The fast and slow kinetics of chlorophyll a fluorescence induction in plants, algae and cyanobacteria: a viewpoint

The light-induced/dark-reversible changes in the chlorophyll (Chl) a fluorescence of photosynthetic cells and membranes in the μs-to-several min time window (fluorescence induction, FI; or Kautsky transient) reflect quantum yield changes (quenching/de-quenching) as well as changes in the number of Chls a in photosystem II (PS II; state transitions). Both relate to excitation trapping in PS II and the ensuing photosynthetic electron transport (PSET), and to secondary PSET effects, such as ion translocation across thylakoid membranes and filling or depletion of post-PS II and post-PS I pools of metabolites. In addition, high actinic light doses may depress Chl a fluorescence irreversibly (photoinhibitory lowering; q(I)). FI has been studied quite extensively in plants an algae (less so in cyanobacteria) as it affords a low resolution panoramic view of the photosynthesis process. Total FI comprises two transients, a fast initial (OPS; for Origin, Peak, Steady state) and a second slower transient (SMT; for Steady state, Maximum, Terminal state), whose details are characteristically different in eukaryotic (plants and algae) and prokaryotic (cyanobacteria) oxygenic photosynthetic organisms. In the former, maximal fluorescence output occurs at peak P, with peak M lying much lower or being absent, in which case the PSMT phases are replaced by a monotonous PT fluorescence decay. In contrast, in phycobilisome (PBS)-containing cyanobacteria maximal fluorescence occurs at M which lies much higher than peak P. It will be argued that this difference is caused by a fluorescence lowering trend (state 1 → 2 transition) that dominates the FI pattern of plants and algae, and correspondingly by a fluorescence increasing trend (state 2 → 1 transition) that dominates the FI of PBS-containing cyanobacteria. Characteristically, however, the FI pattern of the PBS-minus cyanobacterium Acaryochloris marina resembles the FI patterns of algae and plants and not of the PBS-containing cyanobacteria.     

Fluorescence induction in the phycobilisome-containing cyanobacterium Synechococcus sp PCC 7942: Analysis of the slow fluorescence transient

At room temperature, the chlorophyll (Chl) a fluorescence induction (FI) kinetics of plants, algae and cyanobacteria go through two maxima, P at ∼ 0.2-1 and M at ∼ 100-500 s, with a minimum S at ∼ 2-10 s in between. Thus, the whole FI kinetic pattern comprises a fast OPS transient (with O denoting origin) and a slower SMT transient (with T denoting terminal state). Here, we examined the phenomenology and the etiology of the SMT transient of the phycobilisome (PBS)-containing cyanobacterium Synechococcus sp PCC 7942 by modifying PBS → Photosystem (PS) II excitation transfer indirectly, either by blocking or by maximizing the PBS → PS I excitation transfer. Blocking the PBS → PS I excitation transfer route with N-ethyl-maleimide [NEM; A. N. Glazer, Y. Gindt, C. F. Chan, and K.Sauer, Photosynth. Research 40 (1994) 167-173] increases both the PBS excitation share of PS II and Chl a fluorescence. Maximizing it, on the other hand, by suspending cyanobactrial cells in hyper-osmotic media [G. C. Papageorgiou, A. Alygizaki-Zorba, Biochim. Biophys. Acta 1335 (1997) 1-4] diminishes both the PBS excitation share of PS II and Chl a fluorescence. Here, we show for the first time that, in either case, the slow SMT transient of FI disappears and is replaced by continuous P → T fluorescence decay, reminiscent of the typical P → T fluorescence decay of higher plants and algae. A similar P → T decay was also displayed by DCMU-treated Synechococcus cells at 2 °C. To interpret this phenomenology, we assume that after dark adaptation cyanobacteria exist in a low fluorescence state (state 2) and transit to a high fluorescence state (state 1) when, upon light acclimation, PS I is forced to run faster than PS II. In these organisms, a state 2 → 1 fluorescence increase plus electron transport-dependent dequenching processes dominate the SM rise and maximal fluorescence output is at M which lies above the P maximum of the fast FI transient. In contrast, dark-adapted plants and algae exist in state 1 and upon illumination they display an extended P → T decay that sometimes is interrupted by a shallow SMT transient, with M below P. This decay is dominated by a state 1 → 2 fluorescence lowering, as well as by electron transport-dependent quenching processes. When the regulation of the PBS → PS I electronic excitation transfer is eliminated (as for example in hyper-osmotic suspensions, after NEM treatment and at low temperature), the FI pattern of Synechococcus becomes plant-like.     

