Statistical evaluation of confocal microscopy images

BACKGROUND: The coefficient of variation (CV) is defined as the standard deviation (sigma) of the fluorescent intensity of a population of beads or pixels expressed as a proportion or percentage of the mean (mu) intensity (CV = sigma/mu). The field of flow cytometry has used the CV of a population of bead intensities to determine if the flow cytometer is aligned correctly and performing properly. In a similar manner, the analysis of CV has been applied to the confocal laser scanning microscope (CLSM) to determine machine performance and sensitivity. METHODS: Instead of measuring 10,000 beads using a flow cytometer and determining the CV of this distribution of intensities, thousands of pixels are measured from within one homogeneous Spherotech 10-microm bead. Similar to a typical flow cytometry population that consists of 10,000 beads, a CLSM scanned image consists of a distribution of pixel intensities representing a population of approximately 100,000 pixels. In order to perform this test properly, it is important to have a population of homogeneous particles. A biological particle usually has heterogeneous pixel intensities that correspond to the details in the biological image and thus shows more variability as a test particle. RESULTS: The bead CV consisting of a population of pixel intensities is dependent on a number of machine variables that include frame averaging, photomultiplier tube (PMT) voltage, PMT noise, and laser power. The relationship among these variables suggests that the machine should be operated with lower PMT values in order to generate superior image quality. If this cannot be achieved, frame averaging will be necessary to reduce the CV and improve image quality. There is more image noise at higher PMT settings, making it is necessary to average more frames to reduce the CV values and improve image quality. The sensitivity of a system is related to system noise, laser light efficiency, and proper system alignment. It is possible to compare different systems for system performance and sensitivity if the laser power is maintained at a constant value. Using this bead CV test, 1 mW of 488 nm laser light measured on the scan head yielded a CV value of 4% with a Leica TCS-SP1 (75-mW argon-krypton laser) and a CV value of 1.3% with a Zeiss 510 (25-mW argon laser). A biological particle shows the same relationship between laser power, averaging, PMT voltage, and CV as do the beads. However, because the biological particle has heterogeneous pixel intensities, there is more particle variability, which does not make as useful as a test particle. CONCLUSIONS: This CV analysis of a 10-microm Spherotech fluorescent bead can help determine the sensitivity in a confocal microscope and the system performance. The relationship among the factors that influence image quality is explained from a statistical endpoint. The data obtained from this test provides a systematic method of reducing noise and increasing image clarity. Many components of a CLSM, including laser power, laser stability, PMT functionality, and alignment, influence the CV and determine if the equipment is performing properly. Preliminary results have shown that the bead CV can be used to compare different confocal microscopy systems with regard to performance and sensitivity. The test appears to be analogous to CV tests made on the flow cytometer to assess instrument performance and sensitivity. Published 2001 Wiley-Liss, Inc.     

Evaluation of confocal microscopy system performance

BACKGROUND: The confocal laser scanning microscope (CLSM) has been used by scientists to visualize three-dimensional (3D) biological samples. Although this system involves lasers, electronics, optics, and microscopes, there are few published tests that can be used to assess the performance of this equipment. Usually the CLSM is assessed by subjectively evaluating a biological/histological test slide for image quality. Although there is a use for the test slide, there are many other components in the CLSM that need to be assessed. It would be useful if tests existed that produced reference values for machine performance. The aim of this research was to develop quality assurance tests to ensure that the CLSM was stable while delivering reproducible intensity measurements with excellent image quality. METHODS: Our ultimate research objective was to quantify fluorescence using a CLSM. To achieve this goal, it is essential that the CLSM be stable while delivering known parameters of performance. Using Leica TCS-SP1 and TCS-4D systems, a number of tests have been devised to evaluate equipment performance. Tests measuring dichroic reflectivity, field illumination, lens performance, laser power output, spectral registration, axial resolution, laser stability, photomultiplier tube (PMT) reliability, and system noise were either incorporated from the literature or derived in our laboratory to measure performance. These tests are also applicable to other manufacturer's systems with minor modifications. RESULTS: A preliminary report from our laboratory has addressed a number of the QA issues necessary to achieve CLSM performance. This report extends our initial work on the evaluation of CLSM system performance. Tests that were described previously have been modified and new tests involved in laser stability and sensitivity are described. The QA tests on the CLSM measured laser power, PMT function, dichroic reflection, spectral registration, axial registration, system noise and sensitivity, lens performance, and laser stability. Laser power stability varied between 3% and 30% due to various factors, which may include incompatibility of the fiber-optic polarization with laser polarization, thermal instability of the acoustical optical transmission filter (AOTF), and laser noise. The sensitivity of the system was measured using a 10-microm Spherotech bead and the PMTs were assessed with the CV concept (image noise). The maximum sensitivity obtainable on our TCS-SP1 system measured on the 10-microm Spherotech beads was approximately 4% for 488 nm, 2.5% for 568 nm, 20% for 647 nm, and 19% for 365 nm laser light. The values serve as a comparison to test machine sensitivity from the same or different manufacturers. CONCLUSIONS: QA tests are described on the CLSM to assess performance and ensure that reproducing data are obtained. It is suggested strongly that these tests be used in place of a biological/histological sample to evaluate system performance. The tests are more specific and can recognize instrument functionality and problems better than a biological/histological sample. Utilization of this testing approach will eliminate the subjective assessment of the CLSM and may allow the data from different machines to be compared. These tests are essential if one is interested in making intensity measurements on experimental samples as well as obtaining the best signal detection and image resolution from a CLSM. Published 2001 Wiley-Liss, Inc.     

