Lateral energy transfer model for adjacent light-harvesting antennae rods of C-phycocyanins

Modeling of excitation transfer pathways have been carried out for the structure of Spirulina platensis C-phycocyanin. Calculations by Förster mechanism using the crystal structure coordinates determined in our laboratory indicate ultra-fast lateral energy transfer rates between pairs of chromophores attached to two adjacent hexamer disks. The pairwise transfer times of the order of a few pico-seconds correspond to resonance transitions between peripheral β155 chromophores. A quantitative lateral energy transfer model for C-phycocyanin light-harvesting antenna rods that is suggestive to its native structural organization emerges from this study.     

Polarized absorption picosecond kinetics as a probe of energy transfer in phycobilisomes of Synechococcus 6301

The energy transfer between C-phycocyanin chromophores in intact phycobilisomes of Synechococcus 6301 is shown to lead to an anisotropy relaxation with a lifetime of 10 ± 2 ps. However, due to the molecular order within the hexameric units of C-phycocyanin the anisotropy does not decay to zero. The Förster dipole-dipole mechanism of energy transfer can qualitatively explain these data provided that there is no back transfer of excitation energy and that the chromophore distribution is non-random. The rate of energy transfer in phycobilisomes between C-phycocyanin and allophycocyanin can best be described by a double exponential with lifetimes of 12 ± 3 and 84 ± 8 ps.     

The microenvironment around the chromophores and its changes due to the association states in C-phycocyanin isolated from the cyanobacterium Mastigocladus laminosus

The chromophore-protein interaction in C-phycocyanin was investigated as a function of the association state of the protein. Changes in the microenvironment around the chromophores were monitored by the following three indices: (1) the accessibility of a small molecule to the chromophore; (2) the fluorescence from aromatic amino acid residues; and (3) the effect of configurational changes of the chromophore on the conformation of the polypeptide chain. In the C-phycocyanin trimer, all the chromophores are shielded from the aqueous phase, probably by contact between subunits, and by a loop structure which surrounds the chromophores, even though that loop structure is not shown by X-ray analysis (Schirmer, T., Bode, W., Huber, R., Sidler, W. and Zuber, H. (1985) J. Mol. Biol. 184, 257–277). The polypeptide folding depends on the electronic structure of the chromophores; the oxidized chromophore of the α subunit inhibits the formation of the trimer and the reduced state of the chromophore of the α subunit allows the formation of trimers, in which the chromophores have the same electronic structure as in the monomers. The fluorescence from the aromatic amino acid residues showed that the conformational changes were induced by the reduced chromophore. These results indicate that the chromophore structure and the protein conformation affect each other. A definite configuration of the chromophore and also a definite conformation of the polypeptide are necessary for the intact energy transfer within C-phycocyanin.     

Computer simulation of energy migration in the C-phycocyanin of the blue-green algae Agmenellum Quadruplicatum

Two methods for simulation of energy migration in the C-phycocyanin fragments of PBS were developed. Both methods are based on the statistical analysis of an excitation behavior in modeling complexes with a limited number (up to hundreds) of chromophores using the Monte-Carlo approach and calculation of migration rates for the system of linear balance equations. Energy migration rates were calculated in the case of C-phycocyanin of the blue-green algae Agmenellum quadruplicatum. The main channels of energy migration were determined in a monomer, trimer, hexamer, and in the rods consisting of 2-4 hexamers. The influence of the “screw” angle between two adjoining trimers of hexamer on the rates of energy migration and on its efficiencies in 1-4 hexamers was also estimated. The analysis was made for the average (random) and real orientation of chromophores in the C-phycocyanin. For both cases the optimal angle values were determined and the one for real C-phycocyanin structure was found to be very close (Δø ≤ 5°) to the optimal angle calculated.     

