The telomeric dG(GT)4G sequence can adopt a parallel-stranded double helical conformation

Oligonucleotides 3'-d(GTGTGTGTGG)-L-d(GGTGTGTGTG)-3' (hp-GT) and 3'-d(G4STG4TG4STG4STGG)-L-d(GGTGTGTGTG)-3' (hp-SGT), (L=(CH2CH2O)3), were shown by use of several optical techniques to form a novel parallel-stranded (ps) intramolecular double helix with purine-purine and pyrimidine-pyrimidine base pairing. The rotational relaxation time of hp-GT was similar to that of a 10-bp reference duplex, and the fraction of unpaired bases was determined to be approximately 7%, testifying to the formation of an intramolecular double helical hairpin by the sequence under the given experimental conditions. A quasi-two-state mode of ps-double helix formation was validated, yielding a helix-coil transition enthalpy of -135 +/- 5 kJ/mol. The G x G and T x T (or 4ST x T) base pair configurations and conformational parameters of the double helix were derived with molecular modeling by force field techniques. Repetitive d(GT) sequences are abundant in telomers of different genomes and in the regulatory regions of genes. Thus, the observed conformational potential of the repetitive d(GT) sequence may be of importance in the regulation of cell processes.     

Cleavage of parallel-stranded DNA duplex by peplomycin metal complexes.

Peplomycin-mediated degradation of parallel-stranded (ps) duplex was investigated. It was found that Co- and Fe-peplomycins degraded ps DNA duplex by 4'-hydrogen abstraction at 5'-GPy (pyrimidine) site in a similar manner to that of antiparallel B-DNA. While the orientation of two strands of ps and B-form DNA duplexes are reversed, peplomycin metal complex can bind to ps DNA duplex to cause oxidative DNA damage. These results indicate that peplomycin metal complex mainly interacts with one strand which is damaged.     

Structure, stability, and thermodynamics of a short intermolecular purine-purine-pyrimidine triple helix

We have investigated the structure and physical chemistry of the d(C3T4C3).2[d(G3A4G3)] triple helix by polyacrylamide gel electrophoresis (PAGE), 1H NMR, and ultraviolet (UV) absorption spectroscopy. The triplex was stabilized with MgCl2 at neutral pH. PAGE studies verify the stoichiometry of the strands comprising the triplex and indicate that the orientation of the third strand in purine-purine-pyrimidine (pur-pur-pyr) triplexes is antiparallel with respect to the purine strand of the underlying duplex. Imino proton NMR spectra provide evidence for the existence of new purine-purine (pur.pur) hydrogen bonds, in addition to those of the Watson-Crick (W-C) base pairs, in the triplex structure. These new hydrogen bonds are likely to correspond to the interaction between third-strand guanine NH1 imino protons and the N7 atoms of guanine residues on the purine strand of the underlying duplex. Thermal denaturation of the triplex proceeds to single strands in one step, under the conditions used in this study. Binding of the third strand appears to enhance the thermal stability of the duplex by 1-3 degrees C, depending on the DNA concentration. The free energy of triplex formation (-26.0 +/- 0.5 kcal/mol) is approximately twice that of duplex formation (-12.6 +/- 0.7 kcal/mol), suggesting that the overall stability of the pur.pur base pairs is similar to that of the W-C base pairs.(ABSTRACT TRUNCATED AT 250 WORDS)     

Thermodynamics of the various forms of the dodecamer d(ATTACCGGTAAT) and of its constituent hexamers from proton nmr chemical shifts and UV melting curves: three-state and four-state thermodynamic models

