H. Kitzerow, G. Heppke, H. Schmid, B. Jérôme, P. Pieranski
{"title":"First optical observation of Kossel diagrams in chiral smectic phases","authors":"H. Kitzerow, G. Heppke, H. Schmid, B. Jérôme, P. Pieranski","doi":"10.1051/JPHYS:0199000510180208700","DOIUrl":null,"url":null,"abstract":"By means of optical microscopy, Kossel diagrams of chiral smectic phases are observed for the dirst time. Due to Bragg reflection, these diagrams occur in the focal plane of the microscope lens if the sample is illuminated with convergent monochromatic light. The Kossel diagram for the SmC* phase ― observed for the chiral compound CE3 (BDH) ― consists of a central ring corresponding to the periodicity p/2 of the |m|=2 mode of the tensor order parameter e(r) describing the helical structure. The temperature dependence of the pitch p(T) determined by the Kossel method is in agreement with spectroscopic investigations of the Bragg scattering in back reflection. The Kossel diagrams of the unknown chiral smectic structure SmM* consist also of one central ring; no additional reciprocal lattice vectors are observed in the visible wavelength range for this phase. In addition to the Kossel diagrams, we report on the observation of Airy spirals in the SmC* phase Au moyen d'un microscope polarisant en configuration conoscopique on etudie pour la premiere fois les diagrammes de Kossel des phases chirales SmC* et SmM*. Dans le cas de la phase SmC* on observe un seul anneau de Kossel correspondant a la periodicite p/2 de la composante tensorielle |m|=2 de la structure helicoidale du parametre d'ordre e(r). La variation du pas p(T) en fonction de la temperature, obtenue a partir des diagrammes de Kossel, est en accord avec des mesures faites independamment par reflexion de Bragg en incidence normale aux couches smectiques. Le diagramme de Kossel de la phase SmM* comporte aussi un seul anneau central. En plus d'anneau de Kossel, dans le cas de la phase SmC* on observe des spirales d'Airy","PeriodicalId":14747,"journal":{"name":"Journal De Physique","volume":"171 1","pages":"2087-2099"},"PeriodicalIF":0.0000,"publicationDate":"1990-09-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"3","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal De Physique","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1051/JPHYS:0199000510180208700","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 3
Abstract
By means of optical microscopy, Kossel diagrams of chiral smectic phases are observed for the dirst time. Due to Bragg reflection, these diagrams occur in the focal plane of the microscope lens if the sample is illuminated with convergent monochromatic light. The Kossel diagram for the SmC* phase ― observed for the chiral compound CE3 (BDH) ― consists of a central ring corresponding to the periodicity p/2 of the |m|=2 mode of the tensor order parameter e(r) describing the helical structure. The temperature dependence of the pitch p(T) determined by the Kossel method is in agreement with spectroscopic investigations of the Bragg scattering in back reflection. The Kossel diagrams of the unknown chiral smectic structure SmM* consist also of one central ring; no additional reciprocal lattice vectors are observed in the visible wavelength range for this phase. In addition to the Kossel diagrams, we report on the observation of Airy spirals in the SmC* phase Au moyen d'un microscope polarisant en configuration conoscopique on etudie pour la premiere fois les diagrammes de Kossel des phases chirales SmC* et SmM*. Dans le cas de la phase SmC* on observe un seul anneau de Kossel correspondant a la periodicite p/2 de la composante tensorielle |m|=2 de la structure helicoidale du parametre d'ordre e(r). La variation du pas p(T) en fonction de la temperature, obtenue a partir des diagrammes de Kossel, est en accord avec des mesures faites independamment par reflexion de Bragg en incidence normale aux couches smectiques. Le diagramme de Kossel de la phase SmM* comporte aussi un seul anneau central. En plus d'anneau de Kossel, dans le cas de la phase SmC* on observe des spirales d'Airy
利用光学显微镜首次观察到手性晶相的科塞尔图。由于布拉格反射,如果样品用会聚单色光照射,这些图就会出现在显微镜透镜的焦平面上。手性化合物CE3 (BDH)的SmC*相的Kossel图由一个中心环组成,该中心环对应于描述螺旋结构的张量阶参数e(r)的|m|=2模式的周期性p/2。由科塞尔方法确定的节距p(T)的温度依赖性与背反射布拉格散射的光谱研究一致。未知手性微晶结构SmM*的科塞尔图也由一个中心环组成;在该相位的可见波长范围内没有观察到额外的互易晶格矢量。除了科塞尔图外,我们还报道了用光学显微镜观察到的SmC*相中的Airy螺旋现象。Dans le cas de la相SmC* on on observe unseul anneau de Kossel对应于la periodicite p/2 de la composante tensorielle |m|=2 de la structure helicoidale du parameter d' order e(r)。p(T)随温度的变化,得到了科塞尔图的一部分,测试了测量值的独立性与反射的Bragg入射法线的关系。Le diagramme de Kossel de la phase SmM* comcomte aussi un seul anneau central。En + d'anneau de Kossel,在观察airy的螺旋上,研究了相位SmC*的结构