# Quantum Incompleteness of Inflation

**Authors:** Alice Di Tucci, Job Feldbrugge, Jean-Luc Lehners, Neil Turok

arXiv: 1906.09007 · 2019-09-25

## TL;DR

This paper reveals that quantum effects challenge the classical description of inflation at early times, showing the need for new physics to specify initial conditions and maintain stability of fluctuations.

## Contribution

It develops a path integral approach treating background and perturbations quantum mechanically, uncovering a breakdown of QFT in curved spacetime at small initial volumes.

## Key findings

- Two background saddle points contribute at small initial scale factors.
- Quantum fluctuations become unstable without specific initial conditions.
- Proper initial conditions require large initial volume and input of stable fluctuations.

## Abstract

Inflation is most often described using quantum field theory (QFT) on a fixed, curved spacetime background. Such a description is valid only if the spatial volume of the region considered is so large that its size and shape moduli behave classically. However, if we trace an inflating universe back to early times, the volume of any comoving region of interest -- for example the present Hubble volume -- becomes exponentially small. Hence, quantum fluctuations in the trajectory of the background cannot be neglected at early times. In this paper, we develop a path integral description of a flat, inflating patch (approximated as de Sitter spacetime), treating both the background scale factor and the gravitational wave perturbations quantum mechanically. We find this description fails at small values of the initial scale factor, because \emph{two} background saddle point solutions contribute to the path integral. This leads to a breakdown of QFT in curved spacetime, causing the fluctuations to be unstable and out of control. We show the problem may be alleviated by a careful choice of quantum initial conditions, for the background and the fluctuations, provided that the volume of the initial, inflating patch is larger than $\gg H^{-1}$ in Planck units with $H$ the Hubble constant at the start of inflation. The price of the remedy is high: not only the inflating background, but also the stable, Bunch-Davies fluctuations must be input by hand. Our discussion emphasizes that, even if the inflationary scale is far below the Planck mass, new physics is required to explain the initial quantum state of the universe.

## Full text

_Full body text omitted from this summary view._ Fetch the complete paper as Markdown: https://tomesphere.com/paper/1906.09007/full.md

## Figures

23 figures with captions in the complete paper: https://tomesphere.com/paper/1906.09007/full.md

## References

36 references — full list in the complete paper: https://tomesphere.com/paper/1906.09007/full.md

---
Source: https://tomesphere.com/paper/1906.09007