A new pathway of chlorophyll biosynthesis from long-wavelength protochlorophyllide Pchlide 686/676 in juvenile etiolated plants

By spectral methods, the final stages of chlorophyll formation from protochlorophyllide were studied using etiolated pea, bean, barley, wheat and maize plants in early stages (4 days) of growth. For these juvenile plants, along with the reaction chain known for mature (7–9-day-old) plants, a new reaction chain was found, which started with phototransformation of the long-wavelength form Pchlide 686/676(440) into Pchlide 653/648(440). (Pchlide 653/648(440) differs from the main known precursor form Pchlide 655/650(448)). The subsequent photoreduction of Pchlide 653/648(440) leads to the formation of Chlide 684/676(440), which is transformed into Chl 688/680(440) in the course of a dark reaction. After completion of this reaction, fast (20–30 s) quenching of the low-temperature fluorescence of the reaction product is observed with the formation of non-fluorescent Chl 680. The reaction accompanied by pigment fluorescence quenching is absent in pea mutants with depressed function of Photosystem II reaction centers. This suggests that the newly found reaction chain leads to the formation of chlorophyll of the Photosystem II core. This revised version was published online in June 2006 with corrections to the Cover Date.     

莲胚芽叶绿素合成对光照的依赖性

被子植物的叶绿素合成需要光照,但是莲（Nelumbo nucifera Gaertn.)胚芽却一直被猜测具有在黑暗中合成叶绿素的能力,因为莲胚芽变绿是在四重覆盖物（子叶、种皮、果皮和莲蓬）包被下几乎不大可能秀光的环境中发生的,本实验从正反两个方面否定了这种可能性;首先对处于发育早期的莲蓬进行遮光处理。结果发现莲胚芽虽然可以继续发育,但是它的叶绿素合成却受到严重抑制。积累了大量合成叶绿素的前体,并且这些前体主要与依赖光的原叶绿素酸酯氧还酶（LPOR）结合在一起;其次不依赖光的原叶绿素酸酯氧还酶（DPOR）的编码基因在物种间高度保守,但是用PCR的方法在功基因组中却扩增不同源序列,表明莲胚芽不大可能具有在黑暗中合成叶绿素所必需的酶。两方面实验结果表明,莲胚芽的叶绿素合成只能通过依赖光的途径进行。     

Quenching of a room temperature fluorescence band at 693 nm during photoactivation of the water-splitting system of Photosystem II in flashed barley leaves

The modifications of the room temperature fluorescence spectrum during the photoactivation of the water-splitting system by continuous illumination were investigated in flashed barley leaves. A blue shift of the chlorophyll fluorescence band was detected during the first 2 min of illumination. During this shift, a decrease of the fluorescence intensity around 693 nm could be demonstrated in difference spectra and in second derivative spectra. This decrease is interpreted as a quenching of PS II fluorescence during the photoactivation. A relative fluorescence increase around 672 nm also occurred during the same period and is thought to reflect rapid light-induced chlorophyll formation. The flashed leaves contained small amounts of photoactive photochlorophyllide which could be removed by a short flash of intense white light given before continuous illumination. The fact that such flash had only weak effect on the 693 nm fluorescence decrease, whereas it strongly reduced the amplitude of the 672 nm fluorescence increase, favours the above interpretations.Abbreviations chl chlorophyll - PS II Photosystem II - PS I Photosystem I     

