Interactions of water-soluble metalloporphyrins with nucleic acids studied by resonance Raman spectroscopy.

The resonance Raman spectra of water-soluble porphyrins, M(TMpy-P4) (M = Cu(II), Ni(II) and Co(III] and their mixtures with poly(dG-dC)2, poly(dA-dT)2 and calf thymus and salmon DNAs were measured using a divided rotating cell to determine the magnitudes of frequency shift and intensity variation resulting from M(TMpy-P4)-nucleic acid interactions. Bands II(C beta-H bending, approximately 1100 cm-1) and VIII(C beta-C beta stretch, approximately 1570 cm-1) show a large and small upward shift, respectively, when Cu(TMpy-P4) and Ni(TMpy-P4) are intercalated at the G-C sites. In contrast, these bands show a small upward and downward shift, respectively, when Co(TMpy-P4) is groove-bound at the A-T sites of nucleic acids. Both Bands V (approximately 1260 cm-1) and IX (approximately 1646 cm-1) which originate in the N-methylpyridyl group always show small downward shifts due to coulombic interaction between the N-CH3+ group of TMpy-P4 and the PO2 group of the nucleic acid.     

Interaction of water-soluble Cu(II), Ni(II), and Co(III) porphyrins with polynucleotides

The interaction of the Cu(II), Ni(II) and Co(III) complexes of the following six water-soluble cationic porphyrins with calf thymus DNA, poly(dG-dC)2 and poly(dA-dT)2 was studied by UV-visible and resonance Raman spectroscopy: tetrakis(2-N-) and (3-N-methylpyridyl) porphyrin (1, 2); monophenyl-tris(4-N-methylpyridyl)porphyrin (4); cis- and trans-diphenyl-bis (4-N-methylpyridyl)porphyrin (5, 6). The binding to nucleic acids was compared with that of tetrakis(4-N-methylpyridyl)porphyrin (3). If the N(+)-CH3 group is moved from the para (3) to the meta position (2), binding of the free porphyrin as well as that of the metal complexes is only gradually modified; thus, the square-planar Cu- and Ni-2 are intercalated at the G-C site whereas Co-2 is groove-bound at A-T. Additionally, Ni-2 is probably also intercalated at the A-T site. When the N(+)-CH3 group is located at ortho position (1), the high rotation barrier of the 2-N-methylpyridyl group prevents intercalation of Cu- and Ni-1, resulting in weak outside binding. At ionic strength mu = 0.2, there is no evidence of significant interaction of Co-1 with any of the polynucleotides. When the charged N-methylpyridyl groups in 3 are subsequently replaced by phenyl groups (4, 5/6), the tendency of the Cu(II) and Ni(II) complexes to bind to the outside of the helix or to intercalate only partially increases at the expense of full intercalation. The coulombic attraction remains strong, no significant differences can be detected between 3, 4, 5, and 6. Ni-4 binds to poly(dA-dT)2 in the same complicated manner as Ni-3. The outside-binding in Co-4, -5 and -6 differs slightly from that in Co-2 and Co-3.     

不同pH条件下细菌视紫红质的共振拉曼光谱研究

本实验测定了不同pH条件下嗜盐菌紫膜中细菌视紫红质(bR)的共振拉曼光谱.13-顺式视黄醛生色团的特征峰1187cm~(-1)和全反式、13-顺式共有的特征峰1200cm~(-1)带强度之比I_(1187)/I_(1200)在pH1.0-8.9之间约为0.76,而pH高于8.9为0.97.pH3.0-9.0时C=NH~ 振动峰为1640-1642cm~(-1),pH9.4以上为1642-1644cm~(-1),pH9.2附近变化最大,pH3.0以下低于1640cm~(-1).酸性和弱碱性范围时,19-CH_3和20-CH_3的面内变形振动与面外变形振动相互重叠,碱性范围分为双峰.并讨论了对结构及其稳定性的影响.     

