The Big Bang Theory The very early universe All our understanding of the very early universe (cosmogony) is speculative. No accelerator experiments currently probe sufficiently high energies to provide insight into this period. Scenarios differ radically. Some ideas include the Hartle-Hawking initial state, string landscape, brane inflation, string gas cosmology, and the ekpyrotic universe. Some of these ideas are mutually compatible, others are not. The Planck epoch Up to 10-43 seconds after the Big Bang If supersymmetry is correct, then at this time the four fundamental forces – electromagnetism, weak nuclear force, strong nuclear force and gravity – all have the same strength, so they are possibly unified into one fundamental force. Little is known about this epoch, although different theories make different predictions. Einstein's theory of general relativity predicts a gravitational singularity before this time, but under these conditions the theory is expected to break down due to quantum effects. Physicists hope that proposed theories of quantum gravity, such as string theory and loop quantum gravity, will eventually lead to a better understanding of that epoch. The Grand unification epoch Between 10-43 seconds and 10-35 seconds after the Big Bang As the universe expands and cools from the Planck epoch, gravity begins to separate from the fundamental gauge interactions: electromagnetism and the strong and weak nuclear forces. Physics at this scale may be described by a grand unified theory in which the gauge group of the Standard Model is embedded in a much larger group, which is broken to produce the observed forces of nature. Eventually, the grand unification is broken as the strong nuclear force separates from the electroweak force. This should produce magnetic monopoles. The inflationary epoch Between 10-35seconds and 10-32seconds after the Big Bang The temperature, and therefore the time, at which cosmic inflation occurs is not known for certain. During inflation, the universe is flattened and the universe enters a homogeneous and isotropic rapidly expanding phase in which the seeds of structure formation are laid down in the form of a primordial spectrum of nearly-scale-invariant fluctuations. Some energy from photons becomes virtual quarks and hyperons, but these particles decay quickly. One scenario suggests that prior to cosmic inflation, the universe was cold and empty, and the immense heat and energy associated with the early stages of the big bang was created through the phase change associated with the end of inflation. Reheating During reheating, the exponential expansion that occurred during inflation ceases and the potential energy of the inflaton field decays into a hot, relativistic plasma of particles. If grand unification is a feature of our universe, then cosmic inflation must occur during or after the grand unification symmetry is B.Yu Document1 Feb. 9, 16 Page 1 of 6 broken, otherwise magnetic monopoles would be seen in the visible universe. At this point, the universe is dominated by radiation; quarks, electrons and neutrinos form. Baryogenesis No known physics can explain the fact that there are so many more baryons in the universe than antibaryons. In order for this to be explained, the Sakharov conditions must be met at some time after inflation. There are hints that this is possible in known physics and from studying grand unified theories, but the full picture is not known. The early universe After cosmic inflation ends, the universe is filled with a quark-gluon plasma. From this point onwards the physics of the early universe is better understood, and less speculative. The electroweak epoch Between 10-32 seconds and 10-12 seconds after the Big Bang The temperature of the universe is high enough to merge electromagnetism and the weak interaction into a single electroweak interaction. Particle interactions are energetic enough to create large numbers of exotic particles, including W and Z bosons and Higgs bosons. Supersymmetry breaking If supersymmetry is a property of our universe, then it must be broken at an energy as low as 1 TeV, the electroweak symmetry scale. The masses of particles and their superpartners would then no longer be equal, which could explain why no superpartners of known particles have ever been observed. The quark epoch Between 10-12 seconds and 10-6 seconds after the Big Bang In electroweak symmetry breaking, at the end of the electroweak epoch, all the fundamental particles are believed to acquire a mass via the Higgs mechanism in which the Higgs boson acquires a vacuum expectation value. The fundamental interactions of gravitation, electromagnetism, the strong interaction and the weak interaction have now taken their present forms, but the temperature of the universe is still too high to allow quarks to bind together to form hadrons. The hadron epoch Between 10-6 seconds and 1 second after the Big Bang The quark-gluon plasma which composes the universe cools until hadrons, including baryons such as protons and neutrons, can form. At approximately 1 second after the Big Bang neutrinos decouple and begin travelling freely through space. This cosmic neutrino background, while unlikely to ever be observed in detail, is analogous to the cosmic microwave background that was emitted much later. The lepton epoch B.Yu Document1 Between 1 second and 