Kinetic imaging of chlorophyll fluorescence using modulated light

Fluorometers that measure the kinetics of chlorophyll fluorescence have become invaluable tools for determining the photosynthetic performance of plants. Many of these instruments use high frequency modulated light to measure the rate, efficiency and regulation of photosynthesis. The technique is non-invasive and is effective under diverse environmental conditions. Recently, imaging fluorometers have been introduced that reveal variability in photosynthesis over the surface of a leaf or between individual plants. Most imaging instruments depend on continuous light or low frequency modulated light for fluorescence excitation, which imposes serious limitations on measurements of the fluorescence parameters, especially the minimum fluorescence (F₀) and variable fluorescence (F_V). Here, we describe a new instrument that combines the advantage of high frequency modulated light with two-dimensional imaging of chlorophyll fluorescence. The fluorometer produces dynamic images of chlorophyll fluorescence from leaves or plants, providing accurate mapping of F₀ and F_V, and non-photochemical quenching. A significant feature of the instrument is that it can record fluorescence images of leaves in daylight under field conditions. This revised version was published online in June 2006 with corrections to the Cover Date.     

Fluorescence clamp: A direct measure of fluxes into and out of the antenna pool of Photosystem II

Fluorescence clamp (FC) is a method of directly measuring the fluxes out of Photosystem II antenna. This is achieved by a feed-back loop which controls the light intensity of light emitting diodes in order to keep the amplitude of modulated chlorophyll fluorescence constant, and by taking the intensity or the current fed into the light emitting diodes as a measure of the fluxes. Saturating flashes serve to distinguish between fluxes into thermal deactivation and into the photosynthetic electron transfer chain (ETC). As FC is only active in the light period of the measuring light, the background signal (induced by actinic light) is compensated by a second feed-back loop in the dark period of the measuring light. Equations are provided for the interpretation of the FC signals. This includes the quenching parameters of chlorophyll fluorescence, the flux into the electron transfer chain and the redox state of Q_A. Experiments are presented which show that traditional fluorescence (LC) and FC measurements yield the same results. However, the FC method provides a better presentation of fluxes as the scaling factor (flux/signal) is constant for all states of Photosystem II. This leads to a simpler analysis of quenching mechanisms. Examples are given which show that the co-existing quenching mechanisms with different effects on photochemical and non-photochemical fluxes can be better identified by FC rather than by LC. This revised version was published online in June 2006 with corrections to the Cover Date.     

Modulated polarization microscopy: a promising new approach to visualizing cytoskeletal dynamics in living cells

In an effort to visualize cytoskeletal filaments in living cells, we have developed modulated polarization microscopy. Modulated polarization microscopy visualizes cytoskeletal filaments based on their birefringence but differs from the standard polarization microscopy by exploiting the angle dependence of birefringence. A prototype instrument has been developed using two Faraday rotators under computer control to change the angle of plane polarized light at a known rate. By placing one Faraday rotator before and one after the specimen, rotation produced by the first Faraday rotator is cancelled by the second. This allows the use of fixed polarizer and analyzer in a crossed configuration and continuous imaging of the specimen between crossed polarizers. The variation in polarization angle of light illuminating the specimen causes birefringent elements to oscillate in brightness. Images acquired as polarization angle is varied are then processed by a Fourier filter image-processing algorithm. The Fourier filtering algorithm isolates those signals that vary at the proper rate, whereas static or random signals are removed. Here we show that the modulated polarization microscope can reveal cytoskeletal elements including stress fibers and microtubules in living cells.     

Distribution of light excitation in an intact leaf between the two photosystems of photosynthesis. Changes in absorption cross-sections following state 1-state 2 transitions

