DNA probes using fluorescence resonance energy transfer (FRET): designs and applications.

Fluorescence resonance energy transfer (FRET) is widely used in biomedical research as a reporter method. Oligonucleotides with a DNA backbone and one or several chromophore tags have found multiple applications as FRET probes. They are especially advantageous for the real-time monitoring of biochemical reactions and in vivo studies. This paper reviews the design and applications of various DNA-based probes that use FRET The approaches used in the design of new DNA FRET probes are discussed.     

Intracellular oligonucleotide hybridization detected by fluorescence resonance energy transfer (FRET).

Fluorescence resonance energy transfer (FRET) was used to study hybrid formation and dissociation after microinjection of oligonucleotides (ODNs) into living cells. A 28-mer phosphodiester ODN (+PD) was synthesized and labeled with a 3' rhodamine (+PD-R). The complementary, antisense 5'-fluorescein labeled phosphorothioate ODN (-PT-F) was specifically quenched by addition of the +PD-R. In solution, the -PT-F/+PD-R hybrid had a denaturation temperature of 65 +/- 3 degrees C detected by both absorbance and FRET. Hybridization between the ODNs occurred within 1 minute at 17 microM and was not appreciably affected by the presence of non-specific DNA. The pre-formed hybrid slowly dissociated (T1/2 approximately 3 h) in the presence of a 300-fold excess of the unlabeled complementary ODN and could be degraded by DNAse I. Upon microinjection into the cytoplasm of cells, pre-formed fluorescent hybrids dissociated with a half-time of 15 minutes, which is attributed to the degradation of the phosphodiester. Formation of the hybrid from sequentially injected ODNs was detected by FRET transiently in the cytoplasm and later in the cell nucleus, where nearly all injected ODNs accumulate. This suggests that antisense ODNs can hybridize to an intracellular target, of exogenous origin in these studies, in both the cytoplasm and the nucleus.     

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.     

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.     

RecQ helicase-catalyzed DNA unwinding detected by fluorescence resonance energy transfer

A fluorometric assay was used to study the DNA unwinding kinetics induced by Escherichiacoli RecQ helicase.This assay was based on fluorescence resonance energy transfer and carried out onstopped-flow,in which DNA unwinding was monitored by fluorescence emission enhancement of fluoresceinresulting from helicase-catalyzed DNA unwinding.By this method,we determined the DNA unwinding rateof RecQ at different enzyme concentrations.We also studied the dependences of DNA unwinding magnitudeand rate on magnesium ion concentration.We showed that this method could be used to determine thepolarity of DNA unwinding.This assay should greatly facilitate further study of the mechanism for RecQ-catalyzed DNA unwinding.     

DNA tetraplex formation studied with fluorescence resonance energy transfer.

It is emerging that DNA tetraplexes are pivotal for many major cellular processes, and techniques that assess their structure and nature to the point are under development. Here we show how the structural conversion of largely unstructured single-stranded DNA molecules into compact intrastrand DNA tetraplexes can be monitored by fluorescence resonance energy transfer. We recently reported that intrastrand tetraplex formation takes place in a nuclease hypersensitive element upstream of the human c-myc proto-oncogene. Despite the highly repetitive guanine-rich sequence of the hypersensitive element, fluorescence resonance energy transfer measurements indicate that only one well defined tetraplex structure forms therein. The proposed structure, which is specifically stabilized by potassium ions in vitro, has a core of three stacked guanine tetrads that is capped by two intrastrand A-T base pairs.     

Characterization of DNA/lipid complexes by fluorescence resonance energy transfer

Fluorescence resonance energy transfer (FRET) is a potential method for the characterization of DNA-cationic lipid complexes (lipoplexes). In this work, we used FRET models assuming a multilamellar lipoplex arrangement. The application of these models allows the determination of the distance between the fluorescent intercalator on the DNA and a membrane dye on the lipid, and/or the evaluation of encapsulation efficiencies of this liposomal vehicle. The experiments were carried out in 1,2-dioleoyl-3-trimethylammonium-propane/pUC19 complexes with different charge ratios. We used 2-(3-(diphenylhexatrienyl)propanoyl)-1-hexadecanoyl-sn-glycero-3-phosphocholine (DPH-PC) and 2-(4,4-difluoro-5-octyl-4-bora-3a,4a-diaza-s-indacene-3-pentanoyl)-1-hexadecanoyl-sn-glycero-3-phosphocholine (BODIPY-PC) as membrane dyes, and ethidium bromide (EtBr) and BOBO-1 as DNA intercalators. In cationic complexes (charge ratios (+/-) >or= 2), we verified that BOBO-1 remains bound to DNA, and FRET occurs to the membrane dye. This was also confirmed by anisotropy and lifetime measurements. In complexes with all DNA bound to the lipid (charge ratio (+/-) = 4), we determined 27 A as the distance between the donor and acceptor planes (half the repeat distance for a multilamellar arrangement). In complexes with DNA unbound to the lipids (charge ratio (+/-) = 0.5 and 2), we calculated the encapsulation efficiencies. The presented FRET methodology is, to our knowledge, the first procedure allowing quantification of lipid-DNA contact.     

