Methyl group substitution at C(1), C(2) or C(3) of the glycerol backbone of a diether phosphocholine: a comparative study of bilayer chain disorder in the gel and liquid-crystalline phases

Alterations in the inter- and intramolecular packing characteristics of aqueous dispersions of methyl derivatives of di-O-hexadecylglycerophosphocholine (DHPC), an ether lipid in which the methyl group is substituted at the 1, 2 or 3 position of the glycerol backbone, were monitored by changes in the vibrational frequencies and intensities of selected spectral features by Raman spectroscopy. Temperature profiles constructed from spectra reflecting intermolecular order/disorder rearrangements (C-H stretching mode region) and intramolecular order/disorder processes (C-C stretching mode region) provide insight into several important structural properties of diether lipid bilayers. The introduction of a methyl group into any position of the glycerol backbone alters both the characteristics of the DHPC pretransition and the temperature of the gel to liquid-crystalline phase transition. The main gel to liquid-crystalline phase transitions are 42.8 degrees C in the pure diether lipid, 41.6 degrees C for 3-Me-DHPC, 40.5 degrees C for 2-Me-DHPC and 38.1 degrees C for 1-Me-DHPC. Temperature profiles indicate that the degree of disordering for both the gel and liquid-crystalline states follows the sequence 2-Me-DHPC less than 3-Me-DHPC less than DHPC less than 1-Me-DHPC. Phase transition widths, delta T, determined from the spectroscopic temperature profiles, are discussed in terms of van't Hoff enthalpy functions involving both interchain and trans/gauche effects.     

Resonance Raman evidence for substrate reorginization in the active site of papain.

Resonance Raman spectra were obtained for the acylenzyme 4-dimethylamino-3-nitro(alpha-benzamido)cinnamoyl-papain prepared using the chromophoric substrate methyl 4-dimethylamino-3-nitro(alpha-benzamido)cinnamate. These spectra contained vibrational spectral data of the acyl residue while covalently attached to the active site and could be used to follow directly acylation and deacylation kinetics. Spectra were obtained at pH values ranging from those where the acyl-enzyme is relatively stable (pH 3.0, tau 1/2 congruent to 800 s) to those where it is relatively unstable (pH 9.2, tau 1/2 congruent to 223 s). Throughout this range acyl-enzyme spectra differed completely from that of the free substrate or the product (4-dimethylamino-3-nitro(alpha-benzamido)cinnamic acid) indicating that a structural change occurred on combination with the active site. The spectra are consistent with rearrangement of the alpha-benzamido group in the bound substrate, -NH--C(==O)Ph becoming --N==C(--OX)Ph, where the bonding to oxygen is unknown. Superimposed on these large differences, small changes in acyl-enzyme spectra also occurred as pH was raised to decrease the half-life. All of the above spectral perturbations are consistent with a structural change in the acyl-enzyme which precedes the rate-determining step in deacylation. Thus, deacylation proceeds from an acyl residue structure differing from that of the substrate in solution. Upon acid denaturation the spectrum characteristic of the intermediate reverts to one closely resembling the substrate, demonstrating that a functioning active site is necessary to produce the observed differences. Spectra in D2O of native acyl-enzyme were identical with those in H2O, indicating that the observed differences in rate constant were not due to solvent-induced structural changes. Activated papain purified by crystallization or by affinity chromatography formed the acyl-enzyme. However, the kinetics of formation and deacylation differed between these materials, as did the spectral properties. Small differences in active-site structure are considered to be responsible for this effect, and it is suggested that such spectral perturbations may be useful in directly relating small differences in structure of the substrate in the active site with corresponding differences in kinetics.     

Analysis of the vibrational spectra of new OH-containing E-4-arylmethylene-3-isochromanones and 3-arylcoumarins

A combined experimental and theoretical approach is presented to structural characterization of fairly large, newly synthesized organic molecules in order to enhance the effectiveness of their instrumental analysis by vibrational spectroscopy. The method consists of measurement of FT-IR and Raman spectra of the reaction products and subsequent ab initio or DFT quantum mechanical calculations (prediction) of the vibrational spectra for any anticipated structural varieties of the synthesized molecules. Comparison of the measured and computed frequencies as well as the observed and simulated spectra is performed to resolve any uncertainties in identifying the reaction products. Vibrational frequency and normal mode calculations based on scaled quantum mechanical (SQM) force fields performed at the DFT/B3LYP/6-31G* level of theory are demonstrated to provide a wealth of information that have been used in this work to ascertain the molecular structure, probable conformation and H-bond properties of three new isochromanone or coumarin derivatives, namely: 3-([2'-hydroxymethyl]-phenyl)-coumarin (1), E-4-(3'-hydroxyphenylmethylene)-3-isochromanone (2), and 2-[(2'-hydroxymethyl)phenyl]-3H-naphto[2,1-b]pyran-3-one (3).     

Effect of hemolysis on Fourier transform infrared and Raman spectra of blood plasma

Hemolysis is a very common phenomenon and is referred as the release of intracellular components from red blood cells to the extracellular fluid. Hemolyzed samples are often rejected in clinics due to the interference of hemoglobin and intracellular components in laboratory measurements. Plasma and serum based vibrational spectroscopy studies are extensively applied to generate spectral biomarkers for various diseases. However, no studies have reported the effect of hemolysis in blood based vibrational spectroscopy studies. This study was undertaken to evaluate the effect of hemolysis on infrared and Raman spectra of blood plasma. In this study, prostate cancer plasma samples (n = 30) were divided into three groups (nonhemolyzed, mildly hemolyzed, and moderately hemolyzed) based on the degree of hemolysis and FTIR and Raman spectra were recorded using high throughput (HT)‐FTIR and HT‐Raman spectroscopy. Discrimination was observed between the infrared and Raman spectra of nonhemolyzed and hemolyzed plasma samples using principal component analysis. A classical least square fitting analysis showed differences in the weighting of pure components in nonhemolyzed and hemolyzed plasma samples. Therefore, it is worth to consider the changes in spectral features due to hemolysis when comparing the results within and between experiments.     

F.T.-I.R. and laser-raman spectra of d-ribose and 2-deoxy-d-erythro-pentose (“2-deoxy-d-ribose”)

Laser-Raman spectra of d-ribose and 2-deoxy-d-erythro-pentose in aqueous solution are reported. F.t.-i.r. and Raman spectra have been obtained for crystals of these sugars. Assignments of the Raman bands observed in solution are proposed. The spectral differences between the two sugars are discussed in terms of the structural difference. The analysis of the frequencies observed permits identification of each of the sugars and their isomeric analogs, and can be used as a basis for study of nucleosides and nucleotides by vibrational spectroscopy.     

Conformational dependence of CH(CD)-strechings in D-glucose and some deuterated derivatives as revealed by infrