Faculty of Computer Science and Material Science, Institute of Technology and Mechatronics, University of Silesia in Katowice, Katowice, Poland.
Department of Chemistry, University of Hull, Hull HU6 7RX, United Kingdom.
J Chem Phys. 2019 Sep 21;151(11):114908. doi: 10.1063/1.5114824.
Wide band dielectric spectroscopy of bent-shaped achiral liquid-crystal dimers 1″-n″-bis(4-cyanobiphenyl-4'-yl) n-alkanes (CBnCB n = 7, 9, 11) has been investigated in a frequency range 0.1 Hz-100 MHz using planar-aligned cells of sample thicknesses ranging from 2 to 10 (μm) over a temperature range that covers both nematic and twist bend nematic phases. Two peaks in the dielectric spectrum in the higher frequency range are assigned to the molecular relaxation processes. The peak at the highest frequency, ∼40 to 80 MHz, is assigned to an internal precessional rotation of a single unit of the dimer around the director. The mode in the next lower frequency range of 2-10 MHz is assigned to the spinning rotation of the dimer around its long axis. This involves fluctuations of the dipole moment of the bent-shaped conformation that is directed along its arrow direction of the bow shape formed by the dimer. The peak in the frequency range 100 kHz-1 MHz can be assigned to the collective fluctuations of the local director with reference to the helical axis of the N structure. The dependence of its frequency on temperature is reminiscent of the soft mode observed at the SmA to SmC phase transition. This result clearly corresponds to the electro-clinic effect-the response of the director to the applied electric field in an electro-optic experiment. The lowest frequency mode, observed in the frequency range of 0.1 Hz-100 Hz, is identified with the Goldstone mode. This mode is concerned with the long range azimuthal angle fluctuations of the local director. This leads to an alternating compression and expansion of the periodic structure of the N phase.
弯曲手性近晶相液晶二聚体 1″-n″-双(4-氰基联苯-4'-基)正构烷烃(CBnCB,n = 7,9,11)的宽频介电谱研究,使用厚度为 2 至 10μm 的平面排列样品池,在覆盖近晶相与扭曲向列相的温度范围内,频率范围为 0.1Hz-100MHz。介电谱在较高频率范围内的两个峰被分配给分子弛豫过程。最高频率处的峰,约 40 至 80MHz,被分配给双聚体单个单元围绕指向矢的内部预旋旋转。下一个较低频率范围(2-10MHz)的模式被分配给双聚体围绕其长轴的旋转。这涉及到沿其弓形状的双聚体箭头方向定向的弯曲构象的偶极矩波动。在 100kHz-1MHz 的频率范围内的峰可以分配给相对于 N 结构的螺旋轴的局部指向矢的集体波动。其频率对温度的依赖性类似于在 SmA 到 SmC 相变中观察到的软模式。该结果与电致弹性效应的响应非常吻合-即指向矢对电光实验中施加电场的响应。在 0.1Hz-100Hz 的频率范围内观察到的最低频率模式,被识别为戈德斯通模式。该模式与局部指向矢的长程方位角波动有关。这导致 N 相的周期性结构的交替压缩和扩展。