Vacuum ultraviolet circular dichroism of double stranded nucleic acids

Synchrotron-Radiation Vacuum-Ultraviolet Circular-Dichroism Spectroscopy for Characterizing the Structure of Saccharides

Circular-dichroism (CD) spectroscopy is a powerful tool for analyzing the structures of chiral molecules and biomolecules. The development of CD instruments using synchrotron radiation has greatly expanded the utility of this method by extending the spectra to the vacuum-ultraviolet (VUV) region below 190 nm and thereby yielding information that is unobtainable by conventional CD instruments. This technique is especially advantageous for monitoring the structure of saccharides that contain hydroxy and acetal groups with high-energy transitions in the VUV region. Combining VUVCD spectra with theoretical calculations provides new insight into the contributions of anomeric hydroxy groups and rotational isomers of hydroxymethyl groups to the dynamics, intramolecular hydrogen bonds, and hydration of saccharides in aqueous solution.

Synchrotron-radiation vacuum-ultraviolet circular dichroism spectroscopy in structural biology: an overview

Circular dichroism spectroscopy is widely used for analyzing the structures of chiral molecules, including biomolecules. Vacuum-ultraviolet circular dichroism (VUVCD) spectroscopy using synchrotron radiation can extend the short-wavelength limit into the vacuum-ultraviolet region (down to ~160 nm) to provide detailed and new information about the structures of biomolecules in combination with theoretical analysis and bioinformatics. The VUVCD spectra of saccharides can detect the high-energy transitions of chromophores such as hydroxy and acetal groups, disclosing the contributions of inter- or intramolecular hydrogen bonds to the equilibrium configuration of monosaccharides in aqueous solution. The roles of hydration in the fluctuation of the dihedral angles of carboxyl and amino groups of amino acids can be clarified by comparing the observed VUVCD spectra with those calculated theoretically. The VUVCD spectra of proteins markedly improves the accuracy of predicting the contents and number of segments of the secondary structures, and their amino acid sequences when combined with bioinformatics, for not only native but also nonnative and membrane-bound proteins. The VUVCD spectra of nucleic acids confirm the contributions of the base composition and sequence to the conformation in comparative analyses of synthetic poly-nucleotides composed of selected bases. This review surveys these recent applications of synchrotron-radiation VUVCD spectroscopy in structural biology, covering saccharides, amino acids, proteins, and nucleic acids.

On the formation of the double helix between adenine single strands at acidic pH from synchrotron radiation circular dichroism experiments

Here, we present synchrotron radiation circular dichroism spectra for a series of DNA adenine strands, (dA)(n) , n = 2-10, 15, at acidic pH. Reference spectra of a protonated single strand, (dAH(+) )(n) , and a protonated double helix, (dAH(+) )(n) :(dAH(+) )(n) , are provided in the wavelength region from 175 to 330 nm. The largest spectral difference between single and double strands is in the vacuum ultraviolet, where a band changes sign. This new spectral feature that characterizes double helix formation may be useful for analytical purposes but also for shedding light on the underlying complexation mechanism. Furthermore, we find that a minimum of eight or nine bases in a strand is needed for two (dAH(+) )(n) strands to form a duplex. This is a relatively high number as compared with guanine quadruplex and cytosine i-motif formation, which is likely linked to the significant Coulomb repulsion between the all-protonated bases. Finally, spectra recorded as a function of time after sample preparation indicates that the equilibrium is slowly reached, in certain cases taking an hour or more.

Vacuum-ultraviolet circular dichroism spectroscopy of DNA: a valuable tool to elucidate topology and electronic coupling in DNA

Circular dichroism (CD) is a powerful technique to obtain information on electronic transitions and has been used extensively for studies on DNA. Most experiments are done in the UV region but new information is often revealed from extending the wavelength region down into the vacuum ultraviolet (VUV) region. Such experiments are most easily carried out with synchrotron radiation (SR) light sources that provide large photon fluxes. Here we provide a summary of the SRCD data taken on different DNA strands with emphasis on results from our own laboratory within the last five years.(1-3) Signal intensities in the VUV are often significantly larger than those in the UV, and the electronic coupling between bases may increase with excitation energy. CD spectroscopy is particularly useful for investigating the extent of electronic coupling within a strand, i.e., the degree of delocalisation of the excited-state electronic wavefunction. The spatial extent of the wavefunction may be limited to just one base or it extends over two or more bases in a stack or between bases on different strands.(4,5) The actual character of the electronically excited state is linked to base composition and sequence as well as DNA folding motif (A-, B-, Z-DNA, triplexes, quadruplexes, etc.). The latter depends on experimental conditions such as solution acidity, temperature, ionic strength, and solvent.

