Catalysis Research Center, Hokkaido University, Sapporo 001-0021, Japan.
J Chem Phys. 2010 Jul 21;133(3):034705. doi: 10.1063/1.3428673.
In this paper, the results of the modeling calculations carried out for predicting the interference effects expected in the sum frequency generation (SFG) spectra of a specific thin-layer system, described in the accompanying paper, are tested by comparing them with the experimental spectra obtained for a real thin-layer film comprising an organic monolayer/variable thickness dielectric layer/gold substrate. In this system, two contributions to the SFG spectra arise, a resonant contribution from the organic film and a nonresonant contribution from the gold substrate. The modeling calculations are in excellent agreement with the experimental spectra over a wide range of thicknesses and for different polarization combinations. The introduction of another resonant monolayer adjacent to the gold substrate and with the molecules having a reverse orientation has a significant affect on the spectral shapes which is predicted. If a dielectric substrate such as CaF(2) is used instead of a gold substrate, only the spectral intensities vary with the film thickness but not the spectral shapes. The counterpropagating beam geometry will change both the thickness dependent spectral shapes and the intensity of different vibrational modes in comparison with a copropagating geometry. The influences of these experimental factors, i.e., the molecular orientational structure in the thin film, the nature of the substrate, and the selected incident beam geometry, on the experimental SFG spectra are quantitatively predicted by the calculations. The thickness effects on the signals from a SFG active monolayer contained in a thin liquid-layer cell of the type frequently used for in situ electrochemical measurements is also discussed. The modeling calculation is also valid for application to other thin-film systems comprising more than two resonant SFG active interfaces by appropriate choice of optical geometries and relevant optical properties.
本文通过将建模计算结果与实际的包含有机单分子层/可变厚度介电层/金基底的薄层膜的实验光谱进行比较,验证了前文所描述的特定薄层系统和倍频产生(SFG)光谱中预期的干涉效应的预测建模计算结果。在该系统中,SFG 光谱有两个贡献,一个是有机膜的共振贡献,另一个是金基底的非共振贡献。建模计算在很大的厚度范围内和不同的偏振组合下与实验光谱非常吻合。在金基底旁边引入另一个具有相反取向的共振单分子层对光谱形状有显著影响,这一预测得到了证实。如果使用 CaF(2)等介电基底代替金基底,只有光谱强度随薄膜厚度而变化,而光谱形状不变。与共线几何形状相比,对向光束几何形状会改变与厚度相关的光谱形状和不同振动模式的强度。这些实验因素,即薄膜中的分子取向结构、基底的性质以及选择的入射光束几何形状,对实验 SFG 光谱的影响通过计算得到了定量预测。还讨论了对经常用于原位电化学测量的薄液层池中的 SFG 活性单层的信号的厚度效应。通过适当选择光学几何形状和相关的光学性质,该建模计算也可应用于其他包含两个以上共振 SFG 活性界面的薄膜系统。