Abstract

Local nonlinear approximations to the growth of cosmic perturbations are developed, resulting in relations, at a given epoch, between the peculiar velocity and gravity fields and their gradients. Only the equation of motion is approximated, while mass conservation and the computation of the gravitational field are treated exactly. The second-order relation is derived for arbitrary geometry and cosmological parameters. Solutions are developed to fourth order for laminar spherical perturbations in an Einstein-de Sitter universe, but the gain in accuracy for higher orders is modest. All orders become comparable when the peculiar kinetic energy per unit mass equals the peculiar potential, typically at relative density perturbations, $\delta \sim 4$. The general second-order relation, while implicit, is simple to solve. \nbody simulations show that it provides moderate gains in accuracy over other local approximations. It can therefore be easily applied in the comparison of large-scale structures and velocities in the quasi-linear regime, $\delta \sim 1 - 4$, as well as in the reconstruction of the primordial perturbations from which they grew.

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