Abstract

We consider a five dimensional warped spacetime, in presence of the higher curvature term like F(R) = R + alpha R^2 in the bulk, in the context of the two-brane model. Our universe is identified with the TeV scale brane and emerges as a four dimensional effective theory. From the perspective of this effective theory, we examine the possibility of “inflationary scenario” by considering the on-brane metric ansatz as an FRW one. Our results reveal that the higher curvature term in the five dimensional bulk spacetime generates a potential term for the radion field. Due to the presence of radion potential, the very early universe undergoes a stage of accelerated expansion and, moreover, the accelerating period of the universe terminates in a finite time. We also find the spectral index of curvature perturbation (n_s) and the tensor to scalar ratio (r) in the present context, which match with the observational results based on the observations of Planck (Astron. Astrophys. 594, A20, 2016).

Highlights

  • Over the last two decades, extra spatial dimensions [2–14] have been increasingly playing a central role in physics beyond the standard model of particle [15] and cosmology [16]

  • In order to resolve these problems, the idea of inflation was introduced by Guth [28], in which the universe had to go through a stage of accelerated expansion after the big bang

  • Due to the large curvature (∼ Planck scale) in the bulk, the spacetime is considered to be governed by a higher curvature expression like F(R) = R + α R2

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Summary

Introduction

Over the last two decades, extra spatial dimensions [2–14] have been increasingly playing a central role in physics beyond the standard model of particle [15] and cosmology [16]. We take advantage of the modulus field of extra dimensions and address the early time cosmology of our universe in the backdrop of the RS two-brane model. For RS bulk geometry, where the curvature is of the order of Planck scale, the higher curvature terms should play a crucial role Motivated by this idea, we consider a generalized version of RS model by replacing the Einstein–Hilbert bulk gravity Lagrangian, given by the Ricci scalar R by F(R) where F(R) is an analytic function of R[58–60].

Brief description of the RS scenario
Solutions of field equations for corresponding ST theory
Solutions of effective Friedmann equations
Beginning of inflation
End of inflation
Number of e-foldings and slow roll parameters
10 Dashed curve : with slow roll Solid curve : without slow roll
Summary and concluding remarks
Full Text
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