Quantum yield and rate of formation of the carotenoid triplet state in photosynthetic structures

The formation of the triplet state of carotenoids (detected by an absorption peak at 515 nm) and the photo-oxidation of the primary donor of Photosystem II, P-680 (detected by an absorption increase at 820 nm) have been measured by flash absorption spectroscopy in chloroplasts in which the oxygen evolution was inhibited by treatment with Tris. The amount of each transient form has been followed versus excitation flash intensity (at 590 or 694 nm). At low excitation energy the quantum yield of triplet formation (with the Photosystem II reaction center in the state Q⁻) is about 30% that of P-680 photo-oxidation. The yield of carotenoid triplet formation is higher in the state Q⁻ than in the state Q, in nearly the same proportion as chlorophyll a fluorescence. It is concluded that, for excited chlorophyll a, the relative rates of intersystem crossing to the triplet state and of fluorescence emission are the same in vivo as in organic solvent. At high flash intensity the signal of P-680⁺ completely saturates, whereas that of carotenoid triplet continues to increase.

The rate of triplet-triplet energy transfer from chlorophyll a to carotenoids has been derived from the rise time of the absorption change at 515 nm, in chloroplasts and in several light-harvesting pigment-protein complexes. In all cases the rate is very high, around 8 · 10⁷ s⁻¹ at 294 K. It is about 2–3 times slower at 5 K. The transitory formation of chlorophyll triplet has been verified in two pigment-protein complexes, at 5 K.     

Flash-induced absorption changes in Photosystem I,Radical pair or triplet state formation?

Absorption changes induced in chlorophyll protein (CP 1) particles by short laser flashes have been analyzed in order to decide whether a state lasting for a few microseconds at 21°C or 800 μs at 10 K corresponds to the biradical P-700⁺ ... A⁻₁ (A₁ being a chlorophyll a) or to a triplet state produced in a submicrosecond recombination of the preceding state. At 21°C the spectrum of the flash-induced ΔA (720–870 nm) presents a flat-topped band from 740 to 820 nm, clearly different from that of P-700⁺. A saturation curve (ΔA vs. laser energy), obtained with a 2 or 10 ns laser pulse, indicates that ΔA saturates at a value 2- or 3-times smaller than that expected on the basis of the chemical oxidation of P-700. At 21°C the size of flash-induced ΔA is slightly decreased (5–15%) when the sample is subjected to a 400 G magnetic field. The kinetics of decay are not affected; they are not affected either by the oxygen concentration. At 10 K the spectrum of the flash-induced ΔA has been measured between 650 and 1700 nm. Between 650 and 720 nm, the spectrum presents only one major negative peak at 702 nm; it is quite different from that due to the chemical oxidation of P-700 (which has additional peaks at 688 and 677 nm). Between 720 and 870 nm, the spectrum is identical to that obtained at 21°C. Above 870 nm, the spectrum includes a broad band around 1250 nm, which is absent in P-700⁺. A saturation curve leads to a maximum ΔA greater than that at 21°C and which is also greater with a 1 μs dye laser flash than with a 10 ns ruby laser flash. An analysis of the spectral data indicates that these do not fit correctly with the hypothesis of a contribution of P-700⁺ and of a chlorophyll a anion radical. They fit more closely with the hypothesis of a triplet state of P-700, a hypothesis which is discussed in relation to other experimental data.     

Energy transfer in the photochemical apparatus of flashed bean leaves

Fluorescence and energy transfer properties of bean leaves greened by brief, repetitive xenon flashes were studied at −196 °C. The bleaching of P-700 has no influence on the yield of fluorescence at any wavelength of emission. The light-induced fluorescence yield changes which are observed in both the 690 and 730 nm emission bands in the low temperature fluorescence spectra are due to changes in the state of the Photosystem II reaction centers. The fluorescence yield changes in the 730 nm band are attributed to energy transfer from Photosystem II to Photosystem I. Such energy transfer was also confirmed by measurements of the rate of photooxidation of P-700 at −196 °C in leaves in which the Photosystem II reaction centers were either all open or all closed. It is concluded that energy transfer from Photosystem II to Photosystem I occurs in the flashed bean leaves which lack the light-harvesting chlorophyll a/b protein.     

