Enhanced dynamic range in a genetically encoded Ca2+ sensor

Genetically encoded fluorescence resonance energy transfer (FRET) indicators are powerful tools for real-time detection of second messenger molecules and activation of signal proteins. However, these fluorescent protein-based sensors typically display marginal FRET efficiency. To improve their FRET efficiency for optical imaging and screening, we developed a number of fluorescent protein mutants based on cyan fluorescent protein (CFP) and yellow fluorescent protein (YFP). To improve FRET ratios, which were initially within a narrow dynamic range, we used DNA shuffling to develop a new FRET pair called 3xCFP/Venus. The optimized 3xCFP/Venus pair exhibited higher FRET ratios than CyPet/YPet, which has one of the greatest dynamic ranges of protein-based FRET pairs. We converted this FRET pair to a Ca(2+) FRET indicators using circular permutation Venus (cpVenus) linked with 3xCFP to form 3xCFP/cpVenus, which displayed an ～11-fold change in dynamic range in response to Ca(2+) binding. The enhanced dynamic range for Ca(2+) concentration detection using 3xCFP/cpVenus was confirmed in PC12 cells using previously established indicators (TN-XXL, ECFP/cpCitrine). To our knowledge, this FRET pair displays the largest dynamic range so far among genetically-encoded sensors, and can be used for sensitive FRET detection.     

Enhanced dynamic range in a genetically encoded Ca sensor

Genetically encoded fluorescence resonance energy transfer (FRET) indicators are powerful tools for real-time detection of second messenger molecules and activation of signal proteins. However, these fluorescent protein-based sensors typically display marginal FRET efficiency. To improve their FRET efficiency for optical imaging and screening, we developed a number of fluorescent protein mutants based on cyan fluorescent protein (CFP) and yellow fluorescent protein (YFP). To improve FRET ratios, which were initially within a narrow dynamic range, we used DNA shuffling to develop a new FRET pair called 3xCFP/Venus. The optimized 3xCFP/Venus pair exhibited higher FRET ratios than CyPet/YPet, which has one of the greatest dynamic ranges of protein-based FRET pairs. We converted this FRET pair to a Ca²⁺ FRET indicators using circular permutation Venus (cpVenus) linked with 3xCFP to form 3xCFP/cpVenus, which displayed an ∼11-fold change in dynamic range in response to Ca²⁺ binding. The enhanced dynamic range for Ca²⁺ concentration detection using 3xCFP/cpVenus was confirmed in PC12 cells using previously established indicators (TN-XXL, ECFP/cpCitrine). To our knowledge, this FRET pair displays the largest dynamic range so far among genetically-encoded sensors, and can be used for sensitive FRET detection.     

Using GFP in FRET-based applications

The use of green fluorescent protein (GFP) is a powerful technology that has recently enabled investigators to study dynamic molecular events within living cells. One method for detecting molecular interactions involves fluorescence resonance energy transfer (FRET) between two GFPs or between GFP and a second fluorophore. This review summarizes the use of GFP for FRET and illustrates the theme with specific examples on how GFP has been employed as an intracellular molecular sensor.     

Non-conjugated small molecule FRET for differentiating monomers from higher molecular weight amyloid beta species

Background

Systematic differentiation of amyloid (Aβ) species could be important for diagnosis of Alzheimer''s disease (AD). In spite of significant progress, controversies remain regarding which species are the primary contributors to the AD pathology, and which species could be used as the best biomarkers for its diagnosis. These controversies are partially caused by the lack of reliable methods to differentiate the complicated subtypes of Aβ species. Particularly, differentiation of Aβ monomers from toxic higher molecular weight species (HrMW) would be beneficial for drug screening, diagnosis, and molecular mechanism studies. However, fast and cheap methods for these specific aims are still lacking.

Principal Findings

We demonstrated the feasibility of a non-conjugated FRET (Förster resonance energy transfer) technique that utilized amyloid beta (Aβ) species as intrinsic platforms for the FRET pair assembly. Mixing two structurally similar curcumin derivatives that served as the small molecule FRET pair with Aβ40 aggregates resulted in a FRET signal, while no signal was detected when using Aβ40 monomer solution. Lastly, this FRET technique enabled us to quantify the concentrations of Aβ monomers and high molecular weight species in solution.

Significance

We believe that this FRET technique could potentially be used as a tool for screening for inhibitors of Aβ aggregation. We also suggest that this concept could be generalized to other misfolded proteins/peptides implicated in various pathologies including amyloid in diabetes, prion in bovine spongiform encephalopathy, tau protein in AD, and α-synuclein in Parkinson disease.     

