Fluorescence resonance energy transfer analysis of the structure of the four-way DNA junction.

We have carried out fluorescence resonance energy transfer (FRET) measurements on four-way DNA junctions in order to analyze the global structure and its dependence on the concentration of several types of ions. A knowledge of the structure and its sensitivity to the solution environment is important for a full understanding of recombination events in DNA. The stereochemical arrangement of the four DNA helices that make up the four-way junction was established by a global comparison of the efficiency of FRET between donor and acceptor molecules attached pairwise in all possible permutations to the 5' termini of the duplex arms of the four-way structure. The conclusions are based upon a comparison between a series of many identical DNA molecules which have been labeled on different positions, rather than a determination of a few absolute distances. Details of the FRET analysis are presented; features of the analysis with particular relevance to DNA structures are emphasized. Three methods were employed to determine the efficiency of FRET: (1) enhancement of the acceptor fluorescence, (2) decrease of the donor quantum yield, and (3) shortening of the donor fluorescence lifetime. The FRET results indicate that the arms of the four-way junction are arranged in an antiparallel stacked X-structure when salt is added to the solution. The ion-related conformational change upon addition of salt to a solution originally at low ionic strength progresses in a continuous noncooperative manner as the ionic strength of the solution increases. The mode of ion interaction at the strand exchange site of the junction is discussed.     

Single-molecule three-color FRET

Fluorescence resonance energy transfer (FRET) measured at the single-molecule level can reveal conformational changes of biomolecules and intermolecular interactions in physiologically relevant conditions. Thus far single-molecule FRET has been measured only between two fluorophores. However, for many complex systems, the ability to observe changes in more than one distance is desired and FRET measured between three spectrally distinct fluorophores can provide a more complete picture. We have extended the single-molecule FRET technique to three colors, using the DNA four-way (Holliday) junction as a model system that undergoes two-state conformational fluctuations. By labeling three arms of the junction with Cy3 (donor), Cy5 (acceptor 1), and Cy5.5 (acceptor 2), distance changes between the donor and acceptor 1, and between the donor and acceptor 2, can be measured simultaneously. Thus we are able to show that the acceptor 1 arm moves away from the donor arm at the same time as the acceptor 2 arm approaches the donor arm, and vice versa, marking the first example of observing correlated movements of two different segments of a single molecule. Our data further suggest that Holliday junction does not spend measurable time with any of the helices unstacked, and that the parallel conformations are not populated to a detectable degree.     

Distortion of DNA junctions imposed by the binding of resolving enzymes: a fluorescence study.

Junction-resolving enzymes are nucleases that are specific for the structure of the four-way DNA junction. The binding of RuvC of Escherichia coli and Hjc of Sulfolobus solfataricus can be followed by an increase in the fluorescence anisotropy of Cy3 terminally attached to one of the helical arms of a four-way junction. By contrast, there was no change in fluorescein anisotropy with the binding of single dimers of these proteins. Fluorescence resonance energy transfer has therefore been used between fluorescein and Cy3 fluorophores attached to the ends of helical arms to analyse the global structure of the junction on protein binding. The results indicate that both enzymes induce a marked change in the global DNA conformation on the binding of a single dimer. The structure of the protein-junction complexes is independent of the presence or absence of divalent metal ions, unlike that of the protein-free junction. The structures of the RuvC and Hjc complexes are different, but both represent a significant opening of the structure compared to the stacked X-structure of the protein-free junction in the presence of magnesium ions. This protein-induced opening is likely to be important in the function of these enzymes.     