Fingerprints of bonding motifs in DNA duplexes of adenine and thymine revealed from circular dichroism: synchrotron radiation experiments and TDDFT calculations

Synchrotron radiation circular dichroism (SRCD) spectra were recorded for a family of 12 DNA duplexes that all contain nine adenines (A) and nine thymines (T) in each strand but in different combinations. The total number of AT Watson-Crick (WC) base pairs is constant (18), but the number of cross-strand (CS) hydrogen bonds between A and T varies between 0 and 16, the maximum possible. Eleven of the duplexes have one or more A tracts, and one duplex has T tracts. The signals due to hybridization were found from subtraction of spectra of single strands from spectra of the duplexes. The residual spectrum of the T-tract duplex T(9)A(9):A(9)T(9) (5'-3':3'-5') significantly differs from that of the A-tract duplex A(9)T(9):T(9)A(9), but only below 210 nm, which suggests that the signal in this region depends on the superhelicity of the duplex. A principal component analysis of all residual spectra reveals that spectra of A-tract duplexes can be obtained to a good approximation as a linear combination of just two basis spectra. The first component is assigned to the spectrum of 18 WC and 8 CS pairs, whereas the second component is that of 8 CS pairs. This interpretation is supported by separate experiments on duplexes of varying lengths but with similar arrangements of the A and T's and by experiments on two other duplex families of 14 and 30 base pairs. The best correlation is obtained by the assumption that cross-strand interactions occur as long as there are two adenine neighbors in a strand. Our data indicate that a circular dichroism spectrum of a duplex containing only A and T can simply be inferred from the number of WC base pairs and the number of CS interactions, and we provide reference spectra for these two interactions. Finally, time dependent density functional theory calculations of the circular dichroism spectra for an isolated WC base pair and two different CS base pairs (between adenine N-6 amine and thymine O-4 or between adenine C-2-H and thymine O-2) were performed to provide some additional support for the interpretation of the experimental spectra. We find large differences between the two calculated CS spectra. However, there is a reasonable qualitative agreement between the calculated WC and the C-2-H...O-2 CS spectra and those deduced from the experimental data.

Synchrotron radiation circular dichroism spectroscopy of proteins: secondary structure, fold recognition and structural genomics

Recent developments in instrumentation and bioinformatics show that the technique of synchrotron radiation circular dichroism spectroscopy can provide novel information on protein secondary structures and folding motifs, and has the potential to play an important role in structural genomics studies, both as a means of target selection and as a high-throughput, low-sample-requiring screening method. This is possible because of the additional information content in the low-vacuum ultraviolet wavelength data obtainable with intense synchrotron radiation light sources, compared with that present in spectra from conventional lab-based circular dichroism instruments.

An A-form of poly[d(A-C)].poly[d(G-T)] induced by mercury (II) as studied by UV and FTIR spectroscopies

The conformational changes of poly[d(A-C)].poly[d(G-T)] induced by Hg(ClO4)2 in aqueous solution have been studied using UV absorption and fourth derivative spectrophotometries, and FTIR spectroscopy. The UV absorption and fourth derivative spectra reflect changes in the polynucleotide stacking interactions as a result of the metal-polynucleotide interaction. The fourth derivative spectra do not indicate a Z-form either at low or at high metal-to-polynucleotide ratios. Furthermore, the infrared spectrum at high metal-to-polynucleotide ratio (r = 1.2; r = [Hg(ClO4])2/[nucleotide] molar ratio) has the main features of an A-form, in contrast with previous CD studies which proposed that the polynucleotide adopts a Z-form under these conditions. The nature of a different conformation of the polynucleotide induced at low r-ratios (r < or = 0.2) is discussed.

Flow linear dichroism and Fourier transform IR spectra reveal geometry for X-form DNA

Flow linear dichroism measurements extended into the vacuum uv region yield inclinations for the base normal from the helix axis of 21 degrees for dA and 40 degrees for dT in the X-form of poly(dAdT).poly(dAdT). These inclination angles are similar to the B form of the synthetic polymer, but the axes around which the bases incline are different. Hydrogen-bonded base pairs are consistent with the geometry for the standard B, C, D, and Z forms of natural DNA, but will not fit into the A form. Fourier transform ir spectra indicate that the X form has sugar pucker and phosphate geometry similar to B-form DNA, and supports the dinucleotide repeat with two kinds of phosphates seen in earlier work, in analogy to Z-form DNA. Clearly, X-form DNA has a unique geometry.

