big Bang theory.]]
 The early, hot universe appears to be well explained by the Big Bang from roughly 10<sup>−33</sup> seconds onwards, but there are several [[Big Bang#Problems|problems]]. One is that there is no compelling reason, using current particle physics, for the universe to be [[shape of the universe|flat]], homogeneous, and [[isotropic]] ''(see the [[cosmological principle]])''. Moreover, [[grand unified theory|grand unified theories]] of particle physics suggest that there should be [[magnetic monopole]]s in the universe, which have not been found. These problems are resolved by a brief period of [[cosmic inflation]], which drives the universe to [[Flatness (cosmology)|flatness]], smooths out [[Anisotropy|anisotropies]] and inhomogeneities to the observed level, and exponentially dilutes the monopoles.<ref name=Guth1981>{{cite journal | title=Inflationary universe: A possible solution to the horizon and flatness problems | last1=Guth | first1=Alan H. | journal=Physical Review D | volume=23 | issue=2 | date=15 January 1981 | pages=347–356 | doi=10.1103/PhysRevD.23.347 | bibcode=1981PhRvD..23..347G | doi-access=free }}</ref> The physical model behind cosmic inflation is extremely simple, but it has not yet been confirmed by particle physics, and there are difficult problems reconciling inflation and [[quantum field theory]].{{Vague|date=April 2018}} Some cosmologists think that [[string theory]] and [[brane cosmology]] will provide an alternative to inflation.<ref name=Pogosian2003>{{cite journal | title=Observational constraints on cosmic string production during brane inflation | last1=Pogosian | first1=Levon | last2=Tye | first2=S.-H. Henry | last3=Wasserman | first3=Ira | last4=Wyman | first4=Mark | journal=Physical Review D | volume=68 | issue=2 | page=023506 | year=2003 | doi=10.1103/PhysRevD.68.023506 | bibcode=2003PhRvD..68b3506P | arxiv=hep-th/0304188 }}</ref>
-Another major problem in cosmology is what caused the universe to contain far more matter than [[antimatter]]. Cosmologists can observationally deduce that the universe is not split into regions of matter and antimatter. If it were, there would be [[X-ray]]s and [[gamma ray]]s produced as a result of [[annihilation]], but this is not observed. Therefore, some process in the early universe must have created a small excess of matter over antimatter, and this (currently not understood) process is called ''[[baryogenesis]]''. Three required conditions for baryogenesis were derived by [[Andrei Sakharov]] in 1967, and requires a violation of the particle physics [[Symmetry#In physics|symmetry]], called [[CP-symmetry]], between matter and antimatter.<ref name=Canetti2012>{{cite journal | title=Matter and antimatter in the universe | display-authors=1 | first1=Laurent | last1=Canetti | first2=Marco | last2=Drewes | first3=Mikhail | last3=Shaposhnikov | journal=New Journal of Physics | volume=14 | issue=9 | pages=095012 | date=September 2012 | doi=10.1088/1367-2630/14/9/095012 | bibcode=2012NJPh...14i5012C | arxiv=1204.4186 | s2cid=119233888 }}</ref> However, particle accelerators measure too small a violation of CP-symmetry to account for the baryon asymmetry. Cosmologists and particle physicists look for additional violations of the CP-symmetry in the early universe that might account for the baryon asymmetry.<ref name=Pandolfi2017>{{cite web | title=New source of asymmetry between matter and antimatter | first1=Stefania | last1=Pandolfi | date=30 January 2017 | publisher=CERN | url=https://home.cern/about/updates/2017/01/new-source-asymmetry-between-matter-and-antimatter | access-date=2018-04-09 }}</ref>
+Another major problem in cosmology is what caused the universe to contain far more matter than [[antimatter]]. Cosmologists can observationally deduce that the universe is not split into regions of matter and antimatter. If it were, there would be [[X-ray]]s and [[gamma ray]]s produced as a result of [[annihilation]], but this is not observed. Therefore, some process in the early universe must have created a small excess of matter over antimatter, and this (currently not understood) process is called ''[[baryogenesis]]''. Three required conditions for baryogenesis were derived by [[Andrei Sakharov]] in 1967, and requires a violation of the particle physics [[Symmetry#In physics|symmetry]], called [[CP-symmetry]], between matter and antimatter.<ref name=Canetti2012>{{cite journal | title=Matter and antimatter in the universe | display-authors=1 | first1=Laurent | last1=Canetti | first2=Marco | last2=Drewes | first3=Mikhail | last3=Shaposhnikov | journal=New Journal of Physics | volume=14 | issue=9 | pages=095012 | date=September 2012 | doi=10.1088/1367-2630/14/9/095012 | bibcode=2012NJPh...14i5012C | arxiv=1204.4186 | s2cid=119233888 }}</ref> However, particle accelerators measure too small a violation of CP-symmetry to account for the baryon asymmetry. Cosmologists and particle physicists look for additional violations of the CP-symmetry in the early universe that might account for the [[baryon asymmetry]].<ref name=Pandolfi2017>{{cite web | title=New source of asymmetry between matter and antimatter | first1=Stefania | last1=Pandolfi | date=30 January 2017 | publisher=CERN | url=https://home.cern/about/updates/2017/01/new-source-asymmetry-between-matter-and-antimatter | access-date=2018-04-09 }}</ref>
 Both the problems of baryogenesis and cosmic inflation are very closely related to particle physics, and their resolution might come from high energy theory and [[particle accelerator|experiment]], rather than through observations of the universe.{{speculation inline|date=April 2018}}<!-- This statement is both speculative and somewhat obvious. It will either be one, the other, or none. Is it needed? -->
