Anionic lipids play a variety of key roles in biomembrane function, including providing the immediate environment for the integral membrane proteins that catalyze photosynthetic and respiratory energy transduction. Little is known about the molecular basis of these lipid-protein interactions. In this study, x-ray crystallography has been used to examine the structural details of an interaction between cardiolipin and the photoreaction center, a key lightdriven electron transfer protein complex found in the cytoplasmic membrane of photosynthetic bacteria. X-ray diffraction data collected over the resolution range 30.0 -2.1 Å show that binding of the lipid to the protein involves a combination of ionic interactions between the protein and the lipid headgroup and van der Waals interactions between the lipid tails and the electroneutral intramembrane surface of the protein. In the headgroup region, ionic interactions involve polar groups of a number of residues, the protein backbone, and bound water molecules. The lipid tails sit along largely hydrophobic grooves in the irregular surface of the protein. In addition to providing new information on the immediate lipid environment of a key integral membrane protein, this study provides the first, to our knowledge, high-resolution x-ray crystal structure for cardiolipin. The possible significance of this interaction between an integral membrane protein and cardiolipin is considered.

Integral membrane proteins often present daunting challenges for biophysical characterization, a fundamental issue being how to select a surfactant that will optimally preserve the individual structure and functional properties of a given membrane protein. Bacterial reaction centers offer a rare opportunity to compare the properties of an integral membrane protein in different artificial lipid/surfactant environments with those in the native bilayer. Here, we demonstrate that reaction centers purified using a styrene maleic acid copolymer remain associated with a complement of native lipids and do not display the modified functional properties that typically result from detergent solubilization. Direct comparisons show that reaction centers are more stable in this copolymer/lipid environment than in a detergent micelle or even in the native membrane, suggesting a promising new route to exploitation of such photovoltaic integral membrane proteins in device applications.

General rightsThis document is made available in accordance with publisher policies. Please cite only the published version using the reference above. Full terms of use are available: http://www.bristol.ac.uk/pure/about/ebr-terms AbstractIn a quest to fabricate novel solar energy materials, the high quantum efficiency and long charge separated states of photosynthetic pigment-proteins are being exploited through their direct incorporation in bioelectronic devices. In this work, photocurrent generation by bacterial reaction center-light harvesting 1 (RC-LH1) complexes self-assembled on a nanostructured silver substrate yielded a peak photocurrent of 166 µA cm -2 under 1 sun illumination, and a maximum of over 400 µA cm -2 under 4 suns, the highest reported to date.A 2.5-fold plasmonic enhancement of light absorption per RC-LH1 complex was measured on the rough silver substrate. This plasmonic interaction was assessed using confocal fluorescence microscopy, revealing an increase of fluorescence yield and radiative rate of the RC-LH1 complexes. Nano-structuring of the silver substrate also enhanced the stability of the protein under continuous illumination by almost an order of magnitude relative to a nonstructured bulk silver control. Due to its ease of construction, increased protein loading capacity, stability and more efficient use of light, this hybrid material is an excellent candidate for further development of plasmon enhanced biosensors and bio-photovoltaic devices.3

It is generally accepted that electron transfer in bacterial photosynthesis is driven by the first singlet excited state of a special pair of bacteriochlorophylls (P*). We have examined the first steps of electron transfer in a mutant of the Rhodobacter sphaeroides reaction center in which charge separation from P* is dramatically slowed down. The results provide for the first time clear evidence that excitation of the monomeric bacteriochlorophyll in the active branch of the reaction center (B(A)) drives ultrafast transmembrane electron transfer without the involvement of P*, demonstrating a new and efficient mechanism for solar energy transduction in photosynthesis. The most abundant charge-separated intermediate state probably is P+B(A)-, which is formed within 200 fs from B(A)* and decays with a lifetime of 6.5 ps into P+H(A)-. We also see evidence for the involvement of a B(A)+H(A)- state in the alternative pathway.

We report studies ofenergy transfer from the 800-nm absorbing pigment (B800) to the 850-nm absorbing pigment (B850) of the LH2 peripheral antenna complex and from LH2 to the core antenna complex (LH1) in Rhodobacter (Rb.) sphaeroides. The B800 to B850 process was studied in membranes from a LH2-reaction center (no LH1) mutant of Rb. sphaeroides and the LH2 to LH1 transfer was studied in both the wild-type species and in LH2 mutants with blueshifted B850. The measurements were performed by using '100-fs pulses to probe the formation of acceptor excitations in a two-color pump-probe measurement. Our experiments reveal a B800 to B850 transfer time of -0.7 ps at 296 K and energy transfer from LH2 to LH1 is characterized by a time constant of -3 ps at 296 K and -5 ps at 77 K. In the blue-shifted B850 mutants, the transfer time from B850 to LH1 becomes gradually longer with increasing blue-shift of the B850 band as a result of the decreasing spectral overlap between the antennae. The results have been used to produce a model for the association between the ring-like structures that are characteristic of both the LH2 and LH1 antennae.Organization and function of the core antenna complex (LH1) and the peripheral antenna complex (LH2) of purple bacteria have been extensively studied in the past (1, 2, 29). A major step forward in this work was taken very recently when the threedimensional structure of a complex of the peripheral antenna absorbing at 800 nm (B800) and at 850 nm (B850) from Rhodopseudomonas (Rps.) acidophila was solved to high resolution showing a ninefold circular symmetry of a13 pairs (3). From this structure of LH2 and the similar circular structure of LH1 (4), it has become clear that the pigment density in these light harvesting pigments is very high, leading to short intermolecular distances and strong dipole-dipole interactions. Presently, two modes of energy transfer are considered, incoherent F6rster transfer or exciton state relaxation (5-8), and it is a challenge for future research to establish the levels of organization at which the two modes of energy transfer are operative. Until experiments and theory have produced a unified description of the energy transfer dynamics, we have chosen to describe the energy transfer steps within LH2 and LH1 and between the complexes as incoherent Forster hopping. Early work on energy transfer dynamics in photosynthetic purple bacteria (9-16) yielded information about the overall exciton lifetime in the antenna and provided a time scale for energy equilibration within individual complexes (9, 10) and over the whole antenna (11,16). In particular, the LH2 antenna is probably the most extensively studied complex. Picosecond absorption and fluorescence studies performed at room and low temperature on the LH2 pigmentprotein complex of Rhodobacter (Rb.) sphaeroides revealed that B800 -> B850 energy transfer is a very fast and temperature-The publication costs of this article were defrayed in part by page charge payment. This article must therefore be hereb...

