Abstract

We have employed conventional ab initio and density-functional-theory (DFT) methods to study the structure, stability and electric polarizability of small gallium arsenide clusters ${\mathrm{Ga}}_{n}{\mathrm{As}}_{n}$. We relied on purpose-oriented, carefully optimized basis sets of Gaussian-type functions. We have calculated both the mean dipole polarizability $(\overline{\ensuremath{\alpha}})$ and the anisotropy $(\mathrm{\ensuremath{\Delta}}\ensuremath{\alpha})$. Our results show that the differential-per-atom polarizability of the most stable isomers decreases rapidly with cluster size. Compared to the ab initio results, the widely used Becke's three-parameter exchange DFT functional with the Lee, Yang, and Parr correlation functional and Becke's three-parameter exchange DFT functional with Perdew and Wang's 1991 gradient-corrected correlation functional density-functional-theory methods follow clearly the trend of the differential-per-atom polarizability ${\overline{\ensuremath{\alpha}}}_{\mathrm{diff}}∕\mathrm{atom}$ for the most stable isomers and predict values closer to the self-consistent field method but distinctly lower than second-order M\o{}ller-Plesset perturbation theory. All methods predict a positive value for the dimer, ${\overline{\ensuremath{\alpha}}}_{\mathrm{diff}}∕\mathrm{atom}$ $({\mathrm{Ga}}_{2}{\mathrm{As}}_{2})>0$.

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