Using the photoacoustic technique, state 1-state 2 transitions were studied in an intact leaf by direct monitoring of modulated oxygen evolution, excited by modulated light. States 1 and 2 were characterized by the extent of immediate enhancement of the modulated oxygen evolution — ‘Emerson enhancement’ — and the concomitant fluorescence quenching, resulting from the addition of continuous far-red light (greater than 700 nm), absorbed primarily in Photosystem I (light 1). The extent of Emerson enhancement as well as the saturation curve of this effect by far-red light are very sensitive and quantitative indicators for the ratio of light excitation distributed between Photosystems I and II. The enhancement ratios at 650 nm light, a typical light 2, were in a range 1.4–1.8 in state 1, while values as low as 1.06 were observed in state 2. During the transition from state 2 to state 1, monitored in presence of modulated light 2 and background continuous light 1, the modulated oxygen yield increased considerably, indicating a major increase in excitation flux into Photosystem II. Conversely, with modulated light 2 alone in state 1, the modulated oxygen evolution yield was smaller than in state 2, indicating a decrease of the excitation flux in Photosystem I. In a typical example, of the transition to state 1, the fraction of light absorbed by Photosystem II, β, increased from 0.46 to 0.64, while that absorbed by Photosystem II, α, decreased from 0.43 to 0.36. State 1-state 2 transitions, thus, reflect reciprocal changes in the cross-sections of the two photosystems for light absorption. There is no evidence for the operation of a ‘spill-over’ mechanism. The enhancement effect displayed maxima at 480 and 650 nm, related to chlorophyll-b absorption, as well as another band at 500–550 nm. In a chlorophyll-b-less barley mutant, state 1-state 2 transitions, as monitored by modulated oxygen evolution, were absent, and the resulting enhancement corresponded to state 2. These observations are consistent with the model that the light-harvesting $\text{chlorophyll}\text{-}\text{a}\text{b}$ complex plays a role in regulating the distribution of light to the photosystems. It is probable that this complex migrates reversibly in the thylakoid membrane in such a way that it is mainly associated with Photosystem II in state 1, but is more evenly distributed in the two photosystems in state 2.     

Rapid chlorophyll a fluorescence transient of Lemna gibba leaf as an indication of light and hydroxylamine effect on photosystem II activity.

Rapid chlorophyll fluorescence transient induced by saturating flash (3000 micromol of photons m-2 s-1) was investigated when Lemna gibba had been exposed to light (100 micromol of photons m-2 s-1) causing the Kautsky effect or in low light intensity unable to trigger PSII photochemistry. Measurements were made by using, simultaneously, a pulse amplitude modulated fluorometer and plant efficiency analyzer system, either on non-treated L. gibba leaf or those treated with different concentrations of hydroxylamine (1-50 mM) causing gradual inhibition of the water splitting system. When any leaf was exposed to continuous light during the Kautsky effect, a rapid fluorescence transient may reflect current activity of photosystem II within the photosystem II complex. Under those conditions, a variation of transition steps appearing over time was related to a drastic change to the photosystem II functional properties. This value indicated that the energy dissipation through non-photochemical pathways was undergoing extreme change. The change of rapid fluorescence transient, induced under continuous light, when compared to those obtained under very low light intensity, confirmed the ability of photosystem II to be capable to undergo rapid adaptation lasting about two minutes. When the water splitting system was inhibited and electron donation partially substituted by hydroxylamine, the adaptation ability of photosystem II to different light conditions was lost. In this study, the change of rapid fluorescence kinetic and transient appearing over time was shown to be a good indication for the change of the functional properties of photosystem II induced either by light or by hydroxylamine.     

On the advantages of using green light to study fluorescence yield changes in leaves

In photosynthetic chains, the kinetics of fluorescence yield depends on the photochemical rates at the level of both Photosystem I and II and thus on the absorption cross section of the photosynthetic units as well as on the coupling between light harvesting complexes and photosynthetic traps. A new set-up is described which, at variance with the commonly used set-ups, uses of a weakly absorbed light source (light-emitting diodes with maximum output at 520 nm) to excite the photosynthetic electron chain and probe the resulting fluorescence yield changes and their time course. This approach optimizes the homogeneity of the exciting light throughout the leaf and we show that this homogeneity narrows the distribution of the photochemical rates. Although the exciting light is weakly absorbed, the possibility to tune the intensity of the light emitting diodes allows one to reach photochemical rates ranging from 10(4) s(-1) to 0.25 s(-1) rendering experimentally accessible different functional regimes. The variations of the fluorescence yield induced by the photosynthetic activity are qualitatively and quantitatively discussed. When illuminating dark-adapted leaves by a weak light, the kinetics of fluorescence changes displays a pronounced plateau which precedes the fluorescence increase reflecting the full reduction of the plastoquinone pool. We ascribe this plateau to the time delay needed to reduce the photosystem I electron acceptors.     

