A self-repairable high density polymer brush of poly(ethylene glycol) (PEG) is formed at the interface between cross-linked poly(dimethyl siloxane) (PDMS) and water by spontaneous surface segregation of an amphiphilic diblock copolymer consisting of PEG and PDMS. The surface reconstruction by the formation of the brush was observed as the large hysteresis of the contact angle of the water droplet. Neutron reflectivity measurement revealed that the grafting density of the polymer brush is 2.8 chain/ nm 2 , which is comparable to those of polymer brushes by the surfaceinitiated polymerization method. The formation of such a remarkably dense polymer brush by segregation can be well supported by the balance between the mixing enthalpy of PEG and water and the stretching energy of PEG.

The performance of a polymer composite material, in which inorganic fillers are dispersed, is closely related to the aggregation states and dynamics of polymer chains at the interface with the filler. In this study, the local conformation of polyisoprene (PI) at a quartz substrate interface was studied as a model system for the rubber/filler composite material. PI films were prepared from a toluene solution onto quartz substrates by a spin-coating method. Sum-frequency generation spectroscopy revealed that the local conformation of PI chains at the quartz interface depended on the spinning rate. The tilt angle of methyl groups increased with the rotational speed, probably due to the centrifugal force applied to chains and probably also the evaporation rate of the solvent during the solidification process. This result indicates that the interfacial orientation of PI chains can remain even at room temperature, which is 87 K higher than the bulk glass transition temperature (T g b ). The interfacial orientation disappeared at a temperature approximately 120 K higher than T g b .

Aggregation states of polystyrene (PS) and poly-(methyl methacrylate) (PMMA) at hydrophobic deuteratedoctadecyltrichlorosilane (OTS-d) and hydrophilic SiO x interfaces are discussed, focusing on the interaction strength between polymer and substrate. Sum-frequency generation spectroscopy revealed that PS exhibited oriented phenyl groups along the normal direction at the interface in a spin-coated film because of the centrifugal force generated during the film solidification process, whereas it did not in a solvent-cast film. This result was common for both hydrophobic and hydrophilic substrates. That is, the aggregation states of PS depended little on which kind of substrate was used. This is because the interaction between PS and the surfaces is weak. In the case of a PMMA film on the hydrophobic OTS-d substrate, the interfacial local conformation was also dependent on the method of film preparation. PMMA at the hydrophilic SiO x interface, however, exhibited oriented ester methyl groups along the direction normal to the interface, regardless of the film preparation method. This is due to a stronger interaction via hydrogen bonding between carbonyl groups of PMMA and the substrate surface.T he remarkable physical properties of polymers at surfaces and interfaces, which generally substantially deviate from those in the bulk, have been studied intensively. 1−29 One of the most striking and fascinating properties is the segmental dynamics. We have, using time-and space-selective fluorescence spectroscopy, reported that the glass transition temperature (T g ) for a typical glassy polymer, polystyrene (PS), increases in close proximity to the substrate interface and that the extent is dependent on the distance from the substrate and on the interaction with the substrate surface. 30,31 The experimental results were well supported by molecular dynamics simulation, 31 and this is not inconsistent with a recent finding of a dead layer that existed at the substrate interface. 32,33 The T g elevation at the substrate interface indicates that there is a significant effect on the aggregation states of glassy polymers at a solid substrate interface. Recently, we have applied sum-frequency generation (SFG) spectroscopy 34−36 to study the local conformation of PS chains at the solid interface in a film. 37 When a PS film was prepared on a quartz substrate by a spin-coating method, the chains were aligned in the plane at the substrate interface, resulting in the orientation of side chain phenyl groups of PS along the direction normal to the interface. 37 A dissipative particle dynamics simulation revealed that the spinning torque induced the chain orientation during the film preparation process and that the extent of the orientation was a function of the distance from the interface. This interfacial orientation of chains was not observed for a PS film prepared by a solvent-casting method. In this case, chain ends were rather oriented at the interface in a solvent-cast film because the polymer chains could reach a more stable sta...

The relaxation dynamics of polyisoprene (PI) and nitrile butadiene rubber (NBR) chains at the SiO2 interface were directly probed as a function of distance from the SiO2 surface using time-resolved evanescent wave-induced fluorescence anisotropy, dielectric relaxation spectroscopy, and sum-frequency generation spectroscopy. We found the presence of the dynamics gradient of chains in the interfacial region with the SiO2 surface and tried to assign it to the two kinds of adsorbed chains, namely, loosely and strongly adsorbed, at the interface. The segmental relaxation of chains in the strongly adsorbed layer at the interface could be slower than that of bulk chains by more than 10 orders.

Adhesion of a model rubbery material, crosslinked poly(dimethylsiloxane) (PDMS), onto a solid surface was studied by sum-frequency generation spectroscopy and X-ray photoelectron spectroscopy. To do so, here, we have focused on the adhesive deposit and insoluble layer. The former and latter were defined as the residual amount on the substrate after the peeling and residual layer after washing with a good solvent, respectively. The peel strength of a PDMS sheet adhered onto a glass plate increased with the contact time. Both adhesive deposit and insoluble layer also exhibited comparable contact time dependence. Once a hyperbranched polymer (HBP), which was segregated to the adhesive interface, was incorporated into PDMS, the peel strength and adhesive deposit decreased, although the thickness of the insoluble layer remained almost unchanged. These results suggest that the formation of loosely adsorbed chains on the solid surface, which possess not only trains but also many loop portions and tail parts, plays an important role in the macroscopic adhesion behavior of the PDMS sheet and the interfacial segregation of HBP can prevent it.