Solution structure of an arabinonucleic acid (ANA)/RNA duplex in a chimeric hairpin: comparison with 2′-fluoro-ANA/RNA and DNA/RNA hybrids

Hybrids of RNA and arabinonucleic acid (ANA) as well as the 2′-fluoro-ANA analog (2′F-ANA) were recently shown to be substrates of the enzyme RNase H. Although RNase H binds to double-stranded RNA, no cleavage occurs with such duplexes. Therefore, knowledge of the structure of ANA/RNA hybrids may prove helpful in the design of future antisense oligonucleotide analogs. In this study, we have determined the NMR solution structures of ANA/RNA and DNA/RNA hairpin duplexes and compared them to the recently published structure of a 2′F-ANA/RNA hairpin duplex. We demonstrate here that the sugars of RNA nucleotides of the ANA/RNA hairpin stem adopt the C3′-endo (north, A-form) conformation, whereas those of the ANA strand adopt a ‘rigid’ O4′-endo (east) sugar pucker. The DNA strand of the DNA/RNA hairpin stem is flexible, but the average DNA/RNA hairpin structural parameters are close to the ANA/RNA and 2′F-ANA/RNA hairpin parameters. The minor groove width of ANA/RNA, 2′F-ANA/RNA and DNA/RNA helices is 9.0 ± 0.5 Å, a value that is intermediate between that of A- and B-form duplexes. These results rationalize the ability of ANA/RNA and 2′F-ANA/RNA hybrids to elicit RNase H activity.     

The A and B conformations of DNA and RNA subunits. Potential energy calculations for dGpdC

In order to obtain a molecular picture of the A and B forms of a DNA subunit, potential energy calculations have been made for dGpdC with C(3′)-endo and C(2′)-endo [or C(3′)-exo] sugar puckerings. These are compared with results for GpC. The global minima for dGpdC and GpC are almost identical. They are like A-form duplex DNA and RNA, respectively, with bases anti, the ω′, ω angle pair near 300°, 280°, and sugar pucker C(3′)-endo. For dGpdC, a B-form helical conformer, with sugar pucker C(2′)-endo and ω′ = 257°, ω = 298°, is found only 0.4 kcal/mol above the global minimum. A second low-energy conformation (2.3 kcal/mol) has ω′ = 263°, ω = 158° and ψ near 180°. This has dihedral angles like the original Watson–Crick model of the double helix. In contrast, for GpC, the C(2′)-endo B form is 6.9 kcal/mol above the global minimum. These theoretical results are consistent with experimental studies on DNA and RNA fibers. DNA fibers exist in both A and B forms, while RNA fibers generally assume only the A form. A low-energy conformation unlike the A or B forms was found for both dGpdC and GpC when the sugars were C(3′)-endo. This conformation—ω′,ω near 20°,80°—was not observed for C(2′)-endo dGpdC. Energy surface maps in the ω′,ω plane showed that C(2′)-endo dGpdC has one low-energy valley. It is in the B-form helical region (ω′ ～ 260°, ω ～ 300). When the sugar pucker is C(3′)-endo, dGpdC has two low-energy regions: the A-form helical region and the region with the minimum at ω′ = 16°, ω = 85°.     

Molecular mechanics studies of parallel and antiparallel phosphate-methylated DNA

Methylation of phosphate groups in oligo-dT strands leads to a parallel duplex with T · T base pairs. Molecular mechanics calculations on parallel d(TTTTTT)₂ show it to be a symmetric right-handed helix with B-DNA conformational characteristics. Phosphate methylation stabilizes the duplex by ca. 41 kcal/mol, due to removal of the interstrand phosphate electrostatic repulsions. The chirality introduced with phosphate methylation is important for the molecular geometry, since R_P methylation predominantly influences the conformation around the ζ bond (P? O_3′), while S_P methylation mostly changes the α conformation (P? O_5′). This is also true in antiparallel helices with methylated phosphates, as is shown by molecular mechanics calculations on d(GCGCGC)₂. These results may be of relevance to protein–DNA interactions, where phosphate charges are also shielded. As the pro-S_P oxygen is most available in a right-handed helix, we suggest changes around the α bond to occur upon protein complexation, leading to a widening of the major groove in the d(GCGCGC)₂ duplex (from 12 to 13 Å) and reduced minor groove (from 6 to 5 Å).     

