基于单波长激发的定量FRET成像

本文发展了一种针对于固定FRET质粒的单波长激发的E-FRET方法(SDW-E-FRET)。相比于EFRET方法,SDW-E-FRET只需要测量供体激发时供体通道的荧光强度(IDD)和FRET通道的荧光强度(IDA),因此该方法可以实现活细胞的快速定量FRET成像。结合双通道荧光显微成像系统,该方法无需任何机械切换,定量FRET成像的速度只取决于CCD相机的成像速度,因而特别适合活细胞实时动态定量FRET成像。在本研究小组发展的双通道荧光显微镜平台上,应用SDW-E-FRET方法测量了C5V和C17V的FRET效率,得到了与其它方法测量的一致的结果。     

单个活细胞中生物分子动态行为的FRET实时检测

分别采用两种不同绿色荧光蛋白(green fluorescent prote in,GFP)突变体作为荧光共振能量转移(fluo-rescence resonance energy transfer,FRET)对的供体和受体,并利用分子生物学技术将供体和受体分子分别与特定的生物分子融合,这种技术已经成为在单个活细胞中实时长时间检测蛋白质间的动态相互作用的主要技术。主要介绍了基于GFPs的FRET技术在单个活细胞中实时长时间研究生物分子动态行为的应用。     

基于GFP的FRET应用

绿色荧光蛋白（GFP）是一种活性荧光标记,已被用来研究基因表达、分子定位,蛋白质折叠和转运;荧光共振能量转移（FRET）是一种无损伤的光学检测方法,能检测到小于纳米的距离变化。将GFP的活性定位标记功能与FRET的高分辨率相结合。为活体研究生物分子的功能和命运开创了新的篇章。作者在介绍GFP和FRET原理的基础上,综述了基于GFP的FRET在蛋白酶活性,蛋白质间相互作用 构象改变研究中的应用。     

一种改进的荧光共振能量转移方法分析同质二聚体内蛋白质-蛋白质相互作用

荧光共振能量转移(fluorescence resonance energy transfer, FRET)技术日益广泛的应用于检测活细胞中分子内和分子间的相互作用. 由于FRET仅发生于相互作用的供体和受体,即供体-受体复合物之间,所以检测的FRET信号必须经标准化处理以去除供体受体比例和浓度的影响然后才能够进行FRET的比较研究. 由于供体和受体的比例相同,分子内FRET的检测较为简单;而分子间FRET的检测存在更多的不确定因素,导致现有的方法很难精确定量.根据1类特殊的分子间相互作用,同质二聚体的独特特征,推导出供体 受体复合物的含量,进而开发了1种同质二聚体分子间FRET的精确定量的方法,以1种同质二聚体,雌激素受体α(estrogen receptor alpha, ERα)为供体和受体对,通过和其它的方法比较,证实了该方法用于FRET检测可获得更可靠的结果.     

复合探针荧光定量PCR方法的建立

为了对特定基因进行实时检测,根据荧光能量转移(FRET)原理,设计及合成了一种新的FRET复合探针,该探针由一条长的荧光杂交探针和短的淬灭探针构成,其中荧光探针5′端接一荧光素分子,3′端接一延伸阻断分子磷酸,淬灭探针3′端连接一个淬灭分子对甲基红,淬灭探针与荧光探针5′端互补,无模板时,该探针杂交形成复合探针。无荧光产生,当有模板时,荧光探针与模板杂交,荧光不能被淬灭,产生的荧光与模板量成正比。根据复合探针的反应原理,研究了该探针的FRET性质及影响因素包括淬灭探针及扩增片段长度、荧光探针与淬灭探针的合适比例及镁离子浓度。实验结果显示淬灭探针及扩增片段长度对复合探针的作用有明显的影响,本实验采用淬灭探针长21个核苷酸,扩增片段长127bp,荧光探针与淬灭探针的合适比例为1：1,镁离子浓度为3mmo1／L,可获得最佳的反应体系;该复合探针合成简单,淬灭彻底,具有良好的准确性与特异性,敏感性达10^2拷贝,并具有较宽的动力学定量范围,可对10^2—10^9拷贝范围内的待检样品进行准确的定量。复合探针技术可应用于病毒感染水平、转基因拷贝数及单核苷酸多态性等检测。     

生物大分子相互作用检测技术新进展———三色荧光级联荧光共振能量转移技术

荧光共振能量转移(fluorescenceresonanceenergytransfer,FRET),是指能量从一种受激发的荧光基团(fluorophore)以非辐射的方式转移到另一种荧光基团的物理现象.FRET的能量转移效率是两个荧光基团间距离的函数,并对此距离十分敏感,它的有效响应距离一般在1～10nm之间,因而可被用于测定原子间及分子间的距离.这一特点使FRET技术在大分子构象变化、大分子之间相互作用、细胞信号通路等研究中发挥重要作用,成为生物医学研究中的重要方法.但细胞内的生物学过程常常涉及多于两个的大分子间相互作用,二色荧光基团的FRET技术不能满足这种生物学研究的需求.最近,两个研究小组在这方面取得突破,建立了分别基于共聚焦显微镜和流式细胞仪的三色荧光级联FRET技术.这一技术的出现将会极大地促进生物学及相关研究领域的发展.     

一种检测马尔尼菲青霉菌实时荧光定量PCR方法的建立和应用

目的:建立一种检测马尔尼菲青霉菌的实时荧光定量PCR的方法。方法:针对马尔尼菲青霉菌5.8S rRNA设计特异性PCR引物,采用核酸荧光染料SYBR GreenⅠ进行实时荧光定量PCR检测,探讨该方法的灵敏度和特异性,并进行临床样品检测验证。结果:该方法的特异性较好,与该菌属内的其他细菌间无交叉反应;灵敏度可检测出10个细胞/mL全血,在检测范围内线性良好,相关系数R2=0.981。临床样品检测和传统的培养方法结果完全相符。结论:该方法特异性好,灵敏度高,操作简单,检测时间短;临床样品检测具有很好的准确性,从本研究的结果显示实时荧光定量PCR方法在检测马尔尼菲青霉菌中的应用可以大大缩短临床的诊断时间,提高临床诊断的准确度和效率。     

应用荧光实时定量PCR方法检测重组慢病毒滴度及其感染效率

慢病毒载体已经广泛应用于动物模型中基因治疗的研究和转基因动物的制备．而准确地测定重组慢病毒的滴度和感染效率是其关键步骤．通过荧光实时定量PCR的方法定量分析重组慢病毒的颗粒数以及病毒的活性滴度,并以GFP报告基因的方法作为对照来验证定量PCR方法的准确性．研究结果显示,应用荧光实时定量PCR法与GFP报告基因法测定得到的病毒活性滴度成正相关,而且前者可以更加准确地测定病毒滴度和病毒感染效率．     

小波变换及滚球算法在单分子荧光能量共振转移图像分析中的应用

单分子荧光共振能量转移技术是通过检测单个分子内的荧光供体及受体间荧光能量转移的效率来研究分子构象的变化．要得到这些生物大分子的信息就需要对大量的单分子信号进行统计分析,人工分析这些信息,既费时费力又不具备客观性和可重复性,因此本文将小波变换及滚球算法应用到单分子荧光能量共振转移图像中对单分子信号进行统计分析．在保证准确检测到单分子信号的前提下,文章对滚球算法和小波变换算法处理图像后的线性进行了分析,结果表明,滚球算法和小波变换算法不但能够很好地去除单分子FRET图像的背景噪声,同时还能很好地保持单分子荧光信号的线性．最后本文还利用滚球算法处理单分子FRET图像及统计15 bp DNA的FRET效率的直方图,通过计算得到了15 bp DNA的FRET效率值．     

