Effects of metallic silver island films on resonance energy transfer between N,N'-(dipropyl)-tetramethyl- indocarbocyanine (Cy3)- and N,N'-(dipropyl)-tetramethyl- indodicarbocyanine (Cy5)-labeled DNA

Resonance energy transfer (RET) is typically limited to distances below 60 A, which can be too short for some biomedical assays. We examined a new method for increasing the RET distances by placing donor- and acceptor-labeled DNA oligomers between two slides coated with metallic silver particles. A N,N'-(dipropyl)-tetramethylindocarbocyanine donor and a N,N'-(dipropyl)-tetramethylindodicarbocyanine acceptor were covalently bound to opposite 5' ends of complementary 23 base pair DNA oligomers. The transfer efficiency was 25% in the absence of silver particles or if only one slide was silvered, and it increased to an average value near 64% between two silvered slides. The average value of the Forster distance increased from 58 to 77 A. The energy transfer data were analyzed with a model assuming two populations of donor-acceptor pairs: unaffected and affected by silver island films. In an affected fraction of about 28%, the apparent energy transfer efficiency is near 87% and the Forster distance increases to 119 A. These results suggest the use of metallic silver particles to increase the distances over which RET occurs in biomedical and biotechnology assays.     

Effects of metallic silver particles on resonance energy transfer in labeled bovine serum albumin

Resonance energy transfer (RET) is widely used to detect proximity between biomolecules. In transparent solution the maximum donor-to-acceptor distance for RET is about 70 A. We measured the effects of metallic silver island films on RET from the intrinsic tryptophan of a protein to a bound probe as the acceptor. These preliminary experiments revealed a dramatic increase in the apparent F?rster distance increasing from 28.6 to 63 A. These results suggest the use of silver island films for detecting long range proximity between biomolecules and for biotechnology applications based on RET.     

Radiative decay engineering. 2. Effects of Silver Island films on fluorescence intensity, lifetimes, and resonance energy transfer

Metallic surfaces can have unusual effects on fluorophores such as increasing or decreasing the rates of radiative decay and the rates of resonance energy transfer (RET). In the present article we describe the effects of metallic silver island films on the emission spectra, lifetimes, and energy transfer for several fluorophores. The fluorophores are not covalently coupled to the silver islands so that there are a range of fluorophore-to-metal distances. We show that proximity of fluorophores to the silver islands results in increased fluorescence intensity, with the largest enhancement for the lowest-quantum-yield fluorophores. Importantly, the metal-induced increases in intensity are accompanied by decreased lifetimes and increased photostability. These effects demonstrate that the silver islands have increased the radiative decay rates of the fluorophore. For solvent-sensitive fluorophores the emission spectra shifted to shorted wavelengths in the presence of the silver islands, which is consistent with a decrease of the apparent lifetime for fluorophores near the metal islands. We also observed an increased intensity and blue spectral shift for the protein human glyoxalase, which displays a low quantum yield for its intrinsic tryptophan emission. In this case the blue shift is thought to be due to increased emission from a buried low-quantum-yield tryptophan residue. Increased intensities were also observed for the intrinsic emission of the nucleic acid bases adenine and thymine and for single-stranded 15-mers poly(T) and poly(C). And finally, we observed increased RET for donors and acceptors in solution and when bound to double-helical DNA. These results demonstrate that metallic particles can be used to modify the emission from intrinsic and extrinsic fluorophores in biochemical systems.     

Engineering resonance energy transfer for advanced immunoassays: the case of celiac disease

