Institute of Physical Chemistry, University of Stuttgart, Pfaffenwaldring 55, 70569 Stuttgart, Germany.
Phys Rev E. 2018 Mar;97(3-1):032705. doi: 10.1103/PhysRevE.97.032705.
In thermotropic chiral Sm-A^{} phases, an electric field along the smectic layers breaks the D_{∞} symmetry of the Sm-A^{} phase and induces a tilt of the liquid crystal director. This so-called electroclinic effect (ECE) was first reported by Garoff and Meyer in 1977 and attracted substantial scientific and technological interest due to its linear and submicrosecond electro-optic response [S. Garoff and R. B. Meyer, Phys. Rev. A 19, 338 (1979)0556-279110.1103/PhysRevA.19.338]. We now report the observation of an ECE in the pretransitional regime from a lyotropic chiral lamellar L_{α}^{} phase into a lyo-Sm-C^{} phase, the lyotropic analog to the thermotropic Sm-C^{*} phase which was recently discovered by Bruckner et al. [Angew. Chem. Int. Ed. 52, 8934 (2013)1433-785110.1002/anie.201303344]. We further show that the observed ECE has all signatures of its thermotropic counterpart, namely (i) the effect is chiral in nature and vanishes in the racemic L_{α} phase, (ii) the effect is essentially linear in the sign and magnitude of the electric field, and (iii) the magnitude of the effect diverges hyperbolically as the temperature approaches the critical temperature of the second order tilting transition. Specific deviations between the ECEs in chiral lamellar and chiral smectic phases are related to the internal field screening effect of electric double layers formed by inevitable ionic impurities in lyotropic phases.
在热致手性 Sm-A^{} 相中,沿层状排列的电场打破 Sm-A^{} 相的 D_{∞}对称,并诱导液晶指向矢倾斜。这种所谓的电致伸缩效应(ECE)于 1977 年由 Garoff 和 Meyer 首次报道,并因其线性和亚微秒电光响应而引起了广泛的科学和技术关注 [S. Garoff 和 R. B. Meyer, Phys. Rev. A 19, 338 (1979)0556-279110.1103/PhysRevA.19.338]。我们现在报告在手性层状 Lyotropic L_{α}^{} 相转变为 Lyotropic-Sm-C^{} 相的预相变区观察到的电致伸缩效应,Lyotropic-Sm-C^{} 相是 Bruckner 等人最近发现的热致 Sm-C^{} 相的类似物 [Angew. Chem. Int. Ed. 52, 8934 (2013)1433-785110.1002/anie.201303344]。我们进一步表明,观察到的电致伸缩效应具有其热致对应物的所有特征,即(i)该效应本质上是手性的,在无手性的 L_{α} 相消失,(ii)该效应在电场的符号和大小上基本呈线性,以及(iii)随着温度接近二阶倾斜相变的临界温度,效应的大小呈双曲线发散。手性层状和手性向列相之间的电致伸缩效应的具体差异与层状各向异性相中不可避免的离子杂质形成的电双层的内场屏蔽效应有关。