Evidence for a DNA triplex in a recombination-like motif: I. Recognition of Watson-Crick base pairs by natural bases in a high-stability triplex

Data are presented on a triplex type with two parallel homologous strands for which triplex formation is almost as strong as duplex formation at least for some sequences and even at pH 7 and 0.2 M NaCl. The evidence mainly rests upon comparing thermodynamic properties of similar systems. A paperclip oligonucleotide d(A12C4T12C4A12) with two linkers C4 obviously can form a triplex with parallel back-folded adenine strand regions, because the single melting transition of this complex splits in two transitions by introducing mismatches only in the third strand region. Respectively, a hairpin duplex d(A12C4T12) and a single strand d(A12) form a triplex as a 1:1 complex in which the second adenine strand is parallel oriented to the homologous one in the Watson-Crick paired duplex. In this system the melting temperature T(m) of the triplex is practically the same as that of the duplex d(A12)-d(T12), at least within a complex concentration range of 0.2-4.0 microM. The melting behaviour of complexes between triplex stabilizing ligand BePI and the system hairpin duplex plus single strand supports the triplex model. Non-denaturing gel electrophoresis suggests the existence of a triplex for a system in which five of the twelve A-T*A base triads are substituted by C-G*C base triads. The recognition between any substituted Watson-Crick base pair (X-Y) in the hairpin duplex d(A4XA7C4T7YT4) and the correspondingly replaced base (Z) in the third strand d(A4ZA7) is mutually selective. All triplexes with matching base substitutions (Z = X) have nearly the same stability (T(m) values from 29 to 33.5 degrees C), whereas triplexes with non-matching substitutions (Z not equal X) show a clearly reduced stability (T(m) values from 15 to 22 degrees C) at 2microM equimolar oligonucleotide concentration. Most nucleic acid triple helices hitherto known are limited to homopurine-homopyrimidine sequences in the target duplex. A stable triplex formation is demonstrated for inhomogeneous sequences tolerating at least 50% pyrimidine content in the homologous strands. On the basis of the surprisingly similar thermodynamic parameters for duplex and triplex, and of the fact that this triplex type seems to be more stable than many other natural DNA triplexes known, and on the basis of semiempirical and molecule mechanical calculations, we postulate bridging interactions of the third strand with the two other strands in the triplex according to the recombination motif. This triplex, denoted by us 'recombination-like form', tolerates heterogeneous base sequences.     

UV spectroscopic identification and thermodynamic analysis of protonated third strand deoxycytidine residues at neutrality in the triplex d(C(+)-T)6:[d(A-G)6.d(C-T)6]; evidence for a proton switch.

Near-UV difference spectral analysis of the triplex formed from d(C-T)6 and d(A-G)6.d(C-T)6 in neutral and acidic solution shows that the third strand dC residues are protonated at pH 7.0, far above their intrinsic pKa. Additional support for ion-dipole interactions between the third strand dC residues and the G.C target base pairs comes from reduced positive dependence of triplet stability on ionic strength below 0.9 M Na+, inverse dependence above 0.9 M Na+ and strong positive dependence on hydrogen ion concentration. Molecular modeling (AMBER) of C:G.C and C+:G.C base triplets with the third strand base bound in the Hoogsteen geometry shows that only the C+:G.C triplet is energetically feasible. van't Hoff analysis of the melting of the triplex and target duplex shows that between pH 5.0 and 8.5 in 0.15 M NaCl/0.005 M MgCl2 the enthalpy of melting (delta H degree obs) varies from 5.7 to 6.6 kcal.mol-1 for the duplex in a duplex mixture and from 7.3 to 9.7 kcal.mol-1 for third strand dissociation in the triplex mixture. We have extended the condensation-screening theory of Manning to pH-dependent third strand binding. In this development we explicitly include the H+ contribution to the electrostatic free energy and obtain [formula: see text]. The number of protons released in the dissociation of the third strand from the target duplex at pH 7.0, delta n2, is thereby calculated to be 5.5, in good agreement with approximately six third strand dc residues per mole of triplex. This work shows that when third strand binding requires protonated residues that would otherwise be neutral, triplex formation and dissociation are mediated by proton uptake and release, i.e., a proton switch. As a by-product of this study, we have found that at low pH the Watson-Crick duplex d(A-G)6.d(C-T)6 undergoes a transition to a parallel Hoogsteen duplex d(A-G)6.d(C(+)-T)6.     