Properties of inactive Photosystem II centers

A fraction (usually in the range of 10–25%) of PS II centers is unable to transfer electrons from the primary quinone acceptor Q_A to the secondary acceptor Q_B. These centers are inactive with respect to O₂ evolution since their reopening after photochemical charge separation to the S₂O_A ^- state involves predominantly a back reaction to S₁Q_A in the few seconds time range (slower phases are also occurring). Several properties of these centers are analyzed by fluorescence and absorption change experiments. The initial rise phase F_o-F_pl of fluorescence induction under weak illumination reflects both the closure of inactive centers and the modulation of the fluorescence yield by the S-states of the oxygen-evolving system: We estimate typical relative amplitudes of these contributions as, respectively, 65 and 35% of the F_o-F_pl amplitude. The half-rise time of this phase is significantly shorter than for the fluorescence induction in the presence of DCMU (in which all centers are involved). This finding is shown to be consistent with inactive centers sharing the same light-harvesting antenna as normal centers, a view which is also supported by comparing the dependence of the fluorescence yield on the amount of closed active or inactive centers estimated through absorption changes. It is argued that the exponential kinetics of the F_o-F_pl phase does not indicate absence of excitation energy transfer between the antennas of inactive and active centers. We show that the acceptor dichlorobenzoquinone does not restore electron transfer in inactive centers, in disagreement with previous suggestions. We confirm, however, the enhancement of steady-state electron flow caused by this quinone and suggest that it acts by relieving a blocking step involved in the reoxidation of a fraction of the plastoquinone pool. Part of the discrepancies between the present results and those from previous literature may arise from the confusion of inactive centers characterized on a single turnover basis and PS II centers that become blocked under steady-state conditions because of deficient reoxidation of their secondary acceptors.Abbreviations DCBQ 2,6-dichloro-p-benzoquinone - DCMU 3-(3,4-dichlorophenyl)-1,1-dimethylurea - DMQ 2,5-dimethyl-p-benzoquinone - PS photosystem     

Light-dependent modification of Photosystem II in spinach leaves

In dark-adapted spinach leaves approximately one third of the Photosystem II (PS II) reaction centers are impaired in their ability to transfer electrons to Photosystem I. Although these inactive PS II centers are capable of reducing the primary quinone acceptor, Q_A, oxidation of Q_A ^– occurs approximately 1000 times more slowly than at active centers. Previous studies based on dark-adapted leaves show that minimal energy transfer occurs from inactive centers to active centers, indicating that the quantum yield of photosynthesis could be significantly impaired by the presence of inactive centers. The objective of the work described here was to determine the performance of inactive PS II centers in light-adapted leaves. Measurements of PS II activity within leaves did not indicate any increase in the concentration of active PS II centers during light treatments between 10 s and 5 min, showing that inactive centers are not converted to active centers during light treatment. Light-induced modification of inactive PS II centers did occur, however, such that 75% of these centers were unable to sustain stable charge separation. In addition, the maximum yield of chlorophyll fluorescence associated with inactive PS II centers decreased substantially, despite the lack of any overall quenching of the maximum fluorescence yield. The effect of light treatment on inactive centers was reversed in the dark within 10–20 mins. These results indicate that illumination changes inactive PS II centers into a form that quenches fluorescence, but does not allow stable charge separation across the photosynthetic membrane. One possibility is that inactive centers are converted into centers that quench fluorescence by formation of a radical, such as reduced pheophytin or oxidized P680. Alternatively, it is possible that inactive PS II centers are modified such that absorbed excitation energy is dissipated thermally, through electron cycling at the reaction center.Abbreviations A518 absorbance change at 518 nm, reflecting the formation of an electric field across the thylakoid membrane - A_FL1 amplitude of the fast (<100 ms) phase of A518 induced by the first of two saturating, single-turnover flashes spaced 30 ms apart - A_FL2 amplitude of the fast (<100 ms) phase of A518 induced by the second of two saturating, single-turnover flashes spaced 50 ms apart - DCBQ 2,6-dichloro-p-benzoquinone - Fo yield of chlorophyll fluorescence when Q_A is fully oxidized - Fm yield of chlorophyll fluorescence when Q_A is fully reduced - Fx yield of chlorophyll fluorescence when Q_A is fully reduced at inactive PS II centers, but fully oxidized at active PS II centers - Pheo pheophytin - P680 the primary donor of Photosystem II - PPFD photosynthetic photon flux density - Q_A Primary quinone acceptor of PS II - Q_B secondary quinone acceptor of PS II     

Biosynthesis of chlorophyll from protochlorophyll(ide) in green plant leaves

Using spectral methods, the biosynthesis of protochlorophyll(ide) and chlorophyll(ide) in green plant leaves was studied. The main chlorophyll precursors in the green leaves (as in etiolated leaves) were photoactive photocholorophyll(ide) forms Pchl(ide)655/650(448) and Pchl(ide)653/648(440). The contributions into Chl biosynthesis of the shorter-wavelength precursor forms ,which were accumulated in darkened green leaves as well, were completely absent (of Pchl(ide) 633/628(440)) or insignificant (of Pchl(ide)642/635(444)).     