Picosecond study of energy-transfer kinetics in phycobilisomes of Synechococcus 6301 and the mutant AN 112

Excitation-energy-transfer kinetics in isolated phycobilisomes from the cyanobacterium Synechococcus 6301 (Anacystis nidulans) and the mutant AN 112 (rods containing one hexameric C-phycocyanin unit only) was investigated by picosecond absorption and fluorescence techniques. The different chromophores in the phycobilisomes were selectively excited. A lifetime component of about 10 ps was found for both C-phycocyanin and allophycocyanin in both types of phycobilisomes. We assign these signals to a transfer of excitation energy from sensitizing (‘s’) to fluorescing (‘f’) chromophores within C-phycocyanin and allophycocyanin units. A 10 ps component was also observed in the anisotropy relaxation measurements. The anisotropy decay is attributed mainly to differently oriented transition dipole moments of ‘s’- and ‘f’-chromophores and partially to ‘f’ → ‘f’ transfer. An absorption recovery signal of τ ≈ 90 ps at λ ≤ 630 nm in phycobilisomes of Synechococcus 6301 is reduced to 40–50 ps in AN 112 phycobilisomes. This is rationalized in terms of a decreased rod → core transfer time in the shorter rods of AN 112. The 40–50 ps lifetime of fluorescence and absorption recovery in AN 112 phycobilisomes is assigned mainly to a rate-limiting transfer step between C-phycocyanin and the allophycocyanin core. A decay component of allophycocyanin τ ≈ 50 ps was observed both in absorption recovery measurements and in fluorescence decay. It is assigned to energy transfer to the terminal chromophores. The final emitter(s) of the phycobilisomes from AN 112 have fluorescence lifetimes of 1.9 and 1.3 ns. We find a good correlation in the fluorescence kinetics between the decay times of phycocyanin and allophycocyanin and the fluorescence risetimes of the terminal emitters.     

Crystal structure of a light-harvesting protein C-phycocyanin from Spirulina platensis

The crystal structure of C-phycocyanin, a light-harvesting phycobiliprotein from cyanobacteria (blue-green algae) Spirulina platensis has been solved by molecular replacement technique. The crystals belong to space group P2(1) with cell parameters a = 107.20, b = 115.40, c = 183.04 A; beta = 90.2 degrees. The structure has been refined to a crystallographic R factor of 19.2% (R(free) = 23.9%) using the X-ray diffraction data extending up to 2.2 A resolution. The asymmetric unit of the crystal cell consists of two (alphabeta)6-hexamers, each hexamer being the functional unit in the native antenna rod of cyanobacteria. The molecular structure resembles that of other reported C-phycocyanins. However, the unique form of aggregation of two (alphabeta)6-hexamers in the crystal asymmetric unit, suggests additional pathways of energy transfer in lateral direction between the adjacent hexamers involving beta155 phycocyanobilin chromophores.     

Energy transfer kinetics in C-phycocyanin from cyanobacterium Westiellopsis prolifica studied by pump-probe techniques

The relaxation processes of C-phycocyanin at different aggregates have been investigated by pump-probe techniques. The lifetimes of ground state recovery measured at various wavelengths are analyzed by computer fitting of the kinetic data to a sum of three and four exponentials for monomers and trimers according to the nonlinear least-square principle, respectively. The shortest lifetime (about 56ps) is due to beta s----beta f transfer in one monomer, that decreases to 31ps in trimer due to the opening of new transfer channels. The second fastest component (about 151ps) in monomer is attributed tentatively to distribution of excitation energy between alpha and beta f chromophores, that decreases to about 117ps in trimer caused by redistribution of excitation energy between them. The two long-lived components (about 690ps and 1385ps for monomer, 620ps and 1320ps for trimer) from some kinds of heterogeneity in some chromophores, such as alpha and beta 1 chromophores which are emitting, show an equal amplitude ratio of 1:2 in both monomer and trimer.     

Picosecond excitation energy transfer of allophycocyanin studied in solution and in crystals

