Fluorescence Lifetime Readouts of Troponin-C-Based Calcium FRET Sensors: A Quantitative Comparison of CFP and mTFP1 as Donor Fluorophores

We have compared the performance of two Troponin-C-based calcium FRET sensors using fluorescence lifetime read-outs. The first sensor, TN-L15, consists of a Troponin-C fragment inserted between CFP and Citrine while the second sensor, called mTFP-TnC-Cit, was realized by replacing CFP in TN-L15 with monomeric Teal Fluorescent Protein (mTFP1). Using cytosol preparations of transiently transfected mammalian cells, we have measured the fluorescence decay profiles of these sensors at controlled concentrations of calcium using time-correlated single photon counting. These data were fitted to discrete exponential decay models using global analysis to determine the FRET efficiency, fraction of donor molecules undergoing FRET and calcium affinity of these sensors. We have also studied the decay profiles of the donor fluorescent proteins alone and determined the sensitivity of the donor lifetime to temperature and emission wavelength. Live-cell fluorescence lifetime imaging (FLIM) of HEK293T cells expressing each of these sensors was also undertaken. We confirmed that donor fluorescence of mTFP-TnC-Cit fits well to a two-component decay model, while the TN-L15 lifetime data was best fitted to a constrained four-component model, which was supported by phasor analysis of the measured lifetime data. If the constrained global fitting is employed, the TN-L15 sensor can provide a larger dynamic range of lifetime readout than the mTFP-TnC-Cit sensor but the CFP donor is significantly more sensitive to changes in temperature and emission wavelength compared to mTFP and, while the mTFP-TnC-Cit solution phase data broadly agreed with measurements in live cells, this was not the case for the TN-L15 sensor. Our titration experiment also indicates that a similar precision in determination of calcium concentration can be achieved with both FRET biosensors when fitting a single exponential donor fluorescence decay model to the fluorescence decay profiles. We therefore suggest that mTFP-based probes are more suitable for FLIM experiments than CFP-based probes.     

Combination of novel green fluorescent protein mutant TSapphire and DsRed variant mOrange to set up a versatile in planta FRET-FLIM assay