Evidence for localisation of accumulated chlorophyll cation on the D1-accessory chlorophyll in the reaction centre of Photosystem II

Absorption and circular dichroism spectra of Photosystem II (PS II) reaction centres (RC) were studied and compared with spectra calculated on the basis of point-dipole approximation. Chlorophyll cation was accumulated during a light treatment of PS II RC in the presence of artificial electron acceptor silicomolybdate. Light-induced difference spectra and their calculated counterparts revealed the location of accumulated cation at the accessory chlorophyll of the D1 protein subunit.     

Kinetics of EPR signal IIvf in chloroplast Photosystem II

The risetime of EPR signal II_vf (S II_vf) has been measured in oxygen-evolving Photosystem II particles from spinach chloroplasts at pH 6.0. The EPR signal shows an instrument-limited rise upon induction ($\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{? 3 μ}\text{s}$). These data are consistent with a model where the species Z responsible for S II_vf is the immediate electron donor to P-680⁺ in spinach chloroplasts. A new, faster decay component of S II_vf has also been detected in these experiments.     

Primary charge separation in Photosystem II

In this Minireview, we discuss a number of issues on the primary photosynthetic reactions of the green plant Photosystem II. We discuss the origin of the 683 and 679 nm absorption bands of the PS II RC complex and suggest that these forms may reflect the single-site spectrum with dominant contributions from the zero-phonon line and a pronounced ∼80 cm⁻¹ phonon side band, respectively. The couplings between the six central RC chlorins are probably very similar and, therefore, a `multimer' model arises in which there is no `special pair' and in which for each realization of the disorder the excitation may be dynamically localized on basically any combination of neighbouring chlorins. The key features of our model for the primary reactions in PS II include ultrafast (<500 fs) energy transfer processes within the multimer, `slow' (∼20 ps) energy transfer processes from peripheral RC chlorophylls to the RC multimer, ultrafast charge separation (<500 fs) with a low yield starting from the singlet-excited `accessory' chlorophyll of the active branch, cation transfer from this `accessory' chlorophyll to a `special pair' chlorophyll and/or charge separation starting from this `special pair' chlorophyll (∼8 ps), and slow relaxation (∼50 ps) of the radical pair by conformational changes of the protein. The charge separation in the PS II RC can probably not be described as a simple trap-limited or diffusion-limited process, while for the PS II core and larger complexes the transfer of the excitation energy to the PS II RC may be rate limiting. This revised version was published online in June 2006 with corrections to the Cover Date.     

Biosynthesis of non-fluorescent chlorophyll of Photosystem II core in greening plant leaves. Effect of etiolated plants growing under heat shock conditions (38 °C)

Preliminary dark incubation of etiolated pea and maize plants at 38 °C allowed to observe a new dark reaction of Chl biosynthesis occuring after photoconversion of protochlorophyllide Pchld 655/650 into chlorophyllide Chld 684/676. This reaction was accompanied by chlorophyllide esterification and by the bathochromic shift of pigment spectra: Chld 684/676 Chl 688/680. After completion of the reaction, a rapid (20–30 s at 26 °C) quenching of Chl 688/680 low-temperature fluorescence was observed. The reaction Chld 684/676 Chl 688/680 was inhibited under anaerobic conditions as well as in the presence of KCN; the reaction accompanied by Chl fluorescence quenching was inhibited in the leaves of pea mutants with impaired function of Photosystem II reaction centers. The spectra position of newly formed Chl, effects of Chl fluorescence quenching allowed to assume that the new dark reaction is responsible for biosynthesis of P–680, the key pigment of Photosystem II reaction centres.     

