Planckian axions and the Weak Gravity Conjecture
Planckian axions and the Weak Gravity Conjecture
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普朗克轴子和弱引力猜想
DOI:
10.1007/jhep01(2016)091
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发表时间:
2015
影响因子:
5.4
通讯作者:
L. McAllister
中科院分区:
文献类型:
--
作者:
Thomas C. Bachlechner;Cody Long;L. McAllister
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.