Interpretation of DNA Vibration Modes: IV - A Single-Helical Approach to Assign the Phosphate-Backbone Contribution to the Vibrational Spectra in A and B Conformations

Abstract

A calculated approach based on the Higgs method for assigning the vibration modes of an infinite helicoidal polymeric chain has been performed on the basis of a reliable valence force field. The calculated results allowed the phosphate-backbone marker modes of the A and B forms, to be interpreted. In the dynamic models used, the bases have been omitted and no interchain interaction was considered. The calculation can also interprete quite satisfactorily the characteristic Raman peaks and infrared bands in the 1250-700 cm^?1 spectral region arising from the sugar or sugar-phosphate association and reproduce their evolution upon the B→A DNA conformational transition. They clearly show that the phosphate- backbone modes in the above mentioned spectral region constitute the optical branches of the phonon dispersion curves with no detectable variation in the first Brillouin-zone.     

Absolute configuration determination and conformational analysis of (−)‐(3S,6S)‐3α,6β‐diacetoxytropane using vibrational circular dichroism and DFT techniques

The absolute configuration of semisynthetic (?)‐3α,6β‐acetoxytropane 1 , prepared from (?)‐6β‐hydroxyhyoscyamine 2 , has been determined using vibrational circular dichroism (VCD) spectroscopy. The vibrational spectra (IR and VCD) were calculated using DFT at the B3LYP/DGDZVP level of theory for the eight more stable conformers which account for 99.97% of the total relative abundance in the first 10 kcal/mol range. The calculated VCD spectra of all considered conformations showed two distinctive spectral ranges, one between 1300 and 1200 cm^?1, and the other one in the 1150–950 cm^?1 region. When compared with the experimental VCD spectrum, the first spectral region confirmed the calculated conformational preferences, whereas the second region showed little change with conformation, thus allowing the determination of the absolute configuration of 1 as (3S,6S)‐3α,6β‐diacetoxytropane. Also, the bands in the second region showed similarities between 1 and 2 in both the experimental and calculated VCD spectra, suggesting that these bands are mainly related to the absolute configuration of the rigid tropane ring system, since they show conformational independency, no variations with the nature of the substituent, and are composed by closely related vibrational modes. Chirality, 2010. © 2009 Wiley‐Liss, Inc.     

Experimental Study on Localized Surface Plasmon Mode Hybridization in the Near and Mid Infrared

We investigate plasmon excitations within a regular grating of double-layered gold/insulator nanoparticles in the infrared and visible spectral region. Provided a flat gold film as substrate, strong coupling between the localized surface plasmon modes and their image-like excitations in the metal is observed. The interaction results in a strong red shift of the plasmon mode as well as the splitting of the modes into levels of different angular momenta, often referred to as plasmon hybridization. The diameters of the nanoparticles are designed in a way that the splitting of the resonances occurs in the spectral region between 0.1 and 1 eV, thus being accessible using an infrared microscope. Moreover, we investigated the infrared absorption signal of gratings that contain two differently sized nanoparticles. The interaction between two autonomous localized surface plasmon excitations is investigated by analyzing their crossing behavior. In contrast to the interaction between localized surface plasmons and propagating plasmon excitations which results in pronounced anticrossing, the presented structures show no interaction between two autonomous localized surface plasmons. Finally, plasmon excitations of the nanostructured surfaces in the visible spectral region are demonstrated through photographs acquired at three different illumination angles. The change in color of the gratings demonstrates the complex interaction between propagating and localized surface plasmon modes.     

Hydrogen lines in the infrared region and spectral background for the thomson scattering diagnostics of the iter divertor plasma

Calculations are made of the plasma spectral background, which is important for the Thomson scattering diagnostics in the ITER divertor. Theoretical grounds have been elaborated for computing the hydrogen spectral line shapes in the infrared spectral region for a divertor plasma in ITER. The shape of the P-7 Paschen line (transition n = 7 → n = 3) located near the laser scattering signal has been calculated for various lines of sight in the ITER divertor. Contributions from different mechanisms of broadening the P-7 line have been examined. The spectral intensities of bremsstrahlung and photorecombination continuum have been calculated. All calculations use data on the spatial distribution of temperatures and densities of all species of plasma particles computed with the SOLPS4.3 code for basic operation regimes of the ITER divertor.     

