Precision cosmology challenges many aspects of fundamental physics. In particular, quasar absorption lines test the assumed constancy of fundamental constants over cosmological time-scales and distances. Until recently, the most reliable technique was the alkali doublet (AD) method where the measured doublet separation probes variations in the fine-structure constant, \(α ≡ e^2/ c\). However, the recently introduced many-multiplet (MM) method provides several advantages, including a demonstrated ≈10-fold precision gain. This thesis presents detailed MM analyses of 3 independent Keck/HIRES samples containing 128 absorption systems with \(0.2 < zabs < 3.7\). We find \(5.6σ\) statistical evidence for a smaller α in the absorption clouds: \(Δα/α = (-0.574 ± 0.102) × 10⁻⁵\). All three samples separately yield consistent, significant \(Δα/α\). The data marginally prefer constant \(dα/dt\) rather than constant \(Δα/α\). The two-point correlation function for α and the angular distribution of \(Δα/α\) give no evidence for spatial variations. We also analyse 21 Keck/HIRES Si iv doublets, obtaining a 3-fold relative precision gain over previous AD studies: \(Δα/α = (0.5 ± 1.3) × 10⁻⁵\) for \(2.0 < zabs < 3.1\). Our statistical evidence for varying α requires careful consideration of systematic errors. Modelling demonstrates that atmospheric dispersion is potentially important. However, the quasar spectra suggest a negligible effect on \(Δα/α\). Cosmological variation in Mg isotopic abundances may affect \(Δα/α\) at \(zabs < 1.8\). Galactic observations and theory suggest diminished 25,26Mg abundances in the low metallicity quasar absorbers. Removing 25,26Mg isotopes yields more negative \(Δα/α\) values. Overall, known systematic errors can not explain our results. We also constrain variations in \(y = α^2gₚ\), comparing H I 21-cm and millimetre-wave molecular absorption in 2 systems. Fitting both the H I and molecular lines yields the tightest, most reliable current constraints: \(Δ y/y = (-0.20 ± 0.44) × 10⁻⁵\) and \(Δ y/y = (-0.16 ± 0.54) × 10⁻⁵\) at \(zabs = 0.2467\) and 0.6847 respectively. Possible line-of-sight velocity differences between the H I and molecular absorbing regions dominate these \(1σ\) errors. A larger sample of mm/H I comparisons is required to reliably quantify this uncertainty and provide a potentially crucial check on the MM result.
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M. T. Murphy (2003) studied this question.