Resonance Raman spectra of riboflavin and its derivatives in the bound state with egg riboflavin binding proteins

The resonance Raman spectra of riboflavin (RF) and its derivatives, including 3-deuterated (3-D RF), 3-methyl (3-CH3 RF), 3-carboxymethyl (3-CH2COOH RF), and 7,8-dichlororiboflavins (7,8-Cl RF), in H2O and D2O were observed in the 700-1700 cm-1 region. The fluorescence problem of riboflavin was overcome by complex formation of riboflavin with riboflavin binding proteins. The observed frequencies of Raman lines of RF are in good agreement with those of glucose oxidase obtained by Spiro et al. by the resonance CARS method, although the present spectral range is extended to much lower frequency with a higher signal-to-noise ratio than that for glucose oxidase. The observed Raman lines were assigned to the individual ring modes of isoalloxazine on the basis of the Raman spectra of appropriate model compounds such as uracil, pyrazine, and o-xylene. The 1253 cm-1 line of RF was shifted to ca. 1300 cm-1 for 3-D RF, 3-CH3 RF, and 3-CH2COOH RF, and accordingly can be assigned to the CN stretching mode of Ring III. The 1632 cm-1 line of RF was shifted for 7,8-Cl RF and was assigned to a Ring I mode. No Raman line mainly due to C = O stretching mode was observed in the present resonance Raman spectra.     

Application of Raman spectroscopy to biological macromolecules.

The Raman spectra of biological macromolecules arise from molecular vibrations of either the backbone chains or the side chains. The frequencies of the Raman bands lie in a region between 200 cm-1 and 3000 cm-1. From certain frequencies of the vibrations of the backbone chains one can determine the conformation or secondary structure of a macromolecule. Thus for polypeptides and proteins the frequencies of the Amide I and Amide III vibrations allow one to determine the averge conformation of their backbone chain. In polynucleotides and nucleic acids, the frequency of the phosphate diester stretch of the phosphate furanose chain varies between 814 cm-1 for A conformation and 790 cm-1 for B conformation. Raman spectra of the bases in nucleic acids can be used to determine base stacking and hydrogen bonding interactions. Thus Raman spectroscopy is an important tool for determining the conformation structure of proteins and nucleic acids.     

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.     

Interactions of water-soluble porphyrins with hexadeoxyribonucleotides: resonance raman, UV-visible and 1H NMR studies

The interactions of the water-soluble porphyrins M(TMpy-P4) [M = H2, Cu(II), Ni(II), and Co(III); TMpy-P4 = tetrakis(4-N-methylpyridyl)porphyrinato ion], with the hexadeoxyribonucleotides d(CGTACG)2, d(TACGTA)2, d(GCATGC)2, d(TGTGCA)2, and d(CTATAG)2 have been investigated by resonance Raman and/or UV-visible spectroscopy. The results indicate that all hexamers containing the 5'CG3' as well as the 5'GC3' site, and also the mismatched hexamer d(TGTGCA)2, are capable of intercalating the H2, Cu(II) and Ni(II) porphyrins. 1H nuclear magnetic resonance spectra of d(CGTACG)2 mixed with Cu(TMpy-P4) have provided further evidence for the intercalation. For the other cases, outside binding by localized electrostatic interaction is suggested. There is no evidence of groove binding to any of the hexamers. Possible reasons for different binding properties of long and short helices are discussed.     

Haem-rotational disorder in monomeric allosteric cyano-Met insect haemoglobins monitored by resonance Raman spectroscopy

