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Revise the Dark Matter-Phantom Scalar Field Interaction
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abstract
The cosmological history and evolution are examined for gravitational models with interaction in the dark sector of the universe. In particular, we consider the dark energy to be described by a phantom scalar field and the dark matter $\rho _{m}$ as a pressureless ideal gas. We introduce the interacting function $Q=\beta \left( t\right) \rho_{m}$, where the function $% \beta \left( t\right) $ is considered to be proportional to $\dot{\phi}, \dot{\phi}^{2}H^{-1},~H$, or a constant parameter with dimensions of $\left[H_{0}\right] $. For the four interacting models, we study in details the phase space by calculating the stationary points. The latter are applied to reconstruct the cosmological evolution. Compactified variables are essential to understand the complete picture of the phase space and to conclude about the cosmological viability of these interacting models. The detailed analysis is performed for the exponential potential $V\left( \phi \right) =V_{0}e^{\lambda \phi }$. The effects of other scalar field potential functions on the cosmological dynamics are examined.
Forward citations
Cited by 2 Pith papers
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Observational Constraints on Scalar Field--Matter Interaction in Weyl Integrable Spacetime
A Weyl Integrable Spacetime model with one extra parameter fits current late-time cosmological data slightly better than Lambda-CDM, with weak to moderate statistical preference.
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Averaging Dynamics of Scalar Field-Matter Interacting Models in Anisotropic Universes: The Locally Rotationally Symmetric Bianchi I Spacetime
The authors apply averaging methods to classify late-time attractors for nine interacting dark sector models in Bianchi I cosmology, but the general interaction formula does not match the specific models analyzed.
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