The chlorophyll a fluorescence induction pattern in chloroplasts upon repetitive single turnover excitations: Accumulation and function of QB-nonreducing centers

The increase of chlorophyll fluorescence yield in chloroplasts in a 12.5 Hz train of saturating single turnover flashes and the kinetics of fluorescence yield decay after the last flash have been analyzed. The approximate twofold increase in F_m relative to F_o, reached after 30-40 flashes, is associated with a proportional change in the slow (1-20 s) component of the multiphasic decay. This component reflects the accumulation of a sizeable fraction of Q_B-nonreducing centers. It is hypothesized that the generation of these centers occurs in association with proton transport across the thylakoid membrane. The data are quantitatively consistent with a model in which the fluorescence quenching of Q_B-nonreducing centers is reversibly released after second excitation and electron trapping on the acceptor side of Photosystem II.     

Induction kinetics of delayed light emission in spinach chloroplasts

Induction curves of the delayed light emission in spinach chloroplasts were studied by measuring the decay kinetics after each flash of light. This study differs from previous measurements of the induction curves where only the intensities at one set time after each flash of light were recorded. From the decay kinetics after each flash of light, the induction curves of the delayed light emission measured 2 ms after a flash of light were separated into two components: one component due to the last flash only and one component due to all previous flashes before the last one. On comparing the delayed light induction curves of the two components with the fluorescence induction curves in chloroplasts treated with 3-(3,4-dichlorophenyl)-1,1-dimethylurea and in chloroplasts treated with hydroxylamine and 3-(3,4-dichlorophenyl)-1,1-dimethylurea, the component due to the last flash only is found to be dependent on the concentration of open reaction centers and the component due to all previous flashes except the last is dependent on the concentration of closed reaction centers. This implies that the yield of the fast decaying component of the delayed light emission is dependent on the concentration of open reaction centers and the yield of the slow decaying component is dependent on the concentration of closed reaction centers.     

Slow fluorescence fluctuations following high light to low light or dark transitions in Chlamydomonas reinhardi.

Slow fluorescence transients in Chlamydomonas reinhardi arise after transitions from high light intensities to low light or dark conditions. Characteristics of the newly described transient phenomena include: (a) A slow biphasic decrease in fluorescence yield occurs in the dark, followed by an even slower, hour long, increase in fluorescence. (b) A similar, but faster, fluorescence yield decrease and subsequent increase also occurs during low intensity illumination periods separating high light intervals, or after transitions from high intensity to low intensity light. (c) Short (several seconds) flashes of light given during a dark period have no effect on the dark fluorescence decay, regardless of the flash frequency. Such flash regimes accurately monitor the dark decline of the M2 level by tracing the parallel decay of flash-generated P2 (Kautsky) peaks. However, flashes during a low light illumination period do influence the decay kinetics. Frequent flashes allow decay similar to that occurring in dark, but less frequent flashes inhibit the decrease in fluorescence yield.     

Chlorophyll a fluorescence as a monitor of nanosecond reduction of the photooxidized primary donor P-680 Of photosystem II

1. Changes in the fluorescence yield of aerobic Chlorella vulgaris have been measured in laser flashes of 15 ns, 30 ns and 350 ns half time. The kinetics after the first flash given after a 3 min dark period could be simulated on a computer using the hypothesis that the oxidized acceptor Q and primary donor P+ are fluorescence quenchers, and Q- is a weak quencher, and that the reduction time for P+ is 20-35 ns. 2. The P+ reduction time for at least an appreciable part of the reaction centers was found to be longer after the second and subsequent flashes. In the first 5 flashes an oscillation was observed. Under steady state conditions, with a pulse separation of 3 s, a reduction time for P+ of about 400 ns for all reaction centers gave the best correspondence between computed and experimental fluorescence kinetics.     

Reactions between primary and secondary acceptors of photosystem II in Chlorella pyrenoidosa under anaerobic conditions as studied by chlorophyll fluorescence.

