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.     

Photosynthetic Unit Size during the Synchronous Life Cycle of Scenedesmus

Apparent size of the photosynthetic unit (chlorophyll/O₂ per flash) was estimated by O₂ yield of repetitive short flashes on cell samples taken at various times from a synchronized culture (14-hour light, 10-hour dark) of Scenedesmus obliquus. Unit size was essentially invariant (< 10% variation) with a mean value of 1750 chlorophyll/O₂ per flash. In contrast, the light-saturated photosynthetic rate per unit chlorophyll, or turnover rate of the photosynthetic unit, varied with the life cycle, rising 40% in the first three hours of the light period and decaying slowly thereafter. The results are taken as evidence that the metabolic machinery is subject to far greater control and adjustment than is the photochemical machinery.     

Flash kinetics and light intensity dependence of oxygen evolution in the blue-green alga Anacystis nidulans

Patterns of oxygen evolution in flashing light for the blue-green alga Anacystis nidulans are compared with those for broken spinach chloroplasts and whole cells of the green alga Chlorella pyrenoidosa. The oscillations of oxygen yield with flash number that occur in both Anacystis and Chlorella, display a greater degree of damping than do those of isolated spinach chloroplasts. The increase in damping results from a two- to threefold increase in the fraction (α) of reaction centers “missed” by a flash. The increase in α cannot be explained by non-saturating flash intensities or by the dark reduction of the oxidized intermediates formed by the flash. Anaerobic conditions markedly increase α in Anacystis and Chlorella but have no effect on α in broken spinach chloroplasts. The results signify that the mechanism of charge separation and water oxidation involved in all three organisms is the same, but that the pool of secondary electron acceptors between Photosystem II and Photosystem I is more reduced in the dark, in the algal cells, than in the isolated spinach chloroplasts.Oxygen evolution in flashing light for Anacystis and Chlorella show light saturation curves for the oxygen yield of the third flash (Y₃) that differ markedly from those of the steady-state flashes (Y_s). In experiments in which all flashes are uniformly attenuated, Y₃ requires nearly twice as much light as Y_s to reach half-saturation. Under these conditions Y₃ has a sigmoidal dependence on intensity, while that of Y_s is hyperbolic. These differences depend on the number of flashes attenuated. When any one of the first three flashes is attenuated, the variation of Y₃ with intensity resembles that of Y_s. When two of the first three flashes are attenuated, Y₃ is intermediate in shape between the two extremes. A quantitative interpretation of these results based on the model of Kok et al. (Kok, B., Forbush, B. and McGloin, M. (1970) Photochem. Photobiol. 11, 457–475, and Forbush, B., Kok, B. and McGloin, M. P. (1971) Photochem. Photobiol. 14, 307–321) fits the experimental data.     

Oxygen Evolution from Algae Illuminated by Short and Long Flashes of Light

The oxygen produced by illuminating Ankistrodesmus braunii withsingle light flashes has been determined using the Hersch galvanicoxygen cell. Measurements were made with the cells suspendedin alkaline solution equilibrated with nitrogen containing oxygenat a partial pressure of 10^–4 mm. Hg.

1. A single light flash, if very brief (less than 5 millisec.)results in no measurable oxygen production; a longer flash (35millisec.) gave a yield of approximately 1 mole O₂/800 moleschlorophyll.
2. A pair of flashes suitably spaced gave a greateryield thanthe sum of the yields when given individually, althoughonewas so brief that by itself it produced no measurable oxygen.The yield of a long flash preceded by a short flash was twiceas great as that of the long flash given alone; when the flashorder was reversed the combined yield was smaller but stillgreater than for the long flash alone.
3. The combined yieldof a pair of flashes varies with the intervalseparating theflashes, rapidly rising to a maximum and thendecaying moreslowly. With a long and short flash the optimalinterval was0.7 sec. but some enhancement of yield was observedwhen theflashes were separated by as long as 10 or 15 sec.
4. When theflashes were superimposed on background illuminationthe yieldswere increased and were measurable even for the shortflashes.Measured with background illumination the optimal yieldfora pair of short flashes was obtained with flashes separatedby about 0.05 sec.

