Energy migration in the light-harvesting antenna of the photosynthetic bacterium Rhodospirillum rubrum studied by time-resolved excitation annihilation at 77 K.

The intensity dependence of picosecond kinetics in the light-harvesting antenna of the photosynthetic bacterium Rhodospirillum rubrum is studied at 77 K. By changing either the average excitation intensity or the pulse intensity we have been able to discriminate singlet-singlet and singlet-triplet annihilation. It is shown that the kinetics of both annihilation types are well characterized by the concept of percolative excitation dynamics leading to the time-dependent annihilation rates. The time dependence of these two types of annihilation rates is qualitatively different, whereas the dependencies can be related through the same adjustable parameter-a spectral dimension of fractal-like structures. The theoretical dependencies give a good fit to the experimental kinetics if the spectral dimension is equal to 1.5 and the overall singlet-singlet annihilation rate is close to the value obtained at room temperature. The percolative transfer is a consequence of spectral inhomogeneous broadening. The effect is more pronounced at lower temperatures because of the narrowing of homogeneous spectra.     

Low-Intensity picosecond fluorescence kinetics and excitation dynamics in barley chloroplasts

The fluorescence decays of barley chloroplasts have been measured by single-photon counting with tunable picosecond dye laser excitation. The fluorescence decays of dark-adapted chloroplasts are best fitted to a sum of three exponential lifetime components with lifetimes of 112, 380 and 2214 ps. The relative magnitude of each component is shown to be dependent on the excitation wavelength and collected emission wavelength. The excitation wavelength dependence is correlated with the Photosystem (PS) I and PS II action study of Ried [36] and with the measured pigment distributions in the photosynthetic unit [37,41]. Experiments varying the single excitation pulse intensity from 10⁸ to 10¹² photons/cm² pulse show that our results are not distorted by singlet-singlet annihilation. Unflowed samples where the cloroplasts are under constant illumination show 2-fold increases in quantum yield of fluorescence primarily in the two longer lifetime components. Theoretical calculations of Shipman [31] on an isolated reaction center with a homogeneous antenna are discussed and the principles extended to discussion of the measured barley chloroplast fluorescence decay components in terms of photosynthetic unit light-harvesting array models and earlier experimental work. Our data support a photosynthetic unit model in which 70–90% of the photons absorbed are quenched by either PS I or efficiently quenching PS II in a process where the fluorescence lifetime is 100 ps. The origin of the intermediate 380 ps. component is probably due to excitation transfer to a PS II reaction center in a redox state which quenches less efficiently.     

Exciton Annihilation in the Two Photosystems in Chloroplasts at 100°K

The fluorescence yield (F) of spinach chloroplasts at 100°K measured at 735 nm (photosystem I fluorescence—F 735) and at 685 nm (photosystem II fluorescence—F 685) has been determined with different modes of laser excitation. The modes of excitation included a single picosecond pulse, sequences of picosecond pulses (4, 22, and 300 pulses spaced 5 ns apart) and a single nonmode-locked 2-μs pulse (MP mode). The F 735/F 685 intensity ratios decrease from 1.62 to 0.61 when a single picosecond pulse (or low-power continuous helium-neon laser) is replaced by excitation with the 300-ps pulse train (PPT mode) or MP mode. In the PPT mode of excitation, the 735-nm fluorescence band is quenched by a factor of 45 as the intensity is increased from 10¹⁵ to 10¹⁸ photons/cm² per pulse train and the 685-nm fluorescence is quenched by a factor of 10. In the MP mode, the quenching factors are 25 and 7, respectively, in the same intensity range. Fluorescence quantum yield measurements with different picosecond pulse sequences indicate that relatively long-lived quenching species are operative, which survive from one picosecond pulse to another within the pulse train. The excitonic processes possible in the photosynthetic units are discussed in detail. The differences in the quenching factors between the MP and PPT modes of excitation are attributed to singlet-singlet annihilation, possible when picosecond pulses are utilized, but minimized in the MP mode of excitation. The long-lived quenchers are identified as triplets and/or bulk chlorophyll ions formed by singlet-singlet annihilation. The preferential quenching in photosystem I is attributed to triplet excitons. The influence of heating effects, photochemistry, bleaching, and two-photon processes is also considered and is shown to be negligible.     