Quality assessment of confocal microscopy slide based systems: performance.

BACKGROUND: All fluorescence slide-based cytometry detections systems basically include the following components: (1) an excitation light source, (2) intermediate optics, and (3) a detection device consisting of a CCD camera or a PMT. The optical principles employed is slide-based systems are similar to those of confocal microscopes (CLSM). METHODS: The following tests evaluated confocal equipment performance: dichroic reflectivity, field illumination, lens performance, laser power output, spectral registration, axial resolution, PMT reliability, and system noise. RESULTS: Quality assurance tests provide a basis to determine if the equipment is operating correctly. Laser power, PMTs function, dichroic reflection, spectral registration, axial registration, system noise and sensitivity, lens performance and laser stability were tested colocalization of UV and visible peaks of a bead should be less than 210 nm. Interference contrast optics decrease fluorescence resolution. CONCLUSIONS: QA tests that assess CLSM system performance are also applicable to other slide-based systems. By utilization this type of testing approach, the subjective nature of assessing the CLSM may be eliminated. These tests serve as guidelines for other investigators to ensure that their machines are providing data that is accurate with the necessary resolution, sensitivity and precision.     

Quality assessment of confocal microscopy slide-based systems: instability.

BACKGROUND: All slide-based fluorescence cytometry detections systems basically include an excitation light source, intermediate optics, and a detection device (CCD or PMT). Occasionally, this equipment becomes unstable, generating unreliable and inferior data. METHODS: A number of tests have been devised to evaluate equipment performance and instability. The following four instability tests are described: galvanometer scanning, stage drift, correct wavelength spectral detection, and long-term laser power. RESULTS: Quality assurance tests revealed that a confocal microscope can become unstable in the following parameters, yielding inaccurate data: laser power, PMTs functionality, spectrophotometer accuracy, galvanometer scanning and laser stability, and stage drift. Long-term laser power stability has been observed to vary greatly. CONCLUSIONS: Confocal systems can become unstable in the following parameters: long-term laser power, galvanometer scanning, spectrophotometer accuracy, and stage stability. Instability in any of these parameters will affect image quality. Laser power fluctuations result from either a defective Acousto-optic tunable filter or improper heat dissipation. Spectrophotometer instability will generate unreliable spectra data, extra light reflections, and poor image quality. Galvanometer scanning instability yields poor image quality while microscope stage drift results in a sample going out of the plane of focus. With minor modifications, these tests may be applicable to other slide-based systems.     

Reliability of confocal microscopy spectral imaging systems: use of multispectral beads.