Celiac disease (CD) is an immune-mediated disorder affecting genetically predisposed subjects. It is caused by the ingestion of wheat gluten and related prolamins. A final diagnosis for this disease can be obtained by examination of jejunal biopsies. Nevertheless, different analytical approaches have been established to detect the presence of anti-tissue transglutaminase antibodies that represent a serological hallmark of the disease. In this work, we explored a new method for the diagnosis of CD based on the detection of serum anti-transglutaminase antibodies by resonance energy transfer (RET) between donor molecules and acceptor molecules. In particular, we labeled the liver transglutaminase (tTG) enzyme from guinea pig and the rabbit anti-tTG antibodies with a couple of fluorescence probes that are able to make RET if they are located within with Förster distance. We labeled tTG with the fluorescence probe DyLight 594 as donor and the anti-tTG antibodies with the fluorescence probe DyLight 649 as acceptor. However, due to the large size of the formed complex (tTG/anti-tTG), and consequently to the low efficiency energy transfer process between the donor–acceptor molecules, we explored a new experimental approach that allows us to extend the utilizable range of RET between donor:acceptor pairs by using one single molecule as donor and multiple molecules as energy acceptors, instead of using a single acceptor molecule as usually occurs in RET experiments. The obtained results clearly show that the use of one donor and multiacceptor strategy enables for a simple and rapid detection of serum anti-transglutaminase antibodies. In addition, our results point out that it is possible to consider this approach as a new method for a wide variety of analytical assays.     

Effects of fluorophore-to-silver distance on the emission of cyanine-dye-labeled oligonucleotides

We examined the fluorescence spectral properties of Cy3- and Cy5-labeled oligonucleotides at various distances from the surface of silver island films. The distance to the surface was controlled by alternating layers of biotinylated bovine serum albumin (BSA) and avidin, followed by binding of a biotinylated oligonucleotide. The maximum enhancement of fluorescence near a factor of 12 was observed for the first BSA-avidin layer, with the enhancement decreasing to 2-fold for six layers. The minimum lifetimes were observed for the first BSA-avidin layer, and were about 25-fold shorter than on quartz slides without silver, with the lifetimes being about 2-fold shorter for six BSA-avidin layers. These results suggest that maximum fluorescence enhancements occur about 90A from the silver surface, a distance readily obtained by one or two layers of proteins.     

Analysis of resonance energy transfer in model membranes: role of orientational effects

The model of resonance energy transfer (RET) in membrane systems containing donors randomly distributed over two parallel planes separated by fixed distance and acceptors confined to a single plane is presented. Factors determining energy transfer rate are considered with special attention being given to the contribution from orientational heterogeneity of the donor emission and acceptor absorption transition dipoles. Analysis of simulated data suggests that RET in membranes, as compared to intramolecular energy transfer, is substantially less sensitive to the degree of reorientational freedom of chromophores due to averaging over multiple donor-acceptor pairs. The uncertainties in the distance estimation resulting from the unknown mutual orientation of the donor and acceptor are analyzed.     

Fluorescence properties of labeled proteins near silver colloid surfaces

The fluorescence properties of a monolayer of labeled avidin molecules were studied near silver island films. We first adsorbed a monolayer of biotinylated-BSA as a base that was used to capture labeled avidin molecules. For labeled avidin on silver island films, we observed an increase of the fluorescence intensity of between 18 and 80 with one-photon excitation and up to several hundredfold or larger with two-photon excitation. The probes were moderately more photostable in the presence of silver islands. There was also a dramatic decrease in the lifetimes with the amplitude-weighted values decreasing from 7- to 35-fold. The data suggest that these spectral changes are due to both increased rates of excitation near the metallic particles and increases in the rates of radiative decay. Because these silver island surfaces are very heterogeneous, we are hopeful that larger increases in intensity and photostability can be obtained for probes situated at an optimal distance from the ideal island surfaces.     

Fluorescence resonance energy transfer between specific-labeled sites on DNA.

Fluorescence resonance energy transfer on DNA has been studied for the estimation of distances between specific sites. Two kind of fluorophores, donor and acceptor, were incorporated on double-stranded DNA via phosphorothioate linkage (Sp, Rp, or racemic mixture). The thermal stability of labeled DNA's was slightly dependent on the stereochemical orientation of fluorophore, however all of the duplex structures were stable under the conditions for fluorescence study. The distances between donor and acceptor fluorophores, estimated from fluorescence energy transfer, generally agreed with the expected distance in a B-type DNA for the limiting distance.     

