Journal
MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
Volume 391, Issue 4, Pages 1499-1510Publisher
OXFORD UNIV PRESS
DOI: 10.1111/j.1365-2966.2008.13921.x
Keywords
quasars: absorption lines; quasars: individual: Q0913+072; cosmology: observations
Categories
Funding
- NASA Office of Space Science
- Australian Research Council [DP0877998]
- US National Science Foundation [AST-0606912]
- STFC [PP/E001068/1, PP/E00105X/1, ST/F001967/1] Funding Source: UKRI
- Science and Technology Facilities Council [PP/C001214/1, PP/E001068/1, ST/F001967/1, PP/E00105X/1] Funding Source: researchfish
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The most metal-poor damped Ly alpha system known to date, at z(abs) = 2.61843 in the spectrum of the QSO Q0913+072, with an oxygen abundance of only similar to 1/250 of the solar value, shows six well-resolved D (I) Lyman series transitions in high-quality echelle spectra recently obtained with the European Southern Observatory (ESO) VLT. We deduce a value of the deuterium abundance log (D/H) = -4.56 +/- 0.04 which is in good agreement with four out of the six most reliable previous determinations of this ratio in QSO absorbers. We find plausible reasons why in the other two cases the 1 sigma errors may have been underestimated by about a factor of two. The addition of this latest data point does not significantly change the mean value of the primordial abundance of deuterium, suggesting that we are now converging to a reliable measure of this quantity. We conclude that < log (D/H)(p)> = -4.55 +/- 0.03 and Omega(b,0)h(2)(BBN) = 0.0213 +/- 0.0010 (68 per cent confidence limits). Including the latter as a prior in the analysis of the Wilkinson Microwave Anisotropy Probe (WMAP) five-year data leads to a revised best-fitting value of the power-law index of primordial fluctuations n(s) = 0.956 +/- 0.013 (1 sigma) and n(s) < 0.990 with 99 per cent confidence. Considering together the constraints provided by WMAP 5, (D/H)(p), baryon oscillations in the galaxy distribution, and distances to Type Ia supernovae, we arrive at the current best estimates Omega(b,0)h(2) = 0.0224 +/- 0.0005 and n(s) = 0.959 +/- 0.013.
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