In vitro confocal imaging of the rabbit cornea

We were able to observe in vitro the fine structure of the rabbit cornea using a laser scanning confocal microscope, especially in the regions between Descemet's membrane and the epithelial basal lamina. We observed submicrometre filaments throughout the stroma with high concentrations adjacent to Descemet's membrane, and found extensive interconnecting processes between stromal keratocytes. There are numerous regions containing nerve plexuses in the stroma. We found a deeply convoluted basal lamina adjacent to the epithelium, and observed regions containing junctions between endothelial cells in fluorescent images of rabbit corneas stained with the actin-specific compound fluorescein phalloidin.     

Observation of the retina using the tandem scanning confocal microscope

A tandem scanning confocal microscope (TSCM) is currently being used to obtain high-resolution images of the human cornea in vivo. Advantages of confocal microscopy for in vivo imaging include optical sectioning and increased contrast through removal of scattered light. We have adapted the TSCM to view the retina in vivo by constructing an applanating lens and fitting the microscope with an imaging-intensifying camera of increased sensitivity. The microscope uses a spinning disc with 40,000 holes, each of 30 microns diameter, and a 100 W mercury arc lamp light source with a 455 nm long pass filter. The applanating lens is composed of three elements, two of which are movable for focusing. Images of a rabbit retina were obtained in vivo revealing the nerve fiber layer and blood vessels around the optic disc. The power density at the retina was calculated to be 3 mW/cm², which is well below the power levels of a direct or indirect ophthalmoscope. Magnification of the retinal image was approximately 60x and a 1 mm wide area of retina was in view. This prototype TSCM system demonstrates that images of a retina in vivo are obtainable with confocal microscopy and that the sharpness is comparable to standard fundus camera photography. Further modifications to improve the light level and alterations in the design of the objective should improve the quality of the images obtained and achieve the enhanced resolution of which, in theory, the confocal microscope is capable.     

Three-dimensional imaging of corneal cells using in vivo confocal microscopy

Confocal microscopy is a unique and powerful imaging paradigm which allows optical sectioning through intact tissue. Real-time tandem scanning confocal microscopy has previously been used to generate high-magnification two-dimensional (2-D) images of cells in living organ systems. Inherent problems with movement, however, have prevented the in vivo acquisition of complete 3-D datasets. The development of a new objective lens, used in combination with specialized real-time image acquisition procedures, has allowed sequential serial sections to be obtained in vivo from the rabbit cornea for the first time. These sections can be digitially registered and stacked on the computer to provide a 3-D reconstruction of the corneal cells. This technique should serve as a useful method for studying 3-D structures and analysing 4-D phenomena at the cellular level in living animals. Three-dimensional images of a stromal nerve in normal rabbit cornea and of fibroblasts within a rabbit corneal wound are presented as examples of current capabilities.     

Comparison of in vivo and ex vivo cellular structure in rabbit eyes detected by tandem scanning microscopy

Using the tandem scanning microscope, in vivo confocal microscopic images of living eyes were compared to images obtained from ex vivo, freshly enucleated or fixed tissue in the rabbit. In the normal cornea, microscopic details of the superficial epithelium, basal lamina, stromal fibrocyte nuclei, nerves and endothelial cell borders were easily discernible. Removal of the eye from the intact animal resulted in loss of detail with distortion of the normal structural interrelationships within the corneal stroma whilst enhancing details of the corneal epithelium. Formalin fixation further enhanced details of the basal and suprabasal corneal epithelial cell nuclei and the stromal fibrocyte cell borders whilst inducing prominent brightly reflecting folds in the thickened stroma with concomitant enhancement of the edge contrast of the collagen lamellae. These changes appeared to be related, in part, to hydration of the cornea and artefactual pooling of water between structures that may enhance reflectivity by increasing the difference between the refractive index of the cellular and extracellular elements. We conclude that microscopic examination of ex vivo preparations of corneal tissue, although providing increased resolution similar to conventional light microscopic techniques, significantly altered the normal structural relationships and could lead to erroneous measurements of the physiological properties of the tissue as compared to in vivo microscopy of undisturbed, intact tissue.     

