Abstract
In brane-world cosmologies of Randall-Sundrum type, we show that the evolution of large-scale curvature
perturbations may be determined on the brane, without solving the bulk perturbation equations. The influence
of the bulk gravitational field on the brane is felt through a projected Weyl tensor which behaves effectively
like an imperfect radiation fluid with anisotropic stress. We define curvature perturbations on uniform density
surfaces for both the matter and Weyl fluids, and show that their evolution on large scales follows directly from
the energy conservation equations for each fluid. The total curvature perturbation is not necessarily constant for
adiabatic matter perturbations, but can change due to the Weyl entropy perturbation. To relate this curvature
perturbation to the longitudinal gauge metric potentials requires knowledge of the Weyl anisotropic stress
which is not determined by the equations on the brane. We discuss the implications for large-angle anisotropies
on the cosmic microwave background sky.
Original language | English |
---|---|
Article number | 084009 |
Pages (from-to) | 084009 |
Journal | Physical Review D |
Volume | 63 |
Issue number | 8 |
Early online date | 16 Mar 2001 |
DOIs | |
Publication status | Published - 15 Apr 2001 |