The motion of a nucleus after being struck by a particle, a key dark matter signature.Nuclear recoil is the sudden motion of an atomic nucleus after it is struck by a particle, such as a neutron, a neutrino, or a hypothetical dark matter particle. Because the nucleus is heavy, the recoil is typically slow and short-ranged, but it deposits a small amount of energy into the surrounding material. This makes nuclear recoil the primary signature searched for in direct dark matter detection experiments, where a weakly interacting massive particle (WIMP) is expected to collide with a nucleus and cause it to move.
The idea that dark matter could be detected via nuclear recoil was proposed in the mid-1980s by Mark Goodman and Edward Witten, building on earlier suggestions by Michael Dine and colleagues.
When an incoming particle scatters off a nucleus, momentum and energy are conserved. The nucleus gains kinetic energy and begins to move through the detector medium, ionizing atoms or creating phonons (vibrations) as it slows down. The recoil energy is usually tiny — on the order of keV — but it can be distinguished from electron recoils (caused by gamma rays or beta particles) by the different ratio of ionization to heat produced. Detectors like liquid argon or xenon time projection chambers measure both the scintillation light and the ionization charge to identify nuclear recoil events.
Nuclear recoil is the basis for all direct dark matter searches, including experiments like LUX-ZEPLIN, XENONnT, and DarkSide, as well as for neutrino detection via coherent elastic neutrino-nucleus scattering.
Ancient mica crystals have been examined for tracks left by nuclear recoils from dark matter interactions over billions of years, potentially providing a fossil record of dark matter.









