On the stability of relativistic perfect fluids with linear equations of state where
arXiv:2209.06982 · doi:10.1007/s11005-023-01722-7
Abstract
For , we consider the stability of two distinct families of spatially homogeneous solutions to the relativistic Euler equations with a linear equation of state on exponentially expanding FLRW spacetimes. The two families are distinguished by one being spatially isotropic while the other is not. We establish the future stability of nonlinear perturbations of the non-isotropic family for the full range of parameter values , which improves a previous stability result established by the second author that required to lie in the restricted range . As a first step towards understanding the behaviour of nonlinear perturbations of the isotropic family, we construct numerical solutions to the relativistic Euler equations under a -symmetry assumption. These solutions are generated from initial data at a fixed time that is chosen to be suitably close to the initial data of an isotropic solution. Our numerical results reveal that, for the full parameter range , the density contrast associated to a nonlinear perturbation of an isotropic solution develops steep gradients near a finite number of spatial points where it becomes unbounded at future timelike infinity. This behaviour, anticipated by Rendall in \cite{Rendall:2004}, is of particular interest since it is not consistent with the standard picture for inflation in cosmology.
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- The Stability of Relativistic Fluids in Linearly Expanding Cosmologies
- Localized big bang stability for the Einstein-scalar field equations
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