Intramolecular folding of a fragment of the cytosine-rich strand of telomeric DNA into an i-motif.

In the recently discovered i-motif, four stretches of cytosine form two parallel-stranded duplexes whose C.C+ base pairs are fully intercalated. The i-motif may be recognized by characteristic Overhauser cross-peaks of the proton NMR spectrum, reflecting short H1'-H1' distances across the minor groove, and short internucleotide amino-proton-H2'/H2" across the major groove. We report the observation of such cross-peaks in the spectra of a fragment of the C-rich telomeric strand of vertebrates, d[CCCTAA]3CCC. The spectra also demonstrate that the cytosines are base-paired and that proton exchange is very slow, as reported previously for the i-motif. From UV absorbance and gel chromatography measurements, we assign these properties to an i-motif which includes all or nearly all the cytosines, and which is formed by intramolecular folding at slightly acid or neutral pH. A fragment of telomeric DNA of Tetrahymena, d[CCCCAA]3CCCC, has the same properties. Hence four consecutive C stretches of a C-rich telomeric strand can fold into an i-motif. Hypothetically, this could occur in vivo.     

i-motif solution structure and dynamics of the d(AACCCC) and d(CCCCAA) tetrahymena telomeric repeats

Using NMR methods, we have resolved the i-motif structures formed by d(AACCCC) and by d(CCCCAA), two versions of the DNA sequence repeated in the telomeric regions of the C-rich strand of tetrahymena chromosomes. Both oligonucleotides form fully symmetrical i-motif tetramers built by intercalation of two hemiprotonated duplexes containing four C•C⁺ pairs. The structures are extremely stable. In the tetramer of d(AACCCC), the outermost C•C⁺ pairs are formed by the cytidines of the 5′ ends of the cytidine tracts. A2 forms an A2•A2 (H6trans–N7) pair stacked to C3•C3⁺ and cross-strand stacked to A1. At 0°C, the lifetimes of the hemiprotonated pairs range from 1 ms for the outermost pair to ~1 h for the innermost pairs. The tetramer of d(CCCCAA) adopts two distinct intercalation topologies in slow conformational exchange. One, whose outermost C•C⁺ pairs are built by the cytidines of the 5′ end and the other by those of the 3′ end. In both topologies, the adenosine bases are fairly well stacked to the adjacent C•C⁺ pairs. They are not paired but form symmetrical pseudo-pairs with their H6cis amino proton and N1 nitrogen pointing towards each other.     

Structure of a C-rich strand fragment of the human centromeric satellite III: a pH-dependent intercalation topology

Repetitive DNA sequences may adopt unusual pairing arrangements. At acid to neutral pH, cytidine-rich DNA oligodeoxynucleotides can form the i-motif structure in which two parallel-stranded duplexes with C.C(+) pairs are intercalated head-to-tail. The i-motif may be formed by multimeric associations or by intra-molecular folding, depending on the number of cytidine tracts, the nucleotide sequences between them, and the experimental conditions.We have found that a natural fragment of the human centromeric satellite III, d(CCATTCCATTCCTTTCC), can form two monomeric i-motif structures that differ in their intercalation topology and that are favored at pH values higher (the eta-form) and lower (the lambda-form) than 4.6. The change in intercalation may be related to adenine protonation in the loops.We studied the uridine derivative methylated on the first cytidine base, d(5mCCATTCCAUTCCUTTCC), whose proton spectrum is better resolved. The intercalation topologies are (C7.C17)/(5mC1.C11)/(C6.C16)/(C2.C12) for form lambda and (5mC1.C11)/(C7.C17)/(C2.C12)/(C6.C16) for form eta. We have solved the structure of the eta-form, and we present a model for the lambda-form. The switch from eta to lambda involves disruption of the i-motif. In both forms, the central AUT linker crosses the wide groove, and the first and the third linkers loop across the minor grooves. The i-motif core is extended in the eta-form by the inter-loop reverse Watson-Crick A3.U13 pair, whose dissociation constant is around 10(-2) at 0 degrees C, and in the lambda-form by the interloop T5.T15 pair.In contrast, d(5mCCATTCCTTACCTTTCC) folds into a pH-independent structure that has the same intercalation topology as the lambda-form. The i-motif core is extended below by the interloop T5.T15 pair and closed on top by the T8.A10 pair.Thus, the C-rich strand of the human satellite III tandem repeats, like the G-rich strand, can fold into various compact structures. The relevance of these features to centromeric function remains unknown.     