Parallel nucleic acid helices with hoogsteen base pairing: Symmetry and structure

Molecular structures for parallel DNA and RNA double helices with Hoogsteen pairing are proposed for the first time. The DNA helices have sugars in the C2′-endo region and the phosphodiester conformations are (trans, gauche^?), and the RNA helices have sugars in the C3′-endo region and the phosphodiester conformations are (gauche^?, gauche^?). A pseudorotational symmetry relates the two parallel strands of DNA helices and a screw symmetry relates the two strands of RNA helices, which have an associated tilt of the The conformational space of parallel helices with Hoogsteen base pairing, unlike the Watson-Crick duplex, is highly restricted due to the unique positioning of the symmetry axis in the former case. The features of the parallel double helix with Hoogsteen pairing are compared with the Watson-Crick duplex and the corresponding triple helix. © 1994 John Wiley & Sons, Inc.     

RNase H mediated cleavage of RNA by cyclohexene nucleic acid (CeNA)

Cyclohexene nucleic acid (CeNA) forms a duplex with RNA that is more stable than a DNA–RNA duplex (ΔT_m per modification: +2°C). A cyclohexenyl A nucleotide adopts a 3′-endo conformation when introduced in dsDNA. The neighbouring deoxynucleotide adopts an O4′-endo conformation. The CeNA:RNA duplex is cleaved by RNase H. The V_max and K_m of the cleavage reaction for CeNA:RNA and DNA:RNA is in the same range, although the k_cat value is about 600 times lower in the case of CeNA:RNA.     

Polarized Raman scattering from oriented single microcrystals of d(A5T5)2 and d(pTpT)

Polarized Raman spectra have been obtained from single microcrystals of the duplex of the decamer d(A₅T₅)₂ using a Raman microscope. This is the first report of Raman spectra from a crystal of a deoxyoligomer that contains only long, nonalternating sequences of adenine and thymine. Sequences containing d(A)_n and d(T)_n are of interest in view of recent suggestions that they induce bends in DNA and that they might exist in a nonstandard B-conformation. Polarized Raman spectra of a crystal of d(pTpT) have also been obtained. Both crystals display Raman bands whose intensities are very sensitive to the orientation of the crystal with respect to the direction of polarization of the incident laser beam. These spectra indicate that the helical axes of the oligonucleotides are parallel to the long axes of the crystals and that the d(A₅T₅)₂ is not appreciably bent in the crystal. The Raman spectrum from the d(pTpT) crystal indicates that all of the furanose ring puckers are in a C2′-endo configuration since only the C2′-endo marker band at 835 ± 5 cm^?1 is present. Crystals of d(A₅T₅)₂ show measurable Raman intensities in both the 838- and 816-cm^?1 bands. This indicates the presence of both the C2′-endo and C3′-endo, or possibly other non-C2′-endo, furanose conformations. The 816-cm^?1 band is weak so that only a small fraction of the residues are estimated to be in the non-C2′-endo conformation. In both the d(pTpT) and d(A₅T₅)₂ crystals the intensity of the bands due to vibrations of the backbone show only a small dependence on orientation of the crystals. This result is explained by the low symmetry of the puckered sugar rings. It is concluded that Raman spectra obtained from oligonucleotide crystals in which the orientation of the crystal axes to the laser polarization is not carefully controlled may contain intensity artifacts that are due to polarization effects.     

Structures for the polynucleotide complexes poly(dA) · poly(dT) and poly(dT) · poly(dA) · poly(dT)

X-ray diffraction analyses of fibers of polydeoxyadenylic acid · polydeoxythymidylic acid show that this molecule exists as a 10-fold double-helix with axial rise per nucleotide $\text{h = 3.24}\text{to}\text{3.29}\text{A}\text{?}$. The structure is very similar to B-DNA ($\text{h = 3.37}\text{A}\text{?}$) in having C3-exo furanose rings and base-pairs positioned centrally on the helix axis, but distinctive enough to have two packing modes, neither of which has been observed for B-DNA. Although the triple-stranded poly(dT) · poly(dA) · poly(dT) also has a large value of h(3.26 Å), each of the chains is a 12-fold helix of the A-genus with C3-endo furanose rings and bases displaced several Angstrom units from the helix axis.     

