Fluorescence in the tandem scanning microscope

Our studies have shown that the fluorescence mode can be used to good effect in both tandem scanning microscopes (TSM: direct view confocal microscopes) as well as confocal scanning laser microscopes (CSLM). Applications are presented which show that the two great advantages of TSM are real-time viewing and real colour, which allow faster use and interpretation. CSLM are complementary, not competitive, being currently more sophisticated for low-level fluorescence work. This is equally possible with available TSM, but requires further development using CCD cameras and image-processing systems.     

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.     

Image sharpness and contrast transfer in coherent confocal microscopy

Confocal microscopes provide clear, thin optical sections with little disturbance from regions of the specimen that are not in focus. In addition, they appear to provide somewhat greater lateral and axial image resolution than with non-confocal microscope optics. To address the question of resolution and contrast transfer of light microscopes, a new test slide that enables the direct measurement of the contrast transfer characteristics (CTC) of microscope optics at the highest numerical aperature has been developed. With this new test slide, the performance of a confocal scanning laser microscope operating in the confocal reflection mode and the non-confocal transmission mode was examined. The CTC curves show that the confocal instrument maintains exceptionally high contrast (up to twice that with non-confocal optics) as the dimension of the object approaches the diffraction limit of resolution; at these dimensions, image detail is lost with non-confocal microscopes owing to a progressive loss of image contrast. Furthermore, we have calculated theoretical CTC curves by modelling the confocal and non-confocal imaging modes using discrete Fourier analysis. The close agreement between the theoretical and experimental CTC curves supports the earlier prediction that the coherent confocal and the incoherent non-confocal imaging mode have the same limit of resolution (defined here as the inverse of the spatial frequency at which the contrast transfer converges to zero). The apparently greater image resolution of the coherent confocal optics is a consequence of the improved contrast transfer at spacings which are close to the resolution limit.     

Use of a white light supercontinuum laser for confocal interference-reflection microscopy

Shortly after its development, the white light supercontinuum laser was applied to confocal scanning microscopy as a more versatile substitute for the multiple monochromatic lasers normally used for the excitation of fluorescence. This light source is now available coupled to commercial confocal fluorescence microscopes. We have evaluated a supercontinuum laser as a source for a different purpose: confocal interferometric imaging of living cells and artificial models by interference reflection. We used light in the range 460-700 nm where this source provides a reasonably flat spectrum, and obtained images free from fringe artefacts caused by the longer coherence length of conventional lasers. We have also obtained images of cytoskeletal detail that is difficult to see with a monochromatic laser.     

Three-Dimensional imaging of fertilization and early development

The field of biological microscopy has recently enjoyed major technical advances, exemplified by the development of field-emission low-voltage scanning electron microscopes and laser scanning confocal light microscopes. In addition, computer processing of microscopical data is revolutionizing the way morphological information is imaged. In this paper, we illustrate methods by which this new technology can be used to examine events in fertilization and early development in three dimensions. Different types of specimen preparation protocols, using both echinoderm and mammalian gametes and embryos, are evaluated for their ability to preserve accurately the threedimensional organization of these specimens for imaging by both low-voltage scanning electron microscopy and laser scanning confocal light microscopy.     