Förster resonance energy transfer (FRET) measurements based on fluorescence lifetime imaging microscopy (FLIM) are increasingly being used to assess molecular conformations and associations in living systems. Reduction in the excited-state lifetime of the donor fluorophore in the presence of an appropriately positioned acceptor is taken as strong evidence of FRET. Traditionally, cyan fluorescent protein has been widely used as a donor fluorophore in FRET experiments. However, given its photolabile nature, low quantum yield, and multiexponential lifetime, cyan fluorescent protein is far from an ideal donor in FRET imaging. Here, we report the application and use of the TSapphire mutant of green fluorescent protein as an efficient donor to mOrange in FLIM-based FRET imaging in intact plant cells. Using time-correlated single photon counting-FLIM, we show that TSapphire expressed in living plant cells decays with lifetime of 2.93 ± 0.09 ns. Chimerically linked TSapphire and mOrange (with 16-amino acid linker in between) exhibit substantial energy transfer based on the reduction in the lifetime of TSapphire in the presence of the acceptor mOrange. Experiments performed with various genetically and/or biochemically known interacting plant proteins demonstrate the versatility of the FRET-FLIM system presented here in different subcellular compartments tested (cytosol, nucleus, and at plasma membrane). The better spectral overlap with red monomers, higher photostability, and monoexponential lifetime of TSapphire makes it an ideal FRET-FLIM donor to study protein-protein interactions in diverse eukaryotic systems overcoming, in particular, many technical challenges encountered (like autofluorescence of cell walls and fluorescence of pigments associated with photosynthetic apparatus) while studying plant protein dynamics and interactions.Single- and dual-color fluorescence imaging with intrinsically fluorescent proteins is increasingly being used to study the expression, targeting, colocalization, turnover, and associations of diverse proteins involved in different plant signal transduction pathways (for review, see Fricker et al., 2006). Concurrent with the use of fluorescence-based cell biology, Förster resonance energy transfer (FRET) has emerged as a convenient tool to study the dynamics of protein associations in vivo. The technique exploits the biophysical phenomenon of nonradiative energy transfer from a donor fluorophore to an appropriately positioned acceptor at a nanometer scale (1–10 nm; Jares-Erijman and Jovin, 2003). In living cells, FRET occurs when two proteins (or different domains within a single protein) fused to suitable donor and acceptor fluorophores physically interact, thus bringing the donor and the acceptor within the favorable proximity for energy transfer (Immink et al., 2002; Bhat et al., 2006). This results in a decrease in the donor''s fluorescence intensity (or quantum yield [QY]) and excited-state lifetime (Gadella et al., 1999). Furthermore, if the acceptor molecule is a fluorophore, then FRET additionally results in an increase in the acceptor''s emission intensity (sensitized emission; Shah et al., 2001; Bhat et al., 2006).However, the exploitation and use of fluorescent marker proteins to study protein trafficking and associations in plants can be problematic because plant cells contain a number of autofluorescent compounds (e.g. lignin, chlorophyll, phenols, etc.) whose emission spectra interfere with that of the most commonly used green or red fluorescent protein fluorophores and/or their spectral variants. For example, lignin fluorescence in roots, vascular tissues, and cell walls of aerial plant parts interferes with imaging at wavelengths between 490 and 620 nm, whereas the chlorophyll autofluorescence in green aerial plant parts is prevalent between 630 and 770 nm (Chapman et al., 2005). Consequently, conventional imaging of GFP and its closest spectral variants (like cyan fluorescent protein [CFP] and yellow fluorescent protein [YFP]) is most likely to be problematic in roots, whereas red-shifted intrinsic fluorescent proteins (including monomeric red fluorescent protein and recently identified spectral variants like mStrawberry and mCherry) may be hard to discriminate in chloroplast-containing aerial tissues (Chapman et al., 2005). The problems get further compounded in FRET assays because the autofluorescence arising from phenols, lignin, and chlorophyll can limit the choice of fluorophores suitable for in planta FRET assays.CFP and YFP have been widely used as a donor-acceptor pair in in planta FRET measurements (Bhat et al., 2006; Dixit et al., 2006). However, in photophysical terms, this pair is less than ideal for FRET imaging. Both have broad excitation and emission spectra with a small Stokes shift (Chapman et al., 2005). Second, QY of CFP (QY = 0.4) is relatively lower than that of YFP (QY = 0.61), and thus a significantly higher (and rather cell damaging) amount of excitation energy is needed to induce FRET (Dixit et al., 2006). Additionally, CFP displays multiexponential lifetimes with a shorter (1.3 ns) and a longer (2.6 ns) component (Becker et al., 2006). Although the deviation from the single-component decay is reasonably small (Tramier et al., 2002; Becker et al., 2006), the shorter CFP lifetime component can erroneously be interpreted as being the result of lifetime reduction due to energy transfer. At the same time, weak or transient protein associations may get masked and thus remain undetected. Whereas the parental wild-type GFP is extremely photostable and shows a monoexponential decay pattern (excited-state lifetime 3.16 ± 0.03 ns; Striker et al., 1999; Volkmer et al., 2000; Shaner et al., 2005), its close spectral overlap with YFP makes it unsuitable as a donor in GFP-YFP FRET experiments. Likewise, wild-type or enhanced GFP (or YFP) as a donor to red-shifted monomers as acceptors is suboptimal because the 488-nm (or 514-nm) laser line commonly used to excite GFP (or YFP) cross excites most of the red monomers (e.g. mOrange, mStrawberry) because of their broad excitation spectra (Zapata-Hommer and Griesbeck, 2003; Shaner et al., 2004).Recently, TSapphire (Q69M/C70P/V163A/S175G; excitation/emission 399/511 nm), a variant of the Sapphire (T203I) mutant of wild-type GFP with improved folding properties and better pH sensitivity, was described (Zapata-Hommer and Griesbeck, 2003). The T203I mutation in TSapphire (and original Sapphire as well) abolishes the 475-nm excitation peak found in the wild-type GFP (Tsien, 1998). TSapphire is efficiently excited below 410 nm, which makes it ideal for studying plant protein dynamics and interactions because, at this wavelength, there is negligible excitation of the autofluorescing chlorophyll pigments. Furthermore, TSapphire also represents a good donor to red monomer acceptors that are negligibly excited at this wavelength (Shaner et al., 2004). Using a purified Zn²⁺ sensor with TSapphire and mOrange as a donor-acceptor pair, Shaner and colleagues demonstrated the ratiometric intramolecular FRET between the two fluorophores in vitro (Shaner et al., 2004). The sensor yielded a 6-fold ratiometric increase (562/514-nm mOrange/TSapphire emission ratio) upon Zn²⁺ binding.However, currently there are no reports demonstrating the application and use of TSapphire and monomeric red-shifted fluorophores as donor-acceptor FRET pairs to probe intermolecular protein-protein interactions in vivo. In this article, we demonstrate in vivo FRET-fluorescence lifetime imaging microscopy (FLIM) between the donor TSapphire and the acceptor mOrange. We show that TSapphire expressed in living plant cells decays with a monoexponential lifetime of 2.93 ± 0.09 ns, which is in agreement with the published lifetime for its parent wild-type GFP (3.2 ns; Striker et al., 1999; Volkmer et al., 2000). Furthermore, we demonstrate intramolecular FRET-FLIM between chimerically linked TSapphire and mOrange (with a 16-amino acid linker in between). When fused to genetically known interacting proteins and expressed in intact living cells, the donor and the acceptor fluorophores show energy transfer in different subcellular compartments indicative of intermolecular protein-protein interactions. These results validate the versatility of the proposed in vivo FRET-FLIM assay based on the donor TSapphire and the acceptor mOrange, which turns out to work with both soluble and membrane proteins.     

