Raman and infrared studies of nucleosides at high pressures: I. Adenosine.

Room temperature Raman and infrared (IR) spectra of crystalline adenosine at pressures between 1 atm and 10 GPa are reported. Vibrational modes were identified through assignments in the literature. Many modes were found to increase in frequency with pressure; however, some irregularities were observed. Discontinuities were observed in numerous Raman and IR modes near 2.5 GPa, indicating a phase transition. The modes associated with the glycosidic bond shift significantly down in frequency near this pressure, suggesting a weakening of the associated bond. The IR modes associated with hydrogen-stretching motions were found to decrease in frequency with pressure.     

Mid-Infrared Study of Deoxyadenosine at High Pressures: Evidence of Phase Transitions

Abstract

Room temperature mid-infrared experiments between 500 and 1800 cm^?1 have been performed on crystalline deoxyadenosine as a function of pressure up to about 10 GPa. Discontinuities observed near 2 and 4 GPa indicate that two separate phase transitions occur at these pressures. Changes in the spectra suggest that both transitions involve a rearrangement of the pucker of the deoxyribose moiety. The wavenumbers of the vibrational modes shift to higher values with applied pressure. Our results for deoxyadenosine are compared to similar measurements on adenosine. Assignments for the observed modes are made on the basis of work published in the literature.     

Raman and infrared studies of nucleosides at high pressures: II. Cytidine

Raman and mid-infrared (MIR) spectra have been recorded for crystalline cytidine at pressures up to 10 GPa at room temperature. Broadening and positive wavenumber shifts are observed for most of the Raman and MIR peaks with increasing pressure. However, some of the MIR peaks associated with hydrogen-stretching modes display a negative wavenumber shift as a result of charge transfer effects. Evidence of a phase transition near 4 GPa is presented and attributed to a change in the conformation of the five membered sugar ring.     

Vibrational Analysis of Phosphorothioate DNA: II. The POS Group in the Model Compound Dimethyl Phosphorothioate [(CH3O)2(POS)]-

Abstract

The results of Raman and Infrared (IR) spectroscopic investigations on the vibrational modes of dimethyl phosphorothioate (DMPS) anion, [(CH₃O)₂(POS)]^?, are reported. Ab initio calculations of the vibrational modes, the IR and Raman spectra and the interatomic force constants of DMPS were performed. A normal mode calculation was performed and the results were used to calculate the potential energy distribution for the vibrational modes. This analysis shows that in DMPS the P-S stretching mode has a frequency of about 630 cm^?1 and an angle bending mode involving the sulfur atom has a frequency of about 440 cm^?1. The proposed vibrational mode assignments will serve as marker bands in the conformational studies of phosphorothioate oligonucleotides which play a central role in the novel antisense therapeutic paradigm.     

Frecuencia y características del síndrome metabólico y de la resistencia a la insulina en familiares de primer grado de personas con diabetes mellitus tipo 1

AimTo determine the frequency of metabolic syndrome (MS) and insulin resistance (IR) in first-degree relatives of type 1 diabetic patients (FDR1) and to study the relationship between these two disorders and some clinical, biochemical and immunological characteristics.Subjects and methodsWe studied 289 persons, of which 193 were children/adolescents and 96 were adults. Weight, height, waist and hip circumference, blood pressure, blood glucose, insulin, cholesterol, triglycerides, high-density lipoprotein-cholesterol, glutamic acid decarboxylase autoantibodies (GADA) and tyrosine phosphatase autoantibodies were determined. IR was assessed through the insulin resistance index (HOMA-IR). The criteria of the World Health Organization for adults and the Cuban consensus for children and adolescents were used to define MS.ResultsThe prevalence of MS in child and adolescent FDR1 was 5.7% (11/193) while IR was found in 24.9% (48/193). For adult FDR1, the frequency of MS was 6.2% (6/96) and that of IR was 14.6% (14/96). Interestingly, an association was found between IR and MS in adults but not in children and adolescents. IR was more frequent in children and adolescents than in adults (p<0.05). The presence of GADA was associated with IR but not with MS (p<0.05).ConclusionsThe frequency of MS in child and adolescent FDR1 was similar to that found in the general population according to studies using similar definitions of MS. In contrast, the frequency of MS in adults was lower than that reported in Cuba for the first-degree relatives of patients with type 2 diabetes. IR was not only associated with MS in first-degree relatives. The association of IR with the presence of GADA may reflect the fact that β cell hyperactivity increases autoantigen expression.     

