Slow fluorescence quenching of type A chloroplasts. Resolution into two components.

The divalent-cation-specific ionophore A23187 is used to define two components of the slow fluorescence quenching of type a spinach chloroplasts: ionophore-reversible and ionophore-resistant quenching. Ionophore-reversible quenching predominates at relatively low light intensities and approaches saturation as light levels are increased. It is sensitive to uncouplers and to 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU) and is dark reversible. At high light intensities the bulk (greater than 80%) of slow fluorescence quenching is ionophore-resistant. Ionophore-resistant quenching is stimulated by carbonyl cyanide m-chlorophenyl hydrazone (CCCP) at pH 7.6 and by both CCCP and methylamine at pH 9.0. It is insensitive to DCMU and is not reversed in subsequent darkness. Taken together, the two components account for all quenching observed in Type A chloroplasts. Ionophore-reversible quenching is identified with the Mg2+-mediated fluorescence quenching described by Krause (Biochim. Biophys. Acta (1974) 333, 301-313) and by Barber and Telfer (in Membrane Transport in Plants (Dainty, J., AND Zimmermann, U., eds.), pp. 281-288, Springer-Verlag, Berlin, 1974). Ionophore-resistant quenching, a first-order process requiring high light, resembles the quenching reported by Jennings et al. (Biochim. Biophys. Acta (1976) 423, 264-274). The resolution of the fluorescence quenching phenomenon into two distinct components reconciles the apparently contradictory observations of these earlier investigations.     

Studies on the slow fluorescence decline in isolated chloroplasts

Data presented here indicate that the slow fluorescence decline in osmotically disrupted chloroplasts is not associated with the well known divalent cation effect on fluorescence yield. Thus the two phenomena have markedly different magnesium concentration requirements, magnesium addition after the fluorescence decline did not stimulate the dark reversal, and the characteristics of the fluorescence induction kinetics of the two processes are not similar.At pH 7.6 the slow fluorescence decline was stimulated by several uncouplers demonstrated to greatly reduce proton pumping, and at pH 9.2 it was stimulated by all uncouplers tested. Acid-base transition was strongly inhibitory, and this inhibition was relieved by uncoupler. Thus the pH gradient seems to inhibit the process. The involvement of coupling factor is suggested by experiments in which phosphorylation substrates were inhibitory, and this inhibition was prevented by uncoupler. These data are explained in terms of coupling factor structural changes which in an unknown manner influence Photosystem II fluorescence emission.Fluorescence induction curves indicate that the slow quenching decreased only the variable fluorescence. The half rise time was decreased along with the sig-moidicity of the rise curve. These data can be accomodated in terms of a model recently proposed by Butler and Kitajima (Biochim. Biophys Acta (1975) 376, 116–125), involving the transfer of energy from the excited, but closed, reaction centres II to the light harvesting chlorophyll system. The slow fluorescence decline is suggested to represent a decrease of this process.     

A comparison between cation and protein phosphorylation effects on the fluorescence induction curve in chloroplasts treated with 3-(3,4-dichlorophenyl)-1,1-dimethylurea

Fluorescence induction curves in chloroplasts phosphorylated by the thylakoid protein kinase activated at low light intensity and high chlorophyll concentration have been measured. At 5 mM Mg²⁺, phosphorylation did not preferentially quench variable fluorescence. At 1 mM, preferential quenching of variable fluorescence was observed, indicating a second effect of phosphorylation at low Mg²⁺ (Horton, P. and Black, M.T. (1982) Biochim. Biophys. Acta 680, 22–27). Comparison of the extent of fluorescence decrease and the resulting ratio of variable to maximum fluorescence after phosphorylation and after lowering Mg²⁺ concentration demonstrated a difference between these two mechanisms of lowering of fluorescence. The significance of these results in terms of how phosphorylation may alter membrane organization is discussed.     