@@ Line 93: / Line 84: @@
 ===Big Bang Theory===
 {{Main|Big Bang nucleosynthesis}}
-Big Bang nucleosynthesis is the theory of the formation of the elements in the early universe. It finished when the universe was about three minutes old and its [[temperature]] dropped below that at which [[nuclear fusion]] could occur. Big Bang nucleosynthesis had a brief period during which it could operate, so only the very lightest elements were produced. Starting from hydrogen [[ion]]s ([[proton]]s), it principally produced [[deuterium]], [[helium|helium-4]], and [[lithium]]. Other elements were produced in only trace abundances. The basic theory of nucleosynthesis was developed in 1948 by [[George Gamow]], [[Ralph Asher Alpher]], and [[Robert Herman]].<ref name=Peebles2014>{{cite journal | title=Discovery of the hot Big Bang: What happened in 1948 | last1=Peebles | first1=Phillip James Edwin | journal=The European Physical Journal H | volume=39 | issue=2 | pages=205–223 | date=April 2014 | doi=10.1140/epjh/e2014-50002-y | bibcode=2014EPJH...39..205P | arxiv=1310.2146 | s2cid=118539956 }}</ref> It was used for many years as a probe of physics at the time of the Big Bang, as the theory of Big Bang nucleosynthesis connects the abundances of primordial light elements with the features of the early universe.<ref name=Burles2001>{{cite journal | title=Big Bang Nucleosynthesis Predictions for Precision Cosmology | last1=Burles | first1=Scott | last2=Nollett | first2=Kenneth M. | last3=Turner | first3=Michael S. | journal=The Astrophysical Journal | volume=552 | issue=1 | pages=L1–L5 | date=May 2001 | doi=10.1086/320251 | bibcode=2001ApJ...552L...1B | arxiv=astro-ph/0010171 | s2cid=118904816 }}</ref> Specifically, it can be used to test the [[equivalence principle]],<ref name=Boucher2004>{{cite journal | title=Cosmic microwave background constraints on the strong equivalence principle | last1=Boucher | first1=V. | last2=Gérard | first2=J.-M. | last3=Vandergheynst | first3=P. | last4=Wiaux | first4=Y. | journal=Physical Review D | volume=70 | issue=10 | page=103528 | date=November 2004 | doi=10.1103/PhysRevD.70.103528 | bibcode=2004PhRvD..70j3528B | arxiv=astro-ph/0407208 | s2cid=1197376 }}</ref> to probe [[dark matter]], and test [[neutrino]] physics.<ref name=Cyburt2016>{{cite journal | title=Big bang nucleosynthesis: Present status | last1=Cyburt | first1=Richard H. | last2=Fields | first2=Brian D. | last3=Olive | first3=Keith A. | last4=Yeh | first4=Tsung-Han | journal=Reviews of Modern Physics | volume=88 | issue=1 | page=015004 | date=January 2016 | doi=10.1103/RevModPhys.88.015004 | bibcode=2016RvMP...88a5004C | arxiv=1505.01076 | s2cid=118409603}}</ref> Some cosmologists have proposed that Big Bang nucleosynthesis suggests there is a fourth "sterile" species of neutrino.<ref name=Lucente2018>{{cite arXiv| title=Leptogenesis, dark matter and neutrino masses | last1=Lucente | first1=Michele | last2=Abada | first2=Asmaa | last3=Arcadi | first3=Giorgio | last4=Domcke | first4=Valerie  | eprint=1803.10826 | date=March 2018| class=hep-ph }}</ref>
+Big Bang nucleosynthesis is the theory of the formation of the elements in the early universe. It finished when the universe was about three minutes old and its [[temperature]] dropped below that at which [[nuclear fusion]] could occur. Big Bang nucleosynthesis had a brief period during which it could operate, so only the very lightest elements were produced. Starting from hydrogen [[ion]]s ([[proton]]s), it principally produced [[deuterium]], [[helium|helium-4]], and [[lithium]]. Other elements were produced in only trace abundances. The basic theory of nucleosynthesis was developed in 1948 by George Gamow, [[Ralph Asher Alpher]], and [[Robert Herman]].<ref name=Peebles2014>{{cite journal | title=Discovery of the hot Big Bang: What happened in 1948 | last1=Peebles | first1=Phillip James Edwin | journal=The European Physical Journal H | volume=39 | issue=2 | pages=205–223 | date=April 2014 | doi=10.1140/epjh/e2014-50002-y | bibcode=2014EPJH...39..205P | arxiv=1310.2146 | s2cid=118539956 }}</ref> It was used for many years as a probe of physics at the time of the Big Bang, as the theory of Big Bang nucleosynthesis connects the abundances of primordial light elements with the features of the early universe.<ref name=Burles2001>{{cite journal | title=Big Bang Nucleosynthesis Predictions for Precision Cosmology | last1=Burles | first1=Scott | last2=Nollett | first2=Kenneth M. | last3=Turner | first3=Michael S. | journal=The Astrophysical Journal | volume=552 | issue=1 | pages=L1–L5 | date=May 2001 | doi=10.1086/320251 | bibcode=2001ApJ...552L...1B | arxiv=astro-ph/0010171 | s2cid=118904816 }}</ref> Specifically, it can be used to test the [[equivalence principle]],<ref name=Boucher2004>{{cite journal | title=Cosmic microwave background constraints on the strong equivalence principle | last1=Boucher | first1=V. | last2=Gérard | first2=J.-M. | last3=Vandergheynst | first3=P. | last4=Wiaux | first4=Y. | journal=Physical Review D | volume=70 | issue=10 | page=103528 | date=November 2004 | doi=10.1103/PhysRevD.70.103528 | bibcode=2004PhRvD..70j3528B | arxiv=astro-ph/0407208 | s2cid=1197376 }}</ref> to probe [[dark matter]], and test [[neutrino]] physics.<ref name=Cyburt2016>{{cite journal | title=Big bang nucleosynthesis: Present status | last1=Cyburt | first1=Richard H. | last2=Fields | first2=Brian D. | last3=Olive | first3=Keith A. | last4=Yeh | first4=Tsung-Han | journal=Reviews of Modern Physics | volume=88 | issue=1 | page=015004 | date=January 2016 | doi=10.1103/RevModPhys.88.015004 | bibcode=2016RvMP...88a5004C | arxiv=1505.01076 | s2cid=118409603}}</ref> Some cosmologists have proposed that Big Bang nucleosynthesis suggests there is a fourth "sterile" species of neutrino.<ref name=Lucente2018>{{cite arXiv| title=Leptogenesis, dark matter and neutrino masses | last1=Lucente | first1=Michele | last2=Abada | first2=Asmaa | last3=Arcadi | first3=Giorgio | last4=Domcke | first4=Valerie  | eprint=1803.10826 | date=March 2018| class=hep-ph }}</ref>