The RNA i-motif

Oligodeoxynucleotides with stretches of cytidine residues associate into a four-stranded structure, the i-motif, in which two head-to-tail, intercalated, parallel-stranded duplexes are held together by hemiprotonated C.C+ pairs. We have investigated the possibility of forming an i-motif structure with C-rich ribonucleic acids. The four C-rich RNAs studied, r(UC5), r(C5), r(C5U) and r(UC3), associate into multiple intercalated structures at acidic pH. r(UC5) forms two i-motif structures that differ by their intercalation topologies. We report on a structural study of the main form and we analyze the small conformational differences found by comparison with the DNA i-motif. The stacking topology of the main structure avoids one of the six 2'-OH/2'-OH repulsive contacts expected in a fully intercalated structure. The C3'-endo pucker of the RNA sugars and the orientation of the intercalated C.C+ pairs result in a modest widening of the narrow grooves at the steps where the hydroxyl groups are in close contact. The free energy of the RNA i-motif, on average -4 kJ mol(-1) per C.C+ pair, is half of the value found in DNA i-motif structures.     

Structure, internal motions and association-dissociation kinetics of the i-motif dimer of d(5mCCTCACTCC)

At slightly acidic pH, the association of two d(5mCCTCACTCC) strands results in the formation of an i-motif dimer. Using NMR methods, we investigated the structure of [d(5mCCTCACTCC)]₂, the internal motion of the base pairs stacked in the i-motif core, the dimer formation and dissociation kinetics versus pH. The excellent resolution of the ¹H and ³¹P spectra provided the determination of dihedral angles, which together with a large set of distance restraints, improve substantially the definition of the sugar-phosphate backbone by comparison with previous NMR studies of i-motif structures. [d(5mCCTCACTCC)]₂ is built by intercalation of two symmetrical hairpins held together by six symmetrical C•C⁺ pairs and by pair T7•T7. The hairpin loops that are formed by a single residue, A5, cross the narrow grooves on the same side of the i-motif core. The base pair intercalation order is C9•C9⁺/5mC1•5mC1⁺/C8•C8⁺/C2•C2⁺/T7.T7/C6•C6⁺/C4•C4⁺. The T3 bases are flipped out in the wide grooves. The core of the structure includes four long-lived pairs whose lifetimes at 15°C range from 100 s (C8•C8⁺) to 0.18 s (T7•T7). The formation rate and the lifetime of [d(5mCCTCACTCC)]₂ were measured between pH 6.8 and 4.8. The dimer formation rate is three to four magnitude orders slower than that of a B-DNA duplex. It depends on pH, as it must occur for a bimolecular process involving non cooperative association of neutral and protonated residues. In the range of pH investigated, the dimer lifetime, 500 s at 0°C, pH 6.8, varies approximately as 10^−pH.     

Alteration of A.T base-pair opening kinetics by the ammonium cation in DNA A-tracts

We have investigated by NMR the effects of NH(4)(+) on the chemical shifts, on the structure, and on the imino proton exchange kinetics of two duplexes containing an A-tract, [d(CGCGAATTCGCG)](2) and [d(GCA(4)T(4)GC)](2), and of a B-DNA duplex,[d(CGCGATCGCG)](2). Upon NH(4)(+) addition to [d(CGCGAATTCGCG)](2), the adenosine H2 protons, the thymidine imino protons, and the guanosine imino proton of the adjacent G.C pair show unambiguous chemical shifts. Similar shifts are observed in the A-tract of [d(GCA(4)T(4)GC)](2) and for the A5(H2) proton of the B DNA duplex [d(CGCGATCGCG)](2). The localization of the shifted protons suggests an effect related to NH(4)(+) binding in the minor groove. The cross-peak intensities of the NOESY spectra collected at low and high NH(4)(+) concentrations are comparable, and the COSY spectra do not show any change of the sugar pucker. This indicates a modest effect of ammonium binding on the duplex structures. Nevertheless, the imino proton exchange catalysis by ammonia provides evidence for a substantial effect of NH(4)(+) binding on the A.T base-pair kinetics in the A-tracts. Proton exchange experiments performed at high and low NH(4)(+) concentrations show the occurrence of two native conformations in proportions depending on the NH(4)(+) concentration. The base-pair lifetimes and the open-state lifetimes of each conformation are distinct. Exchange from each conformation proceeds via a single open state. But if, and only if, the NH(4)(+) concentration is kept larger than 1 M, the A.T imino proton exchange times of A-tract sequences exhibit a linear dependence versus the inverse of the NH(3) proton acceptor concentration. This had been interpreted as an indication for two distinct base-pair opening modes (W?rml?nder, S., Sen, A., and Leijon, M. (2000) Biochemistry 39, 607-615).     

