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    Spotting stasis in cosmological perturbations

    Keith R. Dienes1,2,*, Lucien Heurtier3,†, Daniel Hoover4,‡, Fei Huang5,§, Anna Paulsen6,∥, and Brooks Thomas4,¶

    • *Contact author: dienes@arizona.edu
    • †Contact author: lucien.heurtier@kcl.ac.uk
    • ‡Contact author: hooverdj@lafayette.edu
    • §Contact author: fei.huang@weizmann.ac.il
    • ∥Contact author: anna_paulsen@brown.edu
    • Contact author: thomasbd@lafayette.edu

    Phys. Rev. D 114, 043554 – Published 31 August, 2026

    DOI: https://doi.org/10.1103/v1m8-q29c

    Abstract

    As discussed in a number of recent papers, cosmological stasis is a phenomenon wherein the abundances of multiple cosmological energy components with different equations of state remain constant for an extended period despite the expansion of the universe. One of the most intriguing aspects of the stasis phenomenon is that it can give rise to cosmological epochs in which the effective equation-of-state parameter ⟨w⟩ for the universe is constant but differs from the canonical values associated with matter, radiation, vacuum energy, etc. Indeed, during such a stasis epoch, the spatial average of the energy density of the universe evolves in precisely the same manner as it would have evolved if the universe were instead dominated by a perfect fluid with an equation-of-state parameter equal to ⟨w⟩. However, as we shall demonstrate, this equivalence is broken at the level of the perturbations of the energy density. To illustrate this point, we consider a stasis epoch involving matter and radiation and demonstrate that within this stasis background the density perturbations associated with a spectator matter component with exceedingly small energy density exhibit a power-law growth that persists across the entire duration of the stasis epoch. This growth can potentially lead to significant enhancements of structure at small scales. Such enhancements are not only interesting in their own right but may also provide a way of observationally distinguishing between a stasis epoch and an epoch of perfect-fluid domination—even if the universe has the same equation of state in both cases.

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