Chemical shifts of base and H1' protons of the single-stranded hexamers d(ATTACC) and d(GGTAAT), of the 1:1 mixtures of these complementary hexamers, and of the self-complementary dodecamer d(ATTACCGGTAAT) were measured at various temperatures in aqueous solution. Four different sample concentrations were used in the case of the dodecamer and of the mixture of the complementary hexamers; the individual hexamers were measured at two different DNA concentrations. Absorbance temperature profiles at five different NaCl concentrations were measured for the dodecamer in order to quantify the effect of the ionic strength on the duplex formation. Under suitable conditions of nucleotide concentration, temperature, and ionic strength, the dodecamer adopts either a B-DNA duplex or a hairpin-loop structure. Chemical shift vs temperature profiles, constructed for all samples, were used to obtain thermodynamic parameters either for the various stacking interactions in the single strands or for the duplex or the hairpin-loop formation. In the analysis of the duplex formation of the hexamers, a two-state approach appeared too simple, because systematic deviations were revealed. Therefore, a new three-state model (DUPSTAK) was developed. In order to investigate the magnitude of error arising from the use of the two-state approach in cases where the DUPSTAK model appears more appropriate, a series of test calculations was made. The magnitude of error in the enthalpy and in the entropy of duplex melting is found to depend linearly upon the actual melting temperature and not upon the individual delta Hd degrees and delta Sd degrees values. Thermodynamic analysis of the chemical shift vs temperature profiles in D2O solution (no added salt) yields an average Tmd value of 341 K (1M DNA) and delta Hd degrees of - 121 kJ.mol-1 for the dimer/random-coil transition of the hexamer duplex d(ATTACC).d(GGTAAT). For the duplex in equilibrium random-coil transition of the 12-mer d(ATTACCGGTAAT) an average Tmd value of 336 K (1M DNA) and delta Hd degrees of -372 kJ.mol-1 are found. The hairpin/random-coil transition of d(ATTACCGGTAAT) is characterized by a rather large delta Hh degrees value, -130 kJ.mol-1, and an average Tmh value of 304 K.     

Parallel-stranded duplex DNA containing dA · dU base pairs

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

A parallel stranded linear DNA duplex incorporating dG.dC base pairs

DNA oligonucleotides with appropriately designed complementary sequences can form a duplex in which the two strands are paired in a parallel orientation and not in the conventional antiparallel double helix of B-DNA. All parallel stranded (ps) molecules reported to date have consisted exclusively of dA.dT base pairs. We have substituted four dA.dT base pairs of a 25-nt parallel stranded linear duplex (ps-D1.D2) with dG.dC base pairs. The two strands still adopt a duplex structure with the characteristic spectroscopic properties of the ps conformation but with a reduced thermodynamic stability. Thus, the melting temperature of the ps duplex with four dG.dC base pairs (ps-D5.D6) is 10-16 degrees C lower and the van't Hoff enthalpy difference delta HvH for the helix-coil transition is reduced by 20% (in NaCl) and 10% (in MgCl2) compared to that of ps-D1.D2. Based on energy minimizations of a ps-[d(T5GA5).d(A5CT5)] duplex using force field calculations we propose a model for the conformation of a trans dG.dC base pair in a ps helix.     

Alternating d(G-A) sequences form a parallel-stranded DNA homoduplex.

The oligonucleotides d[(G-A)7G] and d[(G-A)12G] self-associate under physiological conditions (10 mM MgCl2, neutral pH) into a stable double-helical structure (psRR-DNA) in which the two polypurine strands are in a parallel orientation in contrast to the antiparallel disposition of conventional B-DNA. We have characterized psRR-DNA by gel electrophoresis, UV absorption, vacuum UV circular dichroism, monomer-excimer fluorescence of oligonucleotides end-labelled with pyrene, and chemical probing with diethyl pyrocarbonate and dimethyl sulfate. The duplex is stable at pH 4-9, suggesting that the structure is compatible with, but does not require, protonation of the A residues. The data support a model derived from force-field analysis in which the parallel-stranded d(G-A)n helix is right-handed and constituted of alternating, symmetrical Gsyn.Gsyn and Aanti.Aanti base pairs with N1H...O6 and N6H...N7 hydrogen bonds, respectively. This dinucleotide structure may be the source of a negative peak observed at 190 nm in the vacuum UV CD spectrum, a feature previously reported only for left-handed Z-DNA. The related sequence d[(GAAGGA)4G] also forms a parallel-stranded duplex but one that is less stable and probably involves a slightly different secondary structure. We discuss the potential intervention of psRR-DNA in recombination, gene expression and the stabilization of genomic structure.     