A direct demonstration of closed-state inactivation of K+ channels at low pH

Lowering external pH reduces peak current and enhances current decay in Kv and Shaker-IR channels. Using voltage-clamp fluorimetry we directly determined the fate of Shaker-IR channels at low pH by measuring fluorescence emission from tetramethylrhodamine-5-maleimide attached to substituted cysteine residues in the voltage sensor domain (M356C to R362C) or S5-P linker (S424C). One aspect of the distal S3-S4 linker α-helix (A359C and R362C) reported a pH-induced acceleration of the slow phase of fluorescence quenching that represents P/C-type inactivation, but neither site reported a change in the total charge movement at low pH. Shaker S424C fluorescence demonstrated slow unquenching that also reflects channel inactivation and this too was accelerated at low pH. In addition, however, acidic pH caused a reversible loss of the fluorescence signal (pKa = 5.1) that paralleled the reduction of peak current amplitude (pKa = 5.2). Protons decreased single channel open probability, suggesting that the loss of fluorescence at low pH reflects a decreased channel availability that is responsible for the reduced macroscopic conductance. Inhibition of inactivation in Shaker S424C (by raising external K⁺ or the mutation T449V) prevented fluorescence loss at low pH, and the fluorescence report from closed Shaker ILT S424C channels implied that protons stabilized a W434F-like inactivated state. Furthermore, acidic pH changed the fluorescence amplitude (pKa = 5.9) in channels held continuously at −80 mV. This suggests that low pH stabilizes closed-inactivated states. Thus, fluorescence experiments suggest the major mechanism of pH-induced peak current reduction is inactivation of channels from closed states from which they can activate, but not open; this occurs in addition to acceleration of P/C-type inactivation from the open state.     

Effect of the P700 pre-oxidation and point mutations near A0 on the reversibility of the primary charge separation in Photosystem I from Chlamydomonas reinhardtii

Time-resolved fluorescence studies with a 3-ps temporal resolution were performed in order to: (1) test the recent model of the reversible primary charge separation in Photosystem I (Müller et al., 2003; Holwzwarth et al., 2005, 2006), and (2) to reconcile this model with a mechanism of excitation energy quenching by closed Photosystem I (with P700 pre-oxidized to P700⁺). For these purposes, we performed experiments using Photosystem I core samples isolated from Chlamydomonas reinhardtii wild type, and two mutants in which the methionine axial ligand to primary electron acceptor, A₀, has been change to either histidine or serine. The temporal evolution of fluorescence spectra was recorded for each preparation under conditions where the “primary electron donor,” P700, was either neutral or chemically pre-oxidized to P700⁺. For all the preparations under study, and under neutral and oxidizing conditions, we observed multiexponential fluorescence decay with the major phases of ∼ 7 ps and ∼ 25 ps. The relative amplitudes and, to a minor extent the lifetimes, of these two phases were modulated by the redox state of P700 and by the mutations near A₀: both pre-oxidation of P700 and mutations caused slight deceleration of the excited state decay. These results are consistent with a model in which P700 is not the primary electron donor, but rather a secondary electron donor, with the primary charge separation event occurring between the accessory chlorophyll, A, and A₀. We assign the faster phase to the equilibration process between the excited state of the antenna/reaction center ensemble and the primary radical pair, and the slower phase to the secondary electron transfer reaction. The pre-oxidation of P700 shifts the equilibrium between the excited state and the primary radical pair towards the excited state. This shift is proposed to be induced by the presence of the positive charge on P700⁺. The same charge is proposed to be responsible for the fast A⁺A₀⁻ → AA₀ charge recombination to the ground state and, in consequence, excitation quenching in closed reaction centers. Mutations of the A₀ axial ligand shift the equilibrium in the same direction as pre-oxidation of P700 due to the up-shift of the free energy level of the state A⁺A₀⁻.     

Quaternary structures and low frequency molecular vibrations of haems of deoxy and oxyhaemoglobin studied by resonance Raman scattering

The influence of quaternary structure on the low frequency molecular vibrations of the haem within deoxyhaemoglobin (deoxy Hb) and Oxyhaemoglobin (oxy Hb) was studied by resonance Raman scattering. The FeO₂ stretching frequency was essentially identical between the high affinity (R) state (Hb A) and low affinity (T) state (Hb Kansas and Hb M Milwaukee with inositol hexaphosphate). However in deoxy Hb, only one of the polarized lines showed an appreciable frequency shift upon switch of quaternary structure, i.e. 215 to 218 cm^?1 for the T state (Hb A, des-His(146β) Hb, and des-Arg(141α) Hb (pH 6.5)) and 220 to 221 cm^?1 for the R state (des-Arg(141α) Hb (pH 9.0), des-His(146β)-Arg(141α) Hb and NES des-Arg(141α) Hb). Based on the observed ⁵⁴Fe isotopic frequency shift of the corresponding Raman lines of deoxy Hb A (214 → 217 cm^?1), of deoxy NES des-Arg Hb (220 → 223 cm^?1), of the protoporphyrinato-Fe(II)-(2-methylimidazole) complex in the ferrous high spin state (207 → 211 cm^?1) and of deoxymyoglobin (220 → 222 cm^?1) (Kitagawa et al., 1979), and on substitution of perdeuterated for protonated 2-methylimidazole in the deoxygenated picket fence complex (T_pivPP)Fe²⁺ (2-MeIm) (209 → 206 cm^?1), and on the results of normal co-ordinates calculation carried out previously, we proposed that the 216 cm^?1 line of deoxy Hb is associated primarily with the FeN_ε(HisF8) stretching mode and accordingly that the FeN_ε(HisF8) bond is stretched in the T state due to a strain exerted by globin.     