The 1-Hz fluorometer: A new approach to fast and sensitive long-term studies of active chlorophyll and environmental influences

A new instrument for environmental monitoring, called at 1-Hz fluorometer, provides two modes of application. First, it enables a quantitative determination of algal concentrations down to 20 ng/l. Second, it can be used as a biosensor for changes in environmental conditions. The distinction between the signals from living chlorophyll-containing algae and other fluorescent material is achieved by using two modulated light-sources resulting in a mean fluence rate of 200 μE. The measuring light induces changes in chlorophyll fluorescence (yield) with a frequency of 1 kHz, and the actinic light modulates the redox state of the quenchers of PS II with a frequency of 1 Hz. This leads to a modulation of the yield which is detected by two phase-sensitive rectifiers (double correlation). Measurements from different sites in a river, and in the Baltic and North Seas, show that correction by the built-in simultaneously-measured attenuation is necessary in order to obtain values which are identical with those determined by a photometric analysis (Uvikon 860). This applies if the transmission becomes less than about 95%. Suspensions ofDunaliella salina exposed to ammonia and phosphate were used for illustrating the usage for environmental monitoring. It is shown that this system can measure changes in the chlorophyll fluorescence of living algae caused by changes in concentration of ammonia down to 1 μg/l and of phosphate down to 10 μg/l.     

An integrated portable apparatus for the simultaneous field measurement of photosynthetic CO2 and water vapour exchange, light absorption and chlorophyll fluorescence emission of attached leaves

Abstract. A portable apparatus has been constructed to measure simultaneously the quantum yield of CO₂ assimilation, light absorption, chlorophyll fluorescence emission and water vapour exchange of attached intact leaves in the field. The core of the instrument is a light-integrating spherical leaf chamber which includes ports for a light source, photosynthetically active radiation sensor, fluorescence probes and gas inlet and outlet manifolds. Measurement of the quantum flux inside the empty chamber and with a leaf present allows determination of leaf absorptance. An open gas exchange system is employed using an infra-red analyser to measure leaf CO₂ exchange. Using a DC white light source the quantum yield of CO₂ assimilation based on absorbed light (φ_abs) may be determined rapidly in either ambient air or artificial gas mixtures. Inclusion of capacitance humidity probes into the gas inlet and outlet ports allows simultaneous determination of water vapour exchange and subsequent estimation of stomatal conductance to CO₂ and intercellular CO₂ concentration. Measurement of fluorescence emission by the sample leaf exposed to white light is achieved by a modulated fluorescence detection system. In addition to determination of the minimal, maximal and variable fluorescence levels, a further analysis allows the photochemical and non-photochemical components of fluorescence quenching, to be estimated. The theory and design of this apparatus is described in detail. The use of the apparatus in the field is demonstrated through a study of the photosynthetic performance of a maize and bean crop during the growing season and by analysis of the photosynthetic performance of crops subjected to nitrogen-stress and a herbicide treatment.     

Effects of light quality on the circadian rhythm of leaf movement of a short-day-plant

Studies were made of the effects of blue, green, red and far-red (FR) light on the circadian rhythm of leaf movement of Coleus blumei × C. frederici, a short day plant. Under continuous illumination with blue light, there was a significant lengthening of the period of the rhythm to about 24.0 hr, as compared to 22.5 hr in continuous darkness. Under continuous red light, the period length was significantly shortened to 20.5 hr. Under continuous green or FR, the period length was not significantly different from the dark control. It was observed that under continuous FR illumination, the leaves tended to oscillate in a more downward position. Eight-hr red light signals were effective in advancing the phase of the rhythm as compared to a control under continuous green light. Blue light signals were effective in delaying the phase of the rhythm. FR light signals were ineffective in producing either delay or advance phase shifts. Far-red light did not reverse the effects of either red or blue light signals. On the basis of these results it is suggested, that pigments which absorb blue or red light, rather than phytochrome, mediate the effect of light on the circadian rhythm of leaf movement.     

