2003MNRAS.345..480P


Query : 2003MNRAS.345..480P

2003MNRAS.345..480P - Mon. Not. R. Astron. Soc., 345, 480-496 (2003/October-3)

A homogeneous sample of sub-damped Lyman α systems - II. Statistical, kinematic and chemical properties.

PEROUX C., DESSAUGES-ZAVADSKY M., D'ODORICO S., KIM T.-S. and McMAHON R.G.

Abstract (from CDS):

Damped Lyman α systems (DLAs), with N (H i) > 2x1020 atom cm–2, observed in the spectra of quasars have allowed us to quantify the chemical content of the Universe over cosmological scales. Such studies can be extended to lower column densities, in the sub-DLA range [1019 < N (H i) < 2x1020 atom cm–2 ], which are systems believed to contain a large fraction of the neutral hydrogen at z > 3.5. In this paper, we use a homogeneous sample of sub-DLAs from the European Southern Oberservatory (ESO) Ultraviolet-Visual Echelle Spectrograph (UVES) archives presented in Paper I, to determine observationally for the first time the shape of the column density distribution, f (N), down to N (H i) 1019 atom cm–2. The results are in good agreement with the predictions from Péroux et al. We also present the kinematic and clustering properties of this survey of sub-DLAs, which appear to be marginally different from the DLAs. We compare low- and high-ionization transition widths and find that the properties of the sub-DLAs span roughly the parameter space of DLAs. We also find hints of an increase of metallicity in systems with larger velocity widths in the metal lines, although the statistical significance of this result is low.

Then we analyse the chemical content of this sample in conjunction with a compilation of abundances from 72 DLAs taken from the literature. As previously reported, the individual metallicities traced by [Fe/H] of these systems evolve mildly with redshift. Moreover, we analyse the H i column-density-weighted mean abundance, which is believed to be an indicator of the metallicity of the Universe. Although the number statistics is limited in the current sample, the results suggest a slightly stronger evolution of this quantity in the sub-DLA range. The effect is predominant at z < 2 and most of the evolution observed lies in this redshift range. Observational arguments support the hypothesis that the evolution we probe in the sub-DLA range is not due to their lower dust content. Therefore, these systems might be associated with a different class of objects, which better trace the overall chemical evolution of the Universe. Finally, we present abundance ratios of [Si/Fe], [O/Fe], [C/Fe] and [Al/Fe] for sub-DLAs in conjunction with DLA measurements from the literature. The elemental ratios in sub-DLAs are comparable with those from DLAs. It is difficult to decipher whether the observed values are the effect of nucleosynthesis or are due to differential dust depletion. The metallicities are compared with two different sets of models of galaxy evolution in order to provide constraints on the morphology of quasar absorbers.


Abstract Copyright: 2003 RAS

Journal keyword(s): galaxies: abundances - galaxies: evolution - galaxies: formation - galaxies: high-redshift - quasars: absorption lines - quasars: general

Simbad objects: 23

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Number of rows : 23
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 QSO J0003-2603 QSO 00 03 22.9531962024 -26 03 18.304471908   18 17.53     ~ 293 0
2 QSO J0307-4945 QSO 03 07 22.8949808808 -49 45 48.274545240     18.76     ~ 69 0
3 QSO B0347-383 QSO 03 49 43.6603590912 -38 10 30.825444900     17.3     ~ 196 0
4 QSO J0407-4410 QSO 04 07 18.0880236912 -44 10 13.983623724   17.6 17.6     ~ 103 1
5 QSO B0841+129 BLL 08 44 24.2445546984 +12 45 46.526286780   18.28 18.5     ~ 121 0
6 QSO B0940-1050 QSO 09 42 53.5078384704 -11 04 25.931336376   16.96 16.6 16.6   ~ 102 0
7 QSO B1038-2712 QSO 10 40 32.2200380808 -27 27 49.078018224   17.9 17.7     ~ 44 0
8 PG 1101-264 QSO 11 03 25.2993421704 -26 45 15.808554720   16.08 16.02     ~ 247 1
9 QSO B1104-181 QSO 11 06 33.3845199936 -18 21 23.829049296   15.8 15.9 15.7   ~ 338 1
10 QSO B1151+068 QSO 11 54 11.0745443880 +06 34 27.165655200     18.6     ~ 59 0
11 QSO B1157+014 QSO 11 59 44.8278142392 +01 12 06.985999764   17.87 17.52     ~ 228 1
12 LBQS 1223+1753 QSO 12 26 07.1946195816 +17 36 49.921603812   18.93 18.59     ~ 115 0
13 LBQS 1232+0815 QSO 12 34 37.5514444464 +07 58 43.367750796     18.4     ~ 128 0
14 QSO B1409+0930 QSO 14 12 17.2929417480 +09 16 24.707943048     18.6     ~ 65 0
15 LBQS 1444+0126 QSO 14 46 53.0501441856 +01 13 55.924449276   18.71 18.38     ~ 75 0
16 QSO B1451+123 QSO 14 54 18.5811696336 +12 10 53.897535696     18.6     ~ 88 0
17 QSO B1511+091 QSO 15 13 52.5256082976 +08 55 55.726612572   18.22 17.92     ~ 66 1
18 QSO B2059-360 QSO 21 02 44.6068720464 -35 53 07.081042308   19.18 18.62     ~ 58 0
19 QSO J2119-3536 QSO 21 19 27.6059083752 -35 37 40.547708544   17.50 17.35     ~ 45 0
20 LBQS 2132-4321 QSO 21 36 06.0041920008 -43 08 18.107819196   18.06 17.68     ~ 25 0
21 QSO J2155+1358 QSO 21 55 02.0017063296 +13 58 25.712205816     18.00     ~ 50 0
22 LBQS 2206-1958A QSO 22 08 52.0729138920 -19 43 59.866776948   17.49 17.33     ~ 223 0
23 QSO J2344+0342 QSO 23 44 03.1101598920 +03 42 26.725817304     18.20     ~ 51 0

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