
Methods for detecting dark matter through its interactions with black holes, satellites, or quantum sensors.Dark matter detection refers to experimental efforts to observe particles or phenomena that constitute dark matter, the invisible mass that makes up about 85% of the universe's matter. Since dark matter does not interact electromagnetically, detectors must look for rare scattering events with ordinary matter, or for signals from exotic processes like axion conversion or black hole evaporation. Modern approaches include cryogenic crystal detectors, quantum sensors, and even networks of atomic clocks.
The first direct detection experiments began in the 1980s, with the UK's DAMA and the US's CDMS among the pioneers. No definitive detection has been confirmed as of 2025.
Most detectors rely on measuring the tiny energy deposition when a dark matter particle (like a WIMP) scatters off a nucleus or electron. This requires extremely low backgrounds, achieved by deep underground labs and ultra-clean materials. Alternative methods: axion detectors use strong magnetic fields to convert axions into photons; quantum sensors (e.g., superconducting qubits) can detect single phonons or photons from dark matter interactions; and some proposals use the timing of pulsars or gravitational wave detectors to sense the gravitational effects of dark matter.
Primarily used in fundamental physics research, but the technology developed (ultra-low-noise sensors, cryogenics) has spin-offs in quantum computing and precision metrology.
Some dark matter detectors are so sensitive that they must be shielded from cosmic rays, and even the decay of trace radioactive isotopes in the detector material itself can mimic a dark matter signal.
| C | variable | capture rate of dark matter particles by the star — capture rate per second |
| R | variable | radius of the star — radius metre |
| ρ_χ | variable | mass density of dark matter in the local environment — mass density kilogram per cubic metre |
| m_χ | variable | mass of a single dark matter particle — mass kilogram |
| v | variable | typical relative speed of dark matter particles with respect to the star — velocity metre per second |
| σ | variable | scattering cross-section between dark matter and stellar nucleons — cross section square metre |
| \tau_d | variable | optical depth due to dust — optical depth |
| M_d | variable | total dust mass — mass kilogram |
| \rho_d | variable | mass density of individual dust grains — mass density kilogram per cubic metre |
| v_{\text{ej}} | variable | ejection speed of the dust — velocity metre per second |
| t | variable | time since ejection — time second |

















