A parameter describing the strength of the interaction between axions and photons, constrained by experiments.The axion-photon coupling is a fundamental parameter that quantifies how strongly hypothetical particles called axions interact with light. Axions were originally proposed to solve a deep puzzle in particle physics—the strong CP problem—but they also emerge naturally in string theory and are a leading candidate for dark matter. This coupling determines how readily an axion can convert into a photon (and vice versa) in the presence of a magnetic field, which is the key to nearly all experimental searches for these elusive particles.
The concept was introduced in the late 1970s and early 1980s by Frank Wilczek and Steven Weinberg, who independently realized that the axion, proposed by Roberto Peccei and Helen Quinn in 1977, would necessarily interact with two photons.
In a magnetic field, an axion can transform into a photon and a photon can transform into an axion, a phenomenon known as the Primakoff effect. The strength of this conversion is directly proportional to the axion-photon coupling constant. Experiments exploit this by placing strong magnets in front of sensitive detectors: if axions exist, some of them should convert into detectable X-rays or radio waves. Conversely, powerful lasers shone through magnetic fields could produce axions that escape, leaving a slight dimming of the light.
The coupling is the central target of experiments like ADMX (Axion Dark Matter eXperiment), which searches for dark matter axions converting to microwaves in a resonant cavity, and light-shining-through-a-wall experiments that look for photons regenerated from axions created on the other side of a barrier.
The axion-photon coupling is so weak that a single axion would travel through a light-year of lead with a 50% chance of interacting, making it one of the most weakly interacting particles ever proposed.