 ====Standard model of Big Bang cosmology====
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  |page=A133
 |bibcode = 2016A&A...586A.133P |s2cid=9857299
+ }}</ref><ref name="NYT-20140922">{{cite news |last=Overbye |first=Dennis |author-link=Dennis Overbye |date=22 September 2014 |title=Study Confirms Criticism of Big Bang Finding |url=https://www.nytimes.com/2014/09/23/science/space/study-confirms-criticism-of-big-bang-finding.html |url-access=limited |archive-url=https://ghostarchive.org/archive/20220101/https://www.nytimes.com/2014/09/23/science/space/study-confirms-criticism-of-big-bang-finding.html |archive-date=2022-01-01 |access-date=2014-09-22 |work=[[The New York Times]]}}{{cbignore}}</ref> On 30 January 2015, a joint analysis of BICEP2 and [[Planck (spacecraft)|Planck]] data was published and the [[European Space Agency]] announced that the signal can be entirely attributed to interstellar dust in the Milky Way.<ref name="nature-20150130">{{cite news|last=Cowen|first=Ron|title=Gravitational waves discovery now officially dead|date=30 January 2015|newspaper=nature|doi=10.1038/nature.2015.16830}}<!--|access-date=2015-10-26--></ref>
- }}</ref><ref name="NYT-20140922">{{cite news
- |last=Overbye |first=D. |author-link=Dennis Overbye
- |date=22 September 2014
- |title=Study Confirms Criticism of Big Bang Finding
- |url=https://www.nytimes.com/2014/09/23/science/space/study-confirms-criticism-of-big-bang-finding.html |archive-url=https://ghostarchive.org/archive/20220101/https://www.nytimes.com/2014/09/23/science/space/study-confirms-criticism-of-big-bang-finding.html |archive-date=2022-01-01 |url-access=limited
- |work=[[The New York Times]]
- |access-date=2014-09-22
-}}{{cbignore}}</ref> On 30 January 2015, a joint analysis of BICEP2 and [[Planck (spacecraft)|Planck]] data was published and the [[European Space Agency]] announced that the signal can be entirely attributed to interstellar dust in the Milky Way.<ref name="nature-20150130">{{cite news|last=Cowen|first=Ron|title=Gravitational waves discovery now officially dead|date=30 January 2015|newspaper=nature|doi=10.1038/nature.2015.16830}}<!--|access-date=2015-10-26--></ref>
 ===Formation and evolution of large-scale structure===
 {{Main|Large-scale structure of the cosmos|Structure formation|Galaxy formation and evolution}}
-Understanding the formation and evolution of the largest and earliest structures (i.e., quasars, galaxies, [[galaxy groups and clusters|clusters]] and [[supercluster]]s) is one of the largest efforts in cosmology. Cosmologists study a model of '''hierarchical structure formation''' in which structures form from the bottom up, with smaller objects forming first, while the largest objects, such as superclusters, are still assembling.<ref name=Hess2013>{{cite journal | title=Simulating structure formation of the Local Universe | last1=Heß | first1=Steffen | last2=Kitaura | first2=Francisco-Shu | last3=Gottlöber | first3=Stefan | journal=Monthly Notices of the Royal Astronomical Society | volume=435 | issue=3 | pages=2065–2076 | date=November 2013 | doi=10.1093/mnras/stt1428 | bibcode=2013MNRAS.435.2065H | arxiv=1304.6565 | s2cid=119198359 }}</ref> One way to study structure in the universe is to survey the visible galaxies, in order to construct a three-dimensional picture of the galaxies in the universe and measure the matter [[power spectrum]]. This is the approach of the ''[[Sloan Digital Sky Survey]]'' and the [[2dF Galaxy Redshift Survey]].<ref name=Cole2005>{{cite journal | title=The 2dF Galaxy Redshift Survey: power-spectrum analysis of the final data set and cosmological implications | display-authors=6 | last1=Cole | first1=Shaun | last2=Percival | first2=Will J. | last3=Peacock | first3=John A. | last4=Norberg | first4=Peder | last5=Baugh | first5=Carlton M. | last6=Frenk | first6=Carlos S. | last7=Baldry | first7=Ivan | last8=Bland-Hawthorn | first8=Joss | last9=Bridges | first9=Terry | last10=Cannon | first10=Russell | last11=Colless | first11=Matthew | last12=Collins | first12=Chris | last13=Couch | first13=Warrick | last14=Cross | first14=Nicholas J. G. | last15=Dalton | first15=Gavin | last16=Eke | first16=Vincent R. | last17=De Propris | first17=Roberto | last18=Driver | first18=Simon P. | last19=Efstathiou | first19=George | last20=Ellis | first20=Richard S. | last21=Glazebrook | first21=Karl | last22=Jackson | first22=Carole | last23=Jenkins | first23=Adrian | last24=Lahav | first24=Ofer | last25=Lewis | first25=Ian | last26=Lumsden | first26=Stuart | last27=Maddox | first27=Steve | last28=Madgwick | first28=Darren | last29=Peterson | first29=Bruce A. | last30=Sutherland | first30=Will | last31=Taylor | first31=Keith | journal=Monthly Notices of the Royal Astronomical Society | volume=362 | issue=2 | pages=505–534 | year=2005 | doi=10.1111/j.1365-2966.2005.09318.x | bibcode=2005MNRAS.362..505C | arxiv=astro-ph/0501174 | s2cid=6906627 }}</ref><ref name=Nichol2007>{{cite journal | title=The Shape of the Sloan Digital Sky Survey Data Release 5 Galaxy Power Spectrum | display-authors=1 | last1=Percival | first1=Will J. | last2=Nichol | first2=Robert C. | last3=Eisenstein | first3=Daniel J. | last4=Frieman | first4=Joshua A. | last5=Fukugita | first5=Masataka | last6=Loveday | first6=Jon | last7=Pope | first7=Adrian C. | last8=Schneider | first8=Donald P. | last9=Szalay | first9=Alex S. | last10=Tegmark | first10=Max | last11=Vogeley | first11=Michael S. | last12=Weinberg | first12=David H. | last13=Zehavi | first13=Idit | last14=Bahcall | first14=Neta A. | last15=Brinkmann | first15=Jon | last16=Connolly | first16=Andrew J. | last17=Meiksin | first17=Avery | journal=The Astrophysical Journal | volume=657 | issue=2 | pages=645–663 | year=2007 | doi=10.1086/510615 | bibcode=2007ApJ...657..645P | arxiv=astro-ph/0608636 | s2cid=53141475 }}</ref>