     

Redox transients of P680 associated with the incremental chlorophyll‐a fluorescence yield rises elicited by a series of saturating flashes in diuron‐treated photosystem II core complex of Thermosynechococcus vulcanus

Recent chlorophyll‐a fluorescence yield measurements, using single‐turnover saturating flashes (STSFs), have revealed the involvement of a rate‐limiting step in the reactions following the charge separation induced by the first flash. As also shown here, in diuron‐inhibited PSII core complexes isolated from Thermosynechococcus vulcanus the fluorescence maximum could only be reached by a train of STSFs. In order to elucidate the origin of the fluorescence yield increments in STSF series, we performed transient absorption measurements at 819 nm, reflecting the photooxidation and re‐reduction kinetics of the primary electron donor P680. Upon single flash excitation of the dark‐adapted sample, the decay kinetics could be described with lifetimes of 17 ns (～50%) and 167 ns (～30%), and a longer‐lived component (～20%). This kinetics are attributed to re‐reduction of P680^?+ by the donor side of PSII. In contrast, upon second‐flash (with Δt between 5 μs and 100 ms) or repetitive excitation, the 819 nm absorption changes decayed with lifetimes of about 2 ns (～60%) and 10 ns (～30%), attributed to recombination of the primary radical pair P680^?+Pheo^?–, and a small longer‐lived component (～10%). These data confirm that only the first STSF is capable of generating stable charge separation – leading to the reduction of Q_A; and thus, the fluorescence yield increments elicited by the consecutive flashes must have a different physical origin. Our double‐flash experiments indicate that the rate‐limiting steps, detected by chlorophyll‐a fluorescence, are not correlated with the turnover of P680.     

Reversible inactivation of photosystem II reaction centers in cation-depleted chloroplast membranes

Isolated pea chloroplasts were washed once in 10 mm NaCl and were then suspended in “low-salt” medium. Approximately one-half of the photosystem II reaction centers of these salt-depleted membranes were found to be photochemically inactive. These units became active in the presence of low concentrations of divalent cations (5–10 mm Mg²⁺) or high concentrations of monovalent cations (150–200 mm Na⁺), as evidenced by a twofold increase in the steady-state flash yield of oxygen evolution under short (~10-μs) saturating repetitive flashes (two per second). The half-maximal increase in flash yield occurred at ~2 mM Mg²⁺ or ~75 mm Na⁺. The flash yield of hydroxylamine oxidation in these low-salt chloroplasts increased twofold after Mg²⁺ addition, indicating that the cation action was close to the reaction-center chlorophyll complex. The relation between flash yield and dark time between flashes was not changed significantly by Mg²⁺, indicating that the rate-limiting step of the overall electron transport (H₂0 —→ ferricyanide) was not affected significantly. When the rate-limiting step was bypassed using silicomolybdate as the photosystem II electron acceptor (in the presence of diuron), the reduction rate doubled in the presence of Mg²⁺, even under continuous, saturating light. In glutaraldehyde-fixed chloroplasts, Mg²⁺ did not increase the flash yield of O² evolution; this suggests that protein conformational changes in the chloroplast membranes were involved in Mg²⁺ activation of photosystem II centers.     

Photosynthetic Apparatus Formation during the Cell Cycle of Chlorella

Synchronous cell division in cultures of Chlorella vulgaris Beijerinck was induced by intermittent illumination: 9 hours light, 6 hours darkness. The rate of photosynthetic O₂ evolution per cell increases 4-fold in a one-step manner at the beginning of the light period, to the same extent as the increase in cell number. Over the division cycle, the following accumulation times during the light period were found: chlorophyll a, between 2 and 8 hours, chlorophyll b, between 5 and 8 hours, reaction centers of photosystems I and II, between 2 and 6 hours; and cytochrome f, between 2.5 and 5 hours. Cytochrome f accumulation is closely followed by an increase in amplitude of the rapid phase in light-induced absorption increase at 520 nanometers and in intensity of the delayed light emission. Enhancement of the delayed fluorescence yield per flash under continuous illumination (caused by the establishment of the pH difference across the thylakoid membrane) is maximal by the first hour of the light period.     

Investigation of the CO(2) Dependence of Quantum Yield and Respiration in Eucalyptus pauciflora

In leaves of C₃ plants, the rate of nonphotorespiratory respiration appears to be higher in darkness than in the light. This change from a high to a low rate of carbon loss with increasing photon flux density leads to an increase in the apparent quantum yield of photosynthetic CO₂ assimilation at low photon flux densities (Kok effect). The mechanism of this suppression of nonphotorespiratory respiration is not understood, but biochemical evidence and the observation that a Kok effect is often not observed under low O₂, has led to the suggestion that photorespiration might be involved in some way. This hypothesis was tested with snowgum (Eucalyptus pauciflora Sieb. ex Spreng.) using gas exchange methods. The test was based on the assumption that if photorespiration were involved, then it would be expected that the intercellular partial pressure of CO₂ would also have an influence on the Kok effect. Under normal atmospheric levels of CO₂ and O₂, a Kok effect was found. Changing the intercellular partial pressure of CO₂, however, did not affect the estimate of nonphotorespiratory respiraton, and it was concluded that its decrease with increasing photon flux density did not involve photorespiration. Concurrent measurements showed that the quantum yield of net assimilation of CO₂ increased with increasing intercellular partial pressure of CO₂, and this increase agreed closely with predictions based on recent models of photosynthesis.     

