Dual-laser flow cytometry of single mammalian cells.

An improved dual-laser flow cytometric system for quantitative analysis and sorting of mammalian cells has been developed using a low-power argon and high-power krypton laser as illumination sources, thus permitting the excitation of fluorescent dyes having absorption regions ranging from the ultraviolet to infrared. Cells stained in liquid suspension with fluorescent dyes enter a flow chamber where they intersect two spatially separated laser beams. Separate pairs of quartz beam-shaping optics focus each beam onto the cell stream. Electro-optical sensors measure fluorescence and light scatter signals from cells that are processed electronically and displayed as frequency distribution histograms. Cells also can be electronically separated and microscopically identified. The ease and versatility of operation designed into this system represent a marked technological improvement for dual-laser excited flow systems. Details of this instrument are described along with illustrative examples of cells stained with mithramycin and rhodamine and analyzed for DNA content, total protein, and nuclear and cytoplasmic diameter.     

A high efficiency flow cytometer.

A flow chamber has been developed which collects about 60% of the total cell fluorescence for analysis compared to about 2.5% for conventional flow systems. The chamber, an ellipsoid of revolution, is gold-plated for increased reflectivity. Fluorochrome-stained cells enter the flow cell directly above the primary focus of the ellipsoid at the rate of 1000 cell/sec. A focused argon-ion laser beam enters the flow cell parallel to the semiminor axis and intersects the cell stream at the primary focus. Fluorescent light emanating from this point is reflected toward the secondary focus, where it exits the chamber for analysis. The high efficiency flow cytometer has been used to obtain nucleotide fluorescence distributions from samples of Micrococcus glutamicus bacteria stained with propidium iodide and of spermatozoa stained by the acriflavine-Feulgen procedure.     

A new multiparameter flow cytometer: optical and electrical cell analysis in combination with video microscopy in flow

BACKGROUND: Flow cytometers, which are commercially available, do not necessarily meet all demands of actual biomedical research. This is the case for the investigation of mechanisms involved in cell volume regulation, which requires electrical volume measurement and ratiometric multichannel fluorescence analysis for the simultaneous assessment of different physiologic parameters (intracellular pH and the intracellular concentration of calcium ions, etc). METHODS AND RESULTS: We describe the construction of a new nonsorting flow cytometer designed for the simultaneous acquisition of seven parameters including fluorescence signals, forward and perpendicular light scatter, cell volume according to the electrical Coulter principle, and flow cytometric imaging. The instrument is equipped with three different light sources. A tunable argon-ion laser generates efficient excitation of the most standard fluorescent probes in the visible spectral range, and an arc lamp provides the means for ultraviolet excitation at low cost. Because of the spatial filtering by the excitation and detection optics, two independent sets of dual fluorescence measurements can be performed, a prerequisite for flexible ratiometric fluorescence analysis. A flow video microscope integrated into the optical system optionally generates either brightfield or phase images of selected flowing particles. Only particles whose individual datasets meet predefined gating conditions are imaged in real time. To avoid smear effects, the motion of the object to be imaged (speed approximately 8 m/s) is frozen on the target of a CCD camera by flash illumination. For this purpose, a high radiance gas discharge lamp with 25-mJ electric pulse energy provides an illumination time of 18 ns (full width half maximum). Test results obtained from latex spheres and cells are shown. CONCLUSIONS: Test results indicate that our instrument can perform Coulter measurements in combination with flexible optical analysis. Moreover, integration of an adapted video microscope into a flow cytometer is an approach to overcome the gap between flow and image cytometry.     