Picosecond fluorescence kinetic studies of electron acceptor Q redox heterogeneity

We have investigated the influence of chloroplast organization on the nature of chemical reductive titrations of Photosystem II fluorescence decay kinetics in spinach chloroplasts. Structural changes of the chloroplast membrane system were induced by varying the ionic environment of the thylakoids. A single-photon timing system with picosecond resolution monitored the kinetics of the chlorophyll a fluorescence emission. At all ionic concentrations studied, we have observed biphasic potentiometric titration curves of fluorescence yield; these have been interpreted to be suggestive of electron acceptor Q heterogeneity (Karukstis, K.K. and Sauer, K. (1983) Biochim. Biophys. Acta 722, 364–371; Cramer, W.A. and Butler, W.L. (1969) Biochim. Biophys. Acta 172, 503–510). A direct relation is observed between the E_m value of the low-potential component of Q and the Mg²⁺ concentration of the chloroplast suspending medium. We have attributed these midpoint potential variations to the thylakoid structural rearrangements involved in cation-regulated grana stacking. Ionic effects on the fluorescence decay kinetics at the redox transitions are discussed in terms of the heterogeneity of Photosystem II units (α- and β-centers) and the mechanism of deexcitation at a closed reaction center (fluorescence or nonradiative decay).     

Kinetics of chlorophyll fluorescence at 77 K in Chlorella and chloroplasts. Effects of CCCP,ferricyanide and DCMU

The kinetics of chlorophyll fluorescence at 77 K were studied in Chlorella cells and spinach chloroplasts.During a first illumination, the rise is polyphasic with at least three phases. The slowest one is irreversible and corresponds to the cytochrome oxidation.The dark regeneration of half the variable fluorescence is biphasic, the fast phase being inhibited by 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU) both in Chlorella and chloroplasts.The fluorescence rise during a second illumination is still biphasic.Carbonyl cyanide m-chlorophenylhydrazone (CCCP) slows down the fluorescence rise in Chlorella but has no effect on the dark regeneration. It does not affect the fluorescence of chloroplasts.Ferricyanide which oxidizes cytochrome b-559 at room temperature produces a quenching of the variable fluorescence and an acceleration of the fluorescence rise during the first illumination.Our results fit the idea of the heterogeneity of the Photosystem II centers at low temperature.     

Organization of the photosynthetic apparatus of the chlorina-f2 mutant of barley using chlorophyll fluorescence decay kinetics

The time-resolved chlorophyll fluorescence emission of higher plant chloroplasts monitors the primary processes of photosynthesis and reflects photosynthetic membrane organization. In the present study we compare measurements of the chlorophyll fluorescence decay kinetics of the chlorophyll-b-less chlorina-f2 barley mutant and wild-type barley to investigate the effect of alterations in thylakoid membrane composition on chlorophyll fluorescence. Our analysis characterizes the fluorescence decay of chlorina-f2 barley chloroplasts by three exponential components with lifetimes of approx. 100 ps, 400 ps and 2 ns. The majority of the chlorophyll fluorescence originates in the two faster decay components. Although photo-induced and cation-induced effects on fluorescence yields are evident, the fluorescence lifetimes are independent of the state of the Photosystem-II reaction centers and the degree of grana stacking. Wild-type barley chloroplasts also exhibit three kinetic fluorescence components, but they are distinguished from those of the chlorina-f2 chloroplasts by a slow decay component which displays cation- and photo-induced yield and lifetime changes. A comparison is presented of the kinetic analysis of the chlorina-f2 barley fluorescence to the decay kinetics previously measured for intermittent-light-grown peas (Karukstis, K. and Sauer, K. (1983) Biochim. Biophys. Acta 725, 384–393). We propose that similarities in the fluorescence decay kinetics of both species are a consequence of analogous rearrangements of the thylakoid membrane organization due to the deficiencies present in the light-harvesting chlorophyll $\text{a}\text{b}$ complex.     

