Centre for Liquid Crystal Research, P.O. Box 1329, Jalahalli, Bangalore 560 013, India.
J Phys Chem B. 2010 Feb 11;114(5):1745-50. doi: 10.1021/jp905879n.
We report on measurements of dielectric permittivity epsilon, electrical conductivity sigma, elastic moduli k(ii), and rotational viscosity gamma for a bent-core nematic liquid crystal. The static permittivity anisotropy epsilon(a) = epsilon(parallel)-epsilon(perpendicular) is negative; at a given temperature in the interval 107-123 degrees C, epsilon(parallel) shows two relaxations falling in the frequency bands 20-200 kHz and 0.9-2 MHz; epsilon(perpendicular) also shows a relaxation between 0.9 and 5 MHz. The conductivity anisotropy sigma(a) = sigma(parallel)-sigma(perpendicular) is negative at low frequencies; it changes sign twice at frequencies f(1) and f(2) that increase with temperature, in the ranges 6.5-10 and 95-600 kHz, respectively. Surprisingly, the splay modulus k(11) is considerably greater than the bend modulus k(33) in the entire nematic range. Viscous relaxation is more complex than in calamitic systems involving at least a two-step process. The gamma values are an order of magnitude greater compared to calamitics.
我们报告了一种弯曲状核心向列相液晶的介电常数 ε、电导率 σ、弹性模量 k(ii)和旋转粘度 γ 的测量结果。静态介电各向异性 ε(a) = ε(parallel) - ε(perpendicular) 为负;在 107-123°C 的给定温度范围内,ε(parallel) 显示出两个落在 20-200 kHz 和 0.9-2 MHz 频带中的弛豫;ε(perpendicular) 也在 0.9-5 MHz 之间显示出一个弛豫。在低频时,电导率各向异性 σ(a) = σ(parallel) - σ(perpendicular) 为负;它的符号在频率 f(1) 和 f(2)处发生两次变化,f(1) 和 f(2)随温度增加,分别在 6.5-10 和 95-600 kHz 范围内。令人惊讶的是,在整个向列相范围内,扭曲模量 k(11) 明显大于弯曲模量 k(33)。粘性弛豫比涉及至少两步过程的棒状系统更为复杂。与棒状相比,γ 值大一个数量级。