BACKGROUND: There is a need for a standardized, impartial calibration, and validation protocol on confocal spectral imaging (CSI) microscope systems. To achieve this goal, it is necessary to have testing tools to provide a reproducible way to evaluate instrument performance. METHODS: We evaluated fluorescent spectral beads (FocalCheck) from Molecular Probes/Invitrogen that consist of four pairs with emissions between 500 and 725 nm and a europium macrocycle quantum dye bead. These bead tools compliment our previously published protocol for testing spectral imaging systems that used an inexpensive multi-ion discharge lamp (MIDL) that contains Hg(+), Ar(+), and inorganic fluorophores that emits distinct, stable spectral features. RESULTS: We acquired the spectra of the FocalCheck beads on a Zeiss 510 Meta, a Leica TCS-SP1, a Leica SP2 AOBS, an Olympus FV 1000, and a Nikon C1Si confocal systems and a PARISS microscopic spectral system and of the europium beads on the Leica TCS-SP1 and PARISS spectral imaging systems. A lack of performance with some equipment between 650 and 750 nm was identified using the far red pair of the FocalCheck beads. The position of the slider in front of PMT 2 that reflects light into PMT 1 and PMT 3 affected the measurement of all bead intensities. Unmixing algorithms were used to separate beads with different fluorochromes and separate two fluorochromes on the same bead. CONCLUSIONS: The FocalCheck multi-spectral beads yielded similar profiles on four CSI systems and a PARISS spectral system. The utilization of the spectral FocalCheck beads is helpful to evaluate proper spectral performance, especially in the far red region. Europium beads provide a very narrow spectrum that can help to identify machines that have spectral problems. The dyes located on individual beads or mixed together in ring-core configuration can be used as test particles to demonstrate spectral unmixing with various algorithms.     

Autofluorescent chalcedony in human brains from elderly patients

Abstract

Chalcedony, a microcrystalline form of silica (SiO₂), has been found in the human brains of elderly patients by using a standard optical petrographic microscope. We document here our visualization of chalcedony using a Leica TCS – SP2 confocal laser scanning microscope. Sections of human brain were collected after autopsy from elderly patients. The autofluorescent character of chalcedony allowed us to obtain three-dimensional images of the crystals and mature prismatic quartz (chalcedony) was observed. Chalcedony occurred as rhombohedral (trigonal) crystals approximately 30 μm in size distributed in patches or aggregates. A less mature silica polymorph of about 1–2 μm in size was detected near the crystals. This is the first time that biogenically-produced crystalline mineral as autofluorescent crystal aggregates has been observed in the human central nervous system of elderly patients using confocal laser scanning microscopy.     

Software controlling algorithms for the system performance optimization of confocal laser scanning microscope

The relative slow scanning speed of a galvanometer commonly used in a confocal laser scanning microscopy system can dramatically limit the system performance in scanning speed and image quality, if the data collection is simply synchronized with the galvanometric scanning. Several algorithms for the optimization of the galvanometric CLSM system performance are discussed in this work, with various hardware controlling techniques for the image distortion correction such as pixel delay and interlace line switching; increasing signal-to-noise ratio with data binning; or enhancing the imaging speed with region of interest imaging. Moreover, the pixel number can be effectively increased with Acquire-On-Fly scan, which can be used for the imaging of a large field-of-view with a high resolution.     

Localization and high-resolution imaging of cortical neurotransmitter compartments using confocal laser scanning microscopy: GABA and glutamate interactions in rat cortex.

This report compares the application of confocal laser scanning fluorescence microscopy with standard epifluorescence microscopy for the simultaneous localization of the neurotransmitters gamma-aminobutyric acid and glutamate in rat cerebral cortex. With this approach, sections of fixed rat brain are treated with primary antibodies against gamma-aminobutyric acid (rabbit-derived) and glutamate (mouse-derived), followed by treatment with fluorescein isothiocyanate-tagged donkey anti-rabbit and rhodamine-tagged goat anti-mouse secondary antibodies, respectively. The results demonstrate that images from immunofluorescence localizations with a confocal laser scanning microscope have superior resolution and contrast as a result of significant reductions of background flare caused by emission from out-of-focus structures in the field of view. The confocal microscope achieves this improved image quality by optically sectioning through a specimen at narrow planes of focus and then compiling a composite image of an object of interest. The composite image can be further enhanced by using various image processing options. The combined use of double immunofluorescence and confocal laser scanning microscopy provides an important means to simultaneously study the anatomical relationships of pre- and post-synaptic elements in a complex neural system.     

Confocal microscopy via reciprocal optical fibre image detection

We describe a compact form of confocal scanning microscope using a semiconductor laser. Confocal operation is ensured by the use of a single mode optical fibre for both launching the light into the microscope and collecting the signal from the object. The collected light is allowed to re-enter the laser and the image is detected as a modulation on the signal from the laser power monitor diode. Images are compared with those obtained from traditional point detectors. The alignment tolerances of the reciprocal scheme are found to be greatly reduced over conventional confocal systems.     

