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.     

Polarization of fluorescein fluorescence in single cells.

Measurement of fluorescence polarization (P) gives information about the immediate environment of the fluorescent molecule. We used a flow polarimeter to investigate the factors influencing P of fluorescein in mammalian cells to determine whether such measurements are useful for characterizing heterogeneous cell populations. Fluorescein was introduced into cells by incubation with FDA. Measurements of the intensity of fluorescence (TI) and polarization (P) revealed an unexpected dependence: P decreased with increasing intensity of fluorescence. This may be accounted for by the classical model of the binding of small molecules to protein in which P is dependent on the ratio bound to unbound molecules. We have been able to estimate the quenching due to binding and construct a Scatchard plot. We estimated a wavelength shift from in vitro data consistent with the dependence of P on wavelength seen in our cell work. Generally, the distributions of P are symmetrical. Photon statistics broadens the P distribution of dim cells. However, structure does develop in the P distribution when the cells are deprived of calcium or incubated in the cold. This appears as a shoulder on the P distribution or resolves into two peaks. Calcium deprivation may differentially affect a subpopulation of cells whose significance remains to be explored in various cell types.     

Use of the green fluorescent protein and its mutants in quantitative fluorescence microscopy.

We have investigated properties relevant to quantitative imaging in living cells of five green fluorescent protein (GFP) variants that have been used extensively or are potentially useful. We measured the extinction coefficients, quantum yields, pH effects, photobleaching effects, and temperature-dependent chromophore formation of wtGFP, alphaGFP (F99S/M153T/V163A), S65T, EGFP (F64L/S65T), and a blue-shifted variant, EBFP (F64L/S65T/Y66H/Y145F). Absorbance and fluorescence spectroscopy showed little difference between the extinction coefficients and quantum yields of wtGFP and alphaGFP. In contrast, S65T and EGFP extinction coefficients made them both approximately 6-fold brighter than wtGFP when excited at 488 nm, and EBFP absorbed more strongly than the wtGFP when excited in the near-UV wavelength region, although it had a much lower quantum efficiency. When excited at 488 nm, the GFPs were all more resistant to photobleaching than fluorescein. However, the wtGFP and alphaGFP photobleaching patterns showed initial increases in fluorescence emission caused by photoconversion of the protein chromophore. The wtGFP fluorescence decreased more quickly when excited at 395 nm than 488 nm, but it was still more photostable than the EBFP when excited at this wavelength. The wtGFP and alphaGFP were quite stable over a broad pH range, but fluorescence of the other variants decreased rapidly below pH 7. When expressed in bacteria, chromophore formation in wtGFP and S65T was found to be less efficient at 37 degrees C than at 28 degrees C, but the other three variants showed little differences between 37 degrees C and 28 degrees C. In conclusion, no single GFP variant is ideal for every application, but each one offers advantages and disadvantages for quantitative imaging in living cells.     

Photobleaching. A novel fluorescence method for diffusion studies in lipid system.

(1) The fluorescent molecular 12(9-anthroyloxy)-stearic acid dimerises on irradiation with light of 366 nm wavelength. (2) The dimer is nonfluorescent and can be reconverted to the parent compound by irradiation at 254 nm. (3) Kinetic analysis suggests that the dimerisation proceeds by a diffusion-limited second order mechanism in many solvents. (4) Anomalously high rates seen in other systems can be attributed to localised high concentration regions (clusters) of the fluorescent molecule. (5) The analysis has been extended to oriented lipid bilayers and the results suggest that below the gel-liquid crystalline transition temperature the 12(9-anthroyloxy)-stearic acid is excluded by the lipid matrix and forms regions of localised high concentration. (6) In fluid lipid the results suggest an isotropic distribution of the probe. Calculated diffusion coefficients correspond to those found by other techniques.     

Time-resolved fluorescence microscopy.

In fluorescence microscopy, the fluorescence emission can be characterised not only by intensity and position, but also by lifetime, polarization and wavelength. Fluorescence lifetime imaging (FLIM) can report on photophysical events that are difficult or impossible to observe by fluorescence intensity imaging, and time-resolved fluorescence anisotropy imaging (TR-FAIM) can measure the rotational mobility of a fluorophore in its environment. We compare different FLIM methods: a chief advantage of wide-field time-gating and phase modulation methods is the speed of acquisition whereas for time-correlated single photon counting (TCSPC) based confocal scanning it is accuracy in the fluorescence decay. FLIM has been used to image interactions between proteins such as receptor oligomerisation and to reveal protein phosphorylation by detecting fluorescence resonance energy transfer (FRET). In addition, FLIM can also probe the local environment of fluorophores, reporting, for example, on the local pH, refractive index, ion or oxygen concentration without the need for ratiometric measurements.     