Trajectory of nucleosomal linker DNA studied by fluorescence resonance energy transfer

While the structure of the nucleosome core is known in atomic detail, the precise geometry of the DNA beyond the core particle is still unknown. We have used fluorescence resonance energy transfer (FRET) for determining the end-to-end distance of DNA fragments assembled with histones into nucleosomes. The DNA of a length of 150-220 bp was labeled with rhodamine-X on one end and fluorescein or Alexa 488 on the other. Assembling nucleosomes on these DNA fragments leads to a measurable energy transfer. The end-to-end distance computed from the FRET increases from 60 +/- 5 A at 150 bp to 75 +/- 5 A at 170 bp without measurable change above it. These distances are compatible with different geometries of the linker DNA, all having in common that no crossing can be observed up to 220 bp. Addition of H1 histone leads to an increase in energy transfer, indicating a compaction of the linker DNA toward the nucleosome.     

Detection of programmed cell death using fluorescence energy transfer.

Fluorescence energy transfer (FRET) can be generated when green fluorescent protein (GFP) and blue fluorescent protein (BFP) are covalently linked together by a short peptide. Cleavage of this linkage by protease completely eliminates FRET effect. Caspase-3 (CPP32) is an important cellular protease activated during programmed cell death. An 18 amino acid peptide containing CPP32 recognition sequence, DEVD, was used to link GFP and BFP together. CPP32 activation can be monitored by FRET assay during the apoptosis process.     

Rapid kinetic characterization of hammerhead ribozymes by real-time monitoring of fluorescence resonance energy transfer (FRET)

In established methods for analyzing ribozyme kinetics, radiolabeled RNA substrates are primarily used. Each data point requires the cumbersome sampling, gel electrophoretic separation, and quantitation of reaction products, apart from the continuous loss of substrate by radioactive decay. We have used stable, double fluorescent end-labeled RNA substrates. Fluorescence of one fluorophore is quenched by intramolecular energy transfer (FRET). Upon substrate cleavage, both dyes become separated in two RNA products and fluorescence is restored. This can be followed in real time and ribozyme reactions can be analyzed under multiple (substrate excess) and under single (ribozyme excess) turnover conditions. A detailed comparison of unlabeled, single, and double fluorescent-labeled RNAs revealed moderate kinetic differences. Results with two systems, hammerhead ribozymes in I/II (small ribozyme, large substrate) and in I/III format (large ribozyme, small substrate), are reported.     

Application of spectral imaging microscopy in cytomics and fluorescence resonance energy transfer (FRET) analysis.

BACKGROUND: Specific signal detection has been a fundamental issue in fluorescence microscopy. In the context of tissue samples, this problem has been even more pronounced, with respect to spectral overlap and autofluorescence. METHODS: Recent improvements in confocal laser scanning microscopy combine sophisticated hardware to obtain fluorescence emission spectra on a single-pixel basis and a mathematical procedure called "linear unmixing" of fluorescence signals. By improving both the specificity of fluorescence acquisition and the number of simultaneously detectable fluorochromes, this technique of spectral imaging (SI) allows complex interrelations in cells and tissues to be addressed. RESULTS: In a comparative approach, SI microscopy on a quantitative basis was compared to conventional bandpass (BP) filter detection, demonstrating substantial superiority of SI with respect to detection accuracy and dye combination. An eight-color immunofluorescence protocol for tissue sections was successfully established. Moreover, advanced use of SI in fluorescence resonance energy transfer (FRET) applications using enhanced green fluorescence protein (EGFP) and enhanced yellow fluorescence protein (EYFP) in a confocal set up could be demonstrated. CONCLUSIONS: This novel technology will help to perform complex multiparameter investigations at the cellular level by increasing the detection specificity and permitting simultaneous use of more fluorochromes than with classical techniques based on emission filters. Moreover, SI significantly extends the possibilities for specialized microscopy applications, such as the visualization of macromolecular interactions or conformational changes, by detecting FRET.     

Live cell imaging of protein interactions in poliovirus RNA replication complex using fluorescence resonance energy transfer (FRET)

Poliovirus RNA replication is directed by a replication complex on the rosette-like arrangement of membranous vesicles. Proteins derived from the p3 region of the polioviral genome, such as 3D, 3AB, and 3B (VPg), play key roles in the formation and function of the replication complex. In the present study, by using an acceptor photobleaching protocol for fluorescence resonance energy transfer (FRET) imaging, we visualized the interactions of 3D, 3AB, and VPg in living cells. The interaction of 3AB-VPg was determined by live cell FRET analysis. Quantitative analyses showed that the FRET efficiencies of 3AB-3D, VPg-3D, and 3AB-VPg were 3.9 ± 0.4% (n = 36), 4.5 ± 0.4% (n = 39), and 8.3 ± 0.6% (n = 44), respectively, in the cell cytoplasm where viral replication complexes are formed and function. Poliovirus infection enhanced the protein interactions of VPg-3D and 3AB-3D, with FRET efficiencies in the virus-infected cells of 10.7 ± 1.1% (n = 39) and 9.0 ± 0.9% (n = 37), respectively. This method of live cell analysis of protein interactions in the poliovirus RNA replication complex lays the foundation for further understanding of the real-time process of poliovirus RNA replication.     

