The residence time of the bound water in the hydrophobic minor groove of the carbocyclic-nucleoside analogs of Dickerson-Drew dodecamers

The residence time of the bound water molecules in the antisense oligodeoxyribonucleotides containing 7'-alpha-methyl (TMe) carbocyclic thymidines in duplex (I), d5'(1C2G3C4G5A6A7TMc8TMe9C10G11C12G)23', and 6'-alpha-hydroxy (TOH) carbocyclic thymidines in duplex (II), d5'(1C2G3C4G5AOH6AOH7TOH8 TOH9C10G11C12G)2(3), have been investigated using a combination of NOESY and ROESY experiments. Because of the presence of 7'-alpha-methyl groups of TMe in the centre of the minor groove in duplex (I), the residence time of the bound water molecule is shorter than 0.3 ns. The dramatic reduction of the residence time of the water molecule in the minor groove in duplex (I) compared with the natural counterpart has been attributed to the replacement of second shell of hydration and disruption of hydrogen-bonding with 04' in the minor groove by hydrophobic alpha-methyl groups, as originally observed in the X-ray study. This effect could not be attributed to the change of the width of the minor groove because a comparative NMR study of the duplex (I) and its natural counterpart showed that the widths of their minor grooves are more or less unchanged (r.m.s.d change in the core part is <0.63A). For duplex (II) with polar 6'-alpha-hydroxyl groups pointed to the minor groove, the correlation time is much longer than 0.36 ns as a result of the stabilising hydrogen-bonding interaction with N3 or 02 of the neighbouring nucleotides.     

Elucidation of the Origin of NOEs And ROEs that Show the Hydration in the Minor and Major Grooves of DNA Duplex with ATTAAT Tract by a Combination of NOESY and ROESY Experiments

Abstract

A combination of NOESY and ROESY experiments (using ammonia as a catalyst across the pH range of 5 to 8.6) has given us a clear understanding regarding the origin of nOes that are attributed to the stereochemical location and the residence time of water in the major and the minor grooves of d⁵'(¹C²C³A⁴T⁵T⁶A⁷A⁸T⁹G¹⁰G)₂ ³' duplex Our conclusions are the following: (i) In the major groove, the presence of ammonia in the buffer does not influence on the process of exchange between bound and bulk water, (ii) It has been found that the observation of the bound water in the minor groove is a result of straight dipole-dipole effect at the physiological pH. (iii) The residence time of water near H2 of adenine (H2A) in the minor groove has been estimated to be in the range of 0.3–0.5ns, which is closer to the residence time of the bound water found on the surface of protein, (iv) The hydration pattern in the minor groove in the physiological pH, under our NMR measurement condition, is similar to the ones found in the X-ray structure, (v) It has been shown that at pH > 8.0 the nOe/rOe intensities of the water-H2A crosspeaks dramatically increase due to dipole-dipole and/or relayed magnetization transfer from H2A to water through ammonia catalyst.     

Base-pair exchange kinetics of the imino and amino protons of the 3′-phenazinium tethered DNA-RNA duplex,r(5′GAUUGAA3′):d(5′TCAATC3′-Pzn), and their comparison with those of B-DNA duplex