On the advantages of using green light to study fluorescence yield changes in leaves

In photosynthetic chains, the kinetics of fluorescence yield depends on the photochemical rates at the level of both Photosystem I and II and thus on the absorption cross section of the photosynthetic units as well as on the coupling between light harvesting complexes and photosynthetic traps. A new set-up is described which, at variance with the commonly used set-ups, uses of a weakly absorbed light source (light-emitting diodes with maximum output at 520 nm) to excite the photosynthetic electron chain and probe the resulting fluorescence yield changes and their time course. This approach optimizes the homogeneity of the exciting light throughout the leaf and we show that this homogeneity narrows the distribution of the photochemical rates. Although the exciting light is weakly absorbed, the possibility to tune the intensity of the light emitting diodes allows one to reach photochemical rates ranging from 10⁴ s^− 1 to 0.25 s^− 1 rendering experimentally accessible different functional regimes. The variations of the fluorescence yield induced by the photosynthetic activity are qualitatively and quantitatively discussed. When illuminating dark-adapted leaves by a weak light, the kinetics of fluorescence changes displays a pronounced plateau which precedes the fluorescence increase reflecting the full reduction of the plastoquinone pool. We ascribe this plateau to the time delay needed to reduce the photosystem I electron acceptors.     

Thylakoid protein phosphorylation during State 1—State 2 transitions in osmotically shocked pea chloroplasts

In osmotically shocked pea chloroplasts illuminated with modulated blue-green light (light 2), phosphorylation of the light-harvesting chlorophyll $\text{a}\text{b-}\text{protein}$ complex (LHCP) accompanies the slow decrease in modulated fluorescence that indicates adaptation to light absorbed predominantly by Photosystem II (State 2). On subsequent additional illumination with continuous far-red light (absorbed predominantly by Photosystem I; light 1) both effects are reversed: modulated chlorophyll fluorescence emission increases (indicating adaptation towards State 1) and LHCP is dephosphorylated. Net phosphorylation and dephosphorylation of LHCP induced by light 2 and excess light 1, respectively, occur on the same time scale as the ATP-dependent chlorophyll fluorescence changes indicative of State 2 and State 1 transitions. The phosphatase inhibitor NaF (10 mM), stimulates the effect of blue-green light on fluorescence and prevents the effect of far-red light. These results provide a demonstration that light of different wavelengths can control excitation energy distribution between the two photosystems via the plastoquinol-activated LHCP phosphorylation mechanism suggested previously (Allen, J.F., Bennett, J., Steinback, K.E. and Arntzen, C.J. (1981) Nature 291, 25–29; and Horton, P. and Black, M.T. (1980) FEBS Lett. 119, 141–144).     

Some Optical Properties of Leaves of Eight Temperate Forage Grasses

Two instruments are described for the measurement of the reflectionand transmission of radiation by grass leaves. The first ofthese was used to measure the spatial distribution of reflectedand transmitted light. It was demonstrated that reflection wasinfluenced by the epidermal structure of a leaf, and that theimportance of this layer increased with increasing angle ofincidence. The second instrument was used to compare the reflectance andtransmittance of leaves of different ages taken from eight temperategrasses. There were significant differences between the grassesin leaf transmittance, and generally the young emerging leafhad a greater transmittance than the fully-expanded leaves.The differences in leaf transmittance could be related to differencesin specific leaf weight. There were no significant differencesbetween the species and varieties in leaf reflectance.     

Light-Harvesting Function in the Diatom Phaeodactylum tricornutum: II. Distribution of Excitation Energy between the Photosystems

The distribution of excitation energy between photosystems I and II (PSI and PSII) was investigated in the marine diatom Phaeodactylum tricornutum (Bohlin) using light-induced changes in fluorescence yield and rate of modulated O₂ evolution. The intensity dependence of the fast fluorescence rise in dark adapted cells (±DCMU) suggests that light absorbed by the major antenna complex was not delivered preferentially to PSII but is more equally distributed between the photosystems. Reversible, slow fluorescence yield changes measured in the absence of DCMU were correlated with decreased initial fluorescence and rate constants for PSII photochemistry, increased variable fluorescence, alteration of the fluorescence excitation and emission spectra, and could be effected by either 510 nm (PSII) or 704 nm (PSI) light. Slow, reversible fluorescence yield changes were also observed in the presence of DCMU, but were characterized by a loss of both initial and variable fluorescence and could not be induced by PSI light. The absence of slow changes in the yield of fluorescence and rate of modulated O₂ evolution, following addition or removal of PSI background light to modulated PSII excitation, does not support regulation of excitation energy density in PSI at the expense of PSII. The results suggest that adjustments are made at the level of excitation energy transfer to the PSII reaction center which prevent prolonged loss of photosynthetic capacity. Energy distribution is regulated by ionic distributions independently of the plastoquinone pool redox state. These differences in light-harvesting function are probably a response to the aquatic light field and may account for the success of diatoms in low and variable light environments.     

