PICOSECOND FLUORESCENCE KINETICS IN SPINACH CHLOROPLASTS AT LOW TEMPERATURE

Abstract— At 77 K the fluorescence from spinach chloroplasts excited using picosecond mode-locked laser pulses at 620 nm is made up of 5 separate kinetic components. Three of these are predominant at short wavelengths. between 650 and 690 nm, and they appear to correspond to the 3 decay phases seen at room temperature. The 2 new components. a 100 ps rise and a 3000 ps decay, characterize the longer (730–770 nm) wavelength fluorescence. The temperature dependence of the kinetic components of the long wavelength fluorescence shows that the 3000 ps decay accounts for essentially all of the large increase in fluorescence yield observed at low temperature. Furthermore, it appears that this increase does not result entirely from an increase in the fluorescence lifetime, as has been proposed. The dependences of these 2 new components (the 100 ps rise and 3000 ps decay) on emission wavelength and temperature are similar enough to suggest they have a common origin, presumably the chlorophyll pigment component C705. The amplitudes (yield/lifetime) of these 2 phases are approximately equal, and they are opposite in sign. Thus. we see evidence of time-resolved excitation transfer from those pigment molecules that absorb the 620 nm radiation to those that give rise to the long wavelength fluorescence at low temperature.     

FLUORESCENCE KINETICS OF SPINACH CHLOROPLASTS MEASURED WITH A PICOSECOND OPTICAL KERR GATE

Abstract. An overview of the reported chlorophyll a fluorescence lifetimes from green plant photosystems is presented and the problems encountered in the measurement of fluorescence lifetime using two currently available picosecond techniques are discussed.
The fluorescence intensity of spinach chloroplasts exposed to 10 ps flashes was measured as a function of time after the flash and wavelength of observation by the ultrafast Kerr shutter technique. Using a train of 100 pulses separated by 6ns and with an average photon flux per pulse of ˜2 times 10¹⁴ photons/cm², the fluorescence intensity at 685 nm (room temperature) was found to decay with two components, a fast one with a 56 ps lifetime, and a slow one with a 220 ps lifetime. The 730 nm fluorescence intensity at room temperature decays as a single exponential with a 100 ps lifetime. The 730 nm fluorescence lifetime was found to increase by a factor of 6 when the temperature was lowered from room temperature to 90 K while the lifetime of 685 and 695 nm fluorescence were unchanged. At room temperature, the fast and slow components at 685 nm are attributed to the emission from pigment system I (PS I) and PS II, respectively. It is likely that the absolute values of lifetimes, reported here, may increase if single ps low intensity flashes are used for these measurements.     

OXIDATION-REDUCTION REACTIONS OF P700 AND CYTOCHROME f IN FRACTION 1 PARTICLES PREPARED FROM SPINACH CHLOROPLASTS BY FRENCH PRESS TREATMENT

Abstract— –Fraction-1 particles were prepared by passing spinach chloroplasts three times through the French pressure cell and centrifuging in a sucrose gradient. With the electron donor DAD (diaminodurol or 2,3,5,6-tetramethyl-p-phenylenediamine) and ascorbate, a light-induced difference spectrum revealed the oxidation of both cytochrome f and P700 upon illumination of these particles. The oxidation of cytochrome f was completed in less than 0.5 msec. P700 and cytochrome f thus seem to be tightly bound to each other in these particles. Addition of Triton X-100 abolished the fast oxidation of cytochrome f but not that of P700. Artificial electron donors such as DAD, DCIP (2,6-dichlorophenol indophenol), and PMS (N-methylphenazonium methosulfate) were good electron donors for photoreaction 1 in these particles, while neither plastocyanin, Porphyra cytochrome 553, nor Euglena cytochrome-552 reduced P700 efficiently. However, after treatment of fraction 1 particles with Triton X-100 reduced DAD, DCIP and PMS were no longer efficient electron donors, while plastocyanin and the algal cytochromes were highly active in reducing P700. Mammalian cytochrome c was not a good electron donor either before or after Triton treatment. Measurements of the effectiveness of P700 reduction as a function of concentration in Triton-treated particles showed plastocyanin to be about four times more active than Porphyra or Euglena cytochromes which in turn were about fourteen times more active than mammalian cytochrome c. Recent studies by Murata and Brown have shown that plastocyanin is not required for the reduction of NADP in these particles with DCIP and isoascorbate as electron donors. The present investigation and that of Murata and Brown indicate that disintegration of chloroplasts with the French pressure cell and centrifugation in a sucrose gradient is the best method to separate system-1 particles having an electron-transport system in almost the native state as in chloroplasts.     

