This contribution explores the use of perturbation theory and the chemically oriented, computationally efficient PPP π-electron model Hamiltonian to describe the first three molecular hyperpolarizabilities and their interrelationships. Relationships between various nonlinear phenomena are treated as degeneracy factors, and a more general definition emerges from this analysis. Derivations of formulas describing second- to fourth-order susceptibilities are given for the monoexcited CI (MECI) and doubly excited CI (DECI) perturbation approaches, and numerical results are in good to excellent agreement with experimental values where available for a variety of second- and third-order nonlinear phenomena (second harmonic generation, frequency mixing, linear electrooptic effect, optical rectification, third harmonic generation, dc-induced second harmonic generation, degenerate four-wave mixing, Kerr effect). Additional analysis of chromophore architecture-nonlinear optical relationships reveals that the observable second-order susceptibility, βvec, is quite sensitive to intramolecular charge transfer and molecular distortions. This becomes even more pronounced in fourth-order phenomena since δiiiii is related to charge transfer in a cubic manner rather than linearly as in the case of βiii. Third-order susceptibilities, γijkl, function exactly as αij in a centrosymmetric system and are dominated by the size and shape of the electron cloud. However, in a noncentrosymmetric environment, γijkl has a more complex behavior than either αij or βijk, and charge-transfer excitations can make an important contribution.
|Number of pages||12|
|Journal||Journal of Physical Chemistry|
|Publication status||Published - 1992|
ASJC Scopus subject areas
- Physical and Theoretical Chemistry