Influence of the triplet excited state on the photobleaching kinetics of fluorescein in microscopy.

The investigation in this report aimed at providing photophysical evidence that the long-lived triplet excited state plays an important role in the non-single-exponential photobleaching kinetics of fluorescein in microscopy. Experiments demonstrated that a thiol-containing reducing agent, mercaptoethylamine (MEA or cysteamine), was the most effective, among other commonly known radical quenchers or singlet oxygen scavengers, in suppressing photobleaching of fluorescein while not reducing the fluorescence quantum yield. The protective effect against photobleaching of fluorescein in the bound state was also found in microscopy. The antibleaching effect of MEA let to a series of experiments using time-delayed fluorescence spectroscopy and nanosecond laser flash photolysis. The combined results showed that MEA directly quenched the triplet excited state and the semioxidized radical form of fluorescein without affecting the singlet excited state. The triplet lifetime of fluorescein was reduced upon adding MEA. It demonstrated that photobleaching of fluorescein in microscopy is related to the accumulation of the long-lived triplet excited state of fluorescein and that by quenching the triplet excited state and the semioxidized form of fluorescein to restore the dye molecules to the singlet ground state, photobleaching can be reduced.     

Digital imaging fluorescence microscopy: spatial heterogeneity of photobleaching rate constants in individual cells

Photobleaching and related photochemical processes are recognized experimental barriers to quantification of fluorescence by microscopy. We have measured the kinetics of photobleaching of fluorophores in living and fixed cells and in microemulsions, and have demonstrated the spatial variability of these processes within individual cells. An inverted fluorescence microscope and a high-sensitivity camera, together with high-speed data acquisition by a computer-controlled image processor, have been used to control precisely exposure time to excitation light and to record images. To improve the signal-to-noise ratio, 32 digital images were integrated. After correction for spatial variations in camera sensitivity and background fluorescence, the images of the relative fluorescence intensities for 0.065 micron2 areas in the object plane were obtained. To evaluate photobleaching objectively, an algorithm was developed to fit a three-parameter exponential equation to 20 images recorded from the same microscope field as a function of illumination time. The results of this analysis demonstrated that the photobleaching process followed first-order reaction kinetics with rate constants that were spatially heterogeneous and varied, within the same cell, between 2- and 65-fold, depending on the fluorophore. The photobleaching rate constants increased proportionally with increasing excitation intensity and, for benzo(a)pyrene, were independent of probe concentration over three orders of magnitude (1.25 microM to 1.25 mM). The propensity to photobleach was different with each fluorophore. Under the cellular conditions used in these studies, the average rates of photobleaching decreased in this order: N-(7-nitrobenz-2-oxa-1,3-diazole)-23,24-dinor-5-cholen-22-amine-3 beta-ol greater than acridine orange greater than rhodamine-123 greater than benzo(a)pyrene greater than fluorescein greater than tetramethylrhodamine greater than 1,1'dioctadecyl-3,3,3',3'-tetramethylindocarbocyanine. The photobleaching appears to be an oxidation reaction, in that the addition of saturated solutions of Na2S2O5 to mineral oil microemulsions eliminated photobleaching of N-(7-nitrobenz-2-oxa-1,3-diazole)-23,24-dinor-5-cholen-22-amine-3 beta-ol or benzo(a)pyrene. We identified experimental conditions to observe, without detectable photobleaching, fluorophores in living cells, which can not be studied anaerobically. Useful images were obtained when excitation light was reduced to eliminate photobleaching, as determined from zero-time images calculated from the exponential fit routine.(ABSTRACT TRUNCATED AT 400 WORDS)     

Proton-collecting properties of bovine heart cytochrome C oxidase: kinetic and electrostatic analysis.

