2014
DOI: 10.1088/1475-7516/2014/12/023
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On the no-boundary proposal for ekpyrotic and cyclic cosmologies

Abstract: The no-boundary proposal provides a compelling theory for the initial conditions of our universe. We study the implications of such initial conditions for ekpyrotic and cyclic cosmologies. These cosmologies allow for the existence of a new type of "ekpyrotic instanton", which describes the creation of a universe in the ekpyrotic contraction phase. Remarkably, we find that the ekpyrotic attractor can explain how the universe became classical. In a cyclic context, in addition to the ekpyrotic instantons there ex… Show more

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Cited by 40 publications
(52 citation statements)
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“…The spectrum of curvature fluctuations in the old ekpyrotic scenario was found to be deeply blue [134][135][136][137] (an additional problem is that these modes do not become classical [138] as opposed to the ones resulting from the entropic mechanism [139] described below). As a result, two-field models [140] were introduced to overcome this problem [141][142][143][144].…”
Section: B Ekpyrotic and Cyclic Scenariosmentioning
confidence: 99%
“…The spectrum of curvature fluctuations in the old ekpyrotic scenario was found to be deeply blue [134][135][136][137] (an additional problem is that these modes do not become classical [138] as opposed to the ones resulting from the entropic mechanism [139] described below). As a result, two-field models [140] were introduced to overcome this problem [141][142][143][144].…”
Section: B Ekpyrotic and Cyclic Scenariosmentioning
confidence: 99%
“…By multiplying (27) through by q 2 and solving near q = 0 one can immediately see that a regular solution requires U ,β ± = 0 at q = 0, which, if we assume that the saddle point will still be the Hartle-Hawking one with q(t = 0) = 0, translates into the requirement β ± (0) = 0. This is indeed a Dirichlet condition, which moreover ensures that the constraint (28) can also be satisfied at the South Pole.…”
Section: The Simplest Case: the "No Boundary Term" Proposalmentioning
confidence: 99%
“…The first three equations yield the generalized momenta, while Eqns. (23), (24) are the Friedmann equations of F(R) gravity in the holonomy corrected scenario, and Eqn. (25) is the conservation equation of the scalar field.…”
Section: B Holonomy Improvementmentioning
confidence: 99%