High-redshift cosmography: auxiliary variables versus Padé polynomials

Salvatore Capozziello; Rocco D'Agostino; Orlando Luongo

doi:10.1093/mnras/staa871

paper

High-redshift cosmography: auxiliary variables versus Padé polynomials

arXiv:2003.09341 · doi:10.1093/mnras/staa871

Abstract

Cosmography becomes non-predictive when cosmic data span beyond the red shift limit $z ≃ 1$ . This leads to a \emph{strong convergence issue} that jeopardizes its viability. In this work, we critically compare the two main solutions of the convergence problem, i.e. the $y$ -parametrizations of the redshift and the alternatives to Taylor expansions based on Padé series. In particular, among several possibilities, we consider two widely adopted parametrizations, namely $y_{1} = 1 - a$ and $y_{2} = arctan (a^{- 1} - 1)$ , being $a$ the scale factor of the Universe. We find that the $y_{2}$ -parametrization performs relatively better than the $y_{1}$ -parametrization over the whole redshift domain. Even though $y_{2}$ overcomes the issues of $y_{1}$ , we get that the most viable approximations of the luminosity distance $d_{L} (z)$ are given in terms of Padé approximations. In order to check this result by means of cosmic data, we analyze the Padé approximations up to the fifth order, and compare these series with the corresponding $y$ -variables of the same orders. We investigate two distinct domains involving Monte Carlo analysis on the Pantheon Superovae Ia data, $H (z)$ and shift parameter measurements. We conclude that the (2,1) Padé approximation is statistically the optimal approach to explain low and high-redshift data, together with the fifth-order $y_{2}$ -parametrization. At high redshifts, the (3,2) Padé approximation cannot be fully excluded, while the (2,2) Padé one is essentially ruled out.

arXiv comment17 pages, 3 figures, to appear in MNRAS

High-redshift cosmography: auxiliary variables versus Padé polynomials

Abstract

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