Cyclic electron flow around Photosystem II in vivo

The oxygen flash yield (Y_O2) and photochemical yield of PS II (_{PS II}) were simultaneously detected in intact Chlorella cells on a bare platinum oxygen rate electrode. The two yields were measured as a function of background irradiance in the steady-state and following a transition from light to darkness. During steady-state illumination at moderate irradiance levels, Y_O2 and _{PS II} followed each other, suggesting a close coupling between the oxidation of water and Q_A reduction (Falkowski et al. (1988) Biochim. Biophys. Acta 933: 432–443). Following a light-to-dark transition, however, the relationship between Q_A reduction and the fraction of PS II reaction centers capable of evolving O₂ became temporarily uncoupled. _{PS II} recovered to the preillumination levels within 5–10 s, while the Y_O2 required up to 60 s to recover under aerobic conditions. The recovery of Y_O2 was independent of the redox state of Q_A, but was accompanied by a 30% increase in the functional absorption cross-section of PS II (_{PS II}). The hysteresis between Y_O2 and the reduction of Q_A during the light-to-dark transition was dependent upon the reduction level of the plastoquinone pool and does not appear to be due to a direct radiative charge back-reaction, but rather is a consequence of a transient cyclic electron flow around PS II. The cycle is engaged in vivo only when the plastoquinone pool is reduced. Hence, the plastoquinone pool can act as a clutch that disconnects the oxygen evolution from photochemical charge separation in PS II.Abbreviations ADRY acceleration of the deactivation reactions of the water-splitting enzyme (agents) - Chl chlorophyll - cyt cytochrome - DCMU 3-(3,4-dichlorophenyl)-1,1-dimethylurea - F_O minimum fluorescence yield in the dark-adapted state - F_I minimum fluorescence yield under ambient irradiance or during transition from the light-adapted state - F_M maximum fluorescence yield in the dark-adapted state - F_M maximum fluorescence yield under ambient irradiance or during transition from light-adapted state - F_V, F_V variable fluorescence (F_V=F_M–F_O ; F_V=F_M–F_I) - FRR fast repetition rate (fluorometer) - _{PS II} quantum yield of Q_A reduction (_{PS II}=(F_M – F_O)/F_M or _{PS II})=(F_M= – F_I=)/F_M=) - LHCII Chl a/b light harvesting complexes of Photosystem II - OEC oxygen evolving complex of PS II - P680 reaction center chlorophyll of PS II - PQ plastoquinone - POH₂ plastoquinol - PS I Photosystem I - PS II Photosystem II - RC II reaction centers of Photosystem II - PS II the effective absorption cross-section of PHotosystem II - TL thermoluminescence - Y_O2 oxygen flash yield The US Government right to retain a non-exclusive, royalty free licence in and to any copyright is acknowledged.     

Formation of long-wavelength chlorophyllide (Chlide695) is required for the assembly of Photosystem II in etiolated barley leaves

Chlorophyll(ide) spectroscopic properties and Photosystem II assembly, monitored by 77 K variable fluorescence, were studied in etiolated barley leaves as a function of the extent of protochlorophyllide photoreduction by a single millisecond light flash of different intensities. Variable fluorescence, measured 2 hours after the flash, was only detected when the extent of phototransformation was higher than a threshold value of 0.4. Its development paralleled the formation of a chlorophyll emission component at 685 nm, which itself derived from long-wavelength chlorophyllide with an emission maximum at 695 nm. At low flash intensities, short-wavelength chlorophyllide forms preferentially accumulated and no Photosystem II fluorescence was detected after 2 hours. Chlorophyllide esterification was independent of the extent of phototransformation. These results suggested that the formation of long-wavelength chlorophyllide was essential for further assembly of Photosystem II. This interpretation was strengthened by the observed inhibition of both long-wavelength chlorophyllide formation and of variable fluorescence development in leaves treated with -aminolevulinic acid or in untreated leaves subjected to repeated flashes of low intensity.     

A simple model relating photoinhibitory fluorescence quenching in chloroplasts to a population of altered Photosystem II reaction centers

A model is presented describing the relationship between chlorophyll fluorescence quenching and photoinhibition of Photosystem (PS) II-dependent electron transport in chloroplasts. The model is based on the hypothesis that excess light creates a population of inhibited PS II units in the thylakoids. Those units are supposed to posses photochemically inactive reaction centers which convert excitation energy to heat and thereby quench variable fluorescence. If predominant photoinhibition of PS II and cooperativity in energy transfer between inhibited and active units are presumed, a quasi-linear correlation between PS II activity and the ratio of variable to maximum fluorescence, F_VF_M, is obtained. However, the simulation does not result in an inherent linearity of the relationship between quantum yield of PS II and F_VF_M ratio. The model is used to fit experimental data on photoinhibited isolated chloroplasts. Results are discussed in view of current hypotheses of photoinhibition.Abbreviations F_M maximum total fluorescence - F₀ initial fluorescence - F_V maximum variable fluorescence - PS Photosystem - Q_A, Q_B primary and secondary electron acceptors of Photosystem II     

