Cosmological perturbations for imperfect fluids
arXiv:astro-ph/0504655 · doi:10.1088/0264-9381/22/24/004
Abstract
Interacting fluids, endowed with bulk viscous stresses, are discussed in a unified perspective with the aim of generalizing the treatment of cosmological perturbation theory to the case where both fluctuating decay rates and fluctuating bulk viscosity coefficients are simultaneously present in the relativistic plasma. A gauge-invariant treatment of the qualitatively new phenomena arising in this context is provided. In a complementary approach, faithful gauge-fixed descriptions of the gravitational and hydrodynamical fluctuations are developed and exploited. To deepen the interplay between bulk viscous stresses and fluctuating decay rates, illustrative examples are proposed and discussed both analytically and numerically. Particular attention is paid to the coupled evolution of curvature and entropy fluctuations when, in the relativistic plasma, at least one of the interacting fluids possesses a fluctuating bulk viscosity coefficient. It is argued that this class of models may be usefully employed as an effective description of the decay of the inflaton as well as of other phenomena involving imperfect relativistic fluids.
37 pages, 6 included figures; references added, corrected typos, few details added on specific derivations; title slightly changed
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- Why CMB physics?
- Non-linear curvature inhomogeneities and backreaction for relativistic viscous fluids
- Quasiadiabatic modes from viscous inhomogeneities
- Inflating without a flat potential: Viscous inflation
- Viscous modes, isocurvature perturbations and CMB initial conditions
- Covariant Evolution of Gravitoelectromagnetism