Primary and secondary electron donors in Photosystem II of chloroplasts. Rates of electron transfer and location in the membrane

Absorption changes at 820 or 515 nm after a short laser flash were studied comparatively in untreated chloroplasts and in chloroplasts in which oxygen evolution is inhibited.In chloroplasts pre-treated with Tris, the primary donor of Photosystem II (P-680) is oxidized by the flash, as observed by an absorption increase at 820 nm. After the first flash it is re-reduced in a biphasic manner with half-times of 6 μs (major phase) and 22 μs. After the second flash, the 6 μs phase is nearly absent and P-680⁺ decays with half-times of 130 μs (major phase) and 22 μs. Exogenous electron donors (MnCl₂ or reduced phenylenediamine) have no direct influence on the kinetics of P-680⁺.In untreated chloroplasts the 6 and 22 μs phases are of very small amplitude, either at the 1st, 2nd or 3rd flash given after dark-adaptation. They are observed, however, after incubation with 10 mM hydroxylamine.These results are interpreted in terms of multiple pathways for the reduction of P-680⁺: a rapid reduction (<1 μs) by the physiological donor D₁; a slower reduction (6 and 22 μs) by donor D′₁, operative when O₂ evolution is inhibited; a back-reaction (130 μs) when D′₁ is oxidized by the pre-illumination in inhibited chloroplasts. In Tris-treated chloroplasts the donor system to P-680⁺ has the capacity to deliver only one electron.The absorption change at 515 nm (electrochromic absorption shift) has been measured in parallel. It is shown that the change linked to Photosystem II activity has nearly the same magnitude in untreated chloroplasts or in chloroplasts treated with hydroxylamine or with Tris (first and subsequent flashes). Thus we conclude that all the donors (P-680, D₁, D′₁) are located at the internal side of the thylakoid membrane.     

The Kok Effect in Chlamydomonas reinhardi

A Haxo-Blinks rate-measuring oxygen electrode together with a modulated light source gave an average current signal (change in net O₂ exchange) and a modulated current signal (photosynthetic O₂ evolution). Using this apparatus, net O₂ exchange and photosynthetic O₂ evolution at low intensities have been studied in the green alga, Chlamydomonas reinhardi. At both 645 nm and 695 nm, the curves of net O₂ exchange as a function of light intensity were steeper at lowest intensities than about compensation, indicative of the Kok effect. The effect was greater at 695 nm than at 645 nm. The corresponding curves of photosynthetic O₂ evolution, on the other hand, showed no Kok effect; here, the slope was lowest at lowest intensity. The absence of the Kok effect in O₂ evolution, together with its sensitivity to monofluoroacetic acid, show that it is due to an interaction of photosynthesis and respiration. The effect was exaggerated by 3-(3,4-dichlorophenyl)-1,1-dimethylurea. In the presence of concentrations of this inhibitor sufficient to inhibit O₂ evolution completely, a light-induced change in net O₂ exchange remained. This was interpreted as a system I dependent depression of respiratory O₂ uptake. The Kok effect remained undiminished in concentrations of carbonyl cyanide m-chlorophenylhydrazone and 2,4-dinitrophenol which partially uncoupled either oxidative phosphorylation alone or both oxidative and photosynthetic phosphorylations. The above results can be explained within a model of the Kok effect in which O₂ uptake is depressed by diversion of reductant away from respiratory electron transport and into photosystem I. The same photodepression of O₂ uptake also appears to account for a transient in net O₂ exchange seen in several algae upon turning off the light.     

