Five-colour in vivo imaging of neurons in Caenorhabditis elegans

In the last few years variants of the ‘green fluorescent protein’ (GFP) with different spectral properties have been generated. This has greatly increased the number of possible applications for these fluorochromes in cell biology. The significant overlap of the excitation and emission spectra of the different GFP variants imposes constraints on the number of variants that can be used simultaneously in a single sample. In particular, the two brightest variants, GFP and YFP, are difficult to separate spectrally. This study shows that GFP and YFP can be readily separated with little spectral overlap (cross‐talk) with the use of a confocal microscope equipped with an acusto‐optical beam splitter and freely adjustable emission windows. Under optimal recording conditions cross‐talk is less than 10%. Together with two other fluorescent proteins and the lipophilic dye DiD a total of five different colours can now be used simultaneously to label in vivo distinct anatomical structures such as neurons and their processes. Spatial resolution of the confocal microscope is sufficient to resolve the relative position of labelled axons within a single axon bundle. The use of five distinct marker dyes allows the in vivo analysis of the Caenorhabditis elegans nervous system at unprecedented resolution and richness in detail at the light microscopic level.     

FRET microscopy: from principle to routine technology in cell biology

The phenomenon of resonance energy transfer first described by Theodor Förster presents the opportunity of retrieving information on molecular proximity, orientation and conformation on the nanometre scale from (living) samples with conventional fluorescence microscopes (or even macroscopic devices). During the past 10 years Förster (or fluorescence) resonance energy transfer (FRET) microscopy has been revolutionized by the vast progress in fluorescent protein and in situ fluorescent labelling technology as well as by the commercial availability of advanced quantitative microscopy instrumentation. FRET microscopy is now routinely used in modern cell biology research. This short review will guide the reader through the most established FRET microscopy techniques, their inherent strengths and limitations, potential pitfalls, and assist the reader in making an educated choice on the FRET microscopy method most suited for their specific application.     

Using c-Fos/c-Jun as hetero-dimer interaction model to optimize donor to acceptor concentration ratio range for three-filter fluorescence resonance energy transfer (FRET) measurement

Sensitized emission FRET detection method based on three-filter fluorescence microscopy is widely used and more suitable for live cell FRET imaging and dynamic protein-protein interaction analysis. But when it is applied to detect two proteins interaction in living cells, this intensity-based detection method is complicated by many experimental factors such as spectral crosstalk and spectral bleed-through and variable donor to acceptor concentration ratio. There are several FRET algorithms developed recently to correct those factors in order to quantitatively gauge and compare FRET signals between different experimental groups. But the algorithms are often difficult to choose when they are applied to certain experiments. In this research, we use c-Fos/c-Jun as a simple hetero-dimer interaction model to quantitatively detect and compare the FRET signals based on the following widely used sensitized emission FRET algorithms: N(FRET) , FRET(N) , FR, FRET(R) , E(app) and E(EFF) . We optimized the donor to acceptor concentration ratio range for the above FRET algorithms and facilitate their use in accurate FRET signal determination based on the three-filter FRET microscopy.     

Fluorescence resonance energy transfer of GFP and YFP by spectral imaging and quantitative acceptor photobleaching

To study protein–protein interactions by fluorescence energy transfer (FRET), the proteins of interest are tagged with either a donor or an acceptor fluorophore. For efficient FRET, fluorophores need to have a reasonable overlap of donor emission and acceptor excitation spectra. However, given the relatively small Stokes shift of conventional fluorescent proteins, donor and acceptor pairs with high FRET efficiencies have emission spectra that are difficult to separate. GFP and YFP are widely used in fluorescence microscopy studies. The spectral qualities of GFP and YFP make them one of the most efficient FRET donor–acceptor couples available. However, the emission peaks of GFP (510 nm) and YFP (527 nm) are spectrally too close for separation by conventional fluorescence microscopy. Difficulties in simultaneous detection of GFP and YFP with a fluorescence microscope are eliminated when spectral imaging and subsequent linear unmixing are applied. This allows FRET microscopy using these tags to study protein–protein interactions. We adapted the linear unmixing procedure from commercially available software (Zeiss) for use with acceptor photobleaching FRET using GFP and YFP as FRET pair. FRET efficiencies up to 52% for a GFP-YFP fusion protein were measured. To investigate the applicability of the procedure, we used two constituents of the nucleotide excision repair system, which removes UV-induced single-strand DNA damage. ERCC1 and XPF form a heterodimeric 5' endonuclease in nucleotide excision repair. FRET between ERCC1-GFP and XPF-YFP occurs with an efficiency of 30%.     

Quantitative determination of the reduction of phototoxicity and photobleaching by controlled light exposure microscopy

Phototoxicity and photobleaching are major limitations in live-cell fluorescence microscopy. They are caused by fluorophores in an excited singlet or triplet state that generate singlet oxygen and other reactive oxygen species. The principle of controlled light exposure microscopy (CLEM) is based on non-uniform illumination of the field of view to reduce the number of excited fluorophore molecules. This approach reduces phototoxicity and photobleaching 2- to 10-fold without deteriorating image quality. Reduction of phototoxicity and photobleaching depends on the fluorophore distribution in the studied object, the optical properties of the microscope and settings of CLEM electronics. Here, we introduce the CLEM factor as a quantitative measure of reduction in phototoxicity and photobleaching. Finally, we give a guideline to optimize the effect of CLEM without compromising image quality.     