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.     

DNA interstrand crosslink formation by mechlorethamine at a cytosine-cytosine mismatch pair: kinetics and sequence dependence

Expansion of the triplet repeat DNA sequence d[CGG]n.d[CCG]n is a characteristic of Fragile X syndrome, a human neurodegenerative disease. Stable intrastrand conformations formed by both d[CGG]n and d[CCG]n, and involving G-G and C-C mismatch pairs, respectively, are believed to be of importance in the development of the disease. We have shown previously that C-C mismatch pairs can be crosslinked covalently by mechlorethamine, a nitrogen mustard alkylating agent, and hence this reaction may be of value as a probe for conformers of d[CCG]n. To characterize the mechlorethamine C-C crosslink reaction further, here we report the kinetics and sequence dependence of formation of the crosslink species, using a series of model duplexes. The rate of reaction depends on the base sequence proximal to the C-C mismatch pair. Hence, in 19mer duplexes containing a central d[M4M3M2M1Cn1n2n3n4].d[N4N3N2N1Cm1m2m3m4] sequence, where M-m and N-n are complementary base pairs, the amount of crosslink increased with increasing G-C content of the eight base pairs neighboring the C-C mismatch and with the proximity of the G-C pairs to the C-C mismatch. Molecular dynamics simulations of the solvated duplexes provided an explanation of these data. Hence, for a C-C pair flanked by G-C base pairs the mismatched cytosine bases remain stacked within the duplex, but for a C-C pair flanked by A-T base pairs, the simulations suggested local opening of the duplex around the C-C pair, making it a less effective target for mechlorethamine.     

Structure, dynamics, and thermodynamics of mismatched DNA oligonucleotide duplexes d(CCCAGGG)2 and d(CCCTGGG)2

The structures and hydrogen exchange properties of the mismatched DNA oligonucleotide duplexes d(CCCAGGG)2 and d(CCCTGGG)2 have been studied by high-resolution nuclear magnetic resonance. Both the adenine-adenine and thymine-thymine mismatches are intercalated in the duplexes. The structures of these self-complementary duplexes are symmetric, with the two strands in equivalent positions. The evidence indicates that these mismatches are not stably hydrogen bonded. The mismatched bases in both duplexes are in the anti conformation. The mismatched thymine nucleotide in d(CCCTGGG)2 is intercalated in the duplex with very little distortion of the bases or sugar-phosphate backbone. In contrast, the bases of the adenine-adenine mismatch in d(CCCAGGG)2 must tilt and push apart to reduce the overlap of the amino groups. The thermodynamic data show that the T-T mismatch is less destabilizing than the A-A mismatch when flanked by C-G base pairs in this sequence, in contrast to their approximately equal stabilities when flanked by A-T base pairs in the sequence d(CAAAXAAAG.CTTTYTTTG) where X and Y = A, C, G, and T [Aboul-ela, F., Koh, D., & Tinoco, I., Jr. (1985) Nucleic Acids Res. 13, 4811]. Although the mechanism cannot be determined conclusively from the limited data obtained, exchange of the imino protons with solvent in these destabilized heteroduplexes appears to occur by a cooperative mechanism in which half the helix dissociates.     