Solvent-accessible surfaces of nucleic acids

Static solvent-accessible surface areas were calculated for DNA and RNA double helices of varied conformation, composition and sequence, for the single helix of poly(rC), and for a transfer RNA. The results show that for DNA and RNA double helices, two thirds of the water-accessible surface area become buried on double helix formation; phosphate oxygens retain near maximal exposure while the bases are 80% buried. Transfer RNA exposes slightly less surface per residue than does double-helical RNA, despite the presence of several additional “modified” groups, all of which are exposed significantly.When a probe corresponding to a single water molecule is used, both the total and atom type exposures are very similar for A-DNA and B-DNA, although marked differences appear in the major and minor groove exposures between the two conformations. For a given base-pair, the accessible surface area buried upon double-helical stacking is nearly constant (within 5%) for different sequences of neighboring base-pairs.For probes larger than single water molecules, there exist considerable differences in the total and atom type exposures of A-DNA and B-DNA. Conformational transitions between the A-DNA and B-DNA helical forms can thus be related to differences in the accessible areas for “structured” water, or a secondary hydration shell, rather than to interactions with individual water molecules of the primary hydration shell. The base-composition dependence of DNA helical conformation can be explained in terms of the opposing effects of thymine methyl groups of A · T base-pairs and the amino groups of G · C base-pairs upon the solvent within the grooves.The area calculations show that primarily the major groove of B-DNA and the minor groove of A-DNA have sufficient accessible surface area to be recognized by a probe size corresponding to the side-chains of amino acids.     

Structure of the RNA in tobacco mosaic virus

A model of the RNA of tobacco mosaic virus has been built using computer model-building techniques. The model has good stereochemistry, and fits the electron density map of the virus obtained by fiber diffraction methods considerably better than did earlier models. The three sugar rings in the asymmetric unit all have the A (3′-endo) conformation, One of the bases is in the syn conformation, a conformation observed only rarely in nucleic acid structures.     

Synthesis of the Oligoribonucleotides Incorporating 8-Oxo-Guanosine and Evaluation of their Base Pairing Properties

6-O-7-N-Bis(diphenylcarbamoyl)-2-N-phenoxyacetyl-5′-O-dimethoxytrityl-2′-O-{[(triisopropyl- silyl)oxy]methyl}-8-oxoguanosine-3′-yl-β-cyanoethyl-N,N-diisopropylphosphoramidite (5) was synt- hesized as a new phosphoramidite precursor unit for the synthesis of RNA. Compound 5 was successfully incorporated into the middle of the RNA sequences, and the synthesized RNAs were identified by MALDI-TOF mass measurements. Their properties were evaluated for formation of the RNA duplex and RNA/DNA heteroduplex. ORNs 1 and 4 containing 8-oxo-G can form base pairs with rC or dC in an anti conformation, while it can also interact with rA or dA in a syn conformation in the RNA duplex or RNA/DNA heteroduplex. The described synthetic method is therefore a useful procedure for the synthesis of ORN containing 8-oxo-G and contributes to the study of 8-oxo-G in RNA.     

Alternate g−g−. conformation for dinucleoside phosphates in solution

An alternative g^?g^? conformation (conformer I') for dinucleosides in solution has been deduced, based on potential energy calculations and nuclear magnetic resonance spectroscopy. This conformation is characterized by larger glycosidic torsional angles (X=94–111°) than those of conformer 1 (X=8–35°), although the other torsional angles are similar. There are thus four stable confonners (I, I', II and III) for dinucleosides in equilibrium with the open forms. The structure of conformer I' supports that of the ‘vertical’ double helix constructed by Olson (W.K. Olson. Proc. Natl. Acad. Sci. U.S.A. 74, (1977) 1775). Our data may suggest the possibility of interconversion between the vertical double helix and the regular double helix of A-form DNA, RNA or A'-form RNA.     

