# Decoupling (cosmology)

Part of a series on :
Physical cosmology :
Big Bang · Universe
Age of the universe
Chronology of the universe :
Early universe
Inflation · Nucleosynthesis
Backgrounds
Gravitational wave (GWB)
Microwave (CMB) · Neutrino (CNB) :
Expansion · Future
Hubble's law · Redshift
Expansion of the universe
FLRW metric · Friedmann equations
Inhomogeneous cosmology
Future of an expanding universe
Ultimate fate of the universe :
Components · Structure
Components
Lambda-CDM model
Dark energy · Dark matter
Structure
Shape of the universe
Galaxy filament · Galaxy formation
Large quasar group
Large-scale structure
Reionization · Structure formation :
Experiments
Black Hole Initiative (BHI)
BOOMERanG
Cosmic Background Explorer (COBE)
Dark Energy Survey
Planck space observatory
Sloan Digital Sky Survey (SDSS)
2dF Galaxy Redshift Survey ("2dF")
Wilkinson Microwave Anisotropy Probe (WMAP) :
Scientists
Aaronson
Alfvén
Alpher
Copernicus
de Sitter
Dicke
Ehlers
Einstein
Ellis
Friedmann
Galileo
Gamow
Guth
Hawking
Hubble
Huygens
Kepler
Lemaître
Mather
Newton
Penrose
Penzias
Rubin
Schmidt
Smoot
Suntzeff
Sunyaev
Tolman
Wilson
Zeldovich
List of cosmologists :
Subject history
Discovery of cosmic microwave background radiation
History of the Big Bang theory
Timeline of cosmological theories :
Category
Astronomy portal :
vte :
In cosmology, decoupling is a period in the development of the universe when different types of particles fall out of thermal equilibrium with each other. This occurs as a result of the expansion of the universe, as their interaction rates decrease (and mean free paths increase) up to this critical point. The two verified instances of decoupling since the Big Bang which are most often discussed are photon decoupling and neutrino decoupling, as these led to the cosmic microwave background and cosmic neutrino background, respectively.
Photon decoupling is closely related to recombination, which occurred about 378,000 years after the Big Bang (at a redshift of z = 1100), when the universe was a hot opaque ("foggy") plasma. During recombination, free electrons became bound to protons (hydrogen nuclei) to form neutral hydrogen atoms. Because direct recombinations to the ground state (lowest energy) of hydrogen are very inefficient, these hydrogen atoms generally form with the electrons in a high energy state, and the electrons quickly transition to their low energy state by emitting photons. Because the neutral hydrogen that formed was transparent to light, those photons which were not captured by other hydrogen atoms were able, for the first time in the history of the universe, to travel long distances. They can still be detected today, although they now appear as radio waves, and form the cosmic microwave background ("CMB"). They reveal crucial clues about how the universe formed.

## Photon decoupling

Photon decoupling occurred during the epoch known as the recombination. During this time, electrons combined with protons to form hydrogen atoms, resulting in a sudden drop in free electron density. Decoupling occurred abruptly when the rate of Compton scattering of photons $\Gamma$ was approximately equal to the rate of expansion of the universe $H$, or alternatively when the mean free path of the photons $\lambda$ was approximately equal to the horizon size of the universe $H^{-1}$. After this photons were able to stream freely, producing the cosmic microwave background as we know it, and the universe became transparent.
The interaction rate of the photons is given by
    $\Gamma ={\frac {c}{\lambda }}=n_{e}\sigma _{t}c$
where $n_{e}$ is the number density of free electrons, $\sigma _{t}$ is the electron Thomson scattering area, and $c$ is the speed of light.
In the matter-dominated era (when recombination takes place),
    $H\approx H_{0}a^{-{3/2}}$
where $a$ is the cosmic scale factor and H₀ is the Hubble constant. $\Gamma$ also decreases as a more complicated function of $a$, at a faster rate than $H$. By working out the precise dependence of $H$ and $\Gamma$ on the scale factor and equating $\Gamma =H$, it is possible to show that photon decoupling occurred approximately 380,000 years after the Big Bang, at a redshift of $z=1100$ when the universe was at a temperature around 3000 K.

## Neutrino decoupling

Another example is the neutrino decoupling which occurred within one second of the Big Bang. Analogous to the decoupling of photons, neutrinos decoupled when the rate of weak interactions between neutrinos and other forms of matter dropped below the rate of expansion of the universe, which produced a cosmic neutrino background of freely streaming neutrinos. An important consequence of neutrino decoupling is that the temperature of this neutrino background is lower than the temperature of the cosmic microwave background, since they were no more heated by the shortly following annihilation of positrons.

## WIMPs: non-relativistic decoupling

Decoupling may also have occurred for the dark matter candidate, WIMPs. These are known as "cold relics", meaning they decoupled after they became non-relativistic (by comparison, photons and neutrinos decoupled while still relativistic and are known as "hot relics"). By calculating the hypothetical time and temperature of decoupling for non-relativistic WIMPs of a particular mass, it is possible to find their density. Comparing this to the measured density parameter of cold dark matter today of 0.222 $\pm$ 0.0026 it is possible to rule out WIMPs of certain masses as reasonable dark matter candidates.