Planckian axions and the Weak Gravity Conjecture
By Thomas C. Bachlechner, Cody Long, Liam McAllister. 2015
151 citations recorded by the source corpus.
A bstractSeveral recent works [1-3] have claimed that the Weak Gravity Conjecture (WGC) excludes super-Planckian displacements of axion fields, and hence large-field axion inflation, in the absence of monodromy. We argue that in theories with N ≫ 1 axions, super-Planckian axion diameters D$$ \mathcal{D} $$ are readily allowed by the WGC. We clarify the non-trivial relationship between the kinetic matrix K — unambiguously defined by its form in a Minkowski-reduced basis — and the diameter of the axion fundamental domain, emphasizing that in general the diameter is not solely determined by the eigenvalues f12 ≤ ⋅ ⋅ ⋅ ≤ fN2 of K: the orientations of the eigenvectors with respect to the identifications imposed by instantons must be incorporated. In particular, even if one were to impose the condition fN< Mpl, this would imply neither D$$ \mathcal{D} $$< Mpl nor D$$ \mathcal{D} $$<NMpl$$ \sqrt{N}{M}_{\mathrm{pl}} $$. We then estimate the actions of instantons that fulfill the WGC. The leading instanton action is bounded from below by S≥SMpl/fN$$ S\ge \mathcal{S}\;{M}_{\mathrm{pl}}/{f}_N $$, with S$$ \mathcal{S} $$ a fixed constant, but in the universal limit S≳SNMpl/fN$$ S\gtrsim \mathcal{S}\sqrt{N}\ {M}_{\mathrm{pl}}/{f}_N $$. Thus, having fN> Mpl does not immediately imply the existence of unsuppressed higher harmonic contributions to the potential. Finally, we argue that in effective axion-gravity theories, the zero-form version of the WGC can be satisfied by gravitational instantons that make negligible contributions to the potential.
Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/304d472316d3c01e55e21119263b0f1ac38f70c9
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Citations in the corpus
- Sharpening the weak gravity conjecture with dimensional reduction (2015, background): “In the context of axion inflation, wormhole solutions have previously been studied by [8, 10] and criticized by [9, 12].”
- The Weak Gravity Conjecture in three dimensions (2016, methodology): “In particular, it has been recently applied to large-field inflationary models and relaxions [2–22].”
- The Swampland: Introduction and Review (2019, background): “ means that the decay constants for each axion need to decrease by a factor of p N, so f˘p1 N , which then precisely cancels the enhancement of the total decay constant [105,106,109{111]. However, in [120] it was argued that a similar way out to alignment, with sub-leading instantons, can be impleme”
- Evidence for a sublattice weak gravity conjecture (2016, background): “From a phenomenological perspective, the WGC is especially interesting due to its ability to constrain models of large-field axion inflation [6–25].”
- Backreacted axion field ranges in string theory (2016, unknown): “The complex-structure moduli Kahler potential is the mirror of the P[1,1,1,6,9] CY studied in [61].”