The kinetics of the fluorescence yield phi of chlorophyll a in Chlorella pyrenoidosa were studied under anaerobic conditions in the time range from 50 mus to several minutes after short (t 1/2 = 30 ns or 5 mus) saturating flashes. The fluorescence yield "in the dark" increased from phi = 1 at the beginning to phi approximately 5 in about 3 h when single flashes separated by dark intervals of about 3 min were given. After one saturating flash, phi increased to a maximum value (4-5) at 50 mus, then phi 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 followed 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 (A2-). 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 A2- via System I: Q-R2- + A leads to Q-R + A2- leads to QR- + A2-. 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 A2-. An endogenous electron donor, D2, and Q- complete in reducing the photooxidized donor complex of System II in reactions with half times of the order of 1 s.     

Effects of pH on reactions on the donor side of photosystem II.

The effects of pH on the increase of fluorescence yield measured in the microsecond range, and on the microsecond delayed fluorescence have been studied in dark adapted chloroplasts as a function of flash number. (1) At pH 7, the amplitude of the fast-phase of the microsecond fluorescence yield rise oscillated as a function of flash number with period 4 and with maxima on flashes 1 and 5, and minima on flashes 3 and 7. The damped oscillations were apparent over the range between 6 and 8, although the absolute amplitude of the fast phase was diminished at the lower end of the range. At pH 4, there was no fast phase in the rise and, at pH 9, an enhanced fast-phase occurred only for the first flash. (2) The decay of microsecond delayed fluorescence was described by the sum of exponentials with half-times of 10--15 mus and 40--50 mus. Over the pH range 6- less than 8, the extrapolated initial amplitude and the proportion of the change due to the faster component showed oscillations which were opposite in phase to those observed for the prompt fluorescence yield rise; the slower component showed weaker oscillations of the same phase. At pH 4, there were no oscillations and the slow phase predominated. At pH 9, the delayed fluorescence intensity was diminished on the first flash, and high on subsequent flashes. (3) The results are interpreted in terms of a model in which protons are released during all transitions of the S-states with the exception of S1 leads to S2, and in which ther are two sites of inhibition on the donor side of the photo-system at extreme pH values. At pH 4, electron donation to P+ occurs with a half-time approx. 135 mus, either by a back reaction from Q-, or from D; electron transport is interrupted between Z1 and P. At pH 9, electron transport is inhibited between Z1 and Z2; rapid re-reduction of P+ by Z1 occurs after 1 flash, and on subsequent flashes electrons from D, an alternative donor reduce P+. The location of the positive charge on states S2 and S3 is discussed.     

Chlorophyll a fluorescence transient as an indicator of active and inactive Photosystem II in thylakoid membranes

Upon illumination, a dark-adapted photosynthetic sample shows time-dependent changes in chlorophyll (Chl) a fluorescence yield, known as the Kautsky phenomenon or the OIDPS transient. Based on the differential effects of electron acceptors such as 2,5-dimethyl-p-benzoquinone (DMQ) and 2,6-dichloro-p-benzoquinone (DCBQ) on Chl a fluorescence transients of spinach thylakoids, we suggest that the OID phase reflects the reduction of the electron acceptor QA to QA- in the inactive PS II (see Graan, T. and Ort, D. (1986) Diochim. Biophys. Acta 852, 320-330). In spinach thylakoids, heat-induced increase of the Chl a fluorescence yield is also differentially sensitive to the addition of DMQ and DCBQ suggesting that this increase is mainly on the 'I' level, and thus heating is suggested to convert active PS II to inactive PS II centers. The kinetics of decay of QA-, calculated from variable Chl a fluorescence, was analyzed into three exponential components (365-395 microseconds; 6-7 ms; and 1.4-1.7 s). In heated samples, the decay rate of variable Chl a fluorescence is slower than the normal back-reaction rate; there is a preponderance of the slow component that may be due, partly, to the active centers undergoing slow back reaction between QA- and the S2 state of the oxygen-evolving complex.     

