Related Experiment Video
Updated: Jul 25, 2025

Setting Limits on Supersymmetry Using Simplified Models
Published on: November 15, 2013
Opening up a Window on the Postinflationary QCD Axion
Yunjia Bao1, JiJi Fan2, Lingfeng Li3
1Department of Physics, University of Chicago, Chicago, Illinois 60637, USA.
Abstract:
The QCD axion cosmology depends crucially on whether the QCD axion is present during inflation or not. We point out that contrary to the standard criterion, the Peccei-Quinn (PQ) symmetry could remain unbroken during inflation, even when the axion decay constant, f_{a}, is (much) above the inflationary Hubble scale, H_{I}. This is achieved through the heavy lifting of the PQ scalar field due to its leading nonrenormalizable interaction with the inflaton, encoded in a high-dimensional operator which respects the approximate shift symmetry of the inflaton. The mechanism opens up a new window for the post-inflationary QCD axion and significantly enlarges the parameter space, in which the QCD axion dark matter with f_{a}>H_{I} could be compatible with high-scale inflation and free from constraints on axion isocurvature perturbations. There also exist nonderivative couplings, which still keep the inflaton shift symmetry breaking under control, to achieve the heavy lifting of the PQ field during inflation. Additionally, by introducing an early matter domination era, more parameter space of high f_{a} could yield the observed DM abundance.
Related Concept Videos
The Quantum-Mechanical Model of an Atom
Moment of a Force About an Axis: Scalar
To better understand the concept of moment of force, consider the example of a cyclist riding a bicycle. When the cyclist applies force...
Symmetry in Maxwell's Equations
Perpendicular-Axis Theorem
Consider a circular disc of mass M and radius R lying along an x-y plane. The origin lies at the center of the disc, and the z-axis is perpendicular to the disc's plane. All three axes coincide at the disc's center. The moment of inertia of this...
Subatomic Particles
Atomic Radii and Effective Nuclear Charge