Vital confocal microscopy in bone

We wished to exploit confocal microscopy for high spatial and temporal resolution vital microscopy in bone. To this end, we evolved implants with glass windows supported in titanium, which were placed in the medial proximal tibial plateau of the rabbit, and special small, self-focussing objectives (dry 10/0.25, water immersion 20/0.45, and oil immersion 45/0.65 and 120/1.0) which mated and matched to the conical window entrance section of the metal components. At intervals of up to 21 months after implant healing, these lenses were used to study live tissue using two genera of confocal microscope: multiple aperture disc, tandem scanning, microscopes for observation in reflection, and video rate confocal laser scanning microscopes for recording, mainly in the fluorescence mode. The latter allowed the study of a variety of intravenously administered substances, including fluorescein, fluorescein-dextrans, fluorescent microspheres, acridine orange, DASPMI, calcein, and tetracycline. We were able to remove blood, stain cells with fluorescent markers, and replace them into the circulation. Calcein and tetracycline bind to the mineral front in bone: this labelling was studied in progress. We observed that both substances partition and remain for long periods (at least days) in adipocytes. Further characterisation of the system used both confocal fluorescence and scanning electron microscopy methods in the study of retrieved implants. These studies showed that the subimplant cortical bone remodelled to a less compact structure with a rich microvasculature extremely close to bone. The points of attachment of bone to glass were found to involve coarse fibres, with the matrix containing large numbers of large cells: some of this tissue was cartilage and some immature bone. An amorphous, mineralised matrix was in immediate contact with glass. The results provide further confirmation of the general utility of high-scan speed confocal methodology in physiology.     

A confocal laser microscope scanner for digital recording of optical serial sections

A confocal laser microscope scanner developed at our institute is described. Since an ordinary microscope is used, it is easy to view the specimen prior to scanning. Confocal imaging is obtained by laser spot illumination, and by focusing the reflected or fluorescent light from the specimen onto a pinhole aperture in front of the detector (a photomultiplier tube). Two rotating mirrors are used to scan the laser beam in a raster pattern. The scanner is controlled by a microprocessor which coordinates scanning, data display, and data transfer to a host computer equipped with an array processor. Digital images with up to 1024 × 1024 pixels and 256 grey levels can be recorded. The optical sectioning property of confocal scanning is used to record thin (～ 1 μm) sections of a specimen without the need for mechanical sectioning. By using computer-control to adjust the focus of the microscope, a stack of consecutive sections can be automatically recorded. A computer is then used to display the 3-D structure of the specimen. It is also possible to obtain quantitative information, both geometric and photometric. In addition to confocal laser scanning, it is easy to perform non-confocal laser scanning, or to use conventional microscopic illumination techniques for (non-confocal) scanning. The design has proved reliable and stable, requiring very few adjustments and realignments. Results obtained with this scanner are reported, and some limitations of the technique are discussed.     

Optimizing the performance of confocal point scanning laser microscopes over the full field of view

To examine many of the imaging capabilities of confocal scanning laser microscopes rapidly and reliably over the whole field of view three simple, easily prepared specimens are required: a mirror positioned on a carefully measured shallow gradient, a film of highly fluorescent material and a rectangular grid with a readily defined centre. Using these specimens the adjustment of any combination of confocal scanning laser visualization system and light microscope can be examined throughout the field of view. The effects of misalignment of the various subcomponents of a confocal scanning laser microscope on both the axial spread function of a plane and the shading pattern over the image field are described. Finally, where the design of the confocal optics permits, the three specimens can be used to facilitate the alignment of the various components to the optimal level achievable.     

Scanning microphotolysis: A new photobleaching technique based on fast intensity modulation of a scanned laser beam and confocal imaging

The fluorescence photobleaching method has been widely used to study molecular transport in single living cells and other microsystems while confocal microscopy has opened new avenues to high-resolution, three-dimensional imaging. A new technique, scanning microphotolysis (Scamp), combines the potential of photobleaching, beam scanning and confocal imaging. A confocal scanning laser microscope was equipped with a sufficiently powerful laser and a novel device, the ‘Scamper’. This consisted essentially of a filter changer, an acousto-optical modulator (AOM) and a computer. The computer was programmed to activate the AOM during scanning according to a freely defined image mask. As a result almost any desired pattern could be bleached (‘written’) into fluorescent samples at high definition and then imaged (‘read’) at non-bleaching conditions, employing full confocal resolution. Furthermore, molecular transport could be followed by imaging the dissipation of bleach patterns. Experiments with living cells concerning dynamic processes in cytoskeletal filaments and the lateral mobility of membrane lipids suggest a wide range of potential biological applications. Thus, Scamp offers new possibilities for the optical manipulation and analysis of both technical and biological microsystems.     

