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Excitons Forster radius

T p y+l)/k0j, where k j is the RC trapping rate and V is the ratio of the probabilities of finding the exciton in the antenna system and RC. It can be shown that from nine experimental observables (fluorescence and phosphorescence intensities and quantum yields, 7) qj) only one is independent. In all the transfer regimes, the observables depend only on V which is in general a function of time, intramolecular rate constants, size of the photosynthetic unit and initial conditions. Therefore, V (t) is the maximum information obtainable from the observables. These and further results representing general theoretical answers to problems l)-5) were illustrated on the case of the bacterial photosynthesis (Rhodopseudomonas viridis) where they are valid for the whole range of the physically acceptable values of the Forster radius. [Pg.1780]


See other pages where Excitons Forster radius is mentioned: [Pg.204]    [Pg.213]    [Pg.216]    [Pg.122]    [Pg.123]    [Pg.125]    [Pg.115]    [Pg.262]    [Pg.832]    [Pg.423]    [Pg.290]    [Pg.67]    [Pg.392]    [Pg.20]   
See also in sourсe #XX -- [ Pg.139 ]




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