用绿色荧光蛋白（GFP）作为报告分子筛选有效的siRNA

 建立一种利用绿色荧光蛋白（GFP）作为报告分子筛选能有效抑制目的基因表达的siRNA的方法.以巨噬细胞移动抑制因子（MIF）基因为研究对象,筛选能有效沉默MIF表达的质粒载体介导的siRNA.构建拥有同一Kozak共有翻译启始序列、翻译启始密码子ATG的MIF-GFP融合表达载体pEGFP-MIF.分别将3个靶向MIF的siRNA表达质粒与pEGFP-MIF共转化HEK293细胞,在荧光显微镜下观察HEK293细胞中GFP的表达,并用荧光定量PCR检测HEK293细胞中MIF mRNA的表达水平.同时,将MIF siRNA表达质粒分别与MIF表达载体共转化HEK293细胞,用荧光定量PCR检测HEK293细胞中MIF mRNA的表达水平.定量PCR结果显示,GFP表达低的细胞中,MIF mRNA的表达也明显降低;利用pEGFP-MIF和MIF表达载体筛选到的有效MIF siRNA的结果一致.因此,建立了目的基因与GFP融合表达,以GFP作为报告分子来筛选抑制目的基因表达siRNA的方法,并为进行多个基因的有效siRNA的筛选提供解决方案.     

Quantitative fluorescence resonance energy transfer measurements using fluorescence microscopy.

Fluorescence resonance energy transfer (FRET) is a technique used for quantifying the distance between two molecules conjugated to different fluorophores. By combining optical microscopy with FRET it is possible to obtain quantitative temporal and spatial information about the binding and interaction of proteins, lipids, enzymes, DNA, and RNA in vivo. In conjunction with the recent development of a variety of mutant green fluorescent proteins (mtGFPs), FRET microscopy provides the potential to measure the interaction of intracellular molecular species in intact living cells where the donor and acceptor fluorophores are actually part of the molecules themselves. However, steady-state FRET microscopy measurements can suffer from several sources of distortion, which need to be corrected. These include direct excitation of the acceptor at the donor excitation wavelengths and the dependence of FRET on the concentration of acceptor. We present a simple method for the analysis of FRET data obtained with standard filter sets in a fluorescence microscope. This method is corrected for cross talk (any detection of donor fluorescence with the acceptor emission filter and any detection of acceptor fluorescence with the donor emission filter), and for the dependence of FRET on the concentrations of the donor and acceptor. Measurements of the interaction of the proteins Bcl-2 and Beclin (a recently identified Bcl-2 interacting protein located on chromosome 17q21), are shown to document the accuracy of this approach for correction of donor and acceptor concentrations, and cross talk between the different filter units.     

Modelling Förster resonance energy transfer (FRET) using anisotropy resolved multi-dimensional emission spectroscopy (ARMES)

BackgroundFörster Resonance Energy Transfer (FRET) is widely used to study the structure and dynamics of biomolecular systems and also causes the non-linear fluorescence response observed in multi-fluorophore proteins. Accurate FRET analysis, in terms of measuring changes in donor and acceptor spectra and energy transfer efficiency is therefore critical.MethodsWe demonstrate a novel quantitative FRET analysis using anisotropy resolved multidimensional emission spectroscopy (ARMES) in a Human Serum Albumin (HSA) and 1,8-anilinonaphathalene sulfonate (ANS) model. ARMES combines 4D measurement of polarized excitation emission matrices (pEEM) with multivariate data analysis to spectrally resolve contributing fluorophores. Multivariate analysis (Parallel Factor, PARAFAC and restricted Tucker3) was used to resolve fluorophore contributions and for modelling the quenching of HSA emission and the HSA-ANS interactions.ResultspEEM spectra were modelled using Tucker3 which accommodates non-linearities introduced by FRET and a priori chemical knowledge was used to optimise the solution, thus resolving three components: HSA emission, ANS emission from indirect FRET excitation, and ANS emission from direct excitation. Perpendicular emission measurements were more sensitive to indirectly excited acceptor emission. PARAFAC modelling of HSA, donor emission, separated ANS FRET interacting (Tryptophan) and non-interacting (Tyrosine) components. This enabled a new way of calculating quenching constants using the multi-dimensional emission of individual donor fluorophores.ConclusionsFRET efficiency could be calculated using the multi-dimensional, resolved emission of the interacting donor fluorophores only which yielded higher ET efficiencies compared to conventional methods.General significanceShows the potential of multidimensional fluorescence measurements and data analysis for more accurate FRET modelling in proteins.     