A critical review of the nucleosidic vibration modes appearing in the 800-500-cm-1 spectral region, based on new harmonic dynamics calculations

On the basis of a harmonic dynamics calculation, it is shown that in the 800–500-cm^?1 spectral region of DNA vibrational spectra, the characteristic Raman peaks and ir bands do not arise from the same nucleosidic motions. The Raman spectra involve mainly the ring-breathing modes of nucleic bases while the ir spectra reveal essentially their out-of-plane vibrations. Moreover, the calculated results show the splitting of the guanine- and adenine-residue breathing modes upon their coupling with the sugar-pucker motions. This fact is in agreement with the poly[d(G-C)] and poly[d(A-T)] Raman spectra.     

Vibrational circular dichroism of A-, B-, and Z-form nucleic acids in the PO2-stretching region.

Vibrational circular dichroism (VCD) spectra were measured for H2O solutions of several natural and model DNAs (single and double strands, oligomers and polymers) in the B-form, poly(dG-dC)-poly(dG-dC) in the Z-form, and various duplex RNAs in an A-form over the PO2-stretching region. Only the symmetric PO2 stretch at approximately 1075 cm-1 yields a significant intensity VCD signal. Differences of the PO2-stretching VCD spectra found for these conformational types are consistent with the spectral changes seen in the base region, but no sequence dependence was seen in contrast to VCD for base modes. The B to Z transition is accompanied by an inversion of the PO2- VCD spectra, which is characteristic of the change in the helical sense of the nucleic acid backbone. A-RNAs give rise to the same sense of couplet VCD as do B-DNAs but have a somewhat different shape because of overlapping ribose modes. These PO2- VCD spectral characteristics have been successfully modeled using simple dipole coupling calculations. The invariability of the symmetric PO2- stretching mode VCD spectra to the base sequence as opposed to that found for the C = O stretching and base deformation modes is evidence that this mode will provide a stable indication of the DNA helical sense.     

CD of nucleic acids: III. Calculated CD of RNAs from new A, U, G, and C transition-moment parameters

New adenine (A) and uracil (U) π → π* transition-moment parameters have been derived from a recently developed semiempirical procedure. Using conformational energy probabilities based on the Boltzmann equation, the new parameters were assigned by optimizing the calculated CD of cyclic nucleotides against measured CD. The derived A-and U-parameters (along with guanine and cytosine parameters derived previously by the same procedure) have been assessed in CD spectral calculations of some polyribonucleic acid sequences, in assumed A-class geometries. Comparisons have been made between CD spectra calculated from the newly derived parameters and those calculated from parameters obtained from a combination of crystal optical measurements and quantum-mechanical calculations. Although some spectral differences do occur, for the RNA sequences considered, no major disagreements were found in CD spectral signs and shapes, between measurements and calculations. Overall, the results indicate that the newly derived A-, U-, G-, and C-parameters show better agreement between theory and experiment than those used in previous nucleic acid CD calculations.     

Secondary and tertiary structure of the A-state of cytochrome c from resonance Raman spectroscopy.

Ferricytochrome c can be converted to the partially folded A-state at pH 2.2 in the presence of 1.5 M NaCl. The structure of the A-state has been studied in comparison with the native and unfolded states, using resonance Raman spectroscopy with visible and ultraviolet excitation wavelengths. Spectra obtained with 200 nm excitation show a decrease in amide II intensity consistent with loss of structure for the 50s and 70s helices. The 230-nm spectra contain information on vibrational modes of the single Trp 59 side chain and the four tyrosine side chains (Tyr 48, 67, 74, and 97). The Trp 59 modes indicate that the side chain remains in a hydrophobic environment but loses its tertiary hydrogen bond and is rotationally disordered. The tyrosine modes Y8b and Y9a show disruption of tertiary hydrogen bonding for the Tyr 48, 67, and 74 side chains. The high-wavenumber region of the 406.7-nm resonance Raman spectrum reveals a mixed spin heme iron atom, which arises from axial coordination to His 18 and a water molecule. The low-frequency spectral region reports on heme distortions and indicates a reduced degree of interaction between the heme and the polypeptide chain. A structural model for the A-state is proposed in which a folded protein subdomain, consisting of the heme and the N-terminal, C-terminal, and 60s helices, is stabilized through nonbonding interactions between helices and with the heme.     