Structures of helical junctions in nucleic acids

Our knowledge of the architectural principles of nucleic acid junctions has seen significant recent advances. The conformation of DNA junctions is now well understood, and this provides a new basis for the analysis of important structural elements in RNA. The most significant new data have come from X-ray crystallography of four-way DNA junctions; incidentally showing the great importance of serendipity in science, since none of the three groups had deliberately set out to crystallise a junction. Fortunately the results confirm, and of course extend, the earlier conformational studies of DNA junctions in almost every detail. This is important, because it means that these methods can be applied with greater confidence to new systems, especially in RNA. Methods like FRET, chemical probing and even the humble polyacrylamide gel can be rapid and very powerful, allowing the examination of a large number of sequence variants relatively quickly. Molecular modelling in conjunction with experiments is also a very important component of the general approach. Ultimately crystallography provides the gold standard for structural analysis, but the other, simple approaches have considerable value along the way. At the beginning of this review I suggested two simple folding principles for branched nucleic acids, and it is instructive to review these in the light of recent data. In brief, these were the tendency for pairwise coaxial stacking of helical arms, and the importance of metal ion interactions in the induction of folding. We see that both are important in a wide range of systems, both in DNA and RNA. The premier example is the four-way DNA junction, which undergoes metal ion-induced folding into the stacked X-structure that is based on coaxial stacking of arms. As in many systems, there are two alternative ways to achieve this depending on the choice of stacking partners. Recent data reveal that both forms often exist in a dynamic equilibrium, and that the relative stability of the two conformers depends upon base sequence extending a significant distance from the junction. The three-way junction has provided a good test of the folding principles. Perfect three-way (3H) DNA junctions seem to defy these principles in that they appear reluctant to undergo coaxial stacking of arms, and exhibit little change in conformation with addition of metal ions. Modelling suggests that such a junction is stereochemically constrained in an extended conformation. However, upon inclusion of a few additional base pairs at the centre (to create a 3HS2 junction for example) the additional stereochemical flexibility allows two arms to undergo coaxial stacking. Such a junction exhibits all the properties consistent with the general folding principles, with ion-induced folding into a form based on pairwise coaxial stacking of arms in one of two different conformers. The three-way junction is therefore very much the exception that proves the rule. It is instructive to compare the folding of corresponding species in DNA and RNA, where we find both similarities and differences. The RNA four-way junction can adopt a structure that is globally similar to the stacked X-structure (Duckett et al. 1995a), and the crystal structure of the DNAzyme shows that the stacked X-conformation can include one helical pair in the A-conformation (Nowakowski et al. 1999). However, modelling suggests that the juxtaposition of strands and grooves will be less satisfactory in RNA, and the higher magnesium ion concentration required to fold the RNA junction indicates a lower stability of the antiparallel form. Perhaps the biggest difference between the properties of the DNA and RNA four-way junctions is the lack of an unstacked structure at low salt concentrations for the RNA species. This clearly reflects a major difference in the electrostatic interactions in the RNA junction. In general the folding of branched DNA provides some good indications on the likely folding of the corresponding RNA species, but caution is required in making the extrapolation because the two polymers are significantly different. A number of studies point to the flexibility and malleability of branched nucleic acids, and this turns out to have particular significance in their interactions with proteins. Proteins such as the DNA junction-resolving enzymes exhibit considerable selectivity for the structure of their substrates, which is still not understood at a molecular level. Despite this, it appears to be universally true that these proteins distort the global, and in some cases at least the local, structure of the junctions. The somewhat perplexing result is that the proteins appear to distort the very property that they recognise. In general it seems that four-way DNA junctions are opened to one extent or another by interaction with proteins. (ABSTRACT TRUNCATED)     

The inherent properties of DNA four-way junctions: comparing the crystal structures of holliday junctions

Holliday junctions are four-stranded DNA complexes that are formed during recombination and related DNA repair events. Much work has focused on the overall structure and properties of four-way junctions in solution, but we are just now beginning to understand these complexes at the atomic level. The crystal structures of two all-DNA Holliday junctions have been determined recently from the sequences d(CCGGGACCGG) and d(CCGGTACCGG). A detailed comparison of the two structures helps to distinguish distortions of the DNA conformation that are inherent to the cross-overs of the junctions in this crystal system from those that are consequences of the mismatched dG.dA base-pair in the d(CCGGGACCGG) structure. This analysis shows that the junction itself perturbs the sequence-dependent conformational features of the B-DNA duplexes and the associated patterns of hydration in the major and minor grooves only minimally. This supports the idea that a DNA four-way junction can be assembled at relatively low energetic cost. Both structures show a concerted rotation of the adjacent duplex arms relative to B-DNA, and this is discussed in terms of the conserved interactions between the duplexes at the junctions and further down the helical arms. The interactions distant from the strand cross-overs of the junction appear to be significant in defining its macroscopic properties, including the angle relating the stacked duplexes across the junction.     

Uranyl photoprobing of a four-way DNA junction: evidence for specific metal ion binding.