+Understanding the formation and evolution of the largest and earliest structures (i.e., quasars, galaxies, [[galaxy groups and clusters|clusters]] and [[supercluster]]s) is one of the largest efforts in cosmology. Cosmologists study a model of '''hierarchical structure formation''' in which structures form from the bottom up, with smaller objects forming first, while the largest objects, such as superclusters, are still assembling.<ref name=Hess2013>{{cite journal | title=Simulating structure formation of the Local Universe | last1=Heß | first1=Steffen | last2=Kitaura | first2=Francisco-Shu | last3=Gottlöber | first3=Stefan | journal=Monthly Notices of the Royal Astronomical Society | volume=435 | issue=3 | pages=2065–2076 | date=November 2013 | doi=10.1093/mnras/stt1428 | doi-access=free | bibcode=2013MNRAS.435.2065H | arxiv=1304.6565 | s2cid=119198359 }}</ref> One way to study structure in the universe is to survey the visible galaxies, in order to construct a three-dimensional picture of the galaxies in the universe and measure the matter [[power spectrum]]. This is the approach of the ''[[Sloan Digital Sky Survey]]'' and the [[2dF Galaxy Redshift Survey]].<ref name=Cole2005>{{cite journal | title=The 2dF Galaxy Redshift Survey: power-spectrum analysis of the final data set and cosmological implications | display-authors=6 | last1=Cole | first1=Shaun | last2=Percival | first2=Will J. | last3=Peacock | first3=John A. | last4=Norberg | first4=Peder | last5=Baugh | first5=Carlton M. | last6=Frenk | first6=Carlos S. | last7=Baldry | first7=Ivan | last8=Bland-Hawthorn | first8=Joss | last9=Bridges | first9=Terry | last10=Cannon | first10=Russell | last11=Colless | first11=Matthew | last12=Collins | first12=Chris | last13=Couch | first13=Warrick | last14=Cross | first14=Nicholas J. G. | last15=Dalton | first15=Gavin | last16=Eke | first16=Vincent R. | last17=De Propris | first17=Roberto | last18=Driver | first18=Simon P. | last19=Efstathiou | first19=George | last20=Ellis | first20=Richard S. | last21=Glazebrook | first21=Karl | last22=Jackson | first22=Carole | last23=Jenkins | first23=Adrian | last24=Lahav | first24=Ofer | last25=Lewis | first25=Ian | last26=Lumsden | first26=Stuart | last27=Maddox | first27=Steve | last28=Madgwick | first28=Darren | last29=Peterson | first29=Bruce A. | last30=Sutherland | first30=Will | last31=Taylor | first31=Keith | journal=Monthly Notices of the Royal Astronomical Society | volume=362 | issue=2 | pages=505–534 | year=2005 | doi=10.1111/j.1365-2966.2005.09318.x | doi-access=free | bibcode=2005MNRAS.362..505C | arxiv=astro-ph/0501174 | s2cid=6906627 }}</ref><ref name=Nichol2007>{{cite journal | title=The Shape of the Sloan Digital Sky Survey Data Release 5 Galaxy Power Spectrum | display-authors=1 | last1=Percival | first1=Will J. | last2=Nichol | first2=Robert C. | last3=Eisenstein | first3=Daniel J. | last4=Frieman | first4=Joshua A. | last5=Fukugita | first5=Masataka | last6=Loveday | first6=Jon | last7=Pope | first7=Adrian C. | last8=Schneider | first8=Donald P. | last9=Szalay | first9=Alex S. | last10=Tegmark | first10=Max | last11=Vogeley | first11=Michael S. | last12=Weinberg | first12=David H. | last13=Zehavi | first13=Idit | last14=Bahcall | first14=Neta A. | last15=Brinkmann | first15=Jon | last16=Connolly | first16=Andrew J. | last17=Meiksin | first17=Avery | journal=The Astrophysical Journal | volume=657 | issue=2 | pages=645–663 | year=2007 | doi=10.1086/510615 | bibcode=2007ApJ...657..645P | arxiv=astro-ph/0608636 | s2cid=53141475 }}</ref>
 Another tool for understanding structure formation is simulations, which cosmologists use to study the gravitational aggregation of matter in the universe, as it clusters into [[Galaxy filament|filaments]], superclusters and [[void (astronomy)|voids]]. Most simulations contain only non-baryonic [[cold dark matter]], which should suffice to understand the universe on the largest scales, as there is much more dark matter in the universe than visible, baryonic matter. More advanced simulations are starting to include baryons and study the formation of individual galaxies. Cosmologists study these simulations to see if they agree with the galaxy surveys, and to understand any discrepancy.<ref name=Kuhlen2012>{{cite journal | title=Numerical simulations of the dark universe: State of the art and the next decade | journal=Physics of the Dark Universe | volume=1 | issue=1–2 | date=November 2012 | pages=50–93 | first1=Michael | last1=Kuhlen | first2=Mark | last2=Vogelsberger | first3=Raul | last3=Angulo | doi=10.1016/j.dark.2012.10.002 | arxiv=1209.5745 | bibcode=2012PDU.....1...50K | s2cid=119232040 }}</ref>
+[[File:Gravitational lens found in the DESI Legacy Surveys data (noirlab2104c).jpg|thumb|upright=1.2|An example of a gravitational lens found in the DESI Legacy Surveys data. There are four sets of lensed images in DESI-090.9854-35.9683, corresponding to four distinct background galaxies—from the outermost giant red arc to the innermost bright blue arc, arranged in four concentric circles. All of them are gravitationally warped—or lensed—by the orange galaxy at the very center. Dark matter is expected to produce gravitational lensing also.]]