Changes of the chlorophyll fluorescence induction kinetics of C3 and CAM plants during day/night cycles

The induction kinetics of the 680 nm chlorophyll fluorescence were measured on attached leaves of Kalanchoë daigremontiana R. Hamet et Perr. (CAM plant), Sedum telephium L. and Sedum spectabile Bor. (C₃ plant in spring, CAM plant in summer) and Raphanus sativus L. (C₃ plant) at three different times during a 12/12h day/night cycle. During the fluorescence transient the fluorescence intensity at the O, P and T-level (f_O, f_max, f_st,) was different for the plant species tested; this may be due to their different leaf structure, pigment composition and organization of their photosystems. The kinetics of the fluorescence induction depended on the time of preillumination or dark adaptation during the light/dark cycle but not on the type of primary CO₂ fixation mechanism (C₃ and CAM). For dark adapted leaves measured either at the end of the dark phase or after dark adaptation of plants taken from the light phase a higher P-level fluorescence, a higher variable fluorescence (P-O) and a larger complementary area were found than for leaves of plants taken directly from the light phase. This indicates the presence of largely oxidized photosystem 2 acceptor pools during darkness. During the light phase the fluorescence decline after the P-level was faster than during the dark phase; from this we conclude that the light adaptation of the photosynthetic apparatus (state 1→ state 2 transition, Δ pH) during the induction period proceeded faster in plants taken from the light phase than in plants taken from the dark phase.     

Structural dynamics of bacterial ribosomes: IV. Classification of ribosomes by subunit interaction

Previous studies in this series (M. Noll et al., 1973a,b; Noll & Noll, 1974) have established that in Escherichia coli the ability of subunits to form vacant 70 S ribosome couples at 10 mm-Mg²⁺ is a stringent condition for activity in the translation of natural messenger (R17 RNA). The present study examines the structural basis of subunit interaction. It is found that vacant ribosome couples prepared by various methods fall into two classes, “tight” couples and “loose” couples, that differ in the affinity of their subunits for each other. Detection and separation of the two particle species is possible by ultracentrifugation. When analyzed on sucrose gradients at 6 mm-Mg²⁺ and moderate speed (30,000 revs/min), tight couples sediment as undissociated 70 S ribosomes, whereas loose couples are completely dissociated and sediment as 30 S and 50 S subunits. At 15 mm-Mg²⁺ in the gradient, both species sediment as a 70S peak. At 10 mm-Mg²⁺ and 60,000 revs/min, two peaks (63 S and 55 S) are seen because the high hydrostatic pressure causes more pronounced dissociation of the loose than of the tight couples.Association is dependent on the state of each subunit. Removal of Mg²⁺ produces 30 S b-particles that are unable to associate with 50 S subunits unless reconverted to the 30 S a-form by thermal activation according to Zamir et al. (1971). In the dissociated state, 50 S subunits tend to change irreversibly to a 50 S b-modification that produces loose couples upon association with 30 S a-subunits. The 50 S a → 50 S b transition could not be related to breaks in 23 S RNA detectable by sedimentation analysis. However, mild treatment of 50 S a-subunits with RNase produces particles that associate with 30 S a-subunits to couples that are less stable than the loose couples resulting from a dissociation/association step.Fresh S-30 extracts contain only tight couples (approx. 80%) and subunits (approx. 20%). Our results suggest that loose couples are artefacts derived from tight couples by a structural or conformational modification.Interaction-free subunits that previously were found to form a primitive initiation complex with poly(U) and tRNA_Phe (Schreier & Noll, 1970,1971), and to be active in phenylalanine polymerization, are shown to consist of the b-form of each subunit.It is likely that conflicting results obtained in the study of the mechanism of initiation and other aspects of ribosome function are due to the lack of structural criteria required for standardizing the ribosome preparation used by different investigators. This study provides simple methods and criteria to classify and separate physically all ribosome and ribosome subunits that have been observed into well-defined classes of predictable activity.     

Energy transfer between Photosystem II and Photosystem I in chloroplasts

A model for the photochemical apparatus of photosynthesis is presented which accounts for the fluorescence properties of Photosystem II and Photosystem I as well as energy transfer between the two photosystems. The model was tested by measuring at ?196 °C fluorescence induction curves at 690 and 730 nm in the absence and presence of 5 mM MgCl₂ which presumably changes the distribution of excitation energy between the two photosystems. The equations describing the fluorescence properties involve terms for the distribution of absorbed quanta, α, being the fraction distributed to Photosystem I, and β, the fraction to Photosystem II, and a term for the rate constant for energy transfer from Photosystem II to Photosystem I,k_T(II→I). The data, analyzed within the context of the model, permit a direct comparison of α andk_T(II→I) in the absence (?) and presence (+) of Mg²⁺:α/^?α⁺= 1.2andk/^?_T(II→I)k⁺_T(II→I)= 1.9. If the criterion thatα + β = 1 is applied absolute values can be calculated: in the presence of Mg²⁺,a⁺ = 0.27 and the yield of energy transfer,φ⁺_T(II→I) varied from 0.065 when the Photosystem II reaction centers were all open to 0.23 when they were closed. In the absence of Mg²⁺,α^? = 0.32 andφ_T(II→I) varied from 0.12 to 0.28.The data were also analyzed assuming that two types of energy transfer could be distinguished; a transfer from the light-harvseting chlorophyll of Photosystem II to Photosystem I,k_T(II→I), and a transfer from the reaction centers of Photosystem II to Photosystem I,k_t(II→I). In that caseα/^?α⁺= 1.3,k/^?_T(II→I)k⁺_T(II→I)= 1.3 andk/^?_t(II→I)k⁺_(tII→I)= 3.0. It was concluded, however, that both of these types of energy transfer are different manifestations of a single energy transfer process.     