Quantitative relationship between two reaction centersin the photosynthetic system of blue-green algae

The quantitative relationship between reaction centers I andII was studied with blue-green algae Anabaena cylindrica, Anabaenavariabilis and Anacystis nidulans grown under different lightconditions. The number of reaction centers I was estimated fromthe P700 content and that of reaction centers II, from the O₂yield of repetitive short flashes. Supplementary determinationswere done with three other blue-green algae and one red alga.The maximum number of reaction centers II counted from the O₂yield of repetitive short flashes was markedly smaller thanthe total number of P700 in all algae tested when the algaewere grown under weak light; in the extreme case (Anabaena cylindrica),the ratio was only 0.258?0.015. This ratio became larger andclose to unity when the algae were grown under stronger light.Variation in the number of reaction centers in a single cellsuggested that reaction center I was a variable component. Ourresults indicate that the proportion of the two reaction centersmay markedly vary in blue-green algae depending on the growthconditions (Received November 13, 1978; )     

Is functional manganese involved in hydrogen-peroxide-stimulated anomalous oxygen evolution in CACl2-washed photosystem II membranes?

When detergent-derived photosystem II (PSII) membranes are treated with CaCl₂ to remove the three extrinsic proteins associated with the O₂-evolving complex, the resulting membranes (CaPSII) can still catalyze water oxidation if sufficient Ca²⁺ and Cl^- are present. When CaPSII membranes are exposed to single turnover flashes on an O₂ rate electrode, anomalous O₂ is produced by the first two flashes. The addition of catalase to the membrane suspension completely inhibits O₂ produced by the first two flashes, but not by subsequent flashes. Exogenous H₂O₂ stimulates anomalous O₂ production by the first few flashes in CaPSII membranes, but not in control PSII membranes. Diuron (DCMU) does not inhibit H₂O₂-stimulated O₂ production by the first flash. However, it does inhibit the O₂ yield of all subsequent flashes, indicating that all flash-induced O₂ signals in CaPSII membranes are dependent on photosystem II electron transport. H₂O₂ stimulation of O₂ yields is inhibited in Tris-, heat-, and EDTA-(ethylenediaminetetraacetic acid)-treated CaPSII. In the presence of high salt, H₂O₂ (but not EDTA) treatment of CaPSII, extracts Mn functional in normal photosynthetic O₂ evolution. The addition of exogenous Mn²⁺ reconstitutes anomalous O₂ production in Tris-and H₂O₂/EDTA-treated CaPSII preparations but only in the presence of H₂O₂. Anomalous H₂O₂-stimulated O₂ production can be observed both with a Clark electrode (steady state) and an O₂ rate electrode (flash sequence). The mechanism involves electron donation from H₂O₂, mediated by free Mn²⁺, to PSII, and the 33-kDa extrinsic protein under some conditions can block this process. Since H₂O₂ can remove functional Mn from CaPSII membranes, its presence can convert functional Mn to the Mn²⁺ mediator state required for anomalous O₂ production. EDTA binds Mn in CaPSII disrupted by H₂O₂ and prevents anomalous O₂ evolution.Abbreviations CaPSII a PSII preparation washed with approximately 1M CaCl₂ - Chl chlorophyll - DCBQ 2,6-dichloro-p-benzoquinone - DCMU (diuron) 3-(3,4-dichlorophenyl)-1,1-dimethylurea - EDTA ethylenediaminetetraacetic acid - MES 2-[N-morpholino]-ethanesulfonic acid - PSII a detergent-derived photosystem II membrane preparation - RC reaction center - Tris tris(hydroxymethyl)-aminomethane - Y_n oxygen rate electrode flash yield resulting from the nth flash of a sequence of single turnover flashes of light Operated by the Midwest Research Institute for the U.S. Department of Energy under contract DE-AC02-83CH10093.     

S-state dependence of the miss probability in Photosystem II

The oxygen production of dark-adapted Photosystem II upon illumination by a series of single-turnover flashes shows a damped period four oscillation with flash number. The damping is attributed to `misses' resulting from a statistical probability that a reaction center fails to produce a stable charge separation after a saturating flash. The origin of misses is of interest because its probable dependence on flash number, in principle, affects the quantitative interpretation of all measurements on phenomena associated with the period four oscillation. We show that the kinetics of chlorophyll fluorescence yield transients induced by a flash series can be used to estimate the relative amplitudes of the miss probability on each flash. It is concluded that a major part of the misses must be caused by failure of the reduction of the oxidized primary electron donor chlorophyll P680⁺ by the secondary donor tyrosine Y_Z before the charge separation is lost by recombination. The probability of this failure is found to increase with the oxidation state of the oxygen-evolving complex: more than half of it occurs upon charge separation in the S₃ state, which is attributed to the presence of Y_Z ^ox S₂ in Boltzmann equilibrium with Y_ZS₃. This revised version was published online in June 2006 with corrections to the Cover Date.     

