An intercalation-locked parallel-stranded DNA tetraplex

DNA has proved to be an excellent material for nanoscale construction because complementary DNA duplexes are programmable and structurally predictable. However, in the absence of Watson–Crick pairings, DNA can be structurally more diverse. Here, we describe the crystal structures of d(ACTCGGATGAT) and the brominated derivative, d(AC^BrUCGGA^BrUGAT). These oligonucleotides form parallel-stranded duplexes with a crystallographically equivalent strand, resulting in the first examples of DNA crystal structures that contains four different symmetric homo base pairs. Two of the parallel-stranded duplexes are coaxially stacked in opposite directions and locked together to form a tetraplex through intercalation of the 5′-most A–A base pairs between adjacent G–G pairs in the partner duplex. The intercalation region is a new type of DNA tertiary structural motif with similarities to the i-motif. ¹H–¹H nuclear magnetic resonance and native gel electrophoresis confirmed the formation of a parallel-stranded duplex in solution. Finally, we modified specific nucleotide positions and added d(GAY) motifs to oligonucleotides and were readily able to obtain similar crystals. This suggests that this parallel-stranded DNA structure may be useful in the rational design of DNA crystals and nanostructures.     

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.     

Parallel-stranded linear homoduplexes of d(A+-G)n > 10 and d(A-G)n > 10 manifesting the contrasting ionic strength sensitivities of poly(A+.A+) and DNA.

In contrast to shorter homologs which only form a single-stranded nucleic acid alpha-helix in acid solution at [Na+]</=0.02 M Na+, d(A-G)20,30 form in addition a parallel-stranded duplex with (A+.A+) and (G.G) base pairs and interstrand dA+...PO2-ionic and dA+NH2... O=P H-bonds. Under conditions where duplex prevails over alpha-helix, the contribution of the base-backbone interactions to stability varies directly with [H+] and inversely with [Na+], just as in poly(A+.A+). These duplexes are characterized by intense circular dichroism and a large cooperative thermally-induced hyperchromic transition that is dependent on oligomer concentration. Dimethylsulfate reactivity of the dG residues indicates G.G and therefore dA+.dA+rather than dA+.G base pairs. At much higher ionic strength (Na+>/=0.2 M) the protonated base-backbone interactions are so weakened that duplex stability becomes increasingly dependent upon H-bonded base pairing and stacking and almost independent of pH. Between pH 6 and 8 this duplex structure is devoid of protonated dA residues and shows positive dependence of T m on ionic strength similar to that of DNA.     

Solution-state structure of a fully alternately 2��-F/2��-OMe modified 42-nt dimeric siRNA construct

A high-resolution solution structure of a stable 42-nt RNA dimeric construct has been derived based on a high number of NMR observables including nuclear overhauser effects (NOEs), J-coupling constants and residual dipolar couplings (RDCs), which were all obtained with isotopically unlabeled molecules. Two 21-nt siRNA that efficiently hybridize consist of ribose units that were alternately substituted by 2′-fluoro or 2′-methoxy groups. Structure calculations utilized a set of H-F RDC values for all 21 2′-fluoro modified nucleotides under conditions of weak alignment achieved by Pf1 phages. A completely 2′-F/2′-OMe modified dimeric RNA construct adopts an antiparallel double-helical structure consisting of 19 Watson–Crick base pairs with additional 3′ UU overhangs and a 5′ phosphate group on the antisense strand. NMR data suggest that the stability of individual base pairs is not uniform throughout the construct. While most of the double helical segment exhibits well dispersed imino resonances, the last three base pairs either display uncharacteristic chemical shifts of imino protons or absence of imino resonances even at lower temperatures. Accessibility of imino protons to solvent exchange suggests a difference in stability of duplex ends, which might be of importance for incorporation of the guide siRNA strand into a RISC.     

