A comparison study of detecting gold nanorods in living cells with confocal reflectance microscopy and two‐photon fluorescence microscopy

Two‐photon fluorescence microscopy and confocal reflectance microscopy were compared to detect intracellular gold nanorods in rat basophilic leukaemia cells. The two‐photon photoluminescence images of gold nanorods were acquired by an 800 nm fs laser with the power of milliwatts. The advantages of the obtained two‐photon photoluminescence images are high spatial resolution and reduced background. However, a remarkable photothermal effect on cells was seen after 30 times continuous scanning of the femto‐second laser, potentially affecting the subcellular localization pattern of the nanorods. In the case of confocal reflectance microscopy the images of gold nanorods can be obtained with the power of light source as low as microwatts, thus avoiding the photothermal effect, but the resolution of such images is reduced. We have noted that confocal reflectance images of cellular gold nanorods achieved with 50 μW 800 nm fs have a relatively poor resolution, whereas the 50 μW 488 nm CW laser can acquire reasonably satisfactory 3D reflectance images with improved resolution because of its shorter wavelength. Therefore, confocal reflectance microscopy may also be a suitable means to image intracellular gold nanorods with the advantage of reduced photothermal effect.     

Image scanning fluorescence emission difference microscopy based on a detector array

We propose a novel imaging method that enables the enhancement of three‐dimensional resolution of confocal microscopy significantly and achieve experimentally a new fluorescence emission difference method for the first time, based on the parallel detection with a detector array. Following the principles of photon reassignment in image scanning microscopy, images captured by the detector array were arranged. And by selecting appropriate reassign patterns, the imaging result with enhanced resolution can be achieved with the method of fluorescence emission difference. Two specific methods are proposed in this paper, showing that the difference between an image scanning microscopy image and a confocal image will achieve an improvement of transverse resolution by approximately 43% compared with that in confocal microscopy, and the axial resolution can also be enhanced by at least 22% experimentally and 35% theoretically. Moreover, the methods presented in this paper can improve the lateral resolution by around 10% than fluorescence emission difference and 15% than Airyscan. The mechanism of our methods is verified by numerical simulations and experimental results, and it has significant potential in biomedical applications.     

Enhanced scanning control in a confocal scanning laser microscope

A fast and flexible scanning unit, allowing scanning rates of more than 1 kHz over regions identified in a specimen, has been developed and evaluated. This scanning unit replaces the original scanning unit in the Phoibos confocal scanning laser microscope and features full backward compatibility, while at the same time allowing fast and flexible scanning modes, such as point scanning, line scanning, and scanning along user-selected closed curves. The scanning unit uses two galvanometer-mounted mirrors for scanning. A standard procedure for recordings with this scanning unit would be to scan an overview image with conventional raster scanning to identify a region of interest, mark a point, a line, or a closed curve over this region, and to start the scanner. An iterating algorithm then calculates the waveforms needed by the scanner to follow the identified curves with pixel precision. With this scanning unit and its controlling software, experiments demanding time-resolved recordings within the millisecond range can be performed. Repetition rates up to >1 kHz for line scanning and curve scanning, and >100 kHz for point scanning are obtainable. This allows time-resolved studies of fast reactions in living tissue to be performed with the spatial resolution and signal-to-noise ratio obtainable with a point scanning confocal microscope.     

Enhanced scanning control in a confocal scanning laser microscope

A fast and flexible scanning unit, allowing scanning rates of more than 1 kHz over regions identified in a specimen, has been developed and evaluated. This scanning unit replaces the original scanning unit in the Phoibos confocal scanning laser microscope and features full backward compatibility, while at the same time allowing fast and flexible scanning modes, such as point scanning, line scanning, and scanning along user-selected closed curves. The scanning unit uses two galvanometer-mounted mirrors for scanning. A standard procedure for recordings with this scanning unit would be to scan an overview image with conventional raster scanning to identify a region of interest, mark a point, a line, or a closed curve over this region, and to start the scanner. An iterating algorithm then calculates the waveforms needed by the scanner to follow the identified curves with pixel precision. With this scanning unit and its controlling software, experiments demanding time-resolved recordings within the millisecond range can be performed. Repetition rates up to > 1 kHz for line scanning and curve scanning, and > 100 kHz for point scanning are obtainable. This allows time-resolved studies of fast reactions in living tissue to be performed with the spatial resolution and signal-to-noise ratio obtainable with a point scanning confocal microscope.     

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.     

Multipoint scanning dual‐detection confocal microscopy for fast 3D volumetric measurement

We propose a multipoint scanning dual‐detection confocal microscopy (MS‐DDCM) system for fast 3D volumetric measurements. Unlike conventional confocal microscopy, MS‐DDCM can accomplish surface profiling without axial scanning. Also, to rapidly obtain 2D images, the MS‐DDCM employs a multipoint scanning technique, with a digital micromirror device used to produce arrays of effective pinholes, which are then scanned. The MS‐DDCM is composed of two CCDs: one collects the conjugate images and the other collects nonconjugate images. The ratio of the axial response curves, measured by the two detectors, provides a linear relationship between the height of the sample surface and the ratio of the intensity signals. Furthermore, the difference between the two images results in enhanced contrast. The normalising effect of the MS‐DDCM provides accurate sample heights, even when the reflectance distribution of the surface varies. Experimental results confirmed that the MS‐DDCM achieved high‐speed surface profiling with improved image contrast capability.     