Effects of carbonyl cyanide m-chlorophenylhydrazone and hydroxylamine on the Photosystem II electron exchange mechanism in 3-(3,4-dichlorophenyl)-1,1-dimethylurea treated algae and chloroplasts

The effects of NH₂OH and carbonyl cyanide m-chlorophenylhydrazone (CCCP) on 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU)-treated algae and chloroplasts were studied. In the presence of DCMU, the photochemically separated charges can only disappear through a recombination back reaction; both substances induce an irreversible reduction of the donor side and after sufficient illumination their action in the presence of DCMU leads to the formation of a permanent fluorescent state.

In the DCMU + CCCP system, a fast fluorescence induction curve is observed. The fluorescence yield is brought to its maximum by two flashes. The luminescence emission is strongly inhibited and most centers reach their permanent fluorescent state after one flash.

In the DCMU + NH₂OH system, a slow fluorescence rise is observed and several saturating flashes are needed for the fluorescence yield to reach its maximum. The exhaustion of the NH₂OH oxidizing capacity and the complete transformation to a permanent fluorescent state also require a large number of flashes.

The reduction pathway catalyzed by CCCP appears to be a good competitor to the back reaction, while NH₂OH seems to be a relatively inefficient donor.

In addition the action of NH₂OH and CCCP on fluorescence suggests that the donor side influences the quenching properties of Photosystem II centers. A possible mechanism is proposed.     

Photoinduced quenching of chlorophyll fluorescence in intact chloroplasts and algae. Resolution into two components

The light-induced decline of chlorophyll a fluorescence from a peak (P) to a low stationary level (S) in intact, physiologically active isolated chloroplasts and in intact Chlorella cells is shown to be predominantly composed of two components: (1) fluorescence quenching by partial reoxidation of the quencher Q, the primary acceptor of Photosystem II and (2) energy-dependent fluorescence quenching related to the photoinduced acidification of the intrathylakoid space. These two mechanisms of fluorescence quenching can be distinguished by the different kinetics of the relaxation of quenching observed upon addition of 3-(3′,4′-dichlorophenyl)-1,1-dimethylurea (DCMU). The relaxation of quenching by addition of DCMU is biphasic. The fast phase with a half-time of about 1 s is attributed to the reversal of Q-dependent quenching. The slow phase with a half-time of about 15 s in chloroplasts and 5 s in Chlorella cells is ascribed to relaxation of energy-dependent quenching. As shown by fluorescence spectroscopy at 77 K, the energy-dependent fluorescence quenching essentially is not caused by increased transfer of excitation energy to Photosystem I. By analyzing the energy- and Q-dependent components of quenching, information on the energy state of the thylakoid membranes and on the redox state of Q under various physiological conditions is obtained.     

Excitation-energy distribution in green algae. The existence of two independent light-driven control mechanisms

Three distinct states can be identified for cells of the green alga Chlorella vulgaris; State 1 and State 2 obtained by preillumination in far-red and red light, respectively, and the dark state obtained by dark-adaptation. Addition of the inhibitor DCMU to algal cells leads to an initial rapid increase in chlorophyll-a fluorescence reflecting the closure of Photosystem II traps. This, in the case of dark and state-2-adapted algae is followed by a slow light-dependent increase to a fluorescence yield typical of State-1-adapted cells. Measurements of low temperature (77 K) emission spectra indicate that the low fluorescence yields of dark and State-2-adapted algae reflect similar balances in excitation-energy distribution between the two photosystems. In both cases, the balance favours PS I and the slow fluorescence increase seen in the poisoned algae reflects a redressing of this balance in favour of PS II. The low fluorescence yield of State-2-adapted algae is thought to be associated with the phosphorylation of chlorophyll a/b light-harvesting protein (Biochim. Biophys. Acta (1983) 724, 94–103). Measurements of the uncoupler and ATPase sensitivity of the light-dependent increases seen in DCMU-poisoned cells indicate that the low fluorescence yield of dark-adapted algae is of different origin. Evidence is presented showing that the light-driven changes in excitation-energy distribution seen in green algae involve two distinct processes; a low-intensity, wavelenght-independent change reflecting simple light/dark changes and a higher intensity, wavelength-dependent change reflecting State 1/State 2 adaptation. The former changes appear to be associated with changes in the local ionic environment within the algal chloroplast, whilst the latter appear to reflect changes in the phosphorylation state of chlorophyll a/b light-harvesting protein.     

