Reverse Watson-Crick Base Pairs Research Articles

Double-Headed 2'-Deoxynucleotides That Hybridize to DNA and RNA Targets via Normal and Reverse Watson-Crick Base Pairs.

Through the use of modified nucleotides, synthetic nucleic acids have found several fields of application within biotechnology and in the pharmaceutical industry. We have previously introduced nucleotides with an additional functional nucleobase linked to C2' of arabinonucleotides (BX). These double-headed nucleotides fit neatly into DNA·DNA duplexes, where they can replace the corresponding natural dinucleotides and thus condense the molecular information. Here, we introduce a 2'-deoxy version of the BX design with inversion of the C2' stereochemistry (dSBX) with the aim of obtaining improved RNA recognition. Specifically, dSBX analogues with cytosine or isocytosine attached to C2' of 2'-deoxyuridine (dSUC and dSUiC) were synthesized and evaluated in duplexes. Whereas the dSBX design did not outperform the BX design in terms of mimicking dinucleotides in nucleic acid duplexes, it was able to engage in reverse Watson-Crick pairing using its 2'-base. This was evident from the ability of the dSUC cytosine to form stable mis-matching base pairs with opposite cytosines identified as hemiprotonated C·C+ pairs. Furthermore, specific base-pairing with guanine was only observed for the isocytosine-bearing dSUiC monomer. Very stable duplexes were obtained with dSUC/iC monomers in each strand indicating that fully modified double-headed nucleic acid sequences could be based on the dSBX design.

Structural and Energetic Impact of Non-natural 7-Deaza-8-azaguanine, 7-Deaza-8-azaisoguanine, and Their 7-Substituted Derivatives on Hydrogen-Bond Pairing with Cytosine and Isocytosine.

The impact of 7-deaza-8-azaguanine (DAG) and 7-deaza-8-azaisoguanine (DAiG) modifications on the geometry and stability of the G:C Watson-Crick (cWW) base pair and the G:iC and iG:C reverse Watson-Crick (tWW) base pairs has been characterized theoretically. In addition, the effect on the same base pairs of seven C7-substituted DAG and DAiG derivatives, some of which have been previously experimentally characterized, has been investigated. Calculations indicate that all of these modifications have a negligible impact on the geometry of the above base pairs, and that modification of the heterocycle skeleton has a small impact on the base-pair interaction energies. Instead, base-pair interaction energies are dependent on the nature of the C7 substituent. For the 7-substituted DAG-C cWW systems, a linear correlation between the base-pair interaction energy and the Hammett constant of the 7-substituent is found, with higher interaction energies corresponding to more electron-withdrawing substituents. Therefore, the explored modifications are expected to be accommodated in both parallel and antiparallel nucleic acid duplexes without perturbing their geometry, while the strength of a base pair (and duplex) featuring a DAG modification can, in principle, be tuned by incorporating different substituents at the C7 position.

Differentiating Parallel and Antiparallel DNA Duplexes in the Gas Phase Using Trapped Ion Mobility Spectrometry.

Deoxyribonucleic acids can form a wide variety of structural motifs which differ greatly from the typical antiparallel duplex stabilized by Watson-Crick base pairing. Many of these structures are thought to occur in vivo and may have essential roles in the biology of the cell. Among these is the parallel-stranded duplex-a structural motif in which DNA strands associate in a head-to-head fashion with the 5' ends at the same end of the duplex-which is stabilized by reverse Watson-Crick base pairing. In this study, parallel- and antiparallel-stranded DNA duplexes formed from two different 12-mer oligonucleotides were studied using native electrospray ionization combined with trapped ion mobility spectrometry and mass spectrometry. The DNA duplex charge plays an important role in the gas-phase mobility profile, with a more compact form in negative mode than in positive mode (ΔΩ ≈ 100 Å2 between -4 and +4). Despite sequence mismatches, homo- and hetero-DNA duplexes were formed in solution and transfer to the gas phase, where a more compact structure was observed for the parallel compared to the antiparallel duplexes (ΔΩ ≈ 50 Å2), in good agreement with theoretical calculations. Theoretical studies suggest that a reduction (or compaction) along the helical axis of the parallel and antiparallel DNA duplexes is observed upon transfer to the gas phase.

Structural properties and gene-silencing activity of chemically modified DNA-RNA hybrids with parallel orientation.

