The comoving mass density of MgII from to
arXiv:1708.00304 · doi:10.1093/mnras/stx1985
Abstract
We present the results of a survey for intervening MgII absorbers in the redshift range z 2-6 in the foreground of four high redshift quasar spectra, 5.796.133, obtained with the ESO VLT X-shooter. We identify 24 absorbers at significance in the equivalent width range 0.117$\le W_{2796}\le 3.655\unicode{xC5}$ with the highest redshift absorber at . For weak ($W_{2796}<0.3\unicode{xC5}$) systems, we measure an incidence rate =1.350.58 at <z>=2.34 and find that it almost doubles to =2.580.67 by <z>=4.81. Weak absorbers exceeds the number expected from an exponential fit to stronger systems ($W_{2796}>0.3\unicode{xC5}$). We find that there must be significant evolution in the absorption halo properties of MgII absorbers with $W_{2796} >0.1\unicode{xC5}$ by <z>=4.77 and/or that they are associated with galaxies with luminosities beyond the limits of the current luminosity function at z 5. We find that the incidence rate of strong MgII absorbers ($W_{2796}>1.0\unicode{xC5}$) can be explained if they are associated with galaxies with and/or their covering fraction increases. If they continue to only be associated with galaxies with then their physical cross section () increases from 0.015 Mpc at z=2.3 to 0.041 Mpc at <z>=4.77. We measure =2.1, 1.9, 3.9 at <z>=2.48, 3.41, 4.77, respectively. At <z>=4.77, exceeds the value expected from estimated from the global metallicity of DLAs at z 4.85 by a factor of 44 suggesting that either MgII absorbers trace both ionised and neutral gas and/or are more metal rich than the average DLA at this redshift.
32 pages, 22 figures, 9 tables, accepted for publication to MNRAS
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Cited by in corpus (9)
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