A refined model of the chlorosomal antennae of the green bacterium Chlorobium tepidum from proton chemical shift constraints obtained with high-field 2-D and 3-D MAS NMR dipolar correlation spectroscopy.

Heteronuclear 2-D and 3-D magic-angle spinning NMR dipolar correlation spectroscopy was applied to determine solid-state (1)H shifts for aggregated bacteriochlorophyll c (BChl c) in uniformly (13)C-enriched light harvesting chlorosomes of the green photosynthetic bacterium Chlorobium tepidum. A complete assignment of 29 different observable resonances of the 61 protons of the aggregated BChl c in the intact chlorosomes is obtained. Aggregation shifts relative to monomeric BChl c in solution are detected for protons attached to rings I, II, and III/V and to their side chains. The 2(1)-H(3), 3(2)-H(3), and 3(1)-H resonances are shifted upfield by -2.2, -1, and -3.3 ppm, respectively, relative to monomeric BChl c in solution. Although the resonances are inhomogeneously broadened and reveal considerable global structural heterogeneity, the 5-CH and the 7-Me responses are doubled, which provides evidence for the existence of at least two relatively well-defined structurally different arrangements. Ab initio quantum chemical modeling studies were performed to refine a model for the self-assembled BChl c with two different types of BChl stacks. The BChl in the stacks can adopt either anti- or syn-configuration of the coordinative bond, where anti and syn designate the relative orientation of the Mg-OH bond relative to the direction of the 17-17(1) bond. The analogy between aggregation shifts for BChl c in the chlorosome and for self-assembled chlorophyll a/H(2)O is explored, and a bilayer model for the tubular supra-structure of sheets of BChl c is proposed, from a homology modeling approach.

Photoactivation of rhodopsin: interplay between protein and chromophore.

Data in the literature suggest a finely tuned interaction between ligand (11-cis-retinal) and protein (opsin) in order to allow very efficient photoactivation of the ligand and highly vectorial rhodopsin activation with a huge increase in receptor activity. We have further investigated this interaction using ligand homologues, 13C-ligand labelling or 15N-protein labelling, in combination with Fourier transform infrared (FT-IR) and solid-state magic angle spinning (ss-MAS)-NMR spectroscopy. Using 1D rotational resonance (RR) or double-quantum heteronuclear local field (2Q-HLF) ss-MAS-NMR we report the first structure refinement of the rhodopsin chromophore in situ. These measurements yield a specification of the torsional strain in the for isomerization essential C10-C13 segment of the chromophore. This strain is thought to contribute to the high rate and stereospecificity of the photoisomerization reaction. In agreement with previous data, the C10-C13 segment region reaches a relaxed all-trans configuration at the lumirhodopsin photointermediate. MAS-NMR analysis of [15N]lysine-labelled rhodopsin reveals the presence of a 'soft' counterion, requiring intermediate water molecules for stabilization. FT-IR studies on [2H]tyrosine-labelled rhodopsin demonstrate participation of several tyrosin(at)e residues in receptor activation. One of these, probably Tyr268, is already active at the bathorhodopsin stage. Finally, the effect of ligands with single additional methyl substituents in the C10-C12 region has been investigated. They do not affect the general activation pathway, but perturb the activation kinetics of rhodopsin, suggesting steric interference with protein residues. Possible implications of these results for a structural role of water residues will be discussed, as well.