Structural investigation of poly d(BrU-A) by ultraviolet resonance raman spectroscopy

The resonance Raman spectra of a DNA containing bromodeoxy-uridine (BrdUrd), the poly d(BrU-A), are reported, using U.V. laser as a source of excitation. The conformational change from the ordered, base paired form of poly d(BrU-A) (at 25°C) to the melted form at high temperature (63°C) is reflected in a pronounced hyperchromism of Raman bands at 1627 cm^?1, 1352 cm^?1 and 1230 cm^?1. Particularly the band at 1627 cm^?1 assigned to the vibrations of C4 carbonyl which is hydrogen bonded to adenine increases strongly its intensity upon melting. This represents a new approach for a detection of base unpairing and of modifications in geometry of selective molecules (BrdUrd) in a DNA chain in dilute solutions (10^?4 M).     

Structural and conformational studies of polyriboadenylic acid in neutral and acid solution

Raman spectra of solutions of polyriboadenylic acid have been studied in the pH range of 7.2–5.2. Bands are identified which are sensitive to the characteristics of poly(rA) in the single-and double-stranded helical forms. Thermal melting profiles were obtained as a function of pH to monitor simultaneously the changes in (1) the phosphodiester backbone, (2) the base-stacking interactions, (3) the perturbation of the PO unit, and (4) the degree of protonation at the N-1 position in the adenine base. The temperature dependence of the intensity ratio of the bands at 725 and 705 cm^?1 appears to be sensitive to the noncooperative and the cooperative thermal-melting process for the single-and double-stranded forms of poly(rA), respectively. Concurrently, bands diagnostic of the degree of protonation reveal that the cooperative melting process for the “acid” poly(rA) clearly involves deprotonation. The progressive perturbation of the 1100 cm^?1 band with an increasing degree of protonation of poly(rA) is consistent with earlier suggestions regarding a PO-(6)-NH₂ interaction in the double-helical form of poly(rA). The stability of the double-helix parallels the degree of protonation over the pH range studied as reflected in the t_m values, which increase linearly with decreasing pH.     

Intensity changes of base and backbone Raman modes in the B to Z transition of poly(dG-dm5C)

Raman spectroscopy was employed to investigate the temperature-induced B to Z transition of poly(dG-dm5C). The transition midpoint was about 37 degrees C for a solvent containing 20 mM Mg2+. A 10-fold change in Mg2+ concentration altered the transition midpoint by at least 60 degrees C. Raman spectra of the B and Z forms of poly(dG-dm5C) exhibited characteristics similar to those observed with poly(dG-dC). The 682 cm-1 guanine mode and 835 cm-1 backbone mode were present in the B conformation. In the Z form the intensities of these two bands decrease substantially and new peaks were observed at 621 cm-1, 805 and 819 cm-1. Several bands unique to poly(dG-dm5C) were also observed. Transition profiles of band intensity vs. temperature were determined for fourteen Raman bands. The curves of all of the base vibrations and one backbone mode had the same slope and midpoint. This indicates that conformational changes in the guanine and methycytosine bases occur concurrently.     

Alkaline lysis of mammalian cells for sedimentation analysis of nuclear DNA. Conformation of released DNA as monitored by physical, electron microscopic and enzymological techniques.

The degree of single strandedness of the DNA released from rat liver nuclei by various alkaline lysing solutions (including some with sodium dodecyl sulfate) was determined both before and after sedimentation in alkaline sucrose gradients employing electron microscopy, melting profiles, circular dichroism measurements, and digestibility by S1 nuclease. Regardless of the technique employed, the results obtained following alkaline sucrose gradient centrifugation of the DNA are consistent. The DNA was completely single stranded as judged by electron microscopy, circular dichroism spectra, and digestibility by S1 nuclease, an enzyme that specifically hydrolyzes single-stranded DNA. This was not true if the DNA was analyzed following alkaline lysis of the nuclei but before centrifugation. Under conditions which gave a complete transition to the single-stranded state, as judged by melting profiles and circular dichroism spectra, only 10-15% of the DNA was hydrolyzed by S1 nuclease. An increase in the susceptibility of the released DNA to S1 nuclease was observed with increases in the pH of the lysing solution. In order to release DNA which was single stranded as judged by both physical and enzymological techniques, the rat liver nuclei were lysed for 30 min with a 0.3 M NaOH lysing solution containing 0.5% dodecyl sulfate, 0.3 M NaCl and 0.03 M EDTA.     