EMOSS: an epiillumination microscope objective slit-scan flow system

An epiillumination microscope objective slit-scan flow system has been fabricated utilizing two dimensional slit scanning with hydrodynamic sample stream focussing. Low resolution (4 micron) analysis of cellular fluorescence is facilitated by the definition of a stabilized flow plane through hydrodynamic focussing. Coincidence of the region of stabilized flow with the focal plane of the microscope objective will allow for the collection and subsequent imaging of fluorescence from cells oriented along this plane. Two orthogonal slit-scan contours are generated as a cell traverses the excitation region. It is hoped that the need for a three dimensional system will be precluded by preferential orientation of the cells in the region of stabilized flow. Cellular fluorescence is collected by a high numerical aperture epiillumination optical system and imaged onto two orthogonal slits. Two photomultiplier tubes are used to detect fluorescence. It is anticipated that the epiillumination microscope objective slit-scan flow system will be used with a variety of fluorescent stains and markers, as well as extended to the research of light scattered by cells. (Steen, H.B., Cytometry 1:26-31, 1980.     

Cortical Actin Flow in T Cells Quantified by Spatio-temporal Image Correlation Spectroscopy of Structured Illumination Microscopy Data

Filamentous-actin plays a crucial role in a majority of cell processes including motility and, in immune cells, the formation of a key cell-cell interaction known as the immunological synapse. F-actin is also speculated to play a role in regulating molecular distributions at the membrane of cells including sub-membranous vesicle dynamics and protein clustering. While standard light microscope techniques allow generalized and diffraction-limited observations to be made, many cellular and molecular events including clustering and molecular flow occur in populations at length-scales far below the resolving power of standard light microscopy. By combining total internal reflection fluorescence with the super resolution imaging method structured illumination microscopy, the two-dimensional molecular flow of F-actin at the immune synapse of T cells was recorded. Spatio-temporal image correlation spectroscopy (STICS) was then applied, which generates quantifiable results in the form of velocity histograms and vector maps representing flow directionality and magnitude. This protocol describes the combination of super-resolution imaging and STICS techniques to generate flow vectors at sub-diffraction levels of detail. This technique was used to confirm an actin flow that is symmetrically retrograde and centripetal throughout the periphery of T cells upon synapse formation.     

Flow cytometry of bacteria: a promising tool in experimental and clinical microbiology

The DNA and protein content of individual Escherichia coli cells were measured at a rate of 10(4) cells per second with a sensitive microscope-based flow cytometer. DNA and protein were quantified by measuring the fluorescence from cells stained with a combination of the DNA-binding drugs Mithramycin and ethidium bromide and by scattered light, respectively. Separate experiments demonstrated that the light scatter signal was proportional to protein content. Dual parameter histograms (fluorescence/scattered light) of bacterial cultures gave detailed pictures of changes dependent upon the growth conditions and of the cell cycle kinetics. Effects of antibiotics could be readily detected and characterized after a few hours. The results demonstrate that flow cytometry is a promising method for application in experimental and clinical microbiology.     

STRESS‐INDUCED FILAMENT FRAGMENTATION OF CALOTHRIX ELENKINII (CYANOBACTERIA) IS FACILITATED BY DEATH OF HIGH‐FLUORESCENCE CELLS1

Irradiance power and spectral composition as well as nutrient availability strongly influence differentiation of filamentous cyanobacteria. When monitoring the life cycle of Calothrix elenkinii Kossinsk., we found that low nitrogen concentration and growth under green light led to a transient appearance of high‐fluorescence cells that rapidly bleach and disintegrate, thus breaking the parental filament into shorter parts. The dynamics of the process were monitored in a microscope growth chamber by measuring transmission and chl fluorescence of individual cells by a high‐sensitivity camera. Typically, the high‐fluorescence cells appeared near the center of the parental trichome signaled by a rapid 2‐ to 3‐fold rise in their fluorescence emission. By measuring the fluorescence excitation spectra with resolution of individual cells, we showed that the elevated fluorescence emission was largely due to a high absorption by phycoerythrin and energy transfer to chl. Typically, after no more than 20 min, the fluorescence abruptly disappeared with transmission images, indicating loss of pigmentation. The bleaching was a natural process that was not caused by the measuring light. Depending on the mechanical strain, the cell bleaching was followed by breaking of the parental filament. We propose that the high‐fluorescence cells appear as a phase of programmed cell death, allowing the fragmented filaments to escape from unfavorable environmental conditions.     