The triplet exciton of chlorophyll a and carotenoid in solution and in photosynthetic antenna proteins

We have observed the development and decay of triplet excitons formed in the ‘antenna’ chlorophyll $\text{a}\text{b}$ protein complex by high-intensity laser excitation. The carotenoid triplet (³Car) appeared 5 ns after excitation in the protein isolation, commonly termed CP-II; the risetime in a larger antenna particle, called LHC (light-harvesting complex) was 12 ns. The quantum yield of ³Car in CP-II decreased 11-fold as intensity was increased from 10¹⁶ to 2 · 10¹⁷ photons/cm² per pulse. The effect is attributed to exciton annihilation during the initial period of triplet formation. Above 5 · 10¹⁶ photons/cm² per s, the ³Car lifetime decreases substantially from its low intensity value of 8.7 μs. A comparison of the transient absorption spectrum of CP-II with those of chlorophyll and carotenoid in vitro indicates that ‘trapped’ chlorophyll triplets formed at high intensities. We present a simple model of destructive interaction between ³Car and chlorophyll triplets which is compatible with the observed increased rate of ³Car decay. Indirect evidence suggests similar effects occur in LHC.     

Picosecond time-resolved energy transfer in Porphyridium cruentum. Part II. In the isolated light harvesting complex (phycobilisomes)

The transfer of excitation energy between phycobiliproteins in isolated phycobilisomes has been observed on a picosecond time scale. The photon density of the excitation pulse has been carefully varied so as to control the level of exciton interactions induced in the pigment bed. The 530 nm light pulse is absorbed predominantly by B-phycoerythrin, and the fluorescence of this component rises within the pulse duration and shows a mean 1/e decay time of 70 ps. The main emission band, centred at 672 nm, is due to allophycocyanin and is prominent because of the absence of energy transfer to chlorophyll. Energy transfer to this pigment from B-phycoerythrin via R-phycocyanin produces a risetime of 120 ps to the fluorescence maximum. The lifetime of the allophycocyanin fluorescence is found to be about 4 ns using excitation pulses of low photon densities (10¹³ photons · cm^?2), but decreases to about 2 ns at higher photon densities. The relative quantum yield of the allophycocyanin fluorescence decreases almost 10 fold over the range of laser pulse intensities, 10¹³–10¹⁶ photons · cm^?2. Fluorescence quenching by exciton-exciton annihilation is only observed in allophycocyanin and could be a consequence of the long lifetime of the single exciton in this pigment.     

Chlorophyll fluorescence phenomena in chloroplasts on subnanosecond time-scales probed by picosecond pulse pairs

Fluorescence enhancement phenomena and quenching by exciton-exciton annihilation on subnanosecond and nanosecond time-scales were investigated in spinach chloroplasts utilizing picosecond laser pulse pairs (530 nm, 30 ps wide) of equal intensity, spaced apart in time by variable delays of Δt = 0−6 ns. This new method was devised to study the effect of pulse energies (1·10¹⁰–2·10¹⁵ photons per cm²) on the overall fluorescence yield in order to deduce the degree of correlation between the two pulses as a function of Δt. In the case of open reaction centers (F₀ state) in Photosystem II (PS II), it is shown that the quenching effect of excitons generated by the first pulse on the fluorescence yield of the second pulse diminishes with increasing Δt with a characteristic decorrelation time of 140 ± 60 ps. This effect is attributed to either (1) the decay of mobile excitons in the light-harvesting antenna pigment bed as these excitons migrate towards the PS II reaction centers and the associated smaller core antenna pigment pools, or (2) the decay of a quenching state of the reaction center (and/or core antenna) which appears following a rapid (less than 140 ps) trapping of the excitons initially created in the antenna pigment bed. The absence of a significant decay component of exciton quenchers with a lifetime comparable to the 300–600 ps intermediate phase of fluorescence decay kinetics suggests that this phase, although contributing to more than half of the integrated fluorescence emission signal, is not caused by freely mobile exitons migrating in a lake of pigments, but originates instead from smaller pigment pools to which the excitons have migrated. It is proposed that bimolecular exciton-exciton annihilation in these smaller domains dominates annihilation in the larger antenna pigment bed. In the case of closed reaction centers (F_max state), the decorrelation time between the two pulses is increased to 400 ± 100 ps, which is also attributed to either a mobile exciton component or to the decay of a quenching state of the reaction center. At low pulse intensities (below approx. 2 · 10¹² photons per cm²) anomalous fluorescence enhancement effects are noted, which are clearly linked to the existence of initially open PS II reaction centers. These enhancement effects are different from the well-known fluorescence induction phenomena which occur on longer time-scales, and are tentatively attributed to variations in the quenching efficiencies of transitory photochemical states of PS II reaction centers.     