Comparison of ATP-induced and DCMU-induced increases of chlorophyll fluorescence

A comparative study of the ATP-induced and the DCMU-induced increases of dark chlorophyll fluorescence after activation of the latent ATPase gave the following results: (1) The ATP-induced fluorescence rise exceeds the DCMU-induced rise by an amount equivalent to the rapid component of the biphasic ATP-induced change. There is complementarity between the slow component and any preceding DCMU-induced fluorescence rise. (2) Up to 10^?4 M DCMU (3-(3′,4′-dichlorophenyl)-1,1′-dimethylurea)), with the slow component being completely suppressed, the rapid ATP-induced phase is unaffected. It becomes eliminated, though, with an I₅₀ of about 3 · 10^?4 M. (3) No binary oscillations in dependence of the number of preilluminating flashes are observed for the rapid ATP-induced fluorescence increase. Under identical conditions such oscillations are found upon DCMU-addition. (4) The amplitude of the rapid ATP-induced fluorescence rise is unaffected by closure of Photosystem II reaction centers in presence of DCMU and NH₂OH by a single saturating flash (removal of about 50% of total quenching). With further flashes and gradual complete removal of quenching, the rapid ATP-induced change is eliminated with a two-step dependency. It is concluded that the rapid phase of the ATP-induced increase in fluorescence reflects reverse electron flow at non-B-type reaction centers, while the slow phase is linked to reverse electron flow at B type centers. On the basis of these results a model is proposed for heterogeneous interactions between the ATPase and B-type and non-B-type electron-transport chains. ‘Direct coupling’ appears to be possible between CF₀-CF₁ and those electron-transport chains which are located in the stroma-exposed margin region of the grana stacks (PS IIβ units with non-B-type properties).     

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.     

The effects of low temperature acclimation and photoinhibitory treatments on Photosystem 2 studied by thermoluminescence and fluorescence decay kinetics

The effects of low temperature acclimation and photoinhibitory treatment on Photosystem 2 (PS 2) have been studied by thermoluminescence and chlorophyll fluorescence decay kinetics after a single turnover saturating flash. A comparison of unhardened and hardened leaves showed that, in the hardened case, a decrease in overall and B-band thermoluminescence emissions occurred, indicating the presence of fewer active PS 2 reaction centers. A modification in the form of the B-band emission was also observed and is attributed to a decrease in the apparent activation energy of recombination in the hardened leaves. The acclimated leaves also produced slower Q_A ^– reoxidation kinetics as judged from the chlorophyll fluorescence decay kinetics. This change was mainly seen in an increased lifetime of the slow reoxidation component with only a small increase in its amplitude. Similar changes in both thermoluminescence and fluorescence decay kinetics were observed when unhardened leaves were given a high light photoinhibitory treatment at 4°C, whereas the hardened leaves were affected to a much lesser extent by a similar treatment. These results suggest that the acclimated plants undergo photoinhibition at 4°C even at low light intensities and that a subsequent high light treatment produces only a small additive photoinhibitory effect. Furthermore, it can be seen that photoinhibition eventually gives rise to PS 2 reaction centers which are no longer functional and which do not produce thermoluminescence or variable chlorophyll fluorescence.Abbreviations D1 The 32 kDa protein of Photosystem 2 reaction center - F_m maximum chlorophyll fluorescence yield - F₀ minimal chlorophyll fluorescence yield obtained when all PS 2 centers are open - F_i intermediate fluorescence level corresponding to PS 2 centers which are loosely or not connected to plastoquinone (non-B centers) - F_v maximum variable chlorophyll fluorescence yield (F_v=F_m–F₀) - PS 2 Photosystem 2 - Q_A and Q_B respectively, primary and secondary quinonic acceptors of PS 2 - S1, S2 and S3 respectively, the one, two and three positively charged states of the oxygen evolving system - Z secondary donor of PS 2     

Chlorophyll a fluorescence as a monitor of nanosecond reduction of the photooxidized primary donor P-680 of Photosystem II

1. Changes in the fluorescence yield of aerobic Chlorella vulgaris have been measured in laser flashes of 15 ns, 30 ns and 350 ns half time. The kinetics after the first flash given after a 3 min dark period could be simulated on a computer using the hypothesis that the oxidized acceptor Q and primary donor P⁺ are fluorescence quenchers, and Q⁻ is a weak quencher, and that the reduction time for P⁺ is 20–35 ns.

