178 research outputs found

    Correlation of Low z Lyman-alpha Absorbers with HI-selected Galaxies

    Full text link
    In this work, observational evidence for the connection between low column density Lyman-alpha absorbers and large-scale structure traced by gas-rich galaxies is investigated. The HI Parkes All Sky Survey (HIPASS) galaxy catalogue is cross-correlated with known low redshift, low column density Lyman-alpha absorbers from the literature. The absorber-galaxy cross-correlation function shows that on scales from 1 to 10 h^-1 Mpc, absorbers are imbedded in halos with masses similar to that of galaxy groups. This statistical evidence suggests that galaxy groups could be the dominant environment of low column density Lyman-alpha absorbers at z=0.Comment: 3 pages, 1 figure, to appear in IAU 199 conf. proc.: "Probing Galaxies through Quasar Absorption Lines," eds. Williams, Shu, Menar

    Cross correlation of Lyman-alpha absorbers with gas-rich galaxies

    Full text link
    The HI Parkes All Sky Survey (HIPASS) galaxy catalogue is cross-correlated with known low redshift, low column density (N_HI <10^15 cm^-2) Lyman-alpha absorbers from the literature. The redshift-space correlation is found to be similar in strength to HIPASS galaxy self-clustering (correlation length s_0,ag=6+/-4 and s_0,gg=3.1+/-0.5 h^-1 Mpc respectively). In real-space the cross-correlation is stronger than the galaxy auto-correlation (correlation length r_0,ag=7.2+/-1.4 and r_0,gg=3.5+/-0.7 h^-1 Mpc respectively) on scales from 1-10 h^-1 Mpc, ruling out the mini-halo model for the confinement Lyman-alpha absorbers at the 99 percent confidence level. Provided that the cause of the strong cross-correlation is purely gravitational, the ratio of correlation lengths suggest that absorbers are embedded in dark matter haloes with masses log(M/Msun)=14.2 h^-1, similar to those of galaxy groups. The flattening of the cross-correlation at separations less than ~600 h^-1 kpc could correspond to the thickness of filaments in which absorbers are embedded. This work provides indirect statistical evidence for the notion that galaxy groups and large-scale filaments, particularly those that comprise gas-rich galaxies, are the dominant environments of low column density Lyman-alpha absorbers at z=0.Comment: 10 pages, 10 figures, accepted for publication in MNRAS, minor typos fixed and references update

    Evolution of damped Lyman alpha kinematics and the effect of spatial resolution on 21-cm measurements

    Full text link
    We have investigated the effect of spatial resolution on determining pencil-beam like velocity widths and column densities in galaxies. Three 21-cm datasets are used, the HIPASS galaxy catalogue, a subset of HIPASS galaxies with ATCA maps and a high-resolution image of the LMC. Velocity widths measured from 21-cm emission in local galaxies are compared with those measured in intermediate redshift Damped Lyman alpha (DLA) absorbers. We conclude that spatial resolution has a severe effect on measuring pencil-beam like velocity widths in galaxies. Spatial smoothing by a factor of 240 is shown to increase the median velocity width by a factor of two. Thus any difference between velocity widths measured from global profiles or low spatial resolution 21-cm maps at z=0 and DLAs at z>1 cannot unambiguously be attributed to galaxy evolution. The effect on column density measurements is less severe and the values of dN/dz from local low-resolution 21-cm measurements are expected to be overestimated by only ~10 per cent.Comment: 5 pages, 6 figures, accepted for publication in MNRAS letter

    Intergalactic CIV absorption at redshifts 5.4 to 6

    Get PDF
    We report the discovery of a strong CIV 1548,1550 absorption system at z_abs = 5.7238 in the near-infrared spectrum (J-band) of the z_em = 6.28 QSO SDSS J1030+0524. These observations, obtained with the Infrared Spectrometer And Array Camera (ISAAC) on the European Southern Observatory Very Large Telescope (ESO VLT), demonstrate that, with modern instrumentation, QSO absorption line spectroscopy can be successfully extended to near-infrared wavelengths to probe the intergalactic medium near the end of the reionization epoch. Although the statistics of this pilot study are limited, the mass density of triply ionized carbon implied by our data is comparable to the values of Omega_CIV reported at lower redshifts. Neither the column density distribution of CIV absorbers nor its integral show significant redshift evolution over a period of time which stretches from 1 to 4.5 Gyr after the big bang, suggesting that a large fraction of intergalactic metals may already have been in place at redshifts above 6. Alternatively, the strong CIV system we have detected may be associated with outflowing, highly-ionized, gas from a foreground massive galaxy; deep imaging and spectroscopy of galaxies near the QSO sightline should be able to distinguish between these two possibilities.Comment: 6 pages, 2 figures, accepted for publication in MNRAS on June 28t

