Gravitational instability of cold matter

Abstract

We solve the nonlinear evolution of pressureless, irrotational density fluctuations in a perturbed Robertson-Walker spacetime using a new Lagrangian method based on the velocity gradient and gravity gradient tensors. Borrowing results from general relativity, we obtain a set of Newtonian ordinary differential equations for these quantities following a given mass element. Using these Lagrangian fluid equations we prove the following results: (1) The spherical tophat perturbation, having zero shear, is the slowest configuration to collapse for a given initial density and growth rate. (2) Initial density maxima are not generally the sites where collapse first occurs. (3) Initially underdense regions may undergo collapse if the shear is not too small. If the magnetic part of the Weyl tensor vanishes, the nonlinear evolution is described purely locally by our equations; this condition holds for spherical, cylindrical, and planar perturbations and may be a good approximation in other circumstances. Assuming the vanishing of the magnetic part of the Weyl tensor, we compute the exact nonlinear gravitational evolution of cold matter. We find that 56\% of initially underdense regions collapse in an Einstein-de Sitter universe for a homogeneous and isotropic random field. We also show that, given this assumption, the final stage of collapse is generically two-dimensional, leading to strongly prolate filaments rather than Zel'dovich pancakes. While this result may explain the prevalence of filamentary collapses in N-body simulations, it is not true in general, suggesting that the magnetic part of the Weyl tensor need not vanish in the Newtonian limit.