 Other, complementary observations to measure the distribution of matter in the distant universe and to probe [[reionization]] include:
 * The [[Lyman-alpha forest]], which allows cosmologists to measure the distribution of neutral atomic hydrogen gas in the early universe, by measuring the absorption of light from distant quasars by the gas.<ref name=Weinberg2003>{{Cite book | last1=Weinberg | first1=David H. | last2=Davé | first2=Romeel | last3=Katz | first3=Neal | last4=Kollmeier | first4=Juna A. | chapter=The Lyman-α Forest as a Cosmological Tool | title=AIP Conference Proceedings: The Emergence of Cosmic Structure | date=May 2003 | series=AIP Conference Series | volume=666 | issue=2003 | editor1-first=S.H. | editor1-last=Holt | editor2-first=C. S. | editor2-last=Reynolds | pages=157–169 | arxiv=astro-ph/0301186 | doi=10.1063/1.1581786 | bibcode=2003AIPC..666..157W | citeseerx=10.1.1.256.1928 | s2cid=118868536 }}</ref>
@@ Line 147: / Line 131: @@
 If the universe is [[Flatness (cosmology)|flat]], there must be an additional component making up 73% (in addition to the 23% dark matter and 4% baryons) of the energy density of the universe. This is called dark energy. In order not to interfere with Big Bang nucleosynthesis and the cosmic microwave background, it must not cluster in haloes like baryons and dark matter. There is strong observational evidence for dark energy, as the total energy density of the universe is known through constraints on the flatness of the universe, but the amount of clustering matter is tightly measured, and is much less than this. The case for dark energy was strengthened in 1999, when measurements demonstrated that the expansion of the universe has begun to gradually accelerate.<ref name=Perlmutter1999>{{cite journal | title=Constraining Dark Energy with Type Ia Supernovae and Large-Scale Structure | last1=Perlmutter | first1=Saul | last2=Turner | first2=Michael S. | last3=White | first3=Martin | journal=Physical Review Letters | volume=83 | issue=4 | year=1999 | pages=670–673 | doi=10.1103/PhysRevLett.83.670 | bibcode=1999PhRvL..83..670P | arxiv=astro-ph/9901052 | s2cid=119427069 | url=https://zenodo.org/record/1233929 }}</ref>
-Apart from its density and its clustering properties, nothing is known about dark energy. ''[[Quantum field theory]]'' predicts a cosmological constant (CC) much like dark energy, but 120 [[orders of magnitude]] larger than that observed.<ref name=Adler1995>{{cite journal | title=Vacuum catastrophe: An elementary exposition of the cosmological constant problem | last1=Adler | first1=Ronald J. | last2=Casey | first2=Brendan | last3=Jacob | first3=Ovid C. | journal=American Journal of Physics | volume=63 | issue=7 | pages=620–626 | date=July 1995 | doi=10.1119/1.17850 | bibcode=1995AmJPh..63..620A | doi-access=free }}</ref> [[Steven Weinberg]] and a number of string theorists ''(see [[string landscape]])'' have invoked the 'weak [[anthropic principle]]': i.e. the reason that physicists observe a universe with such a small cosmological constant is that no physicists (or any life) could exist in a universe with a larger cosmological constant. Many cosmologists find this an unsatisfying explanation: perhaps because while the weak anthropic principle is self-evident (given that living observers exist, there must be at least one universe with a cosmological constant which allows for life to exist) it does not attempt to explain the context of that universe.<ref name=Siegfried2006>{{cite journal | title=A 'Landscape' Too Far? | first1=Tom | last1=Siegfried | journal=Science | date=11 August 2006 | volume=313 | issue=5788 | pages=750–753 | doi=10.1126/science.313.5788.750 | pmid=16902104 | s2cid=118891996 }}</ref> For example, the weak anthropic principle alone does not distinguish between:
+Apart from its density and its clustering properties, nothing is known about dark energy. ''[[Quantum field theory]]'' predicts a cosmological constant (CC) much like dark energy, but 120 [[orders of magnitude]] larger than that observed.<ref name=Adler1995>{{cite journal | title=Vacuum catastrophe: An elementary exposition of the cosmological constant problem | last1=Adler | first1=Ronald J. | last2=Casey | first2=Brendan | last3=Jacob | first3=Ovid C. | journal=American Journal of Physics | volume=63 | issue=7 | pages=620–626 | date=July 1995 | doi=10.1119/1.17850 | bibcode=1995AmJPh..63..620A | doi-access=free }}</ref> [[Steven Weinberg]] and a number of string theorists ''(see [[string landscape]])'' have invoked the 'weak [[anthropic principle]]': i.e. the reason that physicists observe a universe with such a small cosmological constant is that no physicists (or any life) could exist in a universe with a larger cosmological constant. Many cosmologists find this an unsatisfying explanation: perhaps because while the weak anthropic principle is self-evident (given that living observers exist, there must be at least one universe with a cosmological constant (CC) which allows for life to exist) it does not attempt to explain the context of that universe.<ref name=Siegfried2006>{{cite journal | title=A 'Landscape' Too Far? | first1=Tom | last1=Siegfried | journal=Science | date=11 August 2006 | volume=313 | issue=5788 | pages=750–753 | doi=10.1126/science.313.5788.750 | pmid=16902104 | s2cid=118891996 }}</ref> For example, the weak anthropic principle alone does not distinguish between:
 * Only one universe will ever exist and there is some underlying principle that constrains the CC to the value we observe.