2. The P⁺ reduction time for at least an appreciable part of the reaction centers was found to be longer after the second and subsequent flashes. In the first 5 flashes an oscillation was observed. Under steady state conditions, with a pulse separation of 3 s, a reduction time for P⁺ of about 400 ns for all reaction centers gave the best correspondence between computed and experimental fluorescence kinetics.     

Isolation of a fast decay in submillisecond Chlorella luminescence

Using a simple He-Ne (632.8-nm) laser phosphoroscope steady-state luminescence from Chlorella pyrenoidosa was studied from 50 μs to 1.1 ms between 1 ms long exciting flashes. The following results were obtained: (1) prior freezing or ultraviolet irradiation changed the time course of the luminescence to a rapid decay with a half-time of about 110 μs; (2) 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU) suppressed the 110-μs luminescence; (3) spectrally, all observed luminescence was, within possible error, identical to fluorescence; (4) no effect on the luminescence intensity from pulsed magnetic fields up to 30 kgauss was observed; (5) the relative fluorescence yield, measured simultaneously with luminescence, was found to be constant.Our principal conclusions, supported mainly by experiments with DCMU, are: (1) the 110-μs decay is a distinct component of the total steady-state luminescence; (2) prior freezing or ultraviolet irradiation isolates this component of the luminescence by suppressing all other components; (3) the half-time and intensity of this component are temperature independent in the interval 0–22 °C.     

The emission yields of delayed and prompt fluorescence from chloroplasts.

1. The decay of delayed fluorescence from chloroplasts blocked with 3-(3,4-dichlorophenyl)-1,1-dimethylurea and uncoupled with gramicidin has been measured in the time range 0.75--45 ms by use of a laser phosphoroscope. 2. The decays have been analysed as the sum of three first-order components of approximate half-lives 0.2, 2.5 and 300 ms by a computer-assisted least-squares fit procedure. 3. The prompt fluorescence yield of the chloroplasts was manipulated by changing the cation concentration of the chloroplast-suspending medium. 4. Analysis of the concentration dependence of the components of the delayed fluorescence decay and of the prompt fluorescence inductions indicates that the emission yield of the intermediate (tau approximately 2.5 ms) component of the decay is equal to the fluorescence yield of a Photosystem II photosynthetic unit with an open trap, and that for the slow (tau approximately 300 ms) component the emission yield is equal to the total Photosystem II prompt fluorescence yield. 5. It is concluded that the delayed fluorescence yield in the time range studied is a complex function of time, which may be due to there being different mechanisms leading to delayed fluorescence production at short and long times after cessation of illumination.     

Energy transfer and distribution in the red alga Porphyra perforata studied using picosecond fluorescence spectroscopy

The detailed process of excitation transfer among the antenna pigments of the red alga Porphyra perforata was investigated by measuring time-resolved fluorescence emission spectra using a single-photon timing system with picosecond resolution. The fluorescence decay kinetics of intact thalli at room temperature revealed wavelength-dependent multi-component chlorophyll a fluorescence emission. Our analysis attributes the majority of chlorophyll a fluorescence to excitation originating in the antennae of PS II reaction centers and emitted with maximum intensities at 680 and 740 nm. Each of these fluorescence bands was characterized by two kinetic decay components, with lifetimes of 340-380 and 1700-2000 ps and amplitudes varying with wavelength and the photochemical state of the PS II reaction centers. In addition, a small contribution to the long-wavelength fluorescence band is proposed to arise from chlorophyll a antennae coupled to PS I. This component displays fast decay kinetics with a lifetime of approx. 150 ps. Desiccation of the thalli dramatically increases the contribution of this fast decay component.     

Inhibition of the reoxidation of the secondary electron acceptor of Photosystem II by bicarbonate depletion

In bicarbonate-depleted chloroplasts, the chlorophyll a fluorescence decayed with a halftime of about 150 ms after the third flash, and appreciably faster after the first and second flash of a series of flashes given after a dark period. After the fourth to twentieth flashes, the decay was also slow. After addition of bicarbonate, the decay was fast after all the flashes of the sequence. This indicates that the bicarbonate depletion inhibits the reoxidation of the secondary acceptor R²⁻ by the plastoquinone pool; R is the secondary electron acceptor of pigment system II, as it accepts electrons from the reduced form of the primary electron acceptor (Q⁻). This conclusion is consistent with the measurements of the DCMU (3-(3,4-dichlorophenyl)-1,1-dimethylurea)-induced chlorophyll a fluorescence after a series of flashes in the presence and the absence of bicarbonate, if it is assumed that DCMU not only causes reduction of Q if added in the state QR⁻, but also if added in the state QR²⁻.     