Molecular recognition in noncovalent antitumor agent-DNA complexes: NMR studies of the base and sequence dependent recognition of the DNA minor groove by netropsin

We have investigated intermolecular interactions and conformational features of the netropsin complexes with d(G1-G2-A3-A4-T5-T6-C7-C8) duplex (AATT 8-mer) and the d(G1-G2-T3-A4-T5-A6-C7-C8) duplex (TATA 8-mer) by one and two-dimensional NMR studies in solution. We have assigned the amide, pyrrole and methylene protons of netropsin and the base and sugar H1' protons of the nucleic acid from an analysis of the nuclear Overhauser effect (NOESY) and correlated (COSY) spectra of the complex at 25 degrees C. The directionality of the observed distance-dependent NOEs demonstrates that the 8-mer helices remain right-handed and that the arrangement of concave and convex face protons of netropsin are retained in the complexes. The observed changes in NOE patterns and chemical shift changes on complex formation suggest small conformational changes in the nucleic acid at the AATT and TATA antibiotic binding sites and possibly the flanking G.C base pairs. We observe intermolecular NOEs between all three amide and both pyrrole protons on the concave face of the antibiotic and the minor groove adenosine H2 proton of the two central A4.T5 base pairs of the AATT 8-mer and TATA 8-mer duplexes. The concave face pyrrole protons of the antibiotic also exhibit NOEs to the sugar H1' protons of residues 5 and 6 in the AATT and TATA 8-mer complexes. We also detect intermolecular NOEs between the guanidino and propioamidino methylene protons at either end of netropsin and the adenosine H2 proton of the two flanking A3.T6 base pairs in the AATT 8-mer and T3.A6 base pairs in the TATA 8-mer duplexes. These studies establish a set of nine contacts between the concave face of the antibiotic and the minor groove AATT segment and TATA segment of the 8-mer duplexes in solution. The observed magnitude of the NOEs require that there be no intervening water molecules sandwiched between the concave face of the antibiotic and the minor groove of the DNA so that release of the minor groove spine of hydration is a prerequisite for netropsin complex formation. The observed differences in the netropsin amide proton chemical shifts in the AATT 8-mer and TATA 8-mer complexes suggest differences in the strength and/or type of intermolecular hydrogen bonds at the AATT and TATA binding sites.(ABSTRACT TRUNCATED AT 400 WORDS)     

Thermodynamic analysis of 5' and 3' single- and 3' double-nucleotide overhangs neighboring wobble terminal base pairs

Thermodynamic parameters are reported for duplex formation of 40 self-complementary RNA duplexes containing wobble terminal base pairs with all possible 3′ single and double-nucleotide overhangs, mimicking the structures of short interfering RNAs (siRNA) and microRNAs (miRNA). Based on nearest neighbor analysis, the addition of a single 3′ dangling nucleotide increases the stability of duplex formation up to 1 kcal/mol in a sequence-dependent manner. The addition of a second dangling nucleotide increases the stability of duplexes closed with wobble base pairs in an idiosyncratic manner. The results allow for the development of a nearest neighbor model, which improves the predication of free energy and melting temperature for duplexes closed by wobble base pairs with 3′ single or double-nucleotide overhangs. Phylogenetic analysis of naturally occurring miRNAs was performed. Selection of the effector miR strand of the mature miRNA duplex appears to be dependent on the orientation of the GU closing base pair rather than the identity of the 3′ double-nucleotide overhang. Thermodynamic parameters for the 5′ single terminal overhangs adjacent to wobble closing base pairs are also presented.     

Thermodynamic stability of base pairs between 2-hydroxyadenine and incoming nucleotides as a determinant of nucleotide incorporation specificity during replication

We investigated the thermodynamic stability of double-stranded DNAs with an oxidative DNA lesion, 2-hydroxyadenine (2-OH-Ade), in two different sequence contexts (5′-GA*C-3′ and 5′-TA*A-3′, A* represents 2-OH-Ade). When an A*–N pair (N, any nucleotide base) was located in the center of a duplex, the thermodynamic stabilities of the duplexes were similar for all the natural bases except A (N = T, C and G). On the other hand, for the duplexes with the A*–N pair at the end, which mimic the nucleotide incorporation step, the stabilities of the duplexes were dependent on their sequence. The order of stability is T > G > C >> A in the 5′-GA*C-3′ sequences and T > A > C > G in the 5′-TA*A-3′ sequences. Because T/G/C and T/A are nucleotides incorporated opposite to 2-OH-Ade in the 5′-GA*C-3′ and 5′-TA*A-3′ sequences, respectively, these results agree with the tendency of mutagenic misincorporation of the nucleotides opposite to 2-OH-Ade in vitro. Thus, the thermodynamic stability of the A*–N base pair may be an important factor for the mutation spectra of 2-OH-Ade.     