CORRELATION BETWEEN DELAYED LIGHT EMISSION AND FLUORESCENCE OF CHLOROPHYLL a IN SYSTEM II PARTICLES DERIVED FROM SPINACH CHLOROPLASTS

Abstract— The induction transient of delayed light of chlorophyll a, excited by repetitive flashes (0.5 ms in duration) and emitted 0.1 - 1.2 ms after the flashes, was measured in system II particles derived from spinach chloroplasts. An uncoupler, gramicidin S, was always added to the particles in order to eliminate the influence of the phosphorylation system on the delayed light and to isolate a direct relationship between the delayed light emission and the primary photochemical reaction, except for the experiments described in the next paragraph. The yield of delayed light emission from the system II particles was found to be about three–times higher than that of chloroplasts on a chlorophyll content basis. System I particles, on the other hand, emitted much weaker delayed light than chloroplasts. Upon intermittent illumination, induction of delayed light in system II particles showed a decrease from the initial rise level to the steady-state level. The initial rise level was the maximum. The fluorescence induction, on the other hand, exhibited an increase from the initial rise level to the maximum steady-state level. The induction of both delayed light emission and fluorescence arrived at their final steady-state levels after the same period of illumination. Induction of delayed light emission was measured under various conditions that changed the oxidation-reduction state of the primary electron acceptor, X, of photoreaction II: by adding an electron acceptor and an inhibitor of electron transport, and by changing the light intensity. The state of A'was monitored by measuring the fluorescence yield. The yield of delayed light emission excited by each flash was found to depend on the amount of oxidized form of X present before the flash. To examine the role of the primary electron donor Y of photoreaction II in delayed light emission, effects of electron donors of photoreaction II such as Mn²⁺, hydroquinone and p-phenylenediamine were investigated. These agents were found to markedly decrease the yield of delayed light emission without altering the pattern of its induction. They had little effect on the induction of fluorescence. These findings are interpreted by a mechanism in which transformation of the reaction center from the form (X^-Y⁺) into (X Y) produces a singlet excitation of chlorophyll a that is the source of millisecond delayed light emission. This reaction is probably non–physiological and must be very slow if compared to the transformation of (X^-Y⁺) into (X^-Y). Since the form (X^-Y⁺) is produced when the excitation is transferred to the reaction center in the form (XY), it is expected in this scheme that the yield of delayed light emission should depend on the amount of the form (X Y) present before the excitation flashes. Electron donors stimulate transformation of the reaction center from (X^-Y⁺) into (X^-Y). Since this reaction competes with the process of delayed light emission, electron donors are expected to suppress delayed light emission.     

