The intrinsic structure and stability of out-of-alternation base pairs in Z-DNA.

Alternating pyrimidine-purine sequences typically form Z-DNA, with the pyrimidines in the anti and purines in the syn conformations. The observation that dC and dT nucleotides can also adopt the syn conformation (i.e. the nucleotides are out-of-alternation) extends the range of sequences that can convert to this left-handed form of DNA. Here, we study the effects of placing two adjacent d(G*C) base pairs as opposed to a single d(G*C) base pair or two d(A*T) base pairs out-of-alternation by comparing the structure of d(m5CGGCm5CG)2with the previously published structures of d(m5CGGGm5CG)*d(m5CGCCm5CG) and d(m5CGATm5CG)2. A high buckle and loss of stacking interactions are observed as intrinsic properties of the out-of-alternation base pairs regardless of sequence and the context of the dinucleotide. From solution titrations, we find that the destabilizing effect of out-of-alternation d(G*C) base pairs are identical whether these base pairs are adjacent or isolated. We can therefore conclude that it is these intrinsic distortions in the structure of the base pairs and not neighboring effects that account for the inability of out-of-alternation base pairs to adopt the left-handed Z conformation.     

Nudged elastic band calculation of minimal energy paths for the conformational change of a GG non-canonical pair

The nudged elastic band (NEB) technique has been implemented in AMBER to calculate low-energy paths for conformational changes. A novel simulated annealing protocol that does not require an initial hypothesis for the path is used to sample low-energy paths. This was used to study the conformational change of an RNA cis Watson-Crick/Hoogsteen GG non-canonical pair, with one G syn around the glycosidic bond and the other anti. A previous solution structure, determined by NMR-constrained modeling, demonstrated that the GG pairs change from (syn)G-(anti)G to (anti)G-(syn)G in the context of duplex r(GCAGGCGUGC) on the millisecond timescale. The set of low-energy paths found by NEB show that each G flips independently around the glycosidic bond, with the anti G flipping to syn first. Guanine bases flip without opening adjacent base-pairs by protruding into the major groove, accommodated by a transient change by the ribose to C2'-exo sugar pucker. Hydrogen bonds between bases and the backbone, which lower the energetic barrier to flipping, are observed along the path. The results show the plasticity of RNA base-pairs in helices, which is important for biological processes, including mismatch repair, protein recognition, and translation. The modeling of the GG conformational change also demonstrates that NEB can be used to discover non-trivial paths for macromolecules and therefore NEB can be used as an exploratory method for predicting putative conformational change paths.     

Structural features and thermodynamics of the J4/5 loop from the Candida albicans and Candida dubliniensis group I introns

The J4/5 loop of group I introns has tertiary interactions with the P1 helix that position the P1 substrate for the self-splicing reaction. The J4/5 loop of Candida albicans and Candida dubliniensis, 5'GAAGG3'/3'UAAUU5', potentially contains two A.A pairs flanked by one G.U pair on one side and two G.U pairs on the other side. Results from optical melting, nuclear magnetic resonance spectroscopy, and functional group substitution experiments with a mimic of the C. albicans and C. dubliniensis J4/5 loop are consistent with the adenosines forming tandem sheared A.A pairs with a cross-strand stack and only the G.U pair not adjacent to an A.A pair forming a static wobble G.U pair. The two G.U pairs adjacent to the tandem A.A pairs are likely in a dynamic equilibrium between multiple conformations. Although Co(NH(3))(6)(3+) stabilizes the loop by several kilocalories per mole at 37 degrees C, addition of Mg(2+) or Co(NH(3))(6)(3+) has no effect on the structure of the loop. The tandem G.U pairs provide a pocket of negative charge for Co(NH(3))(6)(3+) to bind. The results contribute to understanding the structure and dynamics of purine-rich internal loops and potential G.U pairs adjacent to internal loops.     

Solution structures of the individual single strands of the fragile X DNA triplets (GCC)n.(GGC)n.

