Confocal endoscopy via structured illumination

We describe a simple modification to a rigid endoscope so as to provide both high-quality conventional and confocal images of reasonably accessible regions of the body. This versatile system uses a structured illumination approach together with a conventional incoherent illumination source. Images taken in fluorescence are presented using this combined conventional and confocal endoscope.     

Real-time white light reflection confocal microscopy using a fibre-optic bundle

We describe a real-time white light reflection con-focal microscope incorporating an optical fibre bundle and characterise the optical performance of the bundle. The use of an incoherent light source enables us, for the first time, to present speckle-free endoscopic reflected light confocal images. The system has potential application for in vivo studies.     

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.     

Three-dimensional image formation in confocal microscopy

Three-dimensional (3-D) imaging in confocal microscopes is considered in terms of 3-D transfer functions. This leads to an explanation of axial imaging properties. The axial response was observed in both object-scanning and beam-scanning microscopes and the influence of off-axis examination investigated. By simple processing of multi-detector signals, imaging in both the axial and transverse directions can be improved.     

用于激光共聚焦显微镜的光谱扫描机构

随着生物医学技术的发展,组织样本经常被多种荧光标记物标记,需要通过光谱成像的方法区分出样本中不同的成分。本文在共聚焦显微镜基础上,介绍了一种由精密丝杠和步进电机控制的狭缝机构实现光谱成像的方法,讨论了狭缝缝片的具体设计和狭缝运动精度对光谱带宽和波长准确度的影响。     

Novel lambda FRET spectral confocal microscopy imaging method

We report a highly specific, sensitive, and robust method for analyzing fluorescence resonance energy transfer (FRET) based on spectral laser scanning confocal microscopy imaging. The lambda FRET (lambdaFRET) algorithm comprises imaging of a FRET sample at multiple emission wavelengths rendering a FRET spectrum, which is separated into its donor and acceptor components to obtain a pixel-based calculation of FRET efficiency. The method uses a novel off-line precalibration procedure for spectral bleed-through correction based on the acquisition of reference reflection images, which simplifies the method and reduces variability. LambdaFRET method was validated using structurally characterized FRET standards with variable linker lengths and stoichiometries designed for this purpose. LambdaFRET performed better than other well-established methods, such as acceptor photobleaching and sensitized emission-based methods, in terms of specificity, reproducibility, and sensitivity to distance variations. Moreover, lambdaFRET analysis was unaffected by high fluorochrome spectral overlap and cellular autofluorescence. The lambdaFRET method demonstrated outstanding performance in intra- and intermolecular FRET analysis in both fixed and live cell imaging studies.     

Wavelength considerations in confocal microscopy of botanical specimens

We have used a multiple-laser confocal microscope with lines at 325, 442, 488, 514 and 633 nm to investigate optical sectioning of botanical specimens over a wide range of wavelengths. The 442-nm line allowed efficient excitation of Chromomycin A3, with minimal background autofluorescence, to visualize GC-rich heterochromatin as an aid to chromosome identification. Sequential excitation with 442- and 488-nm light enabled ratio imaging of cytosolic pH using BCECF. The red HeNe laser penetrated deep into intact plant tissues, being less prone to scattering than shorter blue lines, and was also used to image fluorescent samples in reflection, prior to fluorescence measurements, to reduce photobleaching. Chromatic corrections are more important in confocal microscope optics than in conventional microscopy. Measured focus differences between blue, green and red wavelengths, for commonly used objectives, were up to half the optical section thickness for both our multi-laser system and a multi-line single-laser instrument. This limited high-resolution sectioning at visible wavelengths caused a loss in signal. For ultraviolet excitation the focus shift was much larger and had to be corrected by pre-focusing the illumination. With this system we have imaged DAPI-stained nuclei, callose in pollen tubes using Aniline Blue and the calcium probe Indo-1.     