Conformations of cyclic 2,3-nucleotides and 2,3-Cyclic-5-diphosphates. Interrelation between the phase angle of pseudorotation of the sugar and the torsions about the glycosyl C(1)-N and the backbone C(4)-C(5) bonds

Semiempirical potential energy calculations have been carried out for cyclic 2′,3′-nucleotides and their 5′-phosphorylated derivatives, which are the intermediates in the hydrolysis of RNA. Calculations have been performed for both purine and pyrimidine bases for the observed O(1′)-endo, O(1′)-exo and the unpuckered planar sugar ring conformations. It is found that the mode of sugar pucker largely determines the preferred conformations of these molecules. For cyclic 2′,3′-nucleotides themselves, the O(1′)-endo sugars show a preference for the syn glycosyl conformation while the O(1′)-exo sugars exclusively favor the anti conformation regardless of whether the base is a purine or pyrimidine. For the unpuckered planar sugar, the syn conformation is favored for purines and anti for pyrimidines. Both the gauche (+) (60°) and trans (180°) conformations about the C(4′)? C(5′) bond are favored for O(1′)-endo sugars, while the gauche (?) (300°) and trans (180°) are favored for O(1′)-exo sugars. On the contrary, the 5′-phosphorylated cyclic 2′,3′-nucleotides of both purines and pyrimidines show a preference for the anti-gauche (+) conformational combination about the glycosyl and C(4′)? C(5′) bonds for the O(1′)-endo sugars and the anti-trans combination for the O(1′)-exo sugars. The correlation between the phase angle of the sugar ring and the favored torsions about the glycosyl and the backbone C(4′)? C(5′) bonds as one traverses along the pseudorotational pathway of the sugar ring is examined.     

Visualization of drug-nucleic acid interactions at atomic resolution. IV. Structure of an aminoacridine--dinucleoside monophosphate crystalline complex, 9-aminoacridine--5-iodocytidylyl (3'--5') guanosine

9-Aminoacridine forms a crystalline complex with the dinucleoside monophosphate, 5-iodocytidylyl(3′–5′)guanosine (iodoCpG). These crystals are monoclinic, space group P2₁ with $\text{a = 13.98}\text{A}\text{?}\text{, b = 30.58}\text{A}\text{?}\text{, c = 22.47}\text{A}\text{?}$ and β = 113.9 °. The structure has been solved to atomic resolution by Patterson and Fourier methods, and refined by a combination of Fourier and sum-function Fourier methods. The asymmetric unit contains four 9-aminoacridine molecules, four iodoCpG molecules and 21 water molecules, a total of 245 atoms. 9-Aminoacridine demonstrates two different intercalative binding modes and, along with these, two slightly different intercalative geometries in this model system.The first of these is very nearly symmetric, the 9-amino group lying in the narrow groove of the intercalated base-paired nucleotide structure. The second shows grossly asymmetric binding to the dinucleotide, the 9-amino group lying in the wide groove of the structure. Associated with these two different intercalative binding modes is a difference in geometries in the structures. Although both structures demonstrate C3′ endo (3′–5′) C2′ endo mixed sugar puckering patterns (i.e. both cytidine residues have C3′ endo sugar conformations, while both guanosine residues have C2′ endo sugar conformations), with corresponding twist angles between base-pairs of about 10 °, they differ in the magnitude of the helical screw axis dislocation accompanying intercalation (Sobell et al., 1977a,b). In the pseudosymmetric intercalative structure, this value is about +0.5 Å, whereas in the asymmetric intercalative structure this value is about +2.7 Å. These conformational differences can be best described as a “sliding” of base-pairs on the intercalated acridine molecule.Although the pseudosymmetric intercalative structure can be used in 9-aminoacridine-DNA binding, the asymmetric intercalative structure cannot since this poses stereochemical difficulties in connecting neighboring sugar-phosphate chains to the intercalated dinucleotide. It is possible, however, that the asymmetric binding mode is related to the mechanism of 9-aminoacridine-induced frameshift mutagenesis (Sakore et al., 1977), and we discuss this possibility here in further detail.     

Examination by the molecular orbital method of the intrinsic conformation preferences of nucleic acid sequence]

This paper reports a systematic PCILO study of the conformation of the nucleic acid backbone. The authors principally studied the ω′ and ω phosphodiester torsion angles of the disugar triphosphate model as a simultaneous function of (1) the sugar nature, ribose or deoxyribose, (2) the different combinations of the sugar ring puckers C(2′)-endo-C(2′)-endo, C(3′)-endo-C(3′)-endo, C(3′)-endo-C(2′)-endo, and C(2′)-endo-C(3′)-endo, and (3) the different conformations around the ψ(C4′–C5′) exocyclic bond. The dependence of the (ω′,ω) conformational energy maps upon these different factors, is discussed. The results are in very good agreement with the observed structures of ribonucleic (RNA10, RNA11, A′-RNA12, tRNA^Phe) and deoxyribonucleic acids (D-DNA, C-DNA 9.3, B-DNA 10, A-DNA 11). Thus the validity of this model, the disugar triphosphate unit, is ensured. The main conclusions that can be drawn from this systematic study are the following:

