A white light confocal microscope for spectrally resolved multidimensional imaging

Spectrofluorometric imaging microscopy is demonstrated in a confocal microscope using a supercontinuum laser as an excitation source and a custom‐built prism spectrometer for detection. This microscope system provides confocal imaging with spectrally resolved fluorescence excitation and detection from 450 to 700 nm. The supercontinuum laser provides a broad spectrum light source and is coupled with an acousto‐optic tunable filter to provide continuously tunable fluorescence excitation with a 1‐nm bandwidth. Eight different excitation wavelengths can be simultaneously selected. The prism spectrometer provides spectrally resolved detection with sensitivity comparable to a standard confocal system. This new microscope system enables optimal access to a multitude of fluorophores and provides fluorescence excitation and emission spectra for each location in a 3D confocal image. The speed of the spectral scans is suitable for spectrofluorometric imaging of live cells. Effects of chromatic aberration are modest and do not significantly limit the spatial resolution of the confocal measurements.     

Backscattered electron imaging and scanning transmission electron microscopy imaging of multi-layers

Experimental and theoretical results on image contrast of semiconductor multi-layers in scanning electron microscopy investigation are reported. Two imaging modes have been considered: backscattered electron imaging of bulk specimen and scanning transmission imaging of thinned specimens. The following main results have been reached. The image resolution of the multi-layers is, in both cases, defined by the probe size. The contrast, governed by density and atomic number differences, is affected by the size of the interaction volume in backscattered electron imaging and by the beam broadening in scanning transmission. Operating in the scanning transmission mode, the contrast of bright field images can be easily related to local variation in atomic number and density of the specimen while the dark field image contrast is strongly affected by electron beam energy, detector collection angles and specimen thickness. All these factors are able to produce contrast reversals that are difficult to explain without the support of a suitable simulation code.     

Backscattered electron imaging of titanium dioxide in frozen hydrated preparations

Backscattered electron (BSE) imaging was used to study ultrafine TiO₂ crystals distribution in a test cream. The cream was fast frozen, cryofractured and observed uncoated at low temperature. The BSE detector was a microchannel plate. The results demonstrate that up-to-date photoprotective preparations can be investigated by this technique.     

Optical modifications enabling simultaneous confocal imaging with dyes excited by ultraviolet- and visible-wavelength light

Optical modifications to a confocal scanning laser microscope are described which allow simultaneous fluorescence imaging of living specimens excited by ultraviolet (UV)- and visible-wavelength light. Modifications to a Bio-Rad MRC 600 Lasersharp confocal microscope include the introduction of UV-path-specific lenses and a specially designed UV transmitting eyepiece and tube lens. Upon UV excitation these modifications provide similar resolution and field flatness when compared with visible confocal microscopy. The UV-path-specific optics could be adjusted to correct for varying amounts of longitudinal chromatic aberration in commercially available objectives. Eyepiece and tube lenses were chromatically corrected for UV through visible wavelengths to minimize lateral chromatic error. With these modifications, UV-wavelength light may be used to excite ratioing dyes to quantify intracellular ion concentrations, or as an energy source to release caged compounds in a spatially restricted volume, while simultaneously imaging with dyes excited by visible-wavelength light.     

Three-dimensional imaging in confocal systems

We discuss the origin of the three-dimensional imaging characteristics of confocal optical systems. Several methods of information display are considered. The important practical question concerning the correct choice of limiting detector aperture is also considered.     

Backscattered electron SEM imaging of cells and determination of the information depth

Backscattered electron imaging of HT29 colon carcinoma cells in a scanning electron microscope was studied. Thin cell sections were placed on indium‐tin‐oxide‐coated glass slides, which is a promising substrate material for correlative light and electron microscopy. The ultrastructure of HT29 colon carcinoma cells was imaged without poststaining by exploiting the high chemical sensitivity of backscattered electrons. Optimum primary electron energies for backscattered electron imaging were determined which depend on the section thickness. Charging effects in the vicinity of the SiO₂ nanoparticles contained in cell sections could be clarified by placing cell sections on different substrates. Moreover, a method is presented for information depth determination of backscattered electrons which is based on the imaging of subsurface nanoparticles embedded by the cells.     

