Abstract
The third-order nonlinear optical properties of thin films of two series of conjugated rigid-rod polyquinolines, exemplified by poly(2, 2’-(l, 4-phenylene)-6, 6’-bis(4-phenyl quinoline)) (PPPQ, 2d) and poly(2, 7-(l, 4-phenylene)-4, 9-diphenyl-l, 6-anthrazoline) (PPDA, 3d), were investigated by third harmonic generation spectroscopy. Of the nine polyquinolines with diverse backbone structures, PPPQ has the largest optical nonlinearity with a gC(3) (−3ω;ω,ω,ω) value of 3.2 x 10-12 esu and 3.3 x 10-11 esu in the off-resonant and three-photon resonant regions, respectively. A comparison of the nonresonant gC(3) of the series of nine systematically derived polyquinolines showed that a scaling law of the form gC(3) ∼ (λmax)v∼ Eg-v does not hold; in fact, the nonresonant gC(3) was essentially independent of the optical bandgap. These results suggest that structure-gC(3) propeny relationships in polymers cannot be inferred from those of oligomers and model compounds.
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Work at university of Rochester was supported by the Amoco Foundation and the National Science Foundation (Grant CHE-881-0024).
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Agrawal, A.K., Jenekhe, S.A., Vanherzeele, H. et al. Third-Order Nonlinear Optical Properties of a Series of Systematically Designed Conjugated Rigid-Rod Polyquinolines. MRS Online Proceedings Library 247, 253–258 (1992). https://doi.org/10.1557/PROC-247-253
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DOI: https://doi.org/10.1557/PROC-247-253