Pressure-tuning infrared and Raman spectra of trans-dichloro-bis[(diperfluoroethyl)phenylphosphine]platinum(II), trans-Pt[PPh(CF3CF2)2]2Cl2

Infrared and Raman spectra of solid trans-dichloro-bis[diperfluoroethyl(phenyl)phosphine]platinum(II), trans-Pt[PPh(CF₃CF₂)₂]₂Cl₂, have been studied at high external pressures up to ∼50 kbar with the aid of a diamond-anvil cell. A gradual, pressure-induced phase transition, most probably second order, was observed in the 21-34 kbar pressure range. In the IR spectra, the bands assigned to the CF stretching modes of the CF₃ groups exhibit larger pressure sensitivities than do those associated with the CF stretching modes of the CF₂ groups, most probably because of their physical location on the outside in the molecules in the unit cell. The fairly high pressure sensitivities of the symmetric PtCl stretching mode in both the low and high pressure phases (0.46 and 37 cm⁻¹/kbar, respectively) are considered to reflect the low force constant associated with the long PtCl bond length thus making this vibration more susceptible to compression.     

Resonance raman spectroscopy of iron (3)--ovotransferrin and iron (3)--human serum transferrin

We report the resonance Raman spectra in the frequency range 300–1800 cm^?1 of Fe (III)-ovotransferrin and Fe (III)-human serum transferrin in aqueous solution at about 10^?4M protein concentration. This is the first observation of resonance Raman scattering ascribable to amino acid ligand vibrational modes of a nonheme iron protein. The resonance Raman spectra of the transferrins are similar except that the resonance band near 1270 cm^?1 is shifted to a higher frequency for Fe(III)-human serum transferrin than that for Fe(III)-ovotransferrin. The resonance Raman bands observed near 1170, 1270, 1500 and 1600 cm^?1 may reflect resonance enhancement of p-hydroxy-phenyl frequencies of tyrosine residues and/or imidazolium frequencies of histidine residues.     

A Raman study of low frequency intrahelical modes in A-, B-, and C-DNA.

We have obtained low frequency (less than 200 cm-1) Raman spectra of calf-thymus DNA and poly(rI).poly(rC) as a function of water content and counterion species and of d(GGTATACC)2 and d(CGCGAATTCGCG)2 crystals. We have found that the Raman scattering from water in the first and second hydration shells does not contribute directly to the Raman spectra of DNA. We have determined the number of strong Raman active modes by comparing spectra for different sample orientations and polarizations and by obtaining fits to the spectra. We have found at least five Raman active modes in the spectra of A- and B-DNA. The frequencies of the modes above 40 cm-1 do not vary with counterion species, and there are only relatively small changes upon hydration. These modes are, therefore, almost completely internal. The mode near 34 cm-1 in A-DNA is mostly internal, whereas the mode near 25 cm-1 is dominated by interhelical interactions. The observed intensity changes upon dehydration were found to be due to the decrease in interhelical distance. Polymer length appears to play a role in the lowest frequency modes.     

Description of Base Motion and Role of Excitations in the Melting of Poly(dG) · Poly(dC)

Abstract

We study the contribution of various vibrational modes to the melting of poly(dG) · poly(dC). We find that the principal contribution comes from the H-bond breathing modes that have been observed in Raman scattering and that we have associated with helix melting. We show the softening of these modes on approach to melting in agreement with the observed behavior. We also describe the contribution to melting from base rotation modes that others have suggested are important in melting.     

Low-frequency vibrational spectra of some homopolypeptides in the solid state

Low-frequency Raman and far-infrared spectra of polyglycine, poly-L -alanine, and poly-L -valine have been measured. The Raman spectra exhibit an intense band near 100 cm^?1 for these homopolypeptides. Lattice calculations of the polyglycines are used to assign the intense Raman band to a rotary lattice mode. For homopolypeptides in the β conformation, an infrared band is observed whose frequency varies inversely with the square root of the mass of the peptide repeating unit. This infrared band is assigned to the hydrogen bond stretching lattice vibration.     