Development of a standing-wave fluorescence microscope with high nodal plane flatness

This article reports about the development and application of a standing-wave fluorescence microscope (SWFM) with high nodal plane flatness. As opposed to the uniform excitation field in conventional fluorescence microscopes an SWFM uses a standing-wave pattern of laser light. This pattern consists of alternating planar nodes and antinodes. By shifting it along the axis of the microscope a set of different fluorescent structures can be distinguished. Their axial separation may just be a fraction of a wavelength so that an SWFM allows distinction of structures which would appear axially unresolved in a conventional or confocal fluorescence microscope. An SWFM is most powerful when the axial extension of the specimen is comparable to the wavelength of light. Otherwise several planes are illuminated simultaneously and their separation is hardly feasible. The objective of this work was to develop a new SWFM instrument which allows standing-wave fluorescence microscopy with controlled high nodal plane flatness. Earlier SWFMs did not allow such a controlled flatness, which impeded image interpretation and processing. Another design goal was to build a compact, easy-to-use instrument to foster a more widespread use of this new technique. The instrument developed uses a green-emitting helium–neon laser as the light source, a piezoelectric movable beamsplitter to generate two mutually coherent laser beams of variable relative phase and two single-mode fibres to transmit these beams to the microscope. Each beam is passed on to the specimen by a planoconvex lens and an objective lens. The only reflective surface whose residual curvature could cause wavefront deformations is a dichroic beamsplitter. Nodal plane flatness is controlled via interference fringes by a procedure which is similar to the interferometric test of optical surfaces. The performance of the instrument was tested using dried and fluorescently labelled cardiac muscle cells of rats. The SWFM enabled the distinction of layers of stress fibres whose axial separation was just a fraction of a wavelength. Layers at such a small distance would lie completely within the depth-of-field of a conventional or confocal fluorescence microscope and could therefore not be distinguished by these two methods. To obtain futher information from the SWFM images it would be advantageous to use the images as input-data to image processing algorithms such as conceived by Krishnamurthi et al. (Proc. SPIE, 2655, 1996, 18–25). To minimize specimen-caused nodal plane distortion, the specimen should be embedded in a medium of closely matched refractive index. The proper match of the refractive indices could be checked via the method presented here for the measurement of nodal plane flatness. For this purpose the fluorescent layer of latex beads would simply be replaced by the specimen. A combination of the developed SWFM with a specimen embedded in a medium of matched refractive index and further image processing would exploit the full potential of standing-wave fluorescence microscopy.     

Three-dimensionally resolved NAD(P)H cellular metabolic redox imaging of the in situ cornea with two-photon excitation laser scanning microscopy

Three-dimensional maps of cellular metabolic oxidation/reduction states of rabbit cornea in situ were obtained by imaging the fluorescence of the naturally occurring reduced pyridine nucleotides (both reduced nicotinamide-adenine dinucleotide, NADH, and reduced nicotinamide-adenine dinucleotide phosphate, NADPH, denoted here as NAD(P)H). Autofluorescence images with submicrometre lateral resolution were obtained throughout the entire 400 μm thickness of the cornea. Two-photon excitation scanning laser microscopy with near-infrared excitation provided high fluorescence collection efficiency, reduced photodamage, and eliminated ultraviolet chromatic aberration, all of which have previously degraded the visualization of pyridine nucleotide fluorescence. Sharp autofluorescence images of the basal epithelium (40 μm within the cornea) show substantial subcellular detail, providing the ability to monitor autofluorescence intensity changes over time, which reflect changes in oxidative metabolism and cellular dynamics necessary for maintenance of the ocular surface. The autofluorescence was confirmed to be mostly of NAD(P)H origin by cyanide exposure, which increased the fluorescence from all cell types in the cornea by about a factor of two. Autofluorescence images of individual keratocytes in the stroma were observed only after cyanide treatment, while in the predominant extracellular collagen (> 90% of the stromal volume), fluorescence was not distinguished from the background. Observation of keratocyte metabolism demonstrates the sensitivity made available by two-photon microscopy for future redox fluorescence imaging of cellular metabolic states.     