In situ microscopy for on-line determination of biomass

A sensor is presented, which allows on-line microscopic observation of microorganisms during fermentations in bioreactors. This sensor, an In Situ Microscope (ISM) consists of a direct-light microscope with a measuring chamber, integrated in a 25 mm stainless steel tube, two CCD-cameras, and two frame-grabbers. The data obtained are processed by an automatic image analysis system. The ISM is connected with the bioreactor via a standard port, and it is immersed directly in the culture liquid-in our case Saccharomyces cerevisiae in a synthetic medium. The microscopic examination of the liquid is performed in the measuring chamber, which is situated near the front end of the sensor head. The measuring chamber is opened and closed periodically. In the open state, the liquid in the bioreactor flows unrestricted through the chamber. In closing, a defined volume of 2,2. 10(-8) mL of the liquid becomes enclosed. After a few seconds, when the movement of the cells in the enclosed culture has stopped, they are examined with the microscope. The microscopic images of the cells are registered with the CCD-cameras and are visualized on a monitor, allowing a direct view of the cell population. After detection, the measuring chamber reopens, and the enclosed liquid is released. The images obtained are evaluated as to cell concentration, cell size, cell volume, biomass, and other relevant parameters simultaneously by automatic image analysis. With a PC (486/33 MHz), image processing takes about 15 s per image. The detection range tested when measuring cells of S. cerevisiae is about 10(6) to 10(9) cells/mL (equivalent to a biomass of 0.01 g/L to 12 g/L). The calculated biomass values correlate very well with those obtained using dry weight analysis. Furthermore, histograms can be calculated, which are comparable to those obtained by flow cytometry.     

Multiple wavelength illumination in flow cytometry using a single arc lamp and a dispersing element

The principle of a multiple wavelength illumination method for flow cytometers, based upon a combination of a helium-neon laser and an arc lamp as illumination sources is described. By using a prism, the light from the arc lamp is dispersed and the different colors are imaged at different places on the sample stream. The small angle light scattering from the helium-neon laser light is measured as a relevant parameter and serves as a trigger signal for subsequent measurements of fluorescence or scattering of light from the arc lamp. Two experimental systems are described utilizing this principle: a system where the emission is detected orthogonally with respect to the direction of the illumination beams, and an epi-illumination system. With the orthogonal set-up multiple wave-length right angle scattering measurements are possible. This is illustrated by showing that the orthogonal scattering from erythrocytes is strongly dependent on the illumination wavelength. It is further shown that the apparatus is suitable for the measurement of intracellular pH using the pH dependence of the excitation spectrum of fluorescein. The epi-illumination system allows excitation of two (or more) fluorescent dyes with different excitation spectra. In this case the emission spectra of the fluorescent dyes may overlap substantially. This is shown by simultaneous measurement of DNA and protein of Chinese hamster lung cells using mitramycin and tetramethyl rhodamin isothiocyanate (TRITC).     

Eliminating Unwanted Far-Field Excitation in Objective-Type TIRF. Part I. Identifying Sources of Nonevanescent Excitation Light

Total internal reflection fluorescence microscopy (TIRFM) achieves subdiffraction axial sectioning by confining fluorophore excitation to a thin layer close to the cell/substrate boundary. However, it is often unknown how thin this light sheet actually is. Particularly in objective-type TIRFM, large deviations from the exponential intensity decay expected for pure evanescence have been reported. Nonevanescent excitation light diminishes the optical sectioning effect, reduces contrast, and renders TIRFM-image quantification uncertain. To identify the sources of this unwanted fluorescence excitation in deeper sample layers, we here combine azimuthal and polar beam scanning (spinning TIRF), atomic force microscopy, and wavefront analysis of beams passing through the objective periphery. Using a variety of intracellular fluorescent labels as well as negative staining experiments to measure cell-induced scattering, we find that azimuthal beam spinning produces TIRFM images that more accurately portray the real fluorophore distribution, but these images are still hampered by far-field excitation. Furthermore, although clearly measureable, cell-induced scattering is not the dominant source of far-field excitation light in objective-type TIRF, at least for most types of weakly scattering cells. It is the microscope illumination optical path that produces a large cell- and beam-angle invariant stray excitation that is insensitive to beam scanning. This instrument-induced glare is produced far from the sample plane, inside the microscope illumination optical path. We identify stray reflections and high-numerical aperture aberrations of the TIRF objective as one important source. This work is accompanied by a companion paper (Pt.2/2).     