Metal ions are very important in mediating the folding of nucleic acids, as exemplified by the folding of the four-way DNA junction into the stacked X-conformation. Uranyl ion-mediated photocleavage provides a method for the localization of high-affinity ion binding sites in nucleic acids, and we have applied this to the four-way DNA junction. We have made the following observations. (i) Uranyl ions (UO2(2+)) suppressed the reactivity of junction thymine bases against attack by osmium tetroxide, indicating that the uranyl ion induces folding of the junction into a stacked conformation. (ii) DNA located immediately at the point of strand exchange on the two exchanging strands was hypersensitive to uranyl photocleavage. The relative hypersensitivity was considerably accentuated when the photocleavage was carried out in the presence of citrate ions. This suggests the presence of a tight binding site for the uranyl ion in the junction. (iii) The same positions were significantly protected from uranyl cleavage by the presence of hexamminecobalt (III) or spermidine. These ions are known to induce the folded conformation of the four-way junction with high efficiency, suggesting a direct competition between the ions. By contrast, magnesium ions failed to generate a similar protection against photocleavage. These results suggest that the uranyl, hexamminecobalt (III) and spermidine ions compete for the same high affinity binding site on the junction. This site is located at the centre of the junction, at the point where the exchanging strands pass between the stacked helices. We believe that we have observed the first known example of a metal ion 'footprint' on a folded nucleic acid structure.     

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.     

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.     

Single-molecule nanopositioning: structural transitions of a helicase-DNA complex during ATP hydrolysis

The conformational states of Escherichia coli Rep helicase undergoing ATP hydrolysis while bound to a partial-duplex DNA (pdDNA) were studied using single-molecule FRET. Crystallographic studies showed that Rep bound to single-stranded DNA can exist in open and closed conformations that differ in the orientation of the 2B subdomain. FRET measurements between eight Rep mutants donor-labeled at different residues and pdDNA acceptor-labeled at the junction were conducted at each of the four nucleotide states. The positions of donor-labeled residues, based on crystal structure, and FRET measurements between these donor molecules and the acceptor fluorophore at the DNA junction were used to predict the most likely position for the DNA junction using a triangulation algorithm. These predicted junction positions are compared with the crystal structure to determine whether the open or closed conformation is more consistent with the FRET data. Our data revealed that there are two distinct Rep-pdDNA conformations in the ATPγS and ADP states, an unexpected finding. The primary conformation is similar to that observed in nucleotide-free and ADP.Pi states, and the secondary conformation is a novel conformation where the duplex DNA and 2B subdomain moved as a unit by 13 Å relative to the rest of the protein. The primary conformation found in all nucleotide states is consistent with the closed conformation of the crystal structure however; the secondary conformation is a new conformation that has not been observed before. We discuss the possible implications of this newly observed conformation.     

Structure, dynamics, and branch migration of a DNA Holliday junction: a single-molecule fluorescence and modeling study

The Holliday junction (HJ) is a central intermediate of various genetic processes, including homologous and site-specific DNA recombination and DNA replication. Elucidating the structure and dynamics of HJs provides the basis for understanding the molecular mechanisms of these genetic processes. Our previous single-molecule fluorescence studies led to a model according to which branch migration is a stepwise process consisting of consecutive migration and folding steps. These data led us to the conclusion that one hop can be more than 1 basepair (bp); moreover, we hypothesized that continuous runs over the entire sequence homology (5 bp) can occur. Direct measurements of the dependence of the fluorescence resonance energy transfer (FRET) value on the donor-acceptor (D-A) distance are required to justify this model and are the major goal of this article. To accomplish this goal, we performed single-molecule FRET experiments with a set of six immobile HJ molecules with varying numbers of bps between fluorescent dyes placed on opposite arms. The designs were made in such a way that the distances between the donor and acceptor were equal to the distances between the dyes formed upon 1-bp migration hops of a HJ having 10-bp homology. Using these designs, we confirmed our previous hypothesis that the migration of the junction can be measured with bp accuracy. Moreover, the FRET values determined for each acceptor-donor separation corresponded very well to the values for the steps on the FRET time trajectories, suggesting that each step corresponds to the migration of the branch at a defined depth. We used the dependence of the FRET value on the D-A distance to measure directly the size for each step on the FRET time trajectories. These data showed that one hop is not necessarily 1 bp. The junction is able to migrate over several bps, detected as one hop and confirming our model. The D-A distances extracted from the FRET properties of the immobile junctions formed the basis for modeling the HJ structures. The composite data fit a partially opened, side-by-side model with adjacent double-helical arms slightly kinked at the four-way junction and the junction as a whole adopting a global X-shaped form that mimics the coaxially stacked-X structure implicated in previous solution studies.     

