PACS 73.21.LaDisorder-induced broadening of the conduction and valence band eigenenergies is calculated for an ensemble of dome-shaped In 0.6 Ga 0.4 As quantum dots of diameter 30 nm using an sp 3 d 5 s* tight binding model. An assumption is made that there is no alloy clustering, so that neighboring cations are uncorrelated. For this case, it is found that the contribution to the broadening from alloy disorder is small (less than 0.35 meV) relative to the total broadening determined from photoluminescence experiments and sensitive to the applied boundary conditions, so that care must be taken to ensure proper convergence of the numerical results.1 Introduction It is well known that the linewidth of any ensemble of quantum dots (QDs) is inhomogeneously broadened by the distribution in QD sizes and strain profile. The best photoluminescence (PL) measurements for ensembles of QDs have found linewidths on the order of 20 meV for selfassembled InGaAs QDs grown on GaAs substrates [1 -3]. Single QD measurements on AlGaAs/GaAs QDs, by contrast, can exhibit very narrow linewidths (~0.9 meV) [4]. However, even in a "perfect" ensemble in which all QDs have the same size and experience identical externally-induced strain, QDs composed of alloyed materials will still exhibit variations in linewidth that arise from differences in the spatial distribution of the constituent cations and anions. In this work we shall examine the magnitude of the broadening of the ground state eigenenergies induced by alloy disorder through the use of an atomistic tight-binding model. We find that for a typical dome-shaped In 0.6 Ga 0.4 As QD of diameter 30 nm, the broadening induced by the disorder is less than 0.35 meV.