The effect of redox potential of the kinetics of fluorescence induction in pea chloroplasts I. Removal of the slow phase

The effect of alteration of redox potential on the kinetics of fluorescence induction in pea chloroplasts has been investigated. Potentiometric titration of the initial (F_i) level of fluorescence recorded upon shutter opening gave a two component curve, with E_m(7) at ?20 mV and ?275 mV, almost, identical to results obtained using continuous low intensity illumination (Horton, P. and Croze, E. (1979) Biochim. Biophys. Acta 545, 188–201). The slow or tail phase of induction observed in the presence of DCMU can be eliminated by poising the redox potential at approx. 0 to +50 mV. At this potential F_i was increased by less than 10% and the higher potential quencher described above was only marginally reduced. The disappearance of the slow phase titrated as an n = 1 component with an E_m(7) of +120 mV. Therefore it seems unlikely that the slow phase of fluorescence induction is due to photoreduction of the ?20 mV quencher. These results are discussed with reference to current ideas concerning heterogeneity on the acceptor side of Photosystem II.     

Induction of photochemical and non-photochemical quenching of chlorophyll fluorescence by low concentrations of m-dinitrobenzene

Chlorophyll fluorescence quenching induced by low concentrations of m-dinitrobenzene (DNB) is investigated. In intact spinach chloroplasts DNB causes photochemical and non-photochemical quenching. The two forms of quenching are distinguished by applying the saturation pulse method with a new type of modulation fluorometer. Half-maximal photochemical quenching is observed at about 3 micromolar DNB. It is inhibited by 3-(3,4 dichlorophenyl)-1, 1-dimethylurea (DCMU) and by 2,5-dibromo-3-methyl-6-isopropyl-p-benzoquinone (DBMIB). Photochemical quenching by DNB leads to suppression of the I-P transient in a fluorescence induction curve. Upon application of saturating continuous light, the increase of fluorescence yield is separated into a photochemical and a thermal part. DNB causes suppression of only the slowest sub-component of the thermal part, in analogy to the action of Hill reagents. Simultaneous measurements of oxygen exchange rate and fluorescence reveal that a part of DNB induced quenching is accompanied by oxygen uptake. Most DNB-induced non-photochemical quenching is prevented by nigericin and, hence, can be considered energy-dependent quenching. The small component persisting in the presence of nigericin is identical to the one observed with methylviologen and other Hill reagents, likely to be due to static quenching by oxidized plastoquinone. The presented data confirm the original finding of Etienne and Lavergne (Biochim Biophys Acta 283: 268–278, 1972) that low concentrations of DNB selectively affect the thermal component of variable fluorescence. However, while these authors interpreted the quenching by a non-photochemical mechanism, the present investigation emphasizes a photochemical mechanism, in analogy to the effect of electron acceptors or mediators.Abbreviations DBMIB 2,5-dibromo-3-methyl-6-isopropyl-p-benzoquinone - DCMU 3-(3,4-dichlorophenyl)-1, 1-dimethylurea - DNB m-dinitrobenzene - PGA 3-phosphoglycerate - PMS phenazinemethosulphate - PS I and PS II photosystems I and II     

Light scattering and quenching of 9-aminoacridine fluorescence as indicators of the phosphorylation state of the adenylate system in intact spinach chloroplasts