PICOSECOND FLUORESCENCE STUDY OF PHOTOSYNTHETIC MUTANTS OF Chlamydomonas reinhardii: ORIGIN OF THE FLUORESCENCE DECAY KINETICS OF CHLOROPLASTS

Abstract— The fluorescence decay kinetics of photosynthetic mutants of Chlamydomonas reinhardii which lack photosystem II (PS II), photosystem I (PS I), and both PS II and PS I have been measured. The PS II mutant strain8–36C exhibits fluorescence decay lifetime components of 53, 424 and 2197 ps. The fluorescence decay of a PS I mutant strain12–7 contains two major fluorescence decay components with lifetimes of 152 and 424 ps. The fluorescence decay of mutant strain C2, which lacks both PS II and PS I, is nearly single exponential with a lifetime of 2561 ± 222 ps. In simulations in which it is assumed that wild-type decays are a simple sum of the major decay components of the isolated parts of the photosynthetic unit as measured in the mutants, curves are obtained that fit the wild-type C. reinhardii fluorescence decay data when the absorption cross-sections of PS II and PS I are weighted approximately equally. The 89 ps lifetime component in the wild-type is an average of 53 and 152 ps components arising from excitation transfer to and trapping in PS I and PS II. The single step transfer time in PS I is estimated to be between 100 and 700 fs depending on assumptions about array size. We find that between two and four visits to the PS I reaction center are required before final trapping.     

LASER PULSE EXCITATION STUDIES OF THE FLUORESCENCE OF CHLOROPLASTS

Abstract. The fluorescence yield, φ, as a function of single picosecond laser pulse intensity was experimentally studied in spinach chloroplasts and for chlorophyll a in ethyl ether solution. The progressive decrease in φ with increasing incident intensity for in vivo chlorophyll was found to be adequately explained within the context of continuum bimolecular kinetics with a singlet-singlet fusion rate constant of γ=5×^-9cm^-3s^-1 at room temperature. We discuss qualitatively how the fluorescence quantum yield depends on the duration and intensity of the incident pulse. The identity of φ vs l (the number of absorbed quanta) curves at the emission maxima of 685 nm and 735 nm for single picosecond pulse mode of excitation is explained within the context of Butler's tripartite model of the fluorescence of chloroplasts at 77 K. Various models relating γ to the singlet exciton diffusion coefficient and the Förster energy transfer rate are used to infer lower bounds to these physical parameters. Predictions and supporting experimental evidence for the tripartite model are discussed.     

PICOSECOND TRANSIENT BEHAVIOR OF REACTION-CENTER PARTICLES OF PHOTOSYSTEM I ISOLATED FROM SPINACH CHLOROPLASTS. ENERGY AND ELECTRON TRANSFER UPON SINGLE AND MULTIPLE PHOTON EXCITATION

Abstract— Both [15-¹³C] and [14-¹³C] all-trans-retinals were synthesized. Bacteriorhodopsin containing [14-¹³C]retinal as a chromophore, when solubilized with octyl-β-D-glucoside, showed characteristic resonances at 125 and 118 ppm from tetramethyl silane. The former was assigned to the signal from free retinal and the latter from protonated Sehiff base. When the bacteriorhodopsin was denatured in sodium dodecyl sulfate, the signal at 118 ppm disappeared, while the signal at 125 ppm rather increased.
In the case of bacteriorhodopsin containing [15-¹³C]retinal, when solubilized with Triton X-100, a characteristic resonance at 169 ppm was distinguishable as a shoulder peak superimposed on the broad signal of carbonyl carbons and it was assigned to the signal from the protonated Sehiff base. The other signal observed at 191 ppm was from free retinal.
These results suggested that the Sehiff base of bacteriorhodopsin is protonated in the dark.     

RAPID REDUCTION OF P-700 PHOTOOXIDIZED BY A FLASH AT LOW TEMPERATURE IN SPINACH CHLOROPLASTS

Abstract—Excitation of chloroplasts at low temperature (down to 4.2 K) by short laser flashes causes largely reversible absorption changes which are attributed to the photooxidation of P-700, the primary electron donor of Photosystem I. At temperatures below 100 K the dark re-reduction of P-700⁺ is biphasic. with half-times of about 122μs and 1.7 ms. The relative contribution of the two phases varies with temperature with the fast phase becoming dominant at the lowest temperatures (˜90% at 5 K). The results are interpreted in terms of tunnelling of the electron from one or two primary accepting sites back to P-700, a process which is largely dominant over the process of charge stabilisation.     

