Departamento de Física Aplicada II, Facultad de Ciencia y Tecnología, Universidad del País Vasco, Apartado 644, E-48080 Bilbao, Spain.
J Phys Chem B. 2011 Aug 18;115(32):9766-75. doi: 10.1021/jp202796y. Epub 2011 Jul 27.
Broadband dielectric spectroscopy (10(3) to 1.8 × 10(9) Hz) and specific heat measurements have been performed on the odd nonsymmetric liquid crystal dimer α-(4-cyanobiphenyl-4'-oxy)-ω-(1-pyreniminebenzylidene-4'-oxy)undecane (CBO11O·Py), as a function of temperature. The mesogenic behavior is restricted to a nematic mesophase which can be supercooled down to its corresponding glassy state if the cooling rate is fast enough (no less than 15 K·min(-1)). Dielectric measurements enable us to obtain the static permittivity and information about the molecular dynamics in the nematic mesophase as well as in the isotropic phase and across the isotropic-to-nematic phase transition. Two orientations (parallel and perpendicular) of the molecular director with regard to the probe electric field have been investigated. In the nematic mesophase, the dielectric anisotropy is revealed to be positive. Measurements of the parallel component of the dielectric permittivity are well explained by means of the molecular theory of dielectric relaxation in nematic dimers (J. Chem. Phys. 2004, 121 (16), 8079). The dimer is seen as a mixture of cis and trans conformers, and the model allows us to estimate their relative populations at each temperature. The main molecular motions are interpreted by the model as independent end-overend rotations of each terminal semirigid unit of the dimer. The nematic-to-isotropic phase transition has been exhaustively studied from the accurate evolution of the specific-heat and the static dielectric permittivity data. It has been concluded that the transition is first order in nature and follows the tricritical hypothesis. As a consequence, the nematic mesophase has been characterized as uniaxial despite the biaxiality and flexibility of the dimer molecule.
宽带介电光谱(10(3) 至 1.8×10(9) Hz)和比热测量已在奇数非对称液晶二聚体 α-(4-氰基联苯-4'-氧基)-ω-(1-芘亚胺苯甲叉-4'-氧基)十一烷(CBO11O·Py)上进行,作为温度的函数。介晶行为仅限于向列相,只要冷却速率足够快(不低于 15 K·min(-1)),就可以将其过冷至相应的玻璃态。介电测量使我们能够获得静态介电常数和向列相以及各向同性相以及各向同性-向列相相变中分子动力学的信息。已经研究了分子指向矢相对于探针电场的两种取向(平行和垂直)。在向列相相中,介电各向异性被揭示为正值。介电常数平行分量的测量可以通过向列二聚体介电弛豫的分子理论很好地解释(J. Chem. Phys. 2004, 121 (16), 8079)。二聚体被视为顺式和反式构象的混合物,该模型允许我们估计每个温度下它们的相对丰度。模型将主要分子运动解释为二聚体每个末端半刚性单元的独立首尾旋转。通过比热和静态介电常数数据的准确演化,彻底研究了向列-各向同性相变。得出的结论是,该转变本质上是一级的,并遵循三叉点假设。因此,尽管二聚体分子具有双轴性和柔韧性,但向列相被表征为单轴相。