• 1 The torsion around P-05′ (angle ω) is, as a general rule, more flexible than the torsion around P-03′ (angle ω′).
• 2 There is no notable difference between the ribose–triphosphate units and the deoxyribose–triphosphate units for the C(3′)-endo–C(3′)-endo and C(3′)-endo–C(2′)-endo sugar puckers.
• 3 The deoxyribose–triphosphate units with C(2′)-endo–C(2′)-endo and C(2′)-endo–C(3′)-endo sugar puckers show much more ω′ flexibility than the ribose–triphosphate units with the same sugar puckers and cis position for the 2′hydroxyl group.
• 4 The preferred values of ω′ are independent of the sugar nature (ribose or deoxyribose) and of ψ values; they are correlated with the sugar pucker of the first sugar-phosphate unit:
  • C(3′)-endo-C(3′)-endo and C(3′)-endo-C(2′)-endo puckers ? ω′ ? 240° (g^? region)
  • C(2′)-endo-C(2′)-endo and C(2′)-endo-C(3′)-endo puckers ? ω′ 180° (t region)
• 5 The preferred values of ω are independent of the nature and the puckering of the sugars; they are correlated with the rotational state of the torsion angle ψ(C4′–C5′): ψ ? 60° (gg) ? ω ? 300° (g^?), ψ ? 180° (gt) or 300° (tg) ? ω ? 60° (g⁺)

     

Conformational analysis of the 2'-deoxyribofuranose ring from proton-proton coupling constants: analysis of a nucleoside-carcinogen adduct formed from 2-acetylaminofluorene utilizing a three-state model

The conformation of the sugar moiety of 8-(N-fluoren-2-ylamino)-2′-deoxyguanosine in solution has been examined as a function of temperature by ¹H-nmr spectroscopy. Analysis of coupling constants shows that lowering the temperature to ?50°C in methanol shifts the conformational equilibrium of the sugar ring resulting in a C2′-endo conformation at a mole fraction of 0.97. The computed phase angle of pseudorotation and amplitude of pucker are 154° and 36°, respectively, with very little discrepancy between the five calculated coupling constants and coupling constants extrapolated from the temperature profiles. A computer program has been written enabling a three-state best-fit analysis. The three-state analysis indicates an equilibrium between C2′-endo, C3′-endo, and 04′-endo conformations. In aqueous solution, the computed mole fraction of the 04′-endo form is 0.18 at 30°C. The conformation associated with the sugar ring and the C4′? C5′ bond is compared to that of 2′-deoxyguanosine.     

The Solution Structure of a Locked Nucleic Acid (LNA) Hybridized to DNA

Abstract

LNA (Locked Nucleic Acids) is a novel oligonucleotide analogue containing a conformationally restricted nucleotide with a 2′-0, 4′-C-methylene bridge that induces unprecedented thermal affinities when mixed with complementary single stranded DNA and RNA. We have used two-dimensional'H NMR spectroscopy obtained at 750 and 500 MHz to determine a high resolution solution structure of an LNA oligonucleotide hybridized to the complementary DNA strand. The determination of the structure was based on a complete relaxation matrix analysis of the NOESY cross peaks followed by restrained molecular dynamics calculations. Forty final structures were generated for the duplex from A-type and B-type dsDNA starting structures. The root-mean-square deviation (RMSD) of the coordinates for the forty structures of the complex was 0.32Å. The structures were analysed by use of calculated helix parameters. This showed that the values for rise and buckle in the LNA duplex is markedly different from canonical B-DNA at the modification site. A value of twist similar to A-DNA is also observed at the modification site. The overall length of the helix which is 27.3Å. The average twist over the sequence are 35.9° ± 0.3°. Consequently, the modification does not cause the helix to unwind. The bis-intercalation of the thiazole orange dye TOTO to the LNA duplex was also investigated by ¹H NMR spectroscopy to sense the structural change from the unmodified oligonucleotide. We observed that the bis-intercalation of TOTO is much less favourable in the 5′-CT^LAG-3′ site than in the unmodified 5′-CT^LAG-3′ site. This was related to the change in the base stacking of the LNA duplex compared to the unmodified duplex.     