Cyanobacteria perform photosynthesis with the use of large light-harvesting antennae called phycobilisomes (PBSs). These hemispherical PBSs contain hundreds of open-chain tetrapyrrole chromophores bound to different peptides, providing an arrangement in which excitation energy is funnelled towards the PBS core from where it can be transferred to photosystem I and/or photosystem II. In the PBS core, many allophycocyanin (APC) trimers are present, red-light-absorbing phycobiliproteins that covalently bind phycocyanobilin (PCB) chromophores. APC trimers were amongst the first light-harvesting complexes to be crystallized. APC trimers have two spectrally different PCBs per monomer, a high- and a low-energy pigment. The crystal structure of the APC trimer reveals the close distance (~21 Å) between those two chromophores (the distance within one monomer is ~51 Å) and this explains the ultrafast (~1 ps) excitation energy transfer (EET) between them. Both chromophores adopt a somewhat different structure, which is held responsible for their spectral difference. Here we used spectrally resolved picosecond fluorescence to study EET in these APC trimers both in crystallized and in solubilized form. We found that not all closely spaced pigment couples consist of a low- and a high-energy pigment. In ~10% of the cases, a couple consists of two high-energy pigments. EET to a low-energy pigment, which can spectrally be resolved, occurs on a time scale of tens of picoseconds. This transfer turns out to be three times faster in the crystal than in the solution. The spectral characteristics and the time scale of this transfer component are similar to what have been observed in the whole cells of Synechocystis sp. PCC 6803, for which it was ascribed to EET from C-phycocyanin to APC. The present results thus demonstrate that part of this transfer should probably also be ascribed to EET within APC trimers.     

Crystal structure analysis and refinement at 2.5 A of hexameric C-phycocyanin from the cyanobacterium Agmenellum quadruplicatum. The molecular model and its implications for light-harvesting

The crystal structure of the light-harvesting protein-pigment complex C-phycocyanin from the cyanobacterium Agmenellum quadruplicatum has been determined by Patterson search techniques on the basis of the molecular model of C-phycocyanin from Mastigocladus laminosus. The crystal unit cell (space group P321) contains three (alpha beta)6 hexamers centred on the crystallographic triads. The hexamer at the origin of the unit cell exhibits crystallographic 32 point symmetry. The other two hexamers (independent of the former) show crystallographic 3-fold and local 2-fold symmetry. The 3-fold redundancy of the asymmetric unit of the crystal cell was used in the refinement process, which proceeded by cyclic averaging, model building and energy-restrained crystallographic refinement. Refinement was terminated with a conventional crystallographic R-value of 0.20 with data to 2.5 A resolution. The two independent hexamers of the unit cell are identical within the limits of error at all levels of aggregation. Two trimers, which closely resemble the M. laminosus C-phycocyanin, are aggregated head-to-head to form the hexamer. Both trimers fit complementarily and are held together by polar and ionic interactions. Conservation of the amino acid residues involved in protein-chromophore and intermonomer interactions suggests common structural features for all biliproteins. Most probably, the hexameric aggregation form present in the crystals is closely related to the discs of native phycobilisome rods. All tetrapyrrole chromophores are extended but with different geometries enforced by different protein surroundings. In particular, interactions of the propionic side-chains with arginine residues and of the pyrrole nitrogen atoms with aspartate residues define configuration and conformation of the chromophores. Relative chromophore distances and orientations have been determined and a preferential pathway for the energy transfer suggested. Accordingly, within a hexamer the absorbed energy is funneled to chromophore B84 and then transduced via B84 chromophores along the phycobilisome rods.     

Studies on chromophore coupling in isolated phycobiliproteins: III. Picosecond excited state kinetics and time-resolved fluorescence spectra of different allophycocyanins from Mastigocladus laminosus

The excited state kinetics of three different allophycocyanin (AP) complexes has been studied by picosecond fluorescence spectroscopy. Both the fluorescence kinetics and the decay-associated fluorescence spectra of the different complexes can be understood on the basis of a structural model for AP which uses (a) an analogy to the known x-ray determined structure of C-phycocyanin, (b) the biochemical analogies of AP and C-phycocyanin, and (c) the biochemical composition of AP-B (AP-681). A model is developed that describes the excited state kinetics as a mixture of internal conversion processes within a coupled exciton pair and energy transfer processes between exciton pairs. We found excited state relaxation times in the range of 13 ps (AP with linker peptide) up to 66 ps (AP-B). The trimeric aggregates AP 660 and AP 665 show one fast relaxation component each, as was expected on the basis of their symmetry properties. The lower symmetry of AP-B (AP-681) gives rise to two fast lifetime components (τ₁ = 23 ps and τ₂ = 66 ps) which are attributed to internal conversion and/or energy transfer between excitonic states formed by the coupling of symmetrically and spectrally nonequivalent chromophores. It is proposed that the internal conversion between exciton states of strongly coupled chromophores fulfills the requirements of the small energy gap limit. Thus, internal conversion rates in the order of tens of picoseconds are feasible. The influence of the interaction of the linker peptide on the properties of the AP trimer are manifested in the fluorescence kinetics. Lack of the linker peptide in AP 660 gives rise to a heterogeneity in the chromophore conformations and chromophore-chromophore interactions.     