Refined purification and further characterization of oxygen-evolving and Tris-treated Photosystem II particles from the thermophilic Cyanobacterium synechococcus sp.

Highly active, monomeric and dimeric Photosystem II complexes were purified from the thermophilic cyanobacterium Synechococcus sp. by two sucrose density gradients, and the size, shape and mass of these complexes have been estimated (Rögner, M., Dekker, J.P., Boekema, E.J. and Witt, H.T. (1987) FEBS Lett. 219, 207–311). (1) Further purification could be obtained by ion-exchange chromatography, by which the 300 kDa monomer could be separated into a highly active, O₂-evolving fraction, and a fraction without O₂-evolving capacity, which has lost its extrinsic 34 kDa protein. Both showed very high reaction center activities as measured by the photoreduction of the primary quinone acceptor, Q_A, at 320 nm, being up to one reaction center per 31 Chl a molecules. (2) Tris-treatment yielded homogeneous 300 kDa particles which had lost their extrinsic 34 kDa polypeptide. Electron microscopy of this complex revealed very similar dimensions compared to the oxygen-evolving 300 kDa particle, except that the smallest dimension was decreased from about 6.5 nm to about 5.8 nm. This difference is attributed to the missing extrinsic 33 kDa protein, and the smallest dimension is attributed to the distance across the membrane. (3) Experiments are presented, allowing an estimation for the contribution of detergent to the other dimensions being about 2 × 1.5 nm for dodecyl β- -maltoside. This leads to dimensions, corrected for detergent size, of 12.3 × 7.5 nm for the monomeric form of PS II and 12 × 15.5 nm for the dimeric form. (4) From some extracts a 35 kDa, chlorophyll-binding complex could be isolated which lacks the characteristic absorbance changes of Q_A and of Chl a_II (P-680) and is therefore supposed to be a light-harvesting complex of cyanobacteria. (5) A model for the in vivo organization of PS II in cyanobacteria is discussed.     

Preparation and properties of the water-soluble chlorophyll-bovine serum albumin complexes

By mixing chlorophyll (Chl) a or b with a dense bovine serum albumin solution, the water-soluble Chl-bovine serum albumin complexes were prepared. These complexes, eluted near the void volume on a gel filtration, were separated well from unreacted bovine serum albumin, indicating an aggregation of such molecules in the complexes. Preparation of chlorophyllide (Chlide) a- or Chlide b-bovine serum albumin complex was unsuccessful, while the phytol-, and β-carotene-bovine serum albumin complexes could be obtained. Chls in the Chl-bovine serum albumin complexes had the following characteristics. (i) Main absorption peak of Chl a or b in the red region occurred at 675 nm or 652 nm, respectively. The Chl a-bovine serum albumin complex having absorption peak at 740 nm was also prepared. As compared with the stabilities of Chl a and b in Triton X-100. (ii) Both Chls in the bovine serum albumin-complexes were stable against oxidative stresses, such as photobleaching, Fenton reagent, peroxidase-H₂O₂ system. But (iii) they were easily hydrolyzed by chlorophyllase. These properties of Chls in the bovine serum albumin-complexes were similar to those of Chls in the isolated light-harvesting Chl a/b protein complex. A possible localization of Chls within the bovine serum albumin complexes was suggested that the porphyrin moiety of Chl was buried in bovine serum albumin; however, the hydrophilic edge of porphyrin ring, adjacent to the phytol group, occurred in the hydrophilic region of a bovine serum albumin molecule.     

