Abstract
An orbital polarization correction to local spin density (LSD) theory is developed in a crystal field basis, and applied to FeO, CoO, NiO, and ${\mathrm{La}}_{2}$${\mathrm{CuO}}_{4}$. The result is a substantial enhancement of the LSD band gap for NiO, and the creation of an insulating ground state for FeO, CoO, and ${\mathrm{La}}_{2}$${\mathrm{CuO}}_{4}$.
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