Three-dimensional structures of the fragile X triplet repeats (GCC)n and (GGC)n are derived by using one- dimensional/two-dimensional NMR. Under a wide range of solution conditions (10-150 mM NaCl,pH6-7)(GCC)5-7 strands form exclusively slipped hairpins with a 3' overhanging C. The slipped hairpins of (GCC)n strands show the following structural characteristics: (i) maximization of Watson-Crick G.C pairs; (ii) formation of C.C mispairs at the CpG steps in the stem; (iii) C2'-endo, anti conformations for all the nucleotides. The ability of (GCC)n strands to form hairpin structures more readily than complementary (GGC)n strands suggests preferential slippage during replication and subsequent expansion of the (GCC)n strands. In addition, the C.C. mispairs at the CpG site of (GCC)n hairpins account for their exceptional substrate efficiencies for human methyltransferase. Gel electrophoresis data show that (GGC)n strands form both hairpin and mismatched duplex structures in 10-150 mM NaCl (ph 6-7) for n < 10, but for n > or + 11 hairpin structures are exclusively present. However, (GGC)n strands remain predominantly in the duplex state for n=4-11 under NMR solution conditions, which require DNA concentrations 100- to 1000-fold higher than in gel electrophoresis. NMR analyses of [(GGC)n]2 duplexes for n=4-6 show the presence of Watson-Crick G.C and mismatched G anti G syn pairs. The mismatches adjacent to the CpG step introduce local structural flexibility in these duplexes. Similar structural properties are also expected in the stem of the hairpins formed by (GGC)n strands.     

Molecular recognition in purine-rich internal loops: thermodynamic,structural, and dynamic consequences of purine for adenine substitutions in 5'(rGGCAAGCCU)2

The contribution of amino groups to the thermodynamics, structure, and dynamics of tandem A.A mismatches is investigated by substitution of purine (P) for adenine (A) within the RNA duplex, 5'(rGGCAAGCCU)(2), to give 5'(rGGCPAGCCU)(2), 5'(rGGCAPGCCU)(2), and 5'(rGGCPPGCCU)(2). The 5'(rGGCAAGCCU)(2) duplex has sheared A(anti).A(anti) (A.A trans Hoogsteen/Sugar-edge) pairs in which the A5 amino group is involved in hydrogen bonds but the A4 amino group is not [Znosko, B. M., Burkard, M. E., Schroeder, S. J., Krugh, T. R., and Turner, D. H. (2002) Biochemistry 41, 14969-14977]. In comparison to 5'(rGGCAAGCCU)(2), replacing the amino group of A4 with a hydrogen stabilizes the duplex by 1.3 kcal/mol, replacement of the A5 amino group destabilizes the duplex by 0.6 kcal/mol, and replacement of both A4 and A5 amino groups destabilizes the duplex by 0.8 kcal/mol. In NMR structures, the P.A noncanonical pairs of the 5'(rGGCPAGCCU)(2) duplex have a sheared anti-anti structure (P.A trans Hoogsteen/Sugar-edge) with P4.A5 interstrand hydrogen bonding and A5 bases that interstrand stack, similar to the structure of 5'(rGGCAAGCCU)(2). In contrast, the A.P pairs of the 5'(rGGCAPGCCU)(2) duplex have a face-to-face conformation (A.P trans Watson-Crick/Watson-Crick) with intrastrand stacking resembling typical A-form geometry. Although the P5 bases in 5'(rGGCPPGCCU)(2) are involved in an interstrand stack, the loop region is largely undefined. The results illustrate that both hydrogen-bonded and non-hydrogen-bonded amino groups play important roles in determining the thermodynamic, structural, and dynamic characteristics of purine rich internal loops.     