The haem-rotational disorder (insertion of haem into globin rotated about the alpha, gamma-meso axis by 180 degrees) has been investigated in the cyano-Met form of the monomeric allosteric insect haemoglobins, CTT III and CTT IV, by resonance Raman spectroscopy. The effect of haem disorder on the resonance Raman spectra has been observed in proto-IX, deutero-IX, and meso-IX CTTs. Most importantly, in the absence of overlapping vinyl vibrations, we have identified two Fe-C-N bending vibrations at 401 cm-1 and 422 cm-1 (pH 9.5) for 57Fe deutero-IX CTT IV ligated with 13C15N-, which are attributed to the two haem-rotational components. One Fe-C-N bending mode at 422 cm-1 shows a pH-induced shift to 424 cm-1 (pH 5.5) indicating the t----r conformational transition, whereas the other bending mode is pH-insensitive, representing a non-allosteric component. By replacing the unsymmetrical porphyrins with the "symmetrical" protoporphyrin-III we eliminate the haem disorder. Then, sharpening of the Fe-N epsilon(His) (at 313 cm-1) and Fe-CN (at 453 cm-1) stretching modes is observed and a single Fe-C-N bending mode (at 412 cm-1) appears. In cyano-Met proto-IX CTT III two vinyl bending vibrations at 412 cm-1 and 591 cm-1 assigned by deuteration of the vinyl groups also reflect the haem disorder. The 412 cm-1 vinyl vibration is intensity-enhanced via through-space coupling with one of the Fe-C-N bending modes (at 412 cm-1). In the cyano-Met form of proto-III CTT III this vinyl vibration is shifted to 430 cm-1 resulting in a dramatic drop in intensity. It is most likely that the specific vinyl-protein interaction at position 4 in one of the haem-rotational components is the origin of the coupling between the Fe-C-N and vinyl bending modes. The Fe-N epsilon(proximal His) and the Fe-CN stretching vibrations as well as the Fe-C-N bending vibration have been identified by 54Fe/57Fe and 13C15N/12C15N/13C14N/12C14N isotope exchange.     

Stereochemistry modulates the stability of reduced interstrand cross-links arising from R- and S-alpha-CH3-gamma-OH-1,N2-propano-2'-deoxyguanosine in the 5'-CpG-3' DNA sequence

The solution structures of 5'-Cp-N2-dG-3'-R-(alpha)-CH3-propyl-5'-Cp-N2-dG-3' and 5'-Cp-N2-dG-3'-S-(alpha)-CH3-propyl-5'-Cp-N2-dG-3' interstrand DNA cross-links in the 5'-CpG-3' sequence were determined by NMR spectroscopy. These were utilized as chemically stable surrogates for the corresponding carbinolamine interstrand cross-links arising from the crotonaldehyde- and acetaldehyde-derived R- and S-alpha-CH3-gamma-OH-1,N2-propanodeoxyguanosine adducts. The results provide an explanation for the observation that interstrand cross-link formation in the 5'-CpG-3' sequence by the R- and S-alpha-CH3-gamma-OH-1,N2-propanodeoxyguanosine adducts is dependent upon stereochemistry, favoring the R-alpha-CH3-gamma-OH-1,N2-propanodeoxyguanosine adduct [Kozekov, I. D., Nechev, L. V., Moseley, M. S., Harris, C. M., Rizzo, C. J., Stone, M. P., and Harris, T. M. (2003) J. Am. Chem. Soc. 125, 50-61]. Molecular dynamics calculations, restrained by NOE-based distances and empirical restraints, revealed that both the 5'-Cp-N2-dG-3'-R-(alpha)-CH3-propyl-5'-Cp-N2-dG-3' and 5'-Cp-N2-dG-3'-S-(alpha)-CH3-propyl-5'-Cp-N2-dG-3' cross-links were located in the minor groove and retained Watson-Crick hydrogen bonds at the tandem cross-linked C.G base pairs. However, for the 5'-Cp-N2-dG-3'-R-(alpha)-CH3-propyl-5'-Cp-N2-dG-3' cross-link, the (alpha)-CH3 group was positioned in the center of the minor groove, whereas for the 5'-Cp-N2-dG-3'-S-(alpha)-CH3-propyl-5'-Cp-N2-dG-3' cross-link, the (alpha)-CH3 group was positioned in the 3' direction, showing steric interference with the DNA helix. The 5'-Cp-N2-dG-3'-S-(alpha)-CH3-propyl-5'-Cp-N2-dG-3' cross-link exhibited a lower thermal stability as evidenced by NMR spectroscopy as a function of temperature. The two cross-links also exhibited apparent differences in the conformation of the interstrand three-carbon cross-link, which may also contribute to the lower apparent thermodynamic stability of the 5'-Cp-N2-dG-3'-S-(alpha)-CH3-propyl-5'-Cp-N2-dG-3' cross-link.     