Observation of the rabbit cornea and lens with a new real-time confocal scanning optical microscope

A new one-sided tandem scanning microscope (OTSM) has been utilized to optically section a transparent cornea and ocular lens with submicron depth and transverse resolution. Its high resolution, image quality, and contrast, together with color capability, real-time operation, and easy alignment, have advantages over previous confocal systems. Planes within the nuclei of surface epithelial cells, the epithelial basement membrane, nerve fibers, the interior of endothelial cells, and the transverse structure of the lens fibers are readily observed. The utility of real-time microscopic observation of live biological structures provides a new paradigm for cell biology and diagnostic ophthalmology.     

Near real time in vivo fibre optic confocal microscopy: sub-cellular structure resolved

We have built a fibre optic confocal reflectance microscope capable of imaging biological tissue in near real time. The measured lateral resolution is 3 µm and axial resolution is 6 µm. Images of epithelial cells, excised tissue biopsies, and the human lip in vivo have been obtained at 15 frames s^?1. Both cell morphology and tissue architecture can be appreciated from images obtained with this microscope. This device has the potential to enable reflected light confocal imaging of internal organs for in situ detection of pathology.     

Potential of CLSM in studying some modern and fossil palynological objects

We have tested possibilities and limitations of confocal laser scanning microscopy to study the morphology of pollen and spores and inner structure of sporoderms. As test objects, we used pollen grains of the modern angiosperm Ribes niveum (Grossulariaceae) and Datura metel (Solanaceae), fossil angiosperm pollen grains of Pseudointegricorpus clarireticulatum and Wodehouseia spinata dated to the Late Cretaceous, fossil gymnosperm pollen grains of Cycadopites‐type dated to the Middle Jurassic, and fossil megaspores Maexisporites rugulaeferus, M. grosstriletus, and Trileites sp. dated to the Early Triassic. For comparative purpose, we studied the same objects with application of conventional light, scanning electron (to entire pollen grains and spores or to semithin sections of their walls), or transmission electron microscopy. The resolution of confocal microscope is much lower than that of electron microscopes, as are its abilities to reconstruct the surface patterns and inner structure. On the other hand, it can provide information that is unreachable by other microscopical methods. Thus, the structure of endoapertures in angiosperm pollen grains can be directly observed. It is also helpful in studies of asymmetrical pollen and pollen grains bearing various appendages and having complicated exine structure, because rotation of 3‐D reconstructions allows one to examine all sides and structures of the pollen grain. The exact location of all visible and concealed structures in the sporoderm can be detected; this information helps to describe the morphology and inner structure of pollen grains and to choose necessary directions of further ultrathin sectioning for a transmission electron microscopical study. In studies of fossil pollen grains that are preserved in clumps and stuck to cuticles, confocal microscope is useful in determining the number of apertures in individual pollen grains. This can be done by means of virtual sections through 3‐D reconstructions of pollen grains. Fossil megaspores are too large and too thick‐walled objects for a confocal study; however, confocal microscope was able to reveal a degree of compression of fossil megaspores, the presence of a cavity between the outer and inner sporoderm layers, and to get some information about sporoderm inner structure.     

Confocal microscopy and image processing in the study of plant nuclear structure

We describe measurements of the point spread function (PSF) for a confocal microscope and compare them with the PSF for a conventional (wide-field) fluorescence microscope. In situ hybridization with probes to telomere and ribosomal rDNA sequences, combined with three-dimensional (3-D) microscopy, has been used to study interphase nuclei in root tissue of Pisum sativum and Vicia faba. Nearly all the telomeres in both species are located at the nuclear envelope, and are highly clustered in the Vicia tissues, suggesting specific binding interactions. rDNA labelling in P. sativum shows four brightly staining knobs, corresponding to condensed regions of the rDNA genes from the two pairs of nucleolar organizer genes in this species, arranged approximately tetrahedrally around each nucleolus. Deconvolution using the measured PSFs can be used to improve these images, revealing a fibrous substructure in the perinucleolar knobs, and a large amount of interconnecting internal structure, which we suggest represents rDNA both in the fibrillar centres and also more diffuse, widely dispersed rDNA. Finally we show that accurate conventional data coupled with deconvolution can produce 3-D reconstructions comparable to those obtainable with confocal microscopy, but that the clearest images are obtained by applying deconvolution to the confocal data.     

