Abstract
Many cosmological models rely on large couplings of axions to gauge fields. Examples include theories of magnetogenesis, inflation on a steep potential, chiral gravitational waves, and chromonatural inflation. Such theories require a mismatch between the axion field range and the mass scale appearing in the aFtilde{F} coupling. This mismatch suggests an underlying monodromy, with the axion winding around its fundamental period a large number of times. We investigate the extent to which this integer can be explained as a product of smaller integers in a UV completion: in the parlance of our times, can the theory be “clockworked”? We argue that a clockwork construction producing a potential {mu}^4 cos left(frac{a}{j{F}_a}right) for an axion of fundamental period Fa will obey the constraint μ < Fa. For a some applications, including chromonatural inflation with sub-Planckian field range, this constraint obstructs a clockwork UV completion. Alternative routes to a large coupling include fields of large charge (an approach limited by strong coupling) or kinetic mixing (requiring a lighter axion). Our results suggest that completions of axion cosmologies that explain the large parameter in the theory potentially alter the phenomenological predictions of the model.
Highlights
Examples include theories of magnetogenesis, inflation on a steep potential, chiral gravitational waves, and chromonatural inflation
Chromonatural inflation models feature an axion with a large coupling to gauge fields, requiring a very large enhancement factor jk — much larger than the O(100) number usually stated in the literature
Large couplings of axion to gauge fields could lead to very interesting cosmology
Summary
K is an anomaly coefficient that depends on the gauge and PQ charges (and the number of flavors) of fermions integrated out at the scale Fa. As discussed in appendix C of ref. [65], larger PQ charges qPQ require small fermion masses ∝ (Fa/Λ)qPQ, and it is not possible to get a very large enhancement by increasing PQ charges alone. We briefly recall the problem with large gauge charges. We imagine that the axion interaction is generated by Nf fermions Q as in the KSVZ axion model [76, 77]: L. where I2(Q) is the Dynkin index of the representation. Requiring that the gauge theory is perturbative at the scale of the PQ breaking requires. In these models the fermions get a mass from the spontaneous breaking of the PQ symmetry, so that mf Fa
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