Expression, purification, crystallization and preliminary x-ray analysis of Cyan fluorescent protein CyPet

The technique of fluorescence (or F?rster) resonance energy transfer (FRET) is widely used to observe bimolecular interaction in living cells. Cyan and yellow fluorescent proteins are the most widely used pair in FRET analysis. CyPet and YPet are two newly optimized fluorescent proteins that have much better dynamic range and sensitivity than CFP/YFP pair, although the crystallographic structure and the mechanism of better fluorescent characteristics of CyPet are still unknown. We have expressed the cyan fluorescent protein CyPet using pT7 prokaryocyte expression system in Escherichia coli strain Rosetta (DE3) pLysS by auto-induction. After purification, the recombinant CyPet protein was crystallized by hanging drop vapor diffusion technique and could diffract to 2.55A resolution. The data showed that the orthorhombic CyPet crystal was in space group P212121 with unit cell parameters (51.55, 61.53, 63.36) and contained one molecule in one asymmetric unit.     

Imaging molecular interactions in living cells by FRET microscopy

F?rster resonance energy transfer (FRET) is applied extensively in all fields of biological research and technology, generally as a 'nanoruler' with a dynamic range corresponding to the intramolecular and intermolecular distances characterizing the molecular structures that regulate cellular function. The complex underlying network of interactions reflects elementary reactions operating under strict spatio-temporal control: binding, conformational transition, covalent modification and transport. FRET imaging provides information about all these molecular processes with high specificity and sensitivity via probes expressed by or introduced from the external medium into the cell, tissue or organism. Current approaches and developments in the field are discussed with emphasis on formalism, probes and technical implementation.     

Resonance energy transfer in cells: a new look at fixation effect and receptor aggregation on cell membrane

Fluorescence resonance energy transfer (FRET) measurements offer a reliable and noninvasive approach to studying protein and lipid colocalization in cells. We have considered systems in which FRET occurs as intramolecular and/or intermolecular process. The proposed dynamic FRET model shows that in the case of intermolecular process the degree of aggregation only slightly affects the energy transfer efficiency. The theory was tested on a set of donor-acceptor pairs in which energy transfer occurs intramolecularly, intermolecularly, or both. The obtained experimental results are in a good agreement with the proposed model. It is well known that the energy transfer efficiency depends both on the distance between the donor and acceptor molecules and the relative orientation of their respective transition dipole moments. This dual dependence often leads to ambiguity. In this article, we show how FRET efficiency can be significantly reduced even in highly coupled system through conformational restrictions in the donor-acceptor pair. Importantly, such restrictions can be imposed on the system by cell fixation, a procedure routinely used when conducting FRET measurements.     

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.     

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.     

Visualization of ternary complexes in living cells by using a BiFC-based FRET assay

Studies of protein interactions have increased our understanding and knowledge of biological processes. Assays that utilize fluorescent proteins, such as fluorescence resonance energy transfer (FRET) and bimolecular fluorescence complementation (BiFC), have enabled direct visualization of protein interactions in living cells. However, these assays are primarily suitable for a pair of interacting proteins, and methods to visualize and identify multiple protein complexes in vivo are very limited. This protocol describes the recently developed BiFC-FRET assay, which allows visualization of ternary complexes in living cells. We discuss how to design the BiFC-FRET assay on the basis of the validation of BiFC and FRET assays and how to perform transfection experiments for acquisition of fluorescent images for net FRET calculation. We also provide three methods for normalization of the FRET efficiency. The assay employs a two-chromophore and three-filter FRET setup and is applicable to epifluorescence microscopes. The entire protocol takes about 2-3 weeks to complete.     

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).     

Development of an optimized backbone of FRET biosensors for kinases and GTPases

Biosensors based on the principle of Förster (or fluorescence) resonance energy transfer (FRET) have shed new light on the spatiotemporal dynamics of signaling molecules. Among them, intramolecular FRET biosensors have been increasingly used due to their high sensitivity and user-friendliness. Time-consuming optimizations by trial and error, however, obstructed the development of intramolecular FRET biosensors. Here we report an optimized backbone for rapid development of highly sensitive intramolecular FRET biosensors. The key concept is to exclude the “orientation-dependent” FRET and to render the biosensors completely “distance-dependent” with a long, flexible linker. We optimized a pair of fluorescent proteins for distance-dependent biosensors, and then developed a long, flexible linker ranging from 116 to 244 amino acids in length, which reduced the basal FRET signal and thereby increased the gain of the FRET biosensors. Computational simulations provided insight into the mechanisms by which this optimized system was the rational strategy for intramolecular FRET biosensors. With this backbone system, we improved previously reported FRET biosensors of PKA, ERK, JNK, EGFR/Abl, Ras, and Rac1. Furthermore, this backbone enabled us to develop novel FRET biosensors for several kinases of RSK, S6K, Akt, and PKC and to perform quantitative evaluation of kinase inhibitors in living cells.     

