Heterodimeric DNA-binding dyes designed for energy transfer: synthesis and spectroscopic properties.

Heterodimeric dyes are described which bind tightly to double-stranded (dsDNA) with large fluorescence enhancements. These dyes are designed to exploit energy transfer between donor and acceptor chromophores to tune the separation between excitation and emission wavelengths. The dyes described here absorb strongly at the 488 nm argon ion line, but emit at different wavelengths, and can be applied to multiplex detection of various targets. The chromophores in these dyes, a thiazole orange-thiazole blue heterodimer (TOTAB), two different thiazole orange-ethidium heterodimers (TOED1 and TOED2), and a fluorescein-ethidium heterodimer (FED), are in each case linked through polymethyleneamine linkers. The emission maxima of the DNA-bound dyes lie at 662 (TOTAB), 614 (TOED 2), and 610 nm (FED). The dyes showed a > 100 fold enhancement of the acceptor chromophore fluorescence on binding to dsDNA and no sequence selectivity. In comparison with direct 488 nm excitation of the constituent monomeric dyes, in the heterodimers the fluorescence of the acceptor chromophores was greatly enhanced and the emission of the donor chromophores quenched by over 90%. The acceptor emission per DNA-bound dye molecule was constant from 100 DNA bp:dye to 20 bp:dye and decreased sharply at higher dye:DNA ratios.     

Quantitative fluorescence resonance energy transfer measurements using fluorescence microscopy.

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

Signal/noise analysis of FRET-based sensors

Molecular sensors based on intramolecular Förster resonance energy transfer (FRET) have become versatile tools to monitor regulatory molecules in living tissue. However, their use is often compromised by low signal strength and excessive noise. We analyzed signal/noise (SNR) aspects of spectral FRET analysis methods, with the following conclusions: The most commonly used method (measurement of the emission ratio after a single short wavelength excitation) is optimal in terms of signal/noise, if only relative changes of this uncalibrated ratio are of interest. In the case that quantitative data on FRET efficiencies are required, these can be calculated from the emission ratio and some calibration parameters, but at reduced SNR. Lux-FRET, a recently described method for spectral analysis of FRET data, allows one to do so in three different ways, each based on a ratio of two out of three measured fluorescence signals (the donor and acceptor signal during a short-wavelength excitation and the acceptor signal during long wavelength excitation). Lux-FRET also allows for calculation of the total abundance of donor and acceptor fluorophores. The SNR for all these quantities is lower than that of the plain emission ratio due to unfavorable error propagation. However, if ligand concentration is calculated either from lux-FRET values or else, after its calibration, from the emission ratio, SNR for both analysis modes is very similar. Likewise, SNR values are similar, if the noise of these quantities is related to the expected dynamic range. We demonstrate these relationships based on data from an Epac-based cAMP sensor and discuss how the SNR changes with the FRET efficiency and the number of photons collected.     

Time-resolved detection of energy transfer: theory and application to immunoassays

Energy-transfer measurements based upon acceptor fluorophore emission are plagued with background fluorescence resulting from absorption of the excitation light by the acceptor fluorophore. The present work examines the use of a long-lifetime donor fluorophore and a short-lifetime acceptor fluorophore, combined with pulsed-laser excitation and electronic gating of detector signals, to separate the component of acceptor emission due to energy transfer from the component due to absorption of the excitation light. Theoretical equations describing the acceptor fluorescence and integrated acceptor fluorescence show that increasing the integration delay relative to the excitation pulse should greatly enhance detection of the energy-transfer component. The time-resolved detection of energy transfer was tested in a competitive immunoassay format in which antibodies to human immunoglobulin G (IgG) F(ab')2 fragments were covalently labeled with pyrenebutyrate (tau = 100 ns) and IgG Fab' fragments were covalently labeled with B-phycoerythrin (tau = 2.5 ns). Solutions containing these two conjugates exhibited energy transfer from the pyrenebutyrate to the B-phycoerythrin upon excitation with a nitrogen laser. Acceptor emission was measured with 0- and 20-ns integration delays and the ratios of the energy-transfer component to the laser-excited component were found to increase by 9- to 15-fold when the 20-ns delay was used in three series of immunoassays. Good agreement between the experimental data and theory was obtained following convolution of the theoretical fluorescence responses with the instrumental response of the fluorometer.     

