The case for dynamical dark energy revisited
Ujjaini Alam, Varun Sahni, A. A. Starobinsky
TL;DR
The paper investigates whether dark energy is dynamical by performing a model-independent reconstruction of the expansion history $H(z)$ in a flat universe, using a flexible ansatz to relate $H(z)$, $ ho_{DE}$, and the equation of state $w(z)$. By fitting to the Riess et al. Gold supernova sample and incorporating CMB information, the authors find that, without priors on $\,Ω_{0m}$ and $h$, evolving dark energy ($w_0<-1$ today) provides a better fit than ΛCDM, with a transition from deceleration to acceleration around $z_T≈0.39$. When ΛCDM-based CMB priors are imposed, the inferred evolution weakens, yielding $z_T≈0.57$ and $w_0$ closer to −1, implying a closer alignment with ΛCDM. The results show strong dependence on the SN data sampling and priors, highlighting the need for more high-redshift data and independent constraints on $\,Ω_{0m}$ and $h$ to robustly determine the nature of dark energy.
Abstract
We investigate the behaviour of dark energy using the recently released supernova data of Riess et al ~(2004) and a model independent parameterization for dark energy (DE). We find that, if no priors are imposed on $Ω_{0m}$ and $h$, DE which evolves with time provides a better fit to the SNe data than $Λ$CDM. This is also true if we include results from the WMAP CMB data. From a joint analysis of SNe+CMB, the best-fit DE model has $w_0 < -1$ at the present epoch and the transition from deceleration to acceleration occurs at $z_T = 0.39 \pm 0.03$. However, DE evolution becomes weaker if the $Λ$CDM based CMB results $Ω_{0m} = 0.27 \pm 0.04$, $h = 0.71 \pm 0.06$ are incorporated in the analysis. In this case, $z_T = 0.57 \pm 0.07$. Our results also show that the extent of DE evolution is sensitive to the manner in which the supernova data is sampled.