Parallel-stranded DNA under topological stress: rearrangement of (dA)15.(dT)15 to a d(A.A.T)n triplex.

DNA oligonucleotides with appropriate sequences can form a stable duplex in which the two strands are paired in a parallel orientation instead of as the conventional antiparallel double helix of B-DNA. In parallel-stranded DNA (ps-DNA) base pairing is noncanonical with the glycosidic bonds in a trans orientation. The two grooves are equivalent. We have synthesized DNA duplexes consisting of a central parallel-stranded (dA)15.(dT)15 tract flanked by normal antiparallel regions, and ligated them into the pUC18 plasmid. The effect of negative supercoiling on the covalently closed circular molecules was studied by two-dimensional agarose gel electrophoresis and by chemical modification with OsO4-pyridine (Os,py) and diethylpyrocarbonate (DEPC). The following results were obtained: (i) The ps insert, and by inference ps-DNA in general, adopts a right handed helical form. (ii) Upon increasing the negative superhelix density (-sigma) to greater than 0.03 the 15 bp ps insert undergoes a major transition leading to a relaxation corresponding to a reduction in twist of approximately 2.5 helical turns. The transition free surgery is approximately kcal/mol. (iii) The chemical modification pattern of the resulting structure suggests that the purine strand folds back and associates with the pyrimidine strand, forming a novel intramolecular triplex structure consisting of d(A.A.T) base triplets. A model for the triplex conformation is proposed and its thermodynamic properties are analyzed by statistical mechanics.     

Parallel-stranded DNA with mixed AT/GC composition: role of trans G.C base pairs in sequence dependent helical stability

Parallel-stranded (ps) DNAs with mixed AT/GC content comprising G.C pairs in a varying sequence context have been investigated. Oligonucleotides were devised consisting of two 10-nt strands complementary either in a parallel or in an antiparallel orientation and joined via nonnucleotide linkers so as to form 10-bp ps or aps hairpins. A predominance of intramolecular hairpins over intermolecular duplexes was achieved by choice of experimental conditions and verified by fluorescence determinations yielding estimations of rotational relaxation times and fractional base pairing. A multistate mode of ps hairpin melting was revealed by temperature gradient gel electrophoresis (TGGE). The thermal stability of the ps hairpins with mixed AT/GC content depends strongly on the specific sequence in a manner peculiar to the ps double helix. The thermodynamic effects of incorporating trans G.C base pairs into an AT sequence are context-dependent: an isolated G. C base pair destabilizes the duplex whereas a block of > or =2 consecutive G.C base pairs exerts a stabilizing effect. A multistate heterogeneous zipper model for the thermal denaturation of the hairpins was derived and used in a global minimization procedure to compute the thermodynamic parameters of the ps hairpins from experimental melting data. In 0.1 M LiCl at 3 degrees C, the formation of a trans G.C pair in a GG/CC sequence context is approximately 3 kJ mol(-)(1) more favorable than the formation of a trans A.T pair in an AT/TA sequence context. However, GC/AT contacts contribute a substantial unfavorable free energy difference of approximately 2 kJ mol(-)(1). As a consequence, the base composition and fractional distribution of isolated and clustered G.C base pairs determine the overall stability of ps-DNA with mixed AT/GC sequences. Thus, the stability of ps-DNA comprising successive > or =2 G.C base pairs is greater than that of ps-DNA with an alternating AT sequence, whereas increasing the number of AT/GC contacts by isolating G.C base pairs exerts a destabilizing effect on the ps duplex. Molecular modeling of the various helices by force field techniques provides insight into the structural basis for these distinctions.     