The Infrared and Raman Spectra of the Duplex of d(GGTATACC) in the Crystal Show Bands Due to Both the A-form and the B-form of DNA

Abstract

The deoxyoligonucleotide, d(GGTATACC), forms a duplex structure that crystallizes in the DNA A form. This has been shown by both X-ray diffraction studies and Raman spectroscopy (1,2). The presence of the DNA B form has been reported using diffuse X-ray scattering from a crystal of the closely related sequence d(GGBrUABrUACC)(3). In this paper the infrared spectrum of the d(GGTATACC) crystal is presented and curve resolution of both the Raman and IR spectra have been carried out. The percentage of A and B forms have been estimated. The %B form in the crystal has been estimated from the IR spectra to be about 15% and from Raman to be about 20%. Moreover the IR spectrum of the A conformation in the crystal is slightly different from the IR spectrum of the A conformation in polynucleotide fibers in particular in the region of the phosphate stretching vibrations and of the in-plane double bond vibrations of the bases. We show that it is feasible to obtain IR as well as Raman spectra of small crystals of oligonucleotides and that this is a good method of identifying all of the different conformations that may be in the crystal.     

Pressure-induced improvement in symmetry and change in electronic properties of SnSe

To explore the structural and electronic properties of SnSe under pressure, we applied hydrostatic pressure from 0 to 8 GPa to a fully relaxed SnSe cell sample based on plane-wave pseudopotential density functional theory. The calculated results indicate that the structure of SnSe changes gradually from an irregular zigzag structure with low symmetry to a B1-like structure with regular arrangement and high symmetry under pressure. The lattice parameters and cell volume of SnSe decrease monotonically as the applied pressure increases. The energy band gap of SnSe becomes narrow under pressure and is finally closed at 6.1 GPa. Moreover, we found that SnSe exhibits non-magnetic and semi-metallic features based on analyzing its electronic state density and spin state density. This can be attributed to the decrease in the lattices constants and the enhancement of the Sn–Se bond interaction under pressure, which causes the density of electronic states to increase near the Fermi surface. Finally, the charge distribution between Se–Sn–Se along the c-axis changes gradually from asymmetric to symmetric as the pressure is increased to 6.1 GPa and beyond. This implies that enhancement of the structure symmetry of SnSe can lead to a symmetrical distribution of charges, which further affects the bonding characteristics of the Sn–Se bond.     

Sequence and temperature dependence of the interbase hydrogen-bond breathing modes in B-DNA polymers: Comparison with low-frequency Raman peaks and their role in helix melting

We carry out temperature-dependent lattice dynamics calculations to determine the vibrational normal modes associated with the interbase H-bond breathing motion in several B-DNA copolymers at temperatures from room temperature to the melting temperatures. We take into consideration Raman selection rules and incorporate a simple empirical model of Raman susceptibility in the interbase H bonds in our calculation and compare them to Raman measurements. Our calculations are carried out using empirical force constants that are not further refined to low-frequency spectra. Our calculations show the existence of strong interbase H-bond breathing modes at frequencies and with relative oscillator strengths close to the observed Raman peaks in the range of 60–140 cm^?1 for the DNA sequences considered except for one helix. The correlation between the calculated and observed frequencies and oscillator strengths indicates that the observed Raman peaks in the frequency range are likely interbase H-bond breathing modes. We find that these modes exhibit sizable temperature as well as sequence dependence. We show the softening of these modes on approaching thermal denaturation that is also in agreement with the observed behavior in Raman and melting measurements. The sensitivity of the calculation on the empirical model of Raman susceptibility and the possible reasons for the discrepancy between a few calculated values and observations are discussed. © 1995 John Wiley & Sons, Inc.     

Mid-infrared study of deoxycytidine at high pressures: evidence of a phase transition

Room temperature mid-infrared experiments between 600 and 1600 cm(-1) have been performed on crystalline deoxycytidine as a function of pressure up to about 10 GPa. The wavenumbers of most vibrational modes shift to higher values with increasing pressures except for a mode near 840 cm(-1). Assignments for the observed modes are made on the basis of work published in the literature. Several anomalies are noted near 4.7 GPa, suggesting a phase transition. Our results for deoxycytidine are compared to similar measurements on cytidine.     

