A second generation monodendron (abbreviated as G 2 NB) based on the AB 2 mesogenic monomer, 13-hydroxy-1-(4-hydroxyphenyl)-2-(4-hydroxy-4‘ ‘- p -terphenylyl)tridecane building blocks, exhibits multiple mesophase transformations with varying temperatures. On the basis of thermal transition behaviors studied by differential scanning calorimetry, structural analyses carried out by wide-angle and small-angle X-ray scatterings and electron diffraction experiments, and morphologies observed in polarized light microscope, the equilibrium phase transition sequence and phase structures have been identified. From the glass transition temperature at 28 °C, the most ordered phase is a highly ordered liquid crystalline (LC) smectic B ( ) phase. This phase is defined on the basis of the relationship between the LC mesogenic orientation direction and the layer normal. Within the layers, a molecular lateral hexagonal packing exists. It is followed by a low ordered LC smectic C (S C ) phase appeared in a narrow temperature range of ∼2 °C and quickly entered a nematic phase. At a high temperature of 92 °C, G 2 NB reaches the isotropic melt. An interesting observation is that the layer spacing of these and S C phases are much larger than the chemical repeat unit of the LC monomer; rather, it is a representative of the whole size of the G 2 NB monodendron. Therefore, the phase is a combined supramolecular layer structure and a lateral molecular hexagonal packing, while the S C phase is a pure supramolecular phase. A surprising finding is that the supramolecular S C phase formation possesses a stronger cooling rate dependence than that of the phase formation. This provides an opportunity to control the appearance of the S C phase formation by only varying the cooling rate. Possible packing structural model and formation mechanisms of this phenomenon are discussed.
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Liu et al. (2002) studied this question.
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