1990
DOI: 10.1103/physrevd.42.1008
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Chaotic inflation as an attractor in initial-condition space

Abstract: We study the evolution of scalar field inhomogeneities in the preinflationary phase of an inflationary universe. We decompose the scalar field configuration in Fourier modes and consider initial conditions in which more than one mode is excited. We find that the long-wavelength modes are stable against perturbations due to short-wavelength excitations and that chaotic inflation results even if at the initial time the short waves contain most of the energy density.

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Cited by 80 publications
(64 citation statements)
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“…Furthermore, the initially large gradient terms also can in turn induce large kinetic energy in the modes. The outcome found in [7,11,13] (see also [9]) for this case is that the universe expansion is noninflationary. On the other hand, for the excited k/a > H modes with smaller amplitudes, their evolution will be oscillatory and once again the universe expansion is noninflationary.…”
Section: A Scalar Fieldmentioning
confidence: 69%
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“…Furthermore, the initially large gradient terms also can in turn induce large kinetic energy in the modes. The outcome found in [7,11,13] (see also [9]) for this case is that the universe expansion is noninflationary. On the other hand, for the excited k/a > H modes with smaller amplitudes, their evolution will be oscillatory and once again the universe expansion is noninflationary.…”
Section: A Scalar Fieldmentioning
confidence: 69%
“…For supercooled inflation, the effect of such interactions has been considered from the perspective of mode mixing for some special cases in [8,9] and through computer simulations of scalar fields in one spatial dimension in [10,11]. Up to the scope of these works, their analysis concludes that nonlinear interactions do not present any additional complications to the initial condition problem.…”
Section: A Scalar Fieldmentioning
confidence: 99%
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“…Consequently, the scalar field would require much more than the available time to relax to thermal equilibrium. This difficulty may not be crucial, however, because true thermal equilibrium is not really necessary: a variety of random configurations give results that are very similar to those of thermal equilibrium (9)(10)(11)(12).…”
Section: The Inflationary Universe Scenariomentioning
confidence: 99%