The significance of 3-D transfer functions in confocal scanning microscopy

The three-dimensional (3-D) transfer function is a useful concept for describing image formation in confocal scanning microscopy. From it we can derive the corresponding 2-D transfer function for in-focus imaging. In confocal transmission this can be derived analytically. The 1-D transfer function for on-axis imaging, which can be expressed in an analytical form even for confocal fluorescence with differing wavelengths of excitation and fluorescence, can be derived from the 3-D transfer function. The 2-D transfer function for in-focus imaging in confocal fluorescence microscopy with a finite-sized detector is also presented, which is shown to exhibit sign changes and can therefore result in reversals of image contrast.     

Three-dimensional image restoration and super-resolution in fluorescence confocal microscopy

Confocal scanning laser microscopy (CSLM) provides optical sectioning of a fluorescent sample and improved resolution with respect to conventional optical microscopy. As a result, three-dimensional (3-D) imaging of biological objects becomes possible. A difficulty is that the lateral resolution is better than the axial resolution and, thus, the microscope provides orientation-dependent images. However, a theoretical investigation of the process of image formation in CSLM shows that it must be possible to improve the resolution obtained in practice. We present two methods for achieving such a result in the case of 3-D fluorescent objects. The first method applies to conventional CSLM, where the image is detected only on the optical axis for any scanning position. Since the resulting 3-D image is the convolution of the object with the impulse-response function of the instrument, the problem of image restoration is a deconvolution problem and is affected by numerical instability. A short introduction to the linear methods developed for obtaining stable solutions of these problems (the so-called regularization theory of ill-posed problems) is given and an application to a real image is discussed. The second method applies to a new version of CSLM proposed in recent years. In such a case the full image must be measured by a suitable array of detectors. For each scanning position the data are not single numbers but vectors. Then, in order to recover the object, one must solve a Fredholm integral equation of the first kind. A method for the solution of this equation is presented and the possibility of achieving super-resolution is demonstrated. More precisely, we show that it is possible to improve by about a factor of 2 the resolution of conventional CSLM both in the lateral and axial directions.     

光纤共聚焦显微内窥镜活体内实时成像系统的设计和研究

介绍了一种光纤共聚焦显微内窥镜实时活体内成像系统。该系统采用高速扫描振镜、超细成像光纤束、大尺度几何形变理论图像拼接技术,并结合自主研发的综合软件,使该系统具有实时检测、探头物理尺寸小、图像分辨力高、用户界面友好、操作方便等多方面优势。实验表明:该系统可为医生提供丰富的组织学和病理学影像信息,提高诊断准确率。该系统为临床医学提供了一种能在活体内进行实时细胞尺寸检测的医疗仪器,是癌症早期诊断的重要工具。     

Real-time confocal imaging, during active air abrasion – substrate cutting

Air abrasion cutting, using particulates accelerated in a controlled compressed gas stream, is currently being re-evaluated as a precision tissue removal technique for dental cavity preparation. The minimal vibrations and heat generated during cutting commend the technique for use in the shaping of fragile or brittle materials that are vulnerable to vibrations and thermal stresses.
Traditional air abrasion studies have relied solely upon post-procedure imaging, and cutting process details have been inferred from the nature of the residual surface. In this paper, however, a real-time confocal microscopic imaging method is described, which for the first time has allowed prior target structure characterization with subsequent imaging of cutting interactions and substrate failure patterns. Using internally focusing long working distance Hill objective lenses, focusing deep to a protective microscope slide and adhesive interfaces, unhindered remote image sampling within the bulk of specimens such as tooth tissue, acrylic and brittle ceramics was possible.
Moreover, areas of active cutting and inactive regions were identified within air abraded cavities during their creation. The characteristics of the finished cut surfaces were demonstrated and confirmed the findings of previous SEM studies. The method allowed direct control over all the known variables influencing cutting with particulate streams.     

The effect of aberrations on the axial response of confocal imaging systems

A confocal scanning microscope permits three-dimensional imaging of a volume specimen. The role of lens aberrations on the axial response of the system is considered both experimentally and theoretically. It is found that primary coma, for example, plays no part in the axial response from a perfect reflector. The role of detector size is also considered and compared with theory. In general, the effect of aberrations is increased as the size of the detector is increased.     