How fast can Photosystem II split water? Kinetic performance at high and low frequencies

Molecular oxygen evolution from water is a universal signature of oxygenic photosynthesis. Detection of the presence, speed and efficiency of the enzymatic machinery that catalyzes this process in vivo has been limited. We describe a laser-based fast repetition rate fluorometer (FRRF) that allows highly accurate and rapid measurements of these properties via the kinetics of Chl-a variable fluorescence yield (Fv) in living cells and leaves at repetition rates up to 10 kHz. Application to the detection of quenching of Fv is described and compared to flash-induced O₂ yield data. Period-four oscillations in both Fv and O₂, caused by stimulation of primary charge recombination by the O₂ evolving complex (WOC) within Photosystem II (PS II), are directly compared. The first quantitative calculations of the enzymatic parameters of the Kok model (α – miss; β – double hit; S-state populations) are reported from Fv data over a 5 kHz range of flash frequencies that is 100-fold wider than previously examined. Comparison of a few examples of cyanobacteria, green algae and spinach reveals that Arthrospira m., a cyanobacterium that thrives in alkaline carbonate lakes, exhibits the fastest water-splitting rates ever observed thus farin vivo. In all oxygenic phototrophs examined thus far, an unprecedented large increase in the Kok α and β parameters occur at both high and low flash frequencies, which together with their strong correlation, indicates that PS II-WOC centers split water at remarkably lower efficiencies and possibly by different mechanisms at these extreme flash frequencies. Revisions to the classic Kok model are anticipated.     

Defining the Far-Red Limit of Photosystem II in Spinach

The far-red limit of photosystem II (PSII) photochemistry was studied in PSII-enriched membranes and PSII core preparations from spinach (Spinacia oleracea) after application of laser flashes between 730 and 820 nm. Light up to 800 nm was found to drive PSII activity in both acceptor side reduction and oxidation of the water-oxidizing CaMn₄ cluster. Far-red illumination induced enhancement of, and slowed down decay kinetics of, variable fluorescence. Both effects reflect reduction of the acceptor side of PSII. The effects on the donor side of PSII were monitored using electron paramagnetic resonance spectroscopy. Signals from the S₂-, S₃-, and S₀-states could be detected after one, two, and three far-red flashes, respectively, indicating that PSII underwent conventional S-state transitions. Full PSII turnover was demonstrated by far-red flash-induced oxygen release, with oxygen appearing on the third flash. In addition, both the pheophytin anion and the Tyr Z radical were formed by far-red flashes. The efficiency of this far-red photochemistry in PSII decreases with increasing wavelength. The upper limit for detectable photochemistry in PSII on a single flash was determined to be 780 nm. In photoaccumulation experiments, photochemistry was detectable up to 800 nm. Implications for the energetics and energy levels of the charge separated states in PSII are discussed in light of the presented results.     

Photodamage to Pigment in the Photosystem Ⅱ Reaction Center D1/D2/Cytochrome b559 Complex

Strong light （800μmol photons/m^2 per s）-induced bleaching of the pigment in the isolated photosystem Ⅱ reaction center （PSII RC） under aerobic conditions （in the absence of electron donors or acceptors） was studied using high-pressure liquid chromatography （HPLC）, absorption spectra, 77K fluorescence spectra and resonance Raman spectra. Changes in pigment composition of the PSII RC as determined by HPLC after light treatment were as follows： with Increasing illumination time chlorophyll （Chl） a and β-carotene （β-car） content decreased. However, decreases in pheophytin （Pheo） could not be observed because of the mixture of the Pheo formed by degraded chlorophyll possibly. On the basis of absorption spectra, it was determined that, with a short time of illuminatlon, the initial bleaching occurred maximally at 680 nm but that with Increasing Illumination time there was a blue shift to 678 nm. It was suggested that P680 was destroyed Initially, followed by the accessory chlorophyll. The activity of P680 was almost lost after 10 mln light treatment. Moreover, the bleaching of Pheo and β-car was observed at the beginning of illumination. After Illumination, the fluorescence emission Intensity changed and the fluorescence maximum blue shifted, showing that energy transfer was disturbed. Resonance Raman spectra of the PSII RC excited at 488.0 and 514.5 nm showed four main bands, peaking at 1 527 cm^-1 （υ101）, 1 159 cm^-1 （υ2）, 1 006 cm^-1 （υ3）, 966 cm^-1 （υ4） for 488.0 nm excitation and 1 525 cm^-1 （υ1）, 1 159 cm^-1 （υ2）, 1 007 cm^-1 （υ3）, 968 cm^-1 （υ4） for 514.5 nm excitation. It was confirmed that two spectroscopically different β-car molecules exist In the PSII RC. After light treatment for 20 mln, band positions and bandwidths were unchanged. This indicates that carotenoid configuration Is not the parameter that regulates photoprotectlon in the PSII RC.     

