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Influence of fluorochrome labeling density on the photobleaching kinetics of fluorescein in microscopy.

The objective of this study was to identify, through kinetic analysis of individual elementary reactions, the conditions under which a simple first-order photobleaching kinetic model is sufficient for quantitative fluorescence measurements, and those under which more complex photobleaching kinetics must be considered. Three model systems of various fluorophore densities and distributions were employed to verify the kinetic analysis. The results showed that the photobleaching kinetics of free fluorescein at concentrations lower than 5 microM corresponded closely to a single exponential function and therefore involved predominantly simple unimolecular or pseudounimolecular photochemical reactions. When fluorescein was bound to polyvinyl alcohol (PVA) molecules, the photobleaching kinetics of the densely labeled PVA deviated more from a single-exponential function than sparsely labeled PVA. When fluorescein was bound to a DNA probe, the photobleaching kinetics were more complex and deviated significantly from a single-exponential function, due to one or more bimolecular processes with apparent concentration-dependent photobleaching rate constants. The practical applications of time-integrated fluorescence emission are discussed in the context of simple and complex photobleaching kinetics.

Centromere↗

Suppression of photobleaching-induced artifacts in frequency-domain FLIM by permutation of the recording order.

BACKGROUND: Photobleaching can lead to significant errors in frequency-domain fluorescence lifetime imaging microscopy (FLIM). Existing correction methods for photobleaching require additional recordings and processing time and can result in additional noise. A method is introduced that suppresses the effects of photobleaching without the need for extra recordings or processing. METHODS: Existing bleach correction methods and the method introduced in this report whereby the recording order of the phases is permuted were compared using numerical simulations. RESULTS: Certain orders were found to make measurements virtually insensitive to photobleaching. At 12 recordings, errors in measured phase and modulation depth decreased by a factor 512 and 393, respectively, compared to recordings using sequential recording order. The optimal order is independent of modulation depth, phase, and extent of photobleaching. Thus, the same order can be used for practically all situations. Application of the method in FLIM measurements of EYFP-transfected HeLa cells was found effectively to suppress photobleaching induced artifacts. CONCLUSIONS: In view of the ease of implementation, its inherent robustness, and the possibility to still apply existing correction methods afterward, there is no good reason not to use the permuted recording order presented in this report instead of a sequential order.

Artifacts↗

Reversible photobleaching of enhanced green fluorescent proteins.

Color variants of green fluorescent protein (GFP) are increasingly used for multicolor imaging, fluorescence resonance energy transfer (FRET), and fluorescence recovery after photobleaching (FRAP). Here we show that experimental settings commonly used in these imaging experiments may induce an as yet uncharacterized reversible photobleaching of fluorescent proteins, which is more pronounced at acidic pH. Whereas the reversible photobleaching spectrum of eCFP corresponds to its absorption spectrum, reversible photobleaching spectra of yellow variants resemble absorption spectra of their protonated states. Fluorescence intensities recover spontaneously with time constants of 25-58 s. The recovery of eCFP can be further accelerated by illumination. The resulting steady-state fluorescence reflects a variable equilibrium between reversible photobleaching, spontaneous recovery, and light-induced recovery. These processes can cause significant artifacts in commonly applied imaging techniques, photobleach-based FRET determinations, and FRAP assays.

Bacterial Proteins↗

Photobleaching kinetics, photoproduct formation, and dose estimation during ALA induced PpIX PDT of MLL cells under well oxygenated and hypoxic conditions.

Fluorescence photobleaching and photoproduct formation were investigated during delta-aminolevulinic acid (ALA) induced protoporphyrin IX (PpIX) PDT of MLL cells in vitro. Cells were incubated in either 0.1 or 1.0 mM ALA for 4 h and were treated with 532 nm or 635 nm light under well oxygenated or hypoxic conditions. Fluorescence spectra were acquired during treatment. Photobleaching and photoproduct formation were quantified using singular value decomposition fitting of fluorescence spectra to experimentally determined basis spectra for PpIX, photoprotoporphyrin (Ppp), product II (peak at 655 nm), and product III (peak at 618 nm). PpIX photobleaching occurred under both normal and hypoxic conditions. The photobleaching kinetics could not be explained by purely first- or second-order photobleaching kinetics, and were attributed to differences in PpIX binding at the two ALA incubation concentrations. Ppp was the main photoproduct and accumulated in higher levels in the absence of oxygen, likely a result of reduced Ppp photobleaching under hypoxia. Increases in product II fluorescence occurred mainly in the presence of oxygen. To assess potential fluorescence based PDT dose metrics, cell viability was measured at select times during treatment using a colony formation assay. Cell survival correlated well to changes in product II fluorescence, independent of oxygenation, sensitizer concentration, and treatment wavelength, suggesting that this product is primarily a result of singlet oxygen mediated reactions and may potentially be useful to quantify singlet oxygen dose during PDT.