Primary Conformation Change in Bacteriorhodopsin on Photoexcitation

Ultrafast dynamics of bacteriorhodopsin (bR) has been extensively studied experimentally and theoretically. However, there are several contradictory results reported, indicating that its detailed dynamics and initial process have not yet been fully clarified. In this work, changes in the amplitude and phase of molecular vibration in the isomerization process of bR were real-time probed simultaneously at 128 different wavelengths through intensity modulation of the electronic transition. Systematic information on the transient change in continuous spectrum extending from 505 nm (2.45 eV) to 675 nm (1.84 eV) showed different dynamics in each spectral region reflecting the difference in the excited states and intermediates dominating the dynamics during the photoisomerization. Careful analysis of the transient spectral changes and spectrograms calculated from the vibrational real-time traces elucidated that the primary event just after photoexcitation is the deformation of the retinal configuration, which decays within 30 fs near the C=N bond in the protonated Schiff base. The intensity of C=N stretching mode starts to decrease before the initiation of the frequency modulation of the C=C stretching mode. The C=C stretching mode frequency was modulated by a coupled torsion around the C₁₃=C₁₄ bond, leading to the photoisomerization around the bond. This study clarified the dynamics of the C=N and C=C stretching modes working as key vibration modes in the photoisomerization of bR. Furthermore, we have elucidated the modulation and decay dynamics of the C=C stretching mode in the photoreaction starting from H (Franck-Condon excited state) followed by I (twisted excited), and J (first intermediate) states.     

Raman,FT-IR spectroscopic analysis and first-order hyperpolarisability of 3-benzoyl-5-chlorouracil by first principles

3-Benzoyl-5-chlorouracil (3B5CU), a biologically active synthetic molecule, has been analysed at DFT/6-311+ + G(d,p) level and reported for the first time as a potential candidate for nonlinear optical (NLO) applications. The optimised skeleton of 3B5CU molecule is non-planar. The frontier orbital energy gap, dipole moment, polarisability and first static hyperpolarisability have been calculated. The first static hyperpolarisability is found to be almost 15 times higher than that of urea. The high value of first static hyperpolarisability (2.930 × 10^? 30 e.s.u.) due to the intra-molecular charge transfer in 3B5CU has been discussed using first principles. A complete vibrational analysis of the molecule has been performed by combining the experimental Raman, FT-IR spectral data and the quantum chemical calculations. In general, a good agreement of calculated modes with the experimental ones has been obtained. The strong vibrational modes contributing towards NLO activity, involving the whole charge transfer path, have been identified and analysed.     

Redox-induced conformational changes in myoglobin and hemoglobin: electrochemistry and ultraviolet-visible and Fourier transform infrared difference spectroscopy at surface-modified gold electrodes in an ultra-thin-layer spectroelectrochemical cell.