Deconvolution of C-phycocyanin beta-84 and beta-155 chromophore absorption and fluorescence spectra of cyanobacterium Mastigocladus laminosus.

Absorption and fluorescence spectra of the C-phycocyanin beta-subunit were quantitatively deconvoluted into component spectra of the beta-84 and beta-155 chromophores. The deconvolution procedure was based on a theoretical treatment of polarization properties. Four kinds of spectra (absorption, emission, emission polarization, and excitation polarization) measured on C-phycocyanin isolated from the cyanobacterium Mastigocladus laminosus were used as the experimental data set. Without any assumption of spectral shape, the absorption and fluorescence spectra of both chromophores were unambiguously resolved and their fluorescence quantum yields were evaluated. By combining the spectra of the alpha-subunit, independently measured, with the resolved spectra of the beta-subunit, the fluorescence and fluorescence polarization spectra and the fluorescence quantum yield of the monomer were estimated; they agree with experimental values to within an acceptable error. Further, the matrix of energy transfer rates in the monomer was estimated; it gave a significantly different result (by up to 40%) from previously estimated ones.     

Some properties of allophycocyanin from a thermophilic blue-green alga

Allophycocyanin was purified from the extremely thermophilic blue-green alga Synechococcus lividus. It was shown to be more stable to thermal or urea denaturation than allophycocyanin from a mesophilic organisms. Its amino acid composition and spectroscopic response to pH were investigated. An analysis was made of the relatively low fluorescence polarization of allophycocyanin compared to that of a comparable sized aggregate of the biliprotein, C-phycocyanin. A rather speculative conclusion was reached that suggests that the lower polarization of allophycocyanin may be caused by orientations or positioning of the chromophores that are more favorable for intra-protein energy transfer.     

X-ray structure of C-phycocyanin from Galdieria phlegrea: Determinants of thermostability and comparison with a C-phycocyanin in the entire phycobilisome

Galdieria phlegrea is a polyextremophilic red alga belonging to Cyanidiophyceae. Galdieria phlegrea C-phycocyanin (GpPC), an abundant light-harvesting pigment with an important role in energy capture and transfer to photosystems, is the C-phycocyanin (C-PC) with the highest thermal stability described so far. GpPC also presents interesting antioxidant and anticancer activities. The X-ray structure of the protein was here solved. GpPC is a [(αβ)₃]₂ hexamer, with the phycocyanobilin chromophore attached to Cys84α, Cys82β and Cys153β. Details of geometry and interaction with solvent of the chromophores are reported. Comparison with the structure of a C-PC in the entire Porphyridium purpureum phycobilisome system reveals that linker polypeptides have a significant effect on the local structure of the chromophores environment. Comparative analyses with the structures of other purified C-PCs, which were carried out including re-refined models of G. sulphuraria C-PC, reveal that GpPC presents a significantly higher number of inter-trimer salt bridges. Notably, the higher number of salt bridges at the (αβ)₃/(αβ)₃ interface is not due to an increased number of charged residues in this region, but to subtle conformational variations of their side chains, which are the result of mutations of close polar and non-polar residues.     

The structure at 2 A resolution of Phycocyanin from Gracilaria chilensis and the energy transfer network in a PC-PC complex

Phycocyanin is a phycobiliprotein involved in light harvesting and conduction of light to the reaction centers in cyanobacteria and red algae. The structure of C-phycocyanin from Gracilaria chilensis was solved by X-ray crystallography at 2.0 A resolution in space group P2(1). An interaction model between two PC heterohexamers was built, followed by molecular dynamic refinement. The best model showed an inter-hexamer rotation of 23 degrees . The coordinates of a PC heterohexamer (alphabeta)(6) and of the PC-PC complex were used to perform energy transfer calculations between chromophores pairs using the fluorescence resonance energy transfer approach (FRET). Two main intra PC ((I)beta(3)(82)-->(I)alpha(1)(84)-->(I)alpha(5)(84)-->(I)beta(6)(82) and (I)beta(3)(153)-->(I)beta(5)(153)) and two main inter PC ((I)beta(6)(82)-->(II)beta(3)(82) and (I)beta(5)(153)-->(II)beta(3)(153)) pathways were proposed based on the values of the energy transfer constants calculated for all the chromophore pairs in the hexamer and in the complex.     