Backscattered electron imaging of immunogold-labeled and silver-enhanced microtubules in cultured mammalian cells

This technique permits the visualization of microtubules in situ by employing silver-enhanced immunogold labeling and backscattered electron imagery. For best results, monolayer cultures of PtK₂ cells are lysed with Triton X-100 in a microtubule stabilizing buffer, fixed with 1% glutaraldehyde, reduced with NaBH₄, incubated with monoclonal antitubulin and 5-nm gold-labeled anti-IgG, silver enhanced, freeze dried, lightly coated with aluminum, and examined in an SEM equipped with a backscattered electron detector. A high contrast view of the entire microtubule complex of each cell is obtained. Microtubules in freeze-dried preparations have relatively smooth surfaces, whereas those in critical point dried preparations are more irregular or beaded. At high magnifications, an unstained inner core of each microtubule can be resolved. Backscattered electron imaging appears to be a promising technique for localizing cytoskeletal proteins and other intracellular antigens that can be labeled with immunogold and enhanced with silver.     

用于生物组织层析成像的共聚焦内窥镜

为了获取生物组织的层析图像,建立了共聚焦内窥镜成像系统,对该系统的横向和轴向分辨能力进行测量和分析,并且对其在猪皮肤组织的层析成像能力进行研究。首先根据系统工作要求,说明系统的工作原理和组成结构,然后给出系统空间分辨能力的理论计算式,最后测试系统性能,说明测量值与理论值存在偏差的主要原因。实验结果表明：建立的系统轴向分辨能力约为10 ;横向分辨能力约为1.9 ;该系统可以对猪皮肤组织进行层析成像。     

Backscattered electron imaging of the undersurface of resin-embedded cells by field-emission scanning electron microscopy

In this study backscattered electron (BSE) imaging was used to display cellular structures stained with heavy metals within an unstained resin by atomic number contrast in successively deeper layers. Balb/c 3T3 fibroblasts were cultured on either 13-mm discs of plastic Thermanox, commercially pure titanium or steel. The cells were fixed, stained and embedded in resin and the disc removed. The resin block containing the cells was sputter coated and examined in a field-emission scanning electron microscope. The technique allowed for the direct visualization of the cell undersurface and immediately overlying areas of cytoplasm through the surrounding embedding resin, with good resolution and contrast to a significant depth of about 2 μm, without the requirement for cutting sections. The fixation protocol was optimized in order to increase heavy metal staining for maximal backscattered electron production. The operation of the microscope was optimized to maximize the number of backscattered electrons produced and to minimize the spot size. BSE images were collected over a wide range of accelerating voltages (keV), from low values to high values to give ‘sections' of information from increasing depths within the sample. At 3–4 keV only structures a very short distance into the material were observed, essentially the areas of cell attachment to the removed substrate. At higher accelerating voltages information on cell morphology, including in particular stress fibres and cell nuclei, where heavy metals were intensely bound became more evident. The technique allowed stepwise ‘sectional’ information to be acquired. The technique should be useful for studies on cell morphology, cycle and adhesion with greater resolution than can be obtained with any light-microscope-based system.     

Three-dimensional imaging in confocal imaging systems with finite sized detectors

We consider the effect of the finite size of the detector on both the lateral and axial resolution of the confocal system. The use of a finite sized detector means that the imaging is no longer truly coherent. We find that the lateral resolution is considerably more sensitive to the detector size than is the axial response. The question of the rejection of flare light is also considered. Experimental results are shown and we find that acceptable extended-focus, auto-focus and height images may be obtained from non truly-confocal systems. We also find that lens apodization has a far greater effect on the axial resolution than the lateral resolution.     

