The period in the early universe when radiation was the dominant form of energy.The radiation-dominated era was the earliest epoch of the universe, lasting from shortly after the Big Bang until the universe was roughly 50,000 years old. During this period, the energy density of the universe was overwhelmingly carried by radiation — photons and other relativistic particles — rather than by matter (baryons or dark matter) or dark energy. Because radiation density scales as the fourth power of the scale factor (while matter scales as the third), radiation inevitably dominated when the universe was very small and hot. This era set the stage for nucleosynthesis, the formation of the cosmic microwave background, and the eventual matter-dominated epoch that allowed galaxies to form.
The concept emerged from the hot Big Bang model developed in the 1940s by George Gamow and collaborators, and was formalized in the 1960s–70s as the standard cosmological model took shape.
In the early universe, temperatures were so extreme that particles moved at relativistic speeds, and the energy of individual photons was enormous. The total energy budget was therefore dominated by radiation, which also drove the expansion rate: the universe expanded as t^(1/2) during this era, faster than the t^(2/3) of the later matter-dominated era. As the universe expanded, radiation cooled and its energy density dropped faster than that of matter, so eventually matter took over — a transition that occurred at a redshift of about 3400. The physics of this era is governed by the Friedmann equations, with the radiation term dominating the right-hand side.
Understanding the radiation-dominated era is essential for interpreting cosmic microwave background anisotropies and for predicting the relic abundances of light elements like helium and deuterium.
During the radiation-dominated era, the entire observable universe was smaller than the Solar System, yet contained more energy than all the matter in today's galaxies combined.



