Electron paramagnetic resonance saturation studies of P-700 reaction center chlorophyll in plant photosynthesis

Electron paramagnetic resonance (EPR) power saturation and saturation recovery methods have been used to determine the spin lattice, T₁, and spin-spin, T₂, relaxation times of P-700⁺ reaction-center chlorophyll in Photosystem I of plant chloroplasts for 10 K T 100 K. T₁ was 200 μs at 100 K and increased to 900 μs at 10 K. T₂ was 40 ns at 40 K and increased to 100 ns at 10 K. T₁ for 40 K T 100 K is inversely proportional to temperature, which is evidence of a direct-lattice relaxation process. At T = 20 K, T₁ deviates from the 1/T dependence, indicating a cross relaxation process with an unidentified paramagnetic species. The individual effects of ascorbate and ferricyanide on T₁ of P-700⁺ were examined: T₁ of P-700⁺ was not affected by adding 10 mM ascorbate to digitonin-treated chloroplast fragments (D144 fragments). The P-700⁺ relaxation time in broken chloroplasts treated with 10 mM ferricyanide was 4-times shorter than in the untreated control at 40 K. Ferricyanide appears to be relaxing the P-700⁺ indirectly to the lattice by a cross-relaxation process. The possibility of dipolar-spin broadening of P-700⁺ due to either the iron-sulfur center A or plastocyanin was examined by determining the spin-packet linewidth for P-700⁺ when center A and plastocyanin were in either the reduced or oxidized states. Neither reduced center A nor oxidized plastocyanin was capable of broadening the spin-packet linewidth of the P-700⁺ signal. The absence of diplolar broadening indicates that both center A and plastocyanin are located at a distance at least 3.0 nm from the P-700⁺ reaction center chlorophyll. This evidence supports previous hypotheses that the electron donor and acceptor to P-700 are situated on opposite sides of the chloroplast membrane. It is also shown that the ratio of photo-oxidized P-700 to photoreduced centers A and B at low temperature is 2 : 1 if P-700 is monitored at a nonsaturating microwave power.     

Evidence for complexed plastocyanin as the immediate electron donor of P-700

The reduction of P-700 by its electron donors shows two fast phases with half-times of 20 and 200 μs in isolated spinach chloroplasts. We have studied this electron transfer and the oxidation kinetics of cytochrome f.

Incubation of chloroplasts with KCN or HgCl₂ decreased the amplitude of the 20 μs phase. This provides evidence for a function of plastocyanin as the immediate electron donor of P-700.

At low concentrations of salt and sugar the fast phases of P-700⁺ reduction were largely inhibited. Increasing concentrations of MgCl₂, KCl and sorbitol (up to 5, 150 and 200 mM, respectively) were found to increase the relative amplitudes of the fast phases to about one-third of the total P-700 signal. Addition of both 3 mM MgCl₂ and 200 mM sorbitol increased the relative amplitude of the 20 μs phase to 70%. The interaction between P-700 and plastocyanin is concluded to be favoured by a low internal volume of the thylakoids and compensation of surface charges of the membrane.

The half-time of 20 μs was not changed when the amplitude of this phase was altered either by salt and sorbitol, or by inhibition of plastocyanin. This is evidence for the existence of a complex between plastocyanin and P-700 with a lifetime long compared to the measuring time. The 200 μs phase exhibited changes in its half-time that indicated the participation of a more mobile pool of plastocyanin.

Cytochrome f was oxidized with a biphasic time course with half-times of 70–130 μs and 440–860 μs at different salt and sorbitol concentrations. The half-time of the faster phase and a short lag of 30–50 μs in the beginning of the kinetics indicate an oxidation of cytochrome f via the 20 μs electron transfer to P-700. An inhibition of this oxidation by MgCl₂ suggests that the electron transfer from cytochrome f to complexed plastocyanin is not controlled by negative charges in contrast to that from plastocyanin to P-700.     