The dynamics of the opening-closing of the constituent base-pairs as well as of the exchange kinetics of the base-paired imino and amino protons with water in a DNA-RNA hybrid, [^5′r(G¹A²U³U⁴G⁵A⁶A⁷)^3′]:^5′p[d(T⁸C⁹A¹⁰A¹¹T¹²C¹³)]^3′-Pzn] duplex (I), are reported here in details for the first time. The exchange kinetics of amino and imino protons in the DNA-RNA hybrid (duplex I) have been compared with identical studies on the following B-DNA duplexes: d(C¹G²T³A⁴C⁵G⁶)₂ (II), d[p(^5′T¹G²T³T⁴T⁵G⁶ G⁷C⁸)^3′]:d[p(^5′C⁹C¹⁰A¹¹A¹²A¹³C¹⁴A¹⁵)^3′] (III), d(C⁵G⁶C⁷G⁸A⁹A¹⁰T¹¹T¹²C¹³G¹⁴C¹⁵G¹⁶)₂ (IV) and d(C¹G²C³G⁴C⁵G⁶C⁷G⁸A⁹A¹⁰T¹¹T¹²C¹³G¹⁴C¹⁵G¹⁶C¹⁷G¹⁸C¹⁹G²⁰)₂ (V). This comparative study shows that the life-times τ_o of various base-pairs in the DNA-RNA hybrid (I) varies in the range of ∼ 1 ms, and they are quite comparable to those of the shorter B-DNA duplexes (II) and (III), but very different from the τ_o of the larger duplexes (IV) and (V): the τ_o for the base pair of T¹¹ and T¹² residues in the 20-mer (duplex V) are 2.9 ± 2.3 ms and 23.2 ± 8.9 ms, respectively, while the corresponding τ_o in the 12-mer (duplex IV) are 2.8 ± 2.2 ms and 17.4 ± 5.4 ms. It has also been shown that the total energy of activation (E_a) assessed from the exchange rates of both imino and amino protons, representing energetic contributions from both base-pair and helix opening-closing as well as from the exchange process of the imino protons from the open state with the bound water, is close to the E_a of the short B-DNA duplex (E_a ≈ 28–47 kcal/mol).     

Molecular Structure of the Core-Modified siRNA Duplexes Containing Diastereomeric Pair of [C6′(R)-OH]- versus [C6′(S)-OH]-carba-LNAs Suggests a Model for RNAi Action

Molecular structures of native and a pair of modified small interfering RNA–RNA duplexes containing carbocyclic [6 ′-(R)-OH/7 ′-(S)-methyl]- and [6 ′-(S)-OH/7 ′-(S)-methyl]-carba-LNA-thymine nucleotides, which are two diastereomeric analogs of the native T nucleotide, incorporated at position 13 in the antisense (AS) strand of siRNA, have been simulated using molecular mechanics/dynamics techniques. The main aim of the project has been to find a plausible structural explanation of why modification of siRNA at T¹³ position by the [6 ′(R)-O-(p-Toluoyl)-7 ′(S)-methyl]-carba-LNA-Thymine [IC₅₀ of 3.32 ± 0.17 nM] is ca 24 times more active as an RNA silencing agent against the target HIV-1 TAR RNA than the [6 ′(S)-O-(p-Toluoyl)-7 ′(S)-methyl]-counterpart [IC₅₀ of 79.8 ± 17 nM] [1]. The simulations reveal that introduction of both C6 ′(R)-OH and C6 ′(S)-OH stereoisomers does not lead even to local perturbation of the siRNA–RNA duplex structures compared to the native, and the only significant difference between 6 ′(S)- and 6 ′(R)-diastereomers found is the exposure of the 6 ′-OH group of the 6 ′(R)-diastereoisomer toward the edge of the duplex while the 6 ′-hydroxyl group of the 6 ′(S)-diastereoisomer is somewhat buried in the minor groove of the duplex. This rules out a hypothesis about any possible local distortion by the nature of chemical modification of the siRNA-target the RNA duplex, which might have influenced the formation of the effective RNA silencing complex (RISC) and puts some weight on the hypothesis about the 6 ′-hydroxy group being directly involved with most probably Ago protein, since it is known from exhaustive X-ray studies [2, 3] that the core residues are indeed involved with hydrogen bonding with the internucleotidyl phosphates. Further systematic investigation is in progress to map the position-dependent functional and nonfunctional interactions of the modified [6 ′(R or S)-O-(p-Toluoyl)-7 ′(S)-methyl]-carba-LNA-T with the Ago2 protein of the RISC.     

A Single Carbocyclic Nucleotide Substitution in a 12mer DNA Gives a Hoogsteen Basepaired Duplex (Till 38°C) and a Hairpin (Till 65°C). A 600 MHz NMR Spectroscopic Study

Abstract

The impact of intramolecular stereoelectronic effects has been examined by comparison of the solution structures of natural oligo-DNA duplex, 5′(¹C²G³C⁴G⁵A⁶A⁷T⁸T⁹C¹⁰G¹¹C¹²G)₂ ³′, and its carbocyclic-nucleotide analogues in which the pentose sugar in 2′-dA residue is replaced with its carbocyclic counterpart (i.e. 2′-deoxyaristeromycin). Based on the NMR evidences, it has been shown, that 2′-deoxyaristeromycin analog exists in a dynamic equilibrium between the two forms of duplexes, one with W-C bp and the second with Hoogsteen bp in ca 1:1 ratio at lower temperature (below 35°C) and as hairpin at higher temperature (from ～40° – 60°C).     

