Helical Twist Sense and Spontaneous Polarization Direction in Ferroelectric Smectic Liquid Crystals.
Helical Twist Sense and Spontaneous Polarization Direction in Ferroelectric Smectic Liquid Crystals.
复制标题
铁电近晶液晶中的螺旋扭转方向和自发极化方向。
DOI:
10.1002/chin.198650052
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发表时间:
1986
期刊:
影响因子:
--
通讯作者:
J. Patel
中科院分区:
文献类型:
--
作者:
J. Goodby;E. Chin;T. Leslie;J. Geary;J. Patel
Liquid-crystalline systems of optically active materials, unlike those of pure amorphous liquids or solutions of chiral materials, exhibit regular alternations for the signs of theiroptical rotations of plane polarized light. In a given homologous series, there is an alternation effect as the asymmetric center is moved incrementally along the terminal carbonskeleton away from the central aromatic core of the molecule. The rotation alternates dextro to levo as the chiral center is moved from one position to the next. Studies on cholesteric phases have related this behavior to the twist sense of the macroscopic helical ordering of the molecules in the phase, to the position of the chiral center within the molecular structure, and to the spatial configuration of the asymmetric center. This present investigation shows that a similar effect also occurs in helical ferroelectric smectic phases, but in this case there are more complex rules relating the above factors to the directionof the spontaneous polarization with respect to the tilt axis of the monoclinic phase, and to the electron distribution aboutthe chiral center itself. General rules that relate these factors are developed which allowfor the predictions of various optical and electrical properties to be made directly from the molecular structure of the smectogen in question. The twist sense of the helical ordering of the molecules is shown to have dipolar origins, and it is therefore sensitive to changes in the electron distribution about the asymmetric center. Similarly, the direction of the spontaneous polarization is also dependent on the lateral dipolar nature and orientationof the chiral center with respect to the long axis of the molecule. Thus variations in the original rules occur for smectics depending on the dipole direction at this center. These general rules also apply to the ferroelectric properties of smectic crystal modifications and to the helical properties in cholesterics.