Grup de Propietas Físiques dels Materials (GRPFM), Departament de Física, E.T.S.E.I.B. Universitat Politècnica de Catalunya, Diagonal 647, E- 08028 Barcelona, Spain.
Departamento de Física Aplicada II, Facultad de Ciencia y Tecnología, Universidad del País Vasco, Apartado 644, E-48080 Bilbao, Spain.
Phys Rev E. 2018 Jan;97(1-1):012704. doi: 10.1103/PhysRevE.97.012704.
In the present work, a detailed analysis of the glassy behavior and the relaxation dynamics of the liquid crystal dimer α-(4-cyanobiphenyl-4'-yloxy)-ω-(1-pyrenimine-benzylidene-4'-oxy) heptane (CBO7O.Py) throughout both nematic and smectic-A mesophases by means of broadband dielectric spectroscopy has been performed. CBO7O.Py shows three different dielectric relaxation modes and two glass transition (T_{g}) temperatures: The higher T_{g} is due to the freezing of the molecular motions responsible for the relaxation mode with the lowest frequency (μ_{1L}); the lower T_{g} is due to the motions responsible for the two relaxation modes with highest frequencies (μ_{1H} and μ_{2}), which converge just at their corresponding T_{g}. It is shown how the three modes follow a critical-like description via the dynamic scaling model. The two modes with lowest frequencies (μ_{1L} and μ_{1H}) are cooperative in the whole range of the mesophases, whereas the highest frequency mode (μ_{2}) is cooperative just below some crossover temperature. In terms of fragility, at the glass transition, the ensemble (μ_{1H}+μ_{2}) presents a value of the steepness index and μ_{1L} a different one, meaning that fragility is a property intrinsic to the molecular motion itself. Finally, the steepness index seems to have a universal behavior with temperature for the dielectric relaxation modes of liquid crystal dimers, being almost constant at high temperatures and increasing drastically when cooling the compound down to the glass transition from a temperature about 3/4T_{NI}.
在本工作中,通过宽带介电谱对液晶二聚体 α-(4-氰基联苯-4'-氧基)-ω-(1-芘亚胺-苯甲叉-4'-氧基)庚烷(CBO7O.Py)在向列相和近晶-A 相整个相区间的玻璃化行为和弛豫动力学进行了详细分析。CBO7O.Py 显示出三种不同的介电弛豫模式和两个玻璃化转变(T_{g})温度:较高的 T_{g}归因于负责具有最低频率(μ_{1L})弛豫模式的分子运动的冻结;较低的 T_{g}归因于负责具有最高频率(μ_{1H}和μ_{2})的两个弛豫模式的分子运动,它们在相应的 T_{g}处收敛。结果表明,这三种模式如何通过动态标度模型呈现出类似临界的描述。在整个介相范围内,频率最低的两种模式(μ_{1L}和μ_{1H})是协同的,而频率最高的模式(μ_{2})仅在某个交叉温度以下是协同的。就脆性而言,在玻璃化转变时,集合(μ_{1H}+μ_{2})呈现出陡峭指数的值,而μ_{1L}呈现出不同的值,这意味着脆性是分子运动本身的固有特性。最后,在液晶二聚体的介电弛豫模式中,陡峭指数似乎具有与温度相关的普遍行为,在高温下几乎保持不变,而在从大约 3/4T_{NI}的温度冷却到玻璃化转变时急剧增加。