Two electron donation sites for exogenous reductants in chloroplast Photosystem II

Two sites are distinguished for the oxidation of exogenous donors by Photosystem II in non-oxygen evolving chloroplasts. In the presence of lipophilic donors (e.g. phenylenediamine, benzidine, diphenylcarbazide), the rate for Signal IIf rereduction following a flash increases as the concentration of exogenous reductant increases. There is a decrease (20–40%) in Signal IIf magnitude accompanying donor addition at low (< 10^?5M) concentrations, but the extent of the decrease does not change further with increasing donor concentration. Complementary polarographic experiments monitoring donor (phenylenediamine) oxidation show an increase in oxidation rate with increasing donor concentration.In the presence of the hydrophilic donor, Mn²⁺, the Signal IIf decay halftime remains constant with increasing Mn²⁺ concentration. However, the flash-induced Signal IIf magnitude progressively decreases with increasing Mn²⁺ concentration.These results are interpreted in terms of two competing paths for the reduction of P680⁺. In one path P680⁺ reduction is accompanied by the appearance of Signal IIf, and lipophilic donors subsequently rereduce the Signal IIf species in a series reaction. This reduction follows pseudo-first order kinetics as a function of donor concentration. In the second path Mn²⁺ reduces P680⁺ in a parallel reaction that competes with the formation of the Signal IIf species. This results in a decrease in the magnitude of Signal IIf, but no change in its decay time.     

Low temperature phototransformations of protochlorophyll(ide) in etiolated leaves

By methods of difference and derivative spectroscopy it was shown that in etiolated leaves at 77 K three photoreactions of P650 protochlorophyllide take place which differ in their rates and positions of spectral maxima of the intermediates formed in the process: P650R668, P650R688, and P650R697. With an increase of temperature up to 233 K, in the dark, R688 and R697 are transformed into the known chlorophyllide forms C695/684 and C684/676, while R668 disappears with formation of a shorter wavelength form of protochlorophyllide with an absorption maximum at 643–644 nm.Along with these reactions, at 77 K phototransformations of the long-wave protochlorophyllide forms with absorption maxima at 658–711 nm into the main short-wave forms of protochlorophyllide are observed. At 233 K in the dark this reaction is partially reversible. This process may be interpreted as a reversible photodisaggregation of the pigment in vivo.The mechanism of P650 reactions and their role in the process of chlorophyll photobiosynthesis are discussed.Abbreviations P650 protochlorophyll(ide) with absorption maximum at 650 nm - C697/684 chlorophyllide with fluorescence maximum at 695 nm and absorption maximum at 684 nm - R697 intermediate with absorption maximum at 697 nm     

The relationship between millisecond luminescence and fluorescence in tobacco leaves during the induction period

Millisecond luminescence and fluorescence, from an intact tobacco (Nicotiana tabacum) leaf, were measured simultaneously during the induction period, as a function of the time. This was accomplished using a luminescence apparatus which separated out the faster luminescence components by subtraction of the accumulated slow-decaying ones. An antiparallel correlation between the two was observed, but only during a part of the induction period starting with the first fluorescence peak where the fluorescence decreases to a quasi plateau level. During this induction phase, luminescence rose very prominently to a maximum while fluorescence decreased. This correlation fits a linear dependence of the luminescence on the extent of RCs openness, as monitored by the photochemical quenching of the fluorescence. It may be concluded that during this induction phase, all other factors, which modulate luminescence (e.g. membrane potential), have become already steady and that the millisecond delayed luminescence reflects the photochemical reaction in an open center (i.e. with Q_A oxidized). This is further supported by steady-state experiments in thylakoid membranes. No correlations between luminescence and either momentary (F) or maximum (F_m) fluorescence during later induction phases can be pinpointed with confidence, although a trend of a parallel decrease at certain time intervals can be seen occasionally. Likewise, there is no relationship between the two in the very initial induction phase, during the rise of fluorescence from F_o to F_m, as noted earlier. This lack of correlation is presumably due to the dependence of luminescence on other parameters, which vary during these induction phases. The implications of these observations are discussed.Abbreviations RC reaction center - F, F_o, F_m momentary fluorescence level and levels for completely open and closed RCs, at any time during the induction period - F_o, F_m maximum values of F_o and F_m obtained for a dark adapted leaf - F_p the first peak fluorescence level in the fluorescence induction curve (F_p F_m) - q_P photochemical quenching coefficient - q_N non-photochemical quenching coefficient - L momentary luminescence intensity - L_m maximum value of L in the luminescence induction curve     