Proton-transfer reactions on the surface of bovine heart cytochrome c oxidase were investigated by combining a laser-induced proton-pulse technique with molecular modeling. The experimental approach simultaneously monitors the state of pyranine protonation in the bulk phase and that of a fluorescein indicator specifically attached to the native Cys(III-115) residue of subunit III of cytochrome oxidase. The reversible dynamics of the acid-base equilibration between the surface and the bulk phase were measured with submicrosecond time resolution and analyzed by numerical integration of coupled nonlinear differential rate equations. Kinetic analysis shows that carboxylates on the surface of the protein act as a proton-collecting antenna, which is able to rapidly transfer protons to nearby histidines that function as a local proton reservoir. These properties enable cytochrome oxidase to carry out its redox-linked proton translocation. Molecular modeling of the fluorescein-binding site indicates that, in addition to the covalent bond, the dye is anchored through a hydrogen bond to the hydroxyl moiety of Tyr(VII-50). The protonation of the dye is mediated through three residues that shuttle protons between the bulk and the dye. A correlation between the measured kinetic properties of the bound fluorescein and the different configurations of the dye allows us to predict the identity of the proton-binding sites in the fluorescein-binding domain.     

Direct measurement of diffusion in olfactory cilia using a modified FRAP approach

The diffusion coefficient of fluorescein in detached cilia of Xenopus laevis olfactory receptor neurons was measured using spatially-resolved FRAP, where the dye along half of the ciliary length was photobleached and its spatiotemporal fluorescence redistribution recorded. Fitting a one-dimensional numerical simulation of diffusion and photobleaching for 35 cilia resulted in a mean value of the diffusion coefficient (1.20 ± 0.23) · 10(-10)m(2)/s and thus a reduction by a factor of 3.4 compared to free diffusion in aqueous solution.     

Light-induced permeabilization and merocyanine 540 staining of mouse spleen cells

Merocyanine 540 (M540) is a potential-sensitive, hydrophobic dye that preferentially incorporates into the 'fluid' domains of cellular membranes, distinguishing between hemopoietic cells according to their differentiation state. A bright staining with M540 is usually achieved by UV illumination of the cells during staining. We show by flow cytometric analysis that: (1) staining is greatly enhanced by UV illumination of mouse spleen cells before addition of the dye; (2) UV treatment causes an increased permeability toward propidium iodide and intracellular fluorescein as well; (3) the increment in M540 fluorescence precedes permeabilization to propidium iodide, while the latter precedes leakage of fluorescein. We also describe an overshoot and accelerated recovery of M540 fluorescence after photobleaching by a 514 nm laser beam. It is suggested that penetration of M540 to the more fluid inner membrane structures explains the fluorescence increment in both experiments.     

Superoxide enhances photobleaching during cellular immune attack against fluorescent lipid monolayer membranes

Lipid hapten-containing monolayer membranes with bound, anti-hapten antibody molecules serve as model immunological target membranes. Targets with bound-IgG trigger guinea pig macrophages to (a) adhere, (b) spread, (c) release lysosomal enzymes, and (d) increase cyanide-insensitive oxygen consumption. When the target membranes are derivatized with fluorescein, there is a 2-3-fold enhancement in the rate of fluorescein photobleaching in regions of cell-monolayer contact. This effect is due to release of O2- from macrophages, as shown by inhibition with superoxide dismutase and by the fact that enhanced photobleaching is not observed with cells of the RAW264 macrophage line, which undergo responses (a)-(d), but do not release O2- extracellularly. The O2- dependent photobleaching reaction appears to be relatively specific for fluorescein, as it did not occur with two other fluorophores, 4-nitrobenz-2-oxa-1,3-diazole and tetramethyl-rhodamine. Because stimulated neutrophils release large quantities of O2-, the photobleaching of fluorescein-labeled target membranes in response to neutrophils was examined. Monolayer membranes with specifically bound IgG caused neutrophils to adhere and become markedly motile during incubation at 37 degrees C. Like macrophages, neutrophils induced O2- -dependent photobleaching of fluorescein-labeled IgG in regions of cell-monolayer contact. In addition, neutrophils gave rise to a slower, nonphotochemical loss of fluorescence in the same contact regions. The latter effect is apparently due to cleavage of target-bound fluorescent IgG by proteolytic enzymes secreted by the neutrophils in response to the target surface.     