Effect of 5-Methylcytosine on the Structure and Stability of DNA. Formation of Triple-Stranded Concatenamers by Overlapping Oligonucleotides

Abstract

A triple helix can be formed upon binding of a pyrimidine oligonucleotide to the major groove of a homopurine-homopyrimidine (R·Y) double-stranded DNA target site. Here, we report that this reaction can be influenced by base methylation. The pyrimidine strand 5′- TmCTmCTmCTmCTTmCT (mY₁₂), whose cytosine residues are methylated at C5, does not bind the duplex 5′-AGAGAGAGAAGA·3′-TCTCTCTCTTCT (R₁₂·Y₁₂) to yield a 12-triad triplex, as would be expected from these DNA sequences. Rather, a complex of overlapping oligonucleotides, which we define concatenamer, is formed. The concatenamer is clearly evidenced by Polyacrylamide gel electrophoresis (PAGE) since it migrates with a smeared band of very low mobility. The stoichiometry of the concatenamer, determined by both UV mixing curves and electrophoresis, is surprisingly found to be (R₁₂· 2mY₁₂)_n, thus showing that the unmethylated Y₁₂ strand is excluded from the complex. Denaturation experiments performed by ultraviolet absorbance (UV) and differential scanning calorimetry (DSC) show that the concatenamers melt with a single and highly cooperative transition whose Tm strongly depends on pH. Overall, the data point to the conclusion that the concatenamers are in triple helix, where the methylated mY₁₂ strand is engaged in both Watson-Crick and Hoogsteen base pairings, thus displacing the Y₁₂ strand from the R₁₂·Y₁₂ duplex. A possible mechanism of concatenamer formation is proposed. The results presented in this paper show that 5-methylcytosine brings about a strong stabilizing effect on both double and triple DNA helices, and that pyrimidine oligonucleotides containing 5-methylcytosine can displace from R·Y duplexes the analogous non-methylated strand. The advantage of using methylated oligonucleotides in antisense technology is discussed.     

Helix-coil transition of the self-complementary dG-dG-dA-dA-dT-dT-dC-dC duplex.

The helix-coil transition of the octanucleotide self-complementary duplex dG-dG-dA-dA-dT-dT-dC-dC has been monitored at the Watson-Crick protons, the base and sugar nonexchangeable protons and the backbone phosphates by high-resolution nuclear magnetic resonance (NMR) spectroscopy. The melting transition of the octanucleotide monitored by ultraviolet absorbance spectroscopy is characterized by the thermodynamic parameters delta H degree = -216.7 kJ/mol and delta S degree (25 degrees C) = -0.632 KJ mol-1 K-1 in 0.1 M NaCl, 10 mM phosphate solution. Correlation of the transition midpoint values monitored by the ultraviolet absorbance studies at strand concentrations below 0.2 mM and by NMR studies at 5.3 mM suggest that both methods are monitoring the octanucleotide duplex-to-strand transition. The NMR spectra of the Watson-Crick ring NH protons of the octanucleotide duplex have been followed as a function of temperature. The resonance from the terminal dG.dC base pairs broadens out at room temperature while the resonances from the other base pairs broaden simultaneously with the onset of the melting transition. The nonexchangeable base and sugar H-1' protons are resolved in the duplex and strand states and shift as average peaks through the melting transition. The experimental shifts on duplex formation have been compared with calculated values based on ring-current and atomic diamagnetic anisotropy contributions for a B-DNA base-pair-overlap geometry in solution. Several nonexchangeable proton resonances broaden in the fast-exchange region during the duplex-to-strand transition and the excess widths yield a duplex dissociation rate constant for the octanucleotide of 1.9 x 10(3) s-1 at 32 degrees C (fraction of duplex = 0.86) in 0.1 M NaCl, 10 mM phosphate buffer. The 31P resonances of the seven internucleotide phosphates are distributed over 0.6 ppm in the duplex state, shift downfield during the duplex-to-strand transition and undergo additional downfield shifts during the stacked-to-unstacked strand transition with increasing temperature.     