Electron transport to oxygen mitigates against the photoinactivation of Photosystem II in vivo

The role of electron transport to O₂ in mitigating against photoinactivation of Photosystem (PS) II was investigated in leaves of pea (Pisum sativum L.) grown in moderate light (250 mol m^–2 s^–1). During short-term illumination, the electron flux at PS II and non-radiative dissipation of absorbed quanta, calculated from chlorophyll fluorescence quenching, increased with increasing O₂ concentration at each light regime tested. The photoinactivation of PS II in pea leaves was monitored by the oxygen yield per repetitive flash as a function of photon exposure (mol photons m^–2). The number of functional PS II complexes decreased nonlinearly with increasing photon exposure, with greater photoinactivation of PS II at a lower O₂ concentration. The results suggest that electron transport to O₂, via the twin processes of oxygenase photorespiration and the Mehler reaction, mitigates against the photoinactivation of PS II in vivo, through both utilization of photons in electron transport and increased nonradiative dissipation of excitation. Photoprotection via electron transport to O₂ in vivo is a useful addition to the large extent of photoprotection mediated by carbon-assimilatory electron transport in 1.1% CO₂ alone.Abbreviations Fm, Fo, Fv- maximal, initial (corresponding to open PS II traps) and variable chlorophyll fluorescence yield, respectively - NPQ- non-photochemical quenching - PS- photosystem - Q_A- primary quinone acceptor - qP- photochemical quenching coefficient     

Period four oscillations in chlorophyll a fluorescence

The discovery of period four oscillations of the fluorescence yield under flashing light demonstrated that not only the redox state of the Photosystem II (PS II) electron acceptor Q_A, but also the oxygen evolving cycle (described by the S states) modulates the fluorescence yield of chlorophyll (Chl). The positive charges accumulated on the donor side of PS II act on the fluorescence yield (measured in the Q_A ⁻ state during a strong flash) through the concentration of the quencher P₆₈₀ ⁺, the oxidized form of PS II reaction center Chl a. However, the period four oscillations of the fluorescence yield detected 1 s after a strong flash (in the P₆₈₀Q_A state) have not yet been fully explained. This revised version was published online in June 2006 with corrections to the Cover Date.     

Bump amplitude,but not latency and time-course,can depend on position of illumination in Limulus photoreceptor cells

Bumps, the responses evoked by single photons in the ventral photoreceptor of Limulus polyphemus, were measured under voltage clamp conditions. The bumps were evoked by illuminating the photoreceptor either with a global flash or a small light spot (diameter about 5 m) which covers only 0.25% of the light-sensitive part of the cell membrane. The light energy of both flash types was adjusted so that each flash on average evoked one bump. Parameters of bumps evoked by local light spots in various membrane areas were compared with those evoked by light flashes which illuminated the whole photoreceptor. The results show that the bump amplitude depends on the location of the illumination. Membrane areas were found where the average value of the bump amplitude was either smaller or larger for a spot illumination than for a whole cell illumination. The latency and the shape (e.g. width) of the bumps does not depend on the location of the illumination.     

Redox Processes in the Blue Light Response of Guard Cell Protoplasts of Commelina communis L

Guard cell protoplasts from Commelina communis L. illuminated with red light responded to a blue light pulse by an H⁺ extrusion which lasted for about 10 minutes. This proton extrusion was accompanied by an O₂ uptake with a 4H⁺ to O₂ ratio. The response to blue light was nil in darkness without a preillumination period of red light and increased with the duration of the red light illumination until about 40 minutes. However, acidification in response to a pulse of blue light was obtained in darkness when external NADH (1 millimolar) was added to the incubation medium, suggesting that redox equivalents necessary for the expression of the response to blue light in darkness may be supplied via red light. In accordance with this hypothesis, the photosystem II inhibitor 3-(3,4-dichlorophenyl)-1, 1-dimethylurea (10 micromolar) decreased the acidification in response to blue light more efficiently when it was added before red light illumination than before the blue light pulse. In the presence of hexacyanoferrate, the acidification in response to a blue light pulse was partly inhibited (53% of control), suggesting a competition for reducing power between ferricyanide reduction and the response to blue light.