The estimation of distances between specific backbone-labeled sites in DNA using fluorescence resonance energy transfer.

A series DNA helices of twenty-four base pairs has been prepared for the study of fluorescence resonance energy transfer. Each of the DNA helices contains two phosphorothioate diesters (one in each strand) at pre-selected sites for introduction of the desired donor and acceptor fluorophores. The phosphorothioate-containing oligodeoxynucleotides have been prepared as pure Rp or Sp derivatives or as deastereomeric mixtures. Fluorescein and eosin are employed as the respective donor and acceptor fluorophores. A series of donor-acceptor pairs was generated by labeling of the appropriate phosphorothioate diester with the desired fluorophore and annealing the two complementary DNA strands (one containing the acceptor and one containing the donor fluorophore) to form the double-stranded helix. The 24-mer helices containing two covalently attached fluorophores exhibited some thermal destabilization and the extent of this destabilization was dependent upon the stereochemical orientation of the fluorophore. The Sp derivatives direct the fluorophore out, away from the the DNA helix, while the Rp derivatives direct the fluorophore toward the major groove. As expected, the Sp labeled duplexes were more stable than the corresponding Rp labeled sequences. However, all of the duplex structures formed were stable under the conditions used to measure energy transfer. Energy transfer could be observed with these complexes from the quenching of the donor fluorescence in the presence of the acceptor fluorophore. Using F?rster's theories, distances separating the fluorophores could be calculated that were generally in reasonable agreement with the distances expected in an idealized B-form DNA helix. However anomalous results were obtained for one donor/acceptor pair where the expected distance was less than 20 A. Fluorescence anisotropy values determined in solutions of varying viscosity were quite high suggesting that the fluorophores did not experience complete freedom of movement when attached to the DNA helix.     

DNA bending induced by high mobility group proteins studied by fluorescence resonance energy transfer.

The HMG domains of the chromosomal high mobility group proteins homologous to the vertebrate HMG1 and HMG2 proteins preferentially recognize distorted DNA structures. DNA binding also induces a substantial bend. Using fluorescence resonance energy transfer (FRET), we have determined the changes in the end-to-end distance consequent on the binding of selected insect counterparts of HMG1 to two DNA fragments, one of 18 bp containing a single dA(2) bulge and a second of 27 bp with two dA(2) bulges. The observed changes are consistent with overall bend angles for the complex of the single HMG domain with one bulge and of two domains with two bulges of approximately 90-100 degrees and approximately 180-200 degrees, respectively. The former value contrasts with an inferred value of 150 degrees reported by Heyduk et al. (1) for the bend induced by a single domain. We also observe that the induced bend angle is unaffected by the presence of the C-terminal acidic region. The DNA bend of approximately 95 degrees observed in the HMG domain complexes is similar in magnitude to that induced by the TATA-binding protein (80 degrees), each monomeric unit of the integration host factor (80 degrees), and the LEF-1 HMG domain (107 degrees). We suggest this value may represent a steric limitation on the extent of DNA bending induced by a single DNA-binding motif.     

Myosin structure. Proximity measurements by fluorescence energy transfer

The results of energy transfer experiments on the proximity of six sites on the globular head region of myosin are discussed. A large hydrophobic crevice has been detected on each myosin head which is sufficiently large to accommodate six aromatic rings simultaneously. In the crevice is located a thiol residue not involved in activation of myosin Ca²⁺ ATPase and a lysine residue which is specifically trinitrophenylated with 2, 4, 6-trinitrobenzenesulfonic acid. A second sulfhydryl whose modification activates the Ca²⁺ ATPase is located near the hydrophobic thiol site. The tryptophan whose fluorescence is enhanced by ATP binding is sufficiently close to the thiols and lysine residue to quantitatively transfer its energy to probes at these sites. The site of myosin ATPase has been tentatively located as being near the other five sites by energy transfer to or from synthetic chromophoric substrates. Implications of these results on the possibility of determining the location of the myosin light chain and actin binding sites are discussed.     

Phospholipid vesicle fusion monitored by fluorescence energy transfer.

A method is presented which allows the observation of phospholipid vesicle fusion by the occurrence of Förster resonance energy transfer between the amphiphilic probes dansyldipalmitoylphosphatidylethanolamine and 3-[4-($\text{p}$-N,N-didecylaminostyryl)-1-pyridinium]-propylsulfonate. This method is applied to the Ca⁺⁺ mediated fusion of phosphatidyl serine vesicles.     

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.