Melting and premelting phenomenon in DNA by laser Raman scattering.

Raman spectra of DNA from calf thymus DNA have been taken over a wide range of temperatures (25°–95°) in both D₂O and H₂O. A study of the temperature dependence of the Raman spectra shows that the temperature profiles of the intensities and frequencies of the various bands fall into four different categories: (1) base bands that show a reversible increase in intensity prior to the melting region, i.e., a definite premelting phenomenon; (2) base bands that show little or no temperature dependence; (3) deoxyribose-phosphate backbone vibrations that show no temperature dependence up to the melting region, at which point large decreases in intensity occur; and (4) slow frequency changes in certain in-plane vibrations of guanine and adenine due to deuteration of the C-8 hydrogen of these purines in D₂O. Certain Raman bands arising from each of the four bases, adenine, thymine, guanine, and cytosine have been found to undergo a gradual increase in intensity prior to the melting region at which point large, abrupt increases in intensity occur. The carbonyl stretching band of thymine, involved in the interbase hydrogen bonding actually undergoes both a gradual shift to a lower frequency as well as an increase in intensity. These changes provide evidence that some change in the geometry of the bases relative to each other begins to occur around 50°C, well below the melting region of 70°–85°C. From the spectra taken at various temperatures, the DNA appears to remain in the B conformation until the melting point is reached, at which time the DNA progresses into a disordered random-coil form. No A-form conformation is found either in the premelting or the melting region.     

Polyribonucleotides containing thiopurines: Synthesis and properties

The synthesis of poly(1-methyl-6-thioinosinic acid) and a comparison of its properties with those of poly(6-thioinosinic acid) and poly(6-methylthiopurinylic acid) are reported. In contrast to 6-thioinosine 5′-diphosphate, 1-methyl-6-thioinosine 5′-diphosphate was found to be a substrate for polynucleotide phosphorylase-catalyzed homopolyribonucleotide synthesis. Poly(1-methyl-6-thioinosinic acid) appears to form a single stranded helical array with a highly cooperative melting transition (Tm = 12°C) and a very large bathochromic shift (12 nm) in the absorption maximum upon melting.     

pH-Dependent Raman spectra and thermal melting profiles for polycytidylic acid

The Raman spectrum of polycytidylic acid was investigated in the pH range of 6.6–4.1. The thermal melting temperatures and the nature of the thermal melting profiles change in this range as monitored by the three Raman band envelopes, which include the 780-, 805-cm^?1 bands, the 1190-, 1285-cm^?1 bands, and the 1527-cm^?1 band. By coupling these data with the theory of Raman scattering intensity and quantitative pH profiles for cytidine, it is shown that the band envelopes studied exhibit specific, yet different information regarding the thermal melting process. The band envelopes at 1170–1310 and 1527 cm^?1, which are a sensitive function of both the extent of protonation and base stacking (hypochromic), reveal T_m values which agree with values derived from uv melting profiles. The 760–830-cm^?1 envelope, which is not directly sensitive to cytosine residue protonation, but includes information associated with base stacking (the 780-cm^?1 band) and the nature of the phosphodiester backbone (the frequency-dependent 805-cm^?1 component), exhibits T_m values which deviate from the values obtained from the other bands. The observed differences are pH-dependent and correlate well with the extent of deprotonation that takes place in the denaturation process. Details of the spectrum of neutral and protonated poly(C) from pH 7 to 4.1 are discussed and related to the nature of the thermal denaturation process.     

Temperature dependence of the Raman spectrum of DNA. II. Raman signatures of premelting and melting transitions of poly(dA).poly(dT) and comparison with poly(dA-dT).poly(dA-dT).