Aminolevulinic Acid↗

Fluorescence resonance energy transfer (FRET) measurement by gradual acceptor photobleaching.

Fluorescence resonance energy transfer (FRET) is an extremely effective tool to detect molecular interaction at suboptical resolutions. One of the techniques for measuring FRET is acceptor photobleaching: the increase in donor fluorescence after complete acceptor photobleaching is a measure of the FRET efficiency. However, in wide-field microscopy, complete acceptor photobleaching is difficult due to the low excitation intensities. In addition, the method is sensitive to inadvertent donor bleaching, autofluorescence and bleed-through of excitation light. In the method introduced in this paper, donor and acceptor intensities are monitored continuously during acceptor photobleaching. Subsequently, curve fitting is used to determine the FRET efficiency. The method was demonstrated on cameleon (YC2.1), a FRET-based Ca(2+) indicator, and on a CFP-YFP fusion protein expressed in HeLa cells. FRET efficiency of cameleon in the presence of 1 mm Ca(2+) was 31 +/- 3%. In the absence of Ca(2+) a FRET efficiency of 15 +/- 2% was found. A FRET efficiency of 28% was found for the CFP-YFP fusion protein in HeLa cells. Advantages of the method are that it does not require complete acceptor photobleaching, it includes correction for spectral cross-talk, donor photobleaching and autofluorescence, and is relatively simple to use on a normal wide-field microscope.

Fluorescence Resonance Energy Transfer↗

Revealing protein dynamics by photobleaching techniques.

Green fluorescent proteins (GFPs) are widely used tools to visualize proteins and study their intracellular distribution. One feature of working with GFP variants, photobleaching, has recently been combined with an older technique known as fluorescence recovery after photobleaching (FRAP) to study protein kinetics in vivo. During photobleaching, fluorochromes get destroyed irreversibly by repeated excitation with an intensive light source. When the photobleaching is applied to a restricted area or structure, recovery of fluorescence will be the result of active or passive diffusion from fluorescent molecules from unbleached surrounding areas. Fluorescence loss in photobleaching (FLIP) is a variant of FRAP where an area is bleached, and loss of fluorescence in surrounding areas is observed. FLIP can be used to study the dynamics of different pools of a protein or can show how a protein diffuses, or is transported through a cell or cellular structure. Here, we discuss these photobleaching fluorescent imaging techniques, illustrated with examples of these techniques applied to proteins of the Saccharomyces cerevisiae pheromone response MAPK pathway.

Escherichia coli↗

High-order photobleaching of green fluorescent protein inside live cells in two-photon excitation microscopy.

Combination of green fluorescent protein (GFP) and two-photon excitation fluorescence microscopy (TPE) has been used increasingly to study dynamic biochemical events within living cells, sometimes even in vivo. However, the high photon flux required in TPE may lead to higher-order photobleaching within the focal volume, which would introduce misinterpretation about the fine biochemical events. Here we first studied the high-order photobleaching rate of GFP inside live cells by measuring the dependence of the photobleaching rate on the excitation power. The photobleaching rate under one- and two-photon excitation increased with 1-power and 4-power of the incident intensity, respectively, implying the excitation photons might interact with excited fluorophore molecules and increase the probability of photobleaching. These results suggest that in applications where two-photon imaging of GFP is used to study dynamic molecular process, photobleaching may ruin the imaging results and attention should be paid in interpreting the imaging results.

Diagnostic Imaging↗

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.

Biophysical Phenomena↗

Photobleaching kinetics of fluorescein in quantitative fluorescence microscopy.

