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Naturalness and the Weak Gravity Conjecture

3 Pith papers cite this work. Polarity classification is still indexing.

3 Pith papers citing it
abstract

The weak gravity conjecture (WGC) is an ultraviolet consistency condition asserting that an Abelian force requires a state of charge $q$ and mass $m$ with $q>m/m_{\rm Pl}$. We generalize the WGC to product gauge groups and study its tension with the naturalness principle for a charged scalar coupled to gravity. Reconciling naturalness with the WGC either requires a Higgs phase or a low cutoff at $\Lambda \sim q m_{\rm Pl}$. If neither applies, one can construct simple models that forbid a natural electroweak scale and whose observation would rule out the naturalness principle.

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2026 3

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UNVERDICTED 3

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representative citing papers

Wormholes and the imaginary distance bound

hep-th · 2026-05-06 · unverdicted · novelty 6.0

Wormhole effects in theories with imaginary massless scalars set an upper limit on analytic continuation of couplings to imaginary values, with string theory examples showing the low-energy theory breaks down at or before this bound.

Bounding axion dark energy

astro-ph.CO · 2026-04-10 · unverdicted · novelty 6.0

An analytic bound on axion parameters in thawing quintessence is derived independently of initial conditions and used with cosmological observations plus quantum gravity constraints to exclude large regions of axion dark energy parameter space.

Sharpening the Supersymmetric Axion Weak Gravity Conjecture

hep-th · 2026-05-21 · unverdicted · novelty 5.0

The paper verifies the bound fS/|n| ≤ (π/(2 κ_d)) sqrt((d-1)/(d-2)) for axion instantons and sharpens it to fS/|n| ≤ (1/κ_4) sqrt(7/2) for supersymmetric 4d instantons using three approaches in the string landscape.

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  • Bounding axion dark energy astro-ph.CO · 2026-04-10 · unverdicted · none · ref 69

    An analytic bound on axion parameters in thawing quintessence is derived independently of initial conditions and used with cosmological observations plus quantum gravity constraints to exclude large regions of axion dark energy parameter space.