The temperature dependence of the Raman spectrum of poly(dA).poly(dT) (dA: deoxyadenosine; dT: thymidine), a model for DNA containing consecutive adenine.thymine (A.T) pairs, has been analyzed using a spectrometer of high spectral precision and sensitivity. Three temperature intervals are distinguished: (a) premelting (10 < t < 70 degrees C), in which the native double helix is structurally altered but not dissociated into single strands; (b) melting (70 < t < 80 degrees C), in which the duplex is dissociated into single strands; and (c) postmelting (80 < t degrees C), in which no significant structural change can be detected. The distinctive Raman difference signatures observed between 10 and 70 degrees C and between 70 and 80 degrees C are interpreted in terms of the structural changes specific to premelting and melting transitions, respectively. Premelting alters the low-temperature conformation of the deoxyribose-phosphate backbone and eliminates base hydrogen bonding that is distinct from canonical Watson-Crick hydrogen bonding; these premelting perturbations occur without disruption of base stacking. Conversely, melting eliminates canonical Watson-Crick pairing and base stacking. The results are compared with those reported previously on poly(dA-dT).poly(dA-dT), the DNA structure consisting of alternating A.T and T.A pairs (L. Movileanu, J. M. Benevides, and G. J. Thomas, Jr. Journal of Raman Spectroscopy, 1999, Vol. 30, pp. 637-649). Poly(dA).poly(dT) and poly(dA-dT).poly(dA-dT) exhibit strikingly dissimilar temperature-dependent Raman profiles prior to the onset of melting. However, the two duplexes exhibit very similar melting transitions, including the same Raman indicators of ruptured Watson-Crick pairing, base unstacking and collapse of backbone order. A detailed analysis of the data provides a comprehensive Raman assignment scheme for adenosine and thymidine residues of B-DNA, delineates Raman markers diagnostic of consecutive A.T and alternating A.T/T.A tracts of DNA, and identifies the distinct Raman difference signatures for premelting and melting transitions in the two types of sequences.     

Raman studies of nucleic acids. VII. Poly A-poly U and poly G-poly C

Laser-excited Raman spectra of the double-helical complexes poly A·poly U and poly G·poly C are reported for ²H₂O and H₂O solutions. The spectra are discussed in relation to their use as quantitative reference spectra for determining the dependence of the Raman scattering of RNA on secondary structure. The Raman line at 815 cm^?1, due to the phosphodiester group, exhibits the same intrinsic intensity in spectra of poly A·poly U and poly G·poly C and is thus dependent only upon the amount of ordering of the helix and not on the kinds of nucleotides involved. The hypochromic Raman lines in spectra of poly A·poly U are identified and their intensity changes are determined quantitatively over the temperature range 32–85°C. Comparison of the spectra in the 1500–1750 cm^?1 region reveals that the Raman lines from carbonyl group vibrations of uracil are about sevenfold more intense than those of guanine and cytosine for both paired and unpaired states and will thus dominate the spectra of RNA. The Raman frequencies in this region are also compared with previously reported infrared frequencies and give evidence of being strongly perturbed by base-stacking interactions in the helices.     

Synthesis and conformational studies of ribooligonucleotides which contain an alternating C-G sequence and show unusual circular dichroism spectra

The poly [r(C-G)] duplex shows an unusually large negative CD band in the long wavelength region. In order to elucidate this phenomenon, r(C-G-C-G) and r(C-G-C-G-C-G) were synthesized by a phosphotriester method and their properties were examined by UV, CD, 1H and 31P NMR spectroscopy. These ribooligomers form self-duplexes at low temperature, the CD spectra of which show negative bands at around 290 nm and positive bands at around 265 nm. The results of 1H nuclear Overhauser effect experiments, 1H chemical shift-temperature profiles of base protons, and the sharp singlet observed for all H1' protons are consistent with a normal A-RNA structure but not with a Z-DNA like structure. The CD-temperature profiles and 31P NMR spectra support this conclusion. These results indicate that RNA duplexes with an alternating C-G sequence can give an unusually large negative CD band in the long wavelength region despite their right-handed helical structure.     

DNA melting investigated by differential scanning calorimetry and Raman spectroscopy.

Thermal denaturation of the B form of double-stranded DNA has been probed by differential scanning calorimetry (DSC) and Raman spectroscopy of 160 base pair (bp) fragments of calf thymus DNA. The DSC results indicate a median melting temperature Tm = 75.5 degrees C with calorimetric enthalpy change delta Hcal = 6.7 kcal/mol (bp), van't Hoff enthalpy change delta HVH = 50.4 kcal/mol (cooperative unit), and calorimetric entropy change delta Scal = 19.3 cal/deg.mol (bp), at the experimental conditions of 55 mg DNA/ml in 5 mM sodium cacodylate at pH 6.4. The average cooperative melting unit (nmelt) comprises 7.5 bp. The Raman signature of 160 bp DNA is highly sensitive to temperature. Analyses of several conformation-sensitive Raman bands indicate the following ranges for thermodynamic parameters of melting: 43 < delta HVH < 61 kcal/mol (cooperative unit), 75 < Tm < 80 degrees C and 6 < (nmelt) < 9 bp, consistent with the DSC results. The changes observed in specific Raman band frequencies and intensities as a function of temperature reveal that thermal denaturation is accompanied by disruption of Watson-Crick base pairs, unstacking of the bases and disordering of the B form backbone. These three types of structural change are highly correlated throughout the investigated temperature range of 20 to 93 degrees C. Raman bands diagnostic of purine and pyrimidine unstacking, conformational rearrangements in the deoxyribose-phosphate moieties, and changes in environment of phosphate groups have been identified. Among these, bands at 834 cm-1 (due to a localized vibration of the phosphodiester group), 1240 cm-1 (thymine ring) and 1668 cm-1 (carbonyl groups of dT, dG and dC), are shown by comparison with DSC results to be the most reliable quantitative indicators of DNA melting. Conversely, the intensities of Raman marker bands at 786 cm-1 (cytosine ring), 1014 cm-1 (deoxyribose ring) and 1092 cm-1 (phosphate group) are largely invariant to melting and are proposed as appropriate standards for intensity normalizations.     

