Distance-dependent energy transfer occurs from the Metal-toLigand Charge Transfer (MLCT) excited state RuðbpyÞ 3 2þÃ to an anthracene-acrylate derivative (Acr-An) incorporated into the polymer network of a semirigid poly(ethyleneglycol)dimethacrylate monolith. Following excitation, RuðbpyÞ 3 2þÃ to Acr-An triplet energy transfer occurs followed by long-range, Acr-3 An-Acr-An → Acr-An-Acr-3 An, energy migration. With methyl viologen dication (MV 2þ ) added as a trap, Acr-3 An þ MV 2þ → Acr-An þ þ MV þ electron transfer results in sensitized electron transfer quenching over a distance of approximately 90 Å.luminescence | time-resolved spectroscopy | polymer matrix M olecular level electron and energy transfer in rigid and semirigid media are important in applications from imaging to electron transfer in biological membranes (1-4). In photosystem II, the chlorophyll singlet excited state 1 P 680 Ã is formed by light absorption by an antenna complex followed by highly efficient long-range energy transfer sensitization (5). Oxidative quenching of 1 P 680 Ã is followed by electron transfer activation of the Oxygen Evolving Complex (OEC) where water is oxidized to oxygen.Although well understood in solution (6-10), molecular level electron and energy transfer are less well understood in rigid media where diffusion is inhibited and reaction barriers significantly altered (11). There is theoretical (12, 13) and experimental insight into both processes in rigid media with the latter studied largely in low temperature glasses and, to a lesser extent, in plastics and polymeric films (14-17). Important fundamental issues remain to be elucidated along with the possible exploitation of randomly oriented, fixed site geometries in local and long-range electron and energy transfer applications.Poly(ethyleneglycol)dimethacrylate (PEG-DMA) films and monoliths, Fig. 1A, or photochemical polymerization under mild conditions (21, 22) to give optically transparent materials with features conformable to the nanoscale. They have proven useful in exploring medium effects on the properties of Metal-to-Ligand Charge Transfer (MLCT) excited states (23). Here, we report the use of a MLCT excited state in demonstrating sensitized electron transfer induced by ultralong-range energy transfer over a distance of approximately 90 Å.Structures relevant to the study are shown in Fig. 1A. They include the PEG-DMA derivative with n ¼ 9 (PEG-DMA550), the salt ½RuðbpyÞ 3 ðPF 6 Þ 2 , (bpy is 2,2′-bipyridine), and an acrylate derivative of anthracene (Acr-An). The acrylate tail allows the energy and electron transfer active anthracene group to be incorporated into the polymer network as it forms. Fig. 1 B and C show corrected emission spectra and emission decay profiles, respectively, for RuðbpyÞ 3 2þÃ with and without added Acr-An in poly-PEG-DMA550. The data provide clear evidence for emission quenching by Acr-An. Emission intensity measurements show that quenching was 55% complete with 300 mM AcrAn in the initial solution. Time-resolved emission measure...