Using suitable surface-modified electrodes, we have developed an electrochemical system which allows a reversible heterogeneous electron transfer at high (approximately 5 mM) protein concentrations between the electrode and myoglobin or hemoglobin in an optically transparent thin-layer electrochemical (OTTLE) cell. With this cell, which is transparent from 190 to 10,000 nm, we have been able to obtain electrochemically-induced Fourier-transform infrared (FTIR) difference spectra of both proteins. Clean protein difference spectra between the redox states were obtained because of the absence of redox mediators in the protein solution. The reduced-minus-oxidized difference spectra are characteristic for each protein and arise from redox-sensitive heme modes as well as from polypeptide backbone and amino acid side chain conformational changes concomitant with the redox transition. The amplitudes of the difference bands, however, are small as compared to the total amide I absorbance, and correspond to approximately 1% (4%) of the reduced-minus-oxidized difference absorbance in the Soret region of myoglobin (hemoglobin) and to less than 0.1% of the total amide I absorbance. Some of the bands in the 1560-1490-cm-1 spectral regions could be assigned to side-chain vibrational modes of aromatic amino acids. In the conformationally sensitive spectral region between 1680 and 1630 cm-1, bands could be attributed to peptide C = O modes because of their small (2-5 cm-1) shift in 2H2O. A similar assignment could be achieved for amide II modes because of their strong shift in 2H2O.(ABSTRACT TRUNCATED AT 250 WORDS)     

Collective vibrational modes in biological molecules investigated by terahertz time-domain spectroscopy

We present well-resolved absorption spectra of biological molecules in the far-IR (FIR) spectral region recorded by terahertz time-domain spectroscopy (THz-TDS). As an illustrative example we discuss the absorption spectra of benzoic acid, its monosubstitutes salicylic acid (2-hydroxy-benzoic acid), 3- and 4-hydroxybenzoic acid, and aspirin (acetylsalicylic acid) in the spectral region between 18 and 150 cm(-1). The spectra exhibit distinct features originating from low-frequency vibrational modes caused by intra- or intermolecular collective motion and lattice modes. Due to the collective origin of the observed modes the absorption spectra are highly sensitive to the overall structure and configuration of the molecules, as well as their environment. The THz-TDS procedure can provide a direct fingerprint of the molecular structure or conformational state of a compound.     

Changes in vibrational modes of water and bioprotectants in solution

Inelastic neutron scattering (INS) measurements have been performed on trehalose and sucrose/H(2)O mixtures at very low temperature as a function of concentration by using the TOSCA spectrometer at the ISIS Facility (DRAL, UK). The aim of this work is to investigate by INS the vibrational behaviour of water in presence of trehalose and sucrose in order to characterize the changes induced by these disaccharides on the H(2)O hydrogen-bonded network. In particular, we obtained information about the effects of the two disaccharides in the translational, librational and bending spectral regions of ice. The disaccharide bioprotective effectiveness can be linked by the high destructuring effect emphasised by the analysis of the librational modes region. On the other hand, the analysis of the vibrational region corresponding to the ice bending modes show a high "crystallinity" degree which can justify the cryptobiotic action of disaccharides.     

Acoustic modes and nonbonded interactions of the double helix

Observations of acoustic velocities in DNA fibers have been used to refine nonbonded force constants for the DNA double helix. Long-range forces are found to be needed for A conformation and are likely to dominate in B conformation as well. The acoustic dispersion curves are described and calculated. A correction due to the effects of water is calculated. The effect of nonbonded interaction on other vibrational modes is calculated.     

Action spectrum for polarotropism of the germ tube of the liverwort Sphaerocarpos Donnellii aust.

Summary A series of dose response curves was worked out in the polarotropically active blue and UV spectral region. These dose response curves show changes in slope as a function of wavelength. In blue the slope values are higher than in UV. As a consequence, both the relative height of the peaks in blue and UV and the fine characteristics in blue of the action spectrum calculated on the basis of these dose response curves change decisively with different response levels taken for calculation. Therefore no decision can be made as to what photoreceptor(s) might be involved. Though at medium response levels the action spectra show similarity with action spectra of other blue-UV-mediated photoresponses, which generally are believed as being indicative of some flavin.     