浅谈共聚焦显微技术

共聚焦显微镜以其高对比度、高分辨率及可重建三维图像的独特优势,在生物医学研究、微细加工、半导体和高分子材料的生产检测等领域获得广泛应用。常用的共聚焦技术方法有:传统的激光扫描共聚焦显微镜(LSCM),其特点是获得的图像对比度和分辨率高,但需要逐点扫描,帧成像时间长,系统复杂,体积大,价格昂贵;碟片共聚焦显微镜(SDCM)是采用多光束扫描的方法来获得共聚焦图像,速度可以大大提高,但牺牲了共聚焦图像的分辨率,系统更为复杂,且不能调整轴向分辨率;结构光显微镜(SIM)具有方法简单,可模块化设计,成本低,成像质量接近于激光扫描共聚焦显微镜,成像速度快,性价比较高。     

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.     

浅谈激光共聚焦显微镜使用技巧

本文简要介绍了激光扫描共聚焦（LSCM）成像原理,并以花粉为例,详细介绍了共聚焦针孔直径、光电倍增管检测器增益、激光强度、扫描速度、扫描方式、Z轴步距等重要参数设置对共聚焦成像的不同影响。探讨了正确使用LSCM的方法与技巧,如获取高质量的图像、图像保存及图像处理,以便为科技人员利用LSCM开展更多植物学与环境科学相关的研究提供参考。     

Scanning and detection techniques used in a confocal scanning laser microscope

A two-mirror scanning mechanism for confocal microscopy is described. No optical components, in addition to the scanning mirrors, are used. Design criteria and performance of the scanner are discussed. The photometric linearity of a detector unit incorporating a photomultiplier tube is reported, and a dual detector unit with tunable split wavelength is described.     

Image scanning microscopy: an overview

For almost a century, the resolution of optical microscopy was thought to be limited by Abbé’s law describing the diffraction limit of light. At the turn of the millennium, aided by new technologies and fluorophores, the field of optical microscopy finally surpassed the diffraction barrier: a milestone achievement that has been recognized by the 2014 Nobel Prize in Chemistry. Many super‐resolution methods rely on the unique photophysical properties of the fluorophores to improve resolution, posing significant limitations on biological imaging, such as multicoloured staining, live‐cell imaging and imaging thick specimens. Structured Illumination Microscopy (SIM) is one branch of super‐resolution microscopy that requires no such special properties of the applied fluorophores, making it more versatile than other techniques. Since its introduction in biological imaging, SIM has proven to be a popular tool in the biologist's arsenal for following biological interaction and probing structures of nanometre scale. SIM continues to see much advancement in design and implementation, including the development of Image Scanning Microscopy (ISM), which uses patterned excitation via either predefined arrays or raster‐scanned single point‐spread functions (PSF). This review aims to give a brief overview of the SIM and ISM processes and subsequent developments in the image reconstruction process. Drawing from this, and incorporating more recent achievements in light shaping (i.e. pattern scanning and super‐resolution beam shaping), this study also intends to suggest potential future directions for this ever‐expanding field.     

Non-destructive and quantitative imaging of a nano-structured microchip by ptychographic hard X-ray scanning microscopy

We used hard X-ray scanning microscopy with ptychographic coherent diffraction contrast to image a front-end processed passivated microchip fabricated in 80 nm technology. No sample preparation was needed to image buried interconnects and contact layers with a spatial resolution of slightly better than 40 nm. The phase shift in the sample is obtained quantitatively. With the additional knowledge of the elemental composition determined in parallel by X-ray fluorescence mapping, quantitative information about specific nanostructures is obtained. A significant enhancement in signal-to-noise ratio and spatial resolution is achieved compared to conventional hard X-ray scanning microscopy.     

受激发射损耗显微术及其在生物医学上的应用

由于受到光学衍射的限制,均匀照明宽视场荧光显微术和激光共焦扫描显微术的分辨率约为200～300nm。近年来受激发射损耗显微术在突破衍射极限以及应用方面取得许多令人瞩目的成果。本文简要介绍受激发射损耗显微术的原理、方法及其在生物医学上的应用。     

High-resolution confocal microscopy using synchrotron radiation

A confocal scanning light microscope coupled to the Daresbury Synchrotron Radiation Source is described. The broad spectrum of synchrotron radiation and the application of achromatic quartz/CaF₂ optics allows for confocal imaging over the wavelength range 200–700 nm. This includes UV light, which is particularly suitable for high-resolution imaging. The results of test measurements using 290-nm light indicate that a lateral resolution better than 100 nm is obtained. An additional advantage of the white synchrotron radiation is that the excitation wavelength can be chosen to match the absorption band of any fluorescent dye. The availability of UV light for confocal microscopy enables studies of naturally occurring fluorophores. The potential applications of the microscope are illustrated by the real-time imaging of hormone traffic using the naturally occurring oestrogen coumestrol. (The IUPAC name for coumestrol is 3,9-dihydroxy-6H-benzofuro[3,2-c][1]benzopyran-6-one ( Chem. Abstr. Reg. No . 479-13-0). The trivial name will be used throughout this paper.)     