Development of dual receptor biosensors: an analysis of FRET pairs

The development of a dual receptor detection method for enhanced biosensor monitoring was investigated by analyzing potential fluorescent resonance energy transfer (FRET) pairs. The dual receptor scheme requires the integration of a chemical transducer system with two unique protein receptors that bind to a single biological agent. The two receptors are tagged with special molecular groups (donors and acceptors fluorophores) while the chemical transduction system relies on the well-known mechanisms of FRET. During the binding event, the two FRET labeled receptors dock at the binding sites on the surface of the biological agent. The resulting close proximity of the two fluorophores upon binding will initiate the energy transfer resulting in fluorescence. The paper focuses on the analysis and optimization of the chemical transduction system. A variety of FRET fluorophore pairs were tested in a spectrofluorimeter and promising FRET pairs were then tagged to the protein, avidin and its ligand, biotin. Due to their affinities, the FRET-tagged biomolecules combine in solution, resulting in a stable, fluorescent signal from the acceptor FRET dye with a simultaneous decrease in fluorescent signal from the donor FRET dye. The results indicate that the selected FRET pairs can be utilized in the development of dual receptor sensors.     

Following FRET through five energy transfer steps: spectroscopic photobleaching, recovery of spectra, and a sequential mechanism of FRET.

We report the acquisition and analysis of spectrally resolved photobleaching data from a model system designed to exhibit FRET. Spectrally resolved photobleaching can be used to determine the presence of FRET in these systems and to investigate multi-step mechanisms of energy transfer. The model system was a previously described set of fluorescent beads consisting of a system of six fluorophores. In standard photobleaching experiments to determine FRET, bleaching of an acceptor molecule resulting in recovery of donor intensity or changes in photobleaching kinetics are used as indicators of FRET. Here, we use the Bateman equations to model growth and decay in a photobleaching experiment. Linked donor-acceptor growth and decay is used as an indicator of FRET. The apparatus required is relatively simple when compared to lifetime imaging systems. Several data analysis strategies, rigorous model building, global fitting procedures, and error analysis are presented. Using these procedures a five-step sequential mechanism of energy transfer was selected for these beads.     

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.     

