Fluorescence emission spectra of photosystem I, photosystem II and the light-harvesting chlorophyll a/b complex of higher plants

Fluorescence emission spectra excited at 514 and 633 nm were measured at -196 degrees C on dark-grown bean leaves which had been partially greened by a repetitive series of brief xenon flashes. Excitation at 514 nm resulted in a greater relative enrichment of the 730 nm emission band of Photosystem I than was obtained with 633 nm excitation. The difference spectrum between the 514 nm excited fluorescence and the 633 nm excited fluorescence was taken to be representative of a pure Photosystem I emission spectrum at -196 degrees C. It was estimated from an extrapolation of low temperature emission spectra taken from a series of flashed leaves of different chlorophyll content that the emission from Photosystem II at 730 nm was 12% of the peak emission at 694 nm. Using this estimate, the pure Photosystem I emission spectrum was subtracted from the measured emission spectrum of a flashed leaf to give an emission spectrum representative of pure Photosystem II fluorescence at -196 degrees C. Emission spectra were also measured on flashed leaves which had been illuminated for several hours in continuous light. Appreciable amounts of the light-harvesting chlorophyll a/b protein, which has a low temperature fluorescence emission maximum at 682 nm, accumulate during greening in continuous light. The emission spectra of Photosystem I and Photosystem II were subtracted from the measured emission spectrum of such a leaf to obtain the emission spectrum of the light-harvesting chlorophyll a/b protein at -196 degrees C.     

Competition between the 735 nm fluorescence and the photochemistry of Photosystem I in chloroplasts at low temperature

Fluorescence emission spectra of chloroplasts, initially frozen to--196 degrees C, were measured at various temperatures as the sample was allowed to warm. The 735 nm emission band attributed to fluorescence from Photosystem I was approx. 10-fold greater at--196 degrees C than at--78 degrees C. The initial rate of photooxidation of P-700 was also measured at--196 degrees C and--78 degrees C and was found to be approximately twice as large at the higher temperature. It is proposed that the 735 nm emission band is fluorescence from a long wavelength form of chlorophyll, C-705, which acts as a trap for excitation energy in the antenna chlorophyl system of Photosystem I. Furthermore, it is proposed that C-705 only forms on cooling to low temperatures and that the temperature dependence of the 735 nm emission is the temperature dependence for the formation of C-705. C-705 and P-700 compete to trap the excitation energy in Photosystem I. It is estimated from the data that at--78 degrees C P-700 traps approx. 20 times more energy than C-705 while, at--196 degrees C, the two traps are approximately equally effective. By analogy, the 695 nm fluorescence which also appears on cooling to--196 degrees C is attributed to traps in Photosystem II which form only on cooling to temperatures near--196 degrees C.     

Fluorescence emission spectra of Photosystem I,Photosystem II and the light-harvesting chlorophyll a/b complex of higher plants

Fluorescence emission spectra excited at 514 and 633 nm were measured at ?196 °C on dark-grown bean leaves which had been partially greened by a repetitive series of brief xenon flashes. Excitation at 514 nm resulted in a greater relative enrichment of the 730 nm emission band of Photosystem I than was obtained with 633 nm excitation. The difference spectrum between the 514 nm excited fluorescence and the 633 nm excited fluorescence was taken to be representative of a pure Photosystem I emission spectrum at ?196 °C. It was estimated from an extrapolation of low temperature emission spectra taken from a series of flashed leaves of different chlorophyll content that the emission from Photosystem II at 730 nm was 12% of the peak emission at 694 nm. Using this estimate, the pure Photosystem I emission spectrum was subtracted from the measured emission spectrum of a flashed leaf to give an emission spectrum representative of pure Photosystem II fluorescence at ?196 °C. Emission spectra were also measured on flashed leaves which had been illuminated for several hours in continuous light. Appreciable amounts of the light-harvesting chlorophyll a/b protein, which has a low temperature fluorescence emission maximum at 682 nm, accumulate during greening in continuous light. The emission spectra of Photosystem I and Photosystem II were subtracted from the measured emission spectrum of such a leaf to obtain the emission spectrum of the light-harvesting chlorophyll a/b protein at ?196 °C.     

