Raman and Infrared Studies of Nucleosides at High Pressures: I. Adenosine

Abstract

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.     

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.     

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.     

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.     

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.     

The effects of high pressure upon ligated and deoxyhemoglobins and myoglobin. An optical spectroscopic study

The effects of high pressure (0.1-3.4 gigapascal (GPa)) on the ferrous heme active sites of human adult hemoglobin, sperm whale myoglobin, and Glycera dibranchiata hemoglobin (Fraction II) were probed using resonance Raman and absorption spectroscopies. High-to-low spin transitions of the heme iron occur for hemoglobin, myoglobin, and Glycera hemoglobin at 0.35, 0.75, and 0.50 GPa, respectively, for the deoxy species. These interspecies differences result from variations in the composition of the hemepockets and/or their rigidity to pressure-induced volume changes. Heme active sites initially bound to CO or O2 exhibit distinctive behavior at high pressures. For all proteins studied, O2 apparently dissociates from the heme at only moderately high pressure, while CO remains bound to the heme moiety even at extreme pressures. The Raman spectra demonstrate the differences in the ligated and deoxy species at 3.4 GPa in the high frequency region. Discrete changes (i.e. iron spin-state transitions and dissociation of O2) occur that are commensurate with the collapse of the distal pocket, while continuous shifts in the absorption and Raman spectra are observed at pressures above those required for pocket collapse.     

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.     

Resonance Raman evidence for the mechanism of the allosteric control of O2-binding in a cobalt-substituted monomeric insect hemoglobin.

The substitution of iron for cobalt in the monomeric insect hemoglobin CTT (Chironomus thummi thummi) III does not alter the Bohr effect for O2-binding. The cobalt substitution in this hemoglobin allows us to identify not only the O-O and Co-O2 stretching mode but also the Co-O-O bending mode by resonance Raman spectroscopy. The assignments were made via 16O2/18O2 isotope exchange. The modes associated with the Co-O-O moiety are pH-dependent. These pH-induced changes of the resonance Raman spectra are correlated with the t = r conformation transition. At high pH (high-affinity state) two unperturbed O-O stretching modes are observed at 1,068 cm-1 (major component) and 1,093 cm-1 (minor component) for the 18O2 complex. These frequencies correspond to split modes at 1,107 cm-1 and 1,136 cm-1 and an unperturbed mode at approximately 1,153 cm-1 for the 16O2 complex. At low pH (low-affinity state) the minor component becomes the major component and vice versa. The Co-O2 stretching frequency varies for approximately 520 cm-1 (pH 5.5) to 537 cm-1 (pH 9.5) indicating a stronger (hence shorter) Co-O2 bond in the high-affinity state. On the other hand, the O-O bond is weakened upon the conversion of the low- to the high-affinity state. The Co-O-O bending mode changes from 390 cm-1 (pH 9.5) to 374 cm-1 (pH 5.5). In the deoxy form the resonance Raman spectra are essentially pH-insensitive except for a vinyl mode at 414 cm-1 (pH 5.5), which is shifted to 416 cm-1 (pH 5.5).     

Pressure effects on the proximal heme pocket in myoglobin probed by Raman and near-infrared absorption spectroscopy.

The influence of high pressure on the heme protein conformation of myoglobin in different ligation states is studied using Raman spectroscopy over the temperature range from 30 to 295 K. Photostationary experiments monitoring the oxidation state marker bands demonstrate the change of rebinding rate with pressure. While frequency changes of vibrational modes associated with rigid bonds of the porphyrin ring are <1 cm(-1), we investigate a significant shift of the iron-histidine mode to higher frequency with increasing pressure (approximately 3 cm(-1) for deltaP = 190 MPa in Mb). The observed frequency shift is interpreted structurally as a conformational change affecting the tilt angle between the heme plane and the proximal histidine and the out-of-plane iron position. Independent evidence for iron motion comes from measurements of the redshift of band III in the near-infrared with pressure. This suggests that at high pressure the proximal heme pocket and the protein are altered toward the bound state conformation, which contributes to the rate increase for CO binding. Raman spectra of Mb and photodissociated MbCO measured at low temperature and variable pressure further support changes in protein conformation and are consistent with glasslike properties of myoglobin below 160 K.     

Resonance Raman evidence for tyrosine involvement in the radical site of galactose oxidase

Resonance Raman data are reported for the redox-activated form of galactose oxidase from Dactylium dendroides. Excitation within the red (659 nm) and blue (457.9 nm) absorption bands leads to strong resonance enhancement of ligated tyrosine vibrational modes at 550, 1170, 1247, 1484, and 1595 cm-1. The ring mode frequencies are unusually low, indicating a decreased bond order in the ring. The spectra clearly differ in both frequencies and relative intensities from those characteristic of known aromatic pi-radicals. Enhancement of tyrosine ring modes on excitation within absorption bands previously associated with the presence of the radical in the active site suggests that the ligated tyrosine residue is present in the radical site and may stabilize this radical species through formation of a charge transfer complex. A dramatically different Raman spectrum is observed for the N3- adduct of galactose oxidase, exhibiting a single strong 1483 cm-1 feature. The intense visible-near IR absorption bands for galactose oxidase may derive from transitions within a charge transfer complex between an aromatic free radical and a tyrosine-copper complex.     