Excitation spectra for Photosystem I and Photosystem II in chloroplasts and the spectral characteristics of the distribution of quanta between the two photosystems

The parameters listed in the title were determined within the context of a model for the photochemical apparatus of photosynthesis.

The fluorescence of variable yield at 750 nm at −196 °C is due to energy transfer from Photosystem II to Photosystem I. Fluorescence excitation spectra were measured at −196 °C at the minimum, F_O, level and the maximum, F_M, level of the emission at 750 nm. The difference spectrum, F_M–F_O, which represents the excitation spectrum for F_V is presented as a pure Photosystem II excitation spectrum. This spectrum shows a maximum at 677 nm, attributable to the antenna chlorophyll a of Photosystem II units, with a shoulder at 670 nm and a smaller maximum at 650 nm, presumably due to chlorophyll a and chlorophyll b of the light-harvesting chlorophyll complex.

Fluorescence at the F_O level at 750 nm can be considered in two parts; one part due to the fraction of absorbed quanta, , which excites Photosystem I more-or-less directly and another part due to energy transfer from Photosystem II to Photosystem I. The latter contribution can be estimated from the ratio of F_O/F_V measured at 692 nm and the extent of F_V at 750 nm. According to this procedure the excitation spectrum of Photosystem I at −196 °C was determined by subtracting 1/3 of the excitation spectrum of F_V at 750 nm from the excitation spectrum of F_O at 750 nm. The spectrum shows a relatively sharp maximum at 681 nm due to the antenna chlorophyll a of Photosystem I units with probably some energy transfer from the light-harvesting chlorophyll complex.

The wavelength dependence of was determined from fluorescence measurements at 692 and 750 nm at −196 °C. is constant to within a few percent from 400 to 680 nm, the maximum deviation being at 515 nm where shows a broad maximum increasing from 0.30 to 0.34. At wavelengths between 680 and 700 nm, increases to unity as Photosystem I becomes the dominant absorber in the photochemical apparatus.     

Photochemical systems in mesophyll and bundle sheath chloroplasts of C4 plants

1. The agranal bundle sheath chloroplasts of Sorghum bicolor possess very low Photosystem II activity compared with the grana-containing mesophyll chloroplasts.

2. Sorghum mesophyll chloroplasts have a chlorophyll (chl) and carotenoid composition similar to that of spinach chloroplasts. In contrast, the sorghum bundle sheath chloroplasts have a higher chl a/chl b ratio; they are enriched in β-carotene and contain relatively less xanthophylls as compared to sorghum mesophyll or spinach chloroplasts.

3. Sorghum mesophyll chloroplasts with 1 cytochrome f, 2 cytochrome b₆ and 2 cytochrome b-559 per 430 chlorophylls have a cytochrome composition similar to spinach chloroplasts. Sorghum bundle sheath chloroplasts contain cytochrome f and cytochrome b₆ in the same molar ratios as for the mesophyll chloroplasts, but cytochrome b-559 is barely detectable.

4. The chl/P700 ratios of mesophyll chloroplasts of S. bicolor and mesophyll and bundle sheath chloroplasts of Atriplex spongiosa are similar to that of spinach chloroplasts suggesting that these chloroplasts possess an identical photosynthetic unit size to that of spinach. The agranal bundle sheath chloroplasts of S. bicolor possess a photosynthetic unit which contains only about half as many chlorophyll molecules per P700 as found in the grana-containing chloroplasts.

5. The similarity of the composition of the bundle sheath chloroplasts of S. bicolor with that of the Photosystem I subchloroplast fragments, together with their smaller photosynthetic unit and low Photosystem II activities suggests that these chloroplasts are highly deficient in the pigment assemblies of Photosystem II.     