Multiplexed FRET to image multiple signaling events in live cells

We report what to our knowledge is a novel approach for simultaneous imaging of two different Förster resonance energy transfer (FRET) sensors in the same cell with minimal spectral cross talk. Previous methods based on spectral ratiometric imaging of the two FRET sensors have been limited by the availability of suitably bright acceptors for the second FRET pair and the spectral cross talk incurred when measuring in four spectral windows. In contrast to spectral ratiometric imaging, fluorescence lifetime imaging (FLIM) requires measurement of the donor fluorescence only and is independent of emission from the acceptor. By combining FLIM-FRET of the novel red-shifted TagRFP/mPlum FRET pair with spectral ratiometric imaging of an ECFP/Venus pair we were thus able to maximize the spectral separation between our chosen fluorophores while at the same time overcoming the low quantum yield of the far red acceptor mPlum. Using this technique, we could read out a TagRFP/mPlum intermolecular FRET sensor for reporting on small Ras GTP-ase activation in live cells after epidermal growth factor stimulation and an ECFP/Venus Cameleon FRET sensor for monitoring calcium transients within the same cells. The combination of spectral ratiometric imaging of ECFP/Venus and high-speed FLIM-FRET of TagRFP/mPlum can thus increase the spectral bandwidth available and provide robust imaging of multiple FRET sensors within the same cell. Furthermore, since FLIM does not require equal stoichiometries of donor and acceptor, this approach can be used to report on both unimolecular FRET biosensors and protein-protein interactions with the same cell.     

Polarized fluorescence resonance energy transfer microscopy

Current methods for fluorescence resonance energy transfer (FRET) microscopy of living cells involve taking a series of images with alternating excitation colors in separate camera exposures. Here we present a new FRET method based on polarization that requires only one camera exposure and thereby offers the possibility for better time resolution of dynamic associations among subcellular components. Polarized FRET (p-FRET) uses a simultaneous combination of excitation wavelengths from two orthogonally polarized sources, along with an emission channel tri-image splitter outfitted with appropriate polarizers, to concurrently excite and collect fluorescence from free donors, free acceptors, and FRET pairs. Based upon the throughput in each emission channel as premeasured on pure samples of each of the three species, decoupling of an unknown sample's three polarized fluorescence images can be performed to calculate the pixel-by-pixel concentrations of donor, acceptor, and FRET pairs. The theory of this approach is presented here, and its feasibility is experimentally confirmed by measurements on mixtures of cyan fluorescent protein (CFP), citrine ((Cit) a yellow fluorescent protein variant), and linked fusion proteins (CFP-L16-Cit, CFP-L7-Cit, CFP-L54-Cit) in living cells. The effects of shot noise, acceptor polarization, and FRET efficiency on the statistical accuracy of p-FRET experimental results are investigated by a noise-simulation program.     

Protein localization in living cells and tissues using FRET and FLIM

Interacting proteins assemble into molecular machines that control cellular homeostasis in living cells. While the in vitro screening methods have the advantage of providing direct access to the genetic information encoding unknown protein partners, they do not allow direct access to interactions of these protein partners in their natural environment inside the living cell. Using wide-field, confocal, or two-photon (2p) fluorescence resonance energy transfer (FRET) microscopy, this information can be obtained from living cells and tissues with nanometer resolution. One of the important conditions for FRET to occur is the overlap of the emission spectrum of the donor with the absorption spectrum of the acceptor. As a result of spectral overlap, the FRET signal is always contaminated by donor emission into the acceptor channel and by the excitation of acceptor molecules by the donor excitation wavelength. Mathematical algorithms are required to correct the spectral bleed-through signal in wide-field, confocal, and two-photon FRET microscopy. In contrast, spectral bleed-through is not an issue in FRET/FLIM imaging because only the donor fluorophore lifetime is measured; also, fluorescence lifetime imaging microscopy (FLIM) measurements are independent of excitation intensity or fluorophore concentration. The combination of FRET and FLIM provides high spatial (nanometer) and temporal (nanosecond) resolution when compared to intensity-based FRET imaging. In this paper, we describe various FRET microscopy techniques and its application to protein-protein interactions.     