Real-time confocal microscopy of keratocyte activity in wound healing after cryoablation in rabbit corneas

A modified tandem scanning confocal microscope was used for real-time in vivo examination of the rabbit cornea following a cryogenic injury. The corneas of New Zealand white rabbits were frozen with aprobe that had been cooled by immersion in liquid nitrogen, effectively destroying keratocytes in a central 5 mm diameter zone throughout the total thickness of the cornea. In these eyes, keratocyte repopulation and corneal stromal wound healing proceeded similarly to that which occurs after epikeratophakia, a refractive surgical procedure designed to change the curvature and optical power of the cornea. In epikeratophakia, a cryolathed donor corneal stroma lenticule is sutured onto the bare stroma of the recipient cornea. The collagen tissue lenticule is repopulated by keratocytes (corneal fibroblasts) that migrate in from the host cornea. In our study, the confocal microscope permitted sequential, noninvasive examination of the corneal stroma in the treated animals. Necrosis of the keratocytes, followed by activation of the remaining viable cells in the corneal periphery, was observed in the first 2 to 3 days after cryo injury. A fine stromal fibrous network was seen to develop; in three eyes, this network progressed to the development of a retrocorneal fibrous membrane and dense stromal fibrosis, both of which resulted in significant loss of corneal clarity. Our results suggest that the confocal microscope may be a valuable tool to provide much needed information on wound healing processes at the cellular level after corneal surgery and injury.     

Real-time confocal microscopy of keratocyte activity in wound healing after cryoablation in rabbit corneas

A modified tandem scanning confocal microscope was used for real-time in vivo examination of the rabbit cornea following a cryogenic injury. The corneas of New Zealand white rabbits were frozen with a probe that had been cooled by immersion in liquid nitrogen, effectively destroying keratocytes in a central 5 mm diameter zone throughout the total thickness of the cornea. In these eyes, keratocyte repopulation and corneal stromal wound healing proceeded similarly to that which occurs after epikeratophakia, a refractive surgical procedure designed to change the curvature and optical power of the cornea. In epikeratophakia, a cryolathed donor corneal stroma lenticule is sutured onto the bare stroma of the recipient cornea. The collagen tissue lenticule is repopulated by keratocytes (corneal fibroblasts) that migrate in from the host cornea. In our study, the confocal microscope permitted sequential, noninvasive examination of the corneal stroma in the treated animals. Necrosis of the keratocytes, followed by activation of the remaining viable cells in the corneal periphery, was observed in the first 2 to 3 days after cryo injury. A fine stromal fibrous network was seen to develop; in three eyes, this network progressed to the development of a retrocorneal fibrous membrane and dense stromal fibrosis, both of which resulted in significant loss of corneal clarity. Our results suggest that the confocal microscope may be a valuable tool to provide much needed information on wound healing processes at the cellular level after corneal surgery and injury.     

Integration of a high‐NA light microscope in a scanning electron microscope

We present an integrated light‐electron microscope in which an inverted high‐NA objective lens is positioned inside a scanning electron microscope (SEM). The SEM objective lens and the light objective lens have a common axis and focal plane, allowing high‐resolution optical microscopy and scanning electron microscopy on the same area of a sample simultaneously. Components for light illumination and detection can be mounted outside the vacuum, enabling flexibility in the construction of the light microscope. The light objective lens can be positioned underneath the SEM objective lens during operation for sub‐10 μm alignment of the fields of view of the light and electron microscopes. We demonstrate in situ epifluorescence microscopy in the SEM with a numerical aperture of 1.4 using vacuum‐compatible immersion oil. For a 40‐nm‐diameter fluorescent polymer nanoparticle, an intensity profile with a FWHM of 380 nm is measured whereas the SEM performance is uncompromised. The integrated instrument may offer new possibilities for correlative light and electron microscopy in the life sciences as well as in physics and chemistry.     

A procedure to determine the correct thickness of an object with confocal microscopy in case of refractive index mismatch

A difference in refractive index (n) between immersion medium and specimen results in increasing loss of intensity and resolution with increasing focal depth and in an incorrect axial scaling in images of a confocal microscope. Axial thickness measurements of an object on such images are therefore not exact. The present paper describes a simple procedure to determine the correct axial thickness of an object with confocal fluorescence microscopy. We study this procedure for a specimen that has a higher refractive index than the immersion medium and with a thickness up to 100 µm. The measuring method was experimentally tested by comparing the thickness of polymer layers measured on axial images of a confocal microscope in case of a water–polymer mismatch to reference values obtained from an independent technique, i.e. scanning electron microscopy. The case when the specimen has a lower refractive index than the immersion medium is also shown by way of illustration. Measured thickness data of a water layer and an oil layer with the same actual thickness were obtained using an oil-immersion objective lens with confocal microscopy. Good agreement between theory and experiment was found in both cases, consolidating our method.     