Influence of dangling thymidine residues on the stability and structure of two DNA duplexes

We have employed temperature-dependent UV spectroscopy, circular dichroism (CD), 400-MHz proton nuclear magnetic resonance (NMR), and computer modeling to characterize both structurally and thermodynamically the influence of unpaired, dangling thymidine residues (T) on the thermal stability and melting behavior of two DNA core duplexes. The specific DNA double helices that we have investigated in this work are core duplexes [d(GC)3]2 (I) and [d(CG)3]2 (IV), 3' dangling T derivatives [d[(GC)3TT]]2 (II) and [d[(CG)3TT]]2 (V), and 5' dangling T derivatives [d[TT(GC)3]]2 (III) and [d[TT(CG)3]]2 (VI). Our experimental data allow us to reach the following conclusions: (1) For both core duplexes (I and IV), the addition of dangling T residues on either the 5' or 3' end causes an increase in the optical melting temperature tm. (2) For both core duplexes, 5' dangling T residues induce a greater increase in the optical tm's than 3' dangling T residues. (3) For both cores duplexes, the increase in tm induced by the addition of dangling T residues is enthalpic in origin, with 5' dangling T residues inducing a greater increase in the van't Hoff transition enthalpy than 3' dangling T's. (4) Dangling T residues cause downfield shifts in all of the nonexchangeable aromatic protons of the [d(GC)3]2 core duplex (I), with the 5' T residues inducing the largest shifts. For the most part, this trend does not hold with the [d(CG)3]2 core duplex (IV). (5) For both core duplexes, the addition of dangling T residues causes an increase in the NMR tm's of almost all the nonexchangeable aromatic protons of the core duplex.(ABSTRACT TRUNCATED AT 250 WORDS)     

Crystal structure of d(gcGXGAgc) with X=G: a mutation at X is possible to occur in a base-intercalated duplex for multiplex formation

DNA fragments with the sequences d(gcGX[Y]n Agc) (n=1, X=A, and Y=A, T, or G)form base-intercalated duplexes, which is a basic unit for formation of multiplexes such as octaplex and hexaplex. To examine the stability of multiplexes, a DNA with X=Y=G and n=1 was crystallized under conditions different from those of the previously determined sequences, and its crystal structure has been determined. The two strands are coupled in an anti-parallel fashion to form a base-intercalated duplex, in which the first and second residues form Watson-Crick type G:C pairs and the third and sixth residues form a sheared G:A pairs at both ends of the duplex. The G4 and G5 bases are stacked alternatively on those of the counter strand to form a long G column of G3-G4-G5*-G5-G4*-G3*, the central four Gs being protruded. In addition, the three duplexes are associated to form a hexaplex around a mixture of calcium and sodium cations on the crystallographic threefold axis. These structural features are similar to those of the previous crystals, though slightly different in detail. The present study indicates that mutation at the 4th position is possible to occur in a base-intercalated duplex for multiplex formations, suggesting that DNA fragments with any sequence sandwiched between the two triplets gcG and Agc can form a multiplex.     

A.T and C.C+ base pairs can form simultaneously in a novel multistranded DNA complex

Previous experiments have established that in certain synthetic oligomeric DNA sequences, including mixtures of d(AACC)5 with d(CCTT)5, adenine-thymine (A.T) base pairs form to the exclusion of neighboring protonated cytosine-cytosine (C.C+) base pairs [Edwards, E., Ratliff, R., & Gray, D. (1988) Biochemistry 27, 5166-5174]. In the present work, circular dichroism and other measurements were used to study DNA oligomers that represented two additional classes with respect to the formation of A.T and/or C.C+ base pairs. (1) One class included two sets of repeating pentameric DNA sequences, d(CCAAT)3-6 and d(AATCC)4,5. For both of these sets of oligomers, an increase in the magnitude of the long-wavelength positive CD band centered at about 280 nm occurred as the pH was lowered from 7 to 5 at 0.1 and 0.5 M Na+, indicating that C.C+ base pairs formed. Even though it may have been possible for these oligomers to form duplexes with two antiparallel A.T base pairs per pentamer, no A.T base pairing was detected by monitoring the CD changes at 250 nm. Thus, spectral data showed that as few as 40% C.C+ base pairs were stable in two sets of oligomers in which A.T base pairs did not form adjacent to, or in place of, C.C+ base pairs. (2) Another class of oligomer was represented by d(C4A4T4C4), which was studied by CD, HPLC, and centrifugation experiments. We confirmed previous work that this sequence was able to form both types of base pairs as the pH and temperature were lowered [Gray, D., Cui, T., & Ratliff, R. (1984) Nucleic Acids Res. 12, 7565-7580].(ABSTRACT TRUNCATED AT 250 WORDS)     