Contribution of Fluorophore Dynamics and Solvation to Resonant Energy Transfer in Protein-DNA Complexes: A Molecular-Dynamics Study

In Förster resonance energy transfer (FRET) experiments, extracting accurate structural information about macromolecules depends on knowing the positions and orientations of donor and acceptor fluorophores. Several approaches have been employed to reduce uncertainties in quantitative FRET distance measurements. Fluorophore-position distributions can be estimated by surface accessibility (SA) calculations, which compute the region of space explored by the fluorophore within a static macromolecular structure. However, SA models generally do not take fluorophore shape, dye transition-moment orientation, or dye-specific chemical interactions into account. We present a detailed molecular-dynamics (MD) treatment of fluorophore dynamics for an ATTO donor/acceptor dye pair and specifically consider as case studies dye-labeled protein-DNA intermediates in Cre site-specific recombination. We carried out MD simulations in both an aqueous solution and glycerol/water mixtures to assess the effects of experimental solvent systems on dye dynamics. Our results unequivocally show that MD simulations capture solvent effects and dye-dye interactions that can dramatically affect energy transfer efficiency. We also show that results from SA models and MD simulations strongly diverge in cases where donor and acceptor fluorophores are in close proximity. Although atomistic simulations are computationally more expensive than SA models, explicit MD studies are likely to give more realistic results in both homogeneous and mixed solvents. Our study underscores the model-dependent nature of FRET analyses, but also provides a starting point to develop more realistic in silico approaches for obtaining experimental ensemble and single-molecule FRET data.     

Contribution of Fluorophore Dynamics and Solvation to Resonant Energy Transfer in Protein-DNA Complexes: A Molecular-Dynamics Study

In Förster resonance energy transfer (FRET) experiments, extracting accurate structural information about macromolecules depends on knowing the positions and orientations of donor and acceptor fluorophores. Several approaches have been employed to reduce uncertainties in quantitative FRET distance measurements. Fluorophore-position distributions can be estimated by surface accessibility (SA) calculations, which compute the region of space explored by the fluorophore within a static macromolecular structure. However, SA models generally do not take fluorophore shape, dye transition-moment orientation, or dye-specific chemical interactions into account. We present a detailed molecular-dynamics (MD) treatment of fluorophore dynamics for an ATTO donor/acceptor dye pair and specifically consider as case studies dye-labeled protein-DNA intermediates in Cre site-specific recombination. We carried out MD simulations in both an aqueous solution and glycerol/water mixtures to assess the effects of experimental solvent systems on dye dynamics. Our results unequivocally show that MD simulations capture solvent effects and dye-dye interactions that can dramatically affect energy transfer efficiency. We also show that results from SA models and MD simulations strongly diverge in cases where donor and acceptor fluorophores are in close proximity. Although atomistic simulations are computationally more expensive than SA models, explicit MD studies are likely to give more realistic results in both homogeneous and mixed solvents. Our study underscores the model-dependent nature of FRET analyses, but also provides a starting point to develop more realistic in silico approaches for obtaining experimental ensemble and single-molecule FRET data.     

Steady-state polarization from cylindrically symmetric fluorophores undergoing rapid restricted motion.

Steady-state fluorescence polarization measurements provide a relatively simple method for investigating the orientation of molecular components in ordered biological systems. However, the observed fluorescence polarization ratios also depend on any mobility of the fluorophores on the time scale of the fluorescence lifetime. Such mobility commonly arises from incomplete immobilization of a fluorescent probe on the macromolecule of interest. A theoretical formalism is presented for the interpretation of steady-state fluorescence polarization ratios in the presence of such rapid fluorophore motion. It is assumed that the fluorophores move freely within a cone between absorption and emission of a photon. Only one new parameter is introduced to describe fluorophore motion, the semi-angle of the cone, and this can be measured in separate experiments on an isotropic system. The fluorophore orientations are assumed to have cylindrical symmetry, but the symmetry axis need not be in the same plane as the center axes of the absorption and emission cones. This geometry applies to muscle and other biological fibers.     

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.     