Upon illumination of suspensions of intact chloroplasts, fluorescence of 9-aminoacridine was quenched, light scattering was increased, chlorophyll fluorescence was decreased after an initial increase, and chloroplast $\text{ATP}\text{ADP}$ ratios were increased. The response of 9-aminoacridine fluorescence quenching and light scattering to light intensity, anaerobiosis and inhibition of electron transport by DCMU was similar to that shown by chloroplast $\text{ATP}\text{ADP}$ ratios. It is discussed under what conditions 9-aminoacridine fluorescence quenching or light scattering can be used to monitor changes in the phosphorylation state of the chloroplast adenylate system.     

On the State 1-State 2 phenomenon in photosynthesis

The State 1-State 2 phenomenon of photosynthesis was studied in Chlorella by measuring the flash yield (Y) and the modulated rate (v) of oxygen evolution induced by weak modulated 650-nm light. From light intensity curves, intensities of 650 and 710 nm background and preilluminations were chosen to give maximum values of Y and v. Following long preilluminations in 710 nm (State 1) or in 650 nm (State 2), Y and v were measured in background light of chosen wavelength. The resulting plots of v vs Y show a discontinuity between State 1 and State 2. They confirm the predictions of Bonaventura and Myers [(1969) Biochim. Biophys. Acta 189, 366–383] and are consistent with changes in α (fraction of absorbed light captured by System II) as explanation of the State 1–State 2 phenomenon. When the intensity of 710 nm preillumination was too low, the characteristics of State 1 were not fully developed and the results then were similar to those of Delrieu [(1972) Biochim. Biophys. Acta 256, 293–299].     

Polyamines stimulate non-photochemical quenching of chlorophyll <Emphasis Type="Italic">a</Emphasis> fluorescence in <Emphasis Type="Italic">Scenedesmus obliquus</Emphasis>

Polyamines (PAs) are small metabolites that are produced and oxidized in chloroplasts with an obscure mode of action. Recently, we showed that qE is stimulated by PAs in higher plants (Nicotiana tabacum) and in genetically modified plants with elevated thylakoid-associated PAs (Ioannidis and Kotzabasis Biochim Biophys Acta 1767:1371–1382, 2007; Ioannidis et al. Biochim Biophys Acta 1787:1215–1222, 2009). Here, we investigated further their quenching properties both in vivo in green algae and in vitro is isolated LHCII. In vivo spermine up-regulates NPQ in Scenedesums obliquus about 30%. In vitro putrescine—the obligatory metabolic precursor of PAs—has a marginal quenching effect, while spermidine and spermine exhibit strong quenching abilities in isolated LHCII up to 40%. Based on available 3D models of LHCII we report a special cavity of about 600 Å³ and a near-by larger pocket in the trimeric LHCII that could be of importance for the stimulation of qE by amines.     

Non-photochemical quenching of chlorophyll a fluorescence by oxidised plastoquinone: new evidences based on modulation of the redox state of the endogenous plastoquinone pool in broken spinach chloroplasts