The hydrogen-bonding structure in parallel-stranded duplex DNA is reverse Watson-Crick

Raman spectra of the parallel-stranded duplex formed from the deoxyoligonucleotides 5'-d-[(A)10TAATTTTAAATATTT]-3' (D1) and 5'-d[(T)10ATTAAAATTTATAAA]-3' (D2) in H2O and D2O have been acquired. The spectra of the parallel-stranded DNA are then compared to the spectra of the antiparallel double helix formed from the deoxyoligonucleotides D1 and 5'-d(AAATATTTAAAATTA-(T)10]-3' (D3). The Raman spectra of the antiparallel-stranded (aps) duplex are reminiscent of the spectra of poly[d(A)].poly[d(T)] and a B-form structure similar to that adopted by the homopolymer duplex is assigned to the antiparallel double helix. The spectra of the parallel-stranded (ps) and antiparallel-stranded duplexes differ significantly due to changes in helical organization, i.e., base pairing, base stacking, and backbone conformation. Large changes observed in the carbonyl stretching region (1600-1700 cm-1) implicate the involvement of the C(2) carbonyl of thymine in base pairing. The interaction of adenine with the C(2) carbonyl of thymine is consistent wtih formation of reverse Watson-Crick base pairing in parallel-stranded DNA. Phosphate-furanose vibrations similar to those observed for B-form DNA of heterogenous sequence and high A,T content are observed at 843 and 1092 cm-1 in the spectra of the parallel-stranded duplex. The 843-cm-1 band is due to the presence of a sizable population of furanose rings in the C2'-endo conformation. Significant changes observed in the regions from 1150 to 1250 cm-1 and from 1340 to 1400 cm-1 in the spectra of the parallel-stranded duplex are attributed to variations in backbone torsional and glycosidic angles and base stacking.     

Spectroscopic properties and helical stabilities of 25-nt parallel-stranded linear DNA duplexes

DNA strands with appropriate sequences of dA and dT can form a stable duplex in which the two strands adopt a parallel (ps) instead of the conventional antiparallel (aps) orientation. Four 25-nt dA.dT-containing deoxyoligonucleotides (D1-4) were synthesized. D1 has the sequence 5'-dA10TA2T4A3TAT3-3'. Viewed with the same polarity, D2, D3, and D4 are the complement, inverted complement, and inverse of D1, respectively. The two combinations D1.D3 and D2.D4 form conventional antiparallel duplexes (aps-D1.D3, aps-D2.D4). D1.D2 and D3.D4, however, constitute stable parallel-stranded duplexes (ps-D1.D2, ps-D3.D4), as established by various criteria including the following: (i) The electrophoretic mobilities of ps-D1.D2 and ps-D3.D4 are similar to those of the antiparallel-stranded duplexes. (ii) The ultraviolet absorption and circular dichroism spectra of the ps duplexes are indicative of a base-paired structure, but differ systematically from those of the aps helices. (iii) Similar salt-dependent thermal transitions are observed for the four duplexes, but the melting temperatures of the ps molecules are lower by 13-18 degrees C.     

Interlocked mismatch-aligned arrowhead DNA motifs.

BACKGROUND: Triplet repeat sequences are of considerable biological importance as the expansion of such tandem arrays can lead to the onset of a range of human diseases. Such sequences can self-pair via mismatch alignments to form higher order structures that have the potential to cause replication blocks, followed by strand slippage and sequence expansion. The all-purine d(GGA)n triplet repeat sequence is of particular interest because purines can align via G.G, A.A and G.A mismatch formation. RESULTS: We have solved the structure of the uniformly 13C,15N-labeled d(G1-G2-A3-G4-G5-A6-T7) sequence in 10 mM Na+ solution. This sequence adopts a novel twofold-symmetric duplex fold where interlocked V-shaped arrowhead motifs are aligned solely via interstrand G1.G4, G2.G5 and A3.A6 mismatch formation. The tip of the arrowhead motif is centered about the p-A3-p step, and symmetry-related local parallel-stranded duplex domains are formed by the G1-G2-A3 and G4-G5-A6 segments of partner strands. CONCLUSIONS: The purine-rich (GGA)n triplet repeat sequence is dispersed throughout the eukaryotic genome. Several features of the arrowhead duplex motif for the (GGA)2 triplet repeat provide a unique scaffold for molecular recognition. These include the large localized bend in the sugar-phosphate backbones, the segmental parallel-stranded alignment of strands and the exposure of the Watson-Crick edges of several mismatched bases.     