Sequence-dependent recognition of DNA duplexes. Netropsin complexation to the AATT site of the d(G-G-A-A-T-T-C-C) duplex in aqueous solution

We have investigated intermolecular interactions and conformational features of the netropsin X d(G-G-A-A-T-T-C-C) complex by one- and two-dimensional NMR studies in aqueous solution. Netropsin removes the 2-fold symmetry of the d(G-G-A-A-T-T-C-C) duplex at the AATT binding site and to a lesser extent at adjacent dG X dC base pairs resulting in doubling of resonances for specific positions in the spectrum of the complex at 25 degrees C. We have assigned the amide, pyrrole, and CH2 protons of netropsin, and the base and sugar H1' protons of the nucleic acid from an analysis of the nuclear Overhauser effect (NOESY) and correlated (COSY) spectra of the complex at 25 degrees C. We observe intermolecular nuclear Overhauser effects (NOE) between all three amide and both pyrrole protons on the concave face of the antibiotic and the minor groove adenosine H2 proton of the two central A4 X T5 base pairs of the d(G1-G2-A3-A4-T5-T6-C7-C8) duplex. Weaker intermolecular NOEs are also observed between the pyrrole concave face protons and the sugar H1' protons of residues T5 and T6 in the AATT minor groove of the duplex. We also detect intermolecular NOEs between the guanidino CH2 protons at one end of netropsin and adenosine H2 proton of the two flanking A3 X T6 base pairs of the octanucleotide duplex. These studies establish a set of intermolecular contacts between the concave face of the antibiotic and the minor groove AATT segment of the d(G-G-A-A-T-T-C-C) duplex in solution. The magnitude of the NOEs require that there be no intervening water molecules sandwiched between the antibiotic and the DNA so that release of the minor groove spine of hydration is a prerequisite for netropsin complex formation.     

Structural studies of the O6meG.T interaction in the d(C-G-T-G-A-A-T-T-C-O6meG-C-G) duplex

High-resolution proton and phosphorus NMR studies are reported on the self-complementary d(C1-G2-T3-G4-A5-A6-T7-T8-C9-O6meG10-C11-G12) duplex (henceforth called O6meG.T 12-mer), which contains T3.O6meG10 interactions in the interior of the helix. The imino proton of T3 is observed at 9.0 ppm, exhibits a temperature-independent chemical shift in the premelting transition range, and broadens out at the same temperature as the imino proton of the adjacent G2.C11 toward the end of the helix at pH 6.8. We observed inter base pair nuclear Overhauser effects (NOEs) between the base protons at the T3.O6meG10 modification site and the protons of flanking G2.C11 and G4.C9 base pairs, indicative of the stacking of the T3 and O6meG10 bases into the helix. Two-dimensional correlated (COSY) and nuclear Overhauser effect (NOESY) studies have permitted assignment of the base and sugar H1', H2', and H2' nonexchangeable protons in the O6meG.T 12-mer duplex. The observed NOEs demonstrate an anti conformation about all the glycosidic bonds, and their directionality supports formation of a right-handed helix in solution. The observed NOEs between the T3.O6meG10 interaction and the adjacent G2.C11 and G4.C9 base pairs at the modification site exhibit small departures from patterns for a regular helix in the O6.meG.T 12-mer duplex. The phosphorus resonances exhibit a 0.5 ppm spectral dispersion indicative of an unperturbed phosphodiester backbone for the O6meG.T 12-mer duplex. We propose a model for pairing of T3 and O6meG10 at the modification site in the O6meG.T 12-mer duplex.(ABSTRACT TRUNCATED AT 250 WORDS)     

