Three tracers give complementary estimates of a cluster's gravitating mass. First, galaxy redshifts measure a line-of-sight velocity dispersion . For a roughly stationary bound cluster, the virial theorem gives a cluster velocity-dispersion mass estimate
with a coefficient depending on the density profile and orbital anisotropy. The galaxy luminosity and plausible stellar mass-to-light ratio supply too little mass to bind typical rich clusters. Foreground interlopers, substructure, velocity anisotropy and a recent merger can bias the dynamical estimate; a large dispersion is not by itself proof of equilibrium.
Second, diffuse X-ray emission measures a hot intracluster plasma, not merely unresolved starlight. Spectral continuum and lines constrain its temperature, while surface-brightness profiles constrain its density after line-of-sight projection and emissivity modeling. If the gas has constant composition and is approximately spherical and in hydrostatic equilibrium,
This cluster hydrostatic mass estimator uses as the mean mass per pressure-supporting particle. The inferred potential requires substantially more mass than the stars plus measured gas, although the gas contains much of the visible baryonic mass. Turbulence, bulk motion, temperature structure and departures from hydrostatic equilibrium are important systematic errors.
Third, strong-lensing arcs and multiple images, together with coherent weak-lensing shear of background galaxies, measure projected gravitational deflection. In general relativity,
This cluster gravitational-lensing mass estimate does not require the cluster galaxies or gas to be in dynamical equilibrium. It does require source-distance information, a lens model and control of point-spread-function-induced shapes, line-of-sight projection, unrelated line-of-sight structure and the mass-sheet degeneracy.
The convergence of dynamical, hydrostatic and lensing masses, exceeding the baryonic inventory, is the principal evidence. The Bullet Cluster adds a spatial test: collisional X-ray gas lags behind the galaxies during the merger, while the inferred lensing concentrations lie nearer the collisionless galaxy component. An additional weakly collisional gravitating mass accounts naturally for that separation.[ref] The conclusion assumes a gravitational framework and does not identify the microscopic dark-matter particle; the different tracer systematics should be evaluated rather than treating three mass estimates as completely assumption free.

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