Detection of Tryptophan to Tryptophan Energy Transfer in Proteins

Förster resonance energy transfer (FRET) studies usually involve observation of intensity or life-time changes in the donor or acceptor molecule and usually these donor and acceptor molecules differ (heterotransfer). The use of polarization to monitor FRET is far less common, although it was one of the first methods utilized. In 1960, Weber demonstrated that homotransfer between tryptophan molecules contributes to depolarization. He also discovered that the efficiency of homotransfer becomes much less effective upon excitation near the red-edge of the absorption. This “red-edge effect” was shown to be a general phenomenon of homotransfer. We have utilized Weber's red-edge effect to study tryptophan homotransfer in proteins. Specifically, we determined the polarization of the tryptophan fluorescence upon excitation at 295 nm and 310 nm (near the red-edge). Rotational diffusion leads to depolarization of the emission excited at either 295 nm or 310 nm, but homotransfer only contributes to depolarization upon excitation at 295 nm. Hence, the 310/295 polarization ratio gives an indication of tryptophan to tryptophan energy transfer. In single tryptophan systems, the 310/295 ratios are generally below 2 whereas in multi-tryptophan systems, the 310/295 ratios can be greater than 3.     

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.     

Characterization of one- and two-photon excitation fluorescence resonance energy transfer microscopy

Advances in molecular biology provide various methods to define the structure and function of the individual proteins that form the component parts of subcellular structures. The ability to see the dynamic behavior of a specific protein inside the living cell became possible through the application of advanced fluorescence resonance energy transfer (FRET) microscope techniques. The fluorophore molecule used for FRET imaging has a characteristic absorption and emission spectrum that should be considered for characterizing the FRET signal. In this article we describe the system development for the image acquisition for one- and two-photon excitation FRET microscopy. We also describe the precision FRET (PFRET) data analysis algorithm that we developed to remove spectral bleed-through and variation in the fluorophore expression level (or concentration) for the donor and acceptor molecules. The acquired images have been processed using a PFRET algorithm to calculate the energy transfer efficiency and the distance between donor and acceptor molecules. We implemented the software correction to study the organization of the apical endosome in epithelial polarized MDCK cells and dimerization of the CAATT/enhancer binding protein alpha (C/EBPalpha). For these proteins, the results revealed that the extent of correction affects the conventionally calculated energy transfer efficiency (E) and the distance (r) between donor and acceptor molecules by 38 and 9%, respectively.     

Improved single nucleotide polymorphisms detection using conjugated polymer/surfactant system and peptide nucleic acid

An improved assay for the detection of single nucleotide polymorphisms (SNP) of mutant DNA using a combination of peptide nucleic acid (PNA) probes, a cationic conjugated polymer (CCP) and non-ionic surfactant is reported. A comparison between CCP/surfactant and CCP alone shows enhancement in the discrimination between mutant and wild type DNA by a factor of two. A discrimination factor of 70% and 92% was calculated for single and five bases mismatched mutants, respectively when using CCP/surfactant. Furthermore, CCP/surfactant provides a strong emissive donor which increases signal to noise ratio and prevents fluctuation in the output signal caused by the suspension nature of the CCP (due to polymer aggregation) in water. The fluorescence resonance energy transfer (FRET) ratio which defined as the ratio of PL emission of the acceptor to that of the donor, was found to be 20% better when the location of the mutation is five bases away from the duplex terminal compared to that in the centre of the duplex. The enhance discrimination referred to the difference in the FRET and reabsorption rates in different types of duplex. The FRET ratio can be very sensitive to the sample excitation strength, emission collection and spectrometer setting.     

Fluorescence resonance energy transfer (FRET) using ssDNA binding fluorescent dye

There is a need for simple and inexpensive methods for genotyping single nucleotide polymorphisms (SNPs) and short insertion/deletion variations (InDels). In this work, I demonstrate that a single-stranded DNA (ssDNA) binding dye can be used as a donor fluorophore for fluorescence resonance energy transfer (FRET). The method presented is a homogenous assay in which detection is based on the FRET from the fluorescence of the ssDNA dye bound to the unmodified detection primer to the fluorescent nucleotide analog incorporated into this detection primer during cyclic template directed primer extension reaction. Collection of the FRET emission spectrum with a scanning fluorescence spectrophotometer allows powerful data analysis. The fluorescence emission signal is modified by the optical properties of the assay vessel. This seems to be a completely neglected parameter. By proper selection of the optical properties of the assay plate one can improve the detection of the fluorescence emission signal.     

