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Improved cosmological constraints on the curvature and equation of state of dark energy (1005.4249v2)

Published 24 May 2010 in astro-ph.CO, gr-qc, and hep-th

Abstract: We apply the Constitution compilation of 397 supernova Ia, the baryon acoustic oscillation measurements including the $A$ parameter, the distance ratio and the radial data, the five-year Wilkinson microwave anisotropy probe and the Hubble parameter data to study the geometry of the universe and the property of dark energy by using the popular Chevallier-Polarski-Linder and Jassal-Bagla-Padmanabhan parameterizations. We compare the simple $\chi2$ method of joined contour estimation and the Monte Carlo Markov chain method, and find that it is necessary to make the marginalized analysis on the error estimation. The probabilities of $\Omega_k$ and $w_a$ in the Chevallier-Polarski-Linder model are skew distributions, and the marginalized $1\sigma$ errors are $\Omega_m=0.279{+0.015}_{-0.008}$, $\Omega_k=0.005{+0.006}_{-0.011}$, $w_0=-1.05{+0.23}_{-0.06}$, and $w_a=0.5{+0.3}_{-1.5}$. For the Jassal-Bagla-Padmanabhan model, the marginalized $1\sigma$ errors are $\Omega_m=0.281{+0.015}_{-0.01}$, $\Omega_k=0.000{+0.007}_{-0.006}$, $w_0=-0.96{+0.25}_{-0.18}$, and $w_a=-0.6{+1.9}_{-1.6}$. The equation of state parameter $w(z)$ of dark energy is negative in the redshift range $0\le z\le 2$ at more than $3\sigma$ level. The flat $\Lambda$CDM model is consistent with the current observational data at the $1\sigma$ level.

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