Photobleaching in two-photon excitation microscopy

The intensity-squared dependence of two-photon excitation in laser scanning microscopy restricts excitation to the focal plane and leads to decreased photobleaching in thick samples. However, the high photon flux used in these experiments can potentially lead to higher-order photon interactions within the focal volume. The excitation power dependence of the fluorescence intensity and the photobleaching rate of thin fluorescence samples ( approximately 1 microm) were examined under one- and two-photon excitation. As expected, log-log plots of excitation power versus the fluorescence intensity and photobleaching rate for one-photon excitation of fluorescein increased with a slope of approximately 1. A similar plot of the fluorescence intensity versus two-photon excitation power increased with a slope of approximately 2. However, the two-photon photobleaching rate increased with a slope > or =3, indicating the presence of higher-order photon interactions. Similar experiments on Indo-1, NADH, and aminocoumarin produced similar results and suggest that this higher-order photobleaching is common in two-photon excitation microscopy. As a consequence, the use of multi-photon excitation microscopy to study thin samples may be limited by increased photobleaching.     

The mechanism of proton transfer between adjacent sites on the molecular surface

The surface of a protein, or a membrane, is spotted with a multitude of proton binding sites, some of which are only few A apart. When a proton is released from one site, it propagates through the water by a random walk under the bias of the local electrostatic potential determined by the distribution of the charges on the protein. Eventually, the released protons are dispersed in the bulk, but during the first few nanoseconds after the dissociation, the protons can be trapped by encounter with nearby acceptor sites. While the study of this reaction on the surface of a protein suffers from experimental and theoretical difficulties, it can be investigated with simple model compounds like derivatives of fluorescein. In the present study, we evaluate the mechanism of proton transfer reactions that proceed, preferentially, inside the Coulomb cage of the dye molecules. Kinetic analysis of the measured dynamics reveals the role of the dimension of the Coulomb cage on the efficiency of the reaction and how the ordering of the water molecules by the dye affects the kinetic isotope effect.     

Fluorescence decay studies of the DNA-3,6-diaminoacridine complexes

The interaction of several 3,6-diaminoacridines with DNAs of various base composition has been studied by steady-state and transient fluorescence measurements. The acridine dyes employed are of the following two classes: class I - proflavine, acriflavine and 10-benzyl proflavine; class II - acridine yellow, 10-methyl acridine yellow and benzoflavine. It is found that the fluorescence decay kinetics follows a single-exponential decay law for free dye and the poly[d(A-T)]-dye complex, while that of the dye bound to DNA obeys a two-exponential decay law. The long lifetime (tau 1) for each complex is almost the same as the lifetime for the poly[d(A-T)]-dye complex, and the amplitude alpha 1 decreases with increasing GC content of DNA. The fluorescence quantum yields (phi F) of dye upon binding to DNA decrease with increasing GC content; the phi F values for class I are nearly zero when bound to poly(dG) X poly(dC), but those for class II are not zero. This is in harmony with the finding that GMP almost completely quenches the fluorescence for class I, whereas a weak fluorescence arises from the GMP-dye complex for class II. The fluorescence spectra of the DNA-dye complexes gradually shift toward longer wavelengths with increasing GC content. In this connection, the fluorescence decay parameters show a dependence on the emission wavelength; alpha 1 decreases with an increase in the emission wavelength. In view of these results, it is proposed that the decay behavior of the DNA-dye complexes has its origin in the heterogeneity of the emitting sites; the long lifetime tau 1 results from the dye bound to AT-AT sites, while the short lifetime tau 2 is attributable to the dye bound in the vicinity of GC pairs. Since GC pairs almost completely quench the fluorescence for class I, partly intercalated or externally bound dye molecules may play an important role in the component tau 2.     