The X-ray crystal structure of a Rhodobacter sphaeroides reaction center with the mutation Ala M260 to Trp (AM260W) has been determined. Diffraction data were collected that were 97.6% complete between 30.0 and 2.1 A resolution. The electron density maps confirm the conclusions of a previous spectroscopic study, that the Q(A) ubiquinone is absent from the AM260W reaction center (Ridge, J. P., van Brederode, M. E., Goodwin, M. G., van Grondelle, R., and Jones, M. R. (1999) Photosynthesis Res. 59, 9-26). Exclusion of the Q(A) ubiquinone caused by the AM260W mutation is accompanied by a change in the packing of amino acids in the vicinity of the Q(A) site that form part of a loop that connects the DE and E helices of the M subunit. This repacking minimizes the volume of the cavity that results from the exclusion of the Q(A) ubiquinone, and further space is taken up by a feature in the electron density maps that has been modeled as a chloride ion. An unexpected finding is that the occupancy of the Q(B) site by ubiquinone appears to be high in the AM260W crystals, and as a result the position of the Q(B) ubiquinone is well-defined. The high quality of the electron density maps also reveals more precise information on the detailed conformation of the reaction center carotenoid, and we discuss the possibility of a bonding interaction between the methoxy group of the carotenoid and residue Trp M75. The conformation of the 2-acetyl carbonyl group in each of the reaction center bacteriochlorins is also discussed.

A pathway of electron transfer is described that operates in the wild-type reaction center (RC) of the photosynthetic bacterium Rhodobacter sphaeroides. The pathway does not involve the excited state of the special pair dimer of bacteriochlorophylls (P*), but instead is driven by the excited state of the monomeric bacteriochlorophyll (B A *) present in the active branch of pigments along which electron transfer occurs. Pump-probe experiments were performed at 77 K on membrane-bound RCs by using different excitation wavelengths, to investigate the formation of the charge separated state P ؉ H A ؊ . In experiments in which P or B A was selectively excited at 880 nm or 796 nm, respectively, the formation of P ؉ H A ؊ was associated with similar time constants of 1.5 ps and 1.7 ps. However, the spectral changes associated with the two time constants are very different. Global analysis of the transient spectra shows that a mixture of P ؉ B A ؊ and P* is formed in parallel from B A * on a subpicosecond time scale. In contrast, excitation of the inactive branch monomeric bacteriochlorophyll (B B ) and the high exciton component of P (P ؉ ) resulted in electron transfer only after relaxation to P*. The multiple pathways for primary electron transfer in the bacterial RC are discussed with regard to the mechanism of charge separation in the RC of photosystem II from higher plants.

The kinetics of primary electron transfer in membrane-bound Rhodobacter sphaeroides reaction centers (RCs) were measured on both wild-type (WT) and site-directed mutant RC's bearing mutations at the tyrosine M210 position. The tyrosine was replaced by histidine (H), phenylalanine (F), leucine (L), or tryptophan (W). A mutant with histidine at both the M210 and symmetry-related L181 positions (YM210H/FL181H) was also examined. Rates of primary charge separation were determined by both single and multiple wavelength pump−probe techniques. The time constants for the decay of stimulated emission in the membrane-bound mutant RC's were approximately 27 ps (F), 36 ps (L), 72 ps (W), 5.8 ps (H), and 4.2 ps (HH), compared with 4.6 ps in WT membrane-bound RC's. For all RC's, the decay of stimulated emission was found to be multiexponential, demonstrating that this phenomenon is not a consequence of the removal of the RC from the membrane. The source of the multiexponential decay of the primary donor excited state was examined, leading to the conclusion that a distribution in the driving force (ΔG) for electron transfer cannot be the sole parameter that determines the multiexponential character. Further measurements on membrane-bound mutant RC's showed that chemical prereduction of the acceptor quinones resulted in a significant slowing of the rate of primary charge separation. This was most marked in those mutants in which the rate of charge separation had already been slowed down as a result of mutagenesis at the M210 position. The phenomenon is discussed in terms of the Coulombic interaction between QA - and the other pigments involved in electron transfer and the influence of this interaction on the driving force for charge separation.