Breaking the axion abundance-isocurvature relation: Scale invariance and high-scale inflation
Abstract
A QCD axion accounting for dark matter through pre-inflationary misalignment is strongly constrained by CMB isocurvature bounds, which place the classic axion window in tension with high-scale inflation. The tension arises because the same decay constant controls both the relic abundance and the primordial axion fluctuations. We show how this link can be broken in a broad class of scale-invariant models, without introducing any dimensionful parameter into the classical action. Rather than imposing a fixed Peccei-Quinn scale, the axion's kinetic normalisation is set by a dynamical field ratio. The resulting field-space metric controls the abundance through its value today and the primordial fluctuations through its value at horizon crossing. A sufficiently large metric during inflation suppresses isocurvature, allowing high-scale inflation in the classic axion window with an untuned misalignment angle and sub-Planckian decay constants. The exact scale and Peccei-Quinn symmetries also enforce a non-turning inflationary attractor, conserving the super-Hubble curvature perturbation and preserving the single-field adiabatic spectrum. We realise the mechanism in the Higgs-Dilaton model by deforming the Peccei-Quinn kinetic term. The same deformation turns the inflaton sector into an α-attractor pinned near the Starobinsky point. This explicit realisation has a super-Planckian present decay constant, which places it in the anthropic window, now reopened at high inflationary scales, with an ultralight QCD axion constrained by black-hole superradiance.
Related
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- A Stepping Stone Solution to the QCD Axion Isocurvature Problem
- Dilaton-flattened axion inflation
- Perturbative Kähler Moduli Inflation
- Reconciling nonminimally coupled Higgs inflation with ACT DR6 observations through reheating
BibTeX
@misc{angelis2026breaking,
title = {{Breaking the axion abundance-isocurvature relation: Scale invariance and high-scale inflation}},
author = {Mariaveronica De Angelis and Javier Rubio},
howpublished = {arXiv},
year = {2026},
month = oct,
doi = {10.48550/arxiv.2610.24070},
eprint = {2610.24070},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2610.24070},
}
RIS
TY - UNPB
TI - Breaking the axion abundance-isocurvature relation: Scale invariance and high-scale inflation
AU - Mariaveronica De Angelis
AU - Javier Rubio
PY - 2026
DA - 2026/10/16
PB - arXiv
DO - 10.48550/arxiv.2610.24070
UR - https://arxiv.org/abs/2610.24070
AB - A QCD axion accounting for dark matter through pre-inflationary misalignment is strongly constrained by CMB isocurvature bounds, which place the classic axion window in tension with high-scale inflation. The tension arises because the same decay constant controls both the relic abundance and the primordial axion fluctuations. We show how this link can be broken in a broad class of scale-invariant models, without introducing any dimensionful parameter into the classical action. Rather than imposing a fixed Peccei-Quinn scale, the axion's kinetic normalisation is set by a dynamical field ratio. The resulting field-space metric controls the abundance through its value today and the primordial fluctuations through its value at horizon crossing. A sufficiently large metric during inflation suppresses isocurvature, allowing high-scale inflation in the classic axion window with an untuned misalignment angle and sub-Planckian decay constants. The exact scale and Peccei-Quinn symmetries also enforce a non-turning inflationary attractor, conserving the super-Hubble curvature perturbation and preserving the single-field adiabatic spectrum. We realise the mechanism in the Higgs-Dilaton model by deforming the Peccei-Quinn kinetic term. The same deformation turns the inflaton sector into an α-attractor pinned near the Starobinsky point. This explicit realisation has a super-Planckian present decay constant, which places it in the anthropic window, now reopened at high inflationary scales, with an ultralight QCD axion constrained by black-hole superradiance.
ER -