We have developed a full-band pseudopotential-based approach to describe semiconductor nanostructures. The method relies on the bulk Bloch functions expansion of the system wave function that guarantees an efficient integration of the full-band approach in self-consistent schemes where Schr\"odinger and Poisson equations are solved iteratively. In order to gain efficiency of the method a suitable separation between structure-dependent and material-dependent contributions to the system Hamiltonian is presented. Results are shown for typical nanostructures.
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Chirico et al. (2001) studied this question.
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