Energy transfer and the distribution of excitation energy in the photosynthetic apparatus of spinach chloroplasts

Equations are derived from our model of the photochemical apparatus of photosynthesis to show that the yield of energy transfer from Photosystem II to Photosystem I, ?_T(II→Iz), can be obtained from measurements on an individual sample of chloroplasts frozen to ?196 °C by comparing the sum of two specifically defined fluorescence excitation spectra with the absorption spectrum of the sample. Then, given that value of ?_T(II→I), the fraction of the quanta absorbed by the photochemical apparatus which is distributed initially to Photosystem I, α, can be determined as a function of the wavelength of excitation from the same fluorescence excitation spectra. The results obtained in this study of individual samples of chloroplasts frozen to ?196 °C in the absence of divalent cations, namely, that ?_T(II→I) varies from a minimum value of 0.10 when the Photosystem II reaction centers are all open to a maximum value of 0.25 when the centers are all closed and that α has a value of about 0.30 which is almost independent of wavelength for wavelengths shorter than 675 nm (α increases rapidly toward unity at wavelengths longer than 675 nm), agrees quite well with results obtained previously from comparative measurements of chloroplasts frozen to ?196 °C in the presence and absence of divalent cations.     

Excitation spectra for photosystem I and photosystem II in chloroplasts and the spectral characteristics of the distributions 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 degrees C is due to energy transfer from Photosystem II to Photosystem I. Fluorescence excitation spectra were measured at -196 degrees C at the minimum, FO, level and the maximum, FM, level of the emission at 750 nm. The difference spectrum, FM-FO, which represents the excitation spectrum for FV 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. Fluoresence at the FO level at 750 nm can be considered in two parts; one part due to the fraction of absorbed quanta, alpha, 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 FO/FV measured at 692 nm and the extent of FV at 750 nm. According to this procedure the excitation spectrum of Photosystem I at -196 degrees C was determined by subtracting 1/3 of the excitation spectrum of FV at 750 nm from the excitation spectrum of FO 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 alpha was determined from fluorescence measurements at 692 and 750 nm at -196 degrees C. Alpha is constant to within a few percent from 400 to 680 nm, the maximum deviation being at 515 nm where alpha shows a broad maximum increasing from 0.30 to 0.34. At wavelengths between 680 and 700 nm, alpha increases to unity as Photosystem I becomes the dominant absorber in the photochemical apparatus.     

Regulation of excitation energy distribution in subchloroplast particles: photosystem I

Mono- and divalent cations were found to increase the transfer of excitation energy within Photosystem I from the light-harvesting chlorophyll a molecules to P700. The P700-chlorophyll a protein of Shiozawa et al. (J. A. Shiozawa, R. S. Alberte, and J. P. Thornber, 1974, Arch. Biochem. Biophys.165, 388–397) was used for these studies. Cations stimulated the quantum yields for electron transport when the light-harvesting chlorophyll a molecules were irradiated. They also decreased chlorophyll a fluorescence. Half-maximal effects were observed at 0.5–0.6 mm for divalent cations and at 5–6 mm for monovalent cations. Triton X-100, 0.02%, also increased energy transfer. The increases in energy transfer are due to an intramolecular conformational change in the protein. A structural change is involved, since there is a correlation between the cation-induced changes in energy transfer and increases in 90 ° light scattering. However, there was no change in the molecular weight upon the addition of MgCl₂. The molecular weight, as determined by gel filtration, was 105,000 in the presence of 0.05% Triton X-100. On the other hand, circular dichroism measurements showed an increase in the α-helical content from 51 to 63% when 5 mm MgCl₂ was added. Changes in the absorption spectra were also observed. We believe that the cation regulation of Photosystem I activity provides a fine-tuning mechanism for the regulation of energy transfer.     

Probing the kinetics of photosystem I and photosystem II fluorescence in pea chloroplasts on a picosecond pulse fluorometer.

Picosecond fluorescence kinetics of pea chloroplasts have been investigated at room temperature using a pulse fluorometer with a resolution time of 10-11 s. Fluorescence has been excited by both a ruby and neodymium-glass mode-locked laser and has been reocrded within the 650 to 800 nm spectral region. We have found three-component kinetics of fluorescence from pea chloroplasts with lifetimes of 80, 300 and 4500 ps, respectively. The observed time dependency of the fluorescence of different components on the functional state of the photosynthetic mechanism as well as their spectra enabled us to conclude that Photosystem I fluoresces with a lifetime of 80 ps (tauI) and Photosystem II fluoresces with a lifetime of 300 ps (tauII). Fluorescence with a lifetime of 4500 ps (tauIII) may be interpreted as originating from chlorophill monomeric forms which are not involved in photosynthesis. It was determined that the rise time of Photosystem I and Photosystem II fluorescence after 530 nm photoexcitation is 200 ps, which corrsponds to the time of energy migration to them from carotenoids.     