    The host galaxies of strong CaII QSO absorption systems at z<0.5

    Full text link
    We present new imaging and spectroscopic observations of the fields of five QSOs with very strong intervening CaII absorption systems at redshifts z<0.5 selected from the Sloan Digital Sky Survey. Recent studies of these very rare absorbers indicate that they may be related to damped Lyman alpha systems (DLAs). In all five cases we identify a galaxy at the redshift of the CaII system with impact parameters up to ~24 kpc. In four out of five cases the galaxies are luminous (L ~L*), metal-rich (Z ~Zsun), massive (velocity dispersion, sigma ~100 km/s) spirals. Their star formation rates, deduced from Halpha emission, are high, in the range SFR = 0.3 - 30 Msun/yr. In our analysis, we paid particular attention to correcting the observed emission line fluxes for stellar absorption and dust extinction. We show that these effects are important for a correct SFR estimate; their neglect in previous low-z studies of DLA-selected galaxies has probably led to an underestimate of the star formation activity in at least some DLA hosts. We discuss possible links between CaII-selected galaxies and DLAs and outline future observations which will help clarify the relationship between these different classes of QSO absorbers.Comment: Accepted for publication in MNRAS, 14 pages, 9 figures. Version with full resolution images available at http://www.ast.cam.ac.uk/~bjz/papers/Zych_etal_2007a.pd

    Probing the nature of dark matter through the metal enrichment of the intergalactic medium

    Get PDF
    We focus on exploring the metal enrichment of the intergalactic medium (IGM) in cold and warm (1.5 and 3 keV) dark matter (DM) cosmologies, and the constraints this yields on the DM particle mass, using a semi-analytic model, DELPHI, that jointly tracks the DM and baryonic assembly of galaxies at z similar or equal to 4-20 including both supernova (SN) and (a range of) reionization feedback (models). We find that while M-UV greater than or similar to -15 galaxies contribute half of all IGM metals in the cold dark matter (CDM) model by z similar or equal to 4.5, given the suppression of low-mass haloes, larger haloes with M-UV greater than or similar to -15 provide about 80 per cent of the IGM metal budget in 1.5 keV warm dark matter (WDM) models using two different models for the metallicity of the interstellar medium. Our results also show that the only models compatible with two different high-redshift data sets, provided by the evolving ultraviolet luminosity function (UV LF) at z similar or equal to 6-10 and IGM metal density, are standard CDM and 3 keV WDM that do not include any reionization feedback; a combination of the UV LF and the Diaz et al. point provides a weaker constraint, allowing CDM and 3 and 1.5 keV WDM models with SN feedback only, as well as CDM with complete gas suppression of all haloes with v(circ) less than or similar to 30 km s(-1). Tightening the error bars on the IGM metal enrichment, future observations, at z greater than or similar to 5.5, could therefore represent an alternative way of shedding light on the nature of DM

    The CGM and IGM at z\sim5: metal budget and physical connection

    Full text link
    We present further results of a survey for absorption line systems in the spectra of four high redshift quasars (5.79 \le zem_{\textrm{em}} \le 6.13) obtained with the ESO Very Large Telescope X-Shooter. We identify 36 CIV\textrm{CIV} and 7 SiIV\textrm{SiIV} systems with a \ge 5σ\sigma significance. The highest redshift CIV\textrm{CIV} and SiIV\textrm{SiIV} absorbers identified in this work are at z = 5.80738 ±\pm 0.00017 and z = 5.77495 ±\pm 0.00038, respectively. We compute the comoving mass density of SiIV\textrm{SiIV} (ΩSiIV\Omega_{\textrm{SiIV}}) and find that it evolves from ΩSiIV\Omega_{\textrm{SiIV}} = 4.32.1+2.1^{+2.1}_{-2.1} ×\times109^{-9} at = 5.05 to ΩSiIV\Omega_{\textrm{SiIV}} = 1.40.4+0.6^{+0.6}_{-0.4} ×\times109^{-9} at = 5.66. We also measure ΩCIV\Omega_{\textrm{CIV}} = 1.60.1+0.4^{+0.4}_{-0.1} ×\times108^{-8} at = 4.77 and ΩCIV\Omega_{\textrm{CIV}} = 3.41.1+1.6^{+1.6}_{-1.1} ×\times109^{-9} at = 5.66. We classify our CIV\textrm{CIV} absorber population by the presence of associated low\textit{low} and/or high ionisation\textit{high ionisation} systems and compute their velocity width (Δ\Deltav90_{90}). We find that all CIV\textrm{CIV} systems with Δ\Deltav90_{90} > 200 kms1^{-1} have associated low ionisation\textit{low ionisation} systems. We investigate two such systems, separated by 550 physical kpc along a line of sight, and find it likely that they are both tracing a multi-phase medium where hot and cold gas is mixing at the interface between the CGM and IGM. We further discuss the \textrm{MgII} systems presented in a previous work and we identify 5 SiII\textrm{SiII}, 10 AlII\textrm{AlII}, 12 FeII\textrm{FeII}, 1 CII\textrm{CII}, 7 MgI\textrm{MgI} and 1 CaII\textrm{CaII} associated transitions. We compute the respective comoving mass densities in the redshift range 2 to 6, as allowed by the wavelength coverage.Comment: Accepted for publication in MNRAS 22 pages, 19 figures, 6 table
    corecore