Intensity Changes of Base and Backbone Raman Modes in the B to Z Transition of poly(dG-dm5C)

Abstract

Raman spectroscopy was employed to investigate the temperature-induced B to Z transition of poly(dG-dm-⁵C). The transition midpoint was about 37°C for a solvent containing 20 mM Mg²⁺. A 10-fold change in Mg²⁺ concentration altered the transition midpoint by at least 60°C. Raman spectra of the B and Z forms of poly(dG-dm⁵C) exhibited characteristics similar to those observed with poly(dG-dC). The 682 cm^?1 guanine mode and 835 cm^?1 backbone mode were present in the B conformation. In the Z form the intensities of these two bands decrease substantially and new peaks were observed at 621 cm^?1, 805 and 819 cm¹. Several bands unique to poly(dG-dm⁵C) were also observed. Transition profiles of band intensity vs. temperature were determined for fourteen Raman bands. The curves of all of the base vibrations and one backbone mode had the same slope and midpoint. This indicates that conformational changes in the guanine and methycytosine bases occur concurrently.     

Triple helical polynucleotidic structures: sugar conformations determined by FTIR spectroscopy.

Fourier Transform Infrared Spectra of triple stranded polynucleotides containing homopurine dA or rA and homopyrimidine dT or rU strands have been obtained in H2O and D2O solutions as well as in hydrated films at various relative humidities. The spectra are interpreted by comparison with those of double stranded helixes with identical base and sugar composition. The study of the spectral domain corresponding to in-plane double bond stretching vibrations of the bases shows that whatever the initial duplex characterized by a different IR spectrum (A family form poly rA.poly rU, heternomous form poly rA.poly dT, B family form poly dA.poly dT), the triplexes present a similar IR spectrum reflecting similar base interactions. A particular attention is devoted to the 950-800 cm-1 region which contains marker bands of the sugar conformation in the nucleic acids. In solution the existence of only N (C3'endo-A family form) type of sugar pucker is detected in poly rU.poly rA.poly rU and poly dt.poly rA.poly rU. On the contrary absorption bands characteristic of both N (C3'endo-A family form) and S (C2'endo-B family form) type sugars are detected for poly rU.poly rA.poly dT, poly rU.poly dA.poly dT and poly dT.poly rA.poly dT. Finally mainly S (C2'endo-B family form) type sugars are observed in poly dT.poly dA.poly dT.     

Resolution of parallel and antiparallel oligonucleotide triple helices formation and melting processes by multivariate curve resolution

A procedure is described for the complete resolution of concentration profiles of oligonucleotide triplexes as a function of pH and temperature. The pH and temperature ranges at which triplexes are present and the relative concentrations of all the species involved in acid-base and conformational equilibria are successfully estimated from Multivariate Curve Resolution analysis of UV absorbance spectra recorded along acid-base titrations and melting experiments of single stranded, hairpin and their mixtures. The dependence of formation constants upon pH was successfully estimated. The hairpin h26 (5'-GAAGGAGGAGA-TTTT-TCTCCTCCTTC-3'), and the single stranded oligonucleotides s11CT (5'-CTTCCTCCTCT-3'), s11AG (5'-AGAGGAGGAAG-3') and s11TG (5'-TGTGGTGGTTG-3') were synthesized and their protonation and conformational equilibria were studied in detail. The procedure was shown to be especially useful for the study of triplexes with a low hypochromism upon formation.     