Effects of monovalent cations on light energy distribution between two pigment systems of photosynthesis in isolated spinach chloroplasts

The effects of monovalent cations on the light energy distribution between two pigment systems of photosynthesis were studied in isolated spinach chloroplasts by measuring chlorophyll a fluorescence and photochemical reactions.

The addition of NaCl to the chloroplast suspension produced a 40–80% increase in fluorescence yield measured at 684 nm at room temperature. The fluorescence increase was completed about 5 min after the addition. The effect saturated at 100 mM NaCl. Low-temperature fluorescence spectra showed that NaCl increased the yields of two fluorescence bands of pigment system II at 684 and 695 nm but decreased that of pigment system I at 735 nm. Similar effects on chlorophyll a fluorescence at room and at low temperatures were obtained with NaBr, NaNO₃, Na₂SO₄, LiCl, KCl, RbCl, CsCl, NH₄Cl and CH₃NH₃Cl.

NaCl suppressed the quantum efficiency of NADP⁺ reduction supported by the ascorbate-2,6-dichlorophenolindophenol (DCIP) couple as an electron donor system in the presence of 3-(3′,4′-chlorophenyl)-1,1-dimethylurea (DCMU). On the other hand, NaCl only slightly enhanced the quantum yield of photoreaction II measured by the Hill reaction with DCIP.

It is concluded that the monovalent cations tested suppressed the excitation transfer from pigment system II to pigment system I; the effects were the same as those of alkaline earth metals and Mn²⁺ (refs. 1, 2).     

Interaction of alkaline metal ions with Ca(2+)-binding sites of Ca(2+)-ATPase of sarcoplasmic reticulum: 23Na-NMR studies.

The analysis of the 23Na-NMR signal shape variations in the presence of vesicles of light sarcoplasmic reticulum (SR) shows the existence of sodium sites on the membranes with Kd values of about 10 mM. Other monovalent cations displace Na+ from SR fragments in a competitive manner according to the row K+ greater than Rb+ greater than Cs+ greater than Li+. Calcium ions also reduce Na+ binding, the Na+ desorption curve being of a two-stage nature, which, as suggested, indicates the existence of two types of Ca(2+)-sensitive Na+ binding sites (I and II). Sites of type I and II are modified by Ca2+ in submicromolar and millimolar concentrations, respectively. Analysis of sodium (calcium) desorption produced by calcium (sodium) allowed us to postulate the competition of these two cations for sites I and identity of these sites to high-affinity Ca(2+)-binding ones on the Ca(2+)-ATPase. Sites I weakly interact with Mg2+ (KappMg approximately 30 mM). Reciprocal effects of sodium and calcium on binding of each other to sites II cannot be described by a simple competition model, which indicates nonhomogeneity of these sites. A portion of sites I (approximately 70%) interacts with Mg2+ (KappMg = 3-4 mM). The pKa value of sites II is nearly 6.0. The number of sites II is three times greater than that of sites I. In addition, sites with intermediate affinity for Ca2+ were found with Kd values of 2-5 microM. These sites were revealed due to the reducing of the sites II affinity for Na+ upon Ca2+ binding to SR membranes. It can thus be concluded that in nonenergized SR there are binding sites for monovalent cations of at least three types: (1) sites I (which also bind Ca2+ at low concentrations), (2) magnesium-sensitive sites II and (3) magnesium-insensitive sites II.     

A quantitative study of the slow decline of chlorophyll a fluorescence in isolated chloroplasts.

