The distribution and shape of dark matter surrounding galaxies, inferred from stellar kinematics.Dark matter halos are the invisible, massive structures that surround galaxies, extending far beyond their visible stars and gas. They are the scaffolding on which galaxies form and evolve, and their shape and distribution are inferred indirectly from the motions of stars and gas within them. The study of dark matter halos is central to understanding galaxy formation, the large-scale structure of the universe, and the nature of dark matter itself.
The concept of dark matter halos emerged in the 1970s from the work of Vera Rubin and Kent Ford, who measured galaxy rotation curves, and earlier theoretical work by Fritz Zwicky in the 1930s on galaxy clusters. The specific term 'halo' became common in the 1980s with the rise of cold dark matter models.
Dark matter halos are not directly observable, but their gravitational influence is. By measuring the rotation curves of galaxies (how fast stars orbit the center) or the velocities of satellite galaxies, astronomers can map the total mass distribution. The observed flat rotation curves, which do not decline as expected from visible matter alone, reveal the presence of a massive, extended halo. The shape of the halo is often modeled as a flattened, triaxial ellipsoid, and its structure can be probed through gravitational lensing, where the halo's gravity bends light from background objects.
Understanding dark matter halos is crucial for interpreting galaxy surveys, predicting gravitational lensing signals, and constraining particle physics models of dark matter candidates.
The Milky Way's dark matter halo is not spherical but is flattened and twisted, likely due to interactions with satellite galaxies.
| Φ_X | variable | dark matter particle flux — particle flux per square metre per second |
| f_X | variable | fraction of dark matter in the form of particle X — dimensionless |
| ρ_DM | variable | dark matter mass density — mass density kilogram per cubic metre |
| m_X | variable | mass of the dark matter particle — mass kilogram |
| v_DM | variable | typical speed of dark matter particles — velocity metre per second |
| b | variable | bias parameter — bias parameter |
| ξ_gal | variable | galaxy two-point correlation function — correlation function |
| ξ_DM | variable | dark matter two-point correlation function — correlation function |
| √ | operator | takes the square root of the ratio — square root |
| 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 |
| \Omega_{\text{DM}} h | variable | Dark matter relic density parameter times squared Hubble constant — density parameter |
| \Gamma | variable | Inflaton decay rate — decay rate per second |
| M_P | variable | Reduced Planck mass — mass kilogram |
| m_{\phi} | variable | Mass of the dark matter particle (or inflaton) — mass kilogram |
| \propto | operator | Indicates direct proportionality — proportionality |
| \sqrt{} | operator | Takes the square root of the argument — square root |
















