EDP Sciences
Free Access
Volume 429, Number 3, January III 2005
Page(s) 807 - 818
Section Cosmology (including clusters of galaxies)
DOI https://doi.org/10.1051/0004-6361:20041168
Published online 05 January 2005

A&A 429, 807-818 (2005)
DOI: 10.1051/0004-6361:20041168

Cosmological parameters from supernova observations: A critical comparison of three data sets

T. R. Choudhury1 and T. Padmanabhan2

1  SISSA/ISAS, via Beirut 2-4, 34014 Trieste, Italy
    e-mail: chou@sissa.it
2  IUCAA, Ganeshkhind, Pune, 411 007, India
    e-mail: nabhan@iucaa.ernet.in

(Received 27 April 2004 / Accepted 15 September 2004 )

We extend our previous analysis of cosmological supernova type Ia data (Padmanabhan & Choudhury 2003) to include three recent compilation of data sets. Our analysis ignores the possible correlations and systematic effects present in the data and concentrates mostly on some key theoretical issues. Among the three data sets, the first set consists of 194 points obtained from various observations while the second discards some of the points from the first one because of large uncertainties and thus consists of 142 points. The third data set is obtained from the second by adding the latest 14 points observed through HST. A careful comparison of these different data sets help us to draw the following conclusions: (i) All the three data sets strongly rule out non-accelerating models. Interestingly, the first and the second data sets favour a closed universe; if  $\Omega_{\rm tot}\equiv \Omega_{\rm m}+\Omega_{\Lambda}$, then the probability of obtaining models with  $\Omega_{\rm tot} > 1$ is $\ga$ 0.97. Hence these data sets are in mild disagreement with the "concordance" flat model. However, this disagreement is reduced (the probability of obtaining models with  $\Omega_{\rm tot} > 1$ being  $\approx$ 0.9) for the third data set, which includes the most recent points observed by HST around  1 < z < 1.6. (ii) When the first data set is divided into two separate subsets consisting of low ( z < 0.34) and high ( z > 0.34) redshift supernova, it turns out that these two subsets, individually, admit non-accelerating models with zero dark energy because of different magnitude zero-point values for the different subsets. This can also be seen when the data is analysed while allowing for possibly different magnitude zero-points for the two redshift subsets. However, the non-accelerating models seem to be ruled out using only the low redshift data for the other two data sets, which have less uncertainties. (iii) We have also found that it is quite difficult to measure the evolution of the dark energy equation of state  wX(z) though its present value can be constrained quite well. The best-fit value seems to mildly favour a dark energy component with current equation of state  wX < -1, thus opening the possibility of existence of more exotic forms of matter. However, the data is still consistent with the the standard cosmological constant at 99 per cent confidence level for  $\Omega_{\rm m} \ga 0.2$.

Key words: supernovae: general -- cosmology: miscellaneous -- cosmological parameters

© ESO 2005

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