Metal-ligand vibrations of cyanoferric myeloperoxidase and cyanoferric horseradish peroxidase: evidence for a constrained heme pocket in myeloperoxidase

The low-frequency FeCN vibrations of cyanoferric myeloperoxidase (MPO) and horseradish peroxidase (HRP) have been measured by resonance Raman spectroscopy. The ordering of the frequencies of the predominantly FeC stretching and FeCN bending normal vibrational modes in the two peroxidases differs. These normal mode vibrations are identified by their wavenumber shifts upon isotopic substitution of the cyanide ligand. For MPO, the stretching mode nu 1 (361 cm-1) occurs at a lower frequency than the bending mode delta 2 (454 cm-1). For HRP, the order is reversed as nu 1 (456 cm-1) is at a higher frequency than delta 2 (404 cm-1). Normal coordinate analyses and model complexes have been used to address the origin of this behavior. The nu 1 stretching frequencies in cyanide complexes of iron porphyrin and iron chlorin model compounds are similar to one another and to that of HRP. Thus, the inverted order and altered frequencies of the nu 1 and delta 2 vibrations in MPO, relative to those in HRP and the model compounds, are not inherent to the proposed iron chlorin prosthetic group in MPO but, rather, are attributed to distinct distal environmental effects in the MPO active site. The normal coordinate analyses for MPO and HRP showed that the nu 1 and delta 2 vibrational frequencies are not pure; the potential energy distributions for these modes respond not only to the geometry but also to the force constants of the nu(FeC) and delta(FeCN) internal coordinates.(ABSTRACT TRUNCATED AT 250 WORDS)     

Z form of poly d(A-C).poly d(G-T) in solution studied by Raman spectroscopy.

Poly d(A-C).poly d(G-T) structures have been studied in solution by Raman spectroscopy, in presence of Na+, Mn2+ and Ni2+ counterions. Increase of the Na+ concentration or addition of Mn2+ ions up to 1M MnCl2 does not modify the B geometry of the polynucleotide. On the contrary, in conditions of low water activity (4M NaCl), the presence of small amounts of nickel ions (65 mM) induces a left-handed geometry of the DNA. The shift of the guanine line located at 682 cm-1 in B form to 622 cm-1 reflects unambiguously the C2'-endo/anti-greater than C3'-endo/syn reorientation of the deoxyribose-purine entities. Moreover modifications in the phosphate backbone lines indicate that the polymer is in a Z conformation. New or displaced lines corresponding to adenosine vibrations are correlated with the left-handed structure. An interaction of the Ni2+ ions specifically with the N7 site of purines, combined with a low water activity is necessary to promote the B-greater than Z transition.     

Resonance Raman spectra of anionic semiquinoid form of a flavoenzyme, D-amino acid oxidase

Resonance Raman (RR) spectra of the complex of anionic semiquinoid D-amino acid oxidase (DAO) with picolinate in H2O and D2O were observed in the 300-1,750 cm-1 region. RR spectra were also measured for the complex of the semiquinoid enzyme reconstituted with isotopically labeled FAD's, i.e., [4a-13C]-, [4,10a-13C2]-, [2-13C]-, [5-15N]-, and [1,3-15N2]-FAD. On the basis of the isotope effects, tentative assignments of the observed bands of the anionic semiquinoid flavin were made. The spectra differ from those of oxidized, neutral semiquinoid, and anionic reduced flavins previously reported. The 1,602 cm-1 band was not shifted for any FAD labeled in ring II and/or ring III and was assigned to a ring I mode. The 1,516 cm-1 band underwent an isotopic shift upon [4a-13C]- or [4,10a-13C2]-labeling. The band was assigned to the mode containing C(4a)-C(10a) stretching. The 1,331 and 1,292 cm-1 bands shifted upon [4a-13C]- or [5-15N]-labeling and were assigned to the modes containing C(4a)-N(5) stretching. The 1,217 and 1,188 cm-1 bands were assigned to the skeletal vibrations of ring III coupled with the N(3)-H bending mode. The RR spectrum of the complex of anionic semiquinoid DAO with alpha-iminopropionate or N-methyl-alpha-iminopropionate was essentially identical with that of the complex with picolinate.     

