2015
DOI: 10.1103/physrevd.91.083513
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Singular inflation

Abstract: We prove that a homogeneous and isotropic universe containing a scalar field with a power-law potential, V (φ) = Aφ n , with 0 < n < 1 and A > 0 always develops a finite-time singularity at which the Hubble rate and its first derivative are finite, but its second derivative diverges. These are the first examples of cosmological models with realistic matter sources that possess weak singularities of 'sudden' type. We also show that a large class of models with even weaker singularities exist for noninteger n > … Show more

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Cited by 82 publications
(104 citation statements)
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References 50 publications
(52 reference statements)
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“…Exact examples displaying a generalised sudden singularity of the type identified by Barrow and Graham [62] for inflationary scalar fields with fractional potentials were found here. Lastly, the ranges for the values of the free parameters of the models have been considered which permit the universe to escape from the inflationary phase.…”
Section: Discussionmentioning
confidence: 81%
See 1 more Smart Citation
“…Exact examples displaying a generalised sudden singularity of the type identified by Barrow and Graham [62] for inflationary scalar fields with fractional potentials were found here. Lastly, the ranges for the values of the free parameters of the models have been considered which permit the universe to escape from the inflationary phase.…”
Section: Discussionmentioning
confidence: 81%
“…For small values of |φ| ,the potential, (67) becomes the power-law potential V (φ) φ − 2 3 , which means that finite-time singularities of the 'generalized sudden' type can follow [62]. Moreover, for the EoS for the scalar field it follows that the effective equation of state is…”
Section: Parabolic: N S − 1 Rmentioning
confidence: 99%
“…In principle, the complex F (R) gravity cosmology can develop quite intriguing features, with the most sound one being the inability to analytically continue the Lorentz signature metric to a metric with a Euclidean signature, in the Jordan frame. Also, as shown in [35][36][37][38], bouncing cosmologies in the Jordan frame are never generated by complex F (R) gravity and also bouncing cosmologies in the Einstein frame never lead to complex F (R) gravity in the Jordan frame. However, as we demonstrated in this section, within the mimetic F (R) framework, a complex F (R) gravity in the Jordan frame may realize the matter bounce scenario, for suitably chosen mimetic potential and Lagrange multiplier.…”
Section: Inverse Reconstruction Methods For the F (R) Gravitymentioning
confidence: 99%
“…In classical general relativity (GR), all inflationary models struggle with the inevitable big bang singularity [4][5][6]. One way to address this issue is to work in loop quantum cosmology (LQC), in which the big bang singularity is replaced by a quantum bounce [7][8][9][10].…”
Section: Introductionmentioning
confidence: 99%