We report, herein, a new class of RNAi trigger molecules based on the unconventional parallel hybridization of two oligonucleotide chains. We have prepared and studied several parallel stranded (ps) duplexes, in which the parallel orientation is achieved through incorporation of isoguanine and isocytosine to form reverse Watson-Crick base pairs in ps-DNA:DNA, ps-DNA:RNA, ps-(DNA-2′F-ANA):RNA, and ps-DNA:2′F-RNA duplexes. The formation of these duplexes was confirmed by UV melting experiments, FRET and CD studies. In addition, NMR structural studies were conducted on a ps-DNA:RNA hybrid for the first time. Finally, we provide evidence for the unprecedented finding that ps-DNA:RNA and ps-DNA:2′F-RNA hybrids can engage the RNAi pathway to silence gene expression in vitro.

Chirality Dependent Potency Enhancement and Structural Impact of Glycol Nucleic Acid Modification on siRNA.

Here we report the investigation of glycol nucleic acid (GNA), an acyclic nucleic acid analogue, as a modification of siRNA duplexes. We evaluated the impact of (S)- or (R)-GNA nucleotide incorporation on RNA duplex structure by determining three individual crystal structures. These structures indicate that the (S)-nucleotide backbone adopts a conformation that has little impact on the overall duplex structure, while the (R)-nucleotide disrupts the phosphate backbone and hydrogen bonding of an adjacent base pair. In addition, the GNA-T nucleobase adopts a rotated conformation in which the 5-methyl group points into the minor groove, rather than the major groove as in a normal Watson-Crick base pair. This observation of reverse Watson-Crick base pairing is further supported by thermal melting analysis of GNA-C and GNA-G containing duplexes where it was demonstrated that a higher thermal stability was associated with isoguanine and isocytosine base pairing, respectively, over the canonical nucleobases. Furthermore, it was also shown that GNA nucleotide or dinucleotide incorporation increases resistance against snake venom phosphodiesterase. Consistent with the structural data, modification of an siRNA with (S)-GNA resulted in greater in vitro potencies over identical sequences containing (R)-GNA. A walk of (S)-GNA along the guide and passenger strands of a GalNAc conjugate duplex targeting mouse transthyretin (TTR) indicated that GNA is well tolerated in the seed region of both strands in vitro, resulting in an approximate 2-fold improvement in potency. Finally, these conjugate duplexes modified with GNA were capable of maintaining in vivo potency when subcutaneously injected into mice.

The effect of the glycosylation position on the base pairing and supramolecular structure of the 5′-deoxyribosyl Janus-type AT nucleosides

The intrinsic structural diversity of the nucleosides is one of the essential properties for their wide participation in myriads of chemical or biochemical processes. Two unique regio-isomeric Janus-type AT nucleosides with the 5′-deoxyribose attached on N1 or N3 position has been synthesized through Vorbrueggen or transglycosylation reactions. These two isomers display different supramolecular morphologies in solution state from their N8 glycosylated counterpart. The underneath structural details of the N3 glycosylated isomer were revealed by the single-crystal X-ray analysis. In addition to a novel base pair pattern was identified which is entirely different from the reverse Watson-Crick base pair adopted by its N8 isomer, an interesting water-filled columnar nanotuble-like structure was also found in its solid state. This study not only enriches the structural varieties of AT Janus-type nucleosides, but also provides specific information concerning the effect of the sugar glycosylation position on the properties of these new type of pyrimido[4,5-d]pyrimidine nucleosides.

Pyrrolo-dC Metal-Mediated Base Pairs in the Reverse Watson-Crick Double Helix: Enhanced Stability of Parallel DNA and Impact of 6-Pyridinyl Residues on Fluorescence and Silver-Ion Binding.

Reverse Watson-Crick DNA with parallel-strand orientation (ps DNA) has been constructed. Pyrrolo-dC (PyrdC) nucleosides with phenyl and pyridinyl residues linked to the 6 position of the pyrrolo[2,3-d]pyrimidine base have been incorporated in 12- and 25-mer oligonucleotide duplexes and utilized as silver-ion binding sites. Thermal-stability studies on the parallel DNA strands demonstrated extremely strong silver-ion binding and strongly enhanced duplex stability. Stoichiometric UV and fluorescence titration experiments verified that a single (2py) PyrdC-(2py) PyrdC pair captures two silver ions in ps DNA. A structure for the PyrdC silver-ion base pair that aligns 7-deazapurine bases head-to-tail instead of head-to-head, as suggested for canonical DNA, is proposed. The silver DNA double helix represents the first example of a ps DNA structure built up of bidentate and tridentate reverse Watson-Crick base pairs stabilized by a dinuclear silver-mediated PyrdC pair.