Two-photon thermal bleaching of single fluorescent molecules

We have studied the fluorescence emission by two-photon excitation of four dyes widely used for bioimaging studies, rhodamine 6G, fluorescein, pyrene and indo-1 at the single molecule level. The single dye molecules, spread on a glass substrate by spin coating, show a constant fluorescence output until a sudden transition to a dark state very close to the background. The bleaching time that is found to vary in the series pyrene, indo-1, fluorescein and rhodamine 6G from the fastest to the slowest one respectively, has a Gaussian distribution indicating that the observed behavior is not due to photobleaching. Moreover, the bleaching time decreases with the glass substrate temperature reaching a vanishing nonmeasurable value for a limiting temperature whose value is found in the same series as for the bleaching time, from the lowest to the highest temperature respectively. The observed bleaching shows a clear correlation to the amount of absorbed power not reirradiated as fluorescence and to the complexity of the molecule. These observations are interpreted as thermal bleaching where the temperature increase is induced by the two-photon absorption of the single dyes as confirmed also by numerical simulations.     

Fluorescence correlation spectroscopy and photobleaching recovery of multiple binding reactions. I. Theory and FCS measurements

Fluorescence correlation spectroscopy (FCS) and fluorescence photobleaching recovery (FPR) are two methods that may be used to measure diffusion and chemical reaction kinetics in small, labile systems such as biological cells. These methods are here applied to systems in which a fluorescent ligand can bind to a polyvalent substrate molecule in a multistep reaction sequence. The analytical theory for both FCS and FPR is extended to allow analysis of these kinds of systems. Experimental measurements of the binding of ethidium bromide to DNA by FCS confirm the theoretical analysis. (FPR measurements on the same system are reported in the accompanying paper.) The analysis shows that FCS and FPR perceive multivalent binding reactions differently. This difference results from the selective effect of the photobleaching process in the chemical reaction system. The development and results we report could have useful applications to a wide range of biopolymeric binding and assembly process.     

Photodegradation and phototransformation of 5,10,15,20-tetrakis(m-hydroxyphenyl)bacteriochlorin (m-THPBC) in solution.

The kinetics of photobleaching and formation of photoproducts upon irradiation (735 nm) of 5,10,15,20-tetrakis(m-hydroxyphenyl)bacteriochlorin (m-THPBC) in phosphate buffer saline (PBS) supplemented with human serum albumin (HSA) were studied by means of absorption and steady-state fluorescence spectroscopy. Measurements were performed either immediately after the dye was dissolved in the HSA solution (0 h) or after six hours incubation in the HSA solution (6 h). Spectroscopic studies indicated that the dye was mainly present as aggregates in freshly prepared solutions, whereas incubation favored monomerisation. Irrespective to incubation time, the rates of photobleaching obtained by fluorescence measurements were higher than those obtained from absorbance measurements. Photobleaching of freshly prepared m-THPBC can be described by a single exponential decay, while the absorbance and fluorescence decays of the incubated dye solutions better fit a bi-exponential decay. Two photobleaching rates probably reflect differences in the photosensitivity of monomer (bound to proteins) and aggregated (non-bound) forms. Irradiation of the freshly prepared m-THPBC solution led to phototransformation of 50% of the bleached m-THPBC into 5,10,15,20-tetrakis(m-hydroxyphenyl)chlorin (m-THPC), a clinically used second generation photosensitizer. For irradiation 6 h after dissolving m-THPBC, different kinetics of m-THPC formation were found. A rapid decrease in concentration of m-THPBC was accompanied by a slow formation of m-THPC. The quantum yield of this process was small since only 5% of m-THPBC was transformed to m-THPC. The kinetics characteristics of m-THPBC photobleaching reported in the present study, together with the different kinetics of photoproduct formation during m-THPBC photobleaching, may provide important indications in the m-THPBC-based PDT dosimetry.     