The inter-monomer interface of the major light-harvesting chlorophyll a/b complexes of photosystem II (LHCII) influences the chlorophyll triplet distribution

Under strong light conditions, long-lived chlorophyll triplets (³Chls) are formed, which can sensitize singlet oxygen, a species harmful to the photosynthetic apparatus of plants. Plants have developed multiple photoprotective mechanisms to quench ³Chl and scavenge singlet oxygen in order to sustain the photosynthetic activities. The lumenal loop of light-harvesting chlorophyll a/b complex of photosystem II (LHCII) plays important roles in regulating the pigment conformation and energy dissipation. In this study, site-directed mutagenesis analysis was applied to investigate triplet–triplet energy transfer and quenching of ³Chl in LHCII. We mutated the amino acid at site 123 located in this region to Gly, Pro, Gln, Thr and Tyr, respectively, and recorded fluorescence excitation spectra, triplet-minus-singlet (TmS) spectra and kinetics of carotenoid triplet decay for wild type and all the mutants. A red-shift was evident in the TmS spectra of the mutants S123T and S123P, and all of the mutants except S123Y showed a decrease in the triplet energy transfer efficiency. We propose, on the basis of the available structural information, that these phenomena are related to the involvement, due to conformational changes in the lumenal region, of a long-wavelength lutein (Lut2) involved in quenching ³Chl.     

Fluorescence induction in the phycobilisome-containing cyanobacterium Synechococcus sp PCC 7942: analysis of the slow fluorescence transient

At room temperature, the chlorophyll (Chl) a fluorescence induction (FI) kinetics of plants, algae and cyanobacteria go through two maxima, P at approximately 0.2-1 and M at approximately 100-500 s, with a minimum S at approximately 2-10 s in between. Thus, the whole FI kinetic pattern comprises a fast OPS transient (with O denoting origin) and a slower SMT transient (with T denoting terminal state). Here, we examined the phenomenology and the etiology of the SMT transient of the phycobilisome (PBS)-containing cyanobacterium Synechococcus sp PCC 7942 by modifying PBS-->Photosystem (PS) II excitation transfer indirectly, either by blocking or by maximizing the PBS-->PS I excitation transfer. Blocking the PBS-->PS I excitation transfer route with N-ethyl-maleimide [NEM; A. N. Glazer, Y. Gindt, C. F. Chan, and K.Sauer, Photosynth. Research 40 (1994) 167-173] increases both the PBS excitation share of PS II and Chl a fluorescence. Maximizing it, on the other hand, by suspending cyanobacterial cells in hyper-osmotic media [G. C. Papageorgiou, A. Alygizaki-Zorba, Biochim. Biophys. Acta 1335 (1997) 1-4] diminishes both the PBS excitation share of PS II and Chl a fluorescence. Here, we show for the first time that, in either case, the slow SMT transient of FI disappears and is replaced by continuous P-->T fluorescence decay, reminiscent of the typical P-->T fluorescence decay of higher plants and algae. A similar P-->T decay was also displayed by DCMU-treated Synechococcus cells at 2 degrees C. To interpret this phenomenology, we assume that after dark adaptation cyanobacteria exist in a low fluorescence state (state 2) and transit to a high fluorescence state (state 1) when, upon light acclimation, PS I is forced to run faster than PS II. In these organisms, a state 2-->1 fluorescence increase plus electron transport-dependent dequenching processes dominate the SM rise and maximal fluorescence output is at M which lies above the P maximum of the fast FI transient. In contrast, dark-adapted plants and algae exist in state 1 and upon illumination they display an extended P-->T decay that sometimes is interrupted by a shallow SMT transient, with M below P. This decay is dominated by a state 1-->2 fluorescence lowering, as well as by electron transport-dependent quenching processes. When the regulation of the PBS-->PS I electronic excitation transfer is eliminated (as for example in hyper-osmotic suspensions, after NEM treatment and at low temperature), the FI pattern of Synechococcus becomes plant-like.     

Differential efficiency of photosynthetic oxygen evolution in flashing light in triazine-resistant and triazine-susceptible biotypes of Senecio vulgaris L.

Photosynthetic oxygen evolution in response to flashing light was studied in triazine-susceptible and triazine-resistant biotypes of Senecio vulgaris L. Studies were conducted to determine if the modification of the herbicide-binding site which confers s-triazine resistance also affects the oxygen-evolving system. Oxygen evolution was measured using a Joliot-type oxygen-specific electrode on broken, stroma-free chloroplasts of both biotypes. We observed abnormal patterns of oxygen evolution in resistant chloroplasts. The S′₁ → S₂ transition is slower while the S₂ decay is faster. The S′₂ → S₃ transition, in contrast, is slightly faster in resistant chloroplasts, while the decay of the S₃ state is the same as in susceptible chloroplasts. These altered kinetics may be due to altered Q → B (B^?) electron flow in resistant chloroplasts. These results are also consistent with the hypothesis that back-reactions from the reducing (acceptor) side of Photosystem II to the oxidizing (donor) side occur with greater frequency in resistant than susceptible chloroplasts. These events are responsible for lower oxygen yield and increased ‘misses’ and ‘double hits,’ resulting in abnormal yield patterns and lower quantum yield of CO₂ fixation in resistant chloroplasts compared to the susceptible ones.     