Quantitative analysis of membrane components in a highly active O2-evolving photosystem II preparation from spinach chloroplasts

Stoichiometry of membrane components associated with Photosystem II was determined in a highly active O₂-evolving Photosystem II preparation isolated from spinach chloroplasts by the treatment with digitonin and Triton X-100. From the analysis with sodium dodecyl sulfate polyacrylamide gel electrophoresis and Triton X-114 phase partitioning, the preparation was shown to contain the reaction center protein (43 kDa), the light-harvesting chlorophyll-protein complex (the main band, 27 kDa), the herbicide-binding protein (32 kDa) and cytochrome b-559 (10 kDa) as hydrophobic proteins, and three proteins (33, 24 and 18 kDa) which probably constitute the O₂-evolution enzyme complex as hydrophilic proteins. These proteins were associated stoichiometrically with the Photosystem II reaction center: one Photosystem II reaction center, approx. 200 chlorophyll, one high-potential form of cytochrome b-559, one low-potential form of cytochrome b-559, one 33 kDa protein, one (to two) 24 kDa protein and one (to two) 18 kDa protein. Measurement of fluorescence induction showed the presence of three electron equivalents in the electron acceptor pool on the reducing side of Photosystem II in our preparation. Three molecules of plastoquinone A were detected per 200 chlorophyll molecules with high-performance liquid chromatography. The Photosystem II preparation contained four managanese atoms per 200 chlorophyll molecules.     

The P-700-chlorophyl a-protein complex and two major light-harvesting complexes of Acrocarpia paniculata and other brown seaweeds

Acrocarpia paniculata thylakoids were fragmented with Triton X-100 and the pigment-protein complexes so released were isolated by sucrose density gradient centrifugation. Three main chlorophyll-carotenoid-protein complexes with distinct pigment compositions were isolated.

1. (1) A P-700-chlorophyll a-protein complex, with a ratio of 1 P-700: 38 chlorophyll a: 4 ta-carotene molecules, had similar absorption and fluorescence characteristics to the chlorophyll-protein complex 1 isolated with Triton X-100 from higher plants, green algae and Ecklonia radiata.

2. (2) An orange-brown complex had a chlorophyll a : c₂ : fucoxanthin molar ratio of 2 : 1 : 2. This complex had no chlorophyll c₁ and contained most of the fucoxanthin present in the chloroplasts. This pigment complex is postulated to be the main light-harvesting complex of brown seaweeds.

3. (3) A green complex had a chlorophyll a : c₁ : c₂ : violaxanthin molar ratio of 8 : 1 : 1 : 1. This also is a light-harvesting complex.

The absorption and fluorescence spectral characteristics and other physical properties were consistent with the pigments of these three major complexes being bound to protein. Differential extraction of brown algal thylakoids with Triton X-100 showed that a chlorophyll c₂-fucoxanthin-protein complex was a minor pigment complex of these thylakoids.     

Studies on well-coupled Photosystem I-enriched subchloroplast vesicles — characteristics and reinterpretation of single-turnover cyclic electron transfer

