Araoka Fumito, Thisayukta Jirakorn, Ishikawa Ken, Watanabe Junji, Takezoe Hideo
Department of Organic and Polymeric Materials, Tokyo Institute of Technology, O-okayama, Meguro-ku, Tokyo 152-8552, Japan.
Phys Rev E Stat Nonlin Soft Matter Phys. 2002 Aug;66(2 Pt 1):021705. doi: 10.1103/PhysRevE.66.021705. Epub 2002 Aug 14.
Second-harmonic generation (SHG) measurements have been conducted in the ferroelectric liquid crystalline phase of a chiral bent-core molecule, P-8-OPIMB6*. Well-aligned cells were obtained by applying an electric field parallel to the substrate surfaces. In-plane anisotropy of the SHG signal observed at normal incidence of light shows two- or four-leaf patterns depending on polarization conditions, indicating a ferroelectric uniform structure. The detailed analysis of the data by taking account of optical anisotropy in the SHG active bulk leads to the determination of nonlinear susceptibility tensor components, d(333)=14.4 pm/V and d(311)=49.2 pm/V. Using the d coefficients thus determined, the hyperpolarizability tensor components of the molecule are also determined as beta(zzz)=14.5 x 10(-30) esu and beta(zxx)=67.6 x 10(-30) esu. These values well agree with those of the achiral homolog P-12-OPIMB previously determined by hyper-Rayleigh scattering.
在手性弯曲核分子P-8-OPIMB6*的铁电液晶相中进行了二次谐波产生(SHG)测量。通过施加平行于基板表面的电场获得了排列良好的单元。在光垂直入射时观察到的SHG信号的面内各向异性根据偏振条件呈现两叶或四叶图案,表明存在铁电均匀结构。通过考虑SHG活性体中的光学各向异性对数据进行详细分析,确定了非线性极化率张量分量,d(333)=14.4 pm/V和d(311)=49.2 pm/V。利用由此确定的d系数,还确定了分子的超极化率张量分量,β(zzz)=14.5×10^(-30) esu和β(zxx)=67.6×10^(-30) esu。这些值与先前通过超瑞利散射确定的非手性同系物P-12-OPIMB的值非常吻合。