Investigations on the electron transfer processes in Photosystem II: New insights by chlorophyll fluorescence decay measurements with additional saturating light pulses

Electron transfer processes in leaves were investigated by chlorophyll fluorescence decay measurements. A fast chlorophyll fluorescence decay was observed in the intact state, reflecting normal electron transfer in Photosystem II. After treatment with DCMU a slow chlorophyll fluorescence decay was measured due to blocked electron transfer after the primary quinone Q_A. Additional saturating light pulses, one between each two measuring pulses, were used to completely reduce Q_A of the intact leaf: the chlorophyll fluorescence decay became similar to that of a DCMU treated leaf. A decreased electron donation rate to the reaction centre P680 was obtained after treatment with hydroxylamine. The intensity of the additional saturating light pulses was not sufficient to reduce all Q_A under this condition and only a small increase of the average chlorophyll fluorescence decay time occurred. Following our previous paper [Berg et al. (1997) Photosynthetica 34, in press], we investigated the effects of water stress with the additional saturating light pulses. An almost complete reduction of Q_A was possible after water stress started. A small, but systematic shortening of the slow chlorophyll fluorescence decay followed, up to a relative loss of leaf mass of 80%. At this time a rapid shortening of the chlorophyll fluorescence decay occurred, caused by an electron deficiency at the donor site of PS II. Additional saturating light pulses had no effects on the chlorophyll fluorescence decay any more, revealing a radiationless recombination between the reduced primary quinone Q and the oxidized reaction centre P680⁺.     

Modulation of the fluorescence yield in heliobacterial cells by induction of charge recombination in the photosynthetic reaction center

Heliobacteria contain a very simple photosynthetic apparatus, consisting of a homodimeric type I reaction center (RC) without a peripheral antenna system and using the unique pigment bacteriochlorophyll (BChl) g. They are thought to use a light-driven cyclic electron transport pathway to pump protons, and thereby phosphorylate ADP, although some of the details of this cycle are yet to be worked out. We previously reported that the fluorescence emission from the heliobacterial RC in vivo was increased by exposure to actinic light, although this variable fluorescence phenomenon exhibited very different characteristics to that in oxygenic phototrophs (Collins et al. 2010). Here, we describe the underlying mechanism behind the variable fluorescence in heliobacterial cells. We find that the ability to stably photobleach P₈₀₀, the primary donor of the RC, using brief flashes is inversely correlated to the variable fluorescence. Using pump-probe spectroscopy in the nanosecond timescale, we found that illumination of cells with bright light for a few seconds put them in a state in which a significant fraction of the RCs underwent charge recombination from P₈₀₀ ⁺A₀ ^? with a time constant of ~20 ns. The fraction of RCs in the rapidly back-reacting state correlated very well with the variable fluorescence, indicating that nearly all of the increase in fluorescence could be explained by charge recombination of P₈₀₀ ⁺A₀ ^?, some of which regenerated the singlet excited state. This hypothesis was tested directly by time-resolved fluorescence studies in the ps and ns timescales. The major decay component in whole cells had a 20-ps decay time, representing trapping by the RC. Treatment of cells with dithionite resulted in the appearance of a ~18-ns decay component, which accounted for ~0.6 % of the decay, but was almost undetectable in the untreated cells. We conclude that strong illumination of heliobacterial cells can result in saturation of the electron acceptor pool, leading to reduction of the acceptor side of the RC and the creation of a back-reacting RC state that gives rise to delayed fluorescence.     

Sensitive Detection of Phosphorus Deficiency in Plants Using Chlorophyll a Fluorescence

