Abstract

In this note, we discuss the implications of the weak gravity conjecture (WGC) for general models of large-field inflation with a large number of axions $N$. We first show that, from the bottom-up perspective, such models admit a variety of different regimes for the enhancement of the effective axion decay constant, depending on the amount of alignment and the number of instanton terms that contribute to the scalar potential. This includes regimes of no enhancement, power-law enhancement and exponential enhancement with respect to $N$. As special cases, we recover the Pythagorean enhancement of $N$-flation, the $N$ and $N^{3/2}$ enhancements derived by Bachlechner, Long and McAllister and the exponential enhancement by Choi, Kim and Yun. We then analyze which top-down constraints are put on such models from the requirement of consistency with quantum gravity. In particular, the WGC appears to imply that the enhancement of the effective axion decay constant must not grow parametrically with $N$ for $N \gg 1$. On the other hand, recent works proposed that axions might be able to violate this bound under certain circumstances. Our general expression for the enhancement allows us to translate this possibility into a condition on the number of instantons that couple to the axions. We argue that, at large $N$, models consistent with quantum gravity must either allow super-Planckian field excursions or have an enormous, possibly even exponentially large, number of dominant instanton terms in the scalar potential.

Highlights

  • The weak gravity conjecture (WGC) [6] — suggests that this is not a coincidence but due to a general principle in string theory

  • In [12], it was shown that contributions to the scalar potential from gravitational instantons forbid a super-Planckian field range, confirming that the WGC bounds the field excursion in models with one or several axions

  • For feff Mp, there is no reason to suspect that anything goes wrong with such an enhancement, while for larger feff it is possible that string theory forbids a further enhancement due to the WGC [6, 9, 11,12,13]

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Summary

The weak gravity conjecture

The WGC postulates that gravity must be the weakest force in any consistent 4D lowenergy EFT [6]. It should be possible to engineer models with an effective axion decay constant feff ∼ N λMp along some diagonal in the axion field space and, obtain super-Planckian field excursions It was argued in [13, 16] that it is unlikely that this loophole can be realized in a consistent string theory model. Another proposed loophole [10] is that, in certain models, instanton corrections may come with extra suppression factors such that they can be suppressed in the scalar potential even if their Euclidean action is small In such models, one might be able to satisfy the strong WGC and still obtain super-Planckian field ranges. It should be worthwhile to analyze the problem from a different point of view, as we will do

The effective axion decay constant
A simple model
General polytopes
Quantum gravity constraints
General considerations
Relation between instantons and enhancement
Discussion
A Enhancement for a general polytope
Trigonometry
Recurrence relation
Full Text
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