The mechanism of proton transfer between adjacent sites on the molecular surface

The surface of a protein, or a membrane, is spotted with a multitude of proton binding sites, some of which are only few Å apart. When a proton is released from one site, it propagates through the water by a random walk under the bias of the local electrostatic potential determined by the distribution of the charges on the protein. Eventually, the released protons are dispersed in the bulk, but during the first few nanoseconds after the dissociation, the protons can be trapped by encounter with nearby acceptor sites. While the study of this reaction on the surface of a protein suffers from experimental and theoretical difficulties, it can be investigated with simple model compounds like derivatives of fluorescein. In the present study, we evaluate the mechanism of proton transfer reactions that proceed, preferentially, inside the Coulomb cage of the dye molecules. Kinetic analysis of the measured dynamics reveals the role of the dimension of the Coulomb cage on the efficiency of the reaction and how the ordering of the water molecules by the dye affects the kinetic isotope effect.     

Lateral mobility of integral proteins in red blood cell tethers.

The red blood cell membrane is a complex material that exhibits both solid- and liquidlike behavior. It is distinguished from a simple lipid bilayer capsule by its mechanical properties, particularly its shear viscoelastic behavior and by the long-range mobility of integral proteins on the membrane surface. Subject to sufficiently large extension, the membrane loses its shear rigidity and flows as a two-dimensional fluid. These experiments examine the change in integral protein mobility that accompanies the mechanical phenomenon of extensional failure and liquidlike flow. A flow channel apparatus is used to create red cell tethers, hollow cylinders of greatly deformed membrane, up to 36-microns long. The diffusion of proteins within the surface of the membrane is measured by the technique of fluorescence redistribution after photobleaching (FRAP). Integral membrane proteins are labeled directly with a fluorescein dye (DTAF). Mobility in normal membrane is measured by photobleaching half of the cell and measuring the rate of fluorescence recovery. Protein mobility in tether membrane is calculated from the fluorescence recovery rate after the entire tether has been bleached. Fluorescence recovery rates for normal membrane indicate that more than half the labeled proteins are mobile with a diffusion coefficient of approximately 4 x 10(-11) cm2/s, in agreement with results from other studies. The diffusion coefficient for proteins in tether membrane is greater than 1.5 x 10(-9) cm2/s. This dramatic increase in diffusion coefficient indicates that extensional failure involves the uncoupling of the lipid bilayer from the membrane skeleton.     

Luminescent/paramagnetic probes for detecting order in biological assemblies: transformation of luminescent probes into pi-radicals by photochemical reduction.

The spectroscopic methods of fluorescence polarization and electron paramagnetic resonance (EPR) are used to study order and orientation of extrinsically labeled protein elements of ordered biological systems. These methods generate complementary information about the order of the system, but a consistent quantitative interpretation of the related data is complicated because the signals arise from different donors. We introduce a new method that allows us to detect both signals from the same donor. Unsubstituted xanthene dyes (eosin, erythrosin, and fluorescein) were irradiated by laser light at their absorption maximum in the presence of different reducing agents. Due to photochemical reduction, the quinoidal structure of the xanthene ring is transformed into a semiquinone, and a pi-radical is formed having a characteristic EPR signal of an unpaired electron spin with proton hyperfine interactions. A strong EPR signal is observed from the dye in solution or when specifically attached to a protein following irradiation in the presence of dithiothreitol or cysteine. We applied this technique to the study of skeletal muscle fibers. The fluorescent dye (iodoacetamido)fluorescein was covalently attached to the reactive thiol of the myosin molecule in muscle fibers. Fluorescence polarization and EPR spectroscopy were performed on the labeled fibers in rigor. Both signals indicate a highly ordered system characteristic of cross-bridges bound to actin. Our use of the same signal donor for fluorescence and EPR studies of probe order is a promising new technique for the study of order in protein elements of biological assemblies.     

Relationship of proton release at the extracellular surface to deprotonation of the schiff base in the bacteriorhodopsin photocycle.