Nonlinear annihilation of excitations in photosynthetic systems.

The theory of the singlet-singlet annihilation in quasi-homogeneous photosynthetic antenna systems is developed further. In the new model, the following important contributions are taken into account: 1) the finite excitation pulse duration, 2) the occupation of higher excited states during the annihilation, 3) excitation correlation effects, and 4) the effect of local heating. The main emphasis is concentrated on the analysis of pump-probe kinetic measurements demonstrating the first two above possible contributions. The difference with the results obtained from low-intensity fluorescence kinetic measurements is highlighted. The experimental data with picosecond time resolution obtained for the photosynthetic bacterium Rhodospirillum rubrum at room temperature are discussed on the basis of this theory.     

Intensity effects on the fluorescence of in vivo chlorophyll

A technique for measuring relative quantum yields of fluorescence with a picosecond streak camera is described. We show that Chlorella pyrenoidosa exhibit an intensity dependent quantum yield when irradiated with single picosecond light pulses. This effect also occurs under conditions that inhibit the activity of the reaction centres, which can therefore be excluded as the cause.When a pulse train (pulse separation 6.9 ns) was used, the quantum yield was further reduced by the light absorbed from previous pulses, which indicates the formation of a quenching species having a relatively long lifetime.Absolute quantum yields calculated from the fluorescence decay show that single excitation pulses of 3 · 10¹³ photons/cm² give results comparable to those obtained by very low intensity methods.     

Fluorescence lifetime heterogeneity in aggregates of LHCII revealed by time-resolved microscopy.

Two-photon excitation, time-resolved fluorescence microscopy was used to investigate the fluorescence quenching mechanisms in aggregates of light-harvesting chlorophyll a/b pigment protein complexes of photosystem II from green plants (LHCII). Time-gated microscopy images show the presence of large heterogeneity in fluorescence lifetimes not only for different LHCII aggregates, but also within a single aggregate. Thus, the fluorescence decay traces obtained from macroscopic measurements reflect an average over a large distribution of local fluorescence kinetics. This opens the possibility to resolve spatially different structural/functional units in chloroplasts and other heterogeneous photosynthetic systems in vivo, and gives the opportunity to investigate individually the excited states dynamics of each unit. We show that the lifetime distribution is sensitive to the concentration of quenchers contained in the system. Triplets, which are generated at high pulse repetition rates of excitation (>1 MHz), preferentially quench domains with initially shorter fluorescence lifetimes. This proves our previous prediction from singlet-singlet annihilation investigations (Barzda, V., V. Gulbinas, R. Kananavicius, V. Cervinskas, H. van Amerongen, R. van Grondelle, and L. Valkunas. 2001. Biophys. J. 80:2409-2421) that shorter fluorescence lifetimes originate from larger domains in LHCII aggregates. We found that singlet-singlet annihilation has a strong effect in time-resolved fluorescence microscopy of connective systems and has to be taken into consideration. Despite that, clear differences in fluorescence decays can be detected that can also qualitatively be understood.     

