The second year project came about when examining a particular C IV system at z=1.937294 toward the quasar PG 1222+228 (z=2.038). In the Keck I/HIRES spectra, I also detected transitions from Si II, Si IV, Al II, and Al III. The velocity distribution of gas revealed something very striking - one absorption component showed Si II and no Al II or Al III, while another only 15 km/s away, showed just the opposite. The only way this would be possible is through an abundance variation in a system. It was an interesting result and marked the time our group attempted to understand the physical conditions of an absorption system. In a broader context, we had taken a step toward examining individual leaves in a tree of the Lyman alpha forest.
I continued studying these C IV systems and found a few that I simply could not understand. In the effort to fit C IV profiles to obtain column densities, I found a subset where the optical depth ratio was not 2:1 as expected for unsaturated doublets. The reason for this, and the subject of Chapter 2, is partial coverage of the background quasar. (One of these systems was again toward PG 1222+228, and so, this quasar will always find special place with me.) This began my descent to the ``darker side'' of quasar absorption line research - absorption intrinsic to the quasar - from which I do not intent to re-ascend.