Anna Diller

15N photochemically induced dynamic nuclear polarization magic-angle spinning NMR analysis of the electron donor of photosystem II

In natural photosynthesis, the two photosystems that operate in series to drive electron transport from water to carbon dioxide are quite similar in structure and function, but operate at widely different potentials. In both systems photochemistry begins by photo-oxidation of a chlorophyll a, but that in photosystem II (PS2) has a 0.7 eV higher midpoint potential than that in photosystem I (PS1), so their electronic structures must be very different. Using reaction centers from 15N-labeled spinach, these electronic structures are compared by their photochemically induced dynamic nuclear polarization (photo-CIDNP) in magic-angle spinning (MAS) NMR measurements. The results show that the electron spin distribution in PS1, apart from its known delocalization over 2 chlorophyll molecules, reveals no marked disturbance, whereas the pattern of electron spin density distribution in PS2 is inverted in the oxidized radical state. A model for the donor of PS2 is presented explaining the inversion of electron spin density based on a tilt of the axial histidine toward pyrrole ring IV causing π-π overlap of both aromatic systems.

The solid-state photo-CIDNP effect

The solid-state photo-CIDNP effect is the occurrence of a non-Boltzmann nuclear spin polarization in rigid samples upon illumination. For solid-state NMR, which can detect this enhanced nuclear polarization as a strong modification of signal intensity, the effect allows for new classes of experiments. Currently, the photo- and spin-chemical machinery of various RCs is studied by photo-CIDNP MAS NMR in detail. Until now, the effect has only been observed at high magnetic fields with 13C and 15N MAS NMR and in natural photosynthetic RC preparations in which blocking of the acceptor leads to cyclic electron transfer. In terms of irreversible thermodynamics, the high-order spin structure of the initial radical pair can be considered as a transient order phenomenon emerging under non-equilibrium conditions and as a first manifestation of order in the photosynthetic process. The solid-state photo-CIDNP effect appears to be an intrinsic property of natural RCs. The conditions of its occurrence seem to be conserved in evolution. The effect may be based on the same fundamental principles as the highly optimized electron transfer. Hence, the effect may allow for guiding artificial photosynthesis.

Photo-CIDNP solid-state NMR on Photosystems I and II:what makes P680 special?

The origin of the extraordinary high redox potential of P680, the primary electron donor of Photosystem II, is still unknown. Photochemically induced dynamic nuclear polarisation (photo-CIDNP) 13C magic-angle spinning (MAS) NMR is a powerful method to study primary electron donors. In order to reveal the electronic structure of P680, we compare new photo-CIDNP MAS NMR data of Photosystem II to those of Photosystem I. The comparison reveals that the electronic structure of the P680 radical cation is a Chl a cofactor with strong matrix interaction, while the radical cation of P700, the primary electon donor of Photosystem I, appears to be a Chl a cofactor which is essentially undisturbed. Possible forms of cofactor–matrix interactions are discussed.

13C Photo-CIDNP MAS NMR on the LH1-RC Complex of Rhodopseudomonas acidophila

The electronic structures of the cofactors involved into the primary radical pairs in LH1-bound RCs of Rhodopseudomonas acidophila and in isolated RCs of Rhodobacter sphaeroides are compared by photochemically induced dynamic nuclear polariziation (photo-CIDNP) magic-angle spinning (MAS) NMR. Only minor differences in the electronic ground-state of the donor and a very similar distribution of the electron spin density in the radical pair state is observed. On the other hand, the ratio between donor and acceptor signals appears to be slightly different. The origin of the effect is discussed.

Magnetic field dependence of13C photo-CIDNP MAS NMR in plant photosystems I and II

Photochemically induced dynamic nuclear polarization is observed in the two photosynthetic reaction centers of plants, photosystem I (PSI) and photosystem II (PSII) by13C magic-angle spinning nuclear magnetic resonance (NMR) at three different magnetic fields 17.6, 9.4, and 4.7 T. There is a significant difference in field dependence detected in the light-induced signal pattern of the two photosystems. For PSII the optimal NMR enhancement factor of about 5000 is observed at 4.7 T. On the other hand, the maximal light-induced signals of PSI are observed at 9.4 T.

13C Photo-CIDNP MAS NMR Studies on Oriented Reaction Centers

In order to study the orientation dependence of photochemically induced dynamic nuclear polarization (photo-CIDNP) occurring photosynthetic reaction centers of Rhodobacter sphaeroides, magic-angle spinning (MAS) NMR has been applied to both, isotropic and oriented RC samples. The sample orientation is obtained by magic-angle oriented sample spinning (MAOSS). In contrast to original expectations, experiments and simulations show that the orientation obtained in MAOSS experiments does not induce significant spectral effects in the polarization pattern.