Trapping and annihilation in the antenna system of Photosystem I

The primary charge separation in Photosystem I of pea chloroplasts was measured as a photovoltage in the pico- and nanosecond time range by applying laser flashes at 532 nm of variable energy and different duration (12 ns and 30 ps, respectively). Contributions to the photovoltage from Photosystem II was eliminated by addition of 3-(3,4-dichlorophenyl)-1,1-dimethylurea and preillumination. The dependence of the photovoltage amplitude on the excitation energy could be described by an exponential saturation law when the excitation flash had a duration of 12 ns. Nearly the same dependence was found when the excitation source was the train of a mode-locked laser (approx. ten 30-ps flashes spaced by 7 ns; highest energy of a single flash, 80 μJ / cm⁻²). Even with single 30-ps flashes the photovoltage was only slightly smaller than the one elicited by 12-ns flashes of the same energy. These findings demonstrate that trapping of excitation energy by the reaction center of Photosystem I is much more effective than losses by annihilation and other loss processes. The photovoltage yield was nearly independent of the fraction of closed traps, thus demonstrating that the absorption cross section of Photosystem I is not altered by the closing of its reaction centers. By recording the rise time of the photovoltage with our highest time resolution we found that the trapping rate of the excitation energy in Photosystem I depended on the energy of the 30-ps flashes: at low excitation energies (less than 10¹⁴ photons / cm² per pulse) trapping occurred within 90 ± 15 ps and at high excitation energy (10¹⁵ photons / cm² per pulse) trapping and charge stabilization occurred within the time resolution of the apparatus, i.e., up to 50 ps. The trapping rate at low energies is in agreement with the one determined by fluorescence decay kinetics. Up to 50 ns there was no further detectable electrogenic phase (neither forward nor backward reactions). This demonstrates that all the electrogenicity, produced by the charge separation, takes place in less than 50 ps.     

Lifetime of fluorescence from light-harvesting chlorophyll a/b proteins. Excitation intensity dependence.

The fluorescence from a purified, aggregate form of the light-harvesting chlorophyll a/b protein has a lifetime of 1.2 +/- 0.5 ns at low excitation intensity, but the lifetime decreases significantly when the intensity of the 20-ps, 530-nm excitation pulse is increased above about 10(16) photons/cm2. A solubilized, monomeric form of the protein, on the other hand, has a fluorescence lifetime of 3.1 +/- 0.3 ns independent of excitation intensity from 10(14)-10(18) photons/cm2/pulse. We interpret the lifetime shortening in the aggregates and the lack of shortening in monomers in terms of exciton annihilation, facilitated in the aggregate by the larger population of interacting chlorophylls.     

Picosecond and microsecond pulse laser studies of exciton quenching and exciton distribution in spinach chloroplasts at low temperatures

Studies of the fluorescence quantum yield and decay times, determined at the emission maxima of 685 and 735 nm, using picosecond laser pulses for excitation, indicate that the pigments which are responsible for the 735 nm emission derive their energy by transfer of singlet excitons from the light-harvesting pigments and not by direct absorption of photons. Microsecond pulse laser studies of the fluorescence quantum yields at these two fluorescence wavelengths indicate that long lived quenchers (most probably triplet states), which quench singlet excitons, accumulate preferentially within the long wavelength pigment system which gives rise to the 735 nm emission band.     

Theory of Picosecond-Laser-Induced Fluorescence from Highly Excited Complexes with Small Numbers of Chromophores

The problem of singlet excitation kinetics and dynamics, especially at high excitation intensities, among a small number of chromophores of a given system has been addressed. A specific scheme for the kinetics is suggested and applied to CPII, a small chlorophyll (Chl)a/b antenna complex the fluorescence lifetime of which has been reported to be independent of excitation intensity over a wide intensity range of picosecond pulses. We have modeled the kinetics from the point of view that Chla molecules in CPII are Förster coupled so that a second excitation received by the group of Chla's either creates a state with two localized excitons or raises the first one to a doubly excited state. The data on CPII can be understood on the basis of a kinetic model that does not exclude exciton annihilation during the excitation pulse. The implied annihilation rate is consistent with our theoretical estimates of that rate obtained by applying excitation transfer theory to pairs of molecules both initially excited.     

Kinetics and spectra of photo-induced changes in the absorption of pigment-protein complexes of photosystem 1 in a picosecond range

The energy transfer from the light-harvesting antenna chlorophylls to the reaction center molecules and subsequent charge separation were investigated using a difference picosecond spectrophotometer with selective excitation. The objects were the pigment-protein complexes of photosystem 1 (Chl/P700 = 60) isolated from bean leaves. The difference absorption spectra of the excited states of light-harvesting antenna chlorophylls and the P700 photooxidation were measured. It was shown that the excited states of antenna chlorophylls were generated within 10 ps and deactivated with three-component kinetics: tau 1 = 20--45 ps, tau 2 = 100--300 ps, tau 3 greater than 500 ps. The process of the P700 photooxidation induced by the 650 nm exciting pulse was approximately monoexponential with tau equal to 15--30 ps. It is established that the P700 photooxidation is due to the efficient transfer of excitation energy from antenna chlorophylls to reaction centers.     