PICOSECOND FLUORESCENCE KINETICS OF N-ALL-TRANS-RETINYLIDENE-AT-BUTYLAMINE

Fluorescence lifetimes are reported for N-all- trans -retinylidene- n -butylamine in hexane. Picosecond resolution was obtained by excitation with a single 355-nm pulse, 25 ps FWHM, from a passive mode-locked YAG-laser and detection with a high speed streak camera. The lifetime dependence on temperature and the spectral characteristics support a vibrational-torsional deactivation model of the singlet excited state of two different conformers. Additional data in decalin are consistent with this model, while the quenching in alcoholic solutions may be supported by the solvent reorientation.     

ANALYSIS OF THE COMPLEX BAND SPECTRUM OF P700 BASED ON PHOTOSELECTION STUDIES WITH PHOTOSYSTEM I PARTICLES

Abstract— The linear dichroism of the flash induced absorption changes of immobilized photosystem I reaction center particles from spinach chloroplasts has been investigated by means of the photoselection technique. Under flash excitation of predominantly β-carotenes at 500 nm, the photoinduced linear dichroism of the absorption changes has been measured in the spectral region from 620–720 nm. The most prominent feature in the spectrum of the dichroic ratio is the symmetrical pole at 687 nm. In parallel to all photoselection experiments, we recorded the light induced absorption changes of P700 under saturating flash excitation. A Gaussian deconvolution of this well-known difference spectrum of P700 has been attempted taking the additional features of the linear dichroism spectrum into account. From 670-720 nm, the best fit for both spectra was obtained by the following components:

• (1) 

  a disappearing wide band at 695.5 nm (σ= 200.0 cm⁻¹) attributed to the reduced special pair of chlorophyll a (Ch1- a );
• (2) 

  an appearing narrower band at 690 nm (σ= 120.0 cm⁻¹) with half the oscillatory strength of the former tentatively attributed to the non-oxidized moiety in the special pair; and
• (3) 

  a bathochromic bandshift centered at 688.4 nm attributed to the local electrochromic response of certain antennae Ch1- a molecules close to the primary electron donor.

The linear dichroism gives no evidence for any substructure within the absorption band of the reduced special pair.     

FLUORESCENCE SPECTROSCOPY OF A P700-CHLOROPHYLL-PROTEIN COMPLEX*

Abstract. Chlorophyll-protein complexes enriched in the Photosystem I reaction center chlorophyll (P700) exhibit a fluorescence emission maximum at 696 nm at - 196°C The height of this 696 nm emission relative to the emission at 683 nm from antenna chlorophyll a increases proportionally with the P700 concentration while the total fluorescence yield of the complex decreases. The 696 nm emission could possibly be from an absorbing form of antenna chlorophyll a that may be somewhat enriched along with P700 in Photosystem I fractions. However, evidence resulting from glycerol treatment which appears to decrease the rate of resonance energy transfer between antenna chlorophyll and P700 favors the hypothesis that the emission comes from a photooxidized P700 dimer (Chl⁺-Chl) absorbing near 690 nm. In turn, this fluorescence evidence provides additional support for the model of a P700 dimer involving exciton interaction. Absorption in the wavelength region of 450 nm specifically excites emission at 696 nm from the P700-chlorophyll complex.     

TIME-RESOLVED FLUORESCENCE STUDIES OF SPINACH CHLOROPLASTS–EVIDENCE FOR THE HETEROGENEOUS BIPARTITE MODEL

Abstract— Fluorescence lifetimes of spinach chloroplasts were measured with a modelocked dye laser and time-correlated single photon counting. Information about energy transport and functional organization of the chloroplasts is revealed by such time-resolved fluorescence studies. Quenching experiments using treatment with UV light or the chemical agent dibromothymoquinone are consistent with the notion that there is heterogeneity associated with PS II units and that such heterogeneity is reflected over the entire time range of fluorescence decay, not just in a single component. Phosphorylation experiments were also carried out which permit us to relate these kinetic studies to previous steady state observations.     