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.     

Low frequency Raman spectra of Z-DNA

We have performed a Raman study of the low frequency modes in three oligo- and polynucleotides in Z-conformation, and we compare the spectra of these samples to those of two polynucleotides in B-conformation. In Z-DNA we find 5 intrahelical modes below 200 cm-1, in addition to the interhelical mode near 30 cm-1 which is only observed in crystalline samples. The most prominent intrahelical mode has a frequency of about 105 cm-1, close to the frequency of the strongest intrahelical mode in A-and B-DNA. The sequence dependence of the frequency of this mode is considerably larger than for the same mode in B-DNA. The other modes are less pronounced, and their frequency variations with base sequence are within the experimental accuracy.     

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.     

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.     

Flavin and heme structures in lactate:cytochrome c oxidoreductase: a resonance Raman study

Resonance Raman spectra of Hansenula anomala L-lactate:cytochrome c oxidoreductase (or flavocytochrome b2), of its cytochrome b2 core, and of a bis(imidazole) iron-protoporphyrin complex were obtained at the Soret preresonance from the oxidized and reduced forms. Raman contributions from both the isoalloxazine ring of flavin mononucleotide (FMN) and the heme b2 were observed in the spectra of oxidized flavocytochrome b2. Raman diagrams showing frequency differences of selected FMN modes between aqueous and proteic environments were drawn for various flavoproteins. These diagrams were closely similar for flavocytochrome b2 and for flavodoxins. This showed that the FMN structure must be very similar in both types of proteins, despite their very different proteic pockets. However, the electron density at this macrocycle was found to be higher in flavocytochrome b2 than in these electron transferases. No significant difference was observed between the heme structures in flavocytochrome b2 and in cytochrome b2 core. The porphyrin center-N(pyrrole) distances in the oxidized and reduced heme b2 were estimated to be 1.990 and 2.022 A from frequencies of porphyrin skeletal modes, respectively. The frequency of the vinyl stretching mode of protoporphyrin was found to be very affected in resonance Raman spectra of flavocytochrome b2 and of cytochrome b2 core (1634-1636 cm-1) relative to those observed in the spectra of iron-protoporphyrin [bis(imidazole)] complexes (1620 cm-1). These specificities were interpreted as reflecting a near coplanarity of the vinyl groups of heme b2 with the pyrrole rings to which they are attached. The low-frequency regions of resonance Raman indicated that the iron atoms of the four hemes b2 are in the porphyrin plane whatever their oxidation state. The histidine-Fe-histidine symmetric stretching mode was located at 205 cm-1 in the spectra of flavocytochrome b2 and of cytochrome b2 core. It was insensitive to the iron oxidation state and indicated strong Fe-His bonds in both states.     

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.     

Vibrational analysis of the all-trans retinal protonated Schiff base.

We have obtained Raman spectra of a series of all-trans retinal protonated Schiff-base isotopic derivatives. 13C-substitutions were made at the 5, 6, 7, 8, 9, 10, 11, 12, 13, 14, and 15 positions while deuteration was performed at position 15. Based on the isotopic shifts, the observed C--C stretching vibrations in the 1,100-1,400 cm-1 fingerprint region are assigned. Normal mode calculations using a modified Urey-Bradley force field have been refined to reproduce the observed frequencies and isotopic shifts. Comparison with fingerprint assignments of all-trans retinal and its unprotonated Schiff base shows that the major effect of Schiff-base formation is a shift of the C14--C15 stretch from 1,111 cm-1 in the aldehyde to approximately 1,163 cm-1 in the Shiff base. This shift is attributed to the increased C14--C15 bond order that results from the reduced electronegativity of the Schiff-base nitrogen compared with the aldehyde oxygen. Protonation of the Schiff base increases pi-electron delocalization, causing a 6 to 16 cm-1 frequency increase of the normal modes involving the C8--C9, C10--C11, C12--C13, and C14--C15 stretches. Comparison of the protonated Schiff base Raman spectrum with that of light-adapted bacteriorhodopsin (BR568) shows that incorporation of the all-trans protonated Schiff base into bacterio-opsin produces an additional approximately 10 cm-1 increase of each C--C stretching frequency as a result of protein-induced pi-electron delocalization. Importantly, the frequency ordering and spacing of the C--C stretches in BR568 is the same as that found in the protonated Schiff base.