激光扫描共聚焦光谱成像系统

在激光扫描共聚焦显微成像技术基础上引入了光谱成像技术以便区分生物组织中的不同荧光成分。采用分光棱镜对荧光进行光谱展开,在光谱谱面处设置两个可移动缝片形成出射狭缝,两个步进电机带动安装其上的两个缝片设置系统在整个工作波长（400~700 nm）内的光谱带宽,其最小光谱带宽优于5 nm。用488 nm激光和低压汞灯实际测量了几条谱线对应的狭缝位置并和理论值做了比较,结果显示实际狭缝位置和理论值的差值均小于0.1 mm。在全光谱和50 μm出射狭缝（对应2.5 nm光谱带宽）对老鼠肾脏组织进行了共聚焦光谱成像实验,获得了老鼠肾脏组织中DAPI标定的细胞核图像和Alexa Fluor^®488标定的肾脏小球曲管图像,实现了对老鼠肾脏组织不同成分的区分。实验结果表明：提出的系统能够进行共聚焦光谱成像,扩大了共聚焦显微镜的适用范围。     

Probing DNA structure and function with a multiwavelength fluorescence confocal laser microscope

Three levels of organization in DNA structure in the interphase cell nucleus are assessed by confocal laser scanning microscopy: (i) the conformational state of the double helix; (ii) the distribution of eu- and heterochromatin; and (iii) the localization of replication complexes throughout S phase. Multi-parameter measurements were carried out in each optical section using two laser sources and combined stereoscopic reconstructions were used to assess the co-localization of nuclear components. DNA is highly polymorphic and can adopt a variety of different helical conformations as well as unusual structures (curved, cruciform, multi-stranded). We have assessed by laser scanning microscopy the presence of left-handed Z-DNA in polytene chromosomes of Diptera as well as the spatio-temporal distribution of Z-DNA binding proteins in whole-mount Drosophila embryos and ovaries. We have determined the 3-D distribution of replication sites relative to heterochromatin regions, nucleoli and nuclear membrane by using short pulses of BrdU incorporation in synchronized mouse and human fibroblasts. Replication sites were visualized with a monoclonal anti-BrdU antibody combined with DNA fluorescent staining and antibody labelling of nuclear lamin. The implications of dynamic DNA movement and structural rearrangement to the organization of the nucleus in domains are discussed.     

Three‐dimensional imaging of porous media using confocal laser scanning microscopy

In the last decade, imaging techniques capable of reconstructing three‐dimensional (3‐D) pore‐scale model have played a pivotal role in the study of fluid flow through complex porous media. In this study, we present advances in the application of confocal laser scanning microscopy (CLSM) to image, reconstruct and characterize complex porous geological materials with hydrocarbon reservoir and CO₂ storage potential. CLSM has a unique capability of producing 3‐D thin optical sections of a material, with a wide field of view and submicron resolution in the lateral and axial planes. However, CLSM is limited in the depth (z‐dimension) that can be imaged in porous materials. In this study, we introduce a ‘grind and slice’ technique to overcome this limitation. We discuss the practical and technical aspects of the confocal imaging technique with application to complex rock samples including Mt. Gambier and Ketton carbonates. We then describe the complete workflow of image processing to filtering and segmenting the raw 3‐D confocal volumetric data into pores and grains. Finally, we use the resulting 3‐D pore‐scale binarized confocal data obtained to quantitatively determine petrophysical pore‐scale properties such as total porosity, macro‐ and microporosity and single‐phase permeability using lattice Boltzmann (LB) simulations, validated by experiments.     