PHOEBE,a prototype scanning laser-feedback microscope for imaging biological cells in aqueous media

Based on the principle of laser-feedback interferometry (LFI), a laser-feedback microscope (LFM) has been constructed capable of providing an axial (z) resolution of a target surface topography of ～ 1 nm and a lateral (x, y) resolution of ～ 200 nm when used with a high-numerical-aperture oil-immersion microscope objective. LFI is a form of interferometry in which a laser's intensity is modulated by light re-entering the illuminating laser. Interfering with the light circulating in the laser resonant cavity, this back-reflected light gives information about an object's position and reflectivity. Using a 1-mW He–Ne (λ = 632·8 nm) laser, this microscope (PHOEBE) is capable of obtaining 256 × 256-pixel images over fields from (10 μm × 10 μm) to (120 μm × 120 μm) in ～ 30 s. An electromechanical feedback circuit holds the optical pathlength between the laser output mirror and a point on the scanned object constant; this allows two types of images (surface topography and surface reflectivity) to be obtained simultaneously. For biological cells, imaging can be accomplished using back-reflected light originating from small refractive-index changes (> 0·02) at cell membrane/water interfaces; alternatively, the optical pathlength through the cell interior can be measured point-by-point by growing or placing a cell suspension on a higher-reflecting substrate (glass or a silicon wafer). Advantages of the laser-feedback microscope in comparison to other confocal optical microscopes include: the simplicity of the single-axis interferometric design; the confocal property of the laser-feedback microscope (a virtual pinhole), which is achieved by the requirement that only light that re-enters the laser meeting the stringent frequency, spatial (TEM₀₀), and coherence requirements of the laser cavity resonator mode modulate the laser intensity; and the improved axial resolution, which is based on interferometric measurement of optical amplitude and phase rather than by use of a pinhole as in other types of confocal microscopes.     

Sample holder for axial rotation of specimens in 3D microscopy

In common light microscopy, observation of samples is only possible from one perspective. However, especially for larger three‐dimensional specimens observation from different views is desirable. Therefore, we are presenting a sample holder permitting rotation of the specimen around an axis perpendicular to the light path of the microscope. Thus, images can be put into a defined multidimensional context, enabling reliable three‐dimensional reconstructions. The device can be easily adapted to a great variety of common light microscopes and is suitable for various applications in science, education and industry, where the observation of three‐dimensional specimens is essential. Fluorescence z‐projection images of copepods and ixodidae ticks at different rotation angles obtained by confocal laser scanning microscopy and light sheet fluorescence microscopy are reported as representative results.     

Study of Golgi-impregnated material using the confocal tandem scanning reflected light microscope

The tandem scanning reflected-light microscope (TSM) is a real-time, direct-view confocal microscope. Only those points in the specimen situated in the focal plane contribute information to the image. A Tracor Northern TMS with piezo-electric control of the objective lens was used to generate 3-D images from Golgi-impregnated hamster cerebral cortex. Stereoscopic pairs of images were recorded as 35-mm colour film transparencies by photographing while automatically through-focusing along inclined axes. Transferring the image via a TV camera to the computer, stereo-pairs were obtained by oblique through-focusing and summing, displaying maximum intensity data in each line of sight. Pseudocolour topographic displays were generated by assigning the pixel value in a z map image as the focal depth at which the back-scattered light signal was maximal. The TSM was also modified so that a conventional transmitted-light image with a large depth of field could be obtained simultaneously as the very shallow depth of field confocal back-scattered-light image seen at any focus level. The conventional image is a silhouette of the impregnated neurons: the top surface of the cell is not visible and the relationships of processes that cross over cell bodies cannot be discerned. TSM gives a high-contrast image. The Golgi precipitate over the neuronal surface is resolved as globular or ovoid, coloured particles. The smaller particles also cover the dendritic spines. All the confocal range (extended focus) image display methods satisfactorily demonstrated the 3-D arrangement of cell bodies and processes in the chosen volume.     