Homopurine and homopyrimidine strands complementary in parallel orientation form an antiparallel duplex at neutral pH with A-C,G-T,and T-C mismatched base pairs

DNA sequences d-TGAGGAAAGAAGGT (a 14-mer) and d-CTCCTTTCTTCC (a 12-mer) are complementary in parallel orientation forming either Donahue (reverse Watson-Crick) base pairing at neutral pH or Hoogsteen base pairing at slightly acidic pH. The structure of the complex formed by dissolving the two strands in equimolar ratio in water has been investigated by nmr. At neutral pH, the system forms an ordered antiparallel duplex with five A : T and four G : C Watson-Crick base pairs and three mismatches, namely G-T, A-C, and T-C. The nuclear Overhauser effect cross-peak pattern suggests an overall B-DNA conformation with major structural perturbations near the mismatches. The duplex has a low melting point and dissociates directly into single strands with a broad melting profile. The hydrogen-bonding schemes in the mismatched base pairs have been investigated. It has been shown earlier that in acidic pH, the system prefers a triple-stranded structure with two pyrimidine strands and one purine strand. One of the pyrimidine strands has protonated cytosines, forms Hoogsteen base pairing, and is aligned parallel to the purine strand; the other has nonprotonated cytosines and has base-pairing scheme similar to the one discussed in this paper. The parallel duplex is therefore less stable than either the antiparallel duplex or the triplex, in spite of its perfect complementarity. © 1997 John Wiley & Sons, Inc. Biopoly 41: 773–784, 1997     

Unwinding of unnatural substrates by a DNA helicase

Helicases separate double-stranded DNA into single-stranded DNA intermediates that are required during replication and recombination. These enzymes are believed to transduce free energy available from ATPase activity to unwind the duplex and translocate along the nucleic acid lattice. The nature of enzyme-substrate interactions between helicases and duplex DNA substrates has not been well-defined. Most helicases require a single-stranded DNA overhang adjacent to duplex DNA in order to initiate unwinding. The strand containing the overhang is referred to as the loading strand whereas the complementary strand is referred to as the displaced strand. We have investigated the interactions between a DNA helicase and the DNA substrate by replacing the displaced strand with a nucleic acid mimic, peptide nucleic acid (PNA). PNA is capable of forming duplex structures with DNA according to Watson-Crick base pairing rules, but contains a N-(2-aminoethyl)glycine backbone in place of the deoxyribose phosphates. The PNA-DNA hybrids had higher melting temperatures than their DNA-DNA counterparts. Dda helicase, from bacteriophage T4, was able to unwind the DNA-PNA substrates at similar rates as DNA-DNA substrates. The results indicate that the rate-limiting step for unwinding is relatively insensitive to the chemical nature of the displaced strand and the thermal stability of oligonucleotide substrates.     

Kinetic and thermodynamic characterization of DNA duplex–hairpin interconversion for two DNA decamers: d(CAACGGGTTG) and d(CAACCCGTTG)