Development of an improved Kelvin probe force microscope for accurate local potential measurements on biased electronic devices

An improved setup for accurate near‐field surface potential measurements and characterisation of biased electronic devices using the Kelvin Probe method has been developed. Using an external voltage source synchronised with the raster‐scan of the KPFM‐AM, this setup allows to avoid potential measurement errors of the conventional Kelvin Probe Force Microscopy in the case of in situ measurements on biased electronic devices. This improved KPFM‐AM setup has been tested on silicon‐based devices and organic semiconductor‐based devices such as organic field effect transistors (OFETs), showing differences up to 25% compared to the standard KPFM‐AM lift‐mode measurement method.     

Concentrated dyes as a source of two-dimensional fluorescent field for characterization of a confocal microscope

The axial spread function is a useful tool for evaluation of a confocal microscope. It can be obtained experimentally by scanning a uniform fluorescent layer whose thickness is significantly below the resolution limit. Previous researchers have created thin fluorescent films by chemical synthesis. We show here that concentrated fluorescent dyes with a strong absorption at the excitation wavelength can serve as a good approximation of thin fluorescent films. The vertical intensity profiles of such dyes are symmetrical and represent the true axial resolution of a microscope. Solutions of dyes sufficiently opaque to test confocal microscopes with high‐NA objectives can be prepared from sodium fluorescein, acid fuchsin and acid blue 9 for excitation at 488 nm, 543 nm and 633 nm, respectively.     

A line scanning confocal fluorescent microscope using a CMOS rolling shutter as an adjustable aperture

Traditional confocal microscopy uses a physical aperture barrier to prevent out-of-focus light from reaching the detector. The physical nature of a conventional aperture limits control over the system confocality. We describe a new line scanning confocal microscope that eliminates a need for a physical aperture by employing a software-controllable rolling shutter on a CMOS camera. A confocal image is obtained by synchronizing motion of the rolling shutter and the laser line scanning over a sample. Confocal resolution of this microscope is adjustable in real time and independently established for each fluorescence channel by changing the rolling shutter width. This technology has been implemented in the IN Cell Analyzer 6000 system by GE Healthcare.     

Adaptive-weighted cubic B-spline using lookup tables for fast and efficient axial resampling of 3D confocal microscopy images

Confocal laser scanning microscopy has become a most powerful tool to visualize and analyze the dynamic behavior of cellular molecules. Photobleaching of fluorochromes is a major problem with confocal image acquisition that will lead to intensity attenuation. Photobleaching effect can be reduced by optimizing the collection efficiency of the confocal image by fast z-scanning. However, such images suffer from distortions, particularly in the z dimension, which causes disparities in the x, y, and z directions of the voxels with the original image stacks. As a result, reliable segmentation and feature extraction of these images may be difficult or even impossible. Image interpolation is especially needed for the correction of undersampling artifact in the axial plane of three-dimensional images generated by a confocal microscope to obtain cubic voxels. In this work, we present an adaptive cubic B-spline-based interpolation with the aid of lookup tables by deriving adaptive weights based on local gradients for the sampling nodes in the interpolation formulae. Thus, the proposed method enhances the axial resolution of confocal images by improving the accuracy of the interpolated value simultaneously with great reduction in computational cost. Numerical experimental results confirm the effectiveness of the proposed interpolation approach and demonstrate its superiority both in terms of accuracy and speed compared to other interpolation algorithms.     

In vivo imaging of human teeth and skin using real-time confocal microscopy

Confocal microscopy is currently being used to obtain images with higher lateral and axial resolution than conventional light microscopic techniques. Most current confocal microscopic applications describe the use of in vitro preparations. The tandem scanning microscope (TSM) can be applied in the in vivo microscopic evaluation of living tissue. This article discusses in vivo applications of the TSM in the study of human teeth and skin.     

Near-field and confocal surface-enhanced resonance Raman spectroscopy at cryogenic temperatures

For laser spectroscopy at variable temperatures with high spatial resolution a combined scanning near‐field optical and confocal microscope was developed. Rhodamine 6G (R6G) dye molecules dispersed on silver nano‐particles or nano‐clusters were investigated. For optical excitation of the molecules, either an aperture probe or a focused laser spot in confocal arrangement were employed. Raman spectra in the wavenumber range between 300 cm^?1 and 3000 cm^?1 at room temperatures down to 8.5 K were recorded. Many of the observed Raman lines can be associated with the structure of the adsorbed molecule. Intensity fluctuations in spectral sequences were observed down to 77 K and are indicative of single molecule sensitivity.