Abstract
A ‘‘missing-state’’ analysis is introduced and used to identify excited states and dynamics important for χ(2) and χ(3). This method is applied to the Pariser-Pople-Parr self-consistent-field configuration-interaction transition moments and energies that are used to calculate the second-harmonic susceptibility χ2ω(2) and the third-harmonic susceptibility χ3ω(3) for a group of organic molecules. Examination of charge and bond-order distributions for the relevant states reveals the nature of the states that contribute to the nonlinear optical processes. Results are presented for benzene, nitrobenzene, p-dinitrobenzene, and p-nitroaniline.

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