Abstract

We compute the graviton one-loop correction to the expectation value of the local expansion rate in slow-roll inflation, with both slow-roll parameters finite. The calculation is based on a recent method to explicitly construct gauge-invariant observables in perturbative quantum gravity at all orders in perturbation theory, and it is particularly suited in cases of highly-symmetrical space-time backgrounds. Our analysis adds to recent calculations of that correction in de Sitter space-time and in single-field inflation with constant deceleration. In the former case a vanishing one-loop correction was found, while in the latter the quantum backreaction produces a secular effect that accelerates the expansion. The quantum correction we describe here produces a finite secular effect that can either accelerated or decelerate the background expansion, depending on the value of the slow-roll parameters.

Highlights

  • According to our current understanding of the evolution of the early Universe, the anisotropies in the cosmological microwave background (CMB) [1,2,3] were created by quantum fluctuations of the metric during the inflationary era [4,5,6,7]

  • Similar calculations were recently performed in de Sitter space-time [26] and in single-field inflation with constant deceleration parameter [27]

  • The one-loop correction needs a huge number of e-folds to become important, this is not rule out as there is no upper bound on the duration of inflation

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Summary

Introduction

According to our current understanding of the evolution of the early Universe, the anisotropies in the cosmological microwave background (CMB) [1,2,3] were created by quantum fluctuations of the metric during the inflationary era [4,5,6,7]. The fast space-time expansion during inflation copiously excites gravitons out of the vacuum [9, 10]. At tree level these quantum excitations created small fluctuations in the density profile of the cosmological fluid by gravitational attraction, which show up in CMB maps today as regions slightly hotter or colder than the background [11, 12]

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