An investigation on the photobleaching behavior of fluorescein in microscopy was carried out through a systematic analysis of photobleaching mechanisms. The individual photochemical reactions of fluorescein were incorporated into a theoretical analysis and mathematical simulation to study the photochemical processes leading to photobleaching of fluorescein in microscopy. The photobleaching behavior of free and bound fluorescein has also been investigated by experimental means. Both the theoretical simulation and experimental data show that photobleaching of fluorescein in microscopy is, in general, not a single-exponential process. The simulation suggests that the non-single-exponential behavior is caused by the oxygen-independent, proximity-induced triplet-triplet or triplet-ground state dye reactions of bound fluorescein in microscopy. The single-exponential process is a special case of photobleaching behavior when the reactions between the triplet dye and molecular oxygen are dominant.

Fluorescein↗

Mathematical description of photobleaching in vivo describing the influence of tissue optics on measured fluorescence signals.

The observed decrease in the fluorescence signal during photodynamic therapy (PDT) may contain dosimetric information as this photobleaching provides direct information on the photodynamic processes occurring in the tissue. A correct interpretation of the photobleaching signal, however, is crucial for its use in dosimetry. In this study the influence of scattering and absorption phenomena in tissue on the emitted fluorescence signal are described mathematically. Analytical solutions of the resulting expression show a difference from the single-decaying-exponential function generally used for describing photobleaching signals. The solutions are a function of the fluence rate at the inner side of tissue boundary psi(0*), the photobleaching dose constant beta, the incident irradiation power I0 and time. The accuracy of the results was investigated by comparison of the analytic solutions with numerical calculations using fluence rate profiles and escape functions obtained by Monte Carlo (MC) simulations. Good resemblance is observed when the value for psi(0*) calculated by the MC simulations is used in the analytical solutions. Experimental results in this study indicate the photobleaching dose constant of ALA-induced PpIX to be 33 +/- 3 J cm-2. Determination of beta for different types of photosensitizer and the development of an accurate method to determine psi(0*) can make monitoring of photobleaching during PDT valuable for dosimetry.

Aminolevulinic Acid↗

Protoporphyrin IX fluorescence photobleaching during ALA-mediated photodynamic therapy of UVB-induced tumors in hairless mouse skin.

Fluorescence photobleaching of protoporphyrin IX (PpIX) during superficial photodynamic therapy (PDT), using 514 nm excitation, was studied in UVB-induced tumor tissue in the SKH-HR1 hairless mouse. The effects of different irradiance and light fractionation regimes upon the kinetics of photobleaching and the PDT-induced damage were examined. Results show that the rate of PpIX photobleaching (i.e., fluorescence intensity vs fluence) and the PDT damage both increase with decreasing irradiance. We have also detected the formation of fluorescent PpIX photoproducts in the tumor during PDT, although the quantity recorded is not significantly greater than generated in normal mouse skin, using the same light regime. The subsequent photobleaching of the photoproducts also occurs at a rate (vs fluence) that increases with decreasing irradiance. In the case of light fractionation, the rate of photobleaching increases upon renewed exposure after the dark period, and there is a corresponding increase in PDT damage although this increase is smaller than that observed with decreasing irradiance. The effect of fractionation is greater in UVB-induced tumor tissue than in normal tissue and the damage is enhanced when fractionation occurs at earlier time points. We observed a variation in the distribution of PDT damage over the irradiated area of the tumor: at high irradiance a ring of damage was observed around the periphery. The distribution of PDT damage became more homogeneous with both lower irradiance and the use of light fractionation. The therapeutic dose delivered during PDT, calculated from an analysis of the fluorescence photobleaching rate, shows a strong correlation with the damage induced in normal skin, with and without fractionation. The same correlation could be made with the data obtained from UVB-induced tumor tissue using a single light exposure. However, there was no such correlation when fractionation schemes were employed upon the tumor tissue.

Aminolevulinic Acid↗

Singlet oxygen- versus nonsinglet oxygen-mediated mechanisms of sensitizer photobleaching and their effects on photodynamic dosimetry.