Twenty-five years ago, non-photochemical quenching of chlorophyll fluorescence by oxidised plastoquinone (PQ) was proposed to be responsible for the lowering of the maximum fluorescence yield reported to occur when leaves or chloroplasts were treated in the dark with 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU), an inhibitor of electron flow beyond the primary quinone electron acceptor (Q_A) of photosystem (PS) II [C. Vernotte, A.L. Etienne, J.-M. Briantais, Quenching of the system II chlorophyll fluorescence by the plastoquinone pool, Biochim. Biophys. Acta 545 (1979) 519-527]. Since then, the notion of PQ-quenching has received support but has also been put in doubt, due to inconsistent experimental findings. In the present study, the possible role of the native PQ-pool as a non-photochemical quencher was reinvestigated, employing measurements of the fast chlorophyll a fluorescence kinetics (from 50 μs to 5 s). The about 20% lowering of the maximum fluorescence yield F_M, observed in osmotically broken spinach chloroplasts treated with DCMU, was eliminated when the oxidised PQ-pool was non-photochemically reduced to PQH₂ by dark incubation of the samples in the presence of NAD(P)H, both under anaerobic and aerobic conditions. Incubation under anaerobic conditions in the absence of NAD(P)H had comparatively minor effects. In DCMU-treated samples incubated in the presence of NAD(P)H fluorescence quenching started to develop again after 20-30 ms of illumination, i.e., the time when PQH₂ starts getting reoxidised by PS I activity. NAD(P)H-dependent restoration of F_M was largely, if not completely, eliminated when the samples were briefly (5 s) pre-illuminated with red or far-red light. Addition to the incubation medium of HgCl₂ that inhibits dark reduction of PQ by NAD(P)H also abolished NAD(P)H-dependent restoration of F_M. Collectively, our results provide strong new evidence for the occurrence of PQ-quenching. The finding that DCMU alone did not affect the minimum fluorescence yield F₀ allowed us to calculate, for different redox states of the native PQ-pool, the fractional quenching at the F₀ level (Q₀) and to compare it with the fractional quenching at the F_M level (Q_M). The experimentally determined Q₀/Q_M ratios were found to be equal to the corresponding F₀/F_M ratios, demonstrating that PQ-quenching is solely exerted on the excited state of antenna chlorophylls.     

Primary reactions of Photosystem II at low pH. 2. Light-induced changes of absorbance and electron spin resonance in spinach chloroplasts

The effects of lowering the pH on Photosystem II have been studied by measuring changes in absorbance and electron spin resonance in spinach chloroplasts.At pH values around 4 a light-induced dark-reversible chlorophyll oxidation by Photosystem II was observed. This chlorophyll is presumably the primary electron donor of system II. At pH values between 5 and 4 steady state illumination induced an ESR signal, similar in shape and amplitude to signal II, which was rapidly reversed in the dark. This may reflect the accumulation of the oxidized secondary donor upon inhibition of oxygen evolution. Near pH 4 the rapidly reversible signal and the stable and slowly decaying components of signal II disappeared irreversibly concomitant with the release of bound manganese.The results are discussed in relation to the effects of low pH on prompt and delayed fluorescence reported earlier (van Gorkom, H. J., Pulles, M. P. J., Haveman, J. and den Haan, G. A. (1976) Biochim. Biophys. Acta 423, 217–226).     

Kinetic study of oxygen evolution parameters in tris-washed,reactivated chloroplasts

Tris-washed chloroplasts which have lost the ability to evolve oxygen can be reactivated by the procedure of Yamashita. T., Tsuji, J. and Tomita, G. ((1971)Plant Cell Physiol. 12, 117–126) [7] to give 100% of the rate of control chloroplasts in continuous illumination. Furthermore, in flashing light the reactivated chloroplasts exhibit oxygen-yield oscillations of period four that are characteristic of the control. Similar kinetic parameters for intermediate steps in the water-splitting process are observed for the two preparations. We conclude that the reactivation procedure restores the native oxygen evolution mechanism to Tris-washed chloroplasts.A relatively rapid and reversible (0.5 s decay) light-induced component of EPR Signal II is observed upon inhibition of O₂ evolution by Tris washing (Babcock G. T. and Sauer, K. (1975) Biochim. Biophys. Acta 376, 315–328) [10]. Reactivated chloroplasts are similar to untreated chloroplasts in that this Signal II transient is not observed. Manganese, which is released by Tris treatment to the interior of the thylakoid membrane in an EPR-detectable state, is returned to an EPR-undetectable state by reactivation. The reactivation procedure does not require light to restore O₂ evolution and EDTA has no effect on the extent of reactivation. These results are discussed in terms of possible mechanisms for manganese incorporation into photosynthetic membranes.     

