method

axion detection

Axion detection involves searching for axion dark matter using astrophysical observations and experimental techniques.
52 related articles · 6 formulas

Description

Axion detection is the search for hypothetical elementary particles called axions, which are prime candidates for dark matter. Axions are extremely light, weakly interacting particles predicted by extensions of the Standard Model to solve the strong CP problem. Detecting them is challenging because they interact so feebly with ordinary matter, but their existence would explain a significant fraction of the universe's missing mass and open a new window into particle physics.

History

The axion was proposed in 1977 by Roberto Peccei and Helen Quinn to explain why the strong nuclear force preserves CP symmetry, with the particle itself named by Frank Wilczek and Steven Weinberg. Experimental searches began in the 1980s and continue today.

How it works

Axions can convert into photons in the presence of strong magnetic fields (the Primakoff effect). Experiments like haloscopes use resonant cavities in strong magnetic fields to detect microwave photons produced by axion conversion. Astrophysical observations look for axion-induced effects, such as anomalous energy loss in stars or polarization changes in light from distant sources. Neutron star polar caps are also proposed as natural axion-to-photon converters.

In practice

Axion detection experiments, such as ADMX, aim to discover dark matter; if successful, they would revolutionize both cosmology and particle physics.

Fun fact

Axions, if they exist, could also explain why neutron stars cool faster than expected, as they would carry away energy from the star's core.

Concept graph →

Formulas

$$m_a \propto \frac{1}{f_a}$$
The axion mass is inversely proportional to the symmetry breaking scale.
What is in the formula
m_avariableAxion mass — mass kilogram
f_avariableAxion decay constant (symmetry breaking scale) — energy joule
∝operatorIndicates a direct proportionality relationship — proportionality
m_a\simeq5.7μ{эв}*\frac{10^{12}{гэв}}{f_a} · 2606.07742v1
m_a\approx5.7μ{ev}*\frac{10^{12}{gev}}{f_a} · 2607.23140v1
$$\nu \propto m_a$$
Axion-photon conversion frequency is proportional to axion mass.
What is in the formula
νvariableFrequency of the converted photon — frequency hertz
m_avariableAxion mass — mass kilogram
∝operatorIndicates that the left side scales linearly with the right side — proportionality
ν\simeq242{мгц}(\frac{m_a}{μ{эв}}) · 2606.04304v1
$$\mathcal{L} = g_{a\gamma\gamma} a \mathbf{E} \cdot \mathbf{B}$$
Lagrangian term coupling axion to electromagnetic fields.
What is in the formula
avariableaxion field — axion field
Evariableelectric field — electric field volt per metre
Bvariablemagnetic field — magnetic field strength tesla
g_{aγγ}constantStrength of the interaction between axions and two photons. — axion photon coupling constant = model-dependent
\mathcal{l}=g_{aγγ}a{e}*{b} · 2606.17067v1
$$H \approx m_a$$
Axion field oscillates when Hubble rate equals mass.
What is in the formula
HvariableHubble parameter — hubble parameter per second
m_avariableAxion mass — mass kilogram
h(t_{\rmosc})\approxm_a · 2607.01333v1
$$\theta = \frac{g_{a\gamma}}{2} \Delta a$$
Axion field difference rotates photon polarization.
What is in the formula
\thetavariableRotation angle of photon polarization — angle radian
g_{a\gamma}variableAxion-photon coupling constant — coupling constant reciprocal gev
\Delta avariableDifference in axion field value — axion field gev
θ_a(t_{\rmobs})=\frac{g_{aγ}}{2}[a(t_{\rmobs},{x}_{\rmobs})-a(t_{\rmem},{x}_{\rmem})] · 2607.04550
$$P_{a\to\gamma} \propto (g_{a\gamma\gamma} B L)^2$$
Probability of axion converting to photon scales with magnetic field and distance squared.
What is in the formula
P_{a\to\gamma}variableprobability of axion-photon conversion — probability
g_{a\gamma\gamma}variableaxion-photon coupling constant — coupling constant reciprocal gev
Bvariablemagnetic field strength — magnetic flux density tesla
Lvariablepath length through the magnetic field — length metre
\proptooperatorindicates proportionality, not equality — proportional to
p_{a\toγ}\approx\frac{(g_{aγγ}bl)^2}{4} · 2607.23140v1

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