Crystal structures of CGG RNA repeats with implications for fragile X-associated tremor ataxia syndrome

The CGG repeats are present in the 5'-untranslated region (5'-UTR) of the fragile X mental retardation gene FMR1 and are associated with two diseases: fragile X-associated tremor ataxia syndrome (FXTAS) and fragile X syndrome (FXS). FXTAS occurs when the number of repeats is 55-200 and FXS develops when the number exceeds 200. FXTAS is an RNA-mediated disease in which the expanded CGG tracts form stable structures and sequester important RNA binding proteins. We obtained and analysed three crystal structures of double-helical CGG repeats involving unmodified and 8-Br modified guanosine residues. Despite the presence of the non-canonical base pairs, the helices retain an A-form. In the G-G pairs one guanosine is always in the syn conformation, the other is anti. There are two hydrogen bonds between the Watson-Crick edge of G(anti) and the Hoogsteen edge of G(syn): O6·N1H and N7·N2H. The G(syn)-G(anti) pair shows affinity for binding ions in the major groove. G(syn) causes local unwinding of the helix, compensated elsewhere along the duplex. CGG helical structures appear relatively stable compared with CAG and CUG tracts. This could be an important factor in the RNA's ligand binding affinity and specificity.     

Nuclear magnetic resonance spectroscopy and molecular modeling reveal that different hydrogen bonding patterns are possible for G.U pairs: one hydrogen bond for each G.U pair in r(GGCGUGCC)(2) and two for each G.U pair in r(GAGUGCUC)(2)

G.U pairs occur frequently and have many important biological functions. The stability of symmetric tandem G.U motifs depends both on the adjacent Watson-Crick base pairs, e.g., 5'G > 5'C, and the sequence of the G.U pairs, i.e., 5'-UG-3' > 5'-GU-3', where an underline represents a nucleotide in a G.U pair [Wu, M., McDowell, J. A., and Turner, D. H. (1995) Biochemistry 34, 3204-3211]. In particular, at 37 degrees C, the motif 5'-CGUG-3' is less stable by approximately 3 kcal/mol compared with other symmetric tandem G.U motifs with G-C as adjacent pairs: 5'-GGUC-3', 5'-GUGC-3', and 5'-CUGG-3'. The solution structures of r(GAGUGCUC)(2) and r(GGCGUGCC)(2) duplexes have been determined by NMR and restrained simulated annealing. The global geometry of both duplexes is close to A-form, with some distortions localized in the tandem G.U pair region. The striking discovery is that in r(GGCGUGCC)(2) each G.U pair apparently has only one hydrogen bond instead of the two expected for a canonical wobble pair. In the one-hydrogen-bond model, the distance between GO6 and UH3 is too far to form a hydrogen bond. In addition, the temperature dependence of the imino proton resonances is also consistent with the different number of hydrogen bonds in the G.U pair. To test the NMR models, U or G in various G.U pairs were individually replaced by N3-methyluridine or isoguanosine, respectively, thus eliminating the possibility of hydrogen bonding between GO6 and UH3. The results of thermal melting studies on duplexes with these substitutions support the NMR models.     

NMR studies of the exocyclic 1,N6-ethenodeoxyadenosine adduct (epsilon dA) opposite deoxyguanosine in a DNA duplex. Epsilon dA(syn).dG(anti) pairing at the lesion site

Proton NMR studies are reported on the complementary d(C-A-T-G-G-G-T-A-C).d(G-T-A-C-epsilon A-C-A-T-G) nonanucleotide duplex (designated epsilon dA.dG 9-mer duplex), which contains exocyclic adduct 1,N6-ethenodeoxyadenosine positioned opposite deoxyguanosine in the center of the helix. The present study focuses on the alignment of dG5 and epsilon dA14 at the lesion site in the epsilon dA.dG 9-mer duplex at neutral pH. This alignment has been characterized by monitoring the NOEs originating from the NH1 proton of dG5 and the H2, H5, and H7/H8 protons of epsilon dA14 in the central d(G4-G5-G6).d(C13-epsilon A14-C15) trinucleotide segment of the epsilon dA.dG 9-mer duplex. These NOE patterns establish that epsilon dA14 adopts a syn glycosidic torsion angle that positions the exocyclic ring toward the major groove edge while all the other bases including dG5 adopt anti glycosidic torsion angles. We detect a set of intra- and interstrand NOEs between protons (exchangeable and nonexchangeable) on adjacent residues in the d(G4-G5-G6).d(C13-epsilon A14-C15) trinucleotide segment which establish formation of right-handed helical conformations on both strands and stacking of the dG5(anti).epsilon dA14(syn) pair between stable dG4.dC15 and dG6.dC13 pairs. The energy-minimized conformation of the central d(G4-G5-G6).d(C13-epsilon A14-C15) segment establishes that the dG5(anti).epsilon dA14(syn) alignment is stabilized by two hydrogen bonds from the NH1 and NH2-2 of dG5(anti) to N9 and N1 of epsilon dA14(syn), respectively.(ABSTRACT TRUNCATED AT 250 WORDS)     

