The Stability of the Cosmological System of Degenerate Scalar Charged Fermions and Higgs Scalar Fields. II. The Evolution of Short-Wave Perturbations
arXiv:2103.13867 · doi:10.1134/S0202289321010114
Abstract
A mathematical model of the evolution of plane perturbations in the cosmological statistical system of completely degenerate scalar-charged fermions with Higgs scalar interaction for short-wave perturbations is formulated. These disturbance modes have been found and investigated. It is shown that in such a model an additional oscillation mode arises, which is associated directly with degenerate fermions, in which monotonically decreasing and increasing perturbations of the metric exist. In this case, there is such a time instant in the system that the potential of the scalar field, together with the energy density, tends to infinity. In this regard, an assumption is made about a possible mechanism for the formation of dark matter condensates.
6 pages, 6 references, 4 figures
References in corpus (4)
- Statistical system with fantom scalar interaction. II. Macroscopic Equations and Cosmological Models
- Statistical system with a fantom scalar interaction in the Gravitation Theory. I. The Microscopic Dynamics
- The Method of Self-Consistent Field and Macroscopical Einstein Equations for the Early Universe
- Cosmological evolution of a scalar-charged degenerate cosmological plasma with Higgs scalar fields
Cited by in corpus (4)
- Cosmological Models Based on a Statistical System of Scalar Charged Degenerate Fermions and an Asymmetric Higgs Scalar Doublet
- Cosmological evolution of a statistical system of degenerate scalar-charged fermions with an asymmetric scalar doublet. I. Two-component system of assorted charges
- Gravitational - Scalar Instability of a Two-Component Degenerate System of Scalar Charged Fermions with Asymmetric Higgs Interaction
- Gravitational-Scalar Instability of a Cosmological Model Based on a Two-Component System of Degenerate Scalarly Charged Fermions with Asymmetric Higgs Interaction. I. Equations for Perturbations