A second generation monodendron (abbreviated as G
2NB) based on the AB
2 mesogenicmonomer, 13-hydroxy-1-(4-hydroxyphenyl)-2-(4-hydroxy-4' '-
p-terphenylyl)tridecane buildingblocks, exhibits multiple mesophase transformations with varying temperatures. On thebasis of thermal transition behaviors studied by differential scanning calorimetry, structuralanalyses carried out by wide-angle and small-angle X-ray scatterings and electron diffractionexperiments, and morphologies observed in polarized light microscope, the equilibrium phasetransition sequence and phase structures have been identified. From the glass transitiontemperature at 28
![](/images/entities/deg.gif)
C, the most ordered phase is a highly ordered liquid crystalline (LC)smectic B (
![](/isubscribe/journals/cmatex/14/i05/eqn/cm01172<font color=)
28e10001.gif">) phase. This phase is defined on the basis of the relationship between the LCmesogenic orientation direction and the layer normal. Within the layers, a molecular lateralhexagonal packing exists. It is followed by a low ordered LC smectic C (S
C) phase appearedin a narrow temperature range of ~2
![](/images/entities/deg.gif)
C and quickly entered a nematic phase. At a hightemperature of 92
![](/images/entities/deg.gif)
C, G
2NB reaches the isotropic melt. An interesting observation is thatthe layer spacing of these
![](/isubscribe/journals/cmatex/14/i05/eqn/cm01172<font color=)
28e10002.gif"> and S
C phases are much larger than the chemical repeat unitof the LC monomer; rather, it is a representative of the whole size of the G
2NB monodendron.Therefore, the
![](/isubscribe/journals/cmatex/14/i05/eqn/cm01172<font color=)
28e10003.gif"> phase is a combined supramolecular layer structure and a lateralmolecular hexagonal packing, while the S
C phase is a pure supramolecular phase. Asurprising finding is that the supramolecular S
C phase formation possesses a stronger coolingrate dependence than that of the
![](/isubscribe/journals/cmatex/14/i05/eqn/cm01172<font color=)
28e10004.gif"> phase formation. This provides an opportunity tocontrol the appearance of the S
C phase formation by only varying the cooling rate. Possiblepacking structural model and formation mechanisms of this phenomenon are discussed.