Axion detection from neutron stars involves observing electromagnetic signals from axion conversions in strong magnetic fields.Axions are hypothetical elementary particles that could explain dark matter and solve a long-standing puzzle in particle physics known as the strong CP problem. They are predicted to interact extremely weakly with ordinary matter, making them notoriously difficult to detect. Neutron stars, however, offer a unique natural laboratory: their intense magnetic fields — the strongest known in the universe — can convert axions into detectable electromagnetic radiation, typically in the radio or X-ray band.
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. The idea of using neutron stars for axion detection gained traction in the 2010s, with detailed predictions published by researchers such as Christopher Dessert and Benjamin Safdi.
In the presence of a strong magnetic field, an axion can convert into a photon (and vice versa) through a process called the Primakoff effect. Near a neutron star, axions produced in the star's core or in the surrounding magnetosphere would traverse the magnetic field, and a fraction would convert into photons. These photons would emerge with energies matching the axion mass, creating a narrow spectral line that telescopes can search for. The conversion probability depends on the field strength and the path length, which is why neutron stars — with fields up to 10^15 gauss — are prime targets.
Searches for axion-induced radio signals from neutron stars are ongoing using observatories like the Green Bank Telescope and the Effelsberg Telescope, aiming to detect dark matter axions or axions produced in stellar interiors.
If axions exist, they would be so light that a single cubic centimeter of dark matter axions would contain roughly 10^14 particles, yet their combined mass would be only about 10^-18 grams.
| P_{a\to\gamma} | variable | probability of axion-photon conversion — probability |
| g_{a\gamma\gamma} | variable | axion-photon coupling constant — coupling constant reciprocal gev |
| B | variable | magnetic field strength — magnetic flux density tesla |
| L | variable | path length through the magnetic field — length metre |
| \propto | operator | indicates proportionality, not equality — proportional to |
| g_{a\gamma} | variable | Axion-photon coupling constant — coupling constant |
| \sim | operator | Indicates the left side is of the order of the right side — approximate equality |
| ν | variable | Frequency of the converted photon — frequency hertz |
| m_a | variable | Axion mass — mass kilogram |
| ∝ | operator | Indicates that the left side scales linearly with the right side — proportionality |
| E_c | variable | Critical energy — energy joule |
| m_a | variable | Axion mass — mass kilogram |
| ω_pl | variable | Plasma frequency — angular frequency radian per second |
| B_perp | variable | Perpendicular magnetic field strength — magnetic field strength tesla |
| g_aγ | variable | Axion-photon coupling constant — coupling constant inverse gev |

