Characterization of DNA structures by Raman spectroscopy: high-salt and low-salt forms of double helical poly(dG-dC) in H2O and D2O solutions and application to B, Z and A-DNA.

Raman spectra of poly(dG-dC) . poly(dG-dC) in D2O solutions of high (4.0M NaCl) and low-salt (0.1M NaCl) exhibit differences due to different nucleotide conformations and secondary structures of Z and B-DNA. Characteristic carbonyl modes in the 1600-1700 cm-1 region also reflect differences in base pair hydrogen bonding of the respective GC complexes. Comparison with A-DNA confirms the uniqueness of C = O stretching frequencies in each of the three DNA secondary structures. Most useful for qualitative identification of B, Z and A-DNA structures are the intense Raman lines of the phosphodiester backbone in the 750-850 cm-1 region. A conformation-sensitive guanine mode, which yields Raman lines near 682, 668, or 625 cm-1 in B (C2'-endo, anti), A (C3'-endo, anti) or Z (C3'-endo, syn) structures, respectively, is the most useful for quantitative analysis. In D2O, the guanine line of Z-DNA is shifted to 615 cm-1, permitting its detection even in the presence of proteins.     

The significance of the 2' OH group and the influence of cations on the secondary structure of the RNA backbone.

In the IR spectra, the coupling of vibrations leads to band splitting and/or bands shifting in opposite directions which provides information on the mutual orientation of groupings. From such band shifts in the range 1800 to 1500 cm-1 one can draw conclusions on the double helix formation of polynucleotides. These band shifts are caused either by vibrational coupling of stretching vibrations within pairs of base residues or by coupling of stretching vibrations with the bending (scissor) vibration of the -NH2 groups; the latter is indicated by band shifts after deuterium substitution within the amino groups. Couplings of phosphate and 1 ibose vibrations in the range 1300 to 1000 cm-1 provide information on the secondary structure of the backbone. In order to obtain information of the structure of the RNA backbone, the IR spectra of poly(ribonucleotides) were studied in neutral media in which they were single-stranded. The shift due to coupling of the band of the 2'OD bending vibration and that of the antisymmetric stretching vibration of the ether group of the ribose residue proves that ribose residues of the backbone are cross-linked via hydrogen bonds. These are formed between the 2'OD or 2'OH groups, respectively, and the O atoms of the ether group of the neighboring ribose residues. This is the reason for the difference between DNA and RNA as regards the 2'OH group. The structure formation caused by these hydrogen bonds results in a stiffening of the RNA backbone. The tendency to form these hydrogen bonds increases in the order poly (U), poly(C), poly (A). This order of secondary structure stabilization is due to an interplay between the influences of (1) the 2'OH hydrogen bonds and (2) the base residues' stacking. Furthermore, the coupling of the antisymmetric stretching vibration of the greater than PO2- groups with a vibration involving the 2'OH group can result in a doublet structure of the band at about 1240 cm-1 if cations with strong fields are present. This probably shows that these cations can turn the greater than PO2-groups-which are usually turned outward at the backbone, as shown by construction of molecular models- towards the basic residues. Thus they cause stiff monohelices which are right-handed screws.     