 * Only one universe will ever exist and although there is no underlying principle fixing the CC, we got lucky.
@@ Line 157: / Line 141: @@
 ===Gravitational waves===
-[[Gravitational wave]]s  are ripples in the [[curvature]] of [[spacetime]] that propagate as [[wave]]s at the speed of light, generated in certain gravitational interactions that propagate outward from their source. [[Gravitational-wave astronomy]] is an emerging branch of [[observational astronomy]] which aims to use gravitational waves to collect observational data about sources of detectable gravitational waves such as [[binary star]] systems composed of [[white dwarf]]s, [[neutron star]]s, and [[black hole]]s; and events such as [[supernova]]e, and the formation of the [[chronology of the universe|early universe]] shortly after the Big Bang.<ref name=Colpi2017>{{cite book | chapter=Gravitational Wave Sources in the Era of Multi-Band Gravitational Wave Astronomy | last1=Colpi | first1=Monica | last2=Sesana | first2=Alberto | title=An Overview of Gravitational Waves: Theory, Sources and Detection | editor1-first=Augar | editor1-last=Gerard | editor2-first=Plagnol | editor2-last=Eric | isbn=978-981-314-176-6 | pages=43–140 | year=2017 | doi=10.1142/9789813141766_0002 | bibcode=2017ogw..book...43C | arxiv=1610.05309 | s2cid=119292265 }}</ref>
+[[Gravitational wave]]s are ripples in the [[curvature]] of [[spacetime]] that propagate as [[wave]]s at the speed of light, generated in certain gravitational interactions that propagate outward from their source. [[Gravitational-wave astronomy]] is an emerging branch of [[observational astronomy]] which aims to use gravitational waves to collect observational data about sources of detectable gravitational waves such as [[binary star]] systems composed of [[white dwarf]]s, [[neutron star]]s, and [[black hole]]s; and events such as [[supernova]]e, and the formation of the [[chronology of the universe|early universe]] shortly after the Big Bang.<ref name=Colpi2017>{{cite book | chapter=Gravitational Wave Sources in the Era of Multi-Band Gravitational Wave Astronomy | last1=Colpi | first1=Monica | last2=Sesana | first2=Alberto | title=An Overview of Gravitational Waves: Theory, Sources and Detection | editor1-first=Augar | editor1-last=Gerard | editor2-first=Plagnol | editor2-last=Eric | isbn=978-981-314-176-6 | pages=43–140 | year=2017 | doi=10.1142/9789813141766_0002 | bibcode=2017ogw..book...43C | arxiv=1610.05309 | s2cid=119292265 }}</ref>
-In 2016, the [[LIGO]] Scientific Collaboration and [[Virgo interferometer|Virgo]] Collaboration teams announced that they had made the [[first observation of gravitational waves]], originating from a [[Binary black hole|pair]] of [[Stellar collision|merging]] black holes using the Advanced LIGO detectors.<ref name="Discovery 2016">{{cite journal |title=Einstein's gravitational waves found at last |journal=Nature News| url=http://www.nature.com/news/einstein-s-gravitational-waves-found-at-last-1.19361 |date=11 February 2016 |last1=Castelvecchi |first1=Davide |last2=Witze |first2=Witze |doi=10.1038/nature.2016.19361  |s2cid=182916902|access-date=2016-02-11 }}</ref><ref name='Abbot'>{{cite journal |title=Observation of Gravitational Waves from a Binary Black Hole Merger| author=B. P. Abbott |collaboration=LIGO Scientific Collaboration and Virgo Collaboration | journal=Physical Review Letters| year=2016| volume=116|issue=6| pages=061102| doi=10.1103/PhysRevLett.116.061102| pmid=26918975| bibcode=2016PhRvL.116f1102A|arxiv = 1602.03837 | s2cid=124959784|display-authors=etal}}</ref><ref name='NSF'>{{cite web|title = Gravitational waves detected 100 years after Einstein's prediction |publisher=National Science Foundation|url = https://www.nsf.gov/news/news_summ.jsp?cntn_id=137628|website = www.nsf.gov|access-date = 11 February 2016}}</ref> On 15 June 2016, a [[GW151226|second detection]] of gravitational waves from coalescing black holes was announced.<ref name="NYT-20160615">{{cite news |last=Overbye |first=Dennis |author-link=Dennis Overbye |title=Scientists Hear a Second Chirp From Colliding Black Holes |url=https://www.nytimes.com/2016/06/16/science/ligo-gravitational-waves-einstein.html |archive-url=https://ghostarchive.org/archive/20220101/https://www.nytimes.com/2016/06/16/science/ligo-gravitational-waves-einstein.html |archive-date=2022-01-01 |url-access=limited |date=15 June 2016 |work=[[The New York Times]] |access-date=15 June 2016 }}{{cbignore}}</ref> Besides LIGO, many other [[Gravitational-wave observatory|gravitational-wave observatories (detectors)]] are under construction.<ref>{{cite web|title=The Newest Search for Gravitational Waves has Begun|url=https://ligo.caltech.edu/news/ligo20150918|website=LIGO Caltech|publisher=[[LIGO]]|access-date=29 November 2015|date=18 September 2015}}</ref>
+In 2016, the [[LIGO]] Scientific Collaboration and [[Virgo interferometer|Virgo]] Collaboration teams announced that they had made the [[first observation of gravitational waves]], originating from a [[Binary black hole|pair]] of [[Stellar collision|merging]] black holes using the Advanced LIGO detectors.<ref name="Discovery 2016">{{cite journal |title=Einstein's gravitational waves found at last |journal=Nature News| url=http://www.nature.com/news/einstein-s-gravitational-waves-found-at-last-1.19361 |date=11 February 2016 |last1=Castelvecchi |first1=Davide |last2=Witze |first2=Witze |doi=10.1038/nature.2016.19361  |s2cid=182916902|access-date=2016-02-11 }}</ref><ref name="Abbot">{{cite journal |author=Abbott |first=B. P. |display-authors=etal |year=2016 |title=Observation of Gravitational Waves from a Binary Black Hole Merger |journal=Physical Review Letters |volume=116 |issue=6 |pages=061102 |arxiv=1602.03837 |bibcode=2016PhRvL.116f1102A |doi=10.1103/PhysRevLett.116.061102 |pmid=26918975 |s2cid=124959784 |collaboration=LIGO Scientific Collaboration and Virgo Collaboration}}</ref><ref name='NSF'>{{cite web|title = Gravitational waves detected 100 years after Einstein's prediction |publisher=National Science Foundation|url = https://www.nsf.gov/news/news_summ.jsp?cntn_id=137628|website = www.nsf.gov|access-date = 11 February 2016}}</ref> On 15 June 2016, a [[GW151226|second detection]] of gravitational waves from coalescing black holes was announced.