Role of DNA minor groove interactions in substrate recognition by the M.SinI and M.EcoRII DNA (cytosine-5) methyltransferases

The SinI and EcoRII DNA methyltransferases recognize sequences (GG^A/_TCC and CC^A/_TGG, respectively), which are characterized by an ^A/_T ambiguity. Recognition of the A·T and T·A base pair was studied by in vitro methyltransferase assays using oligonucleotide substrates containing a hypoxanthine·C base pair in the central position of the recognition sequence. Both enzymes methylated the substituted oligonucleotide with an efficiency that was comparable to methylation of the canonical substrate. These observations indicate that M.SinI and M.EcoRII discriminate between their canonical recognition site and the site containing a G·C or a C·G base pair in the center of the recognition sequence (GG^G/_CCC and CC^G/_CGG, respectively) by interaction(s) in the DNA minor groove. M.SinI mutants displaying a decreased capacity to discriminate between the GG^A/_TCC and GG^G/_CCC sequences were isolated by random mutagenesis and selection for the relaxed specificity phenotype. These mutations led to amino acid substitutions outside the variable region, previously thought to be the sole determinant of sequence specificity. These observations indicate that ^A/_T versus ^G/_C discrimination is mediated by interactions between the large domain of the methyltransferase and the minor groove surface of the DNA.     

The First Example of a Hoogsteen Basepaired DNA Duplex in Dynamic Equilibrium with a Watson-Crick Basepaired Duplex—A Structural (NMR), Kinetic and Thermodynamic Study

Abstract

A single-point substitution of the O4′ oxygen by a CH₂ group at the sugar residue of A ⁶ (i.e. 2′-deoxyaristeromycin moiety) in a self-complementary DNA duplex, 5′- d(C¹G²C³G⁴A⁵A⁶T⁷T⁸C⁹G¹⁰C¹¹G¹²)₂ ^?3, has been shown to steer the fully Watson-Crick basepaired DNA duplex (1A), akin to the native counterpart, to a doubly A ⁶:T⁷ Hoogsteen basepaired (1B) B-type DNA duplex, resulting in a dynamic equilibrium of (1A)→←(1B): K_eq = k₁/k_-1 = 0.56±0.08. The dynamic conversion of the fully Watson-Crick basepaired (1A) to the partly Hoogsteen basepaired (1B) structure is marginally kinetically and thermodynamically disfavoured [k₁ (298K) = 3.9± 0.8 sec^?1; δH°? = 164±14 kJ/mol;-TδS°? (298K) = ?92 kJ/mol giving a δG₂₉₈°? of 72 kJ/mol. Ea (k1) = 167±14 kJ/mol] compared to the reverse conversion of the Hoogsteen (1B) to the Watson-Crick (1A) structure [k-1 (298K) = 7.0±0.6 sec-1, δH°? = 153±13 kJ/mol;-TδS°? (298K) = ?82 kJ/mol giving a δG₂₉₈°? of 71 kJ/mol. Ea (k-1) = 155±13 kJ/mol]. A comparison of δG₂₉₈°? of the forward (k1) and backward (k-1) conversions, (1A)→←(1B), shows that there is ca 1 kJ/mol preference for the Watson-Crick (1A) over the double Hoogsteen basepaired (1B) DNA duplex, thus giving an equilibrium ratio of almost 2:1 in favour of the fully Watson-Crick basepaired duplex. The chemical environments of the two interconverting DNA duplexes are very different as evident from their widely separated sets of chemical shifts connected by temperature-dependent exchange peaks in the NOESY and ROESY spectra. The fully Watson-Crick basepaired structure (1A) is based on a total of 127 intra, 97 inter and 17 cross-strand distance constraints per strand, whereas the double A ⁶:T⁷ Hoogsteen basepaired (1B) structure is based on 114 intra, 92 inter and 15 cross-strand distance constraints, giving an average of 22 and 20 NOE distance constraints per residue and strand, respectively. In addition, 55 NMR-derived backbone dihedral constraints per strand were used for both structures. The main effect of the Hoogsteen basepairs in (1B) on the overall structure is a narrowing of the minor groove and a corresponding widening of the major groove. The Hoogsteen basepairing at the central A ⁶:T⁷ basepairs in (1B) has enforced a syn conformation on the glycosyl torsion of the 2′- deoxyaristeromycin moiety, A ⁶, as a result of substitution of the endocyclic 4′-oxygen in the natural sugar with a methylene group in A ⁶. A comparison of the Watson-Crick basepaired duplex (1A) to the Hoogsteen basepaired duplex (1B) shows that only a few changes, mainly in α, σ and γ torsions, in the sugar-phosphate backbone seem to be necessary to accommodate the Hoogsteen basepair.     