Low measuring temperature induced artifactual increase in chlorophyll a fluorescence

Measurement of in vivo chlorophyll a fluorescence at temperatures lower than 20°C can cause an artifactual, nonphotochemically related overestimation of variable fluorescence leading to the calculation of negative values for the nonphotochemical quenching parameter and an underestimation of the photochemical quenching parameter. This artifact is observed only upon exposure of the leaf sample to actinic light. We suggest that a temperature differential between the fiber-optic probe and the leaf sample results in the deposition of water vapor on the probe that distorts the light path such that an increased modulated fluorescence signal is observed. This artifact is eradicated by ensuring that the end of the fiber-optic probe is kept free of condensation.     

A New In Vivo Fluorimetric Technique To Measure Growth of Adhering Phototrophic Microorganisms

We developed a noninvasive rapid fluorimetric method for the investigation of growth of adhering (benthic) phototrophic microorganisms. The technique is based on the sensitive detection of the in vivo fluorescence of chlorophylls chlorophyll a and bacteriochlorophyll a and monitors increases in signal over time as an indicator for growth. The growth fluorimeter uses modulated excitation light of blue-light-emitting diodes and a photodiode as the detector. The light-emitting diodes are mounted geometrically in an aluminum housing for efficient and uniform illumination of the bottoms of the growth containers. The fluorimeter was characterized with respect to detection limit and dynamic range. This system is capable of resolving in vivo chlorophyll a concentrations of 0.5 (mu)g liter(sup-1) in cyanobacteria and 0.03 (mu)g liter(sup-1) in diatoms as well as in vivo bacteriochlorophyll a concentrations in phototrophic bacteria of 0.3 (mu)g liter(sup-1), which points to an extremely high sensitivity compared with that of similar available techniques. Thus, the new fluorimeter allows the determination of growth at extremely low cell densities. The instrument was used successfully to measure the growth of several adhering isolates of the filamentous cyanobacterium Microcoleus chthonoplastes from benthic microbial mats in seawater of different salinities. The data obtained demonstrate broad growth responses for all strains, which thus can be characterized as euryhaline organisms.     

Changes in the distribution of light energy between the two photosystems in spinach leaves

Time courses of chlorophyll fluorescence at room temperature and fluorescence spectra at 77 K were measured to investigate the light-induced changes in the distribution of light energy between the two photosy stems in young spinach leaves. Illumination of the dark adapted leaves with primarily system II light induced typical fluorescence transients at room temperature. Fluorescence spectra at 77 K showed that the intensity of system II fluorescence at 77 K changed nearly in parallel with the fluorescence transients at room temperature within the range from M₁ to T during illumination of the leaf. Illumination of the dark adapted leaves with light I produced an increase of system II fluorescence measured at 77 K. The characteristics of the changes induced by light I or II were different, showing that these two effects are related to different mechanisms. These results suggest that the dark state in spinach leaves is state II, that light I induces a state II to I transition, while light II induces fluorescence changes that are produced by mechanisms other than state I-state II transitions.     

Analysis of the Heat Stress Induced Quenching of Variable Chlorophyll a Fluorescence in Beet Spinach Leaves: Possible Accumulation of Oxidized Quencher P680+ under High Illumination