Refined three-dimensional structures of two cyanobacterial C-phycocyanins at 2.1 and 2.5 A resolution. A common principle of phycobilin-protein interaction

The crystal structure of the light-harvesting protein-pigment complex C-phycocyanin (C-PC) from Mastigocladus laminosus (at 2.1 A resolution (1 A = 0.1 nm] has been refined by energy-restrained least-squares methods to a conventional R-factor of 21.7%. In the same way, the crystal structure of C-PC from Agmenellum quadruplicatum has been refined further (2.5 A, R = 18.4%); pyrrole rings C and D of the chromophore at position A84 have been corrected with respect to the previously reported structure. The two C-PC structures are very similar, 213 C alpha positions have a root-mean-square deviation of 0.49 A. Polar and ionic side-chain interactions are discussed in detail and the two subunits of C-PC from M. laminosus are compared to each other. All three chromophores are completely defined and their tetrapyrroles exhibit very similar geometry. The structure of a C-PC chromophore resembles a cleaved porphyrin which has been twisted roughly 180 degrees around the C-5-C-6 and C-14-C-15 bonds. Accordingly, the configuration/conformation of the chromophores is Z-anti, Z-syn, Z-anti (with the exception of the "configuration" of C-15 of chromophore B155, which is almost midway between Z and E). The three chromophores interact similarly with the protein. They arch around aspartate residues (A87, B87 and B39), and the nitrogens of pyrroles B and C are within hydrogen-bonding distance of one of the carboxylate oxygens. Most of the propionic side-chains of the chromophores form salt bridges with arginine and lysine residues. The updated relative chromophore distances and orientations confirm our conclusion that hexameric aggregates are probably the basic functional units, and that inter-hexameric energy transfer takes place preferentially via the central B84 chromophores.     

Functional assignment of chromophores and energy transfer in C phycocyanin isolated from the thermophilic cyanobacterium Mastigocladus laminosus

The optical characteristics and pathway of energy transfer in the C phycocyanin trimer isolated from the thermophilic cyanobacterium Mastigocladus laminosus were investigated at steady state by absorption, circular dichroism, fluorescence and fluorescence polarization spectroscopy. Based on the comparison of optical data with the 3-dimensional structure of the C-phycocyanin trimer determined by X-ray analysis (Schirmer, T., Bode, W., Huber, R., Sidler, W. and Zuber, H. (1984) in Proceedings of the Symposium on Optical Properties and Structure of Tetrapyrroles, (Blauer, G. and Sund, M., eds.), pp. 445–449, Walter de Gruyter, Berlin, and (1985) J. Mol. Biol. 184, 257–277), the functional assignment of three types of chromophore was established. An α subunit has an s chromophore and the chromophores at the positions 84 and 155 in the amino acid sequence of the β subunit are assigned as f and s chromophores, respectively. In the C phycocyanin trimer energy transfer occurs from the α chromophore in one monomer to the β_f chromophore in an adjacent monomer, and from the β_s chromophore to the β_f chromophore in the same monomer. The direction of energy flow is from the outside to the inside of the trimer, where the locus for the binding of a colourless polypeptide is postulated. In the phycobilisomes the energy concentrated at the β_f chromophores might be transferred toward the allophycocyanin core mainly by the β_f chromophores in the phycocyanin rods.     