Volume changes correlate with entropies and enthalpies in the formation of nucleic acid homoduplexes: differential hydration of A and B conformations

We have used a combination of densimetric, calorimetric, and uv absorption techniques to obtain a complete thermodynamic characterization for the formation of nucleic acid homoduplexes of known sequence and conformation. The volume change delta V accompanying the formation of four duplexes was interpreted to reflect changes in hydration based on the electrostriction phenomenon. In 10 mM sodium phosphate buffer at pH 7, the magnitude of the measured delta V's ranged from -2.0 to +7.2 ml/mol base pair and followed the order of poly(rA).poly(dT) approximately poly(dA).poly(dT) < poly(rA).poly(dU) approximately poly(rA).poly(rU). Inclusion of 100 mM NaCl in the same buffer gave the range of -17.4 to -2.3 mL/mol base pair and the following order: poly(dA).poly(dT) < poly(rA).poly(dT) < poly(rA).poly(rU) approximately poly(rA).polyr(dU). Standard thermodynamic profiles of forming these duplexes from their corresponding complementary single strands indicated similar free energies that resulted from the compensation of favorable enthalpies with unfavorable entropies along with a similar counterion uptake at both ionic strengths. The differences in these compensating effects of entropy and enthalpy correlated very well with the volume change measurements in a manner suggesting that the homoduplexes in the B conformation are more hydrated than are those in the A conformation. Moreover, the increased thermal stability of these homoduplexes resulted from an increase in the salt concentration corresponding to larger hydration levels as reflected by the delta V results.

The vacuum UV CD spectra of G.G.C triplexes

Vacuum UV circular dichroism (CD) spectra were measured down to 175 nm for d(C)10, d(G)10, the d(G)10.d(C)10 duplex, and the d(G)10.d(G)10.d(C)10 triplex. A CD difference spectrum was calculated for d(G)10.d(C)10 giving the change in CD induced by forming the duplex from d(G)10 and d(C)10. The d(G)10.d(G)10.d(C)10 CD difference spectrum gave the CD induced by triplex formation from binding of d(G)10 to the d(G)10.d(C)10 duplex. In the near-UV, the d(G)10.d(C)10 and d(G)10.d(G)10.d(C)10 difference spectra resembled the difference spectrum for poly[r(G).r(C)] (Biopolymers 29, 325-333). This similarity may be an indication of similar purine base stacking. The d(G)10.d(G)10.d(C)10 vacuum UV difference spectrum had a negative band at 195 nm and a positive band at 180 nm, making it similar to difference spectra for homopolymer triplexes containing T.A.T and U.A.U triplets (Nucl. Acids Res. 19, 2275-2280). The appearance of these bands in difference spectra should be good indicators of triplex formation. The complementary oligonucleotides c-mycI d(CCCCACCCTCCC) and c-mycII d(GGGAGGGTGGGG) are part of the regulatory sequences of the human c-myc gene. G.G.C rich triplexes formed by binding c-mycII or c-mycIII d(GGGGTGGGTGGG) to the c-mycI.c-mycII duplex had CD difference spectra similar to that of d(G)10.d(G)10.d(C)10 in both the vacuum UV and near UV regions, indicating similar triplet structures.

Differential hydration of homopurine sequences relative to alternating purine/pyrimidine sequences

The minor groove ligand distamycin A has been used to probe the relative hydration of the minor groove of eight synthetic polynucleotides of known sequence and composition. A combination of densimetric, calorimetric, and temperature-dependent spectroscopic techniques have been used to obtain complete thermodynamic profiles (delta Gzero, delta Hzero, delta Szero, and delta Vzero) for the association of distamycin A to all polymer duplexes. In 10 mM phosphate buffer, pH 7, binding of the drug to each of the polymeric duplexes resulted in characteristic negative changes in both the volume and enthalpy. Although the binding constants were found to be identical for pairs of isomer polynucleotides having identical compositions but different sequences, the values of delta Hzero, delta Szero, and delta Vzero of each such pair were remarkably different. The entropy changes were found to roughly parallel the volume changes; no such trend was seen between delta Hzero and delta Vzero. The data support the hypothesis that the volume changes observed for these systems reflect the coulombic-hydration contribution to the entropy. The heteropolymer duplexes generated much larger exothermic contributions, less favorable entropies and larger volume contractions than did the corresponding homopolymer duplexes of identical composition, and strongly suggest that polynucleotides with homopurine sequences are more hydrated than polynucleotides with alternating purine/pyrimidine sequences. In addition, it was found that duplexes containing guanine sharply reduced the affinity for the drug, also lowering the exothermicity but raising the entropy. This may be explained by the presence of an amino group in the minor groove that prevents hydrogen bonding. Substitution of the guanine with inosine reversed this trend in the thermodynamic properties. Furthermore, substitution of poly(dA) for poly(rA) in a duplex produced a similar reduction in the affinity, while raising the exothermic contribution and greatly reducing the favorable entropy effect in agreement with an apparent increase in the hydration state.