Effect of preheating of beet spinach leaves on chlorophyll a fluorescence yield was analyzed with the help of additional high intensity illumination pulses using a pulse modulated fluorometer. Preheating at mildly elevated temperature (35–45°C) causes a shift in the redox state of secondary donor of photosystem II, possibly due to uncoupling of phosphorylation because of thermal induced membrane disorganization and associated alkalinization of intra thylakoid space. Also, at these preheating temperatures, a rise in photosystem I catalyzed electron transfer has been shown to occur. These two effects induce rapid quenching of Chi a fluorescence, which drops even in the presence of actinic light, below the level of initial fluorescence (F_o′ monitored by the weak modulated probing light. Preheating of leaf segments induces an increase in fluorescence in the presence of dluron, which blocks electron flow between two photosystems, and thus this increases in fluorescence yield (F_o′ as monitored by weak modulated light, is not solely due to disorganization of light harvesting Chi-protein complex but also due to a shift in the redox equilibrium of the donor at the oxidizing side of photosystem II resulting in rapid reduction of Q_A the stable primary acceptor of photosystem II. In 50°C preheated DCMU treated samples, the fluorescence yield increases in weak modulated light and it approaches that of maximal steady state (F_max) level. At preheating temperature of 48°–50°C, the inactivation of enzymes in the reducing side of photosystem I, causes an impairment of the reoxidation of QA and under this condition, a strong illumination causes quenching of Chi a fluorescence. This quenching seems to arise because of accumulation of the P680⁺, the oxidized physiological donor of photosystem which is a quencher of Chi a fluorescence. This quenching depended on the pulse intensity and duration which saturates P680⁺ accumulation and is greatly manifested when water oxidation complex is damaged.     

Violet laser diodes as light sources for cytometry

BACKGROUND: Violet laser diodes have recently become commercially available. These devices emit 5-25 mW in the range of 395-415 nm, and are available in systems that incorporate the diodes with collimating optics and regulated power supplies in housing incorporating thermoelectric coolers, which are necessary to maintain stable output. Such systems now cost several thousand dollars, but are expected to drop substantially in price. Materials and Methods A 4-mW, 397-nm violet diode system was used in a laboratory-built flow cytometer to excite fluorescence of DAPI and Hoechst dyes in permeabilized and intact cells. Forward and orthogonal light scattering were also measured. RESULTS: DNA content histograms with good precision (G(0)/G(1) coefficient of variation 1.7%) were obtained with DAPI staining; precision was lower using Hoechst 33342. Hoechst 34580, with an excitation maximum nearer 400 nm, yielded the highest fluorescence intensity, but appeared to decompose after a short time in solution. Scatter signals exhibited relatively broad distributions. CONCLUSIONS: Violet laser diodes are relatively inexpensive, compact, efficient, and quiet light sources for DNA fluorescence measurement using DAPI and Hoechst dyes; they can also excite several other fluorescent probes.     

Photosynthesis-related infrared light transmission changes in spinach leaf segments

The time courses of infrared light transmission changes and fluorescence induced by light in spinach leaf segments were measured. The illumination by red light exhibited a complex wave pattern. The transmission approached the baseline after repeating decreases and increases. Illumination by far-red light decreased the transmission. One of the differences between the two responses was the difference between the two amplitudes of the first increasing component. The component in the red light response was larger than the component in the far-red light response. The transmission decrease by far-red light is supposed to correspond to "red drop." The transmission decrease by far-red light was suppressed by red light. This is due to an activation of a transmission-increasing component. This probably corresponds to "enhancement." A proportional correlation existed between the intensity of far-red light and the minimum intensity of red light that suppressed the transmission decrease induced by far-red light. The component which made Peak D in the time course of fluorescence yield and the first increasing component in the transmission changes were suppressed by intense light.     

FLIM on a wide field fluorescence microscope

Summary FLIM (Fluorescence Lifetime Imaging Microscopy) is a new tool to detect interaction between proteins. The proteins under investigation are fused with fluorescent donor and acceptor molecules. Interaction between the two proteins is accompanied by direct energy transfer from donor to acceptor (FRET), resulting in a shorter lifetime of the fluorescence emitted by the donor molecule. This change in lifetime is detected by FLIM. Fluorescence lifetime imaging can now be done on a widefield fluorescence microscope by using an attachment that is easy to install and simple to operate. The new LIFA attachment is equipped to use different excitation sources. High brightness modulated LEDs as well as lasers modulated by an Accousto Optical Modulator can be used as excitation light source. A modulated image intensifier with digital camera is used as a detector. Power supplies and signal generator are integrated in one control unit that is connected to the light source, detector and computer. All parameters for image acquisition, processing and viewing are easy accessible in the user interface of the software package that uses a modular structure. Lifetime images showing FRET in MCF7 cells with ErbB1-GFP as donor and Py72/Cy3 as acceptor that were taken at EMBL, Heidelberg are shown.