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Novel approach towards the large-scale stable Interacting Dark-Energy models and their Astronomical Bounds

Weiqiang Yang, Supriya Pan, David F. Mota

TL;DR

This work introduces a novel dark-sector coupling $Q = \xi \dot{\rho}_x$ that unifies stability regions for interacting dark energy, and analyzes both constant and CPL-dynamical equations of state. Through background and perturbation analyses, it shows that a nonzero coupling is allowed and that $w_x$ can be phantom-like, yet $\xi=0$ remains compatible within 1$\sigma$, with models closely mimicking $\Lambda$CDM in many observables. Using Planck, BAO, JLA, WL, RSD, CC, and Riess $H_0$ priors, the paper constrains the model parameters and finds potential alleviation of the $H_0$ tension for certain phantom-region priors, while noting that very strong phantom behavior could reintroduce tensions. Overall, the approach provides a testable, unified framework for interacting dark energy that remains compatible with current data and offers insights into the $H_0$ discrepancy.

Abstract

Stability analysis of interacting dark energy models generally divides its parameters space into two regions: (i) $w_x \geq -1$ and $ξ\geq 0$ and (ii) $w_x \leq -1$ and $ξ\leq 0$, where $w_x$ is the dark energy equation of state and $ξ$ is the coupling strength of the interaction. Due to this separation, crucial information about the cosmology and phenomenology of these models may be lost. In a recent study it has been shown that one can unify the two regions with a coupling function which depends on the dark energy equation of state. In this work we introduce a new coupling function which also unifies the two regions of the parameter space and generalises the previous proposal. We analyse this scenario considering the equation of state of DE to be either constant or dynamical. We study the cosmology of such models and constrain both scenarios with the use of latest astronomical data from both background evolution as well as large scale structures. Our analysis shows that a non-zero value of the coupling parameter $ξ$ as well as the dark energy equation of state other than `$-1$' are allowed. However, within $1σ$ confidence level, $ξ= 0$, and the dark energy equation of state equal to `$-1$' are compatible with the current data. In other words, the observational data allow a very small but nonzero deviation from the $Λ$-cosmology, however, within $1σ$ confidence-region the interacting models can mimick the $Λ$-cosmology. In fact we observe that the models both at background and perturbative levels are very hard to distinguish form each other and from $Λ$-cosmology as well. Finally, we offer a rigorous analysis on the current tension on $H_0$ allowing different regions of the dark energy equation of state which shows that interacting dark energy models reasonably solve the current tension on $H_0$.

Novel approach towards the large-scale stable Interacting Dark-Energy models and their Astronomical Bounds

TL;DR

This work introduces a novel dark-sector coupling that unifies stability regions for interacting dark energy, and analyzes both constant and CPL-dynamical equations of state. Through background and perturbation analyses, it shows that a nonzero coupling is allowed and that can be phantom-like, yet remains compatible within 1, with models closely mimicking CDM in many observables. Using Planck, BAO, JLA, WL, RSD, CC, and Riess priors, the paper constrains the model parameters and finds potential alleviation of the tension for certain phantom-region priors, while noting that very strong phantom behavior could reintroduce tensions. Overall, the approach provides a testable, unified framework for interacting dark energy that remains compatible with current data and offers insights into the discrepancy.

Abstract

Stability analysis of interacting dark energy models generally divides its parameters space into two regions: (i) and and (ii) and , where is the dark energy equation of state and is the coupling strength of the interaction. Due to this separation, crucial information about the cosmology and phenomenology of these models may be lost. In a recent study it has been shown that one can unify the two regions with a coupling function which depends on the dark energy equation of state. In this work we introduce a new coupling function which also unifies the two regions of the parameter space and generalises the previous proposal. We analyse this scenario considering the equation of state of DE to be either constant or dynamical. We study the cosmology of such models and constrain both scenarios with the use of latest astronomical data from both background evolution as well as large scale structures. Our analysis shows that a non-zero value of the coupling parameter as well as the dark energy equation of state other than `' are allowed. However, within confidence level, , and the dark energy equation of state equal to `' are compatible with the current data. In other words, the observational data allow a very small but nonzero deviation from the -cosmology, however, within confidence-region the interacting models can mimick the -cosmology. In fact we observe that the models both at background and perturbative levels are very hard to distinguish form each other and from -cosmology as well. Finally, we offer a rigorous analysis on the current tension on allowing different regions of the dark energy equation of state which shows that interacting dark energy models reasonably solve the current tension on .

Paper Structure

This paper contains 10 sections, 15 equations, 12 figures, 3 tables.

Figures (12)

  • Figure 1: 68.3% and 95.4% confidence-level contour plots for different combinations of the free parameters of IDE 1 have been shown for the combined analysis Planck TT, TE, EE $+$ lowTEB $+$ BAO $+$ JLA $+$ RSD $+$ WL $+$ CC $+$ R16.
  • Figure 2: The plots show the angular CMB termperature anisotropy spectra for IDE 1 over the standard $\Lambda$CDM cosmology using the joint analysis data Planck TT, TE, EE $+$ lowTEB $+$ BAO $+$ JLA $+$ RSD $+$ WL $+$ CC $+$ R16. In the left panel we have varied the constant EoS $w_x$ while the right panel stands for diferent values of the coupling parameter $\xi$. We note that the curves in the right panel are so close to each other such that they are practically indistinguishable from each other.
  • Figure 3: For different coupling parameters, we show the evolutions of $\mathcal{H}_{eff}/\mathcal{H}$ (left panel) and $G_{eff}/G$ (right panel) for the interacting dark energy model with constant $w_x$. The deviation is measured from the non-interacting scenario (i.e. $\xi =0$) and also from the mean value of $\xi = -0.1690$ obtained from the combined analysis Planck TT, TE, EE $+$ lowTEB $+$ BAO $+$ JLA $+$ RSD $+$ WL $+$ CC $+$ R16.
  • Figure 4: MCMC samples in the $(w_x, \xi)$ plane coloured by the Hubble constant value $H_0$ for IDE 1 analyzed with the combined analysis Planck TT, TE, EE $+$ lowTEB $+$ BAO $+$ JLA $+$ RSD $+$ WL $+$ CC $+$ R16.
  • Figure 5: 68.3% and 95.4% confidence-level contour plots for different combinations of the free parameters of IDE 2 have been shown for the combined analysis Planck TT, TE, EE $+$ lowTEB $+$ BAO $+$ JLA $+$ RSD $+$ WL $+$ CC $+$ R16.
  • ...and 7 more figures