Structure-specific binding of [Co(phen)2(HPIP)] to a DNA duplex containing sheared G:A mismatch base pairs

The binding of a Co(III) complex to the decanucleotide d(CCGAATGAGG)₂ containing two pairs of G:A mismatches was studied by 2D-NMR, UV absorption, and molecular modeling. NMR investigations indicate that racemic [Co(phen)₂(HPIP)]Cl₃ [HPIP = 2-(2-hydroxyphenyl) imidazo [4,5-f][1,10] phenanthroline] binds the decanucleotide by intercalation: the HPIP ligand selectively inserts between the stacked bases from the minor groove at the terminal regions and from the major groove at the sheared region. Further, molecular modeling revealed that the recognition shows strong enantioselectivity: the Λ-isomer preferentially intercalates into the T₆G₇:A₅A₄ region from the DNA major groove, while Δ-isomer favors the terminal C₁C₂:G₁₀G₉ region and intercalates from the minor groove. Detailed energy analysis suggests that the steric interaction, especially the electrostatic effect, is the primary determinants of the recognition event. Melting experiments indicate that binding stabilizes the DNA duplex and increases the melting temperature by 9.5 °C. The intrinsic binding constant of the complex to the mismatched duplex was determined to be 3.5 × 105 M⁻¹.     

Shape readout of AT‐rich DNA by carbohydrates

Gene expression can be altered by small molecules that target DNA; sequence as well as shape selectivities are both extremely important for DNA recognition by intercalating and groove‐binding ligands. We have characterized a carbohydrate scaffold (1) exhibiting DNA “shape readout” properties. Thermodynamic studies with 1 and model duplex DNAs demonstrate the molecule's high affinity and selectivity towards B* form (continuous AT‐rich) DNA. Isothermal titration calorimetry (ITC), circular dichroism (CD) titration, ultraviolet (UV) thermal denaturation, and Differential Scanning Calorimetry were used to characterize the binding of 1 with a B* form AT‐rich DNA duplex d[5′‐G₂A₆T₆C₂‐3′]. The binding constant was determined using ITC at various temperatures, salt concentrations, and pH. ITC titrations were fit using a two‐binding site model. The first binding event was shown to have a 1:1 binding stoichiometry and was predominantly entropy‐driven with a binding constant of approximately 10⁸ M^?1. ITC‐derived binding enthalpies were used to obtain the binding‐induced change in heat capacity (ΔC_p) of ?225 ± 19 cal/mol·K. The ionic strength dependence of the binding constant indicated a significant electrolytic contribution in ligand:DNA binding, with approximately four to five ion pairs involved in binding. Ligand 1 displayed a significantly higher affinity towards AT‐tract DNA over sequences containing GC inserts, and binding experiments revealed the order of binding affinity for 1 with DNA duplexes: contiguous B* form AT‐rich DNA (d[5′‐G₂A₆T₆C₂‐3′]) >B form alternate AT‐rich DNA (d[5′‐G₂(AT)₆C_2‐3′]) > A form GC‐rich DNA (d[5′‐A₂G₆C₆T₂‐3′]), demonstrating the preference of ligand 1 for B* form DNA. © 2013 Wiley Periodicals, Inc. Biopolymers 101: 720–732, 2014.     