Multivalent ions are necessary for poly[d(AC).d(GT)] to assume the Z form: a CD study

In previous work, it was shown that poly[d(AC).d(GT)] could be forced into the Z form by strong dehydrating conditions, provided EDTA was not present. Presumably multivalent impurities were also necessary for the transition. In order to gain control over the B to Z transition for this DNA, we carefully removed all divalent contaminants from the sample and asked the obvious question: What ions are necessary for the transition under dehydrating conditions? We systemically investigated the effect of various multivalent ions. The common contaminants Ca2+, Mg2+, and Fe3+ will not cause the transition, but Co2+ and Ni2+ facilitate the transition, undoubtedly because of their well-known propensity to bind to purine N7. Since the transition also depends on the synergistic dehydrating action of sodium perchlorate and ethanol, we include CD spectra for the independent variations of these two factors. In addition, vacuum-uv CD spectra for the A form and various B forms of poly[d(AC).d(GT)] are presented for the first time.

B to Z transitions of the short DNA hairpins formed from the oligomer sequences: d[(CG)3X4(CG)3] (X = A, T, G, C)

Circular Dichroism (CD) spectra were collected as a function of sodium perchlorate concentration [NaClO4] for the set of DNA hairpins formed from the oligomer sequences d[(CG)3X4(CG)3] where X = A, T, G or C. Over the range in salt concentration from 0 to 4.0 M NaClO4, the CD spectra invert in a manner characteristic of the B to Z transition. A factor analysis routine is described and employed to determine the least number of basis spectra required to fit the measured spectra of each hairpin over the entire salt range examined. In every case, linear combinations of only two sub-spectra fit the experimental spectra of the hairpins with greater than 98% accuracy, indicating the spectrally monitored structural transitions are two-state. From the relative weights of the individual sub-spectra, B-Z transition curves are constructed. The transitions are analyzed in terms of a simple two-state equilibrium model which yields an evaluation of the transition free-energy, delta GB-Z, as a function of NaClO4 concentration. At 1.0 M NaClO4 and 21 degrees C, delta GB-Z = 5.4, 4.9, 3.6 and 2.3 kcal/mole for the G4, T4, A4 and C4 loop hairpins, respectively.

The vacuum UV CD bands of repeating DNA sequences are dependent on sequence and conformation

CD spectra were obtained for eight synthetic double-stranded DNA polymers down to at least 175 nm in the vacuum uv. Three sets of sequence isomers were studied: (a) poly[d(A-C).d(G-T)] and poly[d(A-G).d(C-T)], (b) poly[d(A-C-C).d(G-G-T)] and poly[d(A-C-G).d(C-G-T)], and (c) poly[d(A).d(T)], poly[d(A-T).d(A-T)], poly[d(A-A-T).d(A-T-T)], and poly[d(A-A-T-T).d(A-A-T-T)]. There were significant differences in the CD spectra at short wavelengths among each set of sequence isomers. The (G.C)-containing sequences had the largest vacuum uv bands, which were positive and in the wavelength range of 180-191 nm. There were no large negative bands at longer wavelengths, consistent with the polymers all being in right-handed conformations. Among the set of sequences containing only A.T base pairs, poly[d(A).d(T)] had the largest vacuum uv CD band, which was at 190 nm. This CD band was not present in the spectra of the other (A.T)-rich polymers and was absent from two first-neighbor estimations of the poly[d(A).d(T)] spectrum obtained from the other three sequences. We concluded that the sequence dependence of the vacuum uv spectra of the (A.T)-rich polymers was due in part to the fact that poly[d(A).d(T)] exists in a noncanonical B conformation.