Phosphorus (P) is a finite natural resource and an essential plant macronutrient with major impact on crop productivity and global food security. Here, we demonstrate that time-resolved chlorophyll a fluorescence is a unique tool to monitor bioactive P in plants and can be used to detect latent P deficiency. When plants suffer from P deficiency, the shape of the time-dependent fluorescence transients is altered distinctively, as the so-called I step gradually straightens and eventually disappears. This effect is shown to be fully reversible, as P resupply leads to a rapid restoration of the I step. The fading I step suggests that the electron transport at photosystem I (PSI) is affected in P-deficient plants. This is corroborated by the observation that differences at the I step in chlorophyll a fluorescence transients from healthy and P-deficient plants can be completely eliminated through prior reduction of PSI by far-red illumination. Moreover, it is observed that the barley (Hordeum vulgare) mutant Viridis-zb⁶³, which is devoid of PSI activity, similarly does not display the I step. Among the essential plant nutrients, the effect of P deficiency is shown to be specific and sufficiently sensitive to enable rapid in situ determination of latent P deficiency across different plant species, thereby providing a unique tool for timely remediation of P deficiency in agriculture.The world population is estimated to exceed 9 billion people by 2050. This means that agriculture on a global scale has to increase food production by 70% to 100%, and, at the same time, handle the consequences of global climate changes and reduce its environmental footprint (Food and Agriculture Organization of the United Nations, 2009; Godfray et al., 2010; Foley et al., 2011). A major challenge related to this is the supply and use of phosphorus (P) to support future plant production (Cordell et al., 2009; Gilbert, 2009; MacDonald et al., 2011).P is an essential plant nutrient, which means that plants require P in adequate amounts to fulfill a complete lifecycle. It has been estimated that 30% of the world’s agricultural soils are P deficient and need fertilizer addition to ensure yield and quality (MacDonald et al., 2011). However, phosphate rock, the main source of P fertilizers, is a finite natural resource, and the known rock phosphate reserves are estimated to last as little as 50 years in the gloomiest forecasts (Gilbert, 2009; Edixhoven et al., 2013). This makes P a potential strategic natural resource similar to oil, as very few countries control the vast majority of the known reserves (Gilbert, 2009; Elser and Bennett, 2011; Edixhoven et al., 2013). Presently, an immense overuse of P is found in some parts of the world, causing eutrophication of lakes and seas, while P depletion results in severe yield limitations elsewhere (MacDonald et al., 2011; Obersteiner et al., 2013). An essential aspect of solving both of these problems is to increase P use efficiency in agriculture, thus reducing the negative environmental impact of agriculture and helping to ensure a sustainable use of P resources while increasing the worldwide food production (Schröder et al., 2011; Veneklaas et al., 2012).Here, we present a unique analytical principle based on chlorophyll a fluorescence that allows rapid, nondestructive, onsite assessment of plant P status by recording the so-called OJIP transient of a dark-adapted leaf.When a chlorophyll molecule absorbs light, one of three events will occur: The light may be used to drive photosynthesis, it can be dissipated as heat, or it can be reemitted as fluorescence. Less than 10% of light absorbed by the plant causes emission of chlorophyll a fluorescence (Govindjee, 2004; Stirbet and Govindjee, 2011). When a dark-adapted leaf is exposed to saturating actinic light, the resulting time-dependent fluorescence forms a so-called Kautsky curve (Kautsky and Hirsch, 1931; McAlister and Myers, 1940). Within 300 ms, the fluorescence increases from a minimum level (F₀) to the maximum level. If measured with a sufficiently high time resolution, a polyphasic transient with four distinct steps, designated as O, J, I, and P, is observed. After reaching maximum intensity at the P step, the fluorescence intensity declines until it reaches a steady state within a few minutes (Harbinson and Rosenqvist, 2003; Govindjee, 2004).The physiological mechanisms underlying the polyphasic OJIP transient are still not clarified, but it is believed that the J and I steps represent dynamic bottlenecks in the photosynthetic electron transport chain. The first rise (2 ms) from O to J is referred to as the photochemical phase due to its dependence on the intensity of the incoming light. This phase is assumed to reflect the reduction of the primary quinone electron acceptor in PSII (Stirbet and Govindjee, 2011). The reduction of the primary quinone electron acceptor results in a decreased electron trapping efficiency and therefore an increase in the dissipation of absorbed light energy by fluorescence and heat. The second part, from J over I to P, is called the thermal phase due to its temperature sensitivity. This phase is much slower than the first, and it is believed that the J-I phase primarily reflects a sequential reduction of the remaining plastoquinone pool of PSII and that the I-P phase reflects the subsequent electron flow through cytochrome b₆f to electron sinks at the PSI acceptor side (Stirbet and Govindjee, 2011). Thus, the OJIP transient resembles a titration of the photochemical quantum yield and reflects the complex electron transport properties of PSII and PSI.Consistent with their known influence on photosynthesis, deficiencies of essential plant nutrients such as Fe, Cu, Mg, Mn, and S have previously been shown to affect OJIP transients (Kastori et al., 2000; Mallick and Mohn, 2003; Larbi et al., 2004; Husted et al., 2009; Tang et al., 2012; Yang et al., 2012). As a consequence, several attempts have been made to identify nutrient imbalances and disorders using one or several parameters derived from the transients, but apart from Mn (Husted et al., 2009; Schmidt et al., 2013), attempts have not been successful in terms of sensitivity and specificity. This includes P, which previously has been reported to have an effect on OJIP transients, yet the reported effects seem mutually contradictory and nonspecific to P (Ripley et al., 2004; Weng et al., 2008; Jiang et al., 2009; Lin et al., 2009).Here, we present the unique finding that increasing levels of P deficiency affect the shape of the OJIP transient around the I step at 20 to 50 ms and causes the I step to gradually straighten and disappear. It is demonstrated that this effect is fully reversible and, among the essential plant nutrients, specific for P deficiency using both monocotyledons (barley [Hordeum vulgare]) and dicotyledons (tomato [Solanum lycopersicum]) plant species. Furthermore, it is shown that it is possible to determine whether a plant is P sufficient or deficient and to quantitatively predict the P concentration in leaf tissue using multivariate analysis of the OJIP transients.     

Blue light-modulation of chlorophyll a fluorescence transients in guard cell chloroplasts

Chlorophyll a fluorescence transients from mesophyll and single guard cell pairs of Vicia faba were measured by microspectrofluorometry. In both chloroplast types, fluorescence induction (O to P) was similar under actinic blue and green light. In slow transients from mesophyll cell chloroplasts, blue and green light induced identical, typical rapid quenching from P to S, and the M peak. In contrast, the P to S transient from guard cell (GC) chloroplasts irradiated with blue light showed a much slower quenching rate, and the P to T transition showed no M peak. Actinic green light induced mesophyll-like transients in GC chloroplasts, including rapid quenching from P to S and the M peak. Detection of these transients in single pairs of GC and isolated protoplasts ruled out mesophyll contamination as a signal source. Green light induced a rapid quenching and the M peak in GC chloroplasts from several species. The effect of CO₂ concentration on the fluorescence transients was investigated in the presence of HCO₃⁻ at pH 6.8 and 10.0. In transients induced by green light in both chloroplast types, a pH increase concomitant with a reduction in CO₂ concentration caused an increase in the initial rate of quenching and the elimination of the M peak. Actinic blue light induced mesophyll-like transients from GC chloroplasts in the presence of 10 micromolar KCN, a concentration at which the blue light-induced stomatal opening is inhibited. Addition of 100 to 200 micromolar phosphate also caused large increases in fluorescence quenching rates and a M peak. These results indicate that blue light modulates photosynthetic activity in GC chloroplasts. This blue light effect is not observed in the absence of transduction events connected with the blue light response and in the presence of high phosphate concentrations.     