The surface potential of purple membranes and the release of protons during the bacteriorhodopsin photocycle have been studied with the covalently linked pH indicator dye, fluorescein. The titration of acidic lipids appears to cause the surface potential to be pH-dependent and causes other deviations from ideal behavior. If these anomalies are neglected, the appearance of protons can be followed by measuring the absorption change of fluorescein bound to various residues at the extracellular surface. Contrary to widely held assumption, the activation enthalpies of kinetic components, deuterium isotope effects in the time constants, and the consequences of the D85E, F208R, and D212N mutations demonstrate a lack of direct correlation between proton transfer from the buried retinal Schiff base to D85 and proton release at the surface. Depending on conditions and residue replacements, the proton release can occur at any time between the protonation of D85 and the recovery of the initial state. We conclude that once D85 is protonated the proton release at the extracellular protein surface is essentially independent of the chromophore reactions that follow. This finding is consistent with the recently suggested version of the alternating access mechanism of bacteriorhodopsin, in which the change of the accessibility of the Schiff base is to and away from D85 rather than to and away from the extracellular membrane surface.     

Cytoplasmic viscosity near the cell plasma membrane: translational diffusion of a small fluorescent solute measured by total internal reflection-fluorescence photobleaching recovery.

Total internal reflection-fluorescence recovery after photobleaching (TIR-FRAP) was applied to measure solute translational diffusion in the aqueous phase of membrane-adjacent cytoplasm. TIR fluorescence excitation in aqueous solutions and fluorescently labeled cells was produced by laser illumination at a subcritical angle utilizing a quartz prism; microsecond-resolution FRAP was accomplished by acousto-optic modulators and electronic photomultiplier gating. A mathematical model was developed to determine solute diffusion coefficient from the time course of photobleaching recovery, bleach time, bleach intensity, and evanescent field penetration depth; the model included irreversible and reversible photobleaching processes, with triplet state diffusion. The validity and accuracy of TIR-FRAP measurements were first examined in aqueous fluorophore solutions. Diffusion coefficients for fluorescein isothiocyanate-dextrans (10-2000 kDa) determined by TIR-FRAP (recovery t1/2 0.5-2.2 ms) agreed with values measured by conventional spot photobleaching. Model predictions for the dependence of recovery curve shape on solution viscosity, bleach time, and bleach depth were validated experimentally using aqueous fluorescein solutions. To study solute diffusion in cytosol, MDCK epithelial cells were fluorescently labeled with the small solute 2',7'-bis-2-carboxyethyl-5-carboxyfluorescein-acetoxymethyl-ester (BCECF). A reversible photobleaching process (t1/2 approximately 0.5 ms) was identified that involved triplet-state relaxation and could be eliminated by triplet-state quenching with 100% oxygen. TIR-FRAP t1/2 values for irreversible BCECF bleaching, representing BCECF translational diffusion in the evanescent field, were in the range 2.2-4.8 ms (0.2-1 ms bleach times), yielding a BCECF diffusion coefficient 6-10-fold less than that in water. These results establish the theory and the first experimental application of TIR-FRAP to measure aqueous-phase solute diffusion, and indicate slowed translational diffusion of a small solute in membrane-adjacent cytosol.     

Probing of the substrate binding domain of lactose permease by a proton pulse

The lactose permease of Escherichia coli coupled proton transfer across the bacterial inner membrane with the uptake of beta-galactosides. In the present study we have used the cysteine-less C148 mutant that was selectively labeled by fluorescein maleimide on the C148 residue, which is an active component of the substrate transporting cavity. Measurements of the protonation dynamics of the bound pH indicator in the time resolved domain allowed us to probe the binding site by a free diffusing proton. The measured signal was reconstructed by numeric integration of differential rate equations that comply with the detailed balance principle and account for all proton transfer reactions taking place in the reaction mixture. This analysis yields the rate constants and pK values of all residues participating in the fast proton transfer reaction between the bulk and the protein's surface, revealing the exposed residues that react with free protons in a diffusion controlled reaction and how they transfer protons among themselves. The magnitudes of these rate constants were finally evaluated by comparison with the rate predicted by the Debye-Smoluchowski equation. The analysis of the kinetic and pK values indicated that the protein-fluorescein adduct assumes two conformation states. One is dominant above pH 7.4, while the other exists only below 7.1. In the high pH range, the enzyme assumes a constrained configuration and the rate constant of the reaction of a free diffusing proton with the bound dye is 10 times slower than a diffusion controlled reaction. In this state, the carboxylate moiety of residue E126 is in close proximity to the dye and exchanges a proton with it at a very fast rate. Below pH 7.1, the substrate binding domain is in a relaxed configuration and freely accessed by bulk protons, and the rate of proton exchange between the dye and E126 is 100,000 times slower. The relevance of these observations to the catalytic cycle is discussed.     