Multinuclear nuclear magnetic resonance studies of Na cation-stabilized complex formed by d(G-G-T-T-T-T-C-G-G) in solution. Implications for G-tetrad structures.

There has been much recent interest in the self-association of short deoxyguanosine-rich motifs within single-stranded DNAs to generate monovalent cation modulated four-stranded helical segments called G-quadruplexes stabilized by hydrogen-bonded G-tetrad alignments. We have addressed structural aspects of this novel alignment and report on multinuclear 1H, 31P and 13C nuclear magnetic resonance studies on the d(G2T4CG2) deoxynonanucleotide with Na cation as counterion in aqueous solution at low temperature. This sequence forms stable structures even though it cannot align by Watson-Crick hydrogen bond formation (see the paper on d(G2T5G2) describing optical and calorimetric measurements by Jin, R., Breslauer, K. J., Jones, R. A. & Gaffney, B. L. (1990), Science, 250, 543-546). The four narrow exchangeable protons detected between 11.5 and 12.0 parts per million (p.p.m.), which are common to the d(G2T4CG2) deoxynonanucleotide and the d(G2TCG2) deoxyhexanucleotide sequences, are assigned to deoxyguanosine imino protons hydrogen-bonded to carbonyl acceptor groups. These narrow imino protons are not detected for d(IGN5IG) and d(I2N5G2), where two deoxyguanosine residues are replaced by two deoxyinosine residues in the deoxynonanucleotide sequences. This implies that the 2-amino protons of deoxyguanosine must also participate in hydrogen bond formation and stabilize the structured conformation of d(G2T4CG2) in Na cation-containing solution. We have completely assigned the base and sugar H1', H2',2', H3', and H4' protons of the d(G2T4CG2) oligomer following analysis of two-dimensional nuclear Overhauser enhancement spectroscopy and two-dimensional correlated spectroscopy data sets in 0.1 M-NaCl, 10 mM-sodium phosphate, 2H2O solution at 0 degree C. The relative magnitude of the nuclear Overhauser enhancements (NOEs) between the base H8 and its own sugar H1' protons of individual deoxyguanosine residues establishes that G1 and G8 adopt syn orientations while G2 and G9 adopt anti orientations about the glycosidic bond in the d(G1-G2-T3-T4-T5-T6-C7-G8-G9) sequence in both Na and K cation-containing aqueous solution. Consequently, any structure proposed for the tetramolecular complex of d(G2T4CG2) must exhibit alternating G(syn) and G(anti) glycosidic torsion angles within each strand. The directionality and magnitude of the observed NOEs are consistent with the G(syn)-G(anti) steps adopting right-handed helical conformations in solution. We also note that the H8 protons of G1 and G8 (7.35 to 7.45 p.p.m.) in a syn alignment are shifted significantly upfield from the H8 protons of G2 and G9 (8.0 to 8.3 p.p.m.) in an anti alignment.(ABSTRACT TRUNCATED AT 400 WORDS)     

Thermodynamics of RNA internal loops with a guanosine-guanosine pair adjacent to another noncanonical pair

