Volume 556, August 2013
|Number of page(s)||20|
|Published online||09 August 2013|
The ESO UVES advanced data products quasar sample
II. Cosmological evolution of the neutral gas mass density⋆
Aix Marseille Université, CNRS, LAM (Laboratoire d’Astrophysique de
Marseille) UMR 7326, 13388
2 International Centre for Radio Astronomy Research (ICRAR), The University of Western Australia, 35 Stirling Hwy, WA 6009 Crawley, Australia
3 Department of Astronomy, Ohio State University, 140 West 18th Avenue, Columbus, OH 43210-1173, USA
Accepted: 1 July 2013
Damped absorbers, seen in the spectra of background quasars, are unique probes to select H i-rich galaxies. These galaxies allow one to estimate the neutral gas mass over cosmological scales. The neutral gas mass is a possible indicator of gas consumption as star formation proceeds. The damped Lyα absorbers (DLAs; NH I ≥ 2 × 1020 cm-2) and sub-DLAs (1019 ≤ NH I ≤ 2 × 1020 cm-2) are believed to contain a large fraction of neutral gas mass in the Universe. In Paper I of the series, we presented the results of a search for DLAs and sub-DLAs in the European Southern Observatory (ESO) Ultraviolet Visual Echelle Spectrograph (UVES) advanced data products dataset of 250 quasars. Here we use an unbiased subsample of sub-DLAs from this dataset to derive their statistical properties. We built a subset of 122 quasars ranging from 1.5 < zem < 5.0, suitable for statistical analysis. The statistical sample was analyzed in conjunction with other sub-DLA samples from the literature. This resulted in a combined sample of 89 sub-DLAs over a redshift path of Δz = 193. We derived the redshift evolution of the number density and the line density for sub-DLAs and compared them with the Lyman-limit systems (LLSs) and DLA measurements from the literature. The results indicate that these three classes of absorbers are evolving in the redshift interval 1.0 < z < 5.0. Thanks to the ESO UVES advanced data products data, we were able to determine the column density distribution, fH I(N,z), down to the sub-DLA limit. The flattening of fH I(N,z) in the sub-DLA regime is present in the observations. The redshift evolution of fH I(N,z) down to log NH I = 19.0 cm-2 is also presented, indicating that there are more sub-DLAs at high redshift than at low redshift. fH I(N,z) was also used to determine the neutral gas mass density, Ωg, at 1.5 < z < 5.0. The complete sample shows that sub-DLAs contribute 8–20% to the total Ωg from 1.5 < z < 5.0. In agreement with previous studies, no evolution of Ωg was observed from low to high redshift (i.e., 1.5 < z < 5.0), suggesting that star formation alone cannot explain this non-evolution and replenishment of gas and that recombination of ionized gas is needed.
Key words: galaxies: abundances / galaxies: evolution / galaxies: high-redshift / quasars: absorption lines / quasars: general
Table 1 and Appendix are available in electronic form at http://www.aanda.org
© ESO, 2013
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