IR spectroscopic studies of major cellular components. III. Hydration of protein,nucleic acid,and phospholipid films

The IR absorption spectra of protein, DNA, RNA, and phospholipid films as a function of the water content are reported. We find that the hydration of protein films affects the peak intensity of amide I and amide II bands and the shape of the amide III band. For nucleic acids, the symmetric (nu(S) PO(2) (-)) and antisymmetric (nu(AS) PO(2) (-)) stretching vibrations of the phosphate linkage are the most affected by hydration, because both intensity changes and frequency shifts are observed. The spectra of phospholipid films are also sensitive to hydration, and they exhibit changes in the peak intensities and frequencies of both nu(S) PO(2) (-) and nu(AS) PO(2) (-) vibrations. We interpret the spectral differences between water saturated and dried films both in terms of structural changes and the change in the local dielectric in the vicinity of the polar and solvent exposed groups. In addition, we observe that the most significant change in the absorption intensity, frequency, and shape of the water sensitive vibrations occurs at high hydration levels. The principal component analysis of hydration results and the kinetics of water removal from sample films are also discussed. In addition, protein spectra acquired using film and KBr pellet sampling techniques are compared.     

Resonance Raman studies of the flavin and iron-sulfur centers of milk xanthine oxidase

Resonance Raman spectroscopy has been used to study milk xanthine oxidase, an enzyme containing molybdenum, binuclear iron-sulfur clusters, and FAD as cofactors. The contribution of FAD dominates the resonance Raman spectrum at frequencies above 500 cm-1. As expected, no bands assignable to FAD are observed in deflavo xanthine oxidase. The resonance Raman spectrum below 500 cm-1 reveals the contribution of the Fe2S2(Cys)4 groups with frequencies similar to those of adrenodoxin and putidaredoxin. Resonance enhancement profiles of the Fe2S2(Cys)4 clusters indicate intensity variations among the Fe2S2(Cys)4 peaks that are attributed to different excitation wavelength maxima of their bridging and terminal iron-sulfur vibrations. No evidence for Mo-ligand vibrations could be obtained by using excitation wavelengths between 363.8 and 514.5 nm.     

Direct evidence for singlet-singlet energy transfer in Escherichia coli DNA photolyase.

The active form of native Escherichia coli DNA photolyase contains 1,5-dihydro-FAD (FADH2) plus 5,10-methenyltetrahydropteroylpolyglutamate [5,10-CH(+)-H4Pte(Glu)n]. Enzyme containing FADH2 and/or 5,10-methyltetrahydrofolate (5,10-CH(+)-H4folate) can be prepared in reconstitution experiments. Fluorescence quantum yield measurements at various wavelengths with native or reconstituted enzyme provide a simple method for detecting singlet-singlet energy transfer from pterin to FADH2, a key step in the proposed catalytic mechanism. The data satisfy the following criteria: (1) Wavelength-independent quantum yield values are observed for 5,10-CH(+)-H4folate in the absence (0.434) or presence (3.57 X 10(-2)) of FADH2, for 5,10-CH(+)-H4Pte(Glu)n in the presence of FADH2 (5.58 X 10(-2)) and for FADH2 in the absence of pterin (5.34 X 10(-3)); (2) The observed decrease in pterin fluorescence quantum yield in the presence of FADH2 can be used to estimate the efficiency of pterin fluorescence quenching (EQ = 0.918 or 0.871 with 5,10-CH(+)-H4folate or 5,10-CH(+)-H4Pte(Glu)n, respectively); (3) The fluorescence quantum yield of FADH2 is increased in the presence of pterin and varies depending on the excitation wavelength, in agreement with the predicted effect of energy transfer on acceptor fluorescence quantum yield [phi acceptor (+ donor)/phi acceptor (alone) = 1 + EET(epsilon donor/epsilon acceptor), where EET is the efficiency of the energy transfer process]. With 5,10-CH(+)-H4Pte(Glu)n in native enzyme the value obtained for EET (0.92) is similar to EQ, whereas with 5,10-CH(+)-H4folate in reconstituted enzyme the value obtained for EET (0.46) is 2-fold smaller than EQ.(ABSTRACT TRUNCATED AT 250 WORDS)     

Vibrational analysis of nucleic acids. I. The phosphodiester group in dimethyl phosphate model compounds: (CH3O)2PO2-, (CD3O)2PO2-, and (13CH3O)2PO2-.

