Photoresponsive thin films are commonly encountered as high performance coatings as well as critical component, photoresists, for microelectronics manufacture. Despite intensive investigations into the dynamics of thin glassy polymer films, studies involving reactions of thin films have typically been limited by difficulties in decoupling segregation of reacting components or catalysts due to the interfaces. Here, thin films of coumarin polyesters overcome this limitation where the polyester undergoes predominately cross-linking upon irradiation at 350 nm, while chain scission occurs with exposure to 254 nm light. Spectroscopic ellipsometry is utilized to track these reactions as a function of exposure time to elucidate the associated reaction kinetics for films as thin as 15 nm. The cross-linking appears to follow a second order kinetic rate law, while oxidation of the coumarin that accompanies the chain scission and enables this reaction to be tracked spectroscopically appears to be a first order reaction in coumarin concentration. Because of the asymmetry in the coumarin diol monomer and the associated differences in local structure that result during formation of the polyester, two populations of coumarin are required to fit the reaction kinetics; 10−20% of the coumarin is significantly more reactive, but these groups appear to undergo chain scission/oxidation at both wavelengths. These reaction rate constants are nearly independent (within 1 order of magnitude) of film thickness down to 15 nm. There is maximum rate at a finite thickness for the 254 nm exposure, which we attribute to constructive interference of the UV radiation within the polymer film, rather than typical confinement effects; no thickness dependence in reaction rates is observed for the 350 nm exposure. The utilization of a single polymer with two distinct reactions enables unambiguous investigation of thickness effects on reactions.
■ INTRODUCTIONFor nearly two decades, 1 the physical properties of polymer thin films have been investigated with an emphasis predominately on the glass transition temperature 2−4 as a function of film thickness. In many cases, a thickness dependent glass transition temperature (T g ) is found with the deviations from the bulk T g generally associated with the interfaces, 5 where T g is depressed 6,7 at a free interface (surface) and increased 8,9 at an attractive hard interface. The interactions of the polymer film with the underlying substrate or capping layer as well as the processing history 10−12 can impact the observed changes in T g . However, other physical properties of polymers under confinement can vary inconsistently with intuitive expectations based on the observed T g changes, 13−17 where typical relationships for polymers appear to breakdown for thin films, in particular for mechanical properties. This inconsistency leads to challenges in understanding a priori how polymers will behave when confined to thin films. For example, the rubbery compliance of ultrathin polymer films appears to decrease s...