High-contrast imaging of fluorescent protein FRET by fluorescence polarization microscopy

Detection of Forster resonance energy transfer (FRET) between fluorescent protein labeled targets is a valuable strategy for measurement of protein-protein interactions and other intracellular processes. Despite the utility of FRET, widespread application of this technique to biological problems and high-throughput screening has been limited by low-contrast measurement strategies that rely on the detection of sensitized emission or photodestruction of the sample. Here we report a FRET detection strategy based on detecting depolarized sensitized emission. In the absence of FRET, we show that fluorescence emission from a donor fluorescent protein is highly polarized. Depolarization of fluorescence emission is observed only in the presence of energy transfer. A simple detection strategy was adapted for fluorescence microscopy using both laser scanning and wide-field approaches. This approach is able to distinguish FRET between linked and unlinked Cerulean and Venus fluorescent proteins in living cells with a larger dynamic range than other approaches.     

An ion-insensitive cAMP biosensor for long term quantitative ratiometric fluorescence resonance energy transfer (FRET) measurements under variable physiological conditions

Ratiometric measurements with FRET-based biosensors in living cells using a single fluorescence excitation wavelength are often affected by a significant ion sensitivity and the aggregation behavior of the FRET pair. This is an important problem for quantitative approaches. Here we report on the influence of physiological ion concentration changes on quantitative ratiometric measurements by comparing different FRET pairs for a cAMP-detecting biosensor. We exchanged the enhanced CFP/enhanced YFP FRET pair of an established Epac1-based biosensor by the fluorophores mCerulean/mCitrine. In the case of enhanced CFP/enhanced YFP, we showed that changes in proton, and (to a lesser extent) chloride ion concentrations result in incorrect ratiometric FRET signals, which may exceed the dynamic range of the biosensor. Calcium ions have no direct, but an indirect pH-driven effect by mobilizing protons. These ion dependences were greatly eliminated when mCerulean/mCitrine fluorophores were used. For such advanced FRET pairs the biosensor is less sensitive to changes in ion concentration and allows consistent cAMP concentration measurements under different physiological conditions, as occur in metabolically active cells. In addition, we verified that the described FRET pair exchange increased the dynamic range of the FRET efficiency response. The time window for stable experimental conditions was also prolonged by a faster biosensor expression rate in transfected cells and a greatly reduced tendency to aggregate, which reduces cytotoxicity. These properties were verified in functional tests in single cells co-expressing the biosensor and the 5-HT(1A) receptor.     

A new pair for inter- and intra-molecular FRET measurement

Fluorescence resonance energy transfer between mutant green fluorescent proteins provides powerful means to monitor in vivo protein-protein proximity and intracellular signaling. However, the current widely applied FRET pair of this class (CFP/YFP) requires excitation by expensive UV lasers, thereby hindering FRET imaging on many confocal microscopes. Further challenges arise from the large spectral overlap of CFP/YFP emission. Another FRET pair GFP/DsRed could obviate such limitations. However, the use of DsRed as a FRET acceptor is hampered by several critical problems, including a slow and incomplete maturation and obligate tetramerization. A tandem dimer mutant of DsRed (TDimer2) has similar spectral properties as those of DsRed. The rapid maturation and non-oligomerization make TDimer2 a promising substitute for DsRed in FRET experiments. Here, we have explored the possibility of using TDimer2 as a FRET acceptor for the donor EGFP. FRET was demonstrated between the EGFP-TDimer2 chimeric fusion protein. By substituting CFP/YFP in the Ca2+-sensor cameleon with EGFP/TDimer2, dynamic changes in cytosolic free Ca2+ concentrations were observed with 488nm excitation under conventional wide-field microscopy. The EGFP/TDimer2 pair was further successfully employed to monitor inter-molecular interaction between Syntaxin and SNAP25. These results reveal EGFP/TDimer2 as a promising FRET pair in monitoring intra-molecular conformation change as well as inter-molecular interaction.     

Fluorescence resonance energy transfer (FRET) microscopy imaging of live cell protein localizations

The current advances in fluorescence microscopy, coupled with the development of new fluorescent probes, make fluorescence resonance energy transfer (FRET) a powerful technique for studying molecular interactions inside living cells with improved spatial (angstrom) and temporal (nanosecond) resolution, distance range, and sensitivity and a broader range of biological applications.     