Crystal structure of d(GCGAAAGCT) containing a parallel-stranded duplex with homo base pairs and an anti-parallel duplex with Watson-Crick base pairs

A DNA fragment d(GCGAAAGCT), known to adopt a stable mini-hairpin structure in solution, has been crystallized in the space group I4₁22 with the unit-cell dimensions a = b = 53.4 Å and c = 54.0 Å, and the crystal structure has been determined at 2.5 Å resolution. The four nucleotide residues CGAA of the first half of the oligomer form a parallel duplex with another half through the homo base pairs, C₂:C₂⁺ (singly-protonated between the Watson– Crick sites), G₃:G₃ (between the minor groove sites), A₄:A₄ (between the major groove sites) and A₅:A₅ (between the Watson–Crick sites). The two strands remaining in the half of the parallel duplex are split away in different directions, and they pair in an anti-parallel B-form duplex with the second half extending from a neighboring parallel duplex, so that an infinite column is formed in a head-to-tail fashion along the c-axis. It seems that a hexa-ammine cobalt cation supports such a branched and bent conformation of the oligomer. One end of the parallel duplex is stacked on the corresponding end of the adjacent parallel duplex; between them, the guanine base of the first residue is stacked on the fourth ribose of another duplex.     

Synthesis of the Optically Active Carbocyclic Analogs of the Four 2′-Deoxyribonucleoside Monophosphates

Abstract

The (+)-enantiomer of the carbocyclic analogs of the four 2′-deoxyribonucleoside monophosphate constituents of DNA, C-dAMP² (1: A), C-dGMP (1: G), C-dCMP (1: C), and C-TMP (1: T) have been synthesized via the Mitsunobu coupling reaction. Two new N³-protected thymines were developed en route.     

Structural Basis of Stable Bending in DNA Containing An Tracts. Different Types of Bending

Abstract

Structural determinants of DNA bending of different types have been studied by theoretical conformational analysis of duplexes. Their terminal parts were fixed either in an ordinary low-energy B-like conformation or in “anomalous” conformations with a narrowed minor groove typical of A_n tracts. The anomalous conformations had different negative tilt angles (up to about zero), different propeller twists and minor groove widths. Calculations have been performed for DNA fragments A_nT_m, T_nA_m, A_nGCT_m, A_nCGT_m, T_mGCA_n, T_mCGA_n which are the models of the junction of two anomalous structures on A_n and T_m tracts. On the AT step of the A_nT_m fragment the minor groove can be easily narrowed so that a whole unbent fragment of anomalous structure is formed on A_n T_m. According to our energy estimates, there should not be any reliable bending on A_nT_m. In contrast, in all other cases there was a pronounced roll-like bending into the major groove in the chemical symmetry region. Calculations of the junction between the anomalous and ordinary B-like structure for G_nT_m and C_nA_m have shown that there is an equilibrium bending with a tilt component towards the chain having the anomalous structure at the 5′-end. From our calculations it is impossible to determine precisely the direction of bending, though it can be suggested that the roll component of bending might be directed towards the major groove. The anomalous structure is the main reason of bending; alternations of pyrimidines and purines can modulate the value and the direction of equilibrium bending (only the value in the case of self-complemantary fragments).

The results are consistent with the experimental data and promote a better understanding of the problem of DNA bending.     

Synthesis of 2H,13C-Labelled 2′-Deoxynucleosides and Their Site Specific Incorporation into Oligo-DNA for Structural Studies via Relaxation Time Measurements

Abstract

We have recently shown¹ the usefulness of ²H, ¹³C-labelled 2′-deoxynu-cleoside building blocks for structural studies via relaxation time measurements. The synthesis of phosphoramidite blocks 11 and 12 for their site-specific incorporation (indicated by underlines) into the d⁵′(¹C²G³ A ⁴ T ⁵ T ⁶ A ⁷ A ⁸ T ⁹C¹⁰G)₂ ³′ is briefly described for studying the T₁ and T_1[sgrave] relaxations of ²H and ¹³C at specific deuterated carbons in a large molecule.     