OS-FRET: a new one-sample method for improved FRET measurements

Fluorescence resonance energy transfer (FRET) is a powerful tool for studying macromolecular assemblies in vitro under near-physiological conditions. Here we present a new type of one-sample FRET (OS-FRET) method employing a novel, nonfluorescent methanethiosulfonate-linked acceptor that can be reversibly coupled to a target sulfhydryl residue via a disulfide bond. After the quenched donor emission is quantitated, the acceptor is removed by reduction, allowing measurement of unquenched donor emission in the same sample. Previous one-sample methods provide distinct advantages in specific FRET applications. The new OS-FRET method is a generalizable spectrochemical approach that can be applied to macromolecular systems lacking essential disulfide bonds and eliminates the potential systematic errors of some earlier one-sample methods. In addition, OS-FRET enables quantitative FRET measurements in virtually any fluorescence spectrometer or detection device. Compared to conventional multisample FRET methods, OS-FRET conserves sample, increases the precision of data, and shortens the time per measurement. The utility of the method is illustrated by its application to a protein complex of known structure formed by CheW and the P4-P5 fragment of CheA, both from Thermotoga maritima. The findings confirm the practicality and advantages of OS-FRET. Anticipated applications of OS-FRET include analysis of macromolecular structure, binding and conformational dynamics, and high-throughput screening for interactions and inhibitors.     

Pulsed interleaved excitation

In this article, we demonstrate the new method of pulsed interleaved excitation (PIE), which can be used to extend the capabilities of multiple-color fluorescence imaging, fluorescence cross-correlation spectroscopy (FCCS), and single-pair fluorescence resonance energy transfer (spFRET) measurements. In PIE, multiple excitation sources are interleaved such that the fluorescence emission generated from one pulse is complete before the next excitation pulse arrives. Hence, the excitation source for each detected photon is known. Typical repetition rates used for PIE are between approximately 1 and 50 MHz. PIE has many applications in various fluorescence methods. Using PIE, dual-color measurements can be performed with a single detector. In fluorescence imaging with multicolor detection, spectral cross talk can be removed, improving the contrast of the image. Using PIE with FCCS, we can eliminate spectral cross talk, making the method sensitive to weaker interactions. FCCS measurements with complexes that undergo FRET can be analyzed quantitatively. Under specific conditions, the FRET efficiency can be determined directly from the amplitude of the measured correlation functions without any calibration factors. We also show the application of PIE to spFRET measurements, where complexes that have low FRET efficiency can be distinguished from those that do not have an active acceptor.     

Confocal microscopic dual-laser dual-polarization FRET (2polFRET) at the acceptor side for correlating rotations at different distances on the cell surface

Relationship of donor and acceptor fluorescence anisotropies as well as efficiency of fluorescence resonance energy transfer (FRET) has been investigated in a confocal microscope in the context of FRET systems comprised of donor and acceptor-labeled MHCI and MHCII receptors on the surface of Kit-225 K6 human T-cells. The measurements have been carried out in a 2-laser, 5-signal platform where the total donor fluorescence intensity and 2 acceptor fluorescence intensities with their anisotropies – one at the donor's excitation wavelength, the other at the acceptor's excitation wavelength – have been detected. This configuration enabled the determination of FRET efficiency and correlating it with the two acceptor fluorescence anisotropies as a kind of calibration. Estimations for the FRET-enhanced donor fluorescence anisotropy, the directly excited acceptor fluorescence anisotropy, and the fluorescence anisotropy of sensitized emission have been obtained. Procedures for determining FRET by measuring only the total donor intensity and the acceptor intensity and its anisotropy, or two acceptor intensities and their anisotropies have been elaborated, the errors of which have been estimated based on the fluorescence anisotropy values obtained in the calibration with the method of flow cytometric energy transfer (FCET).The combined detection of the donor and acceptor fluorescence anisotropies enabled also the determination of the lower and upper limits of the orientation factor for FRET (κ²). An increase in range for κ² with increasing FRET efficiency has been observed, with average κ² values different from the dynamic random average of 2/3. These observations call for the need of κ² determination in proximity measurements, where the donor and acceptor orientations are not predictable.An increasing range of κ² with increasing intermolecular proximity of the MHCI and MHCII receptors has been observed. This indicates that molecular flexibility in the clusters of the MHCI and MHCII receptors reduces with increasing cluster density, i.e. a “fluidity gradient” exists in the clusters. More specifically, the local density dependent flexibility can also be taken as a direct proof for that the association of these receptors is non-random, but mediated by some type of physical interaction, a finding as a benefit of FRET detection by polarization spectroscopy.Two new quantities – the quenched donor fluorescence anisotropy and a fluorescence anisotropy analogue, the “dissymmetry index” of the polarized FRET efficiency components – have also been introduced for the characterization of the orientational dynamics of the excited state during FRET.     