The duplex–hairpin interconversion of two DNA decamers, d(CAACGGGTTG) and d(CAACCCGTTG), has been characterized thermodynamically and kinetically by using uv-melting and nmr relaxation methods. Separately, each decamer shows slow exchange between hairpin and duplex conformations. The hairpin conformations have melting points of 47 and 50°C, respectively, and exhibit similar thermodynamic stabilities. The enthalpies of duplex formation, measured by nmr, were found to be very similar (ΔH_DH = 26 ± 3 kcal/mole) for both decanters at low salt concentrations (< 50 mM NaCl). However, as the salt concentration was increased the behavior of ΔH_DH, and kinetics is significantly different for each decamer. The d(CAACGGGTTG) decamer forms a duplex containing two central G·G mismatches at high salt and DNA concentration. Based upon the measurement of high interconversion activation energies and a decrease in hairpin formation rate with increasing salt, the interconversion between hairpin and duplex was concluded to proceed by complete strand dissociation. In contrast, the d(CAAC-CCGTTG) decamer was determined to form a duplex with two centrally located C·C mismatches at pH values less than 6.2, consistent with the formation of a hemiprotonated C⁺·C mismatch. At pH values greater than 6.4, the hairpin–duplex equilibrium is almost completely shifted toward the hairpin conformation at DNA concentrations of 0.5–7.0 mM and salt concentrations of 10–100 mM. The interconversion of duplex and hairpin conformations was ascertained by means of both kinetic and thermodynamic measurements to proceed by a slightly different mechanism than its complementary decamer. Although the interconversion proceeds by complete strand separation as suggested by high duplex-hairpin interconversion activation enthalpies, the increasing hairpin formation rate with increasing ionic strength as well as the ΔH_DH, dependence on sail indicate that an intermediate internally bulged duplex (no C⁺·C formation) is stabilized by increasing ionic strength. These data support an interconversion mechanism where an intermediate internally bulged duplex may be the rate limiting step before strand separation. © 1995 John Wiley & Sons, Inc.     

RecA protein-promoted homologous pairing and strand exchange between intact and partially single-stranded duplex DNA.

In the pairing reaction between circular gapped and fully duplex DNA, RecA protein first polymerizes on the gapped DNA to form a nucleoprotein filament. Conditions that removed the formation of secondary structure in the gapped DNA, such as addition of Escherichia coli single-stranded DNA binding protein or preincubation in 1 mM-MgCl2, optimized the binding of RecA protein and increased the formation of joint molecules. The gapped duplex formed stable joints with fully duplex DNA that had a 5' or 3' terminus complementary to the single-stranded region of the gapped molecule. However, the joints formed had distinct properties and structures depending on whether the complementary terminus was at the 5' or 3' end. Pairing between gapped DNA and fully duplex linear DNA with a 3' complementary terminus resulted in strand displacement, symmetric strand exchange and formation of complete strand exchange products. By contrast, pairing between gapped and fully duplex DNA with a 5' complementary terminus produced a joint that was restricted to the gapped region; there was no strand displacement or symmetric strand exchange. The joint formed in the latter reaction was likely a three-stranded intermediate rather than a heteroduplex with the classical Watson-Crick structure. We conclude that, as in the three-strand reaction, the process of strand exchange in the four-strand reaction is polar and progresses in a 5' to 3' direction with respect to the initiating strand. The present study provides further evidence that in both three-strand and four-strand systems the pairing and strand exchange reactions share a common mechanism.     

Assembly and disassembly of RecA protein filaments occur at opposite filament ends. Relationship to DNA strand exchange

RecA protein primarily associates with and dissociates from opposite ends of nucleoprotein filaments formed on linear duplex DNA. RecA nucleoprotein filaments that are hydrolyzing ATP therefore engage in a dynamic process under some conditions that has some of the properties of treadmilling. We have also investigated whether the net polymerization of recA protein at one end of the filament and/or a net depolymerization at the other end drives unidirectional strand exchange. There is no demonstrable correlation between recA protein association/dissociation and the strand exchange reaction. RecA protein-mediated DNA strand exchange is affected minimally by changes in reaction conditions (dilution, pH shift, or addition of small amounts of adenosine-5'-O-(3-thiotriphosphate) that have large and demonstrable effects on recA protein association, dissociation, or both. Rather than driving strand exchange, these assembly and disassembly processes may simply represent the mechanism by which recA nucleoprotein filaments are recycled in the cell.     