Normal coordinate analyses and vibrational assignments are presented for the dimethyl phosphate anion [(CH3O)2PO2-] and its deuteriomethyl [(CD3O)2PO2-] and carbon-13 [(13CH3O)2PO2-] derivatives in the gauche-gauche conformation. The dimethyl phosphate anion, which is the simplest model for the nucleic acid phosphodiester moiety, exhibits many of the spectral complexities of DNA and RNA and has previously resisted a complete and consistent vibrational analysis. In the present study we make use of new experimental data on the dimethyl phosphate isotopomers, including Raman depolarization measurements, to develop a consistent valence force field for normal modes of the C--O--P--O--C phosphodiester network and its hydrogenic substituents, as well as for stretching and bending modes of the O--P--O network of the anionic phosphodioxy group (PO2-). The force field established for dimethyl phosphate incorporates one significant nonbonded force constant, introduced from ab initio calculations, to account for interaction between the two ester C--O bonds. This study resolves previous problematic assignments for conformation-sensitive symmetric (in-phase) and asymmetric (out-of-phase) skeletal stretching modes of the ester linkages and demonstrates substantial anharmonicity in the hydrogen-stretching vibrations of the methyl substituents. New assignments are proposed for Raman bands of the phosphodioxy group, which may serve as potential indicators of structure and interaction of the DNA phosphates.     

Synthesis of 1-(2-deoxy-beta-D-ribofuranosyl)-2,4-difluoro-5-substituted-benzenes: "thymine replacement" analogs of thymidine for evaluation as anticancer and antiviral agents

A group of unnatural 1-(2-deoxy-beta-D-ribofuranosyl)-2,4-difluorobenzenes having a variety of C-5 two-carbon substituents [-C...C-X, X = I, Br; -C...CH; (E)-CH=CH-X, X = I, Br; -CH=CH2; -CH2CH3; -CH(N3) CH2Br], designed as nucleoside mimics, were synthesized for evaluation as anticancer and antiviral agents. The 5-substituted (E)-CH=CH-I and -CH2CH3 compounds exhibited negligible cytotoxicity in a MTT assay (CC50 = 10(-3) to 10(-4)M range), relative to thymidine (CC50 = 10(-3) to 10(-5)M range), against a variety of cancer cell lines. In contrast, the C-5 substituted -C...C-I and -CH(N3)CH2Br compounds were more cytotoxic (CC50 = 10(-5) to 10(-6)M range). The -C...C-I and -CH2CH3 compounds exhibited similar cytotoxicity against non-transfected (KBALB, 143B) and HSV-1 TK+ gene transfected (KBALB-STK, 143B-LTK) cancer cell lines expressing the herpes simplex virus type 1 (HSV-1) thymidine kinase gene (TK+). This observation indicates that expression of the viral TK enzyme did not provide a gene therapeutic effect. The parent group of 5-substituted compounds, that were evaluated using a wide variety of antiviral assay systems [HSV-1, HSV-2, varicella-zoster virus (VZV), vaccinia virus, vesicular stomatitis, cytomegalovirus (CMV), and human immunodeficiency (HIV-1, HIV-2) viruses], showed that this class of unnatural C-aryl nucleoside mimics are inactive and/or weakly active antiviral agents.     

Study of the hydratation of the double-helical poly A-poly U complex by IR-spectroscopy and piezogravimetry methods

IR-spectra of a double-helical poly A-poly U complex and coiled poly U were studied at various r.h. in a 900-3800 cm-1 region. By the method of piezomicrobalance hydration isotherms for these polynucleotides were obtained. It is concluded that, as in the DNA case, simultaneous hydration of nucleic bases the backbone of polynucleotides occurs at lower r.h., and that the poly A-poly U hydration level is higher than poly A and poly U ones separately. Drastic changes in spectral parameters of poly A poly U uracil and adenine in-ring and out-of-ring absorption bands observed in 44-76% r.h. region were interpreted as a transition to helical conformation of the complex. Calculation of resonance frequencies for these normal vibrations in the dipole-dipole approximation agrees with the experimental data.