Litcius/Paper detail

QCD θ-vacuum energy and axion properties

Zhen-Yan Lu, Meng-Lin Du, Feng-Kun Guo, Ulf-G. Meißner, Thomas Vonk

2020Journal of High Energy Physics31 citationsDOIOpen Access PDF

Abstract

A bstract At low energies, the strong interaction is governed by the Goldstone bosons associated with the spontaneous chiral symmetry breaking, which can be systematically described by chiral perturbation theory. In this paper, we apply this theory to study the θ -vacuum energy density and hence the QCD axion potential up to next-to-leading order with N non-degenerate quark masses. By setting N = 3, we then derive the axion mass, self-coupling, topological susceptibility and the normalized fourth cumulant both analytically and numerically, taking the strong isospin breaking effects into account. In addition, the model-independent part of the axion-photon coupling, which is important for axion search experiments, is also extracted from the chiral Lagrangian supplemented with the anomalous terms up to $$ \mathcal{O}\left({p}^6\right) $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>O</mml:mi> <mml:mfenced> <mml:msup> <mml:mi>p</mml:mi> <mml:mn>6</mml:mn> </mml:msup> </mml:mfenced> </mml:math> .

Topics & Concepts

PhysicsAxionGoldstone bosonQuantum chromodynamicsChiral perturbation theoryParticle physicsChiral symmetry breakingIsospinBosonQuarkSymmetry breakingEffective field theorySpontaneous symmetry breakingChiral symmetryTheoretical physicsQCD vacuumPerturbation theory (quantum mechanics)Order (exchange)Quantum electrodynamicsLagrangianStrong CP problemChiral anomalySymmetry (geometry)Electroweak interactionLow energyTechnicolorEnergy (signal processing)Homogeneous spaceEnergy densityStandard Model (mathematical formulation)Quantum Chromodynamics and Particle InteractionsDark Matter and Cosmic PhenomenaParticle physics theoretical and experimental studies