Higher order structural effects stabilizing the reverse Watson–Crick Guanine-Cytosine base pair in functional RNAs

The G:C reverse Watson–Crick (W:W trans) base pair, also known as Levitt base pair in the context of tRNAs, is a structurally and functionally important base pair that contributes to tertiary interactions joining distant domains in functional RNA molecules and also participates in metabolite binding in riboswitches. We previously indicated that the isolated G:C W:W trans base pair is a rather unstable geometry, and that dicationic metal binding to the Guanine base or posttranscriptional modification of the Guanine can increase its stability. Herein, we extend our survey and report on other H-bonding interactions that can increase the stability of this base pair. To this aim, we performed a bioinformatics search of the PDB to locate all the occurencies of G:C trans base pairs. Interestingly, 66% of the G:C trans base pairs in the PDB are engaged in additional H-bonding interactions with other bases, the RNA backbone or structured water molecules. High level quantum mechanical calculations on a data set of representative crystal structures were performed to shed light on the structural stability and energetics of the various crystallographic motifs. This analysis was extended to the binding of the preQ1 metabolite to a preQ1-II riboswitch.

Janus-type AT nucleosides: synthesis, solid and solution state structures

Novel Janus-type nucleoside analogues (1a-d) were synthesized. Their pyrimido[4,5-d]pyrimidine base moiety has one face with a bidentate Watson-Crick donor-acceptor (DA) H-bond array of adenine and the other face with an acceptor-donor (AD) H-bond array of thymine. These nucleosides may self-associate through the self-complementary base pair. Indeed, in the solid state, compound 6d displayed a honeycomb-like supramolecular structure with tetrameric membered cavities formed through the combination of reverse Watson-Crick base pairs and aromatic stacking, in which the solvent molecules were accommodated. The result of temperature-dependent CD studies showed that the free nucleosides can form higher order chiral structures in aqueous solution.

Magnesium binding sites of the active conformation pf Hammerheadribozyme

The modeling of the active conformation was done by using modeling program InsightII and Discover from the previous NMR, chemical modification and mutation data. This model structure has the reverse Watson-Crick GC base pair between C17 at the cleavage site and G5 at the core region. Two magnesium ions bind to this ribozyme. One binds to the pro-Rp oxygen of the P9 phosphate and the N7 nitrogen of G10.1, similarly to the crystal structure, the other to N3 of C3, the 2'O of C17 and the Sp-O of the scissile phosphate, while the Rp-O of that binds to NH2 of C3.

NMR structure of a parallel-stranded DNA duplex at atomic resolution.

DNA dodecamers have been designed with two cytosines on each end and intervening A and T stretches, such that the oligomers have fully complementary A:T base pairs when aligned in the parallel orientation. Spectroscopic (UV, CD and IR), NMR and molecular dynamics studies have shown that oligomers having the sequences d(CCATAATTTACC) and d(CCTATTAAATCC) form a parallel-stranded duplex when dissolved at 1:1 stoichiometry in aqueous solution. This is due to the C:C+ clamps on either end and extensive mismatches in the antiparallel orientation. The structure is stable at neutral and acidic pH. At higher temperatures, the duplex melts into single strands in a highly cooperative fashion. All adenine, cytosine and thymine nucleotides adopt the anti conformation with respect to the glycosidic bond. The A:T base pairs form reverse Watson-Crick base pairs. The duplex shows base stacking and NOEs between the base protons T(H6)/A(H8) and the sugar protons (H1'/H2'/H2") of the preceding nucleotide, as has been observed in antiparallel duplexes. However, no NOEs are observed between base protons H2/H6/H8 of sequential nucleotides, though such NOEs are observed between T(CH3) and A(H8). A three-dimensional structure of the parallel-stranded duplex at atomic resolution has been obtained using molecular dynamics simulations under NMR constraints. The simulated structures have torsional angles very similar to those found in B-DNA duplexes, but the base stacking and helicoid parameters are significantly different.