CAROTENOID TRIPLET STATE AND CHLOROPHYLL FLUORESCENCE QUENCHING IN CHLOROPLASTS AND SUBCHLOROPLAST PARTICLES

Abstract— Absorption changes attributed to the triplet state of carotenoids and to primary electron donors (P-700. P-680)^: and fluorescence quenching at several wavelengths have been measured with a single apparatus. following flash excitation with a dye or a ruby laser. Spinach chloroplasts as well as subchloroplast particles enriched in Photosystem-1 (F₁), Photosystem-2 (F₁) or the light-harvesting Chl a/h (F_III) have been examined at temperatures varying between 5 and 294 K.
The triplet state of carotenoids has been identified on the basis of its difference spectrum (having a peak at 515 nm) and decay kinetics (⋍ 7 µs at low temperature; accelerated by O₂ at 294 K). It is formed in all of the materials studied. The quantum yield of carotenoid triplet formation in chloroplasts increases at low temperature, but less than the fluorescence yield.
In most cases the fluorescence quenching recovers approximately with the same kinetics as the decay of the carotenoid triplets. The fluorescence recovery is, however, significantly faster for chloroplasts at 730 nm. Fluorescence quenching occurs in all types of materials. The ratio of fluorescence quenching to the concentration of carotenoid triplets varies with the material, being maximum in chloroplasts and minimum in F_m particles.
We conclude that the formation of the carotenoid triplet state is not limited to a few sites in the chloroplast and that a carotenoid triplet is a quencher of chlorophyll fluorescence. A detailed comparison of carotenoid triplets and fluorescence quenching gives some information concerning the organization of the pigments in the photosynthetic apparatus.     

OXYGEN QUENCHING OF CHLOROPHYLL FLUORESCENCE IN CHLOROPLASTS

Abstract— Three phases of chlorophyll a fluorescence quenching by O₂ are observed in green plants. The effects of various inhibitors on photosynthetic partial processes in chloroplasts were investigated in attempts to (1) localize the O₂-quenching sites and (2) assess possible physiological significance of O₂-quenching. Our results localize the most sensitive (and presumably functionally important) phase to a site between plastoquinone and the photosystem I acceptor, chlorophyll (P₇₀₀), possibly plastocyanin. It is suggested that PC may transfer electrons to oxygen in addition to P₇₀₀.     

PICOSECOND TIME RESOLVED FLUORESCENCE OF CHLOROPHYLL IN VIVO

Abstract. The published data concerning the fluorescence kinetics of chlorophyll a in various photosynthetic species are reviewed. The effects of singlet-singlet and singlet-triplet annihilation induced by excessively high incident light intensities are discussed and related to the changes produced in the fluorescence lifetimes and quantum yields. We also review the fluorescence lifetimes of Chlorella pyrenoidosa and spinach chloroplast fragments under a variety of experimental conditions; these measurements were performed at single pulse excitation intensities of less than 5 × 10¹³ photons cm^–2 where distortion due to annihilation processes is negligible. Evidence for and against a time dependent rate equation for energy migration will be discussed with reference to the authors' work on in vitro systems.     

A CORRELATION OF EPR SPINS WITH P700 IN SPINACH SUBCHLOROPLAST PARTICLES

Abstract— The ratio of the concentrations of P₇₀₀, as measured by oxidized-minus-reduced (also light-minus-dark) spectroscopy, and electron paramagnetic resonance (EPR) signal I, as measured by EPR spectroscopy, were determined on aliquots of photosystem I spinach subchloroplast particles. The results substantiated a 1:1 ratio with a precision of ±25%. This constitutes correlative evidence that P₇₀₀ is the molecular source of the EPR signal I.     

