Gauge-invariant cosmological perturbations

1980 Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields 2,237 citations

Abstract

The physical interpretation of perturbations of homogeneous, isotropic cosmological models in the early Universe, when the perturbation is larger than the particle horizon, is clarified by defining a complete set of gauge-invariant variables. The linearized perturbation equations written in these variables are simpler than the usual versions, and easily accommodate an arbitrary background equation of state, entropy perturbations, and anisotropic pressure perturbations. Particular attention is paid to how a scalar (density) perturbation might be generated by stress perturbations at very early times, when the non-gauge-invariant perturbation in the density itself is ill-defined. The amplitude of the fractional energy density perturbation at the particle horizon cannot be larger, in order of magnitude, than the maximum ratio of the stress perturbation to the background energy density at any earlier time, unless the perturbation is inherent in the initial singularity.

Keywords

PhysicsPerturbation (astronomy)Cosmological perturbation theoryClassical mechanicsIsotropyMathematical physicsAmplitudeInvariant (physics)Quantum mechanicsCosmology

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Publication Info

Year
1980
Type
article
Volume
22
Issue
8
Pages
1882-1905
Citations
2237
Access
Closed

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J. Bardeen (1980). Gauge-invariant cosmological perturbations. Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields , 22 (8) , 1882-1905. https://doi.org/10.1103/physrevd.22.1882

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DOI
10.1103/physrevd.22.1882