The magnitude of the non-adiabatic pressure in the cosmic fluid
arXiv:1108.0639 · doi:10.1111/j.1365-2966.2012.20966.x
Abstract
Understanding the non-adiabatic pressure, or relative entropy, perturbation is crucial for studies of early-universe vorticity and Cosmic Microwave Background observations. We calculate the evolution of the linear non-adiabatic pressure perturbation from radiation domination to late times, numerically solving the linear governing equations for a wide range of wavenumbers. Using adiabatic initial conditions consistent with WMAP seven year data, we find nevertheless that the non-adiabatic pressure perturbation is non-zero and grows at early times, peaking around the epoch of matter/radiation equality and decaying in matter domination. At early times or large redshifts (z=10,000) its power spectrum peaks at a comoving wavenumber k~0.2h/Mpc, while at late times (z=500) it peaks at k~0.02 h/Mpc.
5 pages, 4 figures. Replaced with version accepted by MNRAS. One figure removed, added some discussion
References in corpus (6)
- Planck Early Results: The Planck mission
- The Cosmic Linear Anisotropy Solving System (CLASS) IV: Efficient implementation of non-cold relics
- Roles of dark energy perturbations in the dynamical dark energy models: Can we ignore them?
- Isocurvature modes and Baryon Acoustic Oscillations
- Estimating the amount of vorticity generated by cosmological perturbations in the early universe
- Cold Dark Matter Isocurvature Perturbations: Cosmological Constraints and Applications
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- Cosmological Perturbations: Vorticity, Isocurvature and Magnetic Fields