Thermodynamic parameters measured by optical melting are reported for formation of RNA duplexes containing tandem noncanonical pairs with at least one guanosine-guanosine (GG) pair. For selected sequences, imino proton NMR provides evidence that the desired duplex forms and that the structure of a GG pair adjacent to a noncanonical pair depends on context. A GG pair next to a different noncanonical pair is more stable than expected from measurements of adjacent GG pairs. This is likely due to an unfavorable stacking interaction between adjacent GG pairs, where areas of high negative charge probably overlap. The results suggest a model where tandem noncanonical pairs closed by two GC pairs are assigned the following free energy increments at 37 degrees C: 0.8 kcal/mol for adjacent GG pairs, 1.0 kcal/mol for GG next to UU, and -0.3 kcal/mol for all others. These values are adjusted by 0.65 kcal/mol for each closing AU pair.     

NMR studies of an exocyclic 1,N2-propanodeoxyguanosine adduct (X) located opposite deoxyadenosine (A) in DNA duplexes at basic pH: simultaneous partial intercalation of X and A between stacked bases

The NMR parameters for the 1,N2-propanodeoxyguanosine (X) opposite deoxyadenosine positioned in the center of the complementary d(C1-A2-T3-G4-X5-G6-T7-A8-C9).d(G10-T11-A12-C13-A14-C15-A 16-T17-G18) X.A 9-mer duplex are pH dependent. A previous paper established protonated X5(syn).A14(anti) pairing in the X.A 9-mer duplex at pH 5.8 [Kouchakdjian, M., Marinelli, E., Gao, X., Johnson, F., Grollman, A., & Patel, D. J. (1989) Biochemistry 28, 5647-5657]; this paper focuses on the pairing alignment at the lesion site at pH 8.9. The observed NOEs between specific exocyclic CH2 protons and both the imino proton of G6 and the sugar H1' protons of C13 and A14 establish that X5 is positioned toward the G6.C13 base pair with the exocyclic ring directed between C13 and A14 on the partner strand. The observed NOE between the H2 proton of A14 and the imino proton of G4, but not G6, establishes that A14 at the lesion site is directed toward the G4.C15 base pair. NOEs are detected between all exocyclic CH2 protons of X5 and the H2 proton of A14, confirming that both X5 and A14 are directed toward the interior of the helix. The X5(anti).A14(anti) alignment at pH 8.9 is accommodated within the helix with retention of Watson-Crick pairing at flanking G4.C15 and G6.C13 base pairs. The energy-minimized conformation of the (G4-X5-G6).(C13-A14-C15) segment at pH 8.9 establishes that X5 and A14 are directed into the helix, partially stack on each other, and are not stabilized by intermolecular hydrogen bonds. The X5 base is partially intercalated between C13 and A14 on the unmodified strand, while A14 is partially intercalated between G4 and X5 on the modified strand. This results in a larger separation between the G4.C15 and G6.C13 base pairs flanking the lesion site in the basic pH conformation of the X.A 9-mer duplex. The midpoint of the transition between the protonated X5(syn).A14(anti) and X5(anti).A14(anti) conformations occurs at pH 7.6, establishing an unusually high pKa for protonation of the A14 ring opposite the X5 exocyclic adduct site. Thus, the interplay between hydrophobic and hydrogen-bonding contributions modulated by pH defines the alignment of 1,N2-propanodeoxyguanosine opposite deoxyadenosine in the interior of DNA helices.     

Conformational feasibility of a hairpin with two purines in the loop. 5'-d-GGTACIAGTACC-3'

Structural feasibility and conformational requirements for the sequence 5'-d-GGTACIAGTACC-3' to adopt a hairpin loop with I6 and A7 in the loop are studied. It is shown that a hairpin loop containing only two nucleotides can readily be formed without any unusual torsional angles. Stacking is continued on the 5'-side of the loop, with the I6 stacked upon C5. The base A7, on the 3'-side of the loop, can either be partially stacked with I6 or stick outside without stacking. Loop closure can be achieved for both syn and anti conformations of the glycosidic torsions for G8 while maintaining the normal Watson-Crick base pairing with the opposite C5. All torsional angles in the stem fall within the standard B-family of DNA helical structures. The phosphodiesters of the loop have trans,trans conformations. Loop formation might require the torsion about the C4'-C5' bond of G8 to be trans as opposed to the gauche+ observed in B-DNA. These results are discussed in relation to melting temperature studies [Howard et al. (1991) Biochemistry (preceding paper in this issue)] that suggest the formation of very stable hairpin structures for this sequence.     