Photon event distribution sampling: an image formation technique for scanning microscopes that permits tracking of sub-diffraction particles with high spatial and temporal resolutions

In photon event distribution sampling, an image formation technique for scanning microscopes, the maximum likelihood position of origin of each detected photon is acquired as a data set rather than binning photons in pixels. Subsequently, an intensity-related probability density function describing the uncertainty associated with the photon position measurement is applied to each position and individual photon intensity distributions are summed to form an image. Compared to pixel-based images, photon event distribution sampling images exhibit increased signal-to-noise and comparable spatial resolution. Photon event distribution sampling is superior to pixel-based image formation in recognizing the presence of structured (non-random) photon distributions at low photon counts and permits use of non-raster scanning patterns. A photon event distribution sampling based method for localizing single particles derived from a multi-variate normal distribution is more precise than statistical (Gaussian) fitting to pixel-based images. Using the multi-variate normal distribution method, non-raster scanning and a typical confocal microscope, localizations with 8 nm precision were achieved at 10 ms sampling rates with acquisition of ~200 photons per frame. Single nanometre precision was obtained with a greater number of photons per frame. In summary, photon event distribution sampling provides an efficient way to form images when low numbers of photons are involved and permits particle tracking with confocal point-scanning microscopes with nanometre precision deep within specimens.     

The use of laser scanning confocal microscopy (LSCM) in materials science

Laser scanning confocal microscopes are essential and ubiquitous tools in the biological, biochemical and biomedical sciences, and play a similar role to scanning electron microscopes in materials science. However, modern laser scanning confocal microscopes have a number of advantages for the study of materials, in addition to their obvious uses for high resolution reflected and transmitted light optical microscopy. In this paper, we provide several examples that exploit the laser scanning confocal microscope's capabilities of pseudo-infinite depth of field imaging, topographic imaging, photo-stimulated luminescence imaging and Raman spectroscopic imaging.     

Imaging modes for bilateral confocal scanning microscopy

The bilateral scanning approach to confocal microscopy is characterized by the direct generation of the image on a two-dimensional (2-D) detector. This detector can be a photographic plate, a CCD detector or the human eye, the human eye permitting direct visualization of the confocal image. Unlike Nipkow-type systems, laser light sources can be used for excitation. A design called a carousel has been developed, in which the bilateral confocal scan capability can be added to an existing microscope so that rapid exchange and comparison between confocal and non-confocal imaging conditions is possible. The design permits independent adjustment of confocal sectioning properties with lateral resolutions better than, or, in the worst case equivalent to, those available in conventional microscopy. The carousel can be considered as a stationary optical path in which certain imaging conditions, such as confocality, are defined and operate on part of the imaging field. The action of the bilateral scan mirror then extends this image condition over the whole field. A number of optical arrangements for the carousel are presented which realize various forms of confocal fluorescence and reflection imaging, with point, multiple point or slit confocal detection arrangements. Through the addition of active elements to the carousel direct stereoscopic, ratio, time-resolved and other types of imaging can be achieved, with direct image formation on a CCD, eye or other 2-D detectors without the need to modify the host microscope. Depending on the photon flux available, these imaging modes can run in real-time or can use a cooled CCD at (very) low light level for image integration over an extended period.     

Wide-band acousto-optic deflectors for large field of view two-photon microscope

Acousto-optic deflector (AOD) is an attractive scanner for two-photon microscopy because it can provide fast and versatile laser scanning and does not involve any mechanical movements. However, due to the small scan range of available AOD, the field of view (FOV) of the AOD-based microscope is typically smaller than that of the conventional galvanometer-based microscope. Here, we developed a novel wide-band AOD to enlarge the scan angle. Considering the maximum acceptable acoustic attenuation in the acousto-optic crystal, relatively lower operating frequencies and moderate aperture were adopted. The custom AOD was able to provide 60 MHz 3-dB bandwidth and 80% peak diffraction efficiency at 840 nm wavelength. Based on a pair of such AOD, a large FOV two-photon microscope was built with a FOV up to 418.5 μm (40× objective). The spatiotemporal dispersion was compensated simultaneously with a single custom-made prism. By means of dynamic power modulation, the variation of laser intensity within the FOV was reduced below 5%. The lateral and axial resolution of the system were 0.58-2.12 μm and 2.17-3.07 μm, respectively. Pollen grain images acquired by this system were presented to demonstrate the imaging capability at different positions across the entire FOV.     