Energy transfers from Photosystem II to Photosystem I in Cryptomonas rufescens (Cryptophyceae)

In Cryptomonas rufescens (Cryptophyceae), phycoerythrin located in the thylakoid lumen is the major accessory pigment. Oxygen action spectra prove phycoerythrin to be efficient in trapping light energy.The fluorescence excitation spectra at ?196°C obtained by the method of Butler and Kitajima (Butler, W.L. and Kitajima, M. (1975) Biochim. Biophys. Acta 396, 72–85) indicate that like in Rhodophycease, chlorophyll a is the exclusive light-harvesting pigment for Photosystem I.For Photosystem II we can observe two types of antennae: (1) a light-harvesting chlorophyll complex connected to Photosystem II reaction centers, which transfers excitation energy to Photosystem I reaction centers when all the Photosystem II traps are closed. (2) A light-harvesting phycoerythrin complex, which transfers excitation energy exclusively to the Photosystem II reaction complexes responsible for fluorescence at 690 nm.We conclude that in Cryptophyceae, phycoerythrin is an efficient light-harvesting pigment, organized as an antenna connected to Photosystem II centers, antenna situated in the lumen of the thylakoid. However, we cannot afford to exclude that a few parts of phycobilin pigments could be connected to inactive chlorophylls fluorescing at 690 nm.     

Chlorophyll triplet states associated with Photosystem I and Photosystem II in thylakoids of the green alga Chlamydomonas reinhardtii

The analysis of FDMR spectra, recorded at multiple emission wavelengths, by a global decomposition technique, has allowed us to characterise the triplet populations associated with Photosystem I and Photosystem II of thylakoids in the green alga Chlamydomonas reinhardtii. Three triplet populations are observed at fluorescence emissions characteristic of Photosystem II, and their zero field splitting parameters have been determined. These are similar to the zero field parameters for the three Photosystem II triplets previously reported for spinach thylakoids, suggesting that they have a widespread occurrence in nature. None of these triplets have the zero field splitting parameters characteristic of the Photosystem II recombination triplet observed only under reducing conditions. Because these triplets are generated under non-reducing redox conditions, when the recombination triplet is undetectable, it is suggested that they may be involved in the photoinhibition of Photosystem II. At emission wavelengths characteristic of Photosystem I, three triplet populations are observed, two of which are attributed to the P₇₀₀ recombination triplet frozen in two different conformations, based on the microwave-induced fluorescence emission spectra and the triplet minus singlet difference spectra. The third triplet population detected at Photosystem I emission wavelengths, which was previously unresolved, is proposed to originate from the antenna chlorophyll of the core or the unusually blue-shifted outer antenna complexes of this organism.     

Electron donation in Photosystem II

The electron transfer resulting from illumination and dark storage of PS II has been studied using EPR signals from several electron carriers. The recombination of D⁺ (Signal II) and Q⁻_A formed by illumination occurred during dark storage at 77 K and was used to deplete reaction centres of D⁺. The donor D was then shown to be oxidized in the dark by the S₂ state of the oxygen-evolving complex. A slow change which occurred during dark storage of PS II samples was detected using the power saturation characteristics of D. We interpret this effect on D to be an indirect result of a rearrangement of the manganese complex during long-term dark adaptation. A role for D in the stability, protection and perhaps initial manganese binding of the oxygen-evolving complex is suggested.