The base pairing properties of 8-aza-7-deaza-2'-deoxyisoguanosine and 7-halogenated derivatives in oligonucleotide duplexes with parallel and antiparallel chain orientation

The base pairing properties of oligonucleotide duplexes containing 8-aza-7-deaza-2′-deoxyisoguanosine, its 7-bromo or its 7-iodo derivative are described. The nucleosides were synthesized on a convergent route, protected and converted into phosphoramidites. Oligonucleotides were prepared on a solid-phase and were hybridized to yield duplexes with parallel (ps) or antiparallel (aps) chain orientation. The 8-aza-7-deaza-2′-deoxyisoguanosine-containing duplexes show almost identical base pairing stability as those containing 2′-deoxyisoguanosine, while the 7-substituted derivatives induce a significant duplex stabilization both in ps and aps DNA. Self-complementary duplexes with parallel chain orientation are exceptionally stable due to the presence of 5′-overhangs. The bulky halogen substituents were found to be well accommodated in the grooves both of aps and ps DNA.     

Comprehensive thermodynamic analysis of 3' double-nucleotide overhangs neighboring Watson-Crick terminal base pairs

Thermodynamic parameters are reported for duplex formation of 48 self-complementary RNA duplexes containing Watson–Crick terminal base pairs (GC, AU and UA) with all 16 possible 3′ double-nucleotide overhangs; mimicking the structures of short interfering RNAs (siRNA) and microRNAs (miRNA). Based on nearest-neighbor analysis, the addition of a second dangling nucleotide to a single 3′ dangling nucleotide increases stability of duplex formation up to 0.8 kcal/mol in a sequence dependent manner. Results from this study in conjunction with data from a previous study [A. S. O'Toole, S. Miller and M. J. Serra (2005) RNA, 11, 512.] allows for the development of a refined nearest-neighbor model to predict the influence of 3′ double-nucleotide overhangs on the stability of duplex formation. The model improves the prediction of free energy and melting temperature when tested against five oligomers with various core duplex sequences. Phylogenetic analysis of naturally occurring miRNAs was performed to support our results. Selection of the effector miR strand of the mature miRNA duplex appears to be dependent upon the identity of the 3′ double-nucleotide overhang. Thermodynamic parameters for 3′ single terminal overhangs adjacent to a UA pair are also presented.     

Pronounced instability of tandem IU base pairs in RNA

Optical melting was used to determine the stabilities of three series of RNA oligomers containing tandem XU base pairs, GGCXUGCC (5′XU3′), GGCUXGCC (5′UX3′) and GGCXXGGC/CCGUUCCG (5′XX3′), where X is either A, G or I (inosine). The helices containing tandem AU base pairs were the most stable in the first two series (5′XU3′ and 5′UX3′), with an average melting temperature ~11°C higher than the helices with tandem 5′GU3′ base pairs and 25°C higher than the helices with tandem 5′IU3′ base pairs. For the third series (5′XX3′), the helix containing tandem GG is the most stable, with an average melting temperature ~2°C higher than the helix with tandem AA base pairs and ~24°C higher than the helix with tandem II base pairs. The thermodynamic stability of the oligomers with tandem IU base pairs was also investigated as a function of magnesium ion concentration. As with normal A–U or G–U tandem duplexes, the data could best be interpreted as non-specific binding of magnesium ions to the inosine-containing RNA oligonucleotides.     

