We present a self-consistent field algorithm for the restricted open-shell Kohn–Sham method which can be used to calculate excited states that have the same spatial symmetry as the corresponding ground states. The method is applied to π–π* transitions in polyenes, cyanines, and protonated imines. Excitation energies obtained with gradient corrected functionals are found to be significantly redshifted; the shift is constant within a homologous series. Planar excited state geometries have been optimized for all systems.
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Grimm et al. (2003) studied this question.
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