Dynamics of fluorescence dequenching of ostrich-quenched fluorescein biotin: a multifunctional quantitative assay for biotin

We describe a simple and rapid quantitative assay for biotin and biotin conjugates. The assay is based on the kinetic analysis of the enhancement of fluorescence of streptavidin/fluorescein biotin complexes in the presence of biotin. The kinetic response of fluorescence enhancement is proportional to the concentration of biotin. Standard calibration curves based on the kinetic response are obtained and detection limits of approximately 10(-9)M are established. Because the assay is amenable for use in small volumes of 5-50 microL or bead-based assays, the detection limits can be extended to the femtomole range. Since the assay depends on kinetic analysis, routine quantitation can be achieved without reference to standard curves. The dynamic aspects allow the assay to be extended to a broader range of applications including its use as an indicator of reagent mixing in laminar-flow assays carried out in microfluidic devices.     

Mapping fluorophore distributions in three dimensions by quantitative multiple angle-total internal reflection fluorescence microscopy.

The decay of evanescent field intensity beyond a dielectric interface depends upon beam incident angle, enabling the 3-d distribution of fluorophores to be deduced from total internal reflection fluorescence microscopy (TIRFM) images obtained at multiple incident angles. Instrumentation was constructed for computer-automated multiple angle-TIRFM (MA-TIRFM) using a right angle F2 glass prism (n(r) 1.632) to create the dielectric interface. A laser beam (488 nm) was attenuated by an acoustooptic modulator and directed onto a specified spot on the prism surface. Beam incident angle was set using three microstepper motors controlling two rotatable mirrors and a rotatable optical flat. TIRFM images were acquired by a cooled CCD camera in approximately 0.5 degree steps for >15 incident angles starting from the critical angle. For cell studies, cells were grown directly on the glass prisms (without refractive index-matching fluid) and positioned in the optical path. Images of the samples were acquired at multiple angles, and corrected for angle-dependent evanescent field intensity using "reference" images acquired with a fluorophore solution replacing the sample. A theory was developed to compute fluorophore z-distribution by inverse Laplace transform of angle-resolved intensity functions. The theory included analysis of multiple layers of different refractive index for cell studies, and the anisotropic emission from fluorophores near a dielectric interface. Instrument performance was validated by mapping the thickness of a film of dihexyloxacarbocyanine in DMSO/water (n(r) 1.463) between the F2 glass prism and a plano-convex silica lens (458 mm radius, n(r) 1.463); the MA-TIRFM map accurately reproduced the lens spherical surface. MA-TIRFM was used to compare with nanometer z-resolution the geometry of cell-substrate contact for BCECF-labeled 3T3 fibroblasts versus MDCK epithelial cells. These studies establish MA-TIRFM for measurement of submicroscopic distances between fluorescent probes and cell membranes.     

A restaining method to restore faded fluorescence in tissue specimens for quantitative confocal microscopy.

The aim of this study was to develop a procedure to remove the TO-PRO-3 fluorescent dye from tissue sections and restain with TO-PRO-3, still allowing calculation of DNA content and distribution by confocal laser scanning microscopy (CLSM). This would allow repeated measurements on the same tissue sections and prevents loss of tissue material from valuable clinical samples. Thick sections (14 microm) were cut from a paraffin block of adrenal tissue and stained using TO-PRO-3. Image stacks were acquired by CLSM. Thereafter, three destaining approaches were tested based on incubation, at different temperatures and durations, in the medium that is normally used to dissolve TO-PRO-3. The same areas were imaged again to measure residual fluorescence and were subsequently restained and imaged again. The intensity of the images acquired after initial staining and restaining were compared. A number of 3-D (texture) features computed after segmentation of nuclei were compared as well. The best destaining result was obtained by incubation of sections at 37 degrees C in preheated medium twice for 20 min. On average, the 3-D feature values were comparable with those after initial staining. With the described protocol it is possible to remove TO-PRO-3 fluorescence from tissue sections that can successfully be restained with minimal influence on fluorescence intensity and nuclear chromatin distribution.     

Extended resolution fluorescence microscopy.

Fluorescence microscopy is an essential tool of modern biology, but, like all forms of optical imaging, it is subject to physical limits on its resolving power. In recent years, several exciting techniques have been introduced to exceed these limits, including standing wave microscopy, 4Pi confocal microscopy, I5M and structured illumination microscopy. Several such techniques have been definitively demonstrated for the first time during the past year.     

Intracellular oxygen measurements of mouse liver cells using quantitative fluorescence video microscopy

Our currently developed fluorescence video microscope can measure fluorescence intensities with an error of ±1.5% of full scale in 65 536 different positions of a microscope field. With a video frame freeze acquisition time of 33 ms, time-dependent changes of this order of time or slower can be followed. Using cells which have absorbed pyrene-1-butyrate to an intracellular concentration of 0.05 to 1 mM, the changes in fluorescence intensity with oxygen concentration are easily measured. The spatial resolution for data collection is 0.5 μm when a 54X objective is used. The individual Stern-Volmer quenching constants of each individual pixel were measured for agar slices and mouse liver cells treated with pyrenebutyric acid. The distribution of quenching constants for agar follows a normal curve about a mean value of 16 · 10^?4 torr^?1. The data for mouse liver cells gave a non-normal distribution of quenching constants with a mean value of 18 · 10^?4 torr^?1. The greater spread of the data from cells is interpreted as evidence for a real biological variation in the solubility coefficent of oxygen in different locations within the cell. In all the cells examined, this distribution has been observed to be non-random and appears to be associated with specific cell structures.     