Kinetic model of primary energy transfer and trapping in photosynthetic membranes

The picosecond time-domain incoherent singlet excitation transfer and trapping kinetics in core antenna of photosynthetic bacteria are studied in case of low excitation intensities by numerical integration of the appropriate master equation in a wide temperature range of 4-300 K. The essential features of our two-dimensional-lattice model are as follows: Förster excitation transfer theory, spectral heterogeneity of both the light-harvesting antenna and the reaction center, treatment of temperature effects through temperature dependence of spectral bands, inclusion of inner structure of the trap, and transition dipole moment orientation. The fluorescence kinetics is analyzed in terms of distributions of various kinetic components, and the influence of different inhomogeneities (orientational, spectral) is studied.

A reasonably good agreement between theoretical and experimental fluorescence decay kinetics for purple photosynthetic bacterium Rhodospirillum rubrum is achieved at high temperatures by assuming relatively large antenna spectral inhomogeneity: 20 nm at the whole bandwidth of 40 nm. The mean residence time in the antenna lattice site (it is assumed to be the aggregate of four bacteriochlorophyll a molecules bound to proteins) is estimated to be ~12 ps. At 4 K only qualitative agreement between model and experiment is gained. The failure of quantitative fitting is perhaps due to the lack of knowledge about the real structure of antenna or local heating and cooling effects not taken into account.

     

两种不同红藻的R－藻红蛋白激发强度相关的皮秒（10~（－12）秒）荧光动力学研究

本文研究了分别从红藻多管藻（Ｐｏｌｙｓｉｐｈｏｎｉａｕｒｃｅｏｌａｔｅ）和条斑紫菜（Ｐｏｒｐｈｙｒａｙｅｚｏｅｎｓｉｓ）中提取的两种不同光谱类型的Ｒ－藻红蛋白Ｒ－ｐｈｙｃｏｅｒｙｔｈｒｉｎ激发强度相关的皮秒（１０－１２秒）荧光衰减动力学过程。结果发现：随激发光强增大,单重态－单重态激子湮灭发生（其衰减过程约为６０～８０皮秒）,并引起荧光量子产率下降。这两种Ｂ－藻红蛋白在相同光强激发下,表现出不同的单重态一单重态激子湮灭过程,主要因它们处于激发态的发色团数目不同所致。     

Singlet-singlet annihilation at low temperatures in the antenna of purple bacteria

Chromatophores of the purple photosynthetic bacteria Rhodospirillum rubrum and Rhodobacter (Rhodopseudomonas) sphaeroides were excited by means of 35-ps flashes at 532 nm of varying intensities, both at room temperature and at 4 K. With increasing exciting energy densities the integrated yield of fluorescence produced by these flashes was found to decrease considerably due to singlet-singlet annihilation. An analysis of the results showed that in R. rubrum the number of connected antenna molecules between which energy transfer is possible decreases from about 1000 to about 150 when the temperature is lowered from 298 to 4 K. In Rb. sphaeroides the B875 light-harvesting complex appears to contain about 100 connected bacteriochlorophyll (BChl) 875 molecules at 4 K, while the B800–850 complex contains about 45 BChl 850 molecules. The data are explained by a model for the antenna of Rb. sphaeroides in which units of B875, containing about four reaction centres, are separated by an array of B800–850 units that surrounds B875. By applying a random walk model we found that in both species the rate of energy transfer between neighbouring antenna molecules decreased about 10-fold upon lowering the temperature. The rate of energy transfer from antenna molecules to either open or closed reaction centres decreased only 3- to 4-fold in R. rubrum and remained approximately constant in Rb. sphaeroides upon cooling. A blue shift of the emission spectra at 4 K of both species was observed when the excitation energy density was increased to a level where singlet-singlet annihilation plays a significant role. This observation appears to support the notion that an additional long-wave pigment exists in the antenna of these bacteria.     

Energy transfer in the inhomogeneously broadened core antenna of purple bacteria: a simultaneous fit of low-intensity picosecond absorption and fluorescence kinetics.