Fluorescent resonance energy transfer (FRET) based detection of a multiplex ligation-dependent probe amplification assay (MLPA) product

A fluorescent resonance energy transfer (FRET)-based hybridization assay for detecting multiplex ligation-dependent probe amplification (MLPA) products has been developed, extending the diagnostic power of the technique and demonstrating the possibility of combining MLPA with microarrays for the detection of multiple mutations. FRET is one of the most commonly used detection techniques for hybridization assays. To investigate the applicability of FRET based detection of MLPA products, a sandwich assay was designed to detect gene copy number by exploiting an immobilized probe labeled with an acceptor dye, Alexa Fluor 555, which hybridises to specific PCR amplicons, followed by hybridization of a second probe labeled with the donor dye, Alexa Fluor 488. Following excitation of the Alexa Fluor 488, a FRET signal was produced only if a DNA sequence specific to the BRCA1 exon 13 was present in the test sample. We have verified this assay on a DNA sample of a patient carrying a heterozygous BRCA1 exon 13 deletion using male genomic DNA as control. Here we demonstrate that the DNA sample containing the heterozygous deletion generated a considerably reduced FRET signal as compared to the control male human DNA. Our results show that the FRET design presented in this study can differentiate between reduced copy numbers any genomic DNA sequence after MLPA analysis, and the reported format is applicable to multiplex detection of MLPA products, using microarrays, or optical biosensor arrays, and future work will focus on the demonstration of this.     

Proximity of lectin receptors on the cell surface measured by fluorescence energy transfer in a flow system.

Molecules of the lectin concanavalin A have been labeled separately with the fluorescein and rhodamine chromophores and jointly bound to the surface of transformed Friend erythroleukemia cells. The two dyes constitute an ideal donor-acceptor pair for fluorescence resonance energy transfer thereby permitting the determination of the proximity relationships between bound ligand molecules and the corresponding surface receptors. The transfer efficiency at saturation (about 57%) was measured in a multiparameter flow system using laser excitation at 488 nm and detection of fluorescein and rhodamine emission intensities as well as the emission anisotropy of the rhodamine fluorescence for each cell. The degree of energy transfer was estimated from the quenching of donor emission, the sensitization of acceptor emission, and the depolarization of acceptor fluorescence. The system has been modeled according to a formalism developed by Gennis and Cantor (Biochemistry 11: 2509, 1972). We estimate the separation between the surfaces of bound lectin molecules at saturation to be 0-40 A, a range possibly characteristic for micropatches induced by ligand binding.     

Homebuilt single-molecule scanning confocal fluorescence microscope studies of single DNA/protein interactions

Many technical improvements in fluorescence microscopy over the years have focused on decreasing background and increasing the signal to noise ratio (SNR). The scanning confocal fluorescence microscope (SCFM) represented a major improvement in these efforts. The SCFM acquires signal from a thin layer of a thick sample, rejecting light whose origin is not in the focal plane thereby dramatically decreasing the background signal. A second major innovation was the advent of high quantum-yield, low noise, single-photon counting detectors. The superior background rejection of SCFM combined with low-noise, high-yield detectors makes it possible to detect the fluorescence from single-dye molecules. By labeling a DNA molecule or a DNA/protein complex with a donor/acceptor dye pair, fluorescence resonance energy transfer (FRET) can be used to track conformational changes in the molecule/complex itself, on a single molecule/complex basis. In this methods paper, we describe the core concepts of SCFM in the context of a study that uses FRET to reveal conformational fluctuations in individual Holliday junction DNA molecules and nucleosomal particles. We also discuss data processing methods for SCFM.     

Scanning near-field fluorescence resonance energy transfer microscopy

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

Structural changes of yellow Cameleon domains observed by quantitative FRET analysis and polarized fluorescence correlation spectroscopy

Förster resonance energy transfer (FRET) is a widely used method for monitoring interactions between or within biological macromolecules conjugated with suitable donor-acceptor pairs. Donor fluorescence lifetimes in absence and presence of acceptor molecules are often measured for the observation of FRET. However, these lifetimes may originate from interacting and noninteracting molecules, which hampers quantitative interpretation of FRET data. We describe a methodology for the detection of FRET that monitors the rise time of acceptor fluorescence on donor excitation thereby detecting only those molecules undergoing FRET. The large advantage of this method, as compared to donor fluorescence quenching method used more commonly, is that the transfer rate of FRET can be determined accurately even in cases where the FRET efficiencies approach 100% yielding highly quenched donor fluorescence. Subsequently, the relative orientation between donor and acceptor chromophores is obtained from time-dependent fluorescence anisotropy measurements carried out under identical conditions of donor excitation and acceptor detection. The FRET based calcium sensor Yellow Cameleon 3.60 (YC3.60) was used because it changes its conformation on calcium binding, thereby increasing the FRET efficiency. After mapping distances and orientation angles between the FRET moieties in YC3.60, cartoon models of this FRET sensor with and without calcium could be created. Independent support for these representations came from experiments where the hydrodynamic properties of YC3.60 under ensemble and single-molecule conditions on selective excitation of the acceptor were determined. From rotational diffusion times as found by fluorescence correlation spectroscopy and consistently by fluorescence anisotropy decay analysis it could be concluded that the open structure (without calcium) is flexible as opposed to the rather rigid closed conformation. The combination of two independent methods gives consistent results and presents a rapid and specific methodology to analyze structural and dynamical changes in a protein on ligand binding.     

