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axion
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An axion () is a hypothetical elementary particle originally theorized in 1978 independently by Frank Wilczek and Steven Weinberg as the Goldstone boson of Peccei–Quinn theory, which had been proposed in 1977 to solve the strong CP problem in quantum chromodynamics (QCD). If axions exist and have low mass within a specific range, they are of interest as a possible component of cold dark matter.

Key facts

Particle.name
Axion
Particle.status
Hypothetical
Particle.interaction
Gravitational, electromagnetic, strong, weak
Particle.theorized
1978, Wilczek and Weinberg
Particle.symbol
A0, a, θ
Particle.mass
10−7 to 1 eV/c2
Particle.electric_charge
0 e
Particle.spin
0&nbsp;ħ <!--
Particle.Grouping
Goldstone Boson -->

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spin quantum number
0
Commons category
Axions
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~25 min read

Article

31 sections
Contents
  • History
  • Strong CP problem
  • Prediction
  • Axion dark matter
  • Pre-inflationary scenario
  • Post-inflationary scenario
  • Phenomenology of the axion field
  • Searches <span class="anchor" id="K-S-V-Z-vs-D-F-S-Z-anchor"></span>
  • Maxwell's equations with axion modifications
  • Analogous effect for topological insulators
  • Experiments
  • Direct conversion in a magnetic field
  • Polarized light in a magnetic field
  • Light shining through walls
  • Astrophysical axion searches
  • Searches for resonance effects
  • Dark matter recoil searches
  • Nuclear spin precession
  • Searches at particle colliders
  • Disputed detections
  • Properties
  • Predictions
  • Cosmological implications
  • Supersymmetry
  • See also
  • Footnotes
  • References
  • Sources
  • External links
  • Experiments
  • Popular science coverage

An axion () is a hypothetical elementary particle originally theorized in 1978 independently by Frank Wilczek and Steven Weinberg as the Goldstone boson of Peccei–Quinn theory, which had been proposed in 1977 to solve the strong CP problem in quantum chromodynamics (QCD). If axions exist and have low mass within a specific range, they are of interest as a possible component of cold dark matter.

== History == === Strong CP problem === As shown by Gerard 't Hooft, strong interactions of the Standard Model, QCD, possess a non-trivial vacuum structure that in principle permits violation of the combined symmetries of charge conjugation and parity, collectively known as CP. Together with effects generated by weak interactions, the effective periodic strong CP-violating term, , appears as a Standard Model input – its value is not predicted by the theory, but must be measured. However, large CP-violating interactions originating from QCD would induce a large electric dipole moment (EDM) for the neutron. Experimental constraints on the EDM implies that CP violation from QCD must be extremely tiny and thus must itself be extremely small. Since could have any value between 0 and 2, this presents a "naturalness" problem for the Standard Model. Why should this parameter find itself so close to zero? (Or, why should QCD find itself CP-preserving?) This question constitutes what is known as the strong CP problem.

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