Quantitative time domain analysis of lifetime‐based Förster resonant energy transfer measurements with fluorescent proteins: Static random isotropic fluorophore orientation distributions

Förster resonant energy transfer (FRET) measurements are widely used to obtain information about molecular interactions and conformations through the dependence of FRET efficiency on the proximity of donor and acceptor fluorophores. Fluorescence lifetime measurements can provide quantitative analysis of FRET efficiency and interacting population fraction. Many FRET experiments exploit the highly specific labelling of genetically expressed fluorescent proteins, applicable in live cells and organisms. Unfortunately, the typical assumption of fast randomization of fluorophore orientations in the analysis of fluorescence lifetime‐based FRET readouts is not valid for fluorescent proteins due to their slow rotational mobility compared to their upper state lifetime. Here, previous analysis of effectively static isotropic distributions of fluorophore dipoles on FRET measurements is incorporated into new software for fitting donor emission decay profiles. Calculated FRET parameters, including molar population fractions, are compared for the analysis of simulated and experimental FRET data under the assumption of static and dynamic fluorophores and the intermediate regimes between fully dynamic and static fluorophores, and mixtures within FRET pairs, is explored. Finally, a method to correct the artefact resulting from fitting the emission from static FRET pairs with isotropic angular distributions to the (incorrect) typically assumed dynamic FRET decay model is presented.      

Scanning near-field fluorescence resonance energy transfer microscopy

A new microscopic technique is demonstrated that combines attributes from both near-field scanning optical microscopy (NSOM) and fluorescence resonance energy transfer (FRET). The method relies on attaching the acceptor dye of a FRET pair to the end of a near-field fiber optic probe. Light exiting the NSOM probe, which is nonresonant with the acceptor dye, excites the donor dye introduced into a sample. As the tip approaches the sample containing the donor dye, energy transfer from the excited donor to the tip-bound acceptor produces a red-shifted fluorescence. By monitoring this red-shifted acceptor emission, a dramatic reduction in the sample volume probed by the uncoated NSOM tip is observed. This technique is demonstrated by imaging the fluorescence from a multilayer film created using the Langmuir-Blodgett (LB) technique. The film consists of L-alpha-dipalmitoylphosphatidylcholine (DPPC) monolayers containing the donor dye, fluorescein, separated by a spacer group of three arachidic acid layers. A DPPC monolayer containing the acceptor dye, rhodamine, was also transferred onto an NSOM tip using the LB technique. Using this modified probe, fluorescence images of the multilayer film reveal distinct differences between images collected monitoring either the donor or acceptor emission. The latter results from energy transfer from the sample to the NSOM probe. This method is shown to provide enhanced depth sensitivity in fluorescence measurements, which may be particularly informative in studies on thick specimens such as cells. The technique also provides a mechanism for obtaining high spatial resolution without the need for a metal coating around the NSOM probe and should work equally well with nonwaveguide probes such as atomic force microscopy tips. This may lead to dramatically improved spatial resolution in fluorescence imaging.