Fluorescent Protein Based FRET Pairs with Improved Dynamic Range for Fluorescence Lifetime Measurements

Fluorescence Resonance Energy Transfer (FRET) using fluorescent protein variants is widely used to study biochemical processes in living cells. FRET detection by fluorescence lifetime measurements is the most direct and robust method to measure FRET. The traditional cyan-yellow fluorescent protein based FRET pairs are getting replaced by green-red fluorescent protein variants. The green-red pair enables excitation at a longer wavelength which reduces cellular autofluorescence and phototoxicity while monitoring FRET. Despite the advances in FRET based sensors, the low FRET efficiency and dynamic range still complicates their use in cell biology and high throughput screening. In this paper, we utilized the higher lifetime of NowGFP and screened red fluorescent protein variants to develop FRET pairs with high dynamic range and FRET efficiency. The FRET variations were analyzed by proteolytic activity and detected by steady-state and time-resolved measurements. Based on the results, NowGFP-tdTomato and NowGFP-mRuby2 have shown high potentials as FRET pairs with large fluorescence lifetime dynamic range. The in vitro measurements revealed that the NowGFP-tdTomato has the highest Förster radius for any fluorescent protein based FRET pairs yet used in biological studies. The developed FRET pairs will be useful for designing FRET based sensors and studies employing Fluorescence Lifetime Imaging Microscopy (FLIM).     

荧光共振能量转移效率的实时定量测量

荧光共振能量转移（FRET）广泛用于研究分子间的距离及其相互作用,与荧光显微镜结合,可定量获取有关生物活体内蛋白质、脂类、DNA和RNA的时空信息。随着绿色荧光蛋白（GFP）的发展,FRET荧光显微镜有可能实时测量活体细胞内分子的动态性质。提出了一种定量测量FRET效率以及供体与受体间距离的简单方法,仅需使用一组滤光片和测量一个比值,利用供体和受体的发射谱肖除光谱间的串扰。该方法简单快速,可实时定量测量FRET的效率和供体与受体间的距离,尤其适用于基于GFP的供体－受体对。     

Development of a novel FRET immunosensor technique

We report on a novel technique to develop an optical immunosensor based on fluorescence resonance energy transfer (FRET). IgG antibodies were labeled with acceptor fluorophores while one of three carrier molecules (protein A, protein G, or F(ab')2 fragment) was labeled with donor fluorophores. The carrier molecule was incubated with the antibody to allow specific binding to the Fc portion. The labeled antibody-protein complex was then exposed to specific and nonspecific antigens, and experiments were designed to determine the 'in solution' response. The paper reports the results of three different donor-acceptor FRET pairs, fluorescein isothiocyanate/tetramethylrhodamine isothiocyanate, Texas Red/Cy5, and Alexa Fluor 546/Alexa Fluor 594. The effects of the fluorophore to protein conjugation ratio (F/P ratio) and acceptor to donor fluorophore ratios between the antibody and protein (A/D ratio) were examined. In the presence of specific antigens, the antibodies underwent a conformational change, resulting in an energy transfer from the donor to the acceptor fluorophore as measured by a change in fluorescence. The non-specific antigens elicited little or no changes. The Alexa Fluor FRET pair demonstrated the largest change in fluorescence, resulting in a 35% change. The F/P and A/D ratio will affect the efficiency of energy transfer, but there exists a suitable range of A/D and F/P ratios for the FRET pairs. The feasibility of the FRET immunosensor technique was established; however, it will be necessary to immobilize the complexes onto optical substrates so that consistent trends can be obtained that would allow calibration plots.     

Time-resolved FRET fluorescence spectroscopy of visible fluorescent protein pairs

Förster resonance energy transfer (FRET) is a powerful method for obtaining information about small-scale lengths between biomacromolecules. Visible fluorescent proteins (VFPs) are widely used as spectrally different FRET pairs, where one VFP acts as a donor and another VFP as an acceptor. The VFPs are usually fused to the proteins of interest, and this fusion product is genetically encoded in cells. FRET between VFPs can be determined by analysis of either the fluorescence decay properties of the donor molecule or the rise time of acceptor fluorescence. Time-resolved fluorescence spectroscopy is the technique of choice to perform these measurements. FRET can be measured not only in solution, but also in living cells by the technique of fluorescence lifetime imaging microscopy (FLIM), where fluorescence lifetimes are determined with the spatial resolution of an optical microscope. Here we focus attention on time-resolved fluorescence spectroscopy of purified, selected VFPs (both single VFPs and FRET pairs of VFPs) in cuvette-type experiments. For quantitative interpretation of FRET–FLIM experiments in cellular systems, details of the molecular fluorescence are needed that can be obtained from experiments with isolated VFPs. For analysis of the time-resolved fluorescence experiments of VFPs, we have utilised the maximum entropy method procedure to obtain a distribution of fluorescence lifetimes. Distributed lifetime patterns turn out to have diagnostic value, for instance, in observing populations of VFP pairs that are FRET-inactive.     

