Second-order perturbations of cosmological fluids: Relativistic effects of pressure, multi-component, curvature, and rotation

Details Second-order perturbations of cosmological fluids: Relativistic effects of pressure, multi-component, curvature, and rotation Second-order perturbations of cosmological fluids: Relativistic effects of pressure, multi-component, curvature, and rotation

2007-04-16

arxiv.org/abs/0704.1927v1

Phys.Rev.D76:103527,2007

Astronomy and Astrophysics

Astrophysics

41 pages, no figure

Scientific paper

10.1103/PhysRevD.76.103527

We present general relativistic correction terms appearing in Newton's gravity to the second-order perturbations of cosmological fluids. In our previous work we have shown that to the second-order perturbations, the density and velocity perturbation equations of general relativistic zero-pressure, irrotational, single-component fluid in a flat background coincide exactly with the ones known in Newton's theory. Here, we present the general relativistic second-order correction terms arising due to (i) pressure, (ii) multi-component, (iii) background curvature, and (iv) rotation. In case of multi-component zero-pressure, irrotational fluids under the flat background, we effectively do not have relativistic correction terms, thus the relativistic result again coincides with the Newtonian ones. In the other three cases we generally have pure general relativistic correction terms. In case of pressure, the relativistic corrections appear even in the level of background and linear perturbation equations. In the presence of background curvature, or rotation, pure relativistic correction terms directly appear in the Newtonian equations of motion of density and velocity perturbations to the second order. In the small-scale limit (far inside the horizon), relativistic equations including the rotation coincide with the ones in Newton's gravity.

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