Nanosecond fluorescence from chromatophores of Rhodopseudomonas sphaeroides and Rhodospirillum rubrum

Single-photon counting techniques were used to measure the fluorescence decay from Rhodopseudomonas sphaeroides and Rhodospirillum rubrum chromatophores after excitation with a 25-ps, 600-nm laser pulse. Electron transfer was blocked beyond the initial radical-pair state (PF) by chemical reduction of the quinone that serves as the next electron acceptor. Under these conditions, the fluorescence decays with multiphasic kinetics and at least three exponential decay components are required to describe the delayed fluorescence. Weak magnetic fields cause a small increase in the decay time of the longest component. The components of the delayed fluorescence are similar to those found previously with isolated reaction centers. We interpret the multi-exponential decay in terms of two small (0.01-0.02 eV) relaxations in the free energy of PF, as suggested previously for reaction centers. From the initial amplitudes of the delayed fluorescence, it is possible to calculate the standard free-energy difference between the earliest resolved form of PF and the excited singlet state of the antenna complexes in R. rubrum strains S1 and G9. The free-energy gap is found to be about 0.10 eV. It also is possible to calculate the standard free-energy difference between PF and the excited singlet state of the reaction center bacteriochlorophyll dimer (P). Values of 0.17 to 0.19 eV were found in both R. rubrum strains and also in Rps. sphaeroides strain 2.4.1. This free-energy gap agrees well with the standard free-energy difference between PF and P determined previously for reaction centers isolated from Rps. sphaeroides strain R26. The temperature dependence of the delayed fluorescence amplitudes between 180 K and 295 K is qualitatively different in isolated reaction centers and chromatophores. However, the temperature dependence of the calculated standard free-energy difference between P* and PF is similar in reaction centers and chromatophores of Rps. sphaeroides. The different temperature dependence of the fluorescence amplitudes in reaction centers and chromatophores arises because the free-energy difference between P* and the excited antenna is dominated by the entropy change associated with delocalization of the excitation in the antenna. We conclude that the state PF is similar in isolated reaction centers and in the intact photosynthetic membrane. Chromatophores from Rps. sphaeroides strain R-26 exhibit an anomalous fluorescence component that could reflect heterogeneity in their antenna.     

A seconds range component of the reoxidation of the primary Photosystem II acceptor,Q. Effects of bicarbonate depletion in chloroplasts

Broken chloroplasts depleted of bicarbonate (HCO^?₃) show 30–50% inhibition of the Hill reaction in low-intensity light. Also, photoreactions excited by repetitive flashes measured by oxygen evolution, ESR signal IIvf, and absorption changes at 680 and 334 nm show inhibition of 30–50%. An effect of HCO^?₃ was sought to explain these phenomena. The decay of chlorophyll a fluorescence yield in the millisecond and seconds range, following a single flash, was observed to be multiphasic with a very slow component of 1–2 s half-time. In HCO^?₃ -depleted samples this component is enhanced 2- or 3-fold. Since this occurs even after one flash, it is suggested that HCO^?₃ affects the Q^? B → QB^? reaction. In this work it is shown that 40% inhibition of oxygen flash yield is relieved to a great extent if the excitation flash rate is decreased from 2 to 0.33 Hz. A measurement of 520 nm absorption change in the presence of ferricyanide, which is proportional to Photosystem II charge separation, shows a similar inhibition that is dependent on flash rate. The maximum amplitude of variable fluorescence yield and 520 nm absorption change after a single flash are unaffected by HCO^?₃ depletion. The dark distribution of oxygen-evolution S-states is found to be shifted to a more reduced configuration in depleted samples. It is concluded that normal charge separation occurs in HCO^?₃ -depleted Photosystem II reaction centers but that a large fraction of Q^? decays so slowly that not all Q^? is reoxidized between flashes given at a rate of 1 or 2 Hz. Thus, a portion of the Photosystem II centers would be closed to photochemistry. There is a reversible effect of HCO^?₃ depletion on the oxygen-evolution system that is observed as a shift in the dark distribution of S-states.     