Biological imaging using fast laser scanning heterodyne differential phase confocal microscopes

Differential phase microscopy has proved invaluable in the study of live, unstained, thin biological samples because of its ability to image changes in refractive index and topography. Similarly, because of its optical sectioning capability, confocal microscopy is now a well-established technique in the study of relatively thick live biological samples. This paper describes the development and application of two differential phase heterodyne confocal microscopes, and compares their performance. The use of these systems for imaging in-vitro cell and tissue cultures is considered and compared with confocal reflection microscopy. It is demonstrated that the differential phase capability reveals subcellular structural information not readily seen in the confocal reflection images. This technique opens up the possibility of imaging thick unstained live tissues, avoiding cell damage and artefacts associated with staining procedures. Furthermore, the differential phase images can be used to provide a visual frame within which stained features can be located.     

Applications of high-speed confocal imaging techniques in operative dentistry

All confocal scanning optical microscopes are suitable for making high-resolution images of many structures in teeth under near normal conditions. If the microscope can operate at high speed, then the number of applications widens considerably. The high-frame speed of the tandem scanning reflected light microscope (TSM) enables real-time examination of teeth in vivo, especially when the microscope is configured with a stabilising objective, featuring internal focusing elements. Experimental procedures examined microscopically on extracted teeth can include the cutting of the hard tissues, observation of fluid flow in dentine, the application of adhesives, and the fracturing of adhesive interfaces under load. Undertaking experiments where time is an important function has improved our knowledge of many of the materials/substrate interactions involved in dental operative procedures. Storing images on media other than video tape can be expensive, but reductions in the cost of computer memory is making digitisation and storage of images in real-time more widely available.     

Fluorescence resonance energy transfer from cyan to yellow fluorescent protein detected by acceptor photobleaching using confocal microscopy and a single laser

One manifestation of fluorescence resonance energy transfer (FRET) is an increase in donor fluorescence after photobleaching the acceptor. Published acceptor‐photobleaching methods for FRET have mainly used wide‐field microscopy. A laser scanning confocal microscope enables faster and targeted bleaching within the field of view, thereby improving speed and accuracy. Here we demonstrate the approach with CFP and YFP, the most versatile fluorescent markers now available for FRET. CFP/YFP FRET imaging has been accomplished with a single laser (argon) available on virtually all laser‐scanning confocal microscopes. Accordingly, we also describe the conditions that we developed for dual imaging of CFP and YFP with the 458 and 514 argon lines. We detect FRET in a CFP/YFP fusion and also between signalling molecules (TNF‐Receptor‐Associated‐Factors or TRAFs) that are known to homo‐ and heterotrimerize. Importantly, we demonstrate that appropriate controls are essential to avoid false positives in FRET by acceptor photobleaching. We use two types of negative control: (a) an internal negative control (non‐bleached areas of the cell) and (b) cells with donor in the absence of the acceptor (CFP only). We find that both types of negative control can yield false FRET. Given this false FRET background, we describe a method for distinguishing true positive signals. In summary, we extensively characterize a simple approach to FRET that should be adaptable to most laser‐scanning confocal microscopes, and demonstrate its feasibility for detecting FRET between several CFP/YFP partners.     

Scanning interference and confocal microscopy

The form of the interference term image in scanning confocal and scanning conventional interference microscopes is identical in all respects including optical sectioning. This observation is used to obtain confocal images and surface profiles from conventional scanning interference microscope images.     