Effect of high external pressures on the vibrational spectra of crystalline dichloro(1,5-cycloctadiene)platinum(II), Pt(η-C8H12)Cl2

The effects of high external pressures on the principal IR and Raman bands of crystalline dichloro(1,5-cycloctadiene)platinum(II), Pt(COD)Cl₂ (COD = η⁴-C₈H₁₂), have been investigated for pressures up to ∼30 kbar by diamond-anvil cell microspectroscopy. This square-planar Pt(II) complex does not undergo any pressure-induced structural change throughout the pressure range investigated and the pressure dependences (dν/dP) for the vibrational modes range from −0.18 to 0.79 cm⁻¹ kbar⁻¹. The negative dν/dP value observed for the IR band at 1426 cm⁻¹ (−0.18 cm⁻¹ kbar⁻¹) suggests that this band is chiefly associated with a CC stretching mode of the Pt-COD group. This observation provides yet another indication that high-pressure vibrational spectroscopy may indeed be a general method for establishing the presence of π-backbonding in organometallic complexes, such as metal carbonyls and alkenes.     

Ab initio study of phenyl benzoate: structure,conformational analysis,dipole moment,IR and Raman vibrational spectra

The molecular structure (bond distances and angles), conformational properties, dipole moment and vibrational spectroscopic data (vibrational frequencies, IR and Raman intensities) of phenyl benzoate were calculated using Hartree–Fock (HF), density functional (DFT), and second order Møller–Plesset perturbation theory (MP2) with basis sets ranging from 6-31G* to 6-311++G**. The theoretical results are discussed mainly in terms of comparisons with available experimental data. For geometric data, good agreement between theory and experiment is obtained for the MP2, B3LYP and B3PW91 levels with basis sets including diffuse functions. The B3LYP/6-31+G* theory level estimates the shape of the experimental functions for phenyl torsion around the Ph–O and Ph–C bonds well, but reproduces the height of the rotational barriers poorly. The B3LYP/6-31+G* harmonic force constants were scaled by applying the scaled quantum mechanical force field (SQM) technique. The calculated vibrational spectra were interpreted and band assignments were reported. They are in excellent agreement with experimental IR and Raman spectra.Figure Calculated and experimental (GED) potential energy functions for torsional motion of phenyl benzoate relative to the minimum value. a The potential function for torsion about the O₃–C₄ bond. b The potential function for torsion about the C₂–C₁₀ bond.     

Molecular Dynamics Simulation of Structural Phase Transition of AlPO4 Induced by Pressure

Abstract

The mechanism of pressure-induced phase transition of AlPO₄ has been investigated by means of a molecular dynamics method of constant temperature and pressure. A new crystalline phase with space group C2, which has not yet been experimentally found, appears by an instantaneous compression of 60, 70 and 80 GPa at 300 K. At high temperature (2500 K) and pressure (58 GPa), another new phase of AlPo₄ (y-phase), which is composed of PO₆ and AlO₆ octahedra, has been observed.     

Mid-infrared study of deoxyadenosine at high pressures: evidence of phase transitions

Room temperature mid-infrared experiments between 500 and 1800 cm(-1) have been performed on crystalline deoxyadenosine as a function of pressure up to about 10 GPa. Discontinuities observed near 2 and 4 GPa indicate that two separate phase transitions occur at these pressures. Changes in the spectra suggest that both transitions involve a rearrangement of the pucker of the deoxyribose moiety. The wavenumbers of the vibrational modes shift to higher values with applied pressure. Our results for deoxyadenosine are compared to similar measurements on adenosine. Assignments for the observed modes are made on the basis of work published in the literature.     

DFT study of structure and vibrational spectra of ceramide 3: comparison to experimental data

The Fourier transform Raman and infrared (IR) spectra of the Ceramide 3 (CER3) have been recorded in the regions 200–3500 cm^? 1 and 680–4000 cm^? 1, respectively. We have calculated the equilibrium geometry, harmonic vibrational wavenumbers, electrostatic potential surfaces, absolute Raman scattering activities and IR absorption intensities by the density functional theory with B3LYP functionals having extended basis set 6-311G. This work is undertaken to study the vibrational spectra of CER3 completely and to identify the various normal modes with better wavenumber accuracy. Good consistency is found between the calculated results and experimental data for the IR and Raman spectra.     

Theory of Low-Frequency Vibrations in DNA Macromolecules

Abstract

To describe low-frequency dynamics of DNA macromolecules a model is developed taking into account the hydrogen bond stretching in base pairs, the backbone flexibility and intranucleoside mobility. For double-stranded DNA the normal vibrations are found and the structure of low- frequency spectrum is determined. The agreement between theory and Raman spectroscopy data for B-DNA is demonstrated. Conformational dependences of vibration spectrum during the B→A and helix→coil DNA transitions are studied. The contribution coming from low-frequency mobility to the nucleic-protein recognition processes is discussed.