Abstract. The dependences of the 294 and 10 K mobility μ and volume carrier concentration n on thickness (d ¼ 25 to 147 nm) are examined in aluminum-doped zinc oxide (AZO). Two AZO layers are grown at each thickness, one with and one without a 20-nm-thick ZnON buffer layer. Plots of the 10 K sheet concentration n s versus d for buffered (B) and unbuffered (UB) samples give straight lines of similar slope, n ¼ 8.36 × 10 20 and 8.32 × 10 20 cm −3 , but different x -axis intercepts, δd ¼ −4 and þ13 nm, respectively. Plots of n s versus d at 294 K produce substantially the same results. Plots of μ versus d can be well fitted with the equation μðd Þ ¼ μð∞Þ∕½1 þ d à ∕ðd − δdÞ, where d à is the thickness for which μð∞Þ is reduced by a factor 2. For the B and UB samples, dà ¼ 7 and 23 nm, respectively, showing the efficacy of the ZnON buffer. Finally, from n and μð∞Þ we can use degenerate electron scattering theory to calculate bulk donor and acceptor concentrations of 1.23 × 10 21 cm −3 and 1.95 × 10 20 cm −3 , respectively, and Drude theory to predict a plasmonic resonance at 1.34 μm. The latter is confirmed by reflectance measurements.