Fluorescence resonance energy transfer between donor-acceptor pair on two oligonucleotides hybridized adjacently to DNA template

We use fluorescein as the energy donor and rhodamine as the acceptor to measure the efficiency of fluorescence resonance energy transfer (FRET) in a set of hybridized DNA constructs. The two fluorophores are covalently attached via linkers to two separate oligonucleotides with fluorescein at the 3' end of one oligonucleotide and rhodamine at the 5' end or in the middle of another nucleotide. For the FRET analysis both fluorophore-labeled oligonucleotides are hybridized to adjacent sections of the same DNA template to form a three-component duplex with a one base gap between the two labeled oligonucleotides. A similar configuration is implemented for a quantitative real-time polymerase chain reaction (PCR) with LightCycler technology, where a 1-5 base separation between donor and acceptor is recommended to optimize energy transfer efficiencies. Our constructs cover donor-acceptor separations from 2 to 17 base pairs (approximately 10-70 A). The results show that, when the two fluorophores are located at close distances (less than 8 base separation), FRET efficiencies are above 80%, although there may be ground-state interactions between fluorophores when the separation is under about 6 bases. Modeling calculations are used to predict the structure of these three-component constructs. The duplex mostly retains a normal double helical structure, although slight bending may occur near the unpaired base in the DNA template. Stable and reproducible energy transfer is also observed over the distance range investigated here in real-time thermal cycling. The study identifies important parameters that determine FRET response in applications such as real-time PCR.     

Resonance energy transfer between tryptophan 57 in the epsilon subunit and pyrene maleimide labeled gamma subunit of the chloroplast ATP synthase

The intrinsic fluorescence of the catalytic portion of the chloroplast ATP synthase (CF1) is quenched when cysteine 322, the penultimate amino acid of the gamma subunit, is specifically labeled with pyrene maleimide (PM). The epsilon subunit of CF1 contains the only two residues of tryptophan, which dominate the intrinsic fluorescence of unlabeled CF1. CF1 deficient in the epsilon subunit (CF1-epsilon) was reconstituted with mutant epsilon subunits in which phenylalanine replaced tryptophan at position 15 (epsilonW15F) and position 57 (epsilonW15/57F). CF1(epsilonW15F) containing a single tryptophan, epsilonW57, was labeled with PM at gammaC322. Resonance energy transfer (RET) from epsilonW57 to PM on gammaC322 occurred with an efficiency of energy transfer of 20%. RET was also observed from epsilonW57 to PM attached to the disulfide thiols of the gamma subunit (gammaC199,205) with an efficiency of approximately 45%. The R(o) (the distance at which the efficiency of energy transfer is 50%) for the epsilonW57 and PM donor/acceptor pair is 30 A, indicating that both gammaC322 and gammaC199,205 must be within 40 A of epsilonW57. These RET measurements show that both gammaC322 and gammaC199,205 are located near the base of the alpha/beta hexamer. This places the C-terminus of CF1 gamma much closer to epsilon than hypothesized based on homology to crystal structures of mitochondrial F1. These new RET measurements also allow the alignment of the predicted epsilon subunit structure. The orientation is similar to that predicted from cross-linking and mutational studies for the epsilon subunit of Escherichia coli F1.     

On the possibility of long-wavelength long-lifetime high-quantum-yield luminophores

We describe an approach to creating a new class of luminophores which display both long wavelength emissions exceeding 600 nm and long lifetimes. These luminophores are based on resonance energy transfer (RET) from a long lifetime donor to a short lifetime but long wavelength acceptor. We demonstrated the possibility of obtaining these desirable spectral properties using donors and acceptors noncovalently bound to DNA. The donor was a ruthenium (Ru) metal-ligand complex in which one of the diimine ligands intercalated into double-helix DNA. The acceptors were either nile blue, TOTO-3, or TO-PRO-3. Upon binding of the acceptor to donor-labeled DNA, we found that the acceptor quantum yield was remarkably enhanced so that the wavelength-integrated intensities of the donor and acceptor bound to DNA were many-fold greater than the intensity of the donor and acceptor alone when separately bound to DNA. The origin of this effect is efficient energy transfer from the donor. Under these conditions the effective overall quantum yield approaches that of the acceptor. Importantly, the increased quantum yield can be obtained while maintaining usefully long apparent acceptor lifetimes of 30 to 80 ns. The effect of an increased quantum yield from a low quantum yield donor may find use in assays to detect macromolecular binding interactions. These results suggest the synthesis of covalently linked donor-acceptor pairs with the desirable spectral properties of long wavelength emission, high quantum yield, and moderately long lifetimes for gated detection.     