Molecular dynamics simulations of xDNA

xDNA is a modified DNA, which contains natural as well as expanded bases. Expanded bases are generated by the addition of a benzene spacer to the natural bases. A set of AMBER force‐field parameters were derived for the expanded bases and the structural dynamics of the xDNA decamer ( xT5 ′ G xT A xC xG C xA xG T3′ ) · ( xA5′ C T xG C G xT A xC A3′) was explored using a 22 ns molecular dynamics simulation in explicit solvent. During the simulation, the duplex retained its Watson‐Crick base‐pairing and double helical structure, with deviations from the starting B‐form geometry towards A‐form; the deviations are mainly in the backbone torsion angles and in the helical parameters. The sugar pucker of the residues were distributed among a variety of modes; C2′ endo, C1′ exo, O4′ endo, C4′ exo, C2′ exo, and C3′ endo. The enhanced stacking interactions on account of the modification in the bases could help to retain the duplex nature of the helix with minor deviations from the ideal geometry. In our simulation, the xDNA showed a reduced minor groove width and an enlarged major groove width in comparison with the NMR structure. Both the grooves are larger than that of standard B‐DNA, but major groove width is larger than that of A‐DNA with almost equal minor groove width. The enlarged groove widths and the possibility of additional hydration in the grooves makes xDNA a potential molecule for various applications. © 2009 Wiley Periodicals, Inc. Biopolymers 91: 351–360, 2009. This article was originally published online as an accepted preprint. The “Published Online” date corresponds to the preprint version. You can request a copy of the preprint by emailing the Biopolymers editorial office at biopolymers@wiley.com     

Comparative analysis of inosine-substituted duplex DNA by circular dichroism and X-ray crystallography

Leveraging structural biology tools, we report the results of experiments seeking to determine if the different mechanical properties of DNA polymers with base analog substitutions can be attributed, at least in part, to induced changes from classical B-form DNA. The underlying hypothesis is that different inherent bending and twisting flexibilities may characterize non-canonical B-DNA, so that it is inappropriate to interpret mechanical changes caused by base analog substitution as resulting simply from ‘electrostatic’ or ‘base stacking’ influences without considering the larger context of altered helical geometry. Circular dichroism spectra of inosine-substituted oligonucleotides and longer base-substituted DNAs in solution indicated non-canonical helical conformations, with the degree of deviation from a standard B-form geometry depending on the number of I?C pairs. X-ray diffraction of a highly inosine-substituted DNA decamer crystal (eight I?C and two A?T pairs) revealed an A-tract-like conformation with a uniformly narrow minor groove, reduced helical rise, and the majority of sugars adopting a C1′-exo (southeastern) conformation. This contrasts with the standard B-DNA geometry with C2′-endo sugar puckers (south conformation). In contrast, the crystal structure of a decamer with only four I?C pairs has a geometry similar to that of the reference duplex with eight G?C and two A?T pairs. The unique crystal geometry of the inosine-rich duplex is noteworthy given its unusual CD signature in solution and the altered mechanical properties of some inosine-containing DNAs.     

The crystal structure of the RNA/DNA hybrid r(GAAGAGAAGC). d(GCTTCTCTTC) shows significant differences to that found in solution.

The crystal structure of the RNA/DNA hybrid r(GAAGAGAAGC). d(GCTTCTCTTC) has been solved and refined at 2.5 A resolution. The refinement procedure converged at R = 0.181 for all reflections in the range 20.0-2.5 A. In the crystal, the RNA/DNA hybrid duplex has an A' conformation with all but one of the nucleotide sugar moieties adopting a C3'- endo (N) conformation. Both strands in the double helix adopt a global conformation close to the A-form and the width of the minor groove is typical of that found in the crystal structures of other A-form duplexes. However, differences are observed between the RNA and DNA strands that make up the hybrid at the local level. In the central portion of the duplex, the RNA strand has backbone alpha, beta and gamma torsion angles that alternate between the normal gauche -/ trans / gauche + conformation and an unusual trans / trans / trans conformation. Coupled with this so-called 'alpha/gamma flipping' of the backbone torsion angles, the distance between adjacent phosphorous atoms on the RNA strand systematically varies. Neither of these phenomena are observed on the DNA strand. The structure of the RNA/DNA hybrid presented here differs significantly from that found in solution for this and other sequences. Possible reasons for these differences and their implications for the current model of RNase H activity are discussed.