
Hypothetical dark matter particles with extremely low mass, such as axions.Ultralight dark matter refers to hypothetical particles with masses far smaller than the electron, often around 10^-22 eV, such as axions. Unlike heavy dark matter candidates like WIMPs, these particles behave more like waves than particles due to their enormous de Broglie wavelength, which can be as large as a galaxy. This wave-like behavior could leave distinct imprints on cosmic structures, such as suppressing small-scale clumping or creating solitonic cores in dark matter halos.
The axion was first proposed in 1977 by Roberto Peccei and Helen Quinn to solve the strong CP problem in quantum chromodynamics, and later recognized as a dark matter candidate. The ultralight scalar field dark matter idea gained traction in the 2000s with models like fuzzy dark matter.
Because of their tiny mass, ultralight dark matter particles are produced in huge numbers and form a coherent quantum state, like a Bose-Einstein condensate. Their wave interference can create patterns of density fluctuations, and they can form stable, oscillating configurations called solitons. Detection strategies often rely on their coupling to photons or other particles, using resonant cavities or atomic magnetometers to pick up faint signals from axion-photon conversion.
Ultralight dark matter searches drive the development of ultra-sensitive detectors, such as the Axion Dark Matter Experiment (ADMX), which uses a tunable microwave cavity to detect axion signals.
If dark matter is made of ultralight particles, a single 'particle' could have a wavelength spanning thousands of kilometers, making it behave more like a wave than a bullet.
| v_min | variable | Minimum dark matter speed — velocity metre per second |
| m_N | variable | Mass of the target nucleus — mass kilogram |
| E_R | variable | Recoil energy of the nucleus — energy joule |
| μ | variable | Reduced mass of the dark matter-nucleus system — reduced mass kilogram |
| δ | variable | Mass splitting between dark matter states (energy gap) — energy joule |
| m_crit | variable | critical dark matter mass — mass kilogram |
| k_B | variable | Boltzmann constant — boltzmann constant joule per kelvin |
| T | variable | temperature — temperature kelvin |
| v | variable | velocity — velocity metre per second |
| \lambda_{\mathrm{Edd | variable | Eddington luminosity ratio — eddington luminosity ratio |
| L_{\mathrm{bol}} | variable | Bolometric luminosity — luminosity watt |
| L_{\mathrm{Edd}} | variable | Eddington luminosity — luminosity watt |













