corner
corner

Phys. Rev. D 73, 084024 (2006) [10 pages]

Confronting braneworld cosmology with supernova data and baryon oscillations

Download: PDF (335 kB) Buy this article Export: BibTeX or EndNote (RIS)

Ujjaini Alam1,2 and Varun Sahni1
1Inter-University Centre for Astronomy and Astrophysics, Post Bag 4, Ganeshkhind Pune 411 007, India
2International Centre for Theoretical Physics, Strada Costiera 11, 34100 Trieste, Italy

Received 24 November 2005; published 24 April 2006

Braneworld cosmology has several attractive and distinctive features. For instance the effective equation of state in braneworld models can be both quintessencelike (w0≥-1) as well as phantomlike (w0≤-1). Models with w0≥-1 (w0≤-1) are referred to as Brane 2 (Brane 1) and correspond to complementary embeddings of the brane in the bulk. (The equation of state in Brane 1 can successfully cross the “phantom divide“ at w=-1.) In this paper we compare the predictions of braneworld models to two recently released supernova data sets: the “Gold” data (Riess et al., 2004) and the data from the Supernova Legacy Survey (SNLS) (Astier et al., 2005). We also incorporate the recent discovery of the baryon acoustic peak in the Sloan Digital Sky Survey (Eisenstein et al., 2005) into our analysis. Our main results are that braneworld models satisfy both sets of SNe data. Brane 1 (with w0≤-1) shows very good agreement with data for values of the matter density bounded from below: Ω0m≳0.25 (Gold) and Ω0m≳0.2 (SNLS). On the other hand Brane 2 (with w0≥-1) shows excellent agreement with data for values of the matter density which are bounded from above: Ω0m≲0.45 (Gold) and Ω0m≲0.35 (SNLS). The DGP model is excluded at 3σ by SNLS and at 1σ by the Gold dataset. Braneworld models with future “quiescent” singularities (at which the Hubble parameter and the matter density remain finite but higher derivatives of the expansion factor diverge) are excluded by both datasets.

© 2006 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevD.73.084024
DOI:
10.1103/PhysRevD.73.084024
PACS:
04.50.+h, 98.80.−k