Subject |
has start time |
has definition |
is preceded by |
has density |
has synonym |
is followed by |
has duration |
has temperature |
Big bang crossover effect | 1012 s | The epoch during the radiation era when the universe switched from being radiation-dominated to being matter-dominated. | | | world point | | | |
hadron era | 10-43 s after Big Bang | The Big Bang era during which quantum and general-relativistic effects are expected to modify each other in an unknown way. | Planck era | ρ = 1093 g cm-3 | hadron barrier | lepton era | 10-5 s | |
inflation era | 10-35 s | Big Bang era in which the infant universe went through a brief period of extremely rapid (exponential) expansion, after which it settled back into the more leisurely rate of expansion of the standard model. The period of rapid expansion began and ended when the universe was still much less than a second old, yet it provides a physical explanation for the flatness and horizon puzzles. The inflationary universe model also suggests that the universe is vastly larger than the portion of it that is visible to us. (See exponential expansion.) | | | world point | | | |
lepton era | 10-5 s after Big Bang | The Big Bang era when the temperature had dropped to about 1012 K and when the Universe consisted mainly of leptons and photons. It lasted until the temperature fell below 1010 K. At this stage, the characteristic photon energy fell below the rest mass energy of an electron, and the abundance of electron-positron pairs fell by many orders of magnitude. Only one electron survived for every 108 photons. The universe was subsequently radiation-dominated (substantial numbers of neutrinos were also present, but they did not interact directly with the matter or the radiation). | hadron era | | world point | nucleosynthetic era | 1 s | 1010 K to 1012 K |
matter era | 1012 s | The release of photons from constant collisions with massive particles as the universe expanded and its matter density diminished. See decoupling. | radiation era | | decoupling era | | > 1010 years | 3 K to 3000 K |
nucleosynthetic era | 1 s after the Big Bang | The Big Bang era when neutrons were produced and helium and deuterium were synthesized. At t = 200 sec, nucleosynthesis began rather abruptly and virtually all deuterium was synthesized to helium. | lepton era | | world point | radiation era | 1000 s | |
Planck era | 0 s after Big Bang | The Big Bang era, prior to which Einstein's theory of gravitation breaks down and a quantized theory of gravity is needed. Density was so high that gravitational force acted as strongly as the other fundamental forces on the sub-atomic scale. | Big Bang | | world point | hadron era, inflation era | 10-43 s or the time at which the size of the universe was roughly the Planck length (the time it takes light to travel the Planck length; G h bar / c5)1/2 where G is Newton's constant of gravitation, h bar is Planck's constant, and c is the speed of light | |
radiation era | 10 s after Big Bang | The Big Bang era when the temperature had dropped to 109K and the rate of electron-positron pair annihilation exceeded the rate of their production, leaving radiation the dominant constituent of the universe. | nucleosynthetic era | | world point | matter era | 1012 s | 109K |