Double-pulse fluorescence lifetime imaging in confocal microscopy

A theoretical analysis of a new technique for fluorescence lifetime measurement, relying on (near steady state) excitation with short optical pulses, is presented. Application of the technique to confocal microscopy enables local determination of the fluorescence lifetime, which is a parameter sensitive to the local environment of fluorescent probe molecules in biological samples. The novel technique provides high time resolution, since it relies on the laser pulse duration, rather than on electronic gating techniques, and permits, in combination with bilateral confocal microscopy and the use of a (cooled) CCD, sensitive signal detection over a large dynamic range. The principle of the technique is discussed within a theoretical framework. The sensitivity of the technique is analysed, taking into account: photodegradation, the effect of the laser repetition rate and the effect of non-steady-state excitation. The features of the technique are compared to more conventional methods for fluorescence lifetime determination.     

Effects of specimen refractive index on confocal imaging

The aberrations introduced when focusing within a specimen with a refractive index equal to that of water using an oil-immersion objective are investigated theoretically. The peak intensity in the confocal point spread function drops by a factor of two for focusing less than 10 μm into the specimen. The effects on scaling of dimensions in the resulting images are discussed. The image exhibits an axial stretching by a factor of about 1.12.     

High-resolution imaging of organic crystals

The history of high-resolution imaging of organic crystals is summarized, followed by a discussion of radiation damage which reflects current thinking. Methods of specimen preparation and the experimental techniques for high-resolution imaging are described. The results show the application of these techniques to aromatic hydrocarbons, phthalocyanines, and linear-chain aliphatic molecules. Artefacts and image interpretation are also discussed.     

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.     

Combination of multiphoton and reflective confocal imaging of cornea

We combine reflective confocal microscopy with multiphoton microscopy to form a minimally invasive technique to observe the cornea. The two imaging modalities allow detection of complementary information from the cornea. The autofluorescence signal shows the cytoplasm of epithelial cells, and the second harmonic generation signal is used to detect collagen, found mostly in the stroma of the cornea. The reflective confocal imaging allows detection of epithelial cells and keratocytes in the stroma. The system is first tested on bovine cornea. Assessment of the result on the bovine eye will be used to evaluate the potential of the system as a technique for in vivo clinical application.     

Scanning slit aperture confocal microscopy for three-dimensional imaging

A scanning confocal microscope using stationary slit apertures of variable width is described. Scanning is achieved by employing an oscillating mirror galvanometer capable of scanning images at 160 frames/s. The microscope depth-of-focus is characterized for several slit widths and shown to approach diffraction-limited performance as width decreases. Reduction of flare in images taken with narrow slit widths is demonstrated. In addition, the optical sectioning capability of the system is demonstrated using polymer casts of the vasculature of rat kidney.     

Fluorescence photobleaching recovery in the confocal scanning light microscope

Measurement of mobilities of species in liquid systems is of great importance for understanding a number of dynamic phenomena. A well known method for measuring mobilities driven by diffusion is fluorescence photobleaching recovery (FPR), also known as fluorescence recovery after photobleaching (FRAP). New FPR recovery equations for three-dimensional (3-D) apertured scanning using a Gaussian approximation for the axial beam profile have been successfully developed and found to provide a solid basis for extraction of the lateral diffusion coefficient from confocal scanning light microscopy (CSLM)-FPR experimental data. The 2-D diffusion coefficients of fluorescent species can be successfully measured by FPR in the CSLM, which has the great advantage that bleaching can be targeted at a well-defined volume element in bulk samples. Two-dimensional diffusion coefficients of 45-nm latex spheres, of FITC molecules and of a 2·45-nm protein-FITC complex in water-glycerol mixtures, measured by FPR in the CSLM, are in close agreement with those calculated from the size of the diffusing species and viscosity of the medium. Diffusion coefficients as high as 2 times 10^?6 cm²/s can be measured.