
Probing dark energy with baryonic oscillations and future radio surveys of neutral hydrogen
Author(s) -
Abdalla F. B.,
Rawlings S.
Publication year - 2005
Publication title -
monthly notices of the royal astronomical society
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.058
H-Index - 383
eISSN - 1365-2966
pISSN - 0035-8711
DOI - 10.1111/j.1365-2966.2005.08650.x
Subject(s) - physics , dark energy , cosmic microwave background , sky , redshift , astrophysics , baryon acoustic oscillations , baryon , cosmic cancer database , spectral density , galaxy , astronomy , radio telescope , planck , cosmology , optics , anisotropy , statistics , mathematics
Current surveys may be on the verge of measuring the baryonic oscillations in the galaxy power spectrum, which are clearly seen imprinted on the cosmic microwave background. It has recently been proposed that these oscillations allow a ‘standard ruler’ method of probing the equation of state of dark energy. In this paper we present a new calculation of the number of galaxies future radio telescopes will detect in surveys of the sky in neutral hydrogen (H i ). We estimate the likely statistical errors if the standard ruler method were to be applied to such surveys. We emphasize uncertainties in our calculations, and pinpoint the most important features of future H i surveys if they are to provide new constraints on dark energy via baryonic oscillations. Designs of future radio telescopes are required to have a large bandwidth (characterized by β, the ratio of the instantaneous bandwidth to the bandwidth required by survey) and to have the widest instantaneous (1.4 GHz) field of view (FOV) possible. Given the expected sensitivity of a future Square Kilometre Array (SKA), given that half of its collecting area will be concentrated in a core of diameter ∼5 km, and given a reasonable survey duration ( T 0 ∼ 1 yr) , we show that there will be negligible shot noise on a power spectrum derived from H i galaxies out to redshift z ≃ 1.5 . To access the largest cosmic volume possible by surveying all the sky available, we argue that β, T 0 and FOV must obey the relation β FOV T 0 ≳ 10 deg 2 yr . A ∼1‐yr SKA survey would then contain ≳ 10 9 ( f sky /0.5) H i galaxies and provide constraints on the dark energy parameter w of order Δ w ≃ 0.01 ( f sky /0.5) −0.5 , where f sky is the fraction of the whole sky observed.