The contributions of ferredoxin, P-700, plastocyanin and the cytochromes c-554, and b-563 to single-turnover electron transfer in Photosystem (PS) I-enriched subchloroplast vesicles were deconvoluted by fitting the literature-derived spectra of these components to the observed absorption data at a series of wavelengths, according to a linear least-squares method. The obtained corresponding residuals showed that the applied component spectra were satisfactory. The deconvoluted signals of cytochromes c-554 and b-563 differed in some cases significantly from the classical dual-wavelength signals recording at 554–545 nm and 563–575 (or −572) nm, due to interference from other electron-transferring components. KCN, DNP-INT (2-iodo-6-isopropyl-3-methyl-2′,4,4′-trinitrodiphenyl ether), DBMIB (2,5-dibromo-3-methyl-6-isopropyl-p-benzo-quinone) and antimycin A all inhibited electron transfer, although antimycin and DBMIB inhibited only after a few turnovers of the cytochrome bf complex. Fast flash-induced reduction of cytochrome b-563 exclusively reflected oxidant-induced reduction. Fast electron flow from cytochrome c-554 to plastocyanin and P-700 resulted in an apparent rereduction of cytochrome c-554 that was slower than the reduction of cytochrome b-563. Model simulations indicate that under highly oxidizing conditions for the Rieske FeS centre and reducing conditions for cytochrome b-563, the semiquinone at the Q_z site cannot only reduce cytochrome b-563, but can also oxidize cytochrome b-563 and reduce the Rieske FeS centre. The effect of 10 μM gramicidin D was evaluated in order to determine the contributions by electrochromic absorption changes around 518 nm. Gramicidin left electron transfer, monitored in the 550–600 nm range, unchanged. The gramicidin-sensitive (membrane potential-associated) signal at 518 nm differed from the signals recorded in the absence of gramicidin at 518 nm or 518–545 nm, due to spectral interference from electron-transferring components in the latter signals. KCN, DBMIB and antimycin A affected both the fast and slow components of the electrochromic signal, but did not proportionally affect the initial electron transfer from P-700 to ferredoxin (charge separation in PS I). Not only the slow (10–100 ms) component of the 518 nm absorption change, but also part of the fast (less than 1 ms) component appears to minitor electrogenic events in the cytochrome bf complex.     

Binding affinity of Chl b for the Chl a-binding sites in PSI core complexes

Most Chl a in PSI complexes was removed without any loss of P700 by ether treatment, yielding antenna-depleted P700-Chl a protein complexes (CP1s) with a Chl a/P700 ratio of 12. On addition of about 60 molecules of Chl b per P700 with phosphatidylglycerol, about 20 molecules of Chl b per P700 were bound to the complexes. The ratio of the bound Chl b to the added Chl b was about one-third, irrespective of the amount of Chl b added. The same partition ratio was obtained on reconstitution with Chl a, suggesting that the binding affinity of Chl b for the Chl a-binding sites is similar to that of Chl a. The relative quantum efficiency of P700 photooxidation, determined by the increase in its initial rate, increased in proportion to the increase in number of bound Chl b molecules. The degree of the increase was the same as expected if the bound Chl b had the same antenna activity as the bound Chl a. The bound Chl b emitted fluorescence with a peak at 660 nm, and its yield was as high as the Chl a remaining in the complexes. However, the excitation spectrum of the Chl a fluorescence, detected at 680 nm, was almost the same as the absorption spectrum of the Chl b-bound complexes, indicating efficient energy transfer of the bound Chl b to Chl a. These results suggest that Chl b primarily occupies the Chl a-binding sites close to the reaction center region, acting as an efficient antenna for P700.     

A long-wave absorbing form of chlorophyll a responsible for the “red drop” in fluorescence at 298 °K and the F723 band at 77 °K

When Chlorella cells are ruptured at pH 4.6 by sonication in air, its absorption spectrum can be best explained if one assumes that a long-wave chlorophyll a form (Chl a 693) is preferentially destroyed. Using these preparations, and comparing them with the algal suspension and the sonicates prepared at pH 7.8 under argon, we make the following conclusions: (a) The red drop beginning at about 675–680 nm in the action spectrum^* of fluorescence at 298 °K must be due to the presence of a non-(or weakly) fluorescent form of chlorophyll a. We suggest that this form is Chl a 693. The red drop is absent in the aerobic sonicates. (b) The red drop in fluorescence in whole algal cells is not due to any errors in absorption measurements; this drop is clearly present in the anaerobic sonicates. (c) The emission band at 723 nm, discovered by in whole Chlorella cells at 77 °K, may be due to increased fluorescence efficiency of Chl a 693 at low temperature; the F723 band is absent in aerobic sonicates.     