Comparative Studies of the Thermodynamic Stabilities Between Sheared A:G and Watson-Crick A:U(T) Base Pairs in RNA and DNA

Abstract

Thermodynamic parameters for duplex formation were determined from CD melting curves for r(GGACGAGUCC)₂ and d(GGACGAGTCC)₂, both of which form two consecutive ‘sheared’ A:G base pairs at the center [Katahira et al. (1993) Nucleic Acids Res. 21, 5418–5424; Katahira et al., (1994) Nucleic Acids Res. 22, 2752–27591. The parameters were determined also for r(GGACUAGUCC)₂ and d(GGACTAGTCC)₂, where the A:G mismatches are replaced by Watson-Crick A:U(T) base pairs. Thermodynamic properties for duplex formation are compared between the sheared and the Watson-Crick base pairs, and between RNA and DNA. Difference in the thermodynamic stability is analyzed and discussed in terms of enthalpy and entropy changes. The characteristic features in CD spectra of RNA and DNA containing the sheared A:G base pairs are also reported.

     

Structural Properties of Hybrid Triplex of Polycation Deoxyribonucleic S-methylthiourea (DNmt) Strands with a Complementary DNA Strand,Probed by Nanosecond Molecular Dynamics

Abstract

The replacement of phosphodiester linkages of the polyanion DNA with S-methylthiourea linkers provides the polycation deoxyribonucleic S-methylthiourea (DNmt). Molecular dynamics studies to 1,220 ps of the hybrid triplex formed from octameric DNmt strands d(Tmt)₈ with a complementary DNA oligomer strand d(Ap)₈ have been carried out with explicit water solvent and Na counterions under periodic boundary conditions using the CHARMM force field and the Ewald summation method. The Watson-Crick and Hoogsteen hydrogen-bonding patterns of the A/T tracts remained intact without any structural restraints for triplex structures throughout the simulation. The duplex portion of the triplex structure equilibrated at a B-DNA conformation in terms of the helical rise and other helical parameters. The dynamic structures of the DNmt·DNA·DNmt triplex were determined by examining histograms from the last 800 ps of the dynamics run. These included the hydrogen-bonding pattern (sequence recognition), three-centered bifurcating occurrences, minor groove width variations, and bending of tracts for the hybrid triplex structures. Together with the Watson-Crick hydrogen-bondings, the strong Hoogsteen hydrogen-bondings, the partially maintained three-centered bifurcatings in the Watson-Crick pair, and the medium-strength three-centered bifurcatings in the Hoogsteen pair suggest that the hybrid triplex is energetically favorable as compared to a duplex with similar base stacking, van der Waals interactions, and helical parameters. This is in agreement with our previously reported thermody- namic study, in which only triplex structures were observed in solution. The bending angle measured between the local axis vectors of the first and last helical axis segments is about 20° for the Watson-Crick portion of the averaged structure. Propeller twist (associated with three-centered hydrogen-bonding) up to ?30°, native to DNA AT base pairing, was also observed for the triplex structure. The sugar pseudorotation phase angles and the ring rotation angles for the DNA strand are within the C3′-endo domain and C2′-endo domain for the DNmt strand. Water spines are observed in both minor and major grooves throughout the dynamics run. The molecular dynamics simulations of the structural properties of DNmt·DNA·DNmt hybrid triplex is compared to the DNG·DNA·DNG hybrid triplex (In DNG the -O-(PO₂-)-O- linkers in DNA is replaced by -NH-C(=N₂)-NH-).     

Formation of joint DNA molecules by two eukaryotic strand exchange proteins does not require melting of a DNA duplex

We have examined whether DNA strand exchange activities from nuclear extracts of HeLa cells or Drosophila melanogaster embryos have detectable helicase or melting activities. The partially purified recombinases have been shown to recognize homologous single strand and double strand DNA molecules and form joint molecules in a DNA strand exchange reaction. The joint molecule product consists of a linear duplex joined at one end by a region of DNA heteroduplex to a homologous single strand circular DNA. Using two different partially duplex helicase substrates, we are unable to detect any melting of duplex regions under conditions that promote joint molecule formation. One substrate consists of a 32P-labeled oligonucleotide 20 or 30 bases long annealed to M13mp18 circular single strand DNA. The second substrate consists of a linear single strand region flanked at each end by short duplex regions. We observe that even in the presence of excess recombinase protein or after prolonged incubation no helicase activity is apparent. Control experiments rule out the possibility that a helicase is masked by reannealing of displaced single strand fragments. Based on these findings and other data, we conclude that the human and D. melanogaster recombinases recognize and pair homologous sequences without significant melting of duplex DNA prior to strand exchange.     