Monitoring spatio-temporal regulation of Ras and Rho GTPase with GFP-based FRET probes

GFP-based fluorescence resonance energy transfer (FRET) probes that visualize local activity-changes of Ras and Rho GTPases in living cells are now available for examining the spatio-temporal regulation of these proteins. This article describes principles and strategies to develop intramolecular FRET probes for Ras- and Rho-family GTPases. The procedure for characterizing candidate probes, and image acquisition and processing are also explained. An optimal FRET probe should have (i) a wide dynamic range (which means a high sensitivity), (ii) a high fluorescence intensity, (iii) target specificity, and (iv) a minimal perturbation to endogenous signaling cascades. Although an improvement of FRET probes should be executed in a trial-and-error manner, practical tips for optimization are provided here. In addition, we illustrate some applications of FRET probes for neuronal cells, which are composed of diverse subcellular compartments with different functions; thus, tools to decipher the dynamics of GTPase activity in each compartment have long been desired.     

Genome-wide assessment of the carriers involved in the cellular uptake of drugs: a model system in yeast

Background

Gq is a heterotrimeric G protein that plays an important role in numerous physiological processes. To delineate the molecular mechanisms and kinetics of signalling through this protein, its activation should be measurable in single living cells. Recently, fluorescence resonance energy transfer (FRET) sensors have been developed for this purpose.

Results

In this paper, we describe the development of an improved FRET-based Gq activity sensor that consists of a yellow fluorescent protein (YFP)-tagged Gγ2 subunit and a Gαq subunit with an inserted monomeric Turquoise (mTurquoise), the best cyan fluorescent protein variant currently available. This sensor enabled us to determine, for the first time, the k_on (2/s) of Gq activation. In addition, we found that the guanine nucleotide exchange factor p63RhoGEF has a profound effect on the number of Gq proteins that become active upon stimulation of endogenous histamine H1 receptors. The sensor was also used to measure ligand-independent activation of the histamine H1 receptor (H1R) upon addition of a hypotonic stimulus.

Conclusions

Our observations reveal that the application of a truncated mTurquoise as donor and a YFP-tagged Gγ2 as acceptor in FRET-based Gq activity sensors substantially improves their dynamic range. This optimization enables the real-time single cell quantification of Gq signalling dynamics, the influence of accessory proteins and allows future drug screening applications by virtue of its sensitivity.     

Imaging FRET between spectrally similar GFP molecules in single cells

Fluorescence resonance energy transfer (FRET) detection in fusion constructs consisting of green fluorescent protein (GFP) variants linked by a sequence that changes conformation upon modification by enzymes or binding of ligands has enabled detection of physiological processes such as Ca(2+) ion release, and protease and kinase activity. Current FRET microscopy techniques are limited to the use of spectrally distinct GFPs such as blue or cyan donors in combination with green or yellow acceptors. The blue or cyan GFPs have the disadvantages of less brightness and of autofluorescence. Here a FRET imaging method is presented that circumvents the need for spectral separation of the GFPs by determination of the fluorescence lifetime of the combined donor/acceptor emission by fluorescence lifetime imaging microscopy (FLIM). This technique gives a sensitive, reproducible, and intrinsically calibrated FRET measurement that can be used with the spectrally similar and bright yellow and green fluorescent proteins (EYFP/EGFP), a pair previously unusable for FRET applications. We demonstrate the benefits of this approach in the analysis of single-cell signaling by monitoring caspase activity in individual cells during apoptosis.     

Anomalous Surplus Energy Transfer Observed with Multiple FRET Acceptors

Background

Förster resonance energy transfer (FRET) is a mechanism where energy is transferred from an excited donor fluorophore to adjacent chromophores via non-radiative dipole-dipole interactions. FRET theory primarily considers the interactions of a single donor-acceptor pair. Unfortunately, it is rarely known if only a single acceptor is present in a molecular complex. Thus, the use of FRET as a tool for measuring protein-protein interactions inside living cells requires an understanding of how FRET changes with multiple acceptors. When multiple FRET acceptors are present it is assumed that a quantum of energy is either released from the donor, or transferred in toto to only one of the acceptors present. The rate of energy transfer between the donor and a specific acceptor (k_D→A) can be measured in the absence of other acceptors, and these individual FRET transfer rates can be used to predict the ensemble FRET efficiency using a simple kinetic model where the sum of all FRET transfer rates is divided by the sum of all radiative and non-radiative transfer rates.

Methodology/Principal Findings

The generality of this approach was tested by measuring the ensemble FRET efficiency in two constructs, each containing a single fluorescent-protein donor (Cerulean) and either two or three FRET acceptors (Venus). FRET transfer rates between individual donor-acceptor pairs within these constructs were calculated from FRET efficiencies measured after systematically introducing point mutations to eliminate all other acceptors. We find that the amount of energy transfer observed in constructs having multiple acceptors is significantly greater than the FRET efficiency predicted from the sum of the individual donor to acceptor transfer rates.

Conclusions/Significance

We conclude that either an additional energy transfer pathway exists when multiple acceptors are present, or that a theoretical assumption on which the kinetic model prediction is based is incorrect.