Fluorescence and energy transfer in phycobiliprotein-containing algae at low temperature

Fluorescence emission spectra of Anacystis nidulans, Porphyridium cruentum and Cyanidium caldarium, three phycobiliprotein-containing algae, were measured at temperatures between 4 and 120 K in the absence and in the presence of quinones as quenchers of chlorophyll fluorescence. In all species three major emission bands were observed in the chlorophyll a region, near 685 nm (F-685), 695 nm (F-695) and between 710 and 730 nm. Additional bands were observed at shorter wavelengths; these were preferentially excited by light absorbed by the phycobiliproteins and are presumably due to phycocyanins and allophycocyanins.

The amplitudes of F-685, F-695 and the long-wave emission showed a distinct increase upon cooling. For F-685 and F-695 the temperature dependence was similar to that earlier observed with spinach chloroplasts, for the long-wave emission it appeared to depend on the location of the emission bands, which was different for different species. All three bands were strongly quenched by quinones. These and other data suggest that the origin of these bands is the same as in higher plants, and that the fluorescence increase upon cooling can be explained by a lowering of the efficiency of energy transfer between chlorophyll molecules. It is concluded that at most a small percentage of the emission at 685 nm can be ascribed to allophycocyanin B, and that the efficiency of energy transfer between allophycocyanin B and chlorophyll a probably exceeds 99% both at 77 and 4 K. Experiments with isolated phycobilisomes suggest that energy transfer from allophycocyanin to allophycocyanin B occurs with an efficiency of about 90% at low temperature.

The effect of quenchers can be understood by the assumption that the quenching is caused by the formation of non-fluorescent traps in the bulk chlorophyll. Of three quinones tested, the strongest quenching was observed with dibromothymoquinone, which quenched F-685, F-695 and the long-wave emission approximately equally. Menadione and 1,4-naphthoquinone, however, preferentially quenched the long-wave bands, indicating a stronger interaction with Photosystem I than with Photosystem II chlorophylls.     

The P700-chlorophyll a-protein of a blue-green alga

The previously isolated chlorophyll a-protein of blue-green algae has been shown to contain P700 in a ratio of 1 reaction center molecule per 100 light-harvesting chlorophyll molecules. One-fifth of the molecules in the preparation contain P700 together with some 20 light-harvesting molecules, whereas the other molecules contain bulk chlorophyll only. Both pigment-protein entities are considered to be essentially the same and cannot be fractionated. An aggregate containing both types probably makes up the photochemical portion of the algal Photosystem I in vivo. The absorption and emission spectra of the pigment-protein are reported, as well as the spectral changes associated with the photochemical reaction. In addition to chlorophyll, carotenoid and protein the complex contains a quinone, which is not a plastoquinone. This unidentified quinone appears to participate in secondary electron transfer reactions occurring in the complex. Horse cytochrome c can be bound to the complex and will donate electrons to P⁺700 upon illumination. Current hypotheses for the identity of the primary electron acceptor were tested. It appears unlikely that flavins, pteridines or iron fill this role.     

Temperature dependence of optical properties of chlorophyll a incorporated into phosphatidylcholine liposomes

Temperature-dependent spectral changes of chlorophyll a (Chl a) incorporated into liposomes of two types of phosphatidylcholine are studied. When Chl a incorporated into the liposomes is cooled down to 5°C from the temperature of the gel-to-liquid crystalline phase transition of the lipid, the red shift as well as the increase in half-bandwidth of the red peak of Chl a are only slight. By measuring the difference spectra produced by substracting the absorption spectrum at the phase transition temperature of the lipid from that at lower temperature, it is shown that the component absorbing at longer wavelength (675–685 nm) than the peak of the red maximum (about 670 nm) significantly increases at the expense of the component absorbing at shorter wavelength (657–668 nm). The positions of positive and negative peaks depend on the temperature and the molar ratio of the lipid to Chl a. The absorbance change is most pronounced on cooling below the phase transition temperature of the lipid. The temperature-induced absorbance change is almost completely reversible. The results indicate that the aggregated forms of Chl a in liposomes can be spectrophotometrically detected in the gel phase of the lipid.     