Improving lanthanide-based resonance energy transfer detection by increasing donor-acceptor distances

Lanthanide-based resonance energy transfer (LRET) is an established method for measuring or detecting proximity between a luminescent lanthanide (energy donor) and an organic fluorophore (energy acceptor). Because resonance energy transfer is a distance-dependent phenomenon that increases in efficiency to the 6th power of the distance between the donor and the acceptor, assay systems are often designed to minimize donor-acceptor distances. However, the authors show that because of the R(6) relationship between transfer efficiency and sensitized emission lifetime, energy transfer can be difficult to measure in a time-gated manner when the donor-acceptor distance is small relative to the F?rster radius. In such systems, the advantages inherent in time-resolved, ratiometric measurements are lost but can be regained by designing the system such that the average donor-acceptor distance is increased.     

Conformations within soluble oligomers and insoluble aggregates revealed by resonance energy transfer

A fluorescently labeled 20‐residue polyglutamic acid (polyE) peptide 20 amino acid length polyglutamic acid (E₂₀) was used to study structural changes which occur in E₂₀ as it co‐aggregates with other unlabeled polyE peptides. Resonance energy transfer (RET) was performed using an o‐aminobenzamide donor at the N‐terminus and 3‐nitrotyrosine acceptor at the C‐terminus of E₂₀. PolyE aggregates were not defined as amyloid, as they were nonfibrillar and did not bind congo red. Circular dichroism measurements indicate that polyE aggregation involves a transition from α‐helical monomers to aggregated β‐sheets. Soluble oligomers are also produced along with aggregates in the reaction, as determined through size exclusion chromatography. Time‐resolved and steady‐state RET measurements reveal four dominant E₂₀ conformations: (1) a partially collapsed conformation (24 Å donor–acceptor distance) in monomers, (2) an extended conformation in soluble oligomers (>29 Å donor–acceptor distance), (3) a minor partially collapsed conformation (22 Å donor‐acceptor distance) in aggregates, and (4) a major highly collapsed conformation (13 Å donor–acceptor distance) in aggregates. These findings demonstrate the use of RET as a means of determining angstrom‐level structural details of soluble oligomer and aggregated states of proteins. © 2009 Wiley Periodicals, Inc. Biopolymers 93: 299–317, 2010. This article was originally published online as an accepted preprint. The “Published Online” date corresponds to the preprint version. You can request a copy of the preprint by emailing the Biopolymers editorial office at biopolymers@wiley.com     

Classical Molecular Dynamics Simulation of Kappa Squared Factor in Resonance Energy Transfer for Linear Dipole Models

Molecular dynamics simulations of linear models interacting through a dipolar Kihara intermolecular potential are presented. Molecular orientation correlations are used to calculate the orientational factor kappa squared in the resonance energy transfer (RET) as a function of the intermolecular separation. The distance, R 0 (2/3), at which the simulated systems show an isotropic behavior is calculated and an analysis of the dependence of R 0 (2/3) on microscopic properties (molecular aspect ratio and dipole moment) as well on thermodynamics (temperature and density) is presented. An explanation of the use of metallic cations as probes in RET is given and some relations of our models with biological molecules are pointed out.     

A flexible approach to the calculation of resonance energy transfer efficiency between multiple donors and acceptors in complex geometries

Resonance energy transfer provides a practical way to measure distances in the range of 10-100 A between sites in biological molecules. Although the relationship between the efficiency of energy transfer and the distance between sites is well described for a single pair of fluorophores, the situation is more difficult when more than two fluorophores are present. Using a Monte Carlo calculation scheme, we demonstrate how resonance energy transfer can be used to measure distances between fluorophores in complex geometries. We demonstrate the versatility of the approach by calculating the efficiency of energy transfer for individual fluorophores randomly distributed in two and three dimensions, for linked pairs of donors and acceptors and pentameric structures of five linked fluorophores. This approach can be used to relate the efficiency of energy transfer to the distances between fluorophores, R0, molecular concentrations, laser power, and donor/acceptor ratios in ensembles of molecules or when many fluorophores are attached to a single molecule such as in multimeric proteins.     