Vibrational analysis of peptides,polypeptides, and proteins. V. Normal vibrations of β-turns

The normal modes have been calculated for β-turns of types I, II, III, I′, II′, and III′. The complete set of frequencies is given for the first three structures; only the amide I, II, and III modes are given for the latter three structures. Calculations have been done for structures with standard dihedral angles, as well as for structures whose dihedral angles differ from these by amounts found in protein structures. The force field was that refined in our previous work on polypeptides. Transition dipole coupling was included, and is crucial to predicting frequency splittings in the amide I and amide II modes. The results show that in the amide I region, β-turn frequencies can overlap with those of the α-helix and β-sheet structures, and therefore caution must be exercised in the interpretation of protein bands in this region. The amide III modes of β-turns are predicted at significantly higher frequencies than those of α-helix and β-sheet structures, and this region therefore provides the best possibility of identifying β-turn structures. Amide V frequencies of β-turns may also be distinctive for such structures.     

Application of the local regression method interval partial least-squares to the elucidation of protein secondary structure

The infrared amide bands are sensitive to the conformation of the polypeptide backbone of proteins. Since the backbone of proteins folds in complex spatial arrangements, the amide bands of these proteins result from the superimposition of vibration modes corresponding to the different types of structural motifs (alpha helices, beta sheets, etc.). Initially, band deconvolution techniques were applied to determine the secondary structure of proteins, i.e., the abundance of each structural motif in the polypeptide chain was directly related to the area of the suitable deconvolved vibration modes under the amide I band (1700-1600 cm(-1)). Recently, several multivariate regression methods have been used to predict the secondary structure of proteins as an alternative to the previous methods. They are based on establishing a relationship between a matrix of infrared protein spectra and another that includes their secondary structure, expressed as the fractions of the different structural motifs, determined from X-ray analysis. In this study, we investigated the use of the local regression method interval partial least-squares (iPLS) to seek improvements to the full-spectrum PLS and other regression methods. The local character of iPLS avoids the use of spectral regions that can introduce noise or that can be irrelevant for prediction and focuses on finding specific spectral ranges related to each secondary structure motif in all the proteins. This study has been applied to a representative protein data set with infrared spectra covering a large wavenumber range, including amides I-III bands (1700-1200 cm(-1)). iPLS has revealed new structural mode assignments related to less explored amide bands and has offered a satisfactory predictive ability using a small amount of selected specific spectral information.     

Lattice vibrational modes of poly(rU)-poly(rA). A coupled single-helical approach

The eigenvalues and eigenvectors of 11-fold double-helical poly(rU)·poly(rA) have been calculated. The vibrational potential energy of the double-helical structure is initially considered to be a sum of the vibrational potential energy of the single-helical structures poly(rU) and poly(rA). Coupling between the single helices is introduced by including a stretch force constant for each hydrogen bond between the uracil and adenine base residues. In addition, a model is presented for nonbonded interactions between nearest neighbor base pairs, which is consistent with a previous model for such interactions in the single helices. Because of the simple structural relationship between the uncoupled single helices and the double helix we are able to cast the secular equation for poly(rU)·poly(rA) in a form suitable for the use of perturbation theory using the previously calculated normal modes for the single helices as the unperturbed modes. Perturbation theory was found to be inapplicable for the region of the spectrum ?450 cm^?1. In this region an exact Green function technique is used to calculate the strongly coupled modes. We explicitly display one aspect of these double-helical normal modes. The stretching motions of the hydrogen bonds in the region of the spectrum <450 cm^?1 have been plotted as bar graphs for each mode.     

Near-infrared photoacoustic spectroscopy of proteins

A major problem encountered with the use of electronic spectroscopy in the analysis of biological materials in the ultraviolet, visible, and infrared region involves the limited range of the physical state of samples that can be examined. In an attempt to expand this range, photoacoustic spectra of both solid- and solution-state proteins have been obtained in the near-infrared region. Solid proteins generate detailed spectra in the region 1.0–2.6 μm, resulting primarily from hydrogenic overtone and combinational modes. Harmonics and combinations of amide group frequencies which display significant spectral complexity are observed between 1.4 and 1.7 μm, although they appear to manifest only limited conformational sensitivity. Solution spectra in D₂O are of much lower resolution. Assignments of peaks for both solution- and solid-state proteins are presented and the advantages and disadvantages of the use of near-infrared photoacoustic spectroscopy with proteins are discussed.