Measuring and interpreting point spread functions to determine confocal microscope resolution and ensure quality control

This protocol outlines a procedure for collecting and analyzing point spread functions (PSFs). It describes how to prepare fluorescent microsphere samples, set up a confocal microscope to properly collect 3D confocal image data of the microspheres and perform PSF measurements. The analysis of the PSF is used to determine the resolution of the microscope and to identify any problems with the quality of the microscope's images. The PSF geometry is used as an indicator to identify problems with the objective lens, confocal laser scanning components and other relay optics. Identification of possible causes of PSF abnormalities and solutions to improve microscope performance are provided. The microsphere sample preparation requires 2-3 h plus an overnight drying period. The microscope setup requires 2 h (1 h for laser warm up), whereas collecting and analyzing the PSF images require an additional 2-3 h.     

Scanning Microphotolysis: Three-Dimensional Diffusion Measurement and Optical Single-Transporter Recording

Scanning microphotolysis (SCAMP) is a combination of fluorescence microphotolysis and confocal laser scanning microscopy. A laser scanning microscope is equipped with an optical switch able to modulate the power or/and wavelength of the laser beam in less than a microsecond while a dedicated computer program is employed to precisely coordinate scanning process and laser beam modulation. By these means it becomes possible to vary the power or/and wavelength of the laser beam during scanning at a precision of one resolution element. Patterns of almost arbitrary design can be written into the object by photolysis, e.g., photobleaching or photoactivation. The dissipation of the photolysis pattern by diffusion or other types of molecular transport can be followed at confocal resolution and used to characterize the transport process. SCAMP can be employed in conjunction with single-photon or multiphoton excitation. Furthermore, it can be easily installed on virtually any confocal laser scanning microscope. We summarize at first the conceptual and practical basis of SCAMP. Then, two novel applications are discussed: (i) measurements of translational diffusion coefficients in truly three-dimensional systems at diffraction-limited resolution, and (ii) optical recording of single transporters in membrane patches.     

An evaluation of confocal versus conventional imaging of biological structures by fluorescence light microscopy

Scanning confocal microscopes offer improved rejection of out-of-focus noise and greater resolution than conventional imaging. In such a microscope, the imaging and condenser lenses are identical and confocal. These two lenses are replaced by a single lens when epi-illumination is used, making confocal imaging particularly applicable to incident light microscopy. We describe the results we have obtained with a confocal system in which scanning is performed by moving the light beam, rather than the stage. This system is considerably faster than the scanned stage microscope and is easy to use. We have found that confocal imaging gives greatly enhanced images of biological structures viewed with epifluorescence. The improvements are such that it is possible to optically section thick specimens with little degradation in the image quality of interior sections.     

用激光扫描共聚焦显微镜观察雪松花粉和花粉管

为更直观地观察和显示花粉和花粉管中细胞结构及其细胞核的状态与行为。雪松花粉和花粉管经卡诺液固定,分别以埃氏苏木精、曙红、Hoechst 33243单染和曙红-Hoechst 33342双染后,用冬青油整体透明,在激光扫描共聚焦显微镜下观察。4种染色法观察效果不同;以曙红-Hoechst 33342双染的样品观察效果最佳,在紫外光激发下清晰地显示出细胞核,在488 nm激光激发下不仅能清晰看到花粉和花粉管壁结构,且能分辨管细胞、柄细胞及体细胞的结构特点和空间位置关系。建立了一种快速简便的适于在激光扫描共聚焦显微镜下观察花粉和花粉管中成员细胞结构及其细胞核的状态、行为的制片技术;激光扫描共聚焦显微镜具有独特的共轭成像装置、连续光学扫描、图像三维重组和多通道检测等功能,极好地展示了雪松花粉和花粉管的结构特点,相比于传统的光学显微镜和荧光显微镜,其观察到的图像更清晰、更直观、更具立体感。     

Morphology and gelation of thermosensitive chitosan hydrogels

The morphology of physical hydrogels is often difficult to examine due to the delicate nature of the system and therefore has not been studied in detail. Chitosan/GP (glycerophosphate salt) is a significant hydrogel in the biomedical and cosmetic fields as it is thermosensitive and contains less than 5% polysaccharide. The morphology of this system was examined with laser scanning confocal microscopy (LSCM) to image the gel morphology. The images indicate that the gel is quite heterogeneous, and power spectra reveal a fractal-like morphology. A study of composition found that increasing chitosan concentration increased the amount of polymer-rich phase present in the gel, and that the smallest aggregates decreased in size.     