Eliminating Unwanted Far-Field Excitation in Objective-Type TIRF. Part I. Identifying Sources of Nonevanescent Excitation Light

Total internal reflection fluorescence microscopy (TIRFM) achieves subdiffraction axial sectioning by confining fluorophore excitation to a thin layer close to the cell/substrate boundary. However, it is often unknown how thin this light sheet actually is. Particularly in objective-type TIRFM, large deviations from the exponential intensity decay expected for pure evanescence have been reported. Nonevanescent excitation light diminishes the optical sectioning effect, reduces contrast, and renders TIRFM-image quantification uncertain. To identify the sources of this unwanted fluorescence excitation in deeper sample layers, we here combine azimuthal and polar beam scanning (spinning TIRF), atomic force microscopy, and wavefront analysis of beams passing through the objective periphery. Using a variety of intracellular fluorescent labels as well as negative staining experiments to measure cell-induced scattering, we find that azimuthal beam spinning produces TIRFM images that more accurately portray the real fluorophore distribution, but these images are still hampered by far-field excitation. Furthermore, although clearly measureable, cell-induced scattering is not the dominant source of far-field excitation light in objective-type TIRF, at least for most types of weakly scattering cells. It is the microscope illumination optical path that produces a large cell- and beam-angle invariant stray excitation that is insensitive to beam scanning. This instrument-induced glare is produced far from the sample plane, inside the microscope illumination optical path. We identify stray reflections and high-numerical aperture aberrations of the TIRF objective as one important source. This work is accompanied by a companion paper (Pt.2/2).     

Flat-top illumination profile in an epifluorescence microscope by dual microlens arrays

Low uniformity in illumination across the image plane impairs the ability of a traditional epifluorescence microscope to quantify fluorescence intensities. Two microlens arrays (MLAs) were introduced into the illumination path of two different epifluorescence microscope systems to improve the uniformity of the illumination. Measurements of the uniformity of illumination were performed with a CCD camera in the focal plane and with fluorescent beads in the image plane. In semi critical alignment, a uniformity of illumination of 15-23% was found compared with 1-2% in the modified system. Coefficient of variation (CV) of fluorescent beads measured on the unmodified system was 20.4% ± 5.3% in semi critical alignment and 10.8% ± 1.3% in Koehler alignment. On the MLA systems, CV was 7.9% ± 2.0% and on a flow cytometer, the CV was 6.7% ± 0.7%. Implementation of MLAs in an epifluorescence microscope improves the uniformity of illumination, thereby reducing the variation in detection of fluorescent signals of the measured objects and becomes equivalent to that of flow cytometry.     

Fluorescence spectroscopy for detection of malignancy: H-ras overexpressing fibroblasts as a model.

Autofluorescence from intracellular chromophores upon illumination of cells by monochromatic light has been studied towards the development of novel noninvasive and sensitive technology for the early detection of cancer. To investigate the relationship between biochemical and morphological changes underlying malignant disease and resulting fluorescence spectra, an in vitro model system of a paired normal and malignant murine fibroblasts cell lines, differing in cancer-associated H-ras expression was employed. A comparison of fluorescence excitation and emission spectra of proliferative cells revealed that fluorescence intensity of malignant cells was significantly less than that of normal cells upon excitation at 290 nm. Fluorescence of both cell lines decreased with decreasing cell concentration, but at each concentration, normal cells had higher fluorescence intensity than malignant cells. Similar differences between the cell lines were observed when brought to quiescence or at stationary phase. Results suggested that the chromophore contributing most significantly to these spectra is tryptophan and its moieties in proteins. This model system demonstrates the specific contribution of H-ras to subcellular chromophores, resulting in a significant difference in their autofluorescence intensity, and implies the potential use of the technique for cancer detection. This model system is potent for analysis of the contribution of other oncogenes and their combinations towards spectral detection of cancer.     