Covalent carcinogenic lesions in DNA: NMR studies of O6-methylguanosine containing oligonucleotide duplexes

We report on proton and phosphorus high resolution NMR investigations of the self-complementary dodecanucleotide d(C1-G2-N3-G4-A5-A6-T7-T8-C9-O6meG10-C11-G12) duplexes (henceforth called O6 meG.N 12-mers), N = C, T, A and G, which contain N3.O6meG10 interactions in the interior of the helix. These sequences containing a single modified O6meG per strand were prepared by phosphoamidite synthesis and provide an excellent model for probing the structural basis for covalent carcinogenic lesions in DNA. Distance dependent nuclear Overhauser effect (NOE) measurements and line widths of imino protons demonstrate that the N3 and O6meG.10 bases stack into the duplex and are flanked by stable Watson-Crick base pairs at low temperature for all four O6meG.N 12-mer duplexes. The imino proton of T3 in the O6meG.T 12-mer and G3 in the O6meG.N 12-mer helix, which are associated with the modification site, resonate at unusually high field (8.5 to 9.0 ppm) compared to imino protons in Watson-Crick base pairs (12.5 to 14.5 ppm). The nonexchangeable base and sugar protons have been assigned from two dimensional correlated (COSY) and nuclear Overhauser effect (NOESY) measurements on the O6meG.N 12-mer helices. The directionality of the distance dependent NOEs establish all O6meG.N duplexes to be right-handed helices in solution. The glycosidic torsion angles are in the anti range at the N3.O6meG10 modification site except for O6meG10 in the O6meG.G 12-mer duplex which adopts a syn configuration. This results in altered NOEs between the G3 (anti).O6meG10 (syn) pair and flanking G2.C11 and G4.C9 base pairs in the O6meG.G 12-mer duplex. We observe pattern reversal for cross peaks in the COSY spectrum linking the sugar H1' protons with the H2',2" protons at the G2 and O6meG10 residues in the O6meG.N 12-mer duplexes with the effect least pronounced for the O6meG.T 12-mer helix. The proton chemical shift and NOE data have been analyzed to identify regions of conformational perturbations associated with N3.O6meG10 modification sites in the O6meG.N 12-mer duplexes. The proton decoupled phosphorus spectrum of O6meG.T 12-mer duplex exhibits an unperturbed phosphodiester backbone in contrast to the phosphorus spectra of the O6meG.C 12-mer, O6meG.G 12-mer and O6meG.A 12-mer duplexes which exhibit phosphorus resonances dispersed over 2 ppm characteristic of altered phosphodiester backbones at the modification site. Tentative proposals are put forward for N3.O6meG10 pairing models based on the available NMR data and serve as a guide for the design of future experiments.     

Parallel-stranded duplex DNA containing dA · dU base pairs

DNA oligonucleotides with dA and dU residues can form duplexes with trans d(A · U) base pairing and the sugar-phosphate backbone in a parallel-stranded orientation, as previously established for oligonucleotides with d(A · T) base pairs. The properties of such parallel-stranded DNA (ps-DNA) 25-mer duplexes have been characterized by absorption (uv), CD, ir, and fluorescence spectroscopy, as well as by nuclease sensitivity. Comparisons were made with duplex molecules containing (a) dT in both strands, (b) dU in one strand and dT in the second, and (c) the same base combinations in reference antiparallel-stranded (aps) structures. Thermodynamic analysis revealed that total replacement of deoxythymine by deoxyuridine was accompanied by destabilization of the ps-helix (reduction in T_m by −13°C in 2 mM MgGl₂, 10 mM Na-cacodylate). The U-containing ps-helix (U1 · U2) also melted 14°C lower than the corresponding aps-helix under the same ionic conditions; this difference was very close to that observed between ps and aps duplexes with d(A · T) base pairs. Force field minimized structures of the various ps and aps duplexes with either d(A · T) or d(A · U) base pairs ps/aps and dT/dU combinations are presented. The energy-minimized helical parameters did not differ significantly between the DNAs containing dT and dU. © 1996 John Wiley & Sons, Inc.     