Caspase-3 sensitive signaling in vivo in apoptotic HeLa cells by chemically engineered intramolecular fluorescence resonance energy transfer mutants of green fluorescent protein

Green fluorescent protein (UV5) was re-engineered to remove native cysteine residues, and a new cysteine was introduced near the C-terminus, approximately 20 A from the native fluorophore, for site-specific attachment of chemical fluorophores. The resultant efficient intramolecular FRET quenched GFP emission and gave a new emission band from the conjugated fluorophore. Caspase-3 cleavage of constructs with a caspase-3 sequence near the C-terminus in the sequence between the native fluorophore and the new cysteine, located C-terminal to the caspase site, destroyed the FRET, the emitted color reverting to that of unmodified GFP. This process was demonstrated in vitro with caspase-3 and lysates from cells undergoing apoptosis. Real-time emission changes for the Alexa Fluor 532 conjugate of this GFP, studied quantitatively in vivo for single HeLa cells using the ratios of fluorescence at the red and green maxima by confocal microscopy, showed that caspase-3 action in the cytosol preceded that in the nucleus.     

Spectral imaging and linear un-mixing enables improved FRET efficiency with a novel GFP2-YFP FRET pair

Spectral variants of the green fluorescent protein (GFP) have been extensively used as reporters to image molecular interactions in living cells by fluorescence resonance energy transfer (FRET). However, those GFP variants which are the most efficient donor acceptor pairs for FRET measurements show a high degree of spectral overlap which has hampered in the past their use in FRET applications. Here we use spectral imaging and subsequent un-mixing to quantitatively separate highly overlapping donor and acceptor emissions in FRET measurements. We demonstrate the method in fixed and living cells using a novel GFP based FRET pair (GFP2-YFP (yellow)), which has an increased FRET efficiency compared to the most commonly used FRET pair consisting of cyan fluorescent protein and YFP. Moreover, GFP2 has its excitation maximum at 396 nm at which the YFP acceptor is excited only below the detection level and thus this FRET pair is ideal for applications involving sensitized emission.     

Quantification of protein interaction in living cells by two-photon spectral imaging with fluorescent protein fluorescence resonance energy transfer pair devoid of acceptor bleed-through

Fluorescence resonance energy transfer (FRET) between fluorescent proteins (FPs) is a powerful method to visualize and quantify protein-protein interaction in living cells. Unfortunately, the emission bleed-through of FPs limits the usage of this complex technique. To circumvent undesirable excitation of the acceptor fluorophore, using two-photon excitation, we searched for FRET pairs that show selective excitation of the donor but not of the acceptor fluorescent molecule. We found this property in the fluorescent cyan fluorescent protein (CFP)/yellow fluorescent protein (YFP) and YFP/mCherry FRET pairs and performed two-photon excited FRET spectral imaging to quantify protein interactions on the later pair that shows better spectral discrimination. Applying non-negative matrix factorization to unmix two-photon excited spectral imaging data, we were able to eliminate the donor bleed-through as well as the autofluorescence. As a result, we achieved FRET quantification by means of a single spectral acquisition, making the FRET approach not only easy and straightforward but also less prone to calculation artifacts. As an application of our approach, the intermolecular interaction of amyloid precursor protein and the adaptor protein Fe65 associated with Alzheimer's disease was quantified. We believe that the FRET approach using two-photon and fluorescent YFP/mCherry pair is a promising method to monitor protein interaction in living cells.     

