Electronic Energy Migration on Different Time Scales: Concentration Dependence of the Time-Resolved Anisotropy and Fluorescence Quenching of Lumogen Red in Poly(methyl methacrylate)

• Published in: The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, & general theory Molecules, spectroscopy, kinetics, environment, & general theory, 2010-03, Vol.114 (10), p.3471-3482
• Main Authors: Colby, Kathryn A, Burdett, Jonathan J, Frisbee, Robert F, Zhu, Lingyan, Dillon, Robert J, Bardeen, Christopher J
• Format: Article
• Language: English
• Subjects: A: Kinetics, Spectroscopy
• ISSN: 1089-5639; 1520-5215
• DOI: 10.1021/jp910277j

Electronic energy transfer plays an important role in many types of organic electronic devices. Förster-type theories of exciton diffusion provide a way to calculate diffusion constants and lengths, but their applicability to amorphous polymer systems must be evaluated. In this paper, the perylenediimide dye Lumogen Red in a poly(methyl methacrylate) host matrix is used to test theories of exciton motion over Lumogen Red concentrations (C LR’s) ranging from 1 × 10−4 to 5 × 10−2 M. Two experimental quantities are measured. First, time-resolved anisotropy decays in films containing only Lumogen Red provide an estimate of the initial energy transfer rate from the photoexcited molecule. Second, the Lumogen Red lifetime decays in mixed systems where the dyes Malachite Green and Rhodamine 700 act as energy acceptors are measured to estimate the diffusive quenching of the exciton. From the anisotropy measurements, it is found that theory accurately predicts both the C LR −2 concentration dependence of the polarization decay time τpol, as well as its magnitude to within 30%. The theory also predicts that the diffusive quenching rate is proportional to C LR α, where α ranges between 1.00 and 1.33. Experimentally, it is found that α = 1.1 ± 0.2 when Malachite Green is used as an acceptor, and α = 1.2 ± 0.2 when Rhodamine 700 is the acceptor. On the basis of the theory that correctly describes the anisotropy data, the exciton diffusion constant is projected to be 4−9 nm2/ns. By use of several different analysis methods for the quenching data, the experimental diffusion constant is found to be in the range of 0.32−1.20 nm2/ns. Thus the theory successfully describes the early time anisotropy data but fails to quantitatively describe the quenching experiments which are sensitive to motion on longer time scales. The data are consistent with the idea that orientational and energetic disorder leads to a time-dependent exciton migration rate, suggesting that simple diffusion models cannot accurately describe exciton motion within this system.