<ref name="NYT-20160615">{{cite news |last=Overbye |first=Dennis |author-link=Dennis Overbye |title=Scientists Hear a Second Chirp From Colliding Black Holes |url=https://www.nytimes.com/2016/06/16/science/ligo-gravitational-waves-einstein.html |archive-url=https://ghostarchive.org/archive/20220101/https://www.nytimes.com/2016/06/16/science/ligo-gravitational-waves-einstein.html |archive-date=2022-01-01 |url-access=limited |date=15 June 2016 |work=[[The New York Times]] |access-date=15 June 2016 }}{{cbignore}}</ref> Besides LIGO, many other [[Gravitational-wave observatory|gravitational-wave observatories (detectors)]] are under construction.<ref>{{cite web|title=The Newest Search for Gravitational Waves has Begun|url=https://ligo.caltech.edu/news/ligo20150918|website=LIGO Caltech|publisher=[[LIGO]]|access-date=29 November 2015|date=18 September 2015}}</ref>
 ===Other areas of inquiry===
@@ Line 165: / Line 149: @@
 * Whether [[primordial black hole]]s were formed in our universe, and what happened to them.<ref name=Kovetz2017>{{cite journal | title=Probing Primordial Black Hole Dark Matter with Gravitational Waves | last1=Kovetz | first1=Ely D. | journal=Physical Review Letters | volume=119 | issue=13 | page=131301 | year=2017 | doi=10.1103/PhysRevLett.119.131301 | pmid=29341709 | bibcode=2017PhRvL.119m1301K | arxiv=1705.09182 | s2cid=37823911 }}</ref>
 * Detection of cosmic rays with energies above the [[GZK cutoff]],<ref name=Takeda1998>{{cite journal | title=Extension of the Cosmic-Ray Energy Spectrum beyond the Predicted Greisen-Zatsepin-Kuz'min Cutoff | display-authors=1 | last1=Takeda | first1=M. | last2=Hayashida | first2=N. | last3=Honda | first3=K. | last4=Inoue | first4=N. | last5=Kadota | first5=K. | last6=Kakimoto | first6=F. | last7=Kamata | first7=K. | last8=Kawaguchi | first8=S. | last9=Kawasaki | first9=Y. | last10=Kawasumi | first10=N. | last11=Kitamura | first11=H. | last12=Kusano | first12=E. | last13=Matsubara | first13=Y. | last14=Murakami | first14=K. | last15=Nagano | first15=M. | last16=Nishikawa | first16=D. | last17=Ohoka | first17=H. | last18=Sakaki | first18=N. | last19=Sasaki | first19=M. | last20=Shinozaki | first20=K. | last21=Souma | first21=N. | last22=Teshima | first22=M. | last23=Torii | first23=R. | last24=Tsushima | first24=I. | last25=Uchihori | first25=Y. | last26=Yamamoto | first26=T. | last27=Yoshida | first27=S. | last28=Yoshii | first28=H. | journal=Physical Review Letters | volume=81 | issue=6 | date=10 August 1998 | pages=1163–1166 | doi=10.1103/PhysRevLett.81.1163 | bibcode=1998PhRvL..81.1163T | arxiv=astro-ph/9807193 | s2cid=14864921 }}</ref> and whether it signals a failure of [[special relativity]] at high energies.
-* The [[equivalence principle]],<ref name=Boucher2004/> whether or not Einstein's general theory of relativity is the correct theory of [[gravitation]],<ref name=Turyshev2008>{{cite journal | title=Experimental Tests of General Relativity | last1=Turyshev | first1=Slava G. | journal=[[Annual Review of Nuclear and Particle Science]] | volume=58 | issue=1 | pages=207–248 | year=2008 | doi=10.1146/annurev.nucl.58.020807.111839| doi-access=free | bibcode=2008ARNPS..58..207T | arxiv=0806.1731 | s2cid=119199160 }}</ref> and if the fundamental [[laws of physics]] are the same everywhere in the universe.<ref name=Uzan2011>{{cite journal | title=Varying Constants, Gravitation and Cosmology | last1=Uzan | first1=Jean-Philippe | journal=Living Reviews in Relativity | volume=14 | issue=1 | pages=2 | date=March 2011 | doi=10.12942/lrr-2011-2 | pmid=28179829 | pmc=5256069 | bibcode=2011LRR....14....2U | arxiv=1009.5514 }}</ref>
+* The [[equivalence principle]],<ref name=Boucher2004/> whether or not Einstein's general theory of relativity is the correct theory of [[gravitation]],<ref name=Turyshev2008>{{cite journal | title=Experimental Tests of General Relativity | last1=Turyshev | first1=Slava G. | journal=[[Annual Review of Nuclear and Particle Science]] | volume=58 | issue=1 | pages=207–248 | year=2008 | doi=10.1146/annurev.nucl.58.020807.111839| doi-access=free | bibcode=2008ARNPS..58..207T | arxiv=0806.1731 | s2cid=119199160 }}</ref> and if the fundamental [[laws of physics]] are the same everywhere in the universe.<ref name=Uzan2011>{{cite journal | title=Varying Constants, Gravitation and Cosmology | last1=Uzan | first1=Jean-Philippe | journal=Living Reviews in Relativity | volume=14 | issue=1 | pages=2 | date=March 2011 | doi=10.12942/lrr-2011-2 | doi-access=free | pmid=28179829 | pmc=5256069 | bibcode=2011LRR....14....2U | arxiv=1009.5514 }}</ref>
+*{{anchor|Biophysical cosmology}}'''Biophysical cosmology''': a type of physical cosmology that studies and understands [[life]] as part or an inherent part of physical cosmology. It stresses that [[Universe#Habitability|life is inherent to the universe]] and therefore [[Life#In the universe|frequent]].<ref name="v237">{{cite book | last=Dick | first=Steven J. | title=Space, Time, and Aliens | chapter=The Biophysical Cosmology: The Place of Bioastronomy in the History of Science | publisher=Springer International Publishing | publication-place=Cham | date=2020 | isbn=978-3-030-41613-3 | doi=10.1007/978-3-030-41614-0_4 | pages=53–58}}</ref>
 ==See also==
@@ Line 219: / Line 204: @@
 * [http://www.damtp.cam.ac.uk/user/gr/public/cos_home.html Cambridge Cosmology] – from Cambridge University (public home page)
 * [http://map.gsfc.nasa.gov/m_uni.html Cosmology 101] – from the NASA [[WMAP]] group
-* [http://cfcp.uchicago.edu/ Center for Cosmological Physics]. [[University of Chicago]], Chicago.