Base pair mismatches and carcinogen-modified bases in DNA: an NMR study of G.T and G.O4meT pairing in dodecanucleotide duplexes

High-resolution two-dimensional NMR studies have been completed on the self-complementary d(C-G-C-G-A-G-C-T-T-G-C-G) duplex (designated G.T 12-mer) and the self-complementary d(C-G-C-G-A-G-C-T-O4meT-G-C-G) duplex (designated G.O4meT 12-mer) containing G.T and G.O4meT pairs at identical positions four base pairs in from either end of the duplex. The exchangeable and nonexchangeable proton resonances have been assigned from an analysis of two-dimensional nuclear Overhauser enhancement (NOESY) spectra for the G.T 12-mer and G.O4meT 12-mer duplexes in H2O and D2O solution. The guanosine and thymidine imino protons in the G.T mismatch resonate at 10.57 and 11.98 ppm, respectively, and exhibit a strong NOE between themselves and to imino protons of flanking base pairs in the G.T 12-mer duplex. These results are consistent with wobble pairing at the G.T mismatch site involving two imino proton-carbonyl hydrogen bonds as reported previously [Hare, D. R., Shapiro, L., & Patel, D. J. (1986) Biochemistry 25, 7445-7456]. In contrast, the guanosine imino proton in the G.O4meT pair resonates at 8.67 ppm. The large upfield chemical shift of this proton relative to that of the imino proton resonance of G in the G.T mismatch or in G.C base pairs indicates that hydrogen bonding to O4meT is either very weak or absent. This guanosine imino proton has an NOE to the OCH3 group of O4meT across the pair and NOEs to the imino protons of flanking base pairs.(ABSTRACT TRUNCATED AT 250 WORDS)     

The solution structure of [d(CGC)r(aaa)d(TTTGCG)](2): hybrid junctions flanked by DNA duplexes

The solution structure and hydration of the chimeric duplex [d(CGC)r(aaa)d(TTTGCG)]₂, in which the central hybrid segment is flanked by DNA duplexes at both ends, was determined using two-dimensional NMR, simulated annealing and restrained molecular dynamics. The solution structure of this chimeric duplex differs from the previously determined X-ray structure of the analogous B-DNA duplex [d(CGCAAATTTGCG)]₂ as well as NMR structure of the analogous A-RNA duplex [r(cgcaaauuugcg)]₂. Long-lived water molecules with correlation time τ_c longer than 0.3 ns were found close to the RNA adenine H2 and H1′ protons in the hybrid segment. A possible long-lived water molecule was also detected close to the methyl group of 7T in the RNA–DNA junction but not with the other two thymines (8T and 9T). This result correlates with the structural studies that only DNA residue 7T in the RNA–DNA junction adopts an O4′-endo sugar conformation, while the other DNA residues including 3C in the DNA–RNA junction, adopt C1′-exo or C2′-endo conformations. The exchange rates for RNA C2′-OH were found to be ~5–20 s^–1. This slow exchange rate may be due to the narrow minor groove width of [d(CGC)r(aaa)d(TTTGCG)]₂, which may trap the water molecules and restrict the dynamic motion of hydroxyl protons. The minor groove width of [d(CGC)r(aaa)d(TTTGCG)]₂ is wider than its B-DNA analog but narrower than that of the A-RNA analog. It was further confirmed by its titration with the minor groove binding drug distamycin. A possible 2:1 binding mode was found by the titration experiments, suggesting that this chimeric duplex contains a wider minor groove than its B-DNA analog but still narrow enough to hold two distamycin molecules. These distinct structural features and hydration patterns of this chimeric duplex provide a molecular basis for further understanding the structure and recognition of DNA·RNA hybrid and chimeric duplexes.     

O6-ethylguanine carcinogenic lesions in DNA: an NMR study of O6etG.C pairing in dodecanucleotide duplexes

