Abstract

In this paper, we consider the Universe at the late stage of its evolution and deep inside the cell of uniformity. At these scales, the Universe is filled with inhomogeneously distributed discrete structures (galaxies, groups and clusters of galaxies). Supposing that the Universe contains also the cosmological constant and a perfect fluid with a negative constant equation of state (EoS) parameter omega (e.g., quintessence, phantom or frustrated network of topological defects), we investigate scalar perturbations of the Friedmann–Robertson–Walker metrics due to inhomogeneities. Our analysis shows that, to be compatible with the theory of scalar perturbations, this perfect fluid, first, should be clustered and, second, should have the EoS parameter omega =-1/3. In particular, this value corresponds to the frustrated network of cosmic strings. Therefore, the frustrated network of domain walls with omega =-2/3 is ruled out. A perfect fluid with omega =-1/3 neither accelerates nor decelerates the Universe. We also obtain the equation for the nonrelativistic gravitational potential created by a system of inhomogeneities. Due to the perfect fluid with omega = -1/3, the physically reasonable solutions take place for flat, open and closed Universes. This perfect fluid is concentrated around the inhomogeneities and results in screening of the gravitational potential.

Highlights

  • It is well known that frustrated networks of topological defects have the form of perfect fluids with the constant parameter ω [14,16,17,18]

  • We have considered the perfect fluids with the constant negative parameter ω of the equation of state (EoS)

  • We have investigated the role of these fluids for the Universe at late stages of its evolution

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Summary

Introduction

One of the main tasks of the present paper is to study a possibility to get a reasonable form of gravitational potentials in the models with an additional perfect fluid with constant negative ω. If such potentials exist, we can study the relative motion of galaxies in the field of these potentials and compare it with the corresponding motion in the CDM model [29]. 2, we consider scalar perturbations in the Friedmann Universe filled with the cosmological constant, pressureless dustlike matter (baryon and dark matter) and perfect fluid with negative constant EoS. The main results are summarized in the concluding Sect. 4

Homogeneous background
Scalar perturbations
Gravitational potentials
Conclusion
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