A detailed study of the photo-induced decline in chlorophyll a fluorescence intensity (Kautsky phenomenon) in coupled isolated chloroplasts from a high level (P) to a low stationary level (S) is presented. 1. A linear relationship between P leads to S quenching and intrathylakoid H+ concentration was found. When the light-induced proton gradient was abolished by uncoupling, the fluorescence emission at room temperature was lowered proportionally to increased H+ concentration in the medium. 2. Fluorescence spectra at -196 degrees C of samples frozen at the P and S states showed no significant differences in the Photosystem I/Photosystem II ratio of fluorescence emission. Furthermore, freezing to -196 degrees C reversed the P leads to S quenching. This indicates that the P leads to S quenching is not related to an increase of spillover of excitation energy from Photosystem II to Photosystem I. 3. When Mg2+ was added to thylakoids suspended in a medium free of divalent cations, the inhibition of spillover required lower Mg2+ concentrations (half saturation at 0.6 mM). Increased proton concentration in the medium also inhibited spillover. 4. The results are interpreted in terms of two sites of Mg2+ and H+ effects on excitation deactivation in Photosystem II. One site is located on the outer face of the thylakoid membrane; action of both Mg2+ and H+ at this side diminishes spillover. The second site is located on the inner face of the membrane; as Mg2+ is displaced there by protons, a non-photochemical quenching of Photosystem II fluorescence is induced, which is manifested by the P leads to S decline.     

Interaction of valinomycin and monovalent cations with the (Ca2+,Mg2+)-ATPase of skeletal muscle sarcoplasmic reticulum

The interactions of monovalent cations and of the K+-specific ionophore, valinomycin, with the Ca2+-ATPase of skeletal muscle of sarcoplasmic reticulum have been studied in the absence of cation gradients by their effects on enzyme turnover and on the ATP plus Ca2+-dependent enhanced fluorescence of the ATP analogue, 2',3'-O-(2,4,6-trinitrocyclohexyldienylidine)-adenosine 5'-triphosphate (TNP-ATP) (Watanabe, T., and Inesi, G. (1982) J. Biol. Chem. 257, 11510-11516). Monovalent cations decreased turnover-dependent TNP-ATP fluorescence in the series K+ greater than Rb+ approximately equal to Cs+ greater than Na+ greater than Li+ (K0.5 = 49, 73, 75, 94, and 246 mM, respectively), consistent with the known specificity of the monovalent cation binding site that stimulates turnover and E-P hydrolysis. Valinomycin (200 nmol/mg), in the absence of monovalent cations, decreased ATPase activity by 30% and abolished the stimulatory effects of 150 mM KCl or NaCl on turnover. The ionophore alone enhanced TNP-ATP fluorescence by 20% and altered the specificity and affinity of the site that inhibited TNP-ATP fluorescence to Cs+ greater than Rb+ greater than K+ approximately equal to Na+ greater than Li+ (K0.5 = 79, 111, 134, 136, and 270 mM, respectively), which follows the Hofmeister series for effectiveness of monovalent lyotropic cations. TNP-ATP binding was not affected by either monovalent cations or valinomycin. Inhibition of turnover-dependent TNP-ATP fluorescence appears to be a useful parameter for monitoring monovalent cation binding to the Ca2+-ATPase. It is concluded that the ionophore interacts directly with the Ca2+-ATPase, independent of its K+ conductance effects on the lipid bilayer, and modifies the affinity and specificity of the monovalent cation site, either by direct interaction or by the formation of a valinomycin-monovalent cation-enzyme complex.     

Correlation between monovalent cation-induced decreases in chlorophyll a fluorescence and chloroplast structural changes

Low concentrations (~ 3 mm) of salts of monovalent cations such as Na⁺, K⁺, and tetraethylammonium were found to decrease the turbidity of chloroplast suspensions. The turbidity changes (Δ₅₄₀) had the same kinetics, salt concentration dependence, and pH dependence as the monovalent cation-induced decreases in chlorophyll a fluorescence (9), suggesting that structural changes are the cause of the associated increases in spillover. Electron microscopy revealed that the grana are stacked when spillover is inhibited (in the absence of salts or the presence of divalent cations) and that monovalent cations cause the grana to unstack, thereby promoting spillover.     

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.     

