Abstract

It has been recently argued that Higgsing of theories with U(1)n gauge interactions consistent with the Weak Gravity Conjecture (WGC) may lead to effective field theories parametrically violating WGC constraints. The minimal examples typically involve Higgs scalars with a large charge with respect to a U(1) (e.g. charges (Z, 1) in U(1)2 with Z ≫ 1). This type of Higgs multiplets play also a key role in clockwork U(1) theories. We study these issues in the context of heterotic string theory and find that, even if there is no new physics at the standard magnetic WGC scale Λ ∼ gIRMP, the string scale is just slightly above, at a scale sim sqrt{k_{mathrm{IR}}}varLambda . Here kIR is the level of the IR U(1) worldsheet current. We show that, unlike the standard magnetic cutoff, this bound is insensitive to subsequent Higgsing. One may argue that this constraint gives rise to no bound at the effective field theory level since kIR is model dependent and in general unknown. However there is an additional constraint to be taken into account, which is that the Higgsing scalars with large charge Z should be part of the string massless spectrum, which becomes an upper bound kIR ≤ k02, where k0 is the level of the UV currents. Thus, for fixed k0, Z cannot be made parametrically large. The upper bound on the charges Z leads to limitations on the size and structure of hierarchies in an iterated U(1) clockwork mechanism.

Highlights

  • The latter equality shows that A has norm 1, modulo 1/Z2 corrections

  • It has been recently argued that Higgsing of theories with U(1)n gauge interactions consistent with the Weak Gravity Conjecture (WGC) may lead to effective field theories parametrically violating WGC constraints

  • The minimal examples typically involve Higgs scalars with a large charge with respect to a U(1) (e.g. charges (Z, 1) in U(1)2 with Z ≫ 1). This type of Higgs multiplets play a key role in clockwork U(1) theories. We study these issues in the context of heterotic string theory and find that, even if there is no new physics at the sta√ndard magnetic WGC scale Λ ∼ gIRMP, the string scale is just slightly above, at a scale ∼ kIRΛ

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Summary

A string theory embedding

Let us consider a string theory 4D compactification with some U(1)N gauge group and charged matter fields. Consistency with the weakest form of the WGC is still guaranteed, since the particle ψ2 with charge 1 under the unbroken U(1) will obey the first condition (2.4).The same discussion applies as in the field theory case, and a particle ψ1 with charge (1, 0) will couple with a strength ≃ g/Z after Higgsing. This sets the quantum of charge for AIR, so that the charge lattice is Z/Z; we get to the canonical normalization by multiplication by Z, which yields kIR = Z2k0, αIR α0 Z2.

Clockwork
16 MS2 α0 Mp2
Summary

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