Partial geometrization of dark matter in metric gravity: Exact reconstruction and growth constraints
arXiv:2610.30201
Abstract
We ask what fraction of dark matter can be accounted for by the geometry of a stable metric theory, requiring the expansion history to be exactly equal to that of the CDM model. Only a fraction of dark matter clusters as dust, whereas supplies the rest, as well as . We show that the background reconstruction reduces to a linear equation for , whose solution is , with independent of : the departure from general relativity is exactly proportional to the geometrized fraction. We solve this equation in closed form in the matter and radiationmatter eras: in both, the solution is an elementary particular solution plus two hypergeometric modes. Stability requires to decrease monotonically in time, so cannot take its general-relativity value both at early and at late times. The effective gravitational coupling therefore necessarily runs: between the radiation era and the de Sitter attractor, changes by at least . In all stable reconstructions but one, grows as at high curvature, i.e., in dense environments such as the Sun, and local tests of gravity exclude them. The surviving member has at early times: it recovers general relativity at high curvature and attains the minimal running of . Keeping the linear growth factor at within of its CDM value requires , the weakest bound among all stable reconstructions; keeping within requires . Growth-rate data from DESI DR1 and SDSS DR16 give --, and the Cassini bound gives . A smoothly evolving metric background can therefore geometrize only a negligible fraction of dark matter.
arXiv comment14 pages, 7 figures, 2 tables