A statistical approach for intensity loss compensation of confocal microscopy images

In this paper, a probabilistic technique for compensation of intensity loss in confocal microscopy images is presented. For single-colour-labelled specimen, confocal microscopy images are modelled as a mixture of two Gaussian probability distribution functions, one representing the background and another corresponding to the foreground. Images are segmented into foreground and background by applying Expectation Maximization algorithm to the mixture. Final intensity compensation is carried out by scaling and shifting the original intensities with the help of parameters estimated for the foreground. Since foreground is separated to calculate the compensation parameters, the method is effective even when image structure changes from frame to frame. As intensity decay function is not used, complexity associated with estimation of the intensity decay function parameters is eliminated. In addition, images can be compensated out of order, as only information from the reference image is required for the compensation of any image. These properties make our method an ideal tool for intensity compensation of confocal microscopy images that suffer intensity loss due to absorption/scattering of light as well as photobleaching and the image can change structure from optical/temporal section-to-section due to changes in the depth of specimen or due to a live specimen. The proposed method was tested with a number of confocal microscopy image stacks and results are presented to demonstrate the effectiveness of the method.     

激光共焦扫描显微镜及其应用

介绍了共焦激光显微镜的基本光路、成像原理、关键技术及应用。     

Sensitivity of CFP/YFP and GFP/mCherry pairs to donor photobleaching on FRET determination by fluorescence lifetime imaging microscopy in living cells

Fluorescent protein-based FRET is a powerful method for visualizing protein-protein interactions and biochemical reactions in living cells. It can be difficult, however, to avoid photobleaching when observing fluorescent cells under the microscope, especially those expressing CFP. We compared the sensitivity of two protein-based FRET pairs to light-induced fluorescence changes in the donor, on FRET determination by fluorescence lifetime imaging microscopy (FLIM). Thanks to the very low excitation light levels of the time- and space-correlated single photon counting (TSCSPC) method, FLIM acquisitions were achieved without donor photobleaching. Here, we show that photobleaching of CFP by a mercury lamp under the microscope induced a decrease in the mean fluorescence lifetime, which interfered with FRET determination between CFP and YFP. Importantly, the range of light-induced variation of the mean fluorescence lifetime of CFP was not proportional to the decrease in the steady state fluorescence intensity and varied from cell to cell. The choice of the CFP/YFP pair therefore requires that the cells be observed and analyzed at very low light levels during the whole FRET experiment. In contrast, the GFP/mCherry pair provided an accurate FRET measurement by FLIM, even if some GFP photobleaching took place. We thus demonstrate that CFP can be an unreliable donor for FRET determination in living cells, due to its photosensitivity properties. We demonstrate that the GFP/mCherry pair is better suited for FRET measurement by FLIM in living cells than the CFP/YFP pair.     

MRT letter: high speed scanning has the potential to increase fluorescence yield and to reduce photobleaching

True confocal microscopy requires point-shaped illumination and detection. To generate an image, a diffraction limited spot is moved over the sample. Single spot scanning has suffered in the past from low image rates; a solution is the employment of very fast scanning devices (resonant scanners) for x-movement. In the process of introducing resonant scanning devices, it was found that both signal yield is improved and bleaching is decreased-in contrary to the assumed performance. This article will show by a simple and well understood model a straightforward explanation for the potential increase of signal yield and decrease in photobleaching. The time that is ruling the dose-rate effects is the effective time; a fluorochrome is illuminated. This time depends on the diameter of the spot that is moved over the sample and the speed at which the spot moves. In essence, the scan process causes a pulsed illumination of the fluorochromes. Various schemes of pulsed illumination are simulated with a fluorescence model. The model includes a dark state, where fluorochromes will exit the fluorescence process and slowly decay back into the ground state. Upon splitting a single dose into two pulses separated by a dark time-reflecting an increased scan speed-the amount of fluorescence emission is increased and bleaching is reduced. These results show a potential increase of fluorescence and a lower photobleaching upon higher scan speed. As illumination during the bleach-phase in a FRAP-experiment is similar to a light pulse, the findings also suggest to critically consider the very beginning of fluorescence recovery in terms of triplet relaxation process that potentially could falsify the measurements.     

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.     

Structure-orientated fluorescence photobleaching analysis: a method for double fluorescent labelling studies

Differences in the degree of photodegradation can be used for fluorophore identification in double fluorescently labelled specimens. Based on the use of morphological information, a noise-insensitive method is presented for discriminating between the fluorophores, assuming spatially uniform photodegradation. Separate images of the labelled structures can be obtained. Alternatively, with spatially nonuniform photodegradation, the photodynamics of one fluorophore — i.e. photodegradation, concentration associated quenching, etc. — in relation to its microenvironment can be investigated.     

Noise effects and filtering in controlled light exposure microscopy

Phototoxicity and photobleaching are major limitations of fluorescence live-cell microscopy. A straightforward way to limit phototoxicity and photobleaching is reduction of the excitation light dose, but this causes loss of image quality. In confocal fluorescence microscopy, the field of view is illuminated uniformly whereas in controlled light exposure microscopy, illumination is controlled per pixel on the basis of two illumination strategies. The controlled light exposure microscopy foreground strategy discriminates between bright and weak foreground. Bright foreground pixels are illuminated with a reduced light dose resulting in limited excitation of fluorophores and consequently limited phototoxicity and photobleaching. The controlled light exposure microscopy background strategy discriminates between foreground and background. Pixels that are judged to be background are also illuminated with a reduced light dose. The latter illumination strategy may introduce artefacts due to the stochastic character of photon flow. These artefacts are visible as erratic 'darker pixels' in the foreground with a lower pixel value than the neighbouring pixels. This paper describes a special adaptive image processing filter that detects and corrects most of the 'darker pixels'. It opens the possibility to use controlled light exposure microscopy even in high noise (low signal to noise ratio) imaging to further reduce phototoxicity and photobleaching.     

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.     

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。