By J. G. Reich, E. Selkov

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We wish to underline the fact that, based on the present knowledge, we are unable to actually distinguish [P700+A0A-] and [P700+A0B-]. We have assigned to the latter radical pair the faster decay dynamics, which allows us to identify in a simple manner each of the two “parallel” charge separated states. However, this assignment is arbitrary, and further experimental investigations, possibly involving site-directed mutants of specific binding sites of the PsaA and the PsaB subunits, are needed to actually discriminate the kinetic properties of these radical pairs.

2003b). However, this suggestion holds true principally when the energy transfer to the photochemical active centre represents the main kinetic limitation to the overall excited state dynamic, which is often referred to as a purely diffusion-limited model. It is clear, that this is not the case for photosynthetic complexes, where the principal bottlenecks are discussed either in terms of the photochemical reactions only (trap-limited (Muller et al. 2003, Holzwarth et al. 2003, 2005, Slavov et al.

663 85 Figure 4. Photosystem I Core Model. A: Kinetic model mimicking the core complex of PS I, in which the internal antenna is isoenergetic with the reaction centres. Also presented are the numerical values of the rate constants, in units of ns-1, and the resulting lifetimes (inverse of the eigenvalues, units are given on the Figure). B: M: Matrix of the eigenvectors computed for initial population in the internal antenna only. Each column the eigenvector matrix corresponding to a specific eigenvalues, the inverse of which is presented in the vector λ (units are ps).

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