Automated imaging of extended tissue volumes using confocal microscopy

Confocal microscopy enables constitutive elements of cells and tissues to be viewed at high resolution and reconstructed in three dimensions, but is constrained by the limited extent of the volumes that can be imaged. We have developed an automated technique that enables serial confocal images to be acquired over large tissue areas and volumes. The computer-controlled system, which integrates a confocal microscope and an ultramill using a high-precision translation stage, inherently preserves specimen registration, and the user control interface enables flexible specification of imaging protocols over a wide range of scales and resolutions. With this system it is possible to reconstruct specified morphological features in three dimensions and locate them accurately throughout a tissue sample. We have successfully imaged various samples at 1-mum voxel resolution on volumes up to 4 mm3 and on areas up to 75 mm2. Used in conjunction with appropriate embedding media and immuno-histochemical probes, the techniques described in this paper make it possible to routinely map the distributions of key intracellular structures over much larger tissue domains than has been easily achievable in the past.     

Quantitative three-dimensional confocal imaging of the cornea in situ and in vivo: System design and calibration

A new depth encoding system (DES) is presented, which makes it possible to calculate, display, and record the z-axis position continuously during in vivo imaging using tandem scanning confocal microscopy (TSCM). In order to verify the accuracy of the DES for calculating the position of the focal plane in the cornea both in vitro and in vivo, we compared TSCM measurements of corneal thickness to measurements made using an ultrasonic pachymeter (UP, a standard clinical instrument) in both enucleated rabbit, cat, and human eyes (n = 15), and in human patients (n = 7). Very close agreement was found between the UP and TSCM measurements in enucleated eyes; the mean percent difference was 0.50 ± 2.58% (mean ± SD, not significant). A significant correlation (R=0.995, n=15, p< 0.01) was found between UP and TSCM measurements. These results verify that the theoretical equation for calculating focal depth provided by the TSCM manufacturer is accurate for corneal imaging. Similarly, close agreement was found between the in vivo UP and TSCM measurements; the mean percent difference was 1.67 ± 1.38% (not significant), confirming that z-axis drift can be minimized with proper applanation of the objective. These results confirm the accuracy of the DES for imaging of the cornea both ex vivo and in vivo. This system should be of great utility for applications where quantitation of the three-dimensional location of cellular structures is needed.     

Performance comparison between the high-speed Yokogawa spinning disc confocal system and single-point scanning confocal systems

Fluorescence microscopy of the dynamics of living cells presents a special challenge to a microscope imaging system, simultaneously requiring both high spatial resolution and high temporal resolution, but with illumination levels low enough to prevent fluorophore damage and cytotoxicity. We have compared the high-speed Yokogawa CSU10 spinning disc confocal system with several conventional single-point scanning confocal (SPSC) microscopes, using the relationship between image signal-to-noise ratio and fluorophore photobleaching as an index of system efficiency. These studies demonstrate that the efficiency of the CSU10 consistently exceeds that of the SPSC systems. The high efficiency of the CSU10 means that quality images can be collected with much lower levels of illumination; the CSU10 was capable of achieving the maximum signal-to-noise of an SPSC system at illumination levels that incur only at 1/15th of the rate of the photobleaching of the SPSC system. Although some of the relative efficiency of the CSU10 system may be attributed to the use of a CCD rather than a photomultiplier detector system, our analyses indicate that high-speed imaging with the SPSC system is limited by fluorescence saturation at the high levels of illumination frequently needed to collect images at high frame rates. The high speed, high efficiency and freedom from fluorescence saturation combine to make the CSU10 effective for extended imaging of living cells at rates capable of capturing the three-dimensional motion of endosomes moving up to several micrometres per second.     

Parallel confocal microscopy using high‐order axially symmetric polarized beams

A novel scheme of parallel confocal microscopy using high‐order axially symmetric polarized beams (ASPBs) is proposed. The basic concept of ASPBs is introduced first, then the principle of the scheme is presented, finally some numerical results are shown to verify the feasibility of the scheme. Seen from the results, multiple imaging spots are obtained and the size of spots is about 70% of the spot size in the single lens microscopy, and a kind of high temporal and spatial resolution parallel confocal microscopy is achieved, which may find wide applications in the fields of 3D profile measurement and biomedical imaging. Microsc. Res. Tech. 78:302–308, 2015. © 2015 Wiley Periodicals, Inc.