ENERGY-TRANSFER AND TRAPPING IN PHOTOSYSTEM-I REACTION CENTERS FROM CYANOBACTERIA

Citation
L. Dimagno et al., ENERGY-TRANSFER AND TRAPPING IN PHOTOSYSTEM-I REACTION CENTERS FROM CYANOBACTERIA, Proceedings of the National Academy of Sciences of the United Statesof America, 92(7), 1995, pp. 2715-2719
Citations number
30
Categorie Soggetti
Multidisciplinary Sciences
ISSN journal
00278424
Volume
92
Issue
7
Year of publication
1995
Pages
2715 - 2719
Database
ISI
SICI code
0027-8424(1995)92:7<2715:EATIPR>2.0.ZU;2-F
Abstract
A mutant strain of the cyanobacterium Synechocystis 6803, TolE4B, was constructed by genetic deletion of the protein that links phycobilisom es to thylakoid membranes and of the CP43 and CP47 proteins of photosy stem II (PSII), leaving the photosystem I (PSI) center as the sole chr omophore in the photosynthetic membranes. Both intact membrane and det ergent-isolated samples of PSI were characterized by time-resolved and steady-state fluorescence methods. A decay component of approximate t o 25 ps dominates (99% of the amplitude) the fluorescence of the membr ane sample. This result indicates that an intermediate lifetime is not associated with the intact membrane preparation and the charge separa tion in PSI is irreversible. The decay time of the detergent-isolated sample is similar. The 600-nm excited steady-state fluorescence spectr um displays a red fluorescence peak at approximate to 703 nm at room t emperature. The 450-nm excited steady-state fluorescence spectrum is d ominated by a single peak around 700 nm without 680-nm ''bulk'' fluore scence. The experimental results were compared with several computer s imulations. Assuming an antenna size of 130 chlorophyll molecules, an apparent charge separation time of approximate to 1 ps is estimated. A lternatively, the kinetics could be modeled on the basis of a two-doma in antenna for PSI, consistent with the available structural data, eac h containing approximate to 65 chlorophyll a molecules. If excitation can migrate freely within each domain and communication between domain s occurs only close to the reaction center, a charge separation time o f 3-4 ps is obtained instead.