Abstract

Large field inflation is arguably the simplest and most natural variant of slow-roll inflation. Axion monodromy may be the most promising framework for realising this scenario. As one of its defining features, the long-range polynomial potential possesses short-range, instantonic modulations. These can give rise to a series of local minima in the post-inflationary region of the potential. We show that for certain parameter choices the inflaton populates more than one of these vacua inside a single Hubble patch. This corresponds to a dynamical phase decomposition, analogously to what happens in the course of thermal first-order phase transitions. In the subsequent process of bubble wall collisions, the lowest-lying axionic minimum eventually takes over all space. Our main result is that this violent process sources gravitational waves, very much like in the case of a first-order phase transition. We compute the energy density and peak frequency of the signal, which can lie anywhere in the mHz-GHz range, possibly within reach of next-generation interferometers. We also note that this ``dynamical phase decomposition" phenomenon and its gravitational wave signal are more general and may apply to other inflationary or reheating scenarios with axions and modulated potentials.

Highlights

  • The central predictions allowing us to discriminate between inflationary models are the slow roll parameters, most prominently the tilt of the scalar power spectrum ns 0.96 and the tensorto-scalar ratio r 0.08 [1, 2]

  • We show that for certain parameter choices the inflaton populates more than one of these vacua inside a single Hubble patch. This corresponds to a dynamical phase decomposition, analogously to what happens in the course of thermal first-order phase transitions

  • In a stringy setup it is a question of moduli stabilisation: e.g. in the Large Volume Scenario (LVS) [71, 72] decay constants are generically suppressed by the volume of the compactification manifold and are naturally small

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Summary

Introduction

The central predictions allowing us to discriminate between inflationary models are the slow roll parameters, most prominently the tilt of the scalar power spectrum ns 0.96 and the tensorto-scalar ratio r 0.08 [1, 2]. Our message is the following: Due to the typical instantonic modulations of the potential, first order phase-transition-like, violent dynamics may occur after the end of inflation and before reheating. This leads to additional gravitational waves, which are very different in frequency from those studied in the CMB. Appendix B provides some details of an inflection point model of inflation in which our gravitational wave signal may arise

Phases from axion monodromy
Local minima in axion monodromy
Reheating
Field oscillations and damping
Fluctuations and phase decomposition
Inflationary fluctuations
Quantum fluctuations
Enhancement of fluctuations
Gravitational radiation from Phase Transitions
Gravitational waves from bubble collision
Gravitational waves from the matter fluid
Frequency and signal strength of gravitational waves
10 DECIGO aLIGO O5
Conclusions
A Scalar field fluctuations after inflation
Equations of motion
Scalar field as Dark Matter
Equation including non-linearities
B Tuned small field inflation
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