Fluorescence intensity resolution in flow systems.

The factor which can limit fluorescence intensity resolution in a flow cytometer of the type in which cells pass perpendicularly through a focussed laser beam depends on signal intensity. For the brightest sources (e.g. fluorescent DNA stains), the coefficient of variation (CV) is limited in our system to around 3% by stream hydrodynamics, unstable illumination intensity, nonstoichiometric staining, etc. The weakest detectable sources (e.g. fluorescent cell-surface labels) are limited in coefficient of variation by shot noise in the photomultiplier due to constant background light levels. Finally, over a fairly wide brightness range between these extremes, resolution is determined primarily by photoelectron statistical variation on the signal itself (i.e. "photon statistics"). Thus photon collection and detection efficiency (solid angle, barrier filter passband, detector quantum efficiency) become of primary importance.     

Flow cytometry chamber with 4 pi light collection suitable for epifluorescence microscopes

A compact, solid, spherico-ellipsoidal chamber (SEC), which has approaching 4 pi ("all around") light collection, has been developed for flow cytometry. This was mounted onto the stage of a standard fluorescence photomicroscope, and the camera was replaced by a photomultiplier. Both components can be added or removed in minutes. The increased light collection efficiency of the SEC (about 85%) compared with about 4% from standard chambers enabled a fluorescence microscope with a 50 W mercury vapour lamp to "double" as a flow cytometer. The system was tested with microbeads and cells stained for DNA with ethidium bromide, and results were comparable to those obtained with our laser-based instrument.     

Coefficient of variation in flow cytometry of phagocytosis

Fluorescence histograms of V79 Chinese hamster lung cells containing phagocytized fluorescent microspheres were measured by flow cytometry. In the fluorescence histograms, the coefficient of variation (CV) of the peak for cells ingesting microspheres was not constant. Rather, it decreased with the number of microspheres ingested by the cells.     

Fluorescence and oxygen evolution from Chlorella pyrenoidosa

The process of photosynthetic energy conversion in Chlorella pyrenoidosa was investigated by simultaneous measurement of transient and steady-state rates of O₂ evolution and fluorescence.

1. 1. Alternation or superimposition of light 1 and light 2 illumination induces both fast and slow changes in fluorescence and rate of O₂ evolution. The fast changes are ascribed to changes in conditions of the reaction centers in the context of the ¹ model and the kinetic analysis of ². The slow changes are interpreted as adaptations to the intensity and wavelength of illumination. The adaptive mechanism is described in terms of slow variation in fraction () of total absorbed quanta delivered to System 2. At low intensities, the calculated value of for cells adapted to light 2 illumination (light 2 state) is approx. 0.9 of for cells adapted to light 1 illumination (light 1 state).

2. 2. An increase in fluorescence yield was found to accompany the decrease in O₂ yield at the onset of light saturation with either light 1 or light 2 excitation. Variation in is proposed to account for the differences between the maximum fluorescence yield observed in steady-state conditions and the 1.5 times higher maximum yield observed in transient conditions or in cells inhibited by 3(3,4-dichlorophenyl)-1,1-dimethylurea. Variation in can also explain the observation of a higher rate of fluorescence emission with light 1 excitation than with light 2 excitation for a given steady-state rate of O₂ evolution.

3. 3. A model for energy conversion by System 2 is proposed to account for our observations. The model proposes competitive dissipation of absorbed energy by photochemical trapping at reaction centers and by fluorescence and radiationless de-excitation from both the pigment bed and reaction centers of System 2.