CTAB enhancement of FRET in DNA structures

The effect of cetyl‐trimethylammonium bromide (CTAB) on enhancing the fluorescence resonance energy transfer (FRET) between two dye‐conjugated DNA strands was studied using fluorescence emission spectroscopy and dynamic light scattering (DLS). For hybridized DNA where one strand is conjugated with a TAMRA donor and the other with a TexasRed acceptor, increasing the concentration of CTAB changes the fluorescence emission properties and improves the FRET transfer efficiency through changes in the polarity of the solvent, neutralization of the DNA backbone and micelle formation. For the DNA FRET system without CTAB, the DNA hybridization leads to contact quenching between TAMRA donor and TexasRed acceptor producing reduced donor emission and only a small increase in acceptor emission. At 50 µM CTAB, however, the sheathing and neutralization of the dye‐conjugated dsDNA structure significantly reduces quenching by DNA bases and dye interactions, producing a large increase in FRET efficiency, which is almost four fold higher than without CTAB.

     

A new type of phosphorescent nanospheres for use in advanced time-resolved multiplexed bioassays

A new concept to design phosphorescent nanospheres is presented. The spheres are distinguishable by their individual decay time and spectral distribution of their emission spectra. They are composed of a phosphorescent ruthenium metal-ligand complex (MLC) dissolved, along with certain strongly fluorescent cyanine dyes, in modified polyacrylonitrile-based nanospheres. Since the emission spectrum of the MLC overlaps the absorption spectrum of the cyanine and both the MLC (the donor) and the cyanine (the acceptor) are in close spatial proximity, efficient resonance energy transfer (RET) does occur. Thus, the nanospheres emit dual luminescence, one from the acceptor dye and the other from the donor MLC. Variation of the concentrations of the acceptor dye results in a varying efficiency of RET, thus making the spheres distinguishable. Hence, a set of multiplexable sphere labels is obtained by using one MLC (acting as the phosphorescent donor and present in constant concentration) and one acceptor dye (which varies in terms of both spectral properties and concentration). The nanospheres can be identified by the emission maximum (reflecting the kind of acceptor dye) and by decay time (reflecting its concentration). Since the same donor MLC is used throughout, all nanospheres can be excited with the same light source.     

DNA torsional dynamics by multifrequency phase fluorometry.

The time decay of the fluorescence polarization anisotropy of calf thymus DNA-ethidium complexes is obtained from measurements with sine-modulated excitation employing the so-called multifrequency phase fluorometry. A torsional dynamics model developed by J. M. Schurr [(1984) Chemical Physics, Vol. 84, pp. 71-96] and translated into the frequency domain is found here to describe accurately DNA-ethidium fluorescence data collected under modulated excitation. At a low dye/DNA ratio (1:400) the value of the DNA torsional constant (alpha = 4.63 +/- 0.2 10(-12) dyne cm) fitting the data agrees very well with the known values of alpha. When the measurements are extended to a higher ethidium/DNA ratio, energy transfer effects between intercalated dyes are observed. A theoretical prediction of the donor and acceptor dye contributions to the fluorescence polarization anisotropy is made here, taking into account also dye-dye distance distributions.     

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.     

New energy transfer dyes for DNA sequencing.

We have synthesized a set of four energy transfer dyes and demonstrated their use in automated DNA sequencing. The donor dyes are the 5- or 6-carboxy isomers of 4'-aminomethylfluorescein and the acceptor dyes are a novel set of four 4,7-dichloro-substituted rhodamine dyes which have narrower emission spectra than the standard, unsubstituted rhodamines. A rigid amino acid linker, 4-aminomethylbenzoic acid, was used to separate the dyes. The brightness of each dye in an automated sequencing instrument equipped with a dual line argon ion laser (488 and 514 nm excitation) was 2-2.5 times greater than the standard dye-primers with a 2 times reduction in multicomponent noise. The overall improvement in signal-to-noise was 4- to 5-fold. The utility of the new dye set was demonstrated by sequencing of a BAC DNA with an 80 kb insert. Measurement of the extinction coefficients and the relative quantum yields of the dichlororhodamine components of the energy transfer dyes showed their values were reduced by 20-25% compared with the dichlororhodamine dyes alone.