Parallel-stranded DNA with Hoogsteen base pairing stabilized by a trans-[Pt(NH3)2]2+ cross-link: characterization and conversion into a homodimer and a triplex

The oligonucleotides 5'-d(TTTTCTTTTG) and 5'-d(AAAAGAAAAG) were cross-linked with a trans-[Pt(NH3)2]2+ entity via the N7 positions of the 3'-end guanine bases to give parallel-stranded (ps) DNA. At pH 4.2, CD and NMR spectroscopy indicate the presence of Hoogsteen base pairing. In addition, temperature-dependent UV spectroscopy shows an increase in melting temperature for the platinated duplex (35 degrees C) as compared to the non-platinated, antiparallel-stranded duplex formed from the same oligonucleotides (21 degrees C). A monomer-dimer equilibrium for the platinated 20mer is revealed by gel electrophoresis. At pH 4.2, addition of a third strand of composition 5'-d(AGCTTTTCTTTTAG) to the ps duplex leads to the formation of a triple helix with two distinct melting points at 38 degrees C (platinum cross-linked Hoogsteen part) and 21 degrees C (Watson-Crick part), respectively.     

The Telomeric dG(GT)4G Sequence Can Adopt a Parallel-Stranded Double Helical Conformation

Abstract

Oligonucleotides 3′-d(GTGTGTGTGG)-L-d(GGTGTGTGTG)-3′ (hp-GT) and 3′- d(G^4STG^4STG^4STG^4STGG)-L-d(GGTGTGTGTG)-3′ (hp-SGT), (L=(CH₂CH₂O)₃), were shown by use of several optical techniques to form a novel parallel-stranded (ps) intramolecular double helix with purine-purine and pyrimidine-pyrimidine base pairing. The rotational relaxation time of hp-GT was similar to that of a 10-bp reference duplex, and the fraction of unpaired bases was determined to be ～ 7%, testifying to the formation of an intramolecular double helical hairpin by the sequence under the given experimental conditions. A quasi-two- state mode of ps-double helix formation was validated, yielding a helix-coil transition enthalpy of ?135±5 kJ/mol. The G-G and T·T (or ^4ST·T) base pair configurations and conformational parameters of the double helix were derived with molecular modeling by force field techniques. Repetitive d(GT) sequences are abundant in telomers of different genomes and in the regulatory regions of genes. Thus, the observed conformational potential of the repetitive d(GT) sequence may be of importance in the regulation of cell processes.     

Crystal structure of an RNA octamer duplex r(CCCIUGGG)2 incorporating tandem I.U wobbles.

The crystal structure of the RNA octamer duplex r(CCCIUGGG)2has been elucidated at 2.5 A resolution. The crystals belong to the space group P21and have unit cell constants a = 33.44 A, b = 43.41 A, c = 49.39 A and beta = 104.7 degrees with three independent duplexes (duplexes 1-3) in the asymmetric unit. The structure was solved by the molecular replacement method and refined to an Rwork/Rfree of 0.185/0.243 using 3765 reflections between 8.0 and 2.5 A. This is the first report of an RNA crystal structure incorporating I.U wobbles and three molecules in the asymmetric unit. Duplex 1 displays a kink of 24 degrees between the mismatch sites, while duplexes 2 and 3 have two kinks each of 19 degrees and 27 degrees, and 24 degrees and 29 degrees, respectively, on either side of the tandem mismatches. At the I.U/U.I mismatch steps, duplex 1 has a twist angle of 33.9 degrees, close to the average for all base pair steps, but duplexes 2 and 3 are underwound, with twist angles of 24.4 degrees and 26.5 degrees, respectively. The tandem I.U wobbles show intrastrand purine-pyrimidine stacking but exhibit interstrand purine-purine stacking with the flanking C.G pairs. The three independent duplexes are stacked non-coaxially in a head-to-tail fashion to form infinite pseudo-continuous helical columns which form intercolumn hydrogen bonding interactions through the 2'-hydroxyl groups where the minor grooves come together.     

