Abstract

The electronic structures of ${\mathrm{NiSi}}_{2}$/Si(111) A- and B-type interfaces are calculated within the local density approximation (LDA) using large supercells and the LMTO full-potential and ASA methods. The Schottky-barrier heights for the two interfaces differ by 0.14 eV, in agreement with experiment. The difference is caused by a partly filled interface band present in both structures. The LDA barrier heights ${E}_{F}$-${E}_{v}$ are both 0.4 eV too low, and insensitive to interface relaxations and to external potentials. The correct density-functional expression for the barrier height is ${E}_{F}$-${E}_{v}$+\ensuremath{\Delta}${v}_{\mathrm{xc}}$, where \ensuremath{\Delta}${v}_{\mathrm{xc}}$ is a nonlocal correction.

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