Mitchell S A
Steacie Institute for Molecular Sciences, National Research Council of Canada, 100 Sussex Drive, Ottawa, Ontario K1A 0R6, Canada.
J Phys Chem B. 2006 Jan 19;110(2):883-90. doi: 10.1021/jp0541866.
The nonlinear susceptibility tensor, chi(2), for second harmonic generation (SHG) by a monolayer of the cyanobiphenyl derivative 4-n-octyl-4'-cyanobiphenyl (8CB) at the air/water interface has been measured with the fundamental frequency variant Planck's over 2piomega=1.55 eV (lambda=800 nm). The contribution of the water subphase was estimated by measuring the magnitudes and relative phases of the nonlinear susceptibilities of the bare and monolayer-covered water surfaces. All nonzero elements of chi(2) are placed on an absolute scale by comparison with SHG in reflection from a z-cut quartz crystal. The experimental measurements for the 8CB monolayer are compared with computed susceptibilities derived by using standard time-dependent perturbation theory in conjunction with a semiempirical electronic structure model. Good agreement has been found between experimental and computational results when the average tilt angle of the cyanobiphenyl chromophore of 8CB is in the range 60-70 degrees relative to the surface normal. A critique is given of an alternative, simplified measurement procedure of the tilt angle in which only the dominant element of the molecular hyperpolarizability tensor is considered. It is shown that the simplified procedure is invalid for 8CB monolayers when the tilt angle is greater than approximately 70 degrees.
已使用基频为普朗克常数除以(2\pi\omega = 1.55)电子伏特((\lambda = 800)纳米)的光,测量了空气/水界面处一层氰基联苯衍生物4 - 正辛基 - 4'- 氰基联苯(8CB)产生二次谐波(SHG)时的非线性极化率张量(\chi^{(2)})。通过测量裸水面和覆盖有单层分子的水面的非线性极化率的大小和相对相位,估算了水亚相的贡献。通过与z切割石英晶体反射中的SHG进行比较,将(\chi^{(2)})的所有非零元素置于绝对尺度上。将8CB单层的实验测量结果与使用标准含时微扰理论结合半经验电子结构模型得出的计算极化率进行了比较。当8CB的氰基联苯发色团相对于表面法线的平均倾斜角在60 - 70度范围内时,实验结果与计算结果吻合良好。对一种替代的、简化的倾斜角测量程序进行了批判,该程序仅考虑分子超极化率张量的主导元素。结果表明,当倾斜角大于约70度时,简化程序对8CB单层是无效的。