Crystal and solution structures of the B-DNA dodecamer d(CGCAAATTTGCG) probed by Raman spectroscopy: heterogeneity in the crystal structure does not persist in the solution structure

The self-complementary dodecamer d(CGCAAATTTGCG) crystallizes as a double helix of the B form and manifests a Raman spectrum with features not observed in Raman spectra of either DNA solutions or wet DNA fibers. A number of Raman bands are assigned to specific nucleoside sugar and phosphodiester conformations associated with this model B-DNA crystal structure. The Raman bands proposed as markers of the crystalline B-DNA structure are compared and contrasted with previously proposed markers of Z-DNA and A-DNA crystals. The results indicate that the three canonical forms of DNA can be readily distinguished by Raman spectroscopy. However, unlike Z-DNA and A-DNA, which retain their characteristic Raman fingerprints in aqueous solution, the B-DNA Raman spectrum is not completely conserved between crystal and solution states. The Raman spectra reveal greater heterogeneity of nucleoside conformations (sugar puckers) in the DNA molecules of the crystal structure than in those of the solution structure. The results are consistent with conversion of one-third of the dG residues from the C2'-endo/anti conformation in the solution structure to another conformation, deduced to be C1'-exo/anti, in the crystal. The dodecamer crystal also exhibits unusually broad Raman bands at 790 and 820 cm-1, associated with the geometry of the phosphodiester backbone and indicating a wider range of (alpha, zeta) backbone torsion angles in the crystal than in the solution structure. The results suggest that backbone torsion angles in the CGC and GCG sequences, which flank the central AAATTT sequence, are significantly different for crystal and solution structures, the former containing the greater diversity.(ABSTRACT TRUNCATED AT 250 WORDS)     

High pressure fourier transform infrared spectroscopy of poly(dA)poly(dT), poly(dA) and poly(dT)

The effect of hydrostatic pressure upon the DNA duplex, poly(dA)poly(dT), and its component single strands, poly(dA) and poly(dT) has been studied by fourier-transform infrared spectroscopy (FT-IR). The spectral data indicate that at 28 degrees C and pressures up to 12 kbar (1200 MPa) all three polymers retain the B conformation. Pressure causes the band at 967 cm(-1), arising from water-deoxyribose interactions, to shift to higher frequencies, a result consistent with increased hydration at elevated pressures. A larger pressure-induced frequency shift in this band is observed in the single stranded polymers than in the double stranded molecule, suggesting that the effect of pressure on the hydration of single strands may be greater than upon a double stranded complex. A pressure-dependent hypochromicity in the bands attributed to base stacking indicates that pressure facilitates the base stacking in the three polymers, in agreement with previous assessments of the importance of stacking in the stabilization of DNA secondary structure at ambient and high pressures.     

Sequence-dependence of the CD of synthetic double-stranded RNAs containing inosinate instead of guanylate subunits

The CD spectra and melting profiles have been measured for nine synthetic double-stranded RNAs containing I · C instead of G · C base pairs: poly[r(I) · r(C)], poly[r(I-C) · r(I-C)], poly[r(A-I-C) · r(I-C-U)], poly[r(A-C) · r(I-U)], poly[r(A-I) · r(C-U)], poly[r(A-C-C) · r(I-I-U)], poly[r(A-A-C) · r(I-U-U)], poly[r(A-C-U) · r(A-I-U)], and poly[r(A-U-C) · r(I-A-U)]. CD spectra have not previously been reported for the latter six of these polymers. The substitution of inosinate for guanylate led to recognizable CD differences, with all but two of the polymers having two resolved positive bands above 230 nm. Also, the I-containing RNAs differed from their G-containing counterparts in the almost complete absence of negative CD bands at long wavelengths and in the reduction of negative CD bands near 210 nm. First-neighbor comparisons showed that the CD spectra of the I-containing RNAs were consistent with the nearest-neighbor sequences of the polymers, as previously shown for G-containing RNAs (D. M. Gray, J.-J. Liu, R. L. Ratliff, and F. S. Allen, Biopolymers (1981) 20 , 1337–1382). Moreover, two of the first-neighbor comparisons involved spectra of poly[r(A) · r(U)] and poly[r(I) · r(C)], polymers known to be in the A family of conformations in fibers (S. Arnott, D. W. L. Hukins, S. D. Dover, W. Fuller, and A. Hodgson, (1973) J. Mol. Biol. 81 , 107–122). Thus, differences in the CD spectra of I- and G-containing RNAs could be simply explained as resulting from differences in the hypoxanthine and guanine chromophores, without invoking differences in conformation. Finally, melting temperatures of the I-containing RNAs were found to vary much less with base composition than do the melting temperatures of G-containing RNAs, since A · U base pairs are closer to I · C than to G · C base pairs in stability.     