Preparation and melting of single strand circular DNA loops.

A method for preparation of single strand DNA circles of almost arbitrary sequence is described. By ligating two sticky ended hairpins together a linear duplex is formed, closed at both ends by single stranded loops. The melting characteristics of such loops are investigated using optical absorbance and NMR. It is shown by comparison with the corresponding linear sequence (closed circle minus the end loops) that the effects of end fraying and the strand concentration dependence of the melting temperature are eliminated in the circular form. Over the concentration range examined (0.5 to 2.0 micromolar strands), the circular DNA has a monophasic melting curve, while the linear duplex is biphasic, probably due to hairpin formation. Since effects of duplex to single strands dissociation do not contribute to melting of the circular molecules (dumbells), these DNAs present a realistic experimental model for examining local thermal stability in DNA.     

pH and cation effects on the properties of parallel pyrimidine motif DNA triplexes

The effects of cytosine protonation and various cations on the properties of parallel pyrimidine motif DNA triplexes were intensively investigated and characterized by several different techniques, such as circular dichroism (CD) conformation, ultraviolet (UV) melting, differential scanning calorimetry (DSC) thermal denaturation, and surface plasmon resonance (SPR) real-time dynamics. The comparative CD spectra of the triplex and the corresponding homoduplexes showed that the negative peak at approximately 218 nm would be the eigenpeak of the Hoogsteen paired strand, and moreover, the formation pathway of a triplex was significantly pH-dependent and fell into three groups: under acidic conditions, the triplex is formed by a one-step docking, under near physiological conditions, the Watson-Crick duplex is first structured and then accepts the Hoogsteen third strand into its major groove, and under basic conditions, the triplex is not formed. The pH-dependent thermodynamics of the global triplex, the Watson-Crick antiparallel duplex, and the Crick-Hoogsteen parallel duplex were comparatively discussed for the first time. These data revealed that the thermodynamic stabilities of the Watson-Crick-Hoogsteen triplex and the Crick-Hoogsteen duplex would be strongly dependent on cytosine protonation, but a low-pH environment somewhat destabilized the Watson-Crick duplex. The binding energy of triplex formation would be different from the unfolding energy of triplex melting under acidic conditions due to the disparity in the pathway between the formation and unfolding of a triplex. Real-time dynamic measurements showed that the association and dissociation rate constants of a duplex-to-triplex formation are (1.98 +/- 0.24) x 10(3) M(-1) s(-1) and (4.09 +/- 0.96) x 10(-4) s(-1) at 20 degrees C and pH 6.0, respectively. The formation energy of the duplex-to-triplex transition derived from SPR measurements was in agreement with the unfolding energy of the free Hoogsteen paired duplex derived from UV measurements. The calorimetric enthalpies of the triplex-to-duplex-to-single transition were 39.3 and 75.3 kcal/mol under near physiological conditions (pH 7.0), respectively, which were underestimated relative to the van't Hoff enthalpies. In addition, the effects of various cations, ionic strength, mixed-valent cations, and the position of the C(+)xG.C triplets on the thermodynamics of the triplexes were addressed under near physiological conditions. The interaction of metal ions with the triplexes clearly depended on the type and ionic strength of the cations, and the efficiency with which the cations stabilized the global triplex was in the order Mg(2+) > Mn(2+) > Ca(2+) > Ba(2+) > Na(+). These observations would be useful for the design of triplex-forming oligonucleotides for antigene drugs and therapeutic purposes.     