Sequence Specific Molecular Recognition and Binding of a Monocationic Bis-Imidazole Lexitropsin to the Decadeoxyribonucleotide d-[(GATCCGTATG) (CATACGGATC)]: Structural and Dynamic Aspects of Intermolecular Exchange Studied by 1H-NMR

Abstract

The non-exchangeable and imino proton NMR resonances of the non self-complementary decadeoxyribonucleotide d-[(GATCCGTATG) · (GATACGGATC)] as well as those of the 1:1 complex of the monocatonic bis-imidazole lexitropsin 1 to this sequence have been assigned by using a combination of NOE difference, COSY and NOESY techniques. Confirmation of complete annealing of the two non self-complementary decamer strands to give the duplex decadeoxyribonucleotide is obtained by the detection of ten imino protons. It is established that the sugar-base orientations of all the bases in the duplex decamer are anti. From NOE studies, it is concluded that the duplex oligomer is right-handed and adopts a conformation in solution that belongs to the B family. A population analysis reveals that the sugar moieties exist predominantly in the S-form (2′-endo-3′-exo). Addition of 1 to the DNA solution leads to doubling of the resonances for CH6(4,5), GH8(6), TH6(7) and T-CH₃(7). The base, anomeric H1′ and imino proton signals for the base sequence 5′-CCGT undergo the most marked drug-induced chemical shift changes. These results provide evidence that the lexitropsin is bound to the sequence 5′-CCGT in the minor groove of the DNA NOE measurements between the amide protons (NH1 and NH4) and the imino proton (IV and V) signals confirmed the location and orientation of 1 in the 1:1 complex, with the amino terminus oriented to C(4). The specific binding of 1 to the sequence 5′-CCGT-3′ deduced in this study is in agreement with the footprinting data obtained using the Hind III/Nci I fragment from pBR322 DNA [Kissinger et al. 1987 (13)]. Intramolecular NOEs observed between H4 and H9 of the lexitropsin suggest that the molecule is not planar, but subjected to propeller twisting, in both the free and bound forms. Furthermore, NOE measurements permit assignment of the DNA duplex in the 1:1 complex to the B-form, which is similar to that of the free DNA The [(T₇A₈T₉)· (A₁₂T₁₃A₁₄)] segment of the DNA shows better stacking, by propeller twisting, compared to the rest of the molecule in the free as well as the complex forms. The intermolecular rate of exchange of 1 between the equivalent 5′-CCGT sites, at a concentration of 12 mM, is estimated to be ～88s^?1 at 308°K with ΔG≠ of 63±5 K.J mol^?1.     

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

Abstract

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

Molecular Dynamics Simulation of 7, 8-dihydro-8-Oxoguanine DNA

Abstract

To elucidate the effect of guanine lesion produced by the oxidative damage on DNA, 1 nanosecond molecular dynamics simulations of native and oxidized DNA were performed. The target DNA molecules are dodecamer duplex d(CGCGAATTCGCG)2 and its derivative duplex d(C₁G₂C₃(8-oxoG)₄A₅A₆T₇T₈C₉G₁₀C₁₁G₁₂)·d(C₁₃G₁₄C₁₅G₁₆A₁₇A₁₈T₁₉T₂₀C21_G22C₂₃G₂₄), which has one oxidized guanine, 7, 8-dihydro-8-oxoguanine (8-oxoG), at the fourth position. The local structural change due to the lesion of 8-oxoG and the global dynamic structure of the 8-oxoG DNA were studied. It was found that the 8-oxoG DNA remained structurally stable during the simulation due to newly produced hydrogen bonds around the (8-oxoG)₄ residue. However, there were distinguishable differences in structural parameters and dynamic property in the 8-oxoG DNA. The conformation around the (8- oxoG)₄ residue departed from the usual conformation of native DNA and took an unique conformation of ?-ζ in B_II conformation and χ in high anti orientation at the (8-oxoG)₄ residue, and adopted a very low helical twist angle at the C₃:G₂₂—(8-oxoG)₄:C₂₁ step. Further analysis by principal component analysis indicated that the formation of the hydrogen bonds around the (8-oxoG)₄ residue plays a role as a trigger for the conformational transition of the 8-oxoG DNA in the conformational space.     

