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We examine the trends in the self-energy operators of Si, diamond, GaAs, and AlAs, and in their corresponding exchange-correlation potentials Vₗ₂ and their discontinuities. The potentials are calculated from the self-energies, thus avoiding use of a local-density approximation (LDA). In each case about 80% of the LDA band-gap error is also present for the true density-functional theory eigenvalue difference derived from Vₗ₂ and so is caused by. The self-energies themselves, calculated in the Hedin-Lundqvist GW approximation, reproduce the experimental quasiparticle energies accurately, and are also shown to be well modeled by a simple functional form in real space.
Godby et al. (Thu,) studied this question.