+* [http://cfcp.uchicago.edu/ Center for Cosmological Physics]. [[University of Chicago]], Chicago, Illinois
-* [https://www.pbs.org/wgbh/nova/origins/ Origins, Nova Online] – Provided by ''[[Public Broadcasting Service|PBS]]''.
+* [https://www.pbs.org/wgbh/nova/origins/ Origins, Nova Online] – Provided by ''[[Public Broadcasting Service|PBS]]''
 ===From individuals===
 * Gale, George, "[http://plato.stanford.edu/entries/cosmology-30s/ Cosmology: Methodological Debates in the 1930s and 1940s]", ''The Stanford Encyclopedia of Philosophy'', Edward N. Zalta (ed.)
 * Madore, Barry F., "''[http://nedwww.ipac.caltech.edu/level5/ Level 5] : A Knowledgebase for Extragalactic Astronomy and Cosmology''". Caltech and Carnegie. Pasadena, California.
-* Tyler, Pat, and Phil Newman "''[http://universe.gsfc.nasa.gov/ Beyond Einstein]''". Laboratory for High Energy Astrophysics (LHEA) NASA [[Goddard Space Flight Center]].
+* Tyler, Pat, and Newman, Phil, "''[http://universe.gsfc.nasa.gov/ Beyond Einstein]''". Laboratory for High Energy Astrophysics (LHEA) NASA [[Goddard Space Flight Center]].
 * [[Edward L. Wright|Wright, Ned]]. "''[http://www.astro.ucla.edu/~wright/cosmolog.htm Cosmology tutorial and FAQ]''". Division of Astronomy & Astrophysics, UCLA.
-* {{cite news | author=George Musser | author-link=George Musser | title=Four Keys to Cosmology
+* {{cite news |author=Musser |first=George |author-link=George Musser |title=Four Keys to Cosmology |url=http://www.scientificamerican.com/article/four-keys-to-cosmology/ |work=Scientific American |date=February 2004 |access-date=22 March 2015}}
+* {{cite news |author=Burgess |first1=Cliff |author-link=Cliff Burgess |last2=Quevedo |first2=Fernando |author-link2=Fernando Quevedo |title=The Great Cosmic Roller-Coaster Ride |type=print |work=[[Scientific American]] |pages=52–59 |date=November 2007 |quote=(subtitle) Could cosmic inflation be a sign that our universe is embedded in a far vaster realm?}}
-| url=http://www.scientificamerican.com/article/four-keys-to-cosmology/ | work=Scientific American
-| date=February 2004 | access-date=22 March 2015 }}
-* {{cite news | author=Cliff Burgess | author-link=Cliff Burgess | author2=Fernando Quevedo | author-link2=Fernando Quevedo | title=The Great Cosmic Roller-Coaster Ride
-| type=print | work=[[Scientific American]] | pages=52–59 | date=November 2007 | quote=(subtitle) Could cosmic inflation be a sign that our universe is embedded in a far vaster realm? }}
 {{Cosmology topics|state=uncollapsed}}

v t e Cosmology
Background	Age of the universe Big Bang Chronology of the universe Universe Observable universe
History of cosmological theories	Discovery of cosmic microwave background History of the Big Bang theory Religious interpretations of the Big Bang Timeline of cosmological theories
Past universe	Cosmic microwave background Cosmic neutrino background Gravitational wave background Inflation Nucleosynthesis
Present universe	FLRW metric Friedmann equations Hubble's law Expansion of the universe Accelerating expansion Redshift
Future universe	Future of an expanding universe Ultimate fate of the universe
Components	Dark energy Dark fluid Dark matter Quintessence Lambda-CDM model
Structure formation	Galaxy filament Galaxy formation Large quasar group Large-scale structure Reionization Shape of the universe Structure formation
Experiments	2dF 6dF BOOMERanG COBE Illustris project Observational cosmology Planck SDSS WMAP
astronomy portal

v t e Big History
Themes and subjects	Chronology of the universe Cosmic evolution Deep time Time scales Goldilocks principle Modernity
Eight thresholds	1: Creation - Big Bang and cosmogony 2: Stars - creation of stars 3: Elements - creation of chemical elements inside dying stars 4: Planets - formation of planets 5: Life - abiogenesis and evolution of life 6: Humans - development of Homo sapiens Stone Age 7: Agriculture - Agricultural Revolution 8: Modernity - modern era
Web-based education	Big History Project ChronoZoom
Notable people	Walter Alvarez Cynthia Stokes Brown Eric Chaisson David Christian Carl Sagan Fred Spier Graeme Snooks
Related	Big History (2013 series)