MAGNETIC INTERACTIONS BETWEEN PHOTOSYNTHETIC REACTANTS

Supramolecular photochemistry applied to artificial photosynthesis and molecular logic devices

Supramolecular photochemical systems consist of photochemically active components such as chromophores, electron donors or electron acceptors that are associated via non-covalent or covalent interactions and that interact in some functional way. Examples of interactions are singlet–singlet energy transfer, triplet–triplet energy transfer, photoinduced electron transfer, quantum coherence and spin–spin magnetic interactions. Supramolecular photochemical “devices” may have applications in areas such as solar energy conversion, molecular logic, computation and data storage, biomedicine, sensing, imaging, and displays. This short review illustrates supramolecular photochemistry with examples drawn from artificial photosynthesis, molecular logic, analog photochemical devices and models for avian magnetic orientation.

Decoherence-assisted transport in a dimer system

The dynamics of a dimer coupled to two different environments, each in a spin star configuration under the influence of decoherence, is studied. The exact analytical expression for the transition probability in the dimer system is obtained for different situations, i.e., independent and correlated environments. In all cases considered, it is shown that there exist well-defined ranges of parameters for which decoherent interaction with the environment assists energy transfer in the dimer system. In particular, we find that correlated environments can assist energy transfer more efficiently than separate baths.

Making a Molecular Wire: Charge and Spin Transport throughpara-Phenylene Oligomers

Functional molecular wires are essential for the development of molecular electronics. Charge transport through molecules occurs primarily by means of two mechanisms, coherent superexchange and incoherent charge hopping. Rates of charge transport through molecules in which superexchange dominates decrease approximately exponentially with distance, which precludes using these molecules as effective molecular wires. In contrast, charge transport rates through molecules in which incoherent charge hopping prevails should display nearly distance independent, wirelike behavior. We are now able to determine how each mechanism contributes to the overall charge transport characteristics of a donor-bridge-acceptor (D-B-A) system, where D = phenothiazine (PTZ), B = p-oligophenylene, and A = perylene-3,4:9,10-bis(dicarboximide) (PDI), by measuring the interaction between two unpaired spins within the system's charge separated state via magnetic field effects on the yield of radical pair and triplet recombination product.

Solid state NMR studies of photoinduced polarization in photosynthetic reaction centers: mechanism and simulations

We simulate Photo-Chemically Induced Dynamic Nuclear Polarization in the 15N-solid-state NMR of 15N-labeled photosynthetic reaction centers using a Radical Pair Mechanism (RPM). According to the experimental data, the directly polarized nuclei include all eight nitrogens in the ground state of the bacteriochlorophyll special pair (P), and N-II in the bacteriopheophytin acceptor (H) [M.G. Zysmilich, A.E. McDermott, J. Am. Chem. Soc., 116 (1994) 8362-8363.] [M.G. Zysmilich, A. McDermott, J. Am. Chem. Soc., 118 (1996) 5867-5873.] [M.G. Zysmilich, A. McDermott, Proc. Natl. Acad. Sci. U.S.A., 93 (1996) 6857-6860.]; other signals are polarized in nonspecifically labeled samples, but the polarization apparently results from magnetization exchange with neighboring polarized nitrogens, and these are not treated in this work. Two quantitative models for the polarization associated with the RPM are presented and are used to test the validity of the proposal that this mechanism is cooperative in the reaction centers. The kinetic models can treat the steady state polarizations as well as the approach to steady state, and in principle could be expanded to include anisotropic effects, or pulse-probe experiments. Several features of the detailed simulations of the steady-state amplitudes and the kinetics of the approach to steady-state are compared with our data, including the signs and approximate absolute magnitudes of the polarization on the nitrogen nuclei in P and H(L), and the changes in the relative amplitudes with the change in the lifetime of the molecular triplet, photoaccumulation time, nuclear relaxation rate and illumination intensity. The simulations demonstrate that the polarization intensities are in qualitative agreement with those predicted for the RPM, including the curious observation of strong polariza-tion on the pheophytin acceptor for certain experimental conditions. However, this agreement requires efficient relaxation of the nitrogens on H(L) by 3P, due to a fortuitous low nanosecond value for the spin-lattice relaxation for the electrons in the molecular triplet of the donor, T1e of 3P. Whether this fortuitous match is valid is unproven.

Similarity of primary radical pair recombination in photosystem II and bacterial reaction centers

We report temperature and magnetic field dependent measurements of the recombination dynamics of the radical pair P680+Pheo- in D1D2cytb559 reaction centers of photosystem II and compare the results to those obtained in bacterial reaction centers. In photosystem II the rate of recombination to the groundstate is found to be slower than in the bacterial reaction centers by a factor of at least 50. This difference arises from the different redox potentials of the pigments of plant and bacterial reaction centers. In contrast, the rate of recombination to the triplet state is similar in all reaction centers, indicating a similar electronic coupling which allows us to conclude upon the structural similarity.

How carotenoids function in photosynthetic bacteria

Carotenoids are essential for the survival of photosynthetic organisms. They function as light-harvesting molecules and provide photoprotection. In this review, the molecular features which determine the efficiencies of the various photophysical and photochemical processes of carotenoids are discussed. The behavior of carotenoids in photosynthetic bacterial reaction centers and light-harvesting complexes is correlated with data from experiments carried out on carotenoids and model systems in vitro. The status of the carotenoid structural determinations in vivo is reviewed.