The excited state decay kinetics of chromatophores of the purple photosynthetic bacterium Rhodospirillum rubrum have been recorded at 77 K using picosecond absorption difference spectroscopy under strict annihilation free conditions. The kinetics are shown to be strongly detection wavelength dependent. A simultaneous kinetic modeling of these experiments together with earlier fluorescence kinetics by numerical integration of the appropriate master equation is performed. This model, which accounts for the spectral inhomogeneity of the core light-harvesting antenna of photosynthetic purple bacteria, reveals three qualitatively distinct stages of excitation transfer with different time scales. At first a fast transfer to a local energy minimum takes place (approximately 1 ps). This is followed by a much slower transfer between different energy minima (10-30 ps). The third component corresponds to the excitation transfer to the reaction center, which depends on its state (60 and 200 ps for open and closed, respectively) and seems also to be the bottleneck in the overall trapping time. An acceptable correspondence between theoretical and experimental decay kinetics is achieved at 77 K and at room temperature by assuming that the width of the inhomogeneous broadening is 10-15 nm and the mean residence time of the excitation in the antenna lattice site is 2-3 ps.     

Short-pulse pump-and-probe technique for airborne laser assessment of Photosystem II photochemical characteristics

The development of a technique for laser measurement of fPhotosystem II (PS II) photochemical characteristics of phytoplankton and terrestrial vegetation from an airborne platform is described. Results of theoretical analysis and experimental study of pump-and-probe measurement of the PS II functional absorption cross-section and photochemical quantum yield are presented. The use of 10 ns probe pulses of PS II sub-saturating intensity provides a significant, up to 150-fold, increase in the fluorescence signal compared to conventional `weak-probe' protocol. Little effect on the fluorescence yield from the probe-induced closure of PS II reaction centers is expected over the short pulse duration, and thus a relatively intense probe pulse can be used. On the other hand, a correction must be made for the probe-induced carotenoid triplet quenching and singlet-singlet annihilation. A Stern-Volmer model developed for this correction assumes a linear dependence of the quenching rate on the laser pulse fluence, which was experimentally validated. The PS II saturating pump pulse fluence (532 nm excitation) was found to be 10 and 40 μmol quanta m⁻² for phytoplankton samples and leaves of higher plants, respectively. Thirty μs was determined as the optimal delay in the pump-probe pair. Our results indicate that the short-pulse pump-and-probe measurement of PS II photochemical characteristics can be implemented from an airborne platform using existing laser and LIDAR technologies. This revised version was published online in June 2006 with corrections to the Cover Date.     

Kinetics of picosecond bacteriochlorophyll luminescence in vivo as a function of the reaction center state

Bacteriochlorophyll (BChl) luminescence lifetimes (τ) were measured in purple bacteria Rhodospirillum rubrum and Rhodopseudomonas sphaeroides at low-excitation pulse energy with the use of a picosecond luminescence spectrochronograph of high sensitivity and high time-resolution. Average high-frequency excitation light density was changed from about 1 · 10¹³ photons · cm⁻² · s⁻¹ up to 1 · 10¹⁷ photons · cm⁻². s⁻¹. Maximal energy density in a single pulse was in the range 10⁻¹⁴–10⁻¹⁰ J/cm², which completely rules out nonlinear exciton interactions. In this range τ increased as a function of excitation light density from about 60 ps to 210 ps. Luminescence yield (ø) for the bacteria investigated measured under continuous or picosecond excitation changed in a similar manner as τ. The luminescence increase was shown to accompany the conversion of the reaction centers to the closed, photooxidized state. Luminescence decay of R. rubrum and Rps. sphaeroides chromatophores without any chemical additions was well approximated by a single exponential component both at low and at saturating intensities of exciting light. The time necessary for the primary charge separation to occur was shown to be 60 ± 10 ps. The pairwise jump-time of excitation-energy transfer, as well as excitation-diffusion characteristics were estimated from these data. On the basis of life-time measurements in the state of active photosynthesis, the quantum yield of the primary charge separation in the reaction centers was estimated to be equal to 0.95 ± 0.02. In intact cells as well as in chromatophores in the presence of reducing agents, a nanosecond component of emission decay was also observed. The relative amplitude of this component, being several percent of the picosecond one at low-excitation intensity levels, increased (2–3)-times with excitation density. Its life-time was estimated to be 3 ± 1 ns. The nanosecond component appeared only under conditions when a part of the reaction centers were converted to the closed state PQ⁻.