A comparison of donor-acceptor pairs for genetically encoded FRET sensors: application to the Epac cAMP sensor as an example

We recently reported on CFP-Epac-YFP, an Epac-based single polypeptide FRET reporter to resolve cAMP levels in living cells. In this study, we compared and optimized the fluorescent protein donor/acceptor pairs for use in biosensors such as CFP-Epac-YFP. Our strategy was to prepare a wide range of constructs consisting of different donor and acceptor fluorescent proteins separated by a short linker. Constructs were expressed in HEK293 cells and tested for FRET and other relevant properties. The most promising pairs were subsequently used in an attempt to improve the FRET span of the Epac-based cAMP sensor. The results show significant albeit not perfect correlation between performance in the spacer construct and in the Epac sensor. Finally, this strategy enabled us to identify improved sensors both for detection by sensitized emission and by fluorescent lifetime imaging. The present overview should be helpful in guiding development of future FRET sensors.     

Pulsed Interleaved Excitation Fluctuation Imaging

Fluorescence fluctuation imaging is a powerful means to investigate dynamics, interactions, and stoichiometry of proteins inside living cells. Pulsed interleaved excitation (PIE) is the method of nanosecond alternating excitation with time-resolved detection and allows accurate, independent, and quasi-simultaneous determination of fluorescence intensities and lifetimes of different fluorophores. In this work, we combine pulsed interleaved excitation with fluctuation imaging methods (PIE-FI) such as raster image correlation spectroscopy (RICS) or number and brightness analysis (N&B). More specifically, we show that quantitative measurements of diffusion and molecular brightness of Venus fluorescent protein (FP) can be performed in solution with PIE-RICS and compare PIE-RICS with single-point PIE-FCS measurements. We discuss the advantages of cross-talk free dual-color PIE-RICS and illustrate its proficiency by quantitatively comparing two commonly used FP pairs for dual-color microscopy, eGFP/mCherry and mVenus/mCherry. For N&B analysis, we implement dead-time correction to the PIE-FI data analysis to allow accurate molecular brightness determination with PIE-NB. We then use PIE-NB to investigate the effect of eGFP tandem oligomerization on the intracellular maturation efficiency of the fluorophore. Finally, we explore the possibilities of using the available fluorescence lifetime information in PIE-FI experiments. We perform lifetime-based weighting of confocal images, allowing us to quantitatively determine molecular concentrations from 100 nM down to <30 pM with PIE-raster lifetime image correlation spectroscopy (RLICS). We use the fluorescence lifetime information to perform a robust dual-color lifetime-based FRET analysis of tandem fluorescent protein dimers. Lastly, we investigate the use of dual-color RLICS to resolve codiffusing FRET species from non-FRET species in cells. The enhanced capabilities and quantitative results provided by PIE-FI make it a powerful method that is broadly applicable to a large number of interesting biophysical studies.     

Calibration of the parallax fluorescence quenching method for determination of membrane penetration depth: refinement and comparison of quenching by spin-labeled and brominated lipids.

We previously introduced the "parallax" method, which uses fluorescence quenching by spin-labeled lipids in order to measure the depth of molecules within a membrane [Chattopadhyay, A., & London, E. (1987) Biochemistry 26, 39-45]. In this report the accuracy of this method is established by comparison of spin-label quenching to that obtained using brominated lipids. To accomplish this, the fluorescent molecules used were a fatty acid labeled with a carbazole buried deeply within the acyl chain region of the membrane, an acyl-Trp with the Trp residue residing near the polar membrane region, and cytochrome b5, which has Trp residues in its membrane-inserted region. The depths calculated from the amount of bromine quenching agreed with those determined using parallax analysis. This indicates that the depth reported by parallax analysis is accurate and that the spin labels residue very close to their predicted locations in the membrane. Furthermore, there was good agreement when parallax analysis was applied both to quenching by brominated and spin-labeled molecules, suggesting that the analysis is valid in both cases. The effect that different distributions and motions of fluorophores and quenchers would have on parallax analysis was also examined. For uniform distributions of quenchers or fluorophores over a range of depths, it was found that the analysis reports the average fluorophore depth. In addition, experimental data suggest that motional effects do not significantly alter the measured depths. This is consistent with the motions during the short excited state lifetime of the fluorophores being relatively small and/or relatively isotropic.