Thermodynamics of triple helix formation: spectrophotometric studies on the d(A)10.2d(T)10 and d(C+3T4C+3).d(G3A4G3).d(C3T4C3) triple helices.

We have stabilized the d(A)10.2d(T)10 and d(C+LT4C+3).d(G3A4G3).d(C3T4C3) triple helices with either NaCl or MgCl2 at pH 5.5. UV mixing curves demonstrate a 1:2 stoichiometry of purine to pyrimidine strands under the appropriate conditions of pH and ionic strength. Circular dichroic titrations suggest a possible sequence-independent spectral signature for triplex formation. Thermal denaturation profiles indicate the initial loss of the third strand followed by dissociation of the underlying duplex with increasing temperature. Depending on the base sequence and ionic conditions, the binding affinity of the third strand for the duplex at 25 degrees C is two to five orders of magnitude lower than that of the two strands forming the duplex. Thermodynamic parameters for triplex formation were determined for both sequences in the presence of 50 mM MgCl2 and/or 2.0 M NaCl. Hoogsteen base pairs are 0.22-0.64 kcal/mole less stable than Watson-Crick base pairs, depending on ionic conditions and base composition. C+.G and T.A Hoogsteen base pairs appear to have similar stability in the presence of Mg2+ ions at low pH.     

Parallel stranded duplex DNA.

Three linear 21-nt oligonucleotides (C2, C3, C7) have been synthesized with different sequences of A and T residues. One pairwise combination, (C3, C7), hybridizes to form a conventional antiparallel duplex (aps-C3.C7), whereas the pair C2, C3 forms a duplex (ps-C2.C3) in which the two strands are in a parallel orientation and the A.T base-pairs in a reverse Watson-Crick configuration. The existence of the novel ps helical structure was established from the following criteria: (i) The electrophoretic mobilities of the ps and aps duplexes in native and denaturing polyacrylamide gels are similar. (ii) The ps duplex is not a substrate for T4 DNA ligase. (iii) Salt-dependent thermal transitions are observed for the two duplexes, but the melting temperatures of the ps molecules are 15 degrees C lower. (iv) The ultraviolet absorption and circular dichroism spectra of the ps duplex are indicative of a base-paired structure, but differ systematically from that of the aps helix. (v) Based on fluorescent measurements, the bis-benzimidazole drug BBI-258 shows a lower affinity for the ps compared to the aps duplex, whereas the opposite preference holds for the intercalator ethidium bromide. We conclude from the present study that parallel stranded DNA is a stable conformation which can arise by interaction between two conventional strands with appropriate sequence homology.     

A Parallel Stranded Linear DNA Duplex Incorporating dG · dC Base Pairs

Abstract

DNA oligonucleotides with appropriately designed complementary sequences can form a duplex in which the two strands are paired in a parallel orientation and not in the conventional antiparallel double helix of B-DNA. All parallel stranded (ps) molecules reported to date have consisted exclusively of dA · dT base pairs. We have substituted four dA · dT base pairs of a 25-nt parallel stranded linear duplex (ps-D1 · D2) with dG · dC base pairs. The two strands still adopt a duplex structure with the characteristic spectroscopic properties of the ps conformation but with a reduced thermodynamic stability. Thus, the melting temperature of the ps duplex with four dG · dC base pairs (ps-D5 · D6) is 10-16°C lower and the van't Hoff enthalpy difference Δ_vH for the helix-coil transition is reduced by 20% (in NaCl) and 10% (in MgCl₂) compared to that of ps-Dl · D2. Based on energy minimizations of a ps-[d(T₅GA₅) · d(A₅CT₅)] duplex using force field calculations we propose a model for the conformation of a trans dG · dC base pair in a ps helix.     

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

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