Abstract

We propose a simplification of the time-dependent self-interaction correction (TD-SIC) method using two sets of orbitals, applying the optimized effective potential (OEP) method. The resulting scheme is called time-dependent ``generalized SIC-OEP.'' A straightforward approximation, using the spatial localization of one set of orbitals, leads to the ``generalized SIC-Slater'' formalism. We show that it represents a great improvement compared to the traditional SIC-Slater and Krieger-Li-Iafrate formalisms.

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