Fluorescence resonance energy transfer (FRET) and competing processes in donor-acceptor substituted DNA strands: a comparative study of ensemble and single-molecule data

We studied the fluorescence resonance energy transfer (FRET) efficiency of different donor-acceptor labeled model DNA systems in aqueous solution from ensemble measurements and at the single molecule level. The donor dyes: tetramethylrhodamine (TMR); rhodamine 6G (R6G); and a carbocyanine dye (Cy3) were covalently attached to the 5'-end of a 40-mer model oligonucleotide. The acceptor dyes, a carbocyanine dye (Cy5), and a rhodamine derivative (JA133) were attached at modified thymidine bases in the complementary DNA strand with donor-acceptor distances of 5, 15, 25 and 35 DNA-bases, respectively. Anisotropy measurements demonstrate that none of the dyes can be observed as a free rotor; especially in the 5-bp constructs the dyes exhibit relatively high anisotropy values. Nevertheless, the dyes change their conformation with respect to the oligonucleotide on a slower time scale in the millisecond range. This results in a dynamic inhomogeneous distribution of donor/acceptor (D/A) distances and orientations. FRET efficiencies have been calculated from donor and acceptor fluorescence intensity as well as from time-resolved fluorescence measurements of the donor fluorescence decay. Dependent on the D/A pair and distance, additional strong fluorescence quenching of the donor is observed, which simulates lower FRET efficiencies at short distances and higher efficiencies at longer distances. On the other hand, spFRET measurements revealed subpopulations that exhibit the expected FRET efficiency, even at short D/A distances. In addition, the measured acceptor fluorescence intensities and lifetimes also partly show fluorescence quenching effects independent of the excitation wavelength, i.e. either directly excited or via FRET. These effects strongly depend on the D/A distance and the dyes used, respectively. The obtained data demonstrate that besides dimerization at short D/A distances, an electron transfer process between the acceptor Cy5 and rhodamine donors has to be taken into account. To explain deviations from FRET theory even at larger D/A distances, we suggest that the pi-stack of the DNA double helix mediates electron transfer from the donor to the acceptor, even over distances as long as 35 base pairs. Our data show that FRET experiments at the single molecule level are rather suited to resolve fluorescent subpopulations in heterogeneous mixture, information about strongly quenched subpopulations gets lost.     

Analysis of fluorescence energy transfer in duplex and branched DNA molecules

Nonradiative fluorescence energy transfer (FET) is thought to be a highly sensitive measure of distance, occurring through a dipole coupling (Forster) mechanism in which the efficiency of FET depends on the inverse sixth power of the distance between fluorophores. The current work assesses the utility of FET for measuring distances in duplex and branched DNA molecules. The apparent efficiencies of FET between donor (fluorescein) and acceptor (eosin) fluorophores attached to opposite ends of oligonucleotide duplexes of varying length were determined; the results suggest that FET is a useful qualitative indicator of distance in DNA molecules. However, the apparent FET efficiency values cannot be fit to the Forster equation without the specification of highly extended DNA-to-fluorophore tethers and motionally restricted fluorophores, conditions that are unlikely to coexist. Three other lines of evidence further suggest that factors in addition to Forster transfer contribute to apparent FET in DNA: (1) The efficiency of FET appears to depend on the base sequence in some instances. (2) Donor fluorescence changes with the extent of thermally induced DNA melting in a sequence-dependent fashion, indicating dye-DNA interactions. (3) The distances between the ends of various pairwise combinations of arms of a DNA four-way junction do not vary as much as expected from previous work. Thus, the occurrence of any nondipolar effects on energy transfer in oligonucleotide systems must be defined before distances in DNA molecules can be quantified by using FET.     

Electrochemical control of a DNA Holliday Junction nanoswitch by Mg2+ ions

The molecular conformation of a synthetic branched, 4-way DNA Holliday junction (HJ) was electrochemically switched between the open and closed (stacked) conformers. Switching was achieved by electrochemically induced quantitative release of Mg²⁺ ions from the oxidised poly(N-methylpyrrole) film (PPy), which contained polyacrylate as an immobile counter anion and Mg²⁺ ions as charge compensating mobile cations. This increase in the Mg²⁺ concentration screened the electrostatic repulsion between the widely separated arms in the open HJ configuration, inducing switching to the closed conformation. Upon electrochemical reduction of PPy, entrapment of Mg²⁺ ions back into the PPy film induced the reverse HJ switching from the closed to open state. The conformational transition was monitored using fluorescence resonance energy transfer (FRET) between donor and acceptor dyes each located at the terminus of one of the arms. The demonstrated electrochemical control of the conformation of the used probe-target HJ complex, previously reported as a highly sequence specific nanodevice for detecting of unlabelled target [Buck, A.H., Campbell, C.J., Dickinson, P., Mountford, C.P., Stoquert, H.C., Terry, J.G., Evans, S.A.G., Keane, L., Su, T.J., Mount, A.R., Walton, A.J., Beattie, J.S., Crain, J., Ghazal, P., 2007. Anal. Chem., 79, 4724–4728], allows the development of electronically addressable DNA nanodevices and label-free gene detection assays.     

