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One-dimensional exciton fusion kinetics in dilute polymer blends

dc.contributor.authorKopelman, Raoulen_US
dc.contributor.authorLi, C. S.en_US
dc.contributor.authorShi, Zhong-Youen_US
dc.date.accessioned2006-04-10T13:52:12Z
dc.date.available2006-04-10T13:52:12Z
dc.date.issued1990en_US
dc.identifier.citationKopelman, R., Li, C. S., Shi, Z. -Y. (1990)."One-dimensional exciton fusion kinetics in dilute polymer blends." Journal of Luminescence 45(1-6): 40-42. <http://hdl.handle.net/2027.42/28776>en_US
dc.identifier.urihttp://www.sciencedirect.com/science/article/B6TJH-46DF68H-4D/2/c5fcc66b14c17581f1d6f6c0d39b6d9cen_US
dc.identifier.urihttps://hdl.handle.net/2027.42/28776
dc.description.abstractExciton-exciton and exciton-excimer triplet fusion kinetics is monitored in medium molecular weight P1VN/PMMA films with concentrations from 0.005 to 100% (weight), at temperatures of 77 to 300 K, via time-resolved fluorescence and phosphorescence (10 ns to 10 s). The triplet-triplet annihilation is bimolecular at short times but pseudo-monomolecular at long times. Furthermore, the heterogeneity exponent (h) is 0.5 for isolated P1VN chains, zero (classical) for pure P1VN and "fractal-like" (0hh is not monotomic with blend concentration but rather oscillates between zero and 0.5. Correlation is made with morphology changes (phase separation, filamentation). The long-lived decays do fit stretched exponentials, with a parameter [beta]=1-h. Distinction is also made between diffusion- limited and reaction-limited kinetic regimes. Furthermore, the blend topology is also studied with the aid of the time-modulation technique, in which the time decays are obtained for different excitation durations, i.e., single pulse vs. cw or multiple-pulse laser excitation, but with equal global exciton densities at the start (t=0) of the decays. As expected, the triplet exciton kinetics is dominated by short-range hops (about 5 A) and thus monitors the primary topology of the chains. At concentrations below 0.01%, the excitons are constrained to a truly one-dimensional topology. This is probably the most ideal case of a molecular wire conducting elementary excitations.en_US
dc.format.extent250482 bytes
dc.format.extent3118 bytes
dc.format.mimetypeapplication/pdf
dc.format.mimetypetext/plain
dc.language.isoen_US
dc.publisherElsevieren_US
dc.titleOne-dimensional exciton fusion kinetics in dilute polymer blendsen_US
dc.typeArticleen_US
dc.rights.robotsIndexNoFollowen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbsecondlevelNuclear Engineering and Radiological Sciencesen_US
dc.subject.hlbtoplevelScienceen_US
dc.subject.hlbtoplevelEngineeringen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumDepartment of Chemistry, University of Michigan, Ann Arbor, MI 48109, USAen_US
dc.contributor.affiliationumDepartment of Chemistry, University of Michigan, Ann Arbor, MI 48109, USAen_US
dc.contributor.affiliationumDepartment of Chemistry, University of Michigan, Ann Arbor, MI 48109, USAen_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/28776/1/0000608.pdfen_US
dc.identifier.doihttp://dx.doi.org/10.1016/0022-2313(90)90099-Wen_US
dc.identifier.sourceJournal of Luminescenceen_US
dc.owningcollnameInterdisciplinary and Peer-Reviewed


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