A one microsecond component of chlorophyll luminescence suggesting a primary acceptor of system II of photosynthesis different from Q

The kinetics of the luminescence of chlorophyll a in Chlorella vulgaris were studied in the time range from 0.2 μs to 20 μs after a short saturating flash ($\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 25}\text{ns}$) under various pretreatment including anaerobiosis, flashes, continuous illumination and various additions. A 1 μs luminescence component probably originating from System II was found of which the relative amplitude was maximum under anaerobic conditions for reaction centers in the state SPQ^? before the flash, about one third for centers in the state S⁺PQ^? or SPQ before the flash, and about one tenth for centers in the state S⁺PQ before the flash. S is the secondary donor complex with zero charge; S⁺ is the secondary donor complex with 1 to 3 positive charges; P, the primary donor, is the photoactive chlorophyll a, P-680, of reaction center 2; Q^? is the reduced acceptor of System II, Q. Under aerobic conditions, where an endogenous quencher presumably was active, the luminescence was reduced by a factor two.The 1 μs decay of the luminescence is probably caused by the disappearance of P⁺ formed in the laser flash according to the reaction ZP⁺ → Z⁺P in which Z is the molecule which donates an electron to P⁺ and which is part of S. After addition of hydroxylamine, the 1 μs luminescence component changed with the incubation time exponentially (τ = 27 s) into a 30 μs component; during the same time, the variable fluorescence yield, measured 9 μs after the laser flash, decreased by a factor 2 with the same time constant. Hereafter in a second much slower phase the fluorescence yield decreased as an exponential function of the incubation time to about the dark value; meanwhile the 30 μs luminescence increased about 50% with the same time constant (τ = 7 min). Heat treatment abolished both luminescence components.The 1 μs luminescence component saturated at about the same energy as the System II fluorescence yield 60 μs after the laser flash and as the slower luminescence components. From the observation that the amplitude is maximum if the laser flash is given when the fluorescence yield is high after prolonged anaerobic conditions (state SQ^?), we conclude that the 1 μs luminescence is probably caused by the reaction

$\text{PWQ}{}^{\mathrm{?}}\text{+hv →}\text{P}\text{1}\text{WQ}{}^{\mathrm{?}}\text{→}\text{P}{}^{\mathrm{+}}\text{W}{}^{\mathrm{?}}\text{Q}{}^{\mathrm{?}}\text{→}\text{P}\text{1}\text{WQ}{}^{\mathrm{?}}\text{→ PWQ}{}^{\mathrm{?}}\text{+hv}$

in which W is an acceptor different from Q. The presence of S⁺ reduced the luminescence amplitude to about one third. Two models are discussed, one with W as an intermediate between P and Q and another, which gives the best interpretation, with W on a side path.     

Cellular Compartmentation of Zinc in Leaves of the Hyperaccumulator Thlaspi caerulescens