Targeting Holliday junctions by origin DNA-binding protein of herpes simplex virus type 1

In the present paper, the interactions of the origin binding protein (OBP) of herpes simplex virus type 1 (HSV1) with synthetic four-way Holliday junctions (HJs) were studied using electrophoresis mobility shift assay and the FRET method and compared with the interactions of the protein with duplex and single-stranded DNAs. It has been found that OBP exhibits a strong preference for binding to four-way and three-way DNA junctions and possesses much lower affinities to duplex and single-stranded DNAs. The protein forms three types of complexes with HJs. It forms complexes I and II which are reminiscent of the tetramer and octamer complexes with four-way junction of HJ-specific protein RuvA of Escherichia coli. The binding approaches saturation level when two OBP dimers are bound per junction. In the presence of Mg²⁺ ions (≥2 mM) OBP also interacts with HJ in the stacked arm form (complex III). In the presence of 5 mM ATP and 10 mM Mg²⁺ ions OBP catalyzes processing of the HJ in which one of the annealed oligonucleotides has a 3′-terminal tail containing 20 unpaired thymine residues. The observed preference of OBP for binding to the four-way DNA junctions provides a basis for suggestion that OBP induces large DNA structural changes upon binding to Box I and Box II sites in OriS. These changes involve the bending and partial melting of the DNA at A+T-rich spacer and also include the formation of HJ containing Box I and Box II inverted repeats and flanking DNA sequences.     

Stacking-unstacking of the dinucleoside monophosphate guanylyl-3'',5''-uridine studied with molecular dynamics.

Molecular dynamics simulations were carried out on two conformations of the dinucleoside monophosphate guanylyl-3',5'-uridine (GpU) in aqueous solution with one sodium counterion. One stacked conformation and one with the C3'-O3'-P-O5' backbone torsion angle twisted 180 degrees to create an unstacked conformation. We observed a relatively stable behavior of the stacked conformation, which remained stacked throughout the simulation, whereas the unstacked conformation showed major changes in the backbone torsion and glycosidic angles. During the simulation the unstacked conformation transformed into a more stacked form and then back again to an unstacked one. The calculated correlation times for rotational diffusion from the molecular dynamics simulations are in agreement with fluorescence anisotropy and nuclear magnetic resonance data. As expected, the correlation times for rotational diffusion of the unstacked conformation were observed to be longer than for the stacked conformation. The 2'OH group may contribute in stabilizing the stacked conformation, where the O2'-H...O4' hydrogen bond occurred in 82.7% of the simulation.     

The dynamic nature of the four-way junction of the hepatitis C virus IRES

Translation is initiated within the RNA of the hepatitis C virus at the internal ribosome entry site (IRES). The IRES is a 341-nucleotide element that contains a four-way helical junction (IIIabc) as a functionally important element of the secondary structure. The junction has three additional, nonpaired nucleotides at the point of strand exchange on one diagonal. We have studied the global conformation and folding of this junction in solution, using comparative gel electrophoresis and steady-state and time-resolved fluorescence resonance energy transfer. In the absence of divalent metal ions, the junction adopts an extended-square structure, in contrast to perfect four-way RNA junctions, which retain coaxial helical stacking under all conditions. The IIIabc junction is induced to fold on addition of Mg(2+), by pairwise coaxial stacking of arms, into the conformer in which the unpaired bases are located on the exchanging strands. Fluorescence lifetime measurements indicate that in the presence of Mg(2+) ions, the IIIabc junction exists in a dynamic equilibrium comprising approximately equal populations of antiparallel and parallel species. These dynamic properties may be important in mediating interactions between the IRES and the ribosome and initiation factors.     