Evaluation of fracture planes and cell morphology in complementary fractures of cultured cells in the frozen-hydrated state by field-emission secondary electron microscopy: feasibility for ion localization and fluorescence imaging studies

We have employed field-emission secondary electron microscopy (FESEM) for morphological evaluation of freeze-fractured frozen-hydrated renal epithelial LLC-PK₁ cells prepared with our simple cryogenic sandwich-fracture method that does not require any high-vacuum freeze-fracture instrumentation (Chandra et al. (1986) J. Microsc. 144 , 15–37). The cells fractured on the substrate side of the sandwich were matched one-to-one with their corresponding complementary fractured faces on the other side of the sandwich. The FESEM analysis of the frozen-hydrated cells revealed three types of fracture: (i) apical membrane fracture that produces groups of cells together on the substrate fractured at the ectoplasmic face of the plasma membrane; (ii) basal membrane fracture that produces basal plasma membrane-halves on the substrate; and (iii) cross-fracture that passes randomly through the cells. The ectoplasmic face (E-face) and protoplasmic face (P-face) of the membrane were recognized based on the density of intramembranous particles. Feasibility of fractured cells was shown for intracellular ion localization with ion microscopy, and fluorescence imaging with laser scanning confocal microscopy. Ion microscopy imaging of freeze-dried cells fractured at the apical membrane revealed well-preserved intracellular ionic composition of even the most diffusible ions (total concentrations of K⁺, Na⁺ and Ca⁺). Structurally damaged cells revealed lower K⁺ and higher Na⁺ and Ca⁺ contents than in well-preserved cells. Frozen-freeze-dried cells also allowed imaging of fluorescently labelled mitochondria with a laser scanning confocal microscope. Since these cells are prepared without washing away the nutrient medium or using any chemical pretreatment to affect their native chemical and structural makeup, the characterization of fracture faces introduces ideal sample types for chemical and morphological studies with ion and electron microscopes and other techniques such as laser scanning confocal microscopy, atomic force microscopy and near-field scanning optical microscopy.     

Masked illumination scheme for a galvanometer scanning high-speed confocal fluorescence microscope

High-speed beam scanning and data acquisition in a laser scanning confocal microscope system are normally implemented with a resonant galvanometer scanner and a frame grabber. However, the nonlinear scanning speed of a resonant galvanometer can generate nonuniform photobleaching in a fluorescence sample as well as image distortion near the edges of a galvanometer scanned fluorescence image. Besides, incompatibility of signal format between a frame grabber and a point detector can lead to digitization error during data acquisition. In this article, we introduce a masked illumination scheme which can effectively decrease drawbacks in fluorescence images taken by a laser scanning confocal microscope with a resonant galvanometer and a frame grabber. We have demonstrated that the difference of photobleaching between the center and the edge of a fluorescence image can be reduced from 26 to 5% in our confocal laser scanning microscope with a square illumination mask. Another advantage of our masked illumination scheme is that the zero level or the lowest input level of an analog signal in a frame grabber can be accurately set by the dark area of a mask in our masked illumination scheme. We have experimentally demonstrated the advantages of our masked illumination method in detail.     

Quantitative interpretation of binding reactions of rapidly diffusing species using fluorescence recovery after photobleaching

Fluorescence recovery after photobleaching (FRAP) measurements offer an important tool for analyzing diffusion and binding processes. Confocal scanning laser microscopes that are used in FRAP experiments bleach regions with a radially Gaussian distributed profile. Previous attempts to derive analytical expressions in the case of processes governed by fast diffusion have overlooked the characteristics of the instruments used to perform FRAP measurements and therefore led to approximating solutions. In the present paper, bleaching laser beam characteristics are incorporated into an improved model to provide a more rigorous and accurate method. The proposed model simulates binding inside bounded regions, and it leads to FRAP curves that depend on the on and off rates that can be employed to determine the rate constants. It can be used in conjunction with experimental data acquired with confocal scanning laser microscopes to investigate the biophysical properties of proteins in living cells. The model aims to improve the accuracy when determining rate constants by taking into account a more realistic scenario of the light-matter interaction.