Cellular compartmentation of Zn in the leaves of the hyperaccumulator Thlaspi caerulescens was investigated using energy-dispersive x-ray microanalysis and single-cell sap extraction. Energy-dispersive x-ray microanalysis of frozen, hydrated leaf tissues showed greatly enhanced Zn accumulation in the epidermis compared with the mesophyll cells. The relative Zn concentration in the epidermal cells correlated linearly with cell length in both young and mature leaves, suggesting that vacuolation of epidermal cells may promote the preferential Zn accumulation. The results from single-cell sap sampling showed that the Zn concentrations in the epidermal vacuolar sap were 5 to 6.5 times higher than those in the mesophyll sap and reached an average of 385 mm in plants with 20,000 μg Zn g⁻¹ dry weight of shoots. Even when the growth medium contained no elevated Zn, preferential Zn accumulation in the epidermal vacuoles was still evident. The concentrations of K, Cl, P, and Ca in the epidermal sap generally decreased with increasing Zn. There was no evidence of association of Zn with either P or S. The present study demonstrates that Zn is sequestered in a soluble form predominantly in the epidermal vacuoles in T. caerulescens leaves and that mesophyll cells are able to tolerate up to at least 60 mm Zn in their sap.Different mechanisms have been proposed to explain the tolerance of plants to toxic heavy metals (Baker and Walker, 1990; Verkleij and Schat, 1990). Some tolerant plant species, the so-called “excluders,” use exclusion mechanisms by which uptake and/or root-to-shoot transport of heavy metals are restricted. Other tolerant plant species are able to cope with elevated concentrations of toxic metals inside of their tissues through production of metal-binding compounds, cellular and subcellular compartmentation, or alterations of metabolism.An extreme strategy for metal tolerance that is in sharp contrast to metal exclusion is “hyperaccumulation,” a term that was originally used by Brooks et al. (1977) to describe plants that can accumulate more than 1,000 μg Ni g⁻¹ dry weight in their aerial parts. Approximately 400 taxa of terrestrial plants have been identified as hyperaccumulators of various heavy metals, with about 300 being Ni hyperaccumulators (Baker and Brooks 1989; Brooks, 1998). Only 16 species of Zn hyperaccumulators, which are defined as being able to accumulate more than 10,000 μg Zn g⁻¹ in the aboveground parts on a dry weight basis in their natural habitat (Brooks, 1998), have been reported. Thlaspi caerulescens J. & C. Presl (Brassicaceae) is the best-known example of a Zn/Cd hyperaccumulator. Under hydroponic culture conditions T. caerulescens can accumulate up to 25,000 to 30,000 μg Zn g⁻¹ dry weight in the shoots without showing any toxicity symptoms or reduction in growth (Brown et al., 1996a; Shen et al., 1997). Recently, there has been a surge of interest in the phenomenon of heavy-metal hyperaccumulation because this property may be exploited in the remediation of heavy-metal-polluted soils through phytoextraction and phytomining (McGrath et al., 1993; Brown et al., 1995b; Robinson et al., 1997).The mechanisms for metal hyperaccumulation are not fully understood, and this is particularly true in the case of the Zn/Cd hyperaccumulators. To cope with the consequence of hyperaccumulation, plants must also be hypertolerant to the heavy metals that accumulate. Recent studies comparing the different populations of T. caerulescens have shown that hyperaccumulation of Zn is a constitutive property, although the traits are probably separate from those for tolerance (Baker et al., 1994; Meerts and Van Isacker, 1997). Compared with the nonaccumulating species, T. caerulescens possesses an enhanced capacity to take up Zn and transport it from roots to shoots (Baker et al., 1994; Brown et al., 1995a; Shen et al., 1997). Lasat et al. (1996) found that roots of T. caerulescens and the nonaccumulator Thlaspi arvense had similar apparent K_m values for Zn²⁺, but that the V_max in the former was 4.5-fold higher than that in the latter species, indicating that the hyperaccumulator T. caerulescens possessed more Zn²⁺-transport sites in the plasma membranes of root cells. Shen et al. (1997) showed that T. caerulescens was much more effective in exporting the Zn that was accumulated previously in roots to the shoots than an intermediate accumulator species, Thlaspi ochrolucum. Organic acids such as malic acid have been suggested to play a key role in shuttling Zn from cytoplasm to vacuoles (Mathys, 1977). However, the low affinity of malate to chelate Zn (stability constant pK = 3.5 at infinite dilution) does not favor this hypothesis. Moreover, high concentrations of malate found in the shoot tissues of T. caerulescens appear to be a constitutive property (Tolrà et al., 1996; Shen et al., 1997).The extraordinary tolerance of hyperaccumulator plants must also involve compartmentation of toxic metals at the cellular and subcellular levels. Vázquez et al. (1992, 1994) studied localization of Zn in the root and leaf tissues of T. caerulescens using EDXMA. They compared two methods of sample preparation and found that Na₂S fixation was not suitable for preventing the loss of metal ions from the samples. Using cryofixation and freeze substitution, they showed that Zn accumulated mainly in the vacuoles as electron-dense deposits. Many vacuoles of leaf-epidermal and subepidermal cells contained globular crystals that were very rich in Zn. However, it is not known whether the Zn-rich, globular crystal deposits occur inside of the leaf vacuoles in vivo or if they are artifacts caused by sample preparation. Also, the technique used by Vázquez et al. (1992, 1994) allows only semiquantitative determination of Zn concentrations.In this study we used two techniques to investigate cellular compartmentation of Zn in the leaves of T. caerulescens. The first utilized EDXMA of frozen, hydrated tissue to survey the distribution patterns of Zn and other elements across different leaf cells. The second method involved sampling sap from single cells using microcapillaries, followed by fully quantitative determination of Zn and other elements using EDXMA.     

Oligosaccharides on cathepsin D from porcine spleen

Cathepsin D from porcine spleen contained mannose (3.3%), glucosamine (1.4%), and mannose 6-phosphate (0.08%). Essentially all of the oligosaccharides of cathepsin D could be released by endo-β-N-acetylglucosaminidase H, pointing to oligomajmoside types of structures. Three neutral oligosaccharide fractions, containing 5, 6, and 7 mannose residues, respectively, were isolated by gel permeation chromatography on Bio-Gel P-2. Studies using exoglycosidase digestions and 500-MHz ¹H NMR spectroscopy revealed that their structures are [Manα1 → 2]_{0 or 1}Manα1 → 6[Manα1 → 3]Manα1 → 6[(Manα1 → 2)_{0 or 1}Manα1 → 3]Manβ1 → 4GlcNAcβ1 → 4 GlcNAc. These structures are identical to what have recently been proposed by Takahashi et al. for the major oligosaccharide units of cathepsin D from the same source (T. Takahashi P.G. Schimidt, and J. Tang (1983)J. Biol. Chem.258, 2819–2930), except for the occurrence of two isomeric oligosaccharides containing six mannoses. Only a part (3.4%) of the oligosaccharides were acidic, containing phosphates in monoester linkage. The phosphorylated oligosaccharides also consisted of oligomannoside-type chains which were analogous to, but more heterogeneous in size than the neutral oligosaccharides. Cathepsin D was bound to a mannose- and N-acetylglucosamine-specific lectin (mannan-binding protein) isolated from rabbit liver with the K_i value of 5.4 × 10^?6m.