Molecular dynamics simulation of hydrated d(CGGGTACCCG)4 as a four-way DNA Holliday junction and comparison with the crystallographic structure

Molecular dynamics (MD) simulation of decamer sequence (CGGGTACCCG)₄ as a four-way Holliday junction is reported here for 15.0 ns at three different temperatures 100, 200 and 300 K, respectively, using AMBER force field. Particle mesh Ewald method has been utilised to deal long-range interaction potentials. After MD simulation, various parameters of the junction model including backbone and helical parameters have been worked out and the dynamical pathway is discussed. Structural analysis and geometrical calculations were carried out through X3DNA. The computational results obtained are compared with the previously reported crystallographic outcomes. The width and depth of the major and minor grooves of the duplex of the four arms of the DNA junction have been calculated. The variations in the C1′–C1′ distances between the two complementary strands are discussed in detail. A close observation of the results reveals that the conformation of the average simulated structure at low temperature is of ‘B’ form and the structural integrity of the DNA junction having a twofold sequence symmetry is temperature dependent. It also seems that besides the other parameters (i.e. presence of ions, solvents, etc.), temperature may be playing a key role in preserving the structural integrity of the DNA junction.     

The structure of sulfoindocarbocyanine 3 terminally attached to dsDNA via a long, flexible tether

Fluorescence resonance energy transfer (FRET) is an important source of long-range distance information in macromolecules. However, extracting maximum information requires knowledge of fluorophore, donor and acceptor, positions on the macromolecule. We previously determined the structure of the indocarbocyanine fluorophores Cy3 and Cy5 attached to DNA via three-carbon atom tethers, showing that they stacked onto the end of the helix in a manner similar to an additional basepair. Our recent FRET study has suggested that when they are attached via a longer 13-atom tether, these fluorophores are repositioned relative to the terminal basepair by a rotation of ～30°, while remaining stacked. In this study, we have used NMR to extend our structural understanding to the commonly used fluorophore sulfoindocarbocyanine-3 (sCy3) attached to the 5'-terminus of the double-helical DNA via a 13-atom flexible tether (L13). We find that L13-sCy3 remains predominantly stacked onto the end of the duplex, but adopts a significantly different conformation, from that of either Cy3 or Cy5 attached by 3-atom tethers, with the long axes of the fluorophore and the terminal basepair approximately parallel. This result is in close agreement with our FRET data, supporting the contention that FRET data can be used to provide orientational information.     

Definitions and analysis of DNA Holliday junction geometry

A number of single-crystal structures have now been solved of the four-stranded antiparallel stacked-X form of the Holliday junction. These structures demonstrate how base sequence, substituents, and drug and ion interactions affect the general conformation of this recombination intermediate. The geometry of junctions had previously been described in terms of a specific set of parameters that include: (i) the angle relating the ends of DNA duplexes arms of the junction (interduplex angle); (ii) the relative rotation of the duplexes about the helix axes of the stacked duplex arms (J_roll); and (iii) the translation of the duplexes along these helix axes (J_slide). Here, we present a consistent set of definitions and methods to accurately calculate each of these parameters based on the helical features of the stacked duplex arms in the single-crystal structures of the stacked-X junction, and demonstrate how each of these parameters contributes to an overall conformational feature of the structure. We show that the values for these parameters derived from global rather than local helical axes through the stacked bases of the duplex arms are the most representative of the stacked-X junction conformation. In addition, a very specific parameter (J_twist) is introduced which relates the relative orientation of the stacked duplex arms across the junction which, unlike the interduplex angle, is length independent. The results from this study provide a general means to relate the geometric features seen in the crystal structures to those determined in solution.     

Single-laser polarization FRET (polFRET) on the cell surface

A new method for the simultaneous detection of rotational mobility and proximity of cell surface receptors is presented based on cell-by-cell basis measurement of polarized fluorescence intensity components of the donor and acceptor of a FRET system. In addition to the FRET efficiency and the donor and acceptor concentrations, the method makes also possible the determination of the rotational characteristics and the associated fraction of the donors (FRET-fraction). The method is illustrated with flow cytometric and rFLIM measurements on donor–acceptor systems comprising fluorescently labeled whole antibodies and their Fab fragments against epitopes of the MHCI and MHCII cell surface receptors on human lymphoblast cells. Fluorescence anisotropy of donor and acceptor and FRET efficiency were measured for samples of different acceptor-to-donor concentration ratios. Acceptor anisotropy proved to be more sensitive than the donor anisotropy for sensing FRET. After determining the rotational constants of the donor-conjugated antibodies by measurements of FRET in the steady state, and by rFLIM as a reference, the associated fractions of the MHCI and MHCII molecules in their clusters were determined. Besides the flow cytometer and the wide-field rFLIM used in this study, the method can be applied also in other devices capable of dual-anisotropy detection.