Reactions between primary and secondary acceptors of Photosystem II in Chlorella Pyrenoidosa under anaerobic conditions as studied by chlorophyll a fluorescence

The kinetics of the fluorescence yield Ф of chlorophyll a in Chlorella pyrenoidosa were studied under anaerobic conditions in the time range from 50 μs to several minutes after short ($\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 30}\text{ns}$ or 5 μs) saturating flashes. The fluorescence yield “in the dark” increased from $\text{Ф = 1}$ at the beginning to $\text{Ф ≈ 5}$ in about 3 h when single flashes separated by dark intervals of about 3 min were given.After one saturating flash, Ф increased to a maximum value (4–5) at 50 μs, then Ф decreased to about 3 with a half time of about 10 ms and to the initial value with a half time of about 2 s. When two flashes separated by 0.2 s were given, the first phase of the decrease after the second flash occurred within 2 ms. After one flash given at high initial fluorescence yield, the 10-ms decay was followed by a 10 s increase to the initial value. After the two flashes 0.2 s apart, the rapid decay was not follewed by a slow increase.These and other experiments provided additional evidence for and extend an earlier hypothesis concerning the acceptor complex of Photosystem II (Bouges-Bocquet, B. (1973) Biochim. Biophys. Acta 314, 250–256; Velthuys, B. R. and Amesz, J. (1974) Biochim. Biophys. Acta 333, 85–94): reaction center 2 contains an acceptor complex QR consisting of an electron-transferring primary acceptor molecule Q, and a secondary electron acceptor R, which can accept two electrons in succession, but transfers two electrons simultaneously to a molecule of the tertiary acceptor pool, containing plastoquinone (A). Furthermore, the kinetics indicate that 2 reactions centers of System I, excited by a short flash, cooperate directly or indirectly in oxidizing a plastohydroquinone molecule (A^2?). If initially all components between photoreaction 1 and 2 are in the reduced state the following sequence of reactions occurs after a flash has oxidised A^2? via System I: Q^?R^2? + A → Q^?R + A^2? → QR^? + A^2?. During anaerobiosis two slow reactions manifest themselves: the reduction of R (and A) within 1 s, presumably by an endogenous electron donor D₁, and the reduction of Q in about 10 s when R is in the state R^? and A in the state A^2?. An endogenous electron donor, D₂, and Q^? compete in reducing the photooxidized donor complex of System II in reactions with half times of the order of 1 s.     

Light-dependent quenching of chlorophyll fluorescence in pea chloroplasts induced by adenosine 5′-triphosphate

Addition of ATP to chloroplasts causes a reversible 25–30% decrease in chlorophyll fluorescence. This quenching is light-dependent, uncoupler insensitive but inhibited by DCMU and electron acceptors and has a half-time of 3 minutes. Electron donors to Photosystem I can not overcome the inhibitory effect of DCMU, suggesting that light activation depends on the reduced state of plastoquinone. Fluorescence emission spectra recorded at ?196°C indicate that ATP treatment increases the amount of excitation energy transferred to Photosystem I. Examination of fluorescence induction curves indicate that ATP treatment decreases both the initial (F_o) and variable (F_v) fluorescence such that the ratio of F_v to the maximum (F_m) yield is unchanged. The initial sigmoidal phase of induction is slowed down by ATP treatment and is quenched 3-fold more than the exponential slow phase, the rate of which is unchanged. A plot of F_v against area above the induction curve was identical plus or minus ATP. Thus ATP treatment can alter quantal distribution between Photosystems II and I without altering Photosystem II-Photosystem II interaction. The effect of ATP strongly resembles in its properties the phosphorylation of the light-harvesting complex by a light activated, ATP-dependent protein kinase found in chloroplast membranes and could be the basis of physiological mechanisms which contribute to slow fluorescence quenching in vivo and regulate excitation energy distribution between Photosystem I and II. It is suggested that the sensor for this regulation is the redox state of plastoquinone.