Force-induced melting of DNA—evidence for peeling and internal melting from force spectra on short synthetic duplex sequences

Overstretching of DNA occurs at about 60–70 pN when a torsionally unconstrained double-stranded DNA molecule is stretched by its ends. During the transition, the contour length increases by up to 70% without complete strand dissociation. Three mechanisms are thought to be involved: force-induced melting into single-stranded DNA where either one or both strands carry the tension, or a B-to-S transition into a longer, still base-paired conformation. We stretch sequence-designed oligonucleotides in an effort to isolate the three processes, focusing on force-induced melting. By introducing site-specific inter-strand cross-links in one or both ends of a 64 bp AT-rich duplex we could repeatedly follow the two melting processes at 5 mM and 1 M monovalent salt. We find that when one end is sealed the AT-rich sequence undergoes peeling exhibiting hysteresis at low and high salt. When both ends are sealed the AT sequence instead undergoes internal melting. Thirdly, the peeling melting is studied in a composite oligonucleotide where the same AT-rich sequence is concatenated to a GC-rich sequence known to undergo a B-to-S transition rather than melting. The construct then first melts in the AT-rich part followed at higher forces by a B-to-S transition in the GC-part, indicating that DNA overstretching modes are additive.     

Tetraplex Formation of d(GGGGGTTTTT): 1H NMR Study in Solution

Abstract

The oligonucleotide d(G₅T₅) can in principle form a fully matched duplex with G · T pairing and/or a tetraplex. Non-denaturing gel electrophoresis, circular dichroism and NMR experiments show that the tetraplex is exclusively formed by this oligomer in solution. In the presence of its complementary strand d(A₅C₅) at low temperature, d(G₅T₅) forms the tetraplex over the normally expected Watson-Crick duplex. However, when d(G₅T₅) and d(A₅C₅) are mixed together in equimolar amounts and heated for several minutes at 85°C, and then allowed to cool, the product was essentially the Watson-Crick duplex. The lack of resolution in the 500 MHz ¹H NMR spectra and the presence of extensive spin diffusion do not allow us to derive a quantitative structure for the tetraplex from the NMR data. However, we find good qualitative agreement between the NOESY and MINSY data and a theoretically derived stereochemically sound structure in which the G's and T's are part of a parallel tetraplex.     

Activation of DNA strand exchange by cationic comb-type copolymers: effect of cationic moieties of the copolymers

We have previously reported that poly(l-lysine)-graft-dextran cationic comb-type copolymers accelerate strand exchange reaction between duplex DNA and its complementary single strand by >4 orders of magnitude, while stabilizing duplex. However, the stabilization of the duplex is considered principally unfavourable for the accelerating activity since the strand exchange reaction requires, at least, partial melting of the initial duplex. Here we report the effects of different cationic moieties of cationic comb-type copolymers on the accelerating activity. The copolymer having guanidino groups exhibited markedly higher accelerating effect on strand exchange reactions than that having primary amino groups. The high accelerating effect of the former is considered to be due to its lower stabilizing effect on duplex DNA, resulting from its increased affinity to single-stranded DNA. The difference in affinity was clearly demonstrated by a fluorescence correlation spectroscopy study; the interaction of the former with single-stranded DNA still remained high even at 1 M NaCl, while that of the latter completely disappeared. These results suggest that some modes of interactions, such as hydrogen bonding, other than electrostatic interactions between the copolymers having guanidino groups and DNAs may be involved in strand exchange activation.     

The formation of adjacent triplex-duplex domainsin DNA.

The ability of single-stranded DNA oligomers to form adjacent triplex and duplex domains with two DNA structural motifs was examined. Helix-coil transition curves and a gel mobility shift assay were used to characterize the interaction of single-stranded oligomers 12-20 nt in length with a DNA hairpin and with a DNA duplex that has a dangling end. The 12 nt on the 5'-ends of the oligomers could form a triplex structure with the 12 bp stem of the hairpin or the duplex portion of the DNA with a dangling end. The 3'-ends of the 17-20 nt strands could form Watson-Crick pairs to the five base loop of the hairpin or the dangling end of the duplex. Complexes of the hairpin DNA with the single-stranded oligomers showed two step transitions consistent with unwinding of the triplex strand followed by hairpin denaturation. Melting curve and gel competition results indicated that the complex of the hairpin and the 12 nt oligomer was more stable than the complexes involving the extended single strands. In contrast, results indicated that the extended single-stranded oligomers formed Watson-Crick base pairs with the dangling end of the duplex DNA and enhanced the stability of the adjacent triplex region.