We report the effects of singlet oxygen (1O2) and non-1O2-mediated sensitizer photobleaching on oxygen consumption and dosimetry during photodynamic therapy (PDT) of sensitized multicell tumor spheroids. We develop a theoretical model for the description of non-1O2-mediated photobleaching resulting from irreversible reactions of the excited singlet or triplet sensitizer populations with cell substrate. We show that the fluence-dependent simple exponential decay expression of sensitizer degradation is not consistent with these mechanisms and, therefore, with any reasonable mechanism that we consider, because we have shown previously that 1O2-mediated photobleaching cannot be described by a simple exponential with a constant photobleaching coefficient (I. Georgakoudi et al., Photochem. Photobiol. 65, 135-144, 1997). Analysis of oxygen microelectrode measurements performed at the edge of Nile blue selenium (EtNBSe)- and protoporphyrin IX (PpIX)-sensitized spheroids during PDT demonstrates that the former drug photobleaches via a non-1O2-mediated mechanism, while the latter is degraded via a 1O2-mediated mechanism. Comparisons of the cytotoxic effects of EtNBSe with those of Photofrin (a drug that is degraded via a 1O2-mediated mechanism) indicate that the lower threshold 1O2 dose and the higher extinction coefficient and 1O2 yield for EtNBSe do not necessarily result in improved photodynamic effects, thus emphasizing the importance of the sensitizer photobleaching mechanism for dosimetry.

Animals↗

Fluorescence recovery under decaying photobleaching irradiation: concept and experiment.

A novel modification of photobleaching method for measurement of lateral diffusion is developed. In this approach fluorescence recovery kinetics is measured under decaying photobleaching irradiation, termed as fluorescence recovery under decaying photobleaching (FRDP). The time evolution of fluorescence intensity normalized to input irradiation starts from the photobleaching kinetics and transforms into the kinetics of fluorescence recovery at a later stage resulting in appearance of minimum. The analytical solution for the kinetics of fluorescence for Gaussian lineshape of laser beam and hyperbolic decay of irradiation in the first order approximation on bleaching rate was obtained. The accuracy of the analytical function was evaluated with exact numerical solution computed with finite differentiates method. The FRDP method was successfully applied to fluorescein solution in the glycerol/water mixture (80%) under various experimental settings using home-made experimental set-up. The FRDP approach demonstrated 25-30 fold enhancement in signal intensity over classical fluorescence recovery after photobleaching (FRAP) method at 3-5 fold increase in total irradiation. Among other advantages of the FRDP is the opportunity to perform measurements on varying time scales under constant size of the bleaching spot, including "safe" long time measurements. The potential extra advantage of FRDP method for analysis of complex diffusion in the biological system is discussed.

Fluorescence Recovery After Photobleaching↗

The photobleaching of disulfonated aluminium phthalocyanine in microbial systems.

Front-face illumination spectroscopic techniques were used to study photobleaching of disulfonated aluminium phthalocyanine (AlPcS2) in the bacteria and yeast cells Escherichia coil, Porphyromonas gingivalis (Gram-negative bacteria), Streptococcus mutans (a Gram-positive bacterium), and the yeast Candida albicans. The photobleaching of AlPcS2 with the microbes studied is complex, involving reactive species generated by type I and type II processes with the rate dependent on the relative contributions of the different photobleaching mechanisms. The average rate of photobleaching of the AlPcS2 monomer in the presence of both E. coli and C. albicans increases as the fluence of the illumination source decreases. The effects of oxygen and sensitiser concentration on the rate of AlPcS2 photobleaching in these systems are also investigated.

Candida albicans↗

Photobleaching of bacteriorhodopsin solubilized with triton X-100.

In the current studies, we examined the effects of hexagonal lattice formation with lipid membranes on the structural stability of native bacteriorhodopsin (bR). Denaturation kinetic measurements for bR solubilized with the mild nonionic detergent Triton X-100 (TX100) were performed in the dark and under illumination by visible light. The solubilized bR was stable in the dark over a wide concentration range of TX100 (1 to 200 mM). In purple membranes, a bilobed band was observed in visible circular dichroism spectra due to interactions between neighboring chromophores. At all concentrations of TX100, this was replaced by a single positive band. Upon illumination with visible light, TX100-solubilized bR clearly showed photobleaching to bacterioopsin. These experimental results suggest that photobleaching is due to a lack of intermolecular interactions inside the purple membrane lattice. Extensive kinetic measurements further revealed that the rate constant of photobleaching is strongly dependent on the detergent concentration, although the activation energy for photobleaching does not significantly change with the TX100 concentration. The mechanism of photobleaching for the solubilized bR is discussed with respect to detergent micelle properties.