Resonance Raman spectroscopy of complexes of the helix destabilizing proteins GP32 and GP5 with poly(rA) and poly(dA)

The bacteriophage T4 helix destabilizing protein (hdp) gp32 and its complexes with poly(rA) and poly(dA) were studied with ultra-violet resonant Raman spectroscopy. The UV-resonant Raman (UV-RR) spectrum of the complex of gp5, the coat protein of bacteriophage M13, with poly(dA) was also measured and is compared with the spectrum of the gp 32/poly(dA) complex. The excitation wavelength was 245.1 nm. This is on the far UV-side of the first absorption bands of adenine and near a "window" in the protein absorption spectrum. The overlap of fluorescence due to chromophores present in the protein and resonance Raman scattering was prevented by this choice of wavelength. The spectra of the protein/polynucleotide complexes are compared with the native nucleotide spectra measured at varying temperatures. The hyperchromicity which is expected when a nucleotide changes from a stacked to an unstacked conformation was not observed for poly(rA), neither upon temperature increase nor on protein binding. In both cases poly(dA) revealed a clear hyperchromicity. This different behavior of poly(rA) and poly(dA) is probably a consequence of their different conformations. The contributions of the proteins to the spectra is weak except for two bands, at 1550 and 1610 cm-1 due to tryptophan (in case of gp32) and one band near 1610 cm-1 due to tyrosine and phenylalanine.     

Characteristics and variations of B-type DNA conformations in solution: a quantitative analysis of Raman band intensities of eight DNAs

Raman spectra were obtained from four bacterial DNAs varying in GC content and four periodic DNA polymers in 0.1 M NaCl at 25 degrees C. A curve fitting procedure was employed to quantify and compare Raman band characteristics (peak location, height, and width) from 400 to 1600 cm-1. This procedure enabled us to determine the minimum number of Raman bands in regions with overlapping peaks. Quantitative comparison of the Raman bands of the eight DNAs provided several new results. All of the DNAs examined required bands near 809 (+/- 7) and 835 (+/- 5) cm-1 to accurately reproduce the experimental spectra. Since bands at these frequencies are associated with A-family and B-family conformations, respectively, this result indicates that all DNAs in solution have a mixture of conformations on the time scale of the Raman scattering process. Band characteristics in the 800-850-cm-1 region exhibited some dependence on CG content and base pair sequence. As previously noted by Thomas and Peticolas [Thomas, G. A., & Peticolas, W. L. (1983) J. Am. Chem. Soc. 105, 993], the poly[d(A)].poly[d(T)] spectra were qualitatively distinct in this region. The A-family band is clearly observed at 816 cm-1. The intensity of this band and that of the B-family band at 841 cm-1 were similar, however, to intensities in the natural DNA spectra. Three bands at 811, 823, and 841 cm-1 were required to reproduce the 800-850-cm-1 region of the poly[d(A-T)].poly[d(A-T)] spectra. This may indicate the presence of three backbone conformations in this DNA polymer. Analysis of intensity vs. GC content for 42 Raman bands confirmed previous assignments of base and backbone vibrations and provided additional information on a number of bands.     

The structure of triple helical poly(U).poly(A).poly(U) studied by Raman spectroscopy

Using Raman spectroscopy, we examined the ribose-phosphate backbone conformation, the hydrogen bonding interactions, and the stacking of the bases of the poly(U).poly(A).poly(U) triple helix. We compared the Raman spectra of poly(U).poly(A).poly(U) in H2O and D2O with those obtained for single-stranded poly(A) and poly(U) and for double-stranded poly(A).poly(U). The presence of a Raman band at 863 cm-1 indicated that the backbone conformations of the two poly(U) chains are different in the triple helix. The sugar conformation of the poly(U) chain held to the poly(A) by Watson-Crick base pairing is C3' endo; that of the second poly(U) chain may be C2' endo. Raman hypochromism of the bands associated with base vibrations demonstrated that uracil residues stack to the same extent in double helical poly(A).poly(U) and in the triple-stranded structure. An increase in the Raman hypochromism of the bands associated with adenine bases indicated that the stacking of adenine residues is greater in the triple helix than in the double helical form. Our data further suggest that the environment of the carbonyls of the uracil residues is different for the different strands.