The structures and relative stabilities of d(G · G) reverse hoogsteen, d(G·T) reverse wobble, and d(G · C) reverse watson-crick base-pairs in DNA crystals

We have solved the structures of the homoduplex d(Gm5CGCGCG)2, and the heteroduplexes d(GCGCGCG)/d(TCGCGCG) and d(GCGCGCG)/d(CCGCGCG). The structures form six base-pairs of identical Z-DNA duplexes with single nucleotides overhanging at the 5′-ends. The overhanging nucleotide from one strand remains stacked and sandwiched between the blunt-ends of two adjacent Z-DNA duplexes, while the overhanging base of the opposing strand is extra-helical. The stacked and the extra-helical bases from adjacent duplexes pair to form a distorted d(G · G) reverse Hoogsteen base-pair in the d(Gm5CGCGCG)2 homoduplex, and d(G · T) reverse wobble and d(G · C) reverse Watson-Crick base-pairs in the d(GCGCGCG)/d(TCGCGCG) and d(GCGCGCG)/ d(CCGCGCG) heteroduplexes, respectively. Interestingly, only the d(G,T) and d(G · C) base-pairs were observed in the heteroduplexes, suggesting that both the d(G · T) reverse wobble and d(G · C) reverse Watson-Crick base-pairs are more stable in this crystal environment than the d(G · G) reverse Hoogsteen base-pair. To estimate the relative stability of the three types of reverse base-pairs, crystals were grown using various mixtures of sequences and their strand compositions analyzed by mass spectrometry. The d(G · C) reverse Watson-Crick base-pair was estimated to be more stable by ∼1.5 kcal/mol and the d(G · T) reverse wobble base-pair more stable by ∼0.5 kcal/mol than the d(G · G) reverse Hoogsteen base-pair. The step during crystallization responsible for discriminating between the strands in the crystal is highly cooperative, suggesting that it occurs during the initial nucleating event of crystal growth.

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 Donohue (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.

Solution structure of the parallel-stranded hairpin d(T8C4A8) as determined by two-dimensional NMR.

The structure of the oligodeoxynucleotide (3')T8(5')-(5')C4A8(3') hairpin in aqueous solution was studied by two-dimensional (2D) proton and phosphorus nuclear magnetic resonance (NMR) spectroscopy. At 2.5 mM and 10 degrees C, the molecule exists predominantly as a monomolecular hairpin with a C4 loop. At higher concentrations and lower temperatures, NMR signals from multimers are obvious. They account for approximately 25% of the total population at 4 mM and 10 degrees C. Nearly all of the proton NMR signals for the hairpin could be assigned using 2D COSY, HOHAHA, and NOESY experiments. 2D 1H-31P correlation experiments were used to assign all the phosphorus resonances and to provide an additional check for the sequential assignments. A parallel-stranded T8.A8 stem can be formed in the hairpin due to the presence of the unusual 5'-5' linkage in the loop. 2D NOESY experiments indicate that the A H2 and its 5'-end neighbor base pair T methyl protons are within 5 A of each other. This is in accord with reverse Watson-Crick base pairing between T and A, which locates the A H2 and the T methyl protons in the same groove of the duplex. The chemical shifts of A H1', H2', and H2" sugar and the H2 base protons are quite different compared to normal B-DNA. Analysis of the 2D COSY and NOESY cross peak patterns indicates that the deoxyribose rings are mainly in the C2'-endo conformation and that the stem forms a right-handed helix, with the two strands held together by eight reverse Watson-Crick A.T base pairs to form a parallel-stranded duplex. The backbone torsion angles, as determined from the 31P chemical shifts, are slightly different for the A and the T residues. A molecular model was constructed, using a total of 336 proton NOE cross peak intensities as proton-proton distance constraints. In the refined structure, the conformations of the sugar-phosphate linkage, the deoxyribose rings, and the glycosyl bonds for the two parallel strands of the hairpin are close to a regular B-DNA structure. The base-stacking and the hydrogen-bonding interactions are well optimized; however, the two grooves are of approximately equal width. Thus, compared to B-DNA, the parallel-stranded duplex has a very different surface shape, and because of the reverse Watson-Crick base pairing, it has different groups exposed in each groove.

The hydrogen-bonding structure in parallel-stranded duplex DNA is reverse Watson-Crick