X-ray crystallographic structure of the light-harvesting biliprotein C-phycocyanin from the thermophilic cyanobacterium Mastigocladus laminosus and its resemblance to globin structures

The structure of the biliprotein C-phycocyanin from the thermophilic cyanobacterium Mastigocladus laminosus has been determined at 3 A resolution by X-ray diffraction methods. Phases have been obtained by the multiple isomorphous replacement method. The electron density map could be improved by solvent flattening and has been interpreted in terms of the amino acid sequence. The protein consists of three identical (alpha-beta)-units which are arranged around a threefold symmetry axis to form a disc of approximate dimensions 110 A X 30 A with a central channel of 35 A in diameter. This aggregation form is supposed to be the same as that found in the rods of native phycobilisomes. Both subunits, alpha and beta, exhibit a similar structure and are related by a local twofold rotational axis. Each subunit is folded into eight helices and irregular loops. Six helices are arranged to form a globular part, whereas two helices stick out and mediate extensive contact between the subunits. The arrangement of the helices of the globular part resembles the globin fold: 59 equivalent C alpha-atoms have a root-mean-square deviation of 2 X 9 A. The chromophores attached to cystein 84 of the alpha- and beta-subunits are topologically equivalent to the haem. All three chromophores of C-phycocyanin, open-chain tetrapyrroles, are in an extended conformation. alpha 84 and beta 84 are attached to helix E (globin nomenclature), beta 155 is linked to the G--H loop. The shortest centre-to-centre distance between chromophores in trimer is 22 A.     

Structure and function of chromophores in R-Phycoerythrin at 1.9 A resolution

The crystal structure of R-Phycoerythrin (R-PE) from Polysiphonia urceolata has been refined to a resolution of 1.9 A, based on the atomic coordinates of R-PE determined at 2.8 A resolution, through the use of difference Fourier method and steorochemistry parameters restrained refinement with model adjustment according to the electron density map. Crystallographic R-factor of the refined model is 0.195 (Rfree = 0.282) from 8-1.9 A. High resolution structure of R-PE showed precise interactions between the chromophores and protein residues, which explained the spectrum characteristic and function of chromophores. Four chiral atoms of phycourobilin (PUB) were identified as C(4)-S, C(16)-S, C(21)-S, and C(20)-R. In addition to the coupling distances of 19 A to 45 A between the chromophores which were observed and involved in the energy transfer pathway, high resolution structure of R-PE suggested other pathways of energy transfer, such as the ultrashort distance between alpha140a and beta155. It has been proposed that aromatic residues in linker proteins not only influence the conformation of chromophore, but may also bridge chromophores to improve the energy transfer efficiency.     

Attempts to observe through-chain energy transfer and electron transfer on α-helical polypeptide chain

Singlet singlet energy transfer between the two terminal chromophores attached to an α-helical polypeptide chain has been studied. The transfer efficiency was satisfactorily explained by Förster's theory when the interchromophore distance was calculated from the α-helical structure. Therefore, it was concluded that no particular effect from the possible energy band structure of the α-helical conformation was detected in the end-to-end energy transfer. Similarly, end-to-end electron transfer was attempted between the electron donor acceptor pair attached to the ends of α-helcial polypeptide chain. However, no intramolecular interaction was found between the donor acceptor pair, indicating that the exciton structure of the α-helical polypeptides is not effective enough to realize through-chain electron transfer.     

Analysis of the Disk-to-Disk Energy Transfer Processes in C-Phycocyanin Complexes by Computer Simulation Technique

Based on the crystal structure and spectral properties of C-phycocyanin (C-PC) from cyanobacteria, models for complexes with 2 and 3 C-PC hexamer disks were built and the energy transfer dynamic properties were studied by the use of stochastic computer simulation approach. In addition, an experimental parameter of 0.056 ps^–1, corresponding to a time constant of 18 ps, derived from the previous time-resolved measurement, was used for simulation of the energy transfer process from the three terminal symmetrically equivalent ₈₄ chromophores of the core-linked disk to an ₈₄ chromophore of the allophycocyanin (APC) core. The simulation showed: (1) The disk-to-disk energy transfer can be as fast as several picoseconds. (2) The energy transfer efficiencies from the first disk to the core would depend on the length of the rod (i.e. the number of disks). Efficiencies of 0.95, 0.87, and 0.75 were found for the rods with 1, 2 and 3 hexamer disks, respectively. (3) The energy transfer along a rod in a native phycobilisome (PBS) is probably very close to the one-way manner. It is the core of PBS that makes the excitation energy be transferred fast in a nearly one-way manner.