Bacteriorhodopsins↗

Studies on singlet oxygen formation and UVA light-mediated photobleaching of the yellow chromophores in human lenses.

The protein-bound chromophores, which increase with aging in the human lens, act as UVA sensitizers, producing almost exclusively singlet oxygen in vitro. Direct irradiation of whole, aged human lenses with high intensity UVA light (200 mW cm(-2) for 24 hr), however, failed to produce singlet oxygen damage, as evidenced by the lack of either His or Trp photodestruction. Total homogenates of human lenses prepared in a cuvette under air did show destruction of His and Trp residues by UVA light, but no destruction was seen when equivalent homogenates were prepared under argon. These data are consistent with the idea that the low oxygen levels in the lens prevent singlet oxygen damage in vivo.UVA irradiation of aged human lenses in culture caused an extensive photobleaching of the yellow chromophores. A time course indicated that the photobleaching increased with time, with significant color loss apparent after 6 hr. Homogenization of the irradiated and dark control lenses in 6 M guanidine-HCl, followed by determination of the difference spectrum, showed approximately 50% bleaching of compounds with a lambda(max) at 355 nm. Similarly, fluorophores with a lambda(max) for excitation of 355 nm and for emission of 420 nm were 50% destroyed by the UVA light. Similar results were obtained in vitro by the anaerobic irradiation of a sonication-solubilized WI fraction from type II brunescent cataracts and from aged human lenses. In this system, there was an initial bleaching of 15% after 30 min of irradiation, followed by a slow increase over the next 6 hr to a final bleaching of 30%. The addition of 1.0 m M ascorbic acid, but not 1.0 m M glutathione (GSH), increased the photobleaching to 60% under argon, and the loss of ascorbate could be detected under these anaerobic conditions. In the presence of air, UVA light produced no photobleaching, but rather caused a three-fold increase in absorbance at 345 nm, which was prevented by the inclusion of 1.0 m M ascorbic acid and almost 50% inhibited by 1.0 m M GSH. The data are consistent with the conversion of the triplet state of the sensitizers to anion and cation radicals in the absence of oxygen. Photobleaching may occur either by dismutation of the anion radical or by reduction of the anion radical by ascorbate via type I chemistry. UVA irradiation of an enriched fraction of sensitizers from a proteolytic digest from type II cataract lenses produced a 63% bleaching at 330 nm in the absence of oxygen, and the almost complete loss of the A(330) absorbing and 350/450 nm fluorescent peaks upon HPLC separation. This loss correlated with the loss of the ability of the irradiated fraction to produce singlet oxygen in vitro upon subsequent UVA irradiation.

Aged↗

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.

Animals↗

Spatial Fourier analysis of video photobleaching measurements. Principles and optimization.

The major use of the fluorescence recovery after photobleaching (FRAP) technique is to measure the translational motion of the molecular components in various condensed media. In a conventional laser spot photobleaching experiment, a photomultiplier is used to measure the total brightness levels of the bleached region in the sample, so no spatial information can be directly obtained. In video-FRAP, a series of images after photobleaching is acquired, allowing the spatial character of the recovery to be determined; this permits direct detection of both anisotropic diffusion and flow. To utilize all of the available image data to determine the transport coefficients, a two-dimensional spatial Fourier transform analysis of the images after photobleaching was employed. The change in the transform between two time points reflects the action of diffusion during the interim. An important advantage of this method, which involves taking the ratio of image transforms at different time points, is that it does not require a specific initial condition to be created by laser photobleaching. The ability of the analysis to extract transport coefficients from computer-simulated diffusional recovery is assessed in the presence of increasing amounts of noise. Experimental data analysis from the diffusion of proteins in viscous solutions and from the diffusion of protein receptors on cell surfaces demonstrate the feasibility of the Fourier analysis to obtain transport coefficients from the video FRAP measurement.

Biophysical Phenomena↗