A perylene-labeled hyper-branched polymer with a mesogenic shell was observed to migrate toward a field with a large distortion of directors. This polymer was captured by disclination lines of 1/2 strength in its nematic and chiral nematic phases using a confocal fluorescence microscope. In particular, the well-aligned particle array of the hyper-branched polymers was produced by the chiral nematic phase confined in a wedge cell. The hyper-branched polymer with its mesogenic shell was completely dissolved into an isotropic phase. Immediately after a phase transition to the chiral nematic phase, numerous droplets appeared over a wide area owing to phase separation, and the free droplets moved toward the disclination lines via Brownian motion. Finally, the droplets were rapidly attracted to the disclination lines and trapped within them. Polymer Journal (2012) 44, 632-638; doi:10.1038/pj.2012.44; published online 11 April 2012Keywords: confocal fluorescence polarizing microscope; disclination line; fluorescence; hyper-branched polymer; liquid crystal INTRODUCTION Controlling the spatial arrangements of molecules or particles on different length scales is one of the crucial issues of bottom-up nanotechnology. 1,2 Recently, dispersions of colloidal particles and polymers in nematic or cholesteric phases have attracted considerable attention because they demonstrate a diversity of self-assembled arrangements, such as linear or circle chains and 2D lattices. [3][4][5][6] The long-range force of self-assembly originates from the elastic energy of the distortions produced around the particles in the nematic phase. [7][8][9][10][11][12][13][14] The particles have also been observed to be attracted to and to migrate toward a disclination or domain boundary in the nematic field. Because the director distortions of nematic liquid crystals 15,16 are large near the disclination, the elastic energy is higher near the disclination than in uniform director regions. 3 The particles near the disclination might be exposed to an attractive force toward the disclination core, where the highest director gradient is formed.In terms of particle polymers, hyper-branched polymers (HBPs), a novel class of polymer with highly branched structures and large numbers of end groups, are attractive because dendritic chain structures can be produced via an one-pot reaction, and the chemical structure and molecular weight of HBPs can be easily modified. [17][18][19][20][21][22][23] Therefore, the physical properties of the HBPs, such as solubility to a host phase, molecular weight, viscosity, refractive index and fluorescence, can be easily controlled. If the spatial distribution and arrangement of HPBs are further controlled, the range of applications of these materials will expand extensively, especially in photonics and electronics.In this paper, we synthesize perylene-labeled HBPs with mesogenic shells (1) that can be dispersed in a nematic liquid crystal and study