Enhanced uranyl photocleavage across the minor groove of all (A/T)4 sequences indicates a similar narrow minor groove conformation

The uranyl(VI)-mediated photocleavage of a Drew–Dickerson sequence oligonucleotide (5′-dGATCACGCGAATTCGCGT) either as the (self-complementary) duplex or cloned into the BamH1 site of pUC19 has been studied. At pH 6.5 in acetate buffer relatively enhanced photocleavage is observed at the 3′-end of the AATT sequence corresponding to maximum cleavage across the minor groove in the A/T tract. Thus maximum cleavage correlates with minimum minor groove width in the crystal structure and also with the largest electronegative potential according to computations. Using plasmid constructs with cloned inserts of the type [CGCG(A/T₄)]_n, we also analysed all possible sequence combinations of the (A/T)₄ tract and in all cases we observed maximum uranyl-mediated photocleavage across the minor groove in the (A/T)₄ tract without any significant differences between the various sequences. From these results we infer that DNA double helices of all (A/T)₄ sequences share the same narrow minor groove helix conformation.     

Recognition of O6-benzyl-2′-deoxyguanosine by a perimidinone-derived synthetic nucleoside: a DNA interstrand stacking interaction

The 2′-deoxynucleoside containing the synthetic base 1-[(2R,4S,5R)-4-hydroxy-5-(hydroxymethyl)-tetrahydrofuran-2-yl)-1H-perimidin-2(3H)-one] (dPer) recognizes in DNA the O⁶-benzyl-2′-deoxyguanosine nucleoside (O⁶-Bn-dG), formed by exposure to N-benzylmethylnitrosamine. Herein, we show how dPer distinguishes between O⁶-Bn-dG and dG in DNA. The structure of the modified Dickerson–Drew dodecamer (DDD) in which guanine at position G⁴ has been replaced by O⁶-Bn-dG and cytosine C⁹ has been replaced with dPer to form the modified O⁶-Bn-dG:dPer (DDD-XY) duplex [5′-d(C¹G²C³X⁴A⁵A⁶T⁷T⁸Y⁹G¹⁰C¹¹G¹²)-3′]₂ (X = O⁶-Bn-dG, Y = dPer) reveals that dPer intercalates into the duplex and adopts the syn conformation about the glycosyl bond. This provides a binding pocket that allows the benzyl group of O⁶-Bn-dG to intercalate between Per and thymine of the 3′-neighbor A:T base pair. Nuclear magnetic resonance data suggest that a similar intercalative recognition mechanism applies in this sequence in solution. However, in solution, the benzyl ring of O⁶-Bn-dG undergoes rotation on the nuclear magnetic resonance time scale. In contrast, the structure of the modified DDD in which cytosine at position C⁹ is replaced with dPer to form the dG:dPer (DDD-GY) [5′-d(C¹G²C³G⁴A⁵A⁶T⁷T⁸Y⁹G¹⁰C¹¹G¹²)-3′]₂ duplex (Y = dPer) reveals that dPer adopts the anti conformation about the glycosyl bond and forms a less stable wobble pairing interaction with guanine.     

trans-(NH3)2PtII-modified deoxyoligonucleotides as potential antisense agents: cross-linking reactions between two 12-mers

 An approach is presented which probes the possible use of trans-[(NH₃)₂PtCl]⁺-modified deoxyoligonucleotides in the antisense strategy. It consists of (1) the selective platination of an oligonucleotide containing 11 pyrimidine (T, C) bases as well as a single guanine (G) as a Pt-anchoring group at the 5′-end to give trans-[(NH₃)₂Pt{5′-d(G^N7T₂C₂T₂C₂T₂C}Cl]^10– 1 ("antisense strand") and (2) subsequent hybridization with the purine 12-mer 5′-d(GA₂G₂A₂G₂A₂G)^11– ("sense strand"). According to HPLC, three major species 2–4 are formed during reaction (2), all of which are cross-linking adducts between 1 and the sense strand, as confirmed by ESI MS and melting temperature measurements. Only for the major product 3 can a structure be proposed on the basis of 1D and 2D NMR spectra. According to these, G₁ of the antisense strand is cross-linked with G₂₀ via trans-(NH₃)₂Pt^II. The complementary overhangs of the duplex represent "sticky ends" and are, in principle, capable of associating into multimers of the duplex. Received: 29 March 1999 / Accepted: 26 July 1999