Calculation of resonance energy transfer in crowded biological membranes.

Analytical and numerical models were developed to describe fluorescence resonance energy transfer (RET) in crowded biological membranes. It was assumed that fluorescent donors were linked to membrane proteins and that acceptors were linked to membrane lipids. No restrictions were placed on the location of the donor within the protein or the partitioning of acceptors between the two leaflets of the bilayer; however, acceptors were excluded from the area occupied by proteins. Analytical equations were derived that give the average quantum yield of a donor at low protein concentrations. Monte Carlo simulations were used to generate protein and lipid distributions that were linked numerically with RET equations to determine the average quantum yield and the distribution of donor fluorescence lifetimes at high protein concentrations, up to 50% area fraction. The Monte Carlo results show such crowding always reduces the quantum yield, probably because crowding increases acceptor concentrations near donor-bearing proteins; the magnitude of the reduction increases monotonically with protein concentration. The Monte Carlo results also show that the distribution of fluorescence lifetimes can differ markedly, even for systems possessing the same average lifetime. The dependence of energy transfer on acceptor concentration, protein radius, donor position within the protein, and the fraction of acceptors in each leaflet was also examined. The model and results are directly applicable to the analysis of RET data obtained from biological membranes; their application should result in a more complete and accurate determination of the structures of membrane components.     

Resonance energy transfer microscopy: observations of membrane-bound fluorescent probes in model membranes and in living cells

A conventional fluorescence microscope was modified to observe the sites of resonance energy transfer (RET) between fluorescent probes in model membranes and in living cells. These modifications, and the parameters necessary to observe RET between membrane-bound fluorochromes, are detailed for a system that uses N-4-nitrobenzo-2-oxa-1,3-diazole (NBD) or fluorescein as the energy donor and sulforhodamine as the energy acceptor. The necessary parameters for RET in this system were first optimized using liposomes. Both quenching of the energy donor and sensitized fluorescence of the energy acceptor could be directly observed in the microscope. RET microscopy was then used in cultured fibroblasts to identify those intracellular organelles labeled by the lipid probe, N-SRh-decylamine (N-SRh-C10). This was done by observing the sites of RET in cells doubly labeled with N-SRh-C10 and an NBD-labeled lipid previously shown to label the endoplasmic reticulum, mitochondria, and nuclear envelope. RET microscopy was also used in cells treated with fluorescein-labeled Lens culinaris agglutinin and a sulforhodamine derivative of phosphatidylcholine to examine the internalization of plasma membrane lipid and protein probes. After internalization, the fluorescent lectin resided in most, but not all of the intracellular compartments labeled by the fluorescent lipid, suggesting sorting of the membrane-bound lectin into a subset of internal compartments. We conclude that RET microscopy can co-localize different membrane-bound components at high resolution, and may be particularly useful in examining temporal and spatial changes in the distribution of fluorescent molecules in membranes of the living cell.     

Excitation energy transfer studies on the proximity between SH1 and the adenosinetriphosphatase site in myosin subfragment 1

Excitation energy transfer studies were carried out to determine the distance between the adenosinetriphosphatase (ATPase) site and a unique "fast-reacting" sulfhydryl (referred to as SH1) in myosin subfragment 1. The fluorescent moiety of the probe N-(iodoacetyl)-N'-(5-sulfo-1-naphthyl)ethylene-diamine was used as the donor attached at SH1. The chromophoric nucleotide analogue 2'(3')-0-(2,4,6-trinitrophenyl)adenosine 5'-diphosphate was used as the acceptor noncovalently bound at the ATPase site. The energy transfer efficiency was found to be 56% by measuring the decrease in donor fluorescence lifetime. The critical transfer distance, R0(2/3), was determined to be 40.3 A. Since both donor and acceptor are likely to be rigidly attached, a statistical interpretation of the data was applied (Hillel, Z., & Wu, C.-W. (1976) Biochemistry 15, 2105] to determine distances. The method yielded the following conclusions: most probable distance = 38.7 A; maximum possible distance = 52 A; 10% probability for the distance to be less than 20 A; 3% probability to be less than 15 A. It may be concluded that despite the great influence that the two sites exert on each other, it is not likely that SH1 interacts directly with the ATPase site in myosin subfragment 1. This conclusion is in agreement with the findings of Wiedner et al. [Wiedner, H., Wetzel, R., & Eckstein, F. (1978) J. Biol. Chem. 253, 2763] and Botts et al. [Botts, J., Ue., K., Hozumi, T., & Samet, J. (1979) Biochemistry 18, 5157].     

