Frequency-Dependent Second Harmonic Generation in Acentric Chromophoric Self-Assembled NLO Materials | Yitzchaik Group

Frequency-Dependent Second Harmonic Generation in Acentric Chromophoric Self-Assembled NLO Materials

Citation:

S. Yitzchaik, Lundquist, P.M. , Lin, W. , Kanis, D.R. , Ratner, M.A. , Marks, T.J. , and Wong, G.K. . 1994. “Frequency-Dependent Second Harmonic Generation In Acentric Chromophoric Self-Assembled Nlo Materials”. Mrs Proceedings, 351, Pp. 119-125. http://journals.cambridge.org/action/displayAbstract?fromPage=online&aid=8085975&fileId=S1946427400316177.

Abstract:

An attractive and challenging approach to the construction of robust, thin film materials with large second-order optical nonlinearities is the covalent self-assembly of aligned arrays of high-β molecular chromophores into multilayer superlattices. In this paper, we describe the dispersion of second harmonic generation (SHG) in a self-assembled (SA) monolayer containing a stilbazolium chromophore. The frequency-dependent measurements were performed on 25 Å thick monolayers on glass using a tunable (0.4–2 μm) light source based on optical parametric amplification (OPA). The SHG spectrum contains a clear two-photon resonance at hω = 1.3eV. The maximum in the second-order susceptibility coincides with a low energy chromophore-centered charge-transfer excitation at 480 nm. The experimental SHG dispersion values compare favorably with theoretical results computed using a sum-over-states (SOS) formalism. However, the measured values exhibit a somewhat broader band response than the theoretical curve, and the origin of this behavior is discussed.