Temperature dependence and polarization of fluorescence from Photosystem I in the cyanobacterium Synechocystis sp. PCC 6803

To determine the fluorescence properties of cyanobacterial Photosystem I (PS I) in relatively intact systems, fluorescence emission from 20 to 295 K and polarization at 77 K have been measured from phycobilisomes-less thylakoids of Synechocystis sp. PCC 6803 and a mutant strain lacking Photosystem II (PS II). At 295 K, the fluorescence maxima are 686 nm in the wild type from PS I and PS II and at 688 nm from PS I in the mutant. This emission is characteristic of bulk antenna chlorophylls (Chls). The 690-nm fluorescence component of PS I is temperature independent. For wild-type and mutant, 725-nm fluorescence increases by a factor of at least 40 from 295 to 20 K. We model this temperature dependence assuming a small number of Chls within PS I, emitting at 725 nm, with an energy level below that of the reaction center, P700. Their excitation transfer rate to P700 decreases with decreasing temperature increasing the yield of 725-nm fluorescence.Fluorescence excitation spectra of polarized emission from low-energy Chls were measured at 77 and 295 K on the mutant lacking PS II. At excitation wavelengths longer than 715 nm, 760-nm emission is highly polarized indicating either direct excitation of the emitting Chls with no participation in excitation transfer or total alignment of the chromophores. Fluorescence at 760 nm is unpolarized for excitation wavelengths shorter than 690 nm, inferring excitation transfer between Chls before 760-nm fluorescence occurs.Our measurements illustrate that: 1) a single group of low-energy Chls (F725) of the core-like PS I complex in cyanobacteria shows a strongly temperature-dependent fluorescence and, when directly excited, nearly complete fluorescence polarization, 2) these properties are not the result of detergent-induced artifacts as we are examining intact PS I within the thylakoid membrane of S. 6803, and 3) the activation energy for excitation transfer from F725 Chls to P700 is less than that of F735 Chls in green plants; F725 Chls may act as a sink to locate excitations near P700 in PS I.Abbreviations Chl chlorophyll - BChl bacteriochlorophyll - PS Photosystem - S. 6803 Synechocystis sp. PCC 6803 - PGP potassium glycerol phosphate     

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.     

Probing the kinetics of Photosystem I and Photosystem II fluorescence in pea chloroplasts on a picosecond pulse fluorometer

Picosecond fluorescence kinetics of pea chloroplasts have been investigated at room temperature using a pulse fluorometer with a resolution time of 10^?11 s. Fluorescence has been excited by both a ruby and neodymium-glass mode-locked laser and has been recorded within the 650 to 800 nm spectral region.We have found three-component kinetics of fluorescence from pea chloroplasts with lifetimes of 80, 300 and 4500 ps, respectively. The observed time dependency of the fluorescence of different components on the functional state of the photosynthetic mechanism as well as their spectra enabled us to conclude that Photosystem I fluoresces with a lifetime of 80 ps (τ_I) and Photosystem II fluoresces with a lifetime of 300 ps (τ_II). Fluorescence with a lifetime of 4500 ps (τ_III) may be interpreted as originating from chlorophyll monomeric forms which are not involved in photosynthesis.It was determined that the rise time of Photosystem I and Photosystem II fluorescence after 530 nm photoexcitation is 200 ps, which corresponds to the time of energy migration to them from carotenoids.     

Resolution of low-energy chlorophylls in Photosystem I of Synechocystis sp. PCC 6803 at 77 and 295 K through fluorescence excitation anisotropy

Fluorescence excitation spectra of highly anisotropic emission from Photosystem I (PS I) were measured at 295 and 77 K on a PS II-less mutant of the cyanobacterium Synechocystis sp. PCC 6803 (S. 6803). When PS I was excited with light at wavelengths greater than 715 nm, fluorescence observed at 745 nm was highly polarized with anisotropies of 0.32 and 0.20 at 77 and 295 K, respectively. Upon excitation at shorter wavelengths, the 745-nm fluorescence had low anisotropy. The highly anisotropic emission observed at both 77 and 295 K is interpreted as evidence for low-energy chlorophylls (Chls) in cyanobacteria at room temperature. This indicates that low-energy Chls, defined as Chls with first excited singlet-state energy levels below or near that of the reaction center, P700, are not artifacts of low-temperature measurements.If the low-energy Chls are a distinct subset of Chls and a simple two-pool model describes the excitation transfer network adequately, one can take advantage of the low-energy Chls' high anisotropy to approximate their fluorescence excitation spectra. Maxima at 703 and 708 nm were calculated from 295 and 77 K data, respectively. Upper limits for the number of low-energy Chls per P700 in PS I from S. 6803 were calculated to be 8 (295 K) and 11 (77 K).Abbreviations Chl - chlorophyll - BChl - bacteriochlorophyll - LHC - light-harvesting chlorophyll - PS - Photosystem - RC - reaction center - S. 6803 - Synechocystis sp. PCC 6803