Remote focusing in confocal microscopy by means of a modified Alvarez lens

Alvarez lenses are actuated lens‐pairs which allow one to tune the optical power by mechanical displacement of subelements. Here, we show that a recently realized modified Alvarez lens design which does not require mechanical actuation can be integrated into a confocal microscope. Instead of mechanically moving them, the sublenses are imaged onto each other in a 4f‐configuration, where the lateral image shift leading to a change in optical power is created by a galvo‐mirror. The avoidance of mechanical lens shifts leads to a large speed gain for axial (and hence also 3D) image scans compared to classical Alvarez lenses. We demonstrate that the suggested operation principle is compatible with confocal microscopy. In order to optimize the system, we have drawn advantage of the flexibility a liquid‐crystal spatial light modulator offers for the implementation. For given specifications, dedicated diffractive optical elements or freeform elements can be used in combination with resonant galvo‐scanners or acousto‐optic beam deflectors, to achieve even faster z‐scans than reported here, reaching video rate.     

Confocal imaging and second-order stereological analysis of a liquid foam

Foam structures are found in diverse fields of study; the structure of fire-fighting foam, upholstery foams and even the head on a pint of beer all share detailed similarities in their microstructure and dynamics. Despite impressive developments in the theory of two-dimensional foams the challenge in future will be to analyse and model the dynamics of three-dimensional foams. However, the myriad of gas/liquid interfaces in an aqueous foam make direct imaging of their structure difficult. In this study we circumvent this problem by using fluorescence confocal microscopy to acquire three-dimensional images of the structure of a coarsening aqueous foam. A stable aqueous foam was created by mixing commercial shaving foam with ethanol and a small amount of fluorescein solution. The foam was imaged in fluorescence mode such that the liquid fraction of the foam, containing the fluorescent dye, could be seen in optical sections. These images could be acquired in three-dimensional stacks of optical sections up to a depth of about 200 μm. Single images were also acquired as a time series. The time series of single optical section images clearly show the dynamics of the foam. Early images show a structure made mainly of spherical bubbles; later images show the polyhedral structure of the foam which coarsens as a function of time. The polyhedral nature of the foams is shown particularly clearly in stereo pair images of the three-dimensional image sets. The three-dimensional images of the foams were also analysed using second-order stereology (statistical summaries of spatial distribution). The x, y and z coordinates of the foam vertices were extracted from the images and used to compute the nearest neighbour (G-function) and reduced second moment (K-function) statistics. These statistics allow quantification of the range of length scales found in the foams. These results form part of an ongoing study of the coarsening of aqueous foams.     

A prototype two-detector confocal microscope for in vivo corneal imaging

Confocal microscopy through-focusing (CMTF) of the cornea produces a three-dimensional (3-D) display of corneal structure and intensity profiles that allow objective measurements of corneal sublayer thickness and relative assessment backscattering of light. In this study, a prototype confocal instrument was evaluated in which a photon counting photomultiplier tube (PMT) detector was added to provide faster and more quantitative measurements, while still maintaining the imaging capability of the microscope. To acquire images and measure backscattered light simultaneously, an uncoated pellicle beam splitter was incorporated into the light path of the confocal microscope. This beam splitter reflects 8% of the confocal signal to the PMT. The CMTF scans were performed on four rabbits using the prototype instrument. Corneal images and 3-D reconstructions acquired with and without the beam splitter in the light path appeared identical. Both the camera and PMT CMTF curves had easily identifiable peaks corresponding to the epithelium, basal lamina, and endothelium. No significant differences were found between PMT and camera CMTF measurements of epithelial, stromal, or corneal thickness (n = 12 scans). Furthermore, a high correlation was found between camera and PMT measurements (linear regression analysis, y = 0.999 x -0.4, r = 0.99, p < 0.001). The data suggest that by adding a pellicle beam splitter, CMTF intensity data can be acquired using a PMT. The PMT has a faster sampling rate and greater dynamic range than the camera and provides a count of the photons detected. Thus, the instrument has the potential for improving corneal pachymetry and back-scattering measurements while still providing high-resolution corneal images.