what is the inflation theory?

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. The spectral index, ns is one for a scale-invariant Harrison–Zel'dovich spectrum. It also predicts that the total curvature of a space-slice at constant global time is zero. The rapid expansion immediately after the Big Bounce explains why the present Universe at largest scales appears spatially flat, homogeneous and isotropic. The simplest inflation models, those without fine-tuning, predict a tensor to scalar ratio near 0.1. It was very quickly realized that such an expansion would resolve many other long-standing problems. 1. In such models, most of the volume of the Universe is continuously inflating at any given time. [52] At the same time, Starobinsky argued that quantum corrections to gravity would replace the initial singularity of the Universe with an exponentially expanding de Sitter phase. Following the inflationary period, the universe continued to expand, but at a slower rate. In 1978, Zeldovich noted the monopole problem, which was an unambiguous quantitative version of the horizon problem, this time in a subfield of particle physics, which led to several speculative attempts to resolve it. N ... Guth himself did not refer to work of Kazanas until he published a book on the subject under the title "The inflationary universe: the quest for a new theory of cosmic origin" (1997), where he apologizes for not having referenced the work of Kazanas and of others, related to inflation.[58]. [3] Many physicists also believe that inflation explains why the universe appears to be the same in all directions (isotropic), why the cosmic microwave background radiation is distributed evenly, why the universe is flat, and why no magnetic monopoles have been observed. In this model, instead of tunneling out of a false vacuum state, inflation occurred by a scalar field rolling down a potential energy hill. This is a problem with Grand Unified Theories, which propose that at high temperatures (such as in the early universe) the electromagnetic force, strong, and weak nuclear forces are not actually fundamental forces but arise due to spontaneous symmetry breaking from a single gauge theory. In any one causal patch it is likely that only one bubble would nucleate. [74][72][75][76] This is the range that is possible without fine-tuning of the parameters related to energy. Inflation will occur in virtually any universe that begins in a chaotic, high energy state that has a scalar field with unbounded potential energy. Unless the rate of decay to the non-inflating phase is sufficiently fast, new inflating regions are produced more rapidly than non-inflating regions. For Hubble, the expansion was constant, so the symmetry that existed was quite high. Later, Willem de Sitter found a highly symmetric inflating universe, which described a universe with a cosmological constant that is otherwise empty. Inflation in effective field theory 3. Inflation is typically not an exactly exponential expansion, but rather quasi- or near-exponential. Scientific American, May 1984. And if we ask ourselves what drove this hot and dense mixture of energy and matter, the answer is simple, the dark energy, that mysterious energy was what drove the expansion that caused the cooling of the universe and then gave rise to the process of generating matter and the unknown warp of space and time. [95] However, in his model the inflaton field necessarily takes values larger than one Planck unit: for this reason, these are often called large field models and the competing new inflation models are called small field models. Vilenkin put forth one such scenario. The theory of the inflationary universe was elaborated in 1981 by the American physicist Alan Guth of the Massachusetts Institute of Technology. [143], Since its introduction by Alan Guth in 1980, the inflationary paradigm has become widely accepted. The natural scale is naïvely the Planck scale so this small value could be seen as another form of fine-tuning (called a hierarchy problem): the energy density given by the scalar potential is down by 10−12 compared to the Planck density. At that time the universe doubled in size up to 90 times. During inflation, the energy density in the inflaton field is roughly constant. The basic inflationary paradigm is accepted by most physicists, as a number of inflation model predictions have been confirmed by observation;[4] however, a substantial minority of scientists dissent from this position. However, explanations for these fine-tunings have been proposed. Other models explain some of the observations explained by inflation. In the early Universe, it was not possible to send a light signal between the two regions. The process of tunneling between two vacua is a form of old inflation, but new inflation must then occur by some other mechanism. Comparizon with QSO observational data", "Stars and black holes in varying speed of light theories", "String Gas Cosmology and Structure Formation". This theory tells us that the universe is flat and that this can be proved experimentally because the density of matter in a flat universe is closely related to the rate of expansion. {\displaystyle r} It is said that this moment, the shape or geometry of the universe will be very smooth, in contrast to the current shape. Alan H. Guth & Paul J.Steinhardt, "The Inflationary Universe", The theory of inflation thus explains why the temperatures and curvatures of different regions are so nearly equal. [51] It is now believed by some that the inflaton cannot be the Higgs field[90] although the recent discovery of the Higgs boson has increased the number of works considering the Higgs field as inflaton. What is the Inflation Theory? Since Guth's early work, each of these observations has received further confirmation, most impressively by the detailed observations of the cosmic microwave background made by the Planck spacecraft. [47] It was discovered that Einstein's universe is unstable, and that small fluctuations cause it to collapse or turn into a de Sitter universe. One is the amplitude of the spectrum and the spectral index, which measures the slight deviation from scale invariance predicted by inflation (perfect scale invariance corresponds to the idealized de Sitter universe). This results in the observables: Linde proposed a theory known as chaotic inflation in which he suggested that the conditions for inflation were actually satisfied quite generically. Paul Steinhardt, one of the original architects of the inflationary model, introduced the first example of eternal inflation in 1983. In eternal inflation, regions with inflation have an exponentially growing volume, while regions that are not inflating don't. If Earth is not in some special, privileged, central position in the universe, then it would mean all galaxies are moving apart, and the further away, the faster they are moving away. [27] Inflation was first proposed by Alan Guth in 1979 while investigating the problem of why no magnetic monopoles are seen today; he found that a positive-energy false vacuum would, according to general relativity, generate an exponential expansion of space. These problems arise from the observation that to look like it does today, the Universe would have to have started from very finely tuned, or "special" initial conditions at the Big Bang. Whether the correct spectrum of density fluctuations can be produced, and whether the Universe can successfully navigate the Big Bang/Big Crunch transition, remains a topic of controversy and current research. An expanding universe generally has a cosmological horizon, which, by analogy with the more familiar horizon caused by the curvature of Earth's surface, marks the boundary of the part of the Universe that an observer can see. However, for many years it was not clear why or how the universe might be expanding, or what it might signify. As the very early universe cooled it was trapped in a metastable state (it was supercooled), which it could only decay out of through the process of bubble nucleation via quantum tunneling. Other proposals attempt to describe the ex nihilo creation of the Universe based on quantum cosmology and the following inflation. [123] Brane inflation suggests that inflation arises from the motion of D-branes[124] in the compactified geometry, usually towards a stack of anti-D-branes. Therefore, the most likely number of non-compact (large) spatial dimensions is three. This raised the contingent question of why four space-time dimensions became large and the rest became unobservably small. Light (or other radiation) emitted by objects beyond the cosmological horizon in an accelerating universe never reaches the observer, because the space in between the observer and the object is expanding too rapidly. This scale is suggested to be around 1016 GeV or 10−3 times the Planck energy. The detailed form of the spectrum of perturbations, called a nearly-scale-invariant Gaussian random field is very specific and has only two free parameters. [39][40] Monopoles are predicted to be copiously produced following Grand Unified Theories at high temperature,[41][42] and they should have persisted to the present day, to such an extent that they would become the primary constituent of the Universe.

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