Previous attempts to interpret the time-resolved electron paramagnetic resonance spectra of photosynthetic bacteria have been based on the premise that electron spin polarization arises in the primary radical pair (P+I-) formed by photoinduced charge separation. The observed spectrum is assumed to b
Electron paramagnetic resonance of the primary radical pair [D·+ φA·−] in reaction centers of photosynthetic bacteria
✍ Scribed by I.I. Proskuryakov; I.B. Klenina; P.J. Hore; M.K. Bosch; P. Gast; A.J. Hoff
- Publisher
- Elsevier Science
- Year
- 1996
- Tongue
- English
- Weight
- 662 KB
- Volume
- 257
- Category
- Article
- ISSN
- 0009-2614
No coin nor oath required. For personal study only.
✦ Synopsis
Using continuous wave EPR spectroscopy with a high time resolution, a new short-lived signal at g = 2 is observed in bacterial photosynthetic reaction centers in which electron transfer past the bacteriopheophytin @A is blocked. This signal decays with a time constant equal to the rise time of the triplet state of the primary donor 3D, and is therefore attributed to the primary radical pair [D'+ @A-1. Applying the theory of spin-correlated radical pairs, the spectrum could he satisfactorily simulated, yielding the following magnetic interaction parameters between D'+ and @A-: exchange interaction Jo+ = -0.9 + 0.1 mT and Jo, = -1.7 + 0.1 mT for reaction centers of Rhodobacter sphaeroides R26 and Rhodopseudomonas viridis, respectively, and an axial dipolar interaction D,* = -3.0 + 0.5 mT for Rhodopseudomonus viridis. The implications of the magnitude and sign of the exchange parameters for the energetics of photosynthetic electron transfer are discussed.
📜 SIMILAR VOLUMES
Time-resolved spectroscopy in conjunction with magnetic-field-dependent recombination dynamics of the primary radical ion pair in reaction centers of Rb. sphaeroides R26, were used to analyze the mechanism of electron transfer from the bacteriochlorophyll dimer in its excited singlet state ( 'P\*) t
The multipicosecond nonexponential decay of the electronically excited primary electron donor, P \*, observed in isolated photosynthetic reaction centers, is just as readily explained by multistep homogeneous electron transfer as by single-step heterogeneous transfer. With the aid of a one-antenna-s