Surface functions during mitosis. III. Quantitative analysis of ligand- receptor movement into the cleavage furrow: diffusion vs. flow

The surface distribution of concanavalin A (Con A) bound to cell membrane receptors varies dramatically as a function of mitotic phase. The lectin is distributed diffusely on cells labeled and observed between mid-prophase and early anaphase, whereas cells observed in late anaphase or telophase demonstrate a marked accumulation of Con A- receptor complexes over the developing cleavage furrow (Berlin, Oliver, and Walter. 1978. Cell. 15:327-341). In this report, we first use a system based on video intensification fluorescence microscopy to describe the simultaneous changes in cell shape and in lectin-receptor complex topography during progression of single cells through the mitotic cycle. The video analysis establishes that fluorescein succinyl Con A (F-S Con A)-receptor complex redistribution begins coincident with the first appearance of the cleavage furrow and is essentially complete within 2-3 min. This remarkable redistribution of surface fluorescence occurs during only a modest change in cell shape from a sphere to a belted cylinder. It reflects the translocation of complexes and not the accumulation of excess labeled membrane in the cleavage furrow: first, bound fluorescent cholera toxin which faithfully outlines the plasma membrane is not accumulated in the cleavage furrow, and, second, electron microscopy of peroxidase-Con A labeled cells undergoing cleavage shows that there is a high linear density of lectin within the furrow while Con A is virtually eliminated from the poles. The rate of surface movement of F-S Con A was quantitated by photon counting during a repetitive series of laser-excited fluorescence scans across dividing cells. Results were analyzed in terms of two alternative models of movement: a flow model in which complexes moved unidirectionally at constant velocity, and a diffusion model in which complexes could diffuse freely but were trapped at the cleavage furrow. According to these models, the observed rates of accumulation were attainable at either an effective flow velocity of approximately 1 micron/min, or an effective diffusion coefficient of approximately 10(- 9) cm2/s. However, in separate experiments the lectin-receptor diffusion rate measured directly by the method of fluorescence recovery after photobleaching (FRAP) on metaphase cells was only approximately 10(-10) cm2/s. Most importantly, photobleaching experiments during the actual period of F-S Con A accumulation showed that lectin-receptor movement during cleavage occurs unidirectionally. These results rule out diffusion and make a process of oriented flow of ligand-receptor complexes the most likely mechanism for ligand-receptor accumulation in the cleavage furrow.     

Effects of second order photobleaching on recovered diffusion parameters from fluorescence photobleaching recovery

In the original theoretical development of fluorescence photobleaching recovery with circular or Gaussian laser intensity profiles (Axelrod et al., 1976, Biophys. J.) the bleaching process is assumed to obey first order kinetics in the fluorescent probe. While this is reasonable in most cases where oxygen participates in the photolysis reaction, some processes may obey second order kinetics in the fluorophore concentration due to dimerization. Accordingly, we present here an analysis of the fluorescence recovery when the photobleaching process is taken to be second order in the probe. Analytical solutions for small bleaching levels indicate that the fluorescence recovery curve is very similar to that measured following a bleaching process first order in the probe. Numerical solutions for moderate bleaching levels show that the recovery is qualitatively similar, but quantitatively different. Because the shape of the recovery curve provides no evidence as to the order of photobleaching, we recommend continued use of the previous theoretical analysis. However, it must be borne in mind that the diffusion coefficient is increasingly underestimated as the extent of photobleaching is increased. The true diffusion coefficient is obtained in the limit of small levels of photobleaching. Estimates of the fractional recovery are not affected by this approach.