Real-time detection of DNA hybridization on microarray using a CCD-based imaging system equipped with a rotated microlens array disk

This work describes a novel charge-coupled device (CCD)-based imaging system (MB Biochip Reader?) for real-time detection of DNA hybridization to DNA microarrays. The MB Biochip Reader? consisted of a laser light source (532 nm), a microlens array for generation of a multi-beam laser, and a CCD for 2-D signal imaging. The MB Biochip Reader? with a rotated microlens array, allowed large-field imaging (6.2 mm × 7.6 mm with 6.45 μm resolution) with fast time-resolution at 0.2 s without speckle noise. Furthermore, real-time detection of DNA hybridization, which is sufficient to obtain accurate data from tens of thousands of array element per field, was successfully performed without the need for laser scanning. The performance of the MB Biochip Reader? for DNA microarray imaging was similar to the commercially available photomultiplier tube (PMT)-based microarray scanner, ScanArray Lite. The system potentially could be applied toward real-time analysis in many other fluorescent techniques in addition to real-time DNA microarray analysis.     

Profound influence of microarray scanner characteristics on gene expression ratios: analysis and procedure for correction

Background  

High throughput gene expression data from spotted cDNA microarrays are collected by scanning the signal intensities of the corresponding spots by dedicated fluorescence scanners. The major scanner settings for increasing the spot intensities are the laser power and the voltage of the photomultiplier tube (PMT). It is required that the expression ratios are independent of these settings. We have investigated the relationships between PMT voltage, spot intensities, and expression ratios for different scanners, in order to define an optimal scanning procedure.     

激光扫描共聚焦显微镜荧光探针的选择和应用

激光扫描共聚焦显微镜是检测生物荧光信号的最新技术手段。不仅广泛用于荧光定性、定量测量,还可用于活细胞动态荧光监测、组织细胞断层扫描、三维图象重建、共聚焦图象分析、荧光光漂白恢复、激光显微切割手术等。本文拟就激光扫描共聚焦显微镜常用的检测内容及其相关荧光探针的选择和应用做一简单的介绍。     

Anti-Fading Agents for Confocal Immunofluorescence: Colocalization of Nuclear Polypeptides

We evaluated the performance of four anti-fading agents during acquisition of multiple optical sections near the widest diameter of Drosophila accessory gland nuclei using indirect immunofluorescence and confocal laser scanning microscopy. Two commercially available agents, Vectashield® and SlowFade® showed anti-fading properties that alleviated fluorochrome fading associated with the acquisition of multiple fluorescent optical Z-series from a single specimen by a confocal laser scanning system. Using these reagents, we were able to colocalize polypeptides through immunostained whole Drosophila nuclei.     

微流控芯片监测绿色荧光蛋白在枯草芽孢杆菌中的表达

目前主要使用激光共聚焦扫描显微镜观察绿色荧光蛋白的表达,但需要昂贵的仪器并耗费大量时间。本研究开发了一种新型激光诱导的微流芯片检测系统来监测绿色荧光蛋白在枯草芽孢杆菌中的表达。该系统主要由激光装置、光路系统、微流控芯片、光电倍增管和计算机处理系统等5部分组成。对该系统的测试结果显示,随着诱导强度的增强监测信号峰也随之增强,并且与激光共聚焦显微镜观察的结果一致。利用该芯片系统能够快速准确地筛选和鉴定用绿色荧光蛋白作为标记的细胞克隆,可以替代PCR鉴定方法。但该系统仅仅能够监测表达强度,不能够满足蛋白定位等高水平研究,因此,该系统适合应用于环境的微生物监测、药物筛选和其他无需观察蛋白定位等研究。     

Confocal scanning optical microscopy and three-dimensional imaging

Summary— Confocal scanning optical microscopy has significant advantages over conventional fluorescence microscopy: it rejects the out-of-locus light and provides a greater resolution than the wide-field microscope. In laser scanning optical microscopy, the specimen is scanned by a diffraction-limited spot of laser light and the fluorescence emission (or the reflected light) is focused onto a photodetector. The imaged point is then digitized, stored into the memory of a computer and displayed at the appropriate spatial position on a graphic device as a part of a two-dimensional image. Thus, confocal scanning optical microscopy allows accurate non-invasive optical sectioning and further three-dimensional reconstruction of biological specimens. Here we review the recent technological aspects of the principles and uses of the confocal microscope, and we introduce the different methods of three-dimensional imaging.