Flash-induced charge separation and dark recombination in a Photosystem-II subchloroplast particle

The decay time of flash-induced absorption changes in a Photosystem-II subchloroplast fragment is very temperature sensitive down to 210 K, below which it remains constant at 1.25 ± 0.05 ms. The difference spectrum from the near-infra-red to the ultraviolet regions indicates that the monophasic decay represents charge recombination between P-680⁺ and the reduced primary acceptor. The charge recombination proceeds by electron tunneling. The P-680 concentration in the TSF-IIa fragment was estimated to be one in 30 ± 5 total chlorophyll molecules.     

Evidence for slow turnover in a fraction of Photosystem II complexes in thylakoid membranes

We used two different techniques to measure the recovery time of Photosystem II following the transfer of a single electron from P-680 to Q_A in thylakoid membranes isolated from spinach. Electron transfer in Photosystem II reaction centers was probed first by spectroscopic measurements of the electrochromic shift at 518 nm due to charge separation within the reaction centers. Using two short actinic flashes separated by a variable time interval we determined the time required after the first flash for the electrochromic shift at 518 nm to recover to the full extent on the second flash. In the second technique the redox state of Q_A at variable times after a saturating flash was monitored by measurement of the fluorescence induction in the absence of an inhibitor and in the presence of ferricyanide. The objective was to determine the time required after the actinic flash for the fluorescence induction to recover to the value observed after a 60 s dark period. Measurements were done under conditions in which (1) the electron donor for Photosystem II was water and the acceptor was the endogenous plastoquinone pool, and (2) Q₄₀₀, the Fe²⁺ near Q_A, remained reduced and therefore was not a participant in the flash-induced electron-transfer reactions. The electrochromic shift at 518 nm and the fluorescence induction revealed a prominent biphasic recovery time for Photosystem II reaction centers. The majority of the Photosystem II reaction centers recovered in less than 50 ms. However, approx. one-third of the Photosystem II reaction centers required a half-time of 2–3 s to recover. Our interpretation of these data is that Photosystem II reaction centers consist of at least two distinct populations. One population, typically 68% of the total amount of Photosystem II as determined by the electrochromic shift, has a steady-state turnover rate for the electron-transfer reaction from water to the plastoquinone pool of approx. 250 e⁻ / s, sufficiently rapid to account for measured rates of steady-state electron transport. The other population, typically 32%, has a turnover rate of approx. 0.2 e⁻ / s. Since this turnover rate is over 1000-times slower than normally active Photosystem II complexes, we conclude that the slowly turning over Photosystem II complexes are inconsequential in contributing to energy transduction. The slowly turning over Photosystem II complexes are able to transfer an electron from P-680 to Q_A rapidly, but the reoxidation of Q⁻_A is slow (t1/2 = 2 s). The fluorescence induction measurements lead us to conclude that there is significant overlap between the slowly turning over fraction of Photosystem II complexes and PS II_β reaction centers. One corollary of this conclusion is that electron transfer from P-680 to Q_A in PS II_β reaction centers results in charge separation across the membrane and gives rise to an electrochromic shift.     

The effect of pH on the reduction kinetics of P-680 in tris-treated chloroplasts

The primary donor of Photosystem II (PS II), P-680, was photo-oxidized by a short flash and its rate of reduction was measured at different pH values by following the recovery of the absorption change at 820 nm in chloroplasts pretreated with a high concentration of Tris. The re-reduction is biphasic with a fast phase (dominant after the first flash) attributed to the donation by a donor, D₁, and a slow phase (usually dominant after the second flash) attributed to a back-reaction with the primary acceptor.

It is found that pH has a strong influence on the donation from D₁ (τ = 2 μs at pH 9, 44 μs at pH 4), but no influence on the back reaction (τ ≈ 200 μs). pH also influences the stability of the charge separation since the contribution of donation from D₁ at the second flash increases at lower pH, getting close to 100% at pH 4.