The pairing of O6etG with C located four base pairs in from either end of the self-complementary d(C1-G2-C3-O6etG4-A5-G6-C7-T8-C9-G10-C11-G12) duplex (designated O6etG.C 12-mer) has been investigated from an analysis of proton and phosphorus two-dimensional NMR experiments. The structural consequences of increasing the alkyl group size were elucidated from a comparative study of the pairing of O6meG4 with C9 in a related sequence (designated O6meG.C 12-mer). The NMR parameters for both O6alkG-containing dodecanucleotides are also compared with those of the control sequence containing G4.C9 base pairs (designated G.C 12-mer). The NOE cross-peaks detected in the two-dimensional NOESY spectra of the O6alkG.C 12-mer duplexes in H2O solution establish that the O6etG4/O6meG4 and C9 bases at the lesion site stack into the helix between the flanking C3.G10 and A5.T8 Watson-Crick base pairs. The amino protons of C9 at the O6alkG4-C9 lesion site resonate as an average resonance at 7.78 and 7.63 ppm in the O6etG.C 12-mer and O6meG.C 12-mer duplexes, respectively. The observed NOEs between the amino protons of C9 and the CH3 protons of O6alkG4 establish a syn orientation of the O6-alkyl group with respect to the N1 of alkylated guanine. A wobble alignment of the O6alkG4.C9 base pair stablized by two hydrogen bonds, one between the amino group of C9 and N1 of O6alkG and the other between the amino group of O6alkG and N3 of C9, is tentatively proposed on the basis of the NOEs between the amino protons of C9 at the lesion site and the imino protons of flanking Watson-Crick base pairs. The proton and phosphorus chemical shift differences between the O6etG.C 12-mer and O6meG.C 12-mer duplexes are small compared to the differences between these O6alkG-containing duplexes and the control G.C 12-mer duplex.     

Insights into the DNA stabilizing contributions of a bicyclic cytosine analogue: crystal structures of DNA duplexes containing 7,8-dihydropyrido [2,3-d]pyrimidin-2-one

The incorporation of the bicyclic cytosine analogue 7,8-dihydropyrido[2,3-d]pyrimidin-2-one (X) into DNA duplexes results in a significant enhancement of their stability (3–4 K per modification). To establish the effects of X on the local hydrogen-bonding and base stacking interactions and the overall DNA conformation, and to obtain insights into the correlation between the structure and stability of X-containing DNA duplexes, the crystal structures of [d(CGCGAATT-X-GCG)]₂ and [d(CGCGAAT-X-CGCG)]₂ have been determined at 1.9–2.9 Å resolutions. In all of the structures, the analogue X base pairs with the purine bases on the opposite strands through Watson–Crick and/or wobble type hydrogen bonds. The additional ring of the X base is stacked on the thymine bases at the 5′-side and overall exhibits greatly enhanced stacking interactions suggesting that this is a major contribution to duplex stabilization.     

Structure and drug interactions of parallel-stranded DNA studied by infrared spectroscopy and fluorescence.

The infrared spectra of three different 25-mer parallel-stranded DNAs (ps-DNA) have been studied. We have used ps-DNAs containing either exclusively dA x dT base pairs or substitution with four dG x dC base pairs and have them compared with their antiparallel-stranded (aps) reference duplexes in a conventional B-DNA conformation. Significant differences have been found in the region of the thymine C = O stretching vibrations. The parallel-stranded duplexes showed characteristic marker bands for the C2 = O2 and C4 = O4 carbonyl stretching vibrations of thymine at 1685 cm-1 and 1668 cm-1, respectively, as compared to values of 1696 cm-1 and 1663 cm-1 for the antiparallel-stranded reference duplexes. The results confirm previous studies indicating that the secondary structure in parallel-stranded DNA is established by reversed Watson--Crick base pairing of dA x dT with hydrogen bonds between N6H...O2 and N1...HN3. The duplex structure of the ps-DNA is much more sensitive to dehydration than that of the aps-DNA. Interaction with three drugs known to bind in the minor groove of aps-DNA--netropsin, distamycin A and Hoechst 33258--induces shifts of the C = O stretching vibrations of ps-DNA even at low ratio of drug per DNA base pair. These results suggest a conformational change of the ps-DNA to optimize the DNA-drug interaction. As demonstrated by excimer fluorescence of strands labeled with pyrene at the 5'-end, the drugs induce dissociation of the ps-DNA duplex with subsequent formation of imperfectly matched aps-DNA to allow the more favorable drug binding to aps-DNA. Similarly, attempts to form a triple helix of the type d(T)n.d(A)n.d(T)n with ps-DNA failed and resulted in the dissociation of the ps-DNA duplex and reformation of a triple helix based upon an aps-DNA duplex core d(T)10.d(A)10.