1993
DOI: 10.1103/physrevd.48.1629
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Cosmological theory without singularities

Abstract: A theory of gravitation is constructed in which all homogeneous and isotropic solutions are nonsingular, and in which all curvature invariants are bounded. All solutions for which curvature invariants approach their limiting values approach de Sitter space. The action for this theory is obtained by a higher derivative modification of Einstein's theory. We expect that our model can easily be generalized to solve the singularity problem also for anisotropic cosmologies.

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Cited by 230 publications
(298 citation statements)
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“…From the form of the deformed Hubble rate and scale factor in Eq. (12), it can be seen that the values of the parameter α crucially determine the finite time singularity structure of the theory. Particularly, according to the values of α, if α > 1, we now demonstrate that a Type I [55], or so called Big Rip singularity can occur at t s , since both the Hubble rate and the scale factor diverge at t = t s .…”
Section: The Qualitative Features Of the Deformed Matter Bounce Smentioning
confidence: 99%
“…From the form of the deformed Hubble rate and scale factor in Eq. (12), it can be seen that the values of the parameter α crucially determine the finite time singularity structure of the theory. Particularly, according to the values of α, if α > 1, we now demonstrate that a Type I [55], or so called Big Rip singularity can occur at t s , since both the Hubble rate and the scale factor diverge at t = t s .…”
Section: The Qualitative Features Of the Deformed Matter Bounce Smentioning
confidence: 99%
“…Historically, the first models included a scalar mode in addition to the metric (a tensor) of General Relativity; since these scalar tensor theories are equivalent to ordinary GR with a modified matter content, we do not consider them separately. More complicated theories have been suggested, where terms are added to render the cosmological evolution explicitly singularity-free [35]. Such models, which are appropriate to describe a bouncing phase, can be expressed as…”
Section: Modified Gravitymentioning
confidence: 99%
“…A seemingly viable alternative, which also provides a GR-compatible solution to the singularity problem, relies on a nonsingular bouncing cosmology [35,36], whereby an initially contracting phase connects with the currently expanding one through some minimal scale factor (and hence a vanishing Hubble rate). These models have a history that predates inflationary solutions by many decades, as they were proposed shortly after the first observations of the expansion [26,37] by Tolman [38] and Lemaître [39,40] (see also [41] for a more modern viewpoint concerning Tolman's cyclic approach): at this time, the expansion appeared to imply that Einstein's theory of gravity was doomed to fail, as the scale factor reaches infinitesimally small values, such that the Universe emerges from a primordial singularity.…”
mentioning
confidence: 99%
“…This is the main difference from other schemes that constrain curvature invariants and metric related functions. Indeed, in the unimodular gravity proposal, for instance, the determinant of the metric is non-dynamical and the cosmological constant is shown to be an integration constant [25,26,27]; in the limiting curvature proposal, the value of the curvature invariants are bound from above so to avoid singularities [28,29]. Another, curvature-type principle arises in the context of the field theory of closed strings, where minimal area metrics are proposed to solve the problem of generating all Riemann surfaces [30].…”
Section: Discussion and Outlookmentioning
confidence: 99%