2008
DOI: 10.1103/physrevd.77.083513
|View full text |Cite
|
Sign up to set email alerts
|

Classical bounce: Constraints and consequences

Abstract: We perform a detailed investigation of the simplest possible cosmological model in which a bounce can occur, namely that where the dynamics is led by a simple massive scalar field in a general selfinteracting potential and a background spacetime with positively curved spatial sections. By means of a phase space analysis, we give the conditions under which an initially contracting phase can be followed by a bounce and an inflationary phase lasting long enough (i.e., at least 60-70 e-folds) to suppress spatial c… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

0
72
0
1

Year Published

2009
2009
2017
2017

Publication Types

Select...
8

Relationship

3
5

Authors

Journals

citations
Cited by 57 publications
(73 citation statements)
references
References 59 publications
(103 reference statements)
0
72
0
1
Order By: Relevance
“…• How do those results compare with models dealing with classical bounces (see, e.g., [23])? If the IR power suppression is probably a generic feature of bounces, the detailed features are modeldependent.…”
Section: Discussionmentioning
confidence: 99%
“…• How do those results compare with models dealing with classical bounces (see, e.g., [23])? If the IR power suppression is probably a generic feature of bounces, the detailed features are modeldependent.…”
Section: Discussionmentioning
confidence: 99%
“…A generic consequence of violating the null energy condition is the appearance of fields with negative kinetic energy: ghosts; a crucial point in bouncing models is actually to construct a regular model in which such ghosts are absent while still having a bouncing phase. It is possible to generate a bounce in the presence of curvature K = 1 without violating the NEC, but only the strong energy condition, SEC, which demands ρ + P ≥ 0 and ρ + 3P ≥ 0, see [22,49] for concrete models. Such a bounce could leave some amount of spatial curvature in the expanding phase, whose amplitude may require a subsequent inflationary phase to dilute it, hence possibly ruining the alternative-to-inflation program (as emphasized above, we shall not be concerned here with the mixed models in which a bounce permits to avoid a primordial singularity while a subsequent inflation phase solves the other puzzles of the standard hot big-bang model).…”
Section: B What Is Used To Get a Bounce?mentioning
confidence: 99%
“…How spatial curvature can drastically modify a model's prediction is illustrated in [22,49]: here, a simple bouncing model is considered, based on a scalar field and curvature. The former has a potential whose maximum is reached at the bounce, which is canceled by the curvature contribution, such that H → 0 without violating the NEC.…”
Section: Spatial Curvature and Non-gaussianitiesmentioning
confidence: 99%
See 1 more Smart Citation
“…This model might be interesting in its own right, and further details will be presented elsewhere. For previous work on bouncing solutions and their likelihood see, for example, [59,60]. …”
Section: Bounce Solutionmentioning
confidence: 99%