<> "The repository administrator has not yet configured an RDF license."^^ . <> . . "Quasar Environments at z ~ 4"^^ . "In the standard picture of structure formation, the first massive galaxies form in the highest peaks of the density field, which are the cores of massive proto-clusters. Such structures must be exceedingly rare, and thus hard to find. Luminous quasars (QSOs) at z ~ 4 are the most strongly clustered population in the Universe and this large auto-correlation demands that they reside in massive dark matter halos, associated with large overdensities of galaxies. This imply a strong QSO-galaxy cross-correlation for luminous QSOs at z ~ 4. \r\nIn order to put the first observational constrain on the QSO-galaxy clustering properties, I present the measurement of the cross-correlation function between QSOs and both Lyman break galaxies (LBGs) and Lyman alpha emitters (LAEs) at z ~ 4. \r\nI present VLT/FORS1 observations of 6 luminous QSOs fields. Using a novel narrow band filter technique I select LBGs associated with each quasar in a narrow redshift range of Δz ~ 0.2. I measure the QSO-LBG cross correlation function on scales of 0.1 < R < 10 h-1 Mpc (comoving), which is well fitted by a power law form with a correlation length r0 = 9.91+3.28-1.79 h-1 Mpc and a slope gamma = 2.05+0.20-0.46. This is in agreement with the theoretical expected clustering computed from the individual QSO and LBGs auto-correlation, assuming a linear bias model. I also measure the auto-correlation of LBGs in the QSO fields, which shows a stronger clustering in comparison with LBGs in random fields. \r\nThe new technique used for the detection of LBGs is efficient in selecting them in a thin redshift slice, but this shows important shortcomings whereby this result should be carefully considered.\r\nAdditionally, I present VLT/FORS2 observations of 14 luminous QSO fields, designed to search for LAEs in their environments. I find that QSOs and LAEs are not correlated at z ~ 4, and the mean LAEs number density in our fields is consistent with the expected number density in random fields. This could mean either that the QSO auto-correlation length at z ~ 4 is overestimated, or that LAEs preferentially avoid QSO environments on ≲10 Mpc h-1 scales."^^ . "2016" . . . . . . . "Cristina"^^ . "Garcia Vergara"^^ . "Cristina Garcia Vergara"^^ . . . . . . "Quasar Environments at z ~ 4 (Other)"^^ . . . . . . "preview.jpg"^^ . . . "Quasar Environments at z ~ 4 (Other)"^^ . . . . . . "medium.jpg"^^ . . . "Quasar Environments at z ~ 4 (Other)"^^ . . . . . . "small.jpg"^^ . . . "Quasar Environments at z ~ 4 (Other)"^^ . . . . . . "indexcodes.txt"^^ . . . "Quasar Environments at z ~ 4 (Other)"^^ . . . . . . "lightbox.jpg"^^ . . . "Quasar Environments at z ~ 4 (PDF)"^^ . . . "PhD_Thesis_Garcia2016_v01.pdf"^^ . . "HTML Summary of #20846 \n\nQuasar Environments at z ~ 4\n\n" . "text/html" . . . "520 Astronomie"@de . "520 Astronomy and allied sciences"@en . .