3 seconds after the Big Bang Feb. 9, 16 Page 2 of 6 The majority of hadrons and anti-hadrons annihilate each other at the end of the hadron epoch, leaving leptons and anti-leptons dominating the mass of the universe. Approximately 3 seconds after the Big Bang the temperature of the universe falls to the point where new lepton/anti-lepton pairs are no longer created and most leptons and anti-leptons are eliminated in annihilation reactions, leaving a small residue of leptons. The photon epoch Between 3 seconds and 380,000 years after the Big Bang After most leptons and anti-leptons are annihilated at the end of the lepton epoch the energy of the universe is dominated by photons. These photons are still interacting frequently with charged protons, electrons and (eventually) nuclei, and continue to do so for the next 300,000 years. Nucleosynthesis Between 100 seconds and 300 seconds after the Big Bang During the photon epoch the temperature of the universe falls to the point where atomic nuclei can begin to form. Protons (hydrogen ions) and neutrons begin to combine into atomic nuclei in the process of nuclear fusion. However, nucleosynthesis only lasts for about three minutes, after which time the temperature and density of the universe has fallen to the point where nuclear fusion cannot continue. At this time, there are about three times more hydrogen ions than helium-4 nuclei and only trace quantities of other nuclei. Matter domination: 70,000 years At this time, the densities of non-relativistic matter (atomic nuclei) and relativistic radiation (photons) are equal. The Jeans length, which determines the smallest structures that can form (due to competition between gravitational attraction and pressure effects), begins to fall and perturbations, instead of being wiped out by radiation free-streaming, can begin to grow in amplitude. Recombination: 300,000 years Hydrogen and helium atoms begin to form and the density of the universe falls. During recombination decoupling occurs, causing the photons to evolve independently from the matter. Most importantly, this means that the photons that compose the cosmic microwave background are a picture of the universe during this epoch. WMAP data shows the microwave background radiation variations throughout the Universe from our perspective, though the actual variations are much smoother than the diagram suggests Dark ages In this epoch, very few atoms are ionized, so the only radiation emitted is the 21 cm spin line of neutral hydrogen. There is currently an observational effort underway to detect this faint radiation, as it is in principle an even more powerful tool than the cosmic microwave background for studying the early universe. B.Yu Document1 Feb. 9, 16 Page 3 of 6 B.Yu Document1 Feb. 9, 16 Page 4 of 6 Structure formation The Hubble Ultra Deep Fields often showcase galaxies from an ancient era that tell us what the early Stelliferous Age was like. Another Hubble image shows an infant galaxy forming nearby, which means this happened very recently on the cosmological timescale. This is evidence that the Universe is not quite finished with galaxy formation yet. Structure formation in the big bang model proceeds hierarchically, with smaller structures forming before larger ones. The first structures to form are quasars, which are thought to be bright, early active galaxies and population III stars. Before this epoch, the evolution of the universe could be understood through linear cosmological perturbation theory: that is, all structures could be understood as small deviations from a perfect homogeneous universe. This is computationally relatively easy to study. At this point non-linear structures begin to form, and the computational problem becomes much more difficult, involving, for example, N-body simulations with billions of particles. Reionization The first quasars form from gravitational collapse. The intense radiation they emit reionizes the surrounding universe. From this point on, most of the universe is composed of plasma. Formation of stars The first stars, most likely Population III stars, form and start the process of turning the light elements that were formed in the Big Bang (hydrogen, helium and lithium) into heavier elements. Formation of galaxies Large volumes of matter collapse to form a galaxy. Population II stars are formed early on in this process, with Population I stars formed later. Formation of groups, clusters and superclusters Gravitational attraction pulls galaxies towards each other to form groups, clusters and superclusters. Formation of the solar system, 8 billion years B.Yu Document1 Feb. 9, 16 Page 5 of 6 Finally, objects on the scale of our solar system form. Our sun is a late-generation star, incorporating the debris from many generations of earlier stars, and formed roughly 5 billion years ago, or roughly 8 to 9 billion years after the big bang. Today, 13.7 billion years The best current data estimates the age of the universe today as 13.7 billion years since the big bang. Since the expansion of the universe appears to be accelerating, superclusters are likely to be the largest structures that will ever form in the universe. The present accelerated expansion prevents any more inflationary structures entering the horizon and prevents new gravitationally bound structures from forming. B.Yu Document1 Feb. 9, 16 Page 6 of 6