A.U and G.C base pairs in synthetic RNAS have characteristic vacuum UV CD bands

The vacuum UV CD spectra of GpC, CpG, GpG, poly[r(A)], poly[r(C)], poly[r(U)], poly[r(A-U)], poly[r(G).r(C)], poly[r(A).r(U)], and poly[r(A-U).r(A-U)] were measured down to at least 174 nm. These spectra, together with the published spectra of poly[r(G-C).r(G-C)], CMP, and GMP, were sufficient to estimate the CD changes upon base pairing for four double-stranded RNAs. The vacuum UV CD bands of poly[r(A)], poly[r(C)], and the dinucleotides GpC and CpG were temperature dependent, suggesting that they were due to intrastrand base stacking. The dinucleotide sequence isomers GpC and CpG had very different vacuum UV CD bands, indicating that the sequence can play a role in the vacuum UV CD of single-stranded RNA. The vacuum UV CD bands of the double-stranded (G.C)-containing RNAs, poly[r(G).r(C)] and poly[r(G-C).r(G-C)], were larger than the measured or estimated vacuum UV CD bands of their constituent single-stranded RNAs and were similar in having an exceptionally large positive band at about 185 nm and negative bands near 176 and 209 nm. These similarities were enhanced in difference-CD spectra, obtained by subtracting the CD spectra of the single strands from the CD spectra of the corresponding double strands. The (A.U)-containing double-stranded RNAs poly[r(A).r(U)] and poly[r(A-U).r(A-U)] were similar only in that their vacuum UV CD spectra had a large positive band at 177 nm. The spectrum of poly[r(A).r(U)] had a shoulder at 188 nm and a negative band at 206 nm, whereas the spectrum of poly[r(A-U).r(A-U)] had a positive band at 201 nm. On the other hand, difference spectra of both of the (A.U)-containing polymers had positive bands at about 177 and 201 nm. Thus, the difference-CD spectra revealed CD bands characteristic of A.U and G.C base pairing. (ABSTRACT TRUNCATED AT 250 WORDS)

Interaction of the antitumor antibiotic mitomycin C with Z-DNA

Mitomycin C (MC), an antitumor antibiotic, alkylated Z-DNAs such as poly(dG-dC)/Co(NH3)3+(6), poly(dG-m5dC)/Mg2+ and brominated poly(dG-dC) upon reductive activation. Computer-generated energy-minimized molecular models indicated that monofunctional alkylation of Z-DNA at the N2-position of guanine by MC did not distort Z-DNA geometry, but bifunctional alkylation, leading to interstrand crosslinks between two N2-positions of guanine was sterically unfavorable. The above three Z-DNA's were exposed both to monofunctionally and bifunctionally activated MC in separate experiments and the resulting covalent MC-polynucleotide complexes were examined for conformation and for covalent MC-adducts, by circular dichroism (CD) spectroscopy and HPLC analysis of nuclease digests, respectively. Monofunctionally activated MC alkylated all three polynucleotides in their Z-forms, resulting in the same monofunctional N2-guanine adduct as that known to be formed with B-DNA. Upon bifunctional activation of MC, poly(dG-dC/Co(NH3)3+(6) reverted to the B-form and bifunctional (cross-link) adducts were detected, identical again with those formed with B-DNA. Poly(dG-m5dC), however, remained in the Z-form after the alkylation and only a monofunctional adduct could be detected. It was concluded that Z-DNA is subject to monofunctional alkylation by MC but cannot be cross-linked. The latter process occurs only when the Z-DNA is labile enough [as is in the case of poly(dG-dC)] to have some B-form in equilibrium at the site of the first formed monolinked adduct; the cross-linking then occurs at such local B-sites, pulling the overall B in equilibrium Z equilibrium irreversibly to the left. These results are in accord with the predictions from the above modeling. The irreversible "lock" by the MC cross-link on B-DNA may be exploited for probing Z-DNA intermediacy in various DNA functions.

Vacuum UV circular dichroism is diagnostic for the left-handed Z form of poly [d(A-C).d(G-T)] and other polydeoxynucleotides

Circular dichroism spectra are extended into the vacuum UV to about 178 nm for four polydeoxynucleotides of various sequences capable of assuming the left-handed Z form. It is found that each of these polymers, including those with brominated bases and those with the four different bases, have a characteristic negative feature at short wavelengths when in the Z form. In contrast, the B form only has a positive band between 180 and 200 nm. Furthermore, a blue shift of the short wavelength crossover is diagnostic of the B- to Z-form transition for all polymers studied so far. These results confirm that poly[d(A-C).d(G-T)] can assume the Z form in solution at low concentration.