Identification of riboflavin transport by MDCK cells using quantitative fluorescence video microscopy

Summary MDCK cells, when examined by low-light level video microscopy displayed an endogenous fluorescence with two differing patterns. A low intensity emission which was punctate and associated with cell organelles was observed with emission and excitation conditions generally used to observe either fluorescein (450–500 nm excitation/>510 nm emission) or rhodamine (514 nm excitation/>530 emission) type dyes. A second 5- to 10-fold brighter emission for 450–500 nm excitation was observed, which was unusual in that each cell appeared to be outlined. Evidence obtained from spectroscopy and from using culture media of altered composition supported the conclusion that the water-soluble vitamin riboflavin accumulated in the basolateral spaces and fluid-filled domes and was the source of this fluorescent emission. Quantitative measurements showed that exposure to cultures to 10 m riboflavin resulted in accumulation in domes of 565±80 m. The transport rate was calculated to be 189±30 pmol/min-cm². Onemm probenecid, a known inhibitor of riboflavin transport in vivo, reduced transport to 54% of control, while 10mm nearly abolished the uptake. The results demonstrate that removal of riboflavin reduces MDCK cell fluorescence to levels compatable with low-light level imaging. Furthermore, these cells actively transport riboflavin and provide a new in vitro model for this process.     

Direct determination of free fatty acid transport across the adipocyte plasma membrane using quantitative fluorescence microscopy.

Movement of free fatty acids (FFA) across the plasma membrane has been directly measured for the first time, using fluorescent FFA analogs and quantitative fluorescence microscopy. The rate of short chain FFA (less than or equal to 12 carbons) transport from the extracellular medium into intracellular lipid droplets of 3T3F442A adipocytes was more than 40-fold faster than long chain FFA (16 and 18 carbons). The membrane-impermeable amino reagent 4,4'-diisothiocyanostilbene-2,2'-disulfonate, inhibited greater than or equal to 50% of the long chain FFA transport but had no effect on short chain FFA transport. Oleic acid (2 microM) inhibited 90% of the fluorescent oleate transport but had no effect on the 11-carbon analog. These results indicate that a large fraction of long chain FFA uptake is mediated by a plasma membrane protein (s).     

Quantitative fluorescence resonance energy transfer measurements using fluorescence microscopy.

Fluorescence resonance energy transfer (FRET) is a technique used for quantifying the distance between two molecules conjugated to different fluorophores. By combining optical microscopy with FRET it is possible to obtain quantitative temporal and spatial information about the binding and interaction of proteins, lipids, enzymes, DNA, and RNA in vivo. In conjunction with the recent development of a variety of mutant green fluorescent proteins (mtGFPs), FRET microscopy provides the potential to measure the interaction of intracellular molecular species in intact living cells where the donor and acceptor fluorophores are actually part of the molecules themselves. However, steady-state FRET microscopy measurements can suffer from several sources of distortion, which need to be corrected. These include direct excitation of the acceptor at the donor excitation wavelengths and the dependence of FRET on the concentration of acceptor. We present a simple method for the analysis of FRET data obtained with standard filter sets in a fluorescence microscope. This method is corrected for cross talk (any detection of donor fluorescence with the acceptor emission filter and any detection of acceptor fluorescence with the donor emission filter), and for the dependence of FRET on the concentrations of the donor and acceptor. Measurements of the interaction of the proteins Bcl-2 and Beclin (a recently identified Bcl-2 interacting protein located on chromosome 17q21), are shown to document the accuracy of this approach for correction of donor and acceptor concentrations, and cross talk between the different filter units.     

Enumeration of Archaea and Bacteria in seafloor basalt using real-time quantitative PCR and fluorescence microscopy

A SYBR Green real-time quantitative PCR (Q-PCR) assay for the detection and quantification of Bacteria and Archaea present in the glassy rind of seafloor basalts of different ages and water depths is presented. Two sets of domain-specific primers were designed and validated for specific detection and quantification of bacterial and archaeal 16S rRNA genes in DNA extracted from basaltic glass. Total cell numbers were also estimated by fluorescence microscopy analysis of SYBR Gold-stained samples. The results from the two different approaches were concurrent, and Q-PCR results showed that the total number of cells present in basalts was in the range from 6 x 10(5) to 4 x 10(6) cells g(-1) basaltic glass. Further, it was demonstrated that these cells were almost exclusively from the domain Bacteria. When applying the same methods on samples of different ages (22 years-0.1 Ma) and water depths (139-3390 mbsl), no significant differences in cell concentrations or in the relative abundance of Archaea and Bacteria were detected.