The dependence to be expected by the experimentally observed diffusivity of As in Hg 0.8 Cd 0.2 Te, D(As), on the Hg pressure, P Hg , and on the As concentration has been calculated for various modes of As incorporation described in the literature and for interstitial and vacancy diffusion mechanisms. Comparison with experimental data which shows D(As) to be independent of As concentration (at least up to 5 × 10 18 cm −3 ), to vary as 1/P Hg at moderate pressures and as 1/P 3 Hg at high pressures, confirms that these features can only be accounted for if As substitutes on the cation sub-lattice as As • Hg and on the anion sub-lattice as As Te . Diffusion occurs on the cation sub-lattice due to the mobile As • Hg diffusing by a vacancy mechanism. Significant concentrations of As dimer or tetramer complexes give rise to D(As) depending on the As concentration as well as incorrect variations with P Hg . A further important result is that Hg 0.8 Cd 0.2 Te is electrically intrinsic for these As concentrations down to at least 250 • C.