A SINGLE PULSE PICOSECOND LASER STUDY OF EXCITON DYNAMICS IN CHLOROPLASTS

Abstract. Using single picosecond laser pulses at 610 nm, the fluorescence yield (φ) of spinach chloroplasts as a function of intensity ( I ) (10¹²-10¹⁶ photons/pulse/cm²) was studied in the range of 21–300 K. The quantum yield decreases with increasing intensity and the φ vs I curves are identical at the emission maxima of 685 and 735 nm. This result is interpreted in terms of singlet exciton-exciton annihilation on the level of the light-harvesting pigments which occurs before energy is transferred to the Photosystem I pigments which emit at 735 nm.
The yield φ is decreased by factors of 12 and 43 at 300 and 21 K, respectively. The shapes of the φ vs I curves are not well accounted for in terms of a model which is based on a Poisson distribution of photon hits in separate photosynthetic units, but can be satisfactorily described using a one-parameter fit and an exciton-exciton annihilation model. The bimolecular annihilation rate constant is found to be γ= (5–15) times 10^-9cm³s^-1 and to exhibit only a minor temperature dependence. Lower bound values of the singlet exciton diffusion coefficient (≥ 10^-3cm²s^-1), diffusion length (≥ 2 times 10^-6cm) and Förster energy transfer rates (≥ 3 ≥ 10¹⁰s^-1) are estimated from γ using the appropriate theoretical relationships.     

PICOSECOND FLUORESCENCE STUDIES OF EXCITON MIGRATION AND ANNIHILATION IN PHOTOSYNTHETIC SYSTEMS. A REVIEW*

Abstract. In this paper we review picosecond fluorescence studies of exciton dynamics in photosynthesis. We discuss some of the exciton interactions that led to artifacts in early picosecond data and outline procedures for avoiding their presence. In the case of high intensity single pulse excitation (> 10¹³ photons cm²), the dominant mechanism is singlet-singlet fusion, manifesting itself by a decrease in the observed lifetime and quantum efficiency of fluorescence. The manner in which excitons interact in vivo provides an indicator of the topology of the photosynthetic unit (PSU). The shape of the fluorescence quenching curve, as a function of intensity, in particular, can be used to test various models. In addition to fluorescence quenching curves, we also report the results of fluorescence decay following ps laser flashes, using an ultrafast streak camera in four types of systems: (1) organic crystal anologues, (2) chromatophores of various mutants of the photosynthetic bacteria, Rhodopseudomonas sphaeroides, (3) intact cells of the green alga, Chlorella and (4) chloroplasts of higher plants (e.g. spinach).     

SUPPRESSION OF LIPID PHOTOPEROXIDATION BY QUERCETIN AND ITS GLYCOSIDES IN SPINACH CHLOROPLASTS

Abstract— Quercetin, quercitrin and rutin suppressed lipid photoperoxidation in spinach chloroplasts in the presence of 100 μ M carbonylcyanide m -chlorophenylhydrazone (CCCP) or 100 μ M methyl viologen (MV). Fifty percent inhibition of lipid peroxidation by quercetin was observed between 30 and 50 μ M . Concentrations of quercetin and rutin higher than 100 μ M were required to obtain 50% inhibition. Ouercitrin was more effective than rutin in the suppression of lipid photoperoxidation.
Photooxidation of the flavonols by chloroplasts in the presence of MV was suppressed by superoxide dismutase (SOD) more than 90%, and the rates of the oxidation decreased in order of quercetin, quer citrin and rutin suggesting that the reactivity of the flavonols with O₂-decreased in that order. The photooxidation of the flavonols by CCCP-poisoned chloroplasts was partially suppressed by SOD. Radicals generated in the course of lauroyl peroxide degradation also oxidized the flavonols and the oxidation was insensitive to SOD. In these experiments, oxidation rate of quercetin was faster than those of its glycosides. The results obtained suggest that flavonols can function as antioxidants in chloroplasts by scavenging both O₂-and the radicals formed during lipid peroxidation.