Structure of purine-purine mispairs during misincorporation and extension by Escherichia coli DNA polymerase I

The mechanism by which purine-purine mispairs are formed and extended was examined with the high-fidelity Klenow fragment of Escherichia coli DNA polymerase I with the proofreading exonuclease activity inactivated. The structures of the purine-purine mispairs were examined by comparing the kinetics of mispair formation with adenine versus 7-deazaadenine and guanine versus 7-deazaguanine at four positions in the DNA, the incoming dNTP, the template base, and both positions of the terminal base pair. A decrease in rate associated with a 7-deazapurine substitution would suggest that the nucleotide is in a syn conformation in a Hoogsteen base pair with the opposite base. During mispair formation, the k(pol)/K(d) values for the insertion of dATP opposite A (dATP/A) as well as dATP/G and dGTP/G were decreased greater than 10-fold with the deazapurine in the dNTP. These results suggest that during mispair formation the newly forming base pair is in a Hoogsteen geometry with the incoming dNTP in the syn conformation and the template base in the anti conformation. During mispair extension, the only decrease in k(pol)/K(d) was associated with the G/G base pair in which 7-deazaguanine was in the template strand. These results as well as previous results [McCain et al. (2005) Biochemistry 44, 5647-5659] in which a hydrogen bond was found between the 3-position of guanine at the primer terminus and Arg668 during G/A and G/G mispair extension indicate that the conformation of the purine at the primer terminus is in the anti conformation during mispair extension. These results suggest that purine-purine mispairs are formed via a Hoogsteen geometry in which the dNTP is in the syn conformation and the template is in the anti conformation. During extension, however, the conformation of the primer terminus changes to an anti configuration while the template base may be in either the syn or anti conformations.     

Alternating d(GA)n DNA sequences form antiparallel stranded homoduplexes stabilized by the formation of G.A base pairs.

Alternating d(GA)n DNA sequences form antiparallel stranded homoduplexes which are stabilized by the formation of G.A pairs. Three base pairings are known to occur between adenine and guanine: AH+ (anti).G(syn), A(anti).G(anti) and A(syn).G(anti). Protonation of the adenine residues is not involved in the stabilization of this structure, since it is observed at any pH value from 8.3 to 4.5; at pH < or = 4.0 antiparallel stranded d(GA.GA) DNA is destabilized. The results reported in this paper strongly suggest that antiparallel stranded d(GA.GA) homoduplexes are stabilized by the formation of alternating A(anti).G(anti) and G(anti).A(syn) pairs. In this structure, all guanine residues are in the anti conformation with their N7 position freely accessible to DMS methylation. On the other hand, adenines in one strand adopt the anti conformation, with their N7 position also free for reaction, while those of the opposite strand are in the syn conformation, with their N7 position hydrogen bonded to the guanine N1 group of the opposite strand. A regular right-handed helix can be generated using alternating G(anti).A(syn) and A(anti).G(anti) pairs.     

Characterization by 1H NMR of glycosidic conformations in the tetramolecular complex formed by d(GGTTTTTGG).

We have conducted two dimensional NOESY studies on the molecule d(G2T5G2) to characterize the structure of the tetramolecular complex previously identified by calorimetric and spectroscopic studies (1). Analysis of the NOE and exchange cross peaks observed in the NOESY spectra establishes the formation of structured conformations at low temperature (5 degrees C). Significantly, within each strand of these structured conformations, the G1 and G8 residues adopt syn glycosidic torsion angles, while the G2 and G9 residues adopt anti glycosidic torsion angles. Consequently, any structure proposed for the tetramolecular complex of d(G2T5G2) must have alternating G(syn) and G(anti) glycosidic torsion angles within each strand. The implications of this observation for potential structures of the tetramolecular complex of d(G2T5G2) are discussed.     