Raman spectra of the parallel-stranded duplex formed from the deoxyoligonucleotides 5'-d-[(A)10TAATTTTAAATATTT]-3' (D1) and 5'-d[(T)10ATTAAAATTTATAAA]-3' (D2) in H2O and D2O have been acquired. The spectra of the parallel-stranded DNA are then compared to the spectra of the antiparallel double helix formed from the deoxyoligonucleotides D1 and 5'-d(AAATATTTAAAATTA-(T)10]-3' (D3). The Raman spectra of the antiparallel-stranded (aps) duplex are reminiscent of the spectra of poly[d(A)].poly[d(T)] and a B-form structure similar to that adopted by the homopolymer duplex is assigned to the antiparallel double helix. The spectra of the parallel-stranded (ps) and antiparallel-stranded duplexes differ significantly due to changes in helical organization, i.e., base pairing, base stacking, and backbone conformation. Large changes observed in the carbonyl stretching region (1600-1700 cm-1) implicate the involvement of the C(2) carbonyl of thymine in base pairing. The interaction of adenine with the C(2) carbonyl of thymine is consistent wtih formation of reverse Watson-Crick base pairing in parallel-stranded DNA. Phosphate-furanose vibrations similar to those observed for B-form DNA of heterogenous sequence and high A,T content are observed at 843 and 1092 cm-1 in the spectra of the parallel-stranded duplex. The 843-cm-1 band is due to the presence of a sizable population of furanose rings in the C2'-endo conformation. Significant changes observed in the regions from 1150 to 1250 cm-1 and from 1340 to 1400 cm-1 in the spectra of the parallel-stranded duplex are attributed to variations in backbone torsional and glycosidic angles and base stacking.

Helix-coil transition of parallel-stranded DNA. Thermodynamics of hairpin and linear duplex oligonucleotides.

The stabilities have been determined of different DNA double helices constructed with the two constituent strands in a parallel orientation. These molecules incorporate polarity-inverting loop structures (hairpins) or nucleotide sequences (duplexes) which impose the desired polarity on the two strands constituting the sugar-phosphate backbone. The hairpins consisted of d(A.T)n stems (n = 8 or 10) and either a 5'-p-5' linkage in a d(C)4 loop (ps-C8 and ps-C10) or a 3'-p-3' linkage in a d(G)4 loop (ps-G10). The linear duplexes had 21-nt (ps-C2.C3) and 25-nt (ps-D1.D2, ps-D3.D4) mixed A,T sequences and normal chemical linkages throughout. Reference molecules with normal antiparallel helical orientations (hairpins aps-C8, aps-C10, and aps-G10 and duplexes aps-C3.C7, aps-D1.D3, and aps-D2.D4) were also synthesized and studied. Hydrogen bonding in ps-DNA is via reverse Watson-Crick base pairs, and the various constructs display spectroscopic, chemical, biochemical, and electrophoretic properties distinct from those of their aps counterparts. For example, both the ps and aps molecules show a pronounced UV absorption hyperchromicity upon melting, but the spectral distribution is not the same. Thus, the difference spectra (ps-aps) in the native state are characterized by a positive peak at 252 nm, an isosbestic point at 267 nm, and a negative peak at 282 nm. Temperature-dependent absorbances were recorded at selected wavelengths and in the form of complete spectra to derive the thermodynamic parameters for the helix-coil transitions.(ABSTRACT TRUNCATED AT 250 WORDS)

Parallel stranded DNA.

A series of four hairpin deoxyoligonucleotides was synthesized with a four-nucleotide central loop (either C or G) flanked by the complementary sequences d(T)10 and d(A)10. Two of the molecules contain either a 3'-p-3' or 5'-p-5' linkage in the loop, so that the strands in the stem have the same, that is, parallel (ps) polarity. The pair of reference oligonucleotides have normal phosphodiester linkages throughout and antiparallel (aps) stem regions. All the molecules adopt a duplex helical structure in that (i) the electrophoretic mobilities in polyacrylamide gels of the ps and aps oligomers are similar. (ii) The ps hairpins are substrates for T4 polynucleotide kinase, T4 DNA ligase, and Escherichia coli exonuclease III. (iii) Salt-dependent thermal transitions are observed for all hairpins, but the ps molecules denature 10 degrees C lower than the corresponding aps oligomers. (iv) The ultraviolet absorption and circular dichroism spectra are indicative of a base-paired duplex in the stems of the ps hairpins but differ systematically from those of the aps counterparts. (v) The bis-benzimidazole drug Hoechst-33258, which binds in the minor groove of B-DNA, exhibits very little fluorescence in the presence of the ps hairpins but a normal, enhanced emission with the aps oligonucleotides. In contrast, the intercalator ethidium bromide forms a strongly fluorescent complex with all hairpins, the intensity of which is even higher for the ps species. (vi) The pattern of chemical methylation is the same for both the ps and aps hairpins. The combined results are consistent with the prediction from force field analysis of a parallel stranded right-handed helical form of d(A)n.d(T)n with a secondary structure involving reverse Watson-Crick base pairs and a stability not significantly different from that of the B-DNA double helix. Models of the various hairpins optimized with force field calculations are described.