THE USE of FLOW CYTOMETRY FOR RAPID IDENTIFICATION of SALMONELLAE

Flow cell cytometry can be used in a sensitive fluorescent immunoassay to rapidly identify salmonellae of Groups D and E. Staphylococcal Protein A couples with the Fc region of many antibodies, especially immunoglobulin G. When a fluorescent marker, fluorescein isothiocyanate, is conjugated to Protein A, an antibody-antigen reaction can be visualized in a flow cell cytometer with an appropriate optical sensor after excitation. Ten thousand cells were individually analyzed in each cytometer run within a minute. the resultant data, presented as histograms and tables, indicated the number of cells in the suspension reacting positively with the antiserum by fluorescence, cell size, distribution and light scatter. This provides an in-depth analysis of the antibody-antigen reaction not possible with other types of immunoassays.     

Variable incidence angle fluorescence interference contrast microscopy for z-imaging single objects

Surface-generated structured illumination microscopies interrogate the position of fluorescently labeled objects near surfaces with nanometer resolution along the z axis. However, these techniques are either experimentally cumbersome or applicable to a limited set of experimental systems. We present a new type of surface-generated structured illumination fluorescence microscopy, variable incidence angle fluorescence interference contrast microscopy (VIA-FLIC), in which the fluorescent sample is assembled above a reflective Si surface and the incidence angle of excitation light is varied by placing annular photomasks with different radii in the aperture diaphragm plane of the microscope. The variation in incidence angle alters the interference pattern of excitation light, and hence the intensity of detected fluorescence. Quantitative VIA-FLIC is tested by using a set of fluorophore-containing supported membranes separated from the Si surface by SiO2 layers of variable thicknesses. The resulting fluorescence intensity versus incidence angle curves depends on the separation from the Si surface and when fit with an appropriate model yield precise SiO2 thicknesses that are accurate with respect to the known SiO2 thicknesses. Since only a simple modification to a standard epifluorescence microscope is required, VIA-FLIC offers a versatile method to produce z-reconstructions with high resolution for a wide range of biological systems.     

Polarization-Controlled TIRFM with Focal Drift and Spatial Field Intensity Correction

Total internal reflection fluorescence microscopy (TIRFM) is becoming an increasingly common methodology to narrow the illumination excitation thickness to study cellular process such as exocytosis, endocytosis, and membrane dynamics. It is also frequently used as a method to improve signal/noise in other techniques such as in vitro single-molecule imaging, stochastic optical reconstruction microscopy/photoactivated localization microscopy imaging, and fluorescence resonance energy transfer imaging. The unique illumination geometry of TIRFM also enables a distinct method to create an excitation field for selectively exciting fluorophores that are aligned either parallel or perpendicular to the optical axis. This selectivity has been used to study orientation of cell membranes and cellular proteins. Unfortunately, the coherent nature of laser light, the typical excitation source in TIRFM, often creates spatial interference fringes across the illuminated area. These fringes are particularly problematic when imaging large cellular areas or when accurate quantification is necessary. Methods have been developed to minimize these fringes by modulating the TIRFM field during a frame capture period; however, these approaches eliminate the possibility to simultaneously excite with a specific polarization. A new, to our knowledge, technique is presented, which compensates for spatial fringes while simultaneously permitting rapid image acquisition of both parallel and perpendicular excitation directions in ∼25 ms. In addition, a back reflection detection scheme was developed that enables quick and accurate alignment of the excitation laser. The detector also facilitates focus drift compensation, a common problem in TIRFM due to the narrow excitation depth, particularly when imaging over long time courses or when using a perfusion flow chamber. The capabilities of this instrument were demonstrated by imaging membrane orientation using DiO on live cells and on lipid bilayers that were supported on a glass slide (supported lipid bilayer). The use of the approach to biological problems was illustrated by examining the temporal and spatial dynamics of exocytic vesicles.