Fluorescence resonance energy transfer study of the associative state of membrane-bound complexes of complement proteins C5b-8

Human complement protein C8 was labeled with the fluorescent chromophores fluorescein-5-isothiocyanate (FITC), 3-(4-isothiocyanatophenyl)-7-diethylamine-4-methyl coumarin (IPM), eosin-5-isothiocyanate (EOS), or Texas Red (sulforhodamine-101-sulfonyl chloride; TR) with only minor reduction in the specific hemolytic activity of the protein. The distribution of C5b-8 complexes bound to sheep erythrocyte membranes was investigated by monitoring fluorescence resonance energy transfer (RET) between the following RET donor/acceptor pairs of labeled C8: FITC-C8/EOS-C8, IPM-C8/EOS-C8, and FITC-C8/TR-C8. On binding to membranes containing pre-formed C5b67 complexes, specific RET was detected for each of the donor/acceptor pairs of labeled C8 investigated. In contrast, no energy transfer was observed for these RET donor/acceptor pairs of labeled C8 incubated in the presence of control membranes or in membrane-free solution. On the basis of a consideration of the transfer efficiency that would be expected for donor/acceptor pairs of labeled C8 that were uniformly dispersed on the membrane surface, these results suggest that C5b-8 complexes are aggregated into polymeric clusters when membrane-bound. The efficiency of donor-C8 to acceptor-C8 RET--and the hemolytic activity of membrane-bound C5b-8 (in the absence of C9)--are both related to the surface density of membrane-bound C5b67, suggesting that the physical clustering of the membrane-inserted C5b-8 complex may be related to the expression of its cytolytic activity.     

Fluorescence lifetime imaging of nuclear DNA: effect of fluorescence resonance energy transfer

BACKGROUND: DNA fluorescence dyes have been used to study DNA dynamics, chromatin structure, and cell cycle analysis. However, most microscopic fluorescence studies of DNA use only steady-state measurements and do not take advantage of the additional information content of the time-resolved fluorescence. In this paper, we combine fluorescence imaging of DNA with time-resolved measurements to examine the proximity of donors and acceptors bound to chromatin. METHODS: We used frequency-domain fluorescence lifetime imaging microscopy to study the spatial distribution of DNA-bound donors and acceptors in fixed 3T3 nuclei. Over 50 cell nuclei were imaged in the presence of an AT-specific donor, Hoechst 33258 (Ho), and a GC-specific acceptor, 7-aminoactinomycin D (7-AAD). RESULTS: The intensity images of Ho alone showed a spatially irregular distribution due to the various concentrations of DNA or AT-rich DNA throughout the nuclei. The lifetime imaging of the Ho-stained nuclei was typically flat. Addition of 7-AAD decreased the fluorescence intensity and lifetime of the Ho-stained DNA. The spatially dependent phase and modulation values of Ho in the presence of 7-AAD showed that the Ho decay becomes nonexponential, as is expected for a resonance energy transfer (RET) with multiple acceptors located over a range of distances. In approximately 40 nuclei, the intensity and lifetime decrease was spatially homogeneous. In approximately 10 nuclei, addition of 7-AAD resulted in a spatially nonhomogeneous decrease in intensity and lifetime. The RET efficiency was higher in G(2)/M than in G(0/1) phase cells. CONCLUSIONS: Because RET efficiency depends on the average distance between Ho and 7-AAD, data suggest that the heterogeneity of lifetimes and spatial variation of the RET efficiency are caused by the presence of highly condensed regions of DNA in nuclei.