- Article
We study the Kretschmann invariant K of the post-Newtonian spacetime of a slowly rotating, axially symmetric clump of collisionless matter with a prescribed Miyamoto–Nagai potential, whose metric and matter content to second order in the compactness were constructed in a companion paper. At , K is a quadratic form in the Hessian of the potential, with closed-form central and asymptotic values. At we show that the static part of K is a closed-form local function of the potential and of the matter fields at every point: the second-order metric functions, which solve a Poisson-type problem and encode the global mass distribution, enter only through the Ricci tensor, that is, only through the local matter. This follows from an exact expression of K for static spacetimes in terms of the tidal tensor of static observers and the local stresses, and holds for any regular prescribed potential. At a centre with isotropic stresses it reduces to
21 October 2026