X-ray analyses of two DNA dodecamers containing N4-methoxy-cytosine paired with adenine or guanine.

To investigate mismatch of base-pairings in relation to mutagenesis by oxyamines, crystal structures of two DNA dodecamers with the sequence d(CGCZAA TTmo4CGCG) (Z = A or G), containing N4-methoxy-cytosine (mo4C), have been determined by X-ray analysis. These dodecamers essentially form right-handed B-form duplexes, respectively. In the dodecamer with Z = A, the two mo4C residues are adapted in imino form with the anti methoxyl group to form pairs with A on the opposite strand in a manner of Watson-Crick fashion. While in the dodecamer with Z = G, one mo4C in amino form with the anti methoxyl group forms a normal Watson-Crick pair with G, but the other one in imino form with syn methoxyl conformation wobbles with G. Based on these results, possible mutation mechanism has been proposed.     

NMR studies for identification of dI:dG mismatch base-pairing structure in DNA.

One- and two-dimensional NMR experiments have been undertaken to investigate deoxyinosine:deoxyguanosine (dI:dG) base pairing in a self-complementary dodecadeoxyribonucleotide, d(C1-G2-C3-I4-A5-A6-T7-T8-G9-G10-G11-G12) (designated IG-12), duplex. The NMR data indicate formation of a dI(syn):dG(anti) base pair in a B-DNA helix. This unusual base pairing results in altered NOE patterns between the base protons (H8 and H2) of the I4 residue and the sugar protons of its own and the 5'-flanking C3 residues. The dI(syn):dG(anti) base pair is accommodated in the B-DNA duplex with only a subtle distortion of the local conformation. Identification of the dI:dG base pairing in this study confirms that a hypoxanthine base can form hydrogen-bonded base pairs with all of the four normal bases, C, A, T, and G, in DNA.     

Infrared spectral studies of the non regularly alternating purine-pyrimidine hexamers d(m5CGGCM5CG), d(CBr8GGCCBr8G) and d(CGCGGC)

The oligonucleotides d(m5CGGCm5CG), d(CBr8GGCCBr8G) and d(CGCGGC) have been prepared and studied by infrared spectroscopy. The three sequences contain two GC pairs which are out of purine-pyrimidine alternation with the rest of the sequence. From the IR data of the d(m5CGGCm5CG) hexamer, it is shown that all of the dG residues adopt a syn conformation. The marker IR bands for the C3' endo syn conformation are at 1410, 1354, 1320 and 925 cm-1 whereas those for the C2' endo anti conformation at 1420, 1374 and 890 cm-1 are clearly absent. This result implies that the two adjacent guanines of the d(m5CGGCm5CG) sequence are in syn conformation. It is suggested that duplex formation occurs in d(CGCGGC) films and that all of the guanines are in syn conformation. In contrast, the central non-brominated guanine of the d(CBr8GGCCBr8G) hexamer is found in anti conformation, as expected in a Z type structure of the non-alternating region.     

Electronic structure of DNA by DV-X alpha cluster calculations: II. d(GG).d(CC), d(CG)2, d(GC)2 A and B conformations. (Part 2) Sugars and bases

The electronic structure of d(GG).d(CC), d(CG)2, d(GC)2 which are stacked base pairs in the DNA double helix, are elucidated for both A and B conformations in detail by DV-X alpha cluster calculations. These three DNA double helix fragments are contracted from the same bases, G and C, but the electronic structures of the fragments for both A and B conformations are different from each other characteristically. There are some delicate differences in the admixture of the orbital components and the overlap populations of intra- and inter- strand stacked bases among the stacking isomers. On the other hand, the electronic states of sugars differ in the 5'-3' direction, but are not almost dependent on stacked base pairs.