Picosecond fluorescence kinetics and energy transfer in chloroplasts and algae

Single-photon timing with picosecond resolution is used to investigate the kinetics of the fluorescence emission of chlorophyll a in chloroplasts from spinach and pea and in the algae Chlorella pyrenoidosa and Chlamydomonas reinhardii. The fluorescence decay is best described by three exponential components in all species. At low light intensity and with open reaction centers of Photosystem II (F₀), we find lifetimes of approx. 100, 400 and 1100 ps for the three components. Closing the reaction centers by addition of 3-(3′,4′-dichlorophenyl)-1,1-dimethylurea plus hydroxylamine and by increasing light intensity produces only minor changes in the almost constant fast- and medium-lifetime components; however, there is a dramatic increase in the yield of the slow component, by a factor of about 20, accompanied by only a modest increase in the lifetime to 2200 ps (F_max). In good agreement with previous fluorescence lifetime measurements, we find an increase in the averaged lifetime of the three components from 0.5 to 2.0 ns, which is proportional to the 4-fold increase in the total fluorescence yield. Our time-resolved results are inconsistent with models which are based on the proportionality between lifetime and yield and which involve a homogeneous origin of fluorescence that is sensitive to the state of the reaction centers. We conclude that the variable part of the fluorescence, which is dominated by the slow phase, reflects the kinetics of charge recombination in the reaction center, as proposed previously (Klimov, V.V., Allakhverdiev, S.I. and Paschenko, V.Z. (1978) Dokl. Akad. Nauk S.S.S.R. 242, 1204–1207). The modest increase in lifetime of the slow phase indicates the presence of some energy transfer between photosynthetic units.     

Evidence for the contribution of the S-state transitions of oxygen evolution to the initial phase of fluorescence induction

Fluorescence induction of isolated spinach chloroplasts was measured by using weak continuous light. It is found that the kinetics of the initial phase of fluorescence induction as well as the initial fluorescence level F_j are influenced by the number of preilluminating flashes, and shows damped period 4 oscillation. Evidence is given to show that it is correlated with the S-state transitions of oxygen evolution. Based on the previous observations that the S states can modulate the fluorescence yield of Photosystem II, a simulating calculation suggests that, in addition to the Photosystem II centers inactive in the plastoquinone reduction, the S-state transitions can also make a contribution to the intial phase of fluorescence induction.Abbreviations DCMU 3-(3,4-dichlorophenyl)-1,1-dimethyl urea - F₀ non-variable fluorescence level emitted when all PS II centers are open - F_i initial fluorescence level immediately after shutter open - F_pt intermediate plateau fluorescence level - F_m maximum fluorescence level emitted when all PS II centers are closed - PS II Photosystem II - Q_A primary quinone acceptor of PS II - Q_B secondary quinone acceptor of PS II     

Examination of chlorophyll fluorescence decay kinetics in sulfur deprived algae Chlamydomonas reinhardtii

Chlorophyll fluorescence decay kinetics was measured in sulfur deprived cells of green alga Chlamydomonas reinhardtii with a home made picosecond fluorescence laser spectrometer. The measurements were carried out on samples either shortly adapted to the dark ('Fo conditions') or treated to reduce Qa ('Fm conditions'). Bi-exponential fitting of decay kinetics was applied to distinguish two components one of them related to energy trapping (fast component) and the other to charge stabilization and recombination in PS 2 reaction centers (slow component). It was found that the slow component yield increased by 2.0 and 1.2 times when measured under 'Fo' and 'Fm conditions', respectively, in sulfur deprived cells as compared to control ones. An additional rapid rise of the slow component yield was observed when incubation was carried out in a sealed bioreactor and cell culture turned to anaerobic conditions. The obtained results strongly indicate the existence of the redox control of PS 2 activity during multiphase adaptation of C. reinhardtii to sulfur deficiency stress. Probable mechanisms responsible for the observed increased recombinant fluorescence yield in starved cells are discussed.