The formation pathway of i-motif tetramers

The i-motif is a four-stranded structure formed by two intercalated parallel duplexes containing hemiprotonated C•C⁺ pairs. In order to describe the sequence of reactions by which four C-rich strands associate, we measured the formation and dissociation rates of three [TC_n]₄ tetramers (n = 3, 4 and 5), their dissociation constant and the reaction order for tetramer formation by NMR. We find that TC_n association results in the formation of several tetramers differing by the number of intercalated C•C⁺ pairs. The formation rates of the fully and partially intercalated species are comparable but their lifetimes increase strongly with the number of intercalated C•C⁺ pairs, and for this reason the single tetramer detected at equilibrium is that with optimal intercalation. The tetramer half formation times vary as the power −2 of the oligonucleotide concentration indicating that the reaction order for i-motif formation is 3. This observation is inconsistent with a model supposing association of two preformed duplex and suggests that quadruplex formation proceeds via sequential strand association into duplex and triplex intermediate species and that triplex formation is rate limiting.     

NMR studies of complex formation between the modified oligonucleotide d(T*TCTGT) covalently linked to an acridine derivative and its complementary sequence d(GCACAGAA)

The oligodeoxynucleotide d(TTCTGT) was covalently attached to the 9-amino group of 2-methoxy-6-chloro-9-aminoacridine (Acr) through its 3'-phOsphate via a pentamethylene linker (m5). In order to avoid its hydrolysis by nucleases inside the cel., one of its phosphates (TpT) was substituTed with a neopentyl group. Complex formation between each of the two purified isomers and the complementary strand d(GCACAGAA) was investigated by nuclear magnetic resonance. The COSY and NOESY connectivities allowed us to assign all the proton resonances of the bases, the sugars (except the overlapping 5'-5' resonances), the acridine, and the pentamethylene chain. Structural information derived from the relative intensity of COSY and NOESY maps revealed that the duplex d(T*TCTGT).d(GCACAGAA) adopts a B-type conformation and that the deoxyriboses preferentially adopt a 2'-endo conformation. The NOE connectivities observed between the protons of the bases or the sugars and the protons of the dye show the intercalation of the acridine between the base pairs. NOE connectivities as well as imino proton resonances show that, at room temperature, the C7 base and the G8 base belonging to two different duplexes are paired. The pseudoaxial and pseudoequatorial isomers were assigned, and the differences in stability of their complex with the complementary strand are discussed.     

Stability of the I-motif structure is related to the interactions between phosphodiester backbones

The i-motif DNA tetrameric structure is formed of two parallel duplexes intercalated in a head-to-tail orientation, and held together by hemiprotonated cytosine pairs. The four phosphodiester backbones forming the structure define two narrow and wide grooves. The short interphosphate distances across the narrow groove induce a strong repulsion which should destabilize the tetramer. To investigate this point, molecular dynamics simulations were run on the [d(C2)]4 and [d(C4)]4 tetramers in 3'E and 5'E topologies, for which the interaction of the phosphodiester backbones through the narrow groove is different. The analysis of the simulations, using the Molecular Mechanics Generalized Born Solvation Area and Molecular Mechanics Poisson-Boltzmann Solvation Area approaches, shows that it is the van der Waals energy contribution which displays the largest relative difference between the two topologies. The comparison of the solvent-accessible area of each topology reveals that the sugar-sugar interactions account for the greater stability of the 3'E topology. This stresses the importance of the sugar-sugar contacts across the narrow groove which, enforcing the optimal backbone twisting, are essential to the base stacking and the i-motif stability. Tighter interactions between the sugars are observed in the case of N-type sugar puckers.     

Thermodynamics of DNA duplexes with adjacent G.A mismatches.

The sequence 5'-d(ATGAGCGAAT) forms a very stable self-complementary duplex with four G.A mismatch base pairs (underlined) out of ten total base pairs [Li et al. (1991) Proc. Natl. Acad. Sci. U.S.A. 88, 26-30]. The conformation is in the general B-family and is stabilized by base-pair hydrogen bonding of an unusual type, by favorable base dipole orientations, and by extensive purine-purine stacking at the mismatched sites. We have synthesized 13 decamers with systematic variations in the sequence above to determine how the flanking sequences, the number of G.A mismatches, and the mismatch sequence order (5'-GA-3' or 5'-AG-3') affect the duplex stability. Changing A.T to G.C base pairs in sequences flanking the mismatches stabilizes the duplexes, but only to the extent observed with B-form DNA. The sequence 5'-pyrimidine-GA-purine-3', however, is considerably more stable than 5'-purine-GA-pyrimidine-3'. The most stable sequences with two pairs of adjacent G.A mismatches have thermodynamic parameters for duplex formation that are comparable to those for fully Watson-Crick base-paired duplexes. Similar sequences with single G.A pairs are much less stable than sequences with adjacent G.A mismatches. Reversing the mismatch order from 5'-GA-3' to 5'-AG-3' results in an oligomer that does not form a duplex. These results agree with predictions from the model derived from NMR and molecular mechanics and indicate that the sequence 5'-pyrimidine-GA-purine-3' forms a stable conformational unit that fits quite well into a B-form double helix.(ABSTRACT TRUNCATED AT 250 WORDS)     

Imino proton exchange and base-pair kinetics in RNA duplexes

Using NMR magnetization transfer from water and ammonia-catalyzed exchange of the imino proton, we have measured the base-pair lifetimes and the dissociation constants of six RNA duplexes: [r(CGCGAUCGCG)](2), [r(CGCGAAUUCGCG)](2), [r(CCUUUCGAAAGG)](2), [r(CGCACGUGCG)](2), [r(GGU(8)CC).r(GGA(8)CC)], and [poly(rA).poly(rU)], and we compare them with those of their DNA homologues. As predicted by a two-state (closed/open) model of the pair, the imino proton exchange times decrease linearly vs. the inverse of catalyst concentration. As in DNA duplexes, base pairs open one at a time, and the kinetics is in most cases insensitive to the nature of the adjacent residues. The lifetime of the r(G.C) pairs, 40 to 50 ms, is longer than that of the equivalent in the corresponding oligodeoxynucleotides, and the dissociation constants, about 10(-)(7), are slightly smaller. The r(A.U) opening and closing rates are much larger than those of the d(A.T) pairs, but the stabilities are comparable.     

Massive parallel analysis of DNA-Hoechst 33258 binding specificity with a generic oligodeoxyribonucleotide microchip.

A generic oligodeoxyribonucleotide microchip was used to determine the sequence specificity of Hoechst 33258 binding to double-stranded DNA. The generic microchip contained 4096 oxctadeoxynucleo-tides in which all possible 4(6)= 4096 hexadeoxy-nucleotide sequences are flanked on both the 3'- and 5'-ends with equimolar mixtures of four bases. The microchip was manufactured by chemical immobilization of presynthesized 8mers within polyacrylamide gel pads. A selected set of immobilized 8mers was converted to double-stranded form by hybridization with a mixture of fluorescently labeled complementary 8mers. Massive parallel measurements of melting curves were carried out for the majority of 2080 6mer duplexes, in both the absence and presence of the Hoechst dye. The sequence-specific affinity for Hoechst 33258 was calculated as the increase in melting temperature caused by ligand binding. The dye exhibited specificity for A:T but not G:C base pairs. The affinity is low for two A:T base pairs, increases significantly for three, and reaches a plateau for four A:T base pairs. The relative ligand affinity for all trinucleotide and tetranucleotide sequences (A/T)(3)and (A/T)(4)was estimated. The free energy of dye binding to several duplexes was calculated from the equilibrium melting curves of the duplexes formed on the oligonucleotide microchips. This method can be used as a general approach for massive screening of the sequence specificity of DNA-binding compounds.     

Formation of the G-quadruplex and i-motif structures in retinoblastoma susceptibility genes (Rb)

The formation of G-quadruplex and i-motif structures in the 5′ end of the retinoblastoma (Rb) gene was examined using chemical modifications, circular dichroism (CD) and fluorescence spectroscopy. It was found that substitutions of 8-methylguanine at positions that show syn conformations in antiparallel G-quadruplexes stabilize the structure in the G-rich strand. The complementary C-rich 18mer forms an i-motif structure, as suggested by CD spectroscopy. Based on the C to T mutation experiments, C bases participated in the C–C⁺ base pair of the i-motif structure were determined. Experiments of 2-aminopurine (2-AP) substitution reveal that an increase of fluorescence in the G-quadruplex relative to duplex is attributed to unstacked 2-AP within the loop of G-quadruplex. The fluorescence experiments suggest that formation of the G-quadruplex and i-motif can compete with duplex formation. Furthermore, a polymerase arrest assay indicated that formation the G-quadruplex structure in the Rb gene acts as a barrier in DNA synthesis.     

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)