液晶中近晶相的微观有序

M. Zgonik, M. Rey-Lafon, C. Destrade, C. Leon, H. Nguyen
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引用次数: 12

摘要

铁电液晶材料4′-(2S,3S)-2″-氯-3″-甲基戊氧基苯基-4-癸氧基硫苯甲酸酯(简称10.S)的取向顺序用红外吸收光谱法对C1Isolleu进行了表征。在书架和各向同性排列几何中制备了定向样品。选择了几种较强的红外振动来表征分子的不同部分和方向。结果表明,从sa相到sc *相,分子核心部分的分子倾斜度变化很小,表明分子核心部分在sa相已经倾斜。核心部分的轴线在sa相的锥体上无序,开始彼此对齐,但在降低温度进入sc *相时仍保持在该锥体上。该模型与先前的一些研究结果相一致,这些结果是通过对材料晶体液体铁电体,四烷基氧基-4-硫苯酸盐[(2S,3S)-氯-2-甲基-3-戊氧基]-4'-苯基的光谱分析得出的。两种类型的力学取向,一种类型的同向异性,一种类型的构型,一种类型的克拉克-拉格沃尔,一种类型的制备,一种类型的多波段强度,一种类型的特征,一种类型的分子取向,一种类型的选择。Les results montrent que l' ininaison des parties centrales (cœurs) des molecules varies peu de la phase sa A la phase sc *, ce qui implque Les cœurs des molecules sonja injines dans la phase sa。在温度恒定的情况下,低轴、低轴、低轴、低轴、低轴、低轴、低轴、低轴、低轴、低轴、低轴、低轴、低轴、低轴。该模型的测试结果与实验结果一致
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Microscopic ordering in smectic phases of liquid crystals
Orientationa order in smectic phases of a ferroelectric liquid-crystalline material 4'-(2S,3S)-2″-chloro-3″-methylpentanoyloxyphenyl-4-decyloxy thiobenzoate, abbreviated 10.S.C1Isolleu, was examined by IR absorption spectroscopy. Oriented samples were prepared in both bookshelf and homeotropic alignment geometry. Several stronger IR vibrations were selected characterizing different parts and orientations of the molecules. Results show that the molecular tilt of the core parts of the molecules changes very little from the S A to the S C * phase implying that the core parts of the molecules are already tilted in the S A phase. Axes of the core parts, that are disordered on a cone in the S A phase, start to align with each other but remain on this cone on lowering the temperature into the S C * phase. The model agrees with some previous results On a etudie par spectroscopie d'absorption infrarouge l'ordre orientationnel dans les phases smectiques d'un materiau cristal liquide ferroelectrique, le decyloxy-4-thiobenzoate de [(2S,3S)-chloro-2-methyl-3-pentanoyloxy]-4'-phenyle, en abrege 10.S.C1Isoleu. Deux types d'echantillons orientes, l'un homeotrope, l'autre en configuration Clark-Lagerwall, ont ete prepares et plusieurs bandes intenses en infrarouge, caracteristiques des differentes parties et orientations des molecules, ont ete choisies. Les resultats montrent que l'inclinaison des parties centrales (cœurs) des molecules varie tres peu de la phase S A a la phase S C *, ce qui implique que les cœurs des molecules sont deja inclines dans la phase S A . Leurs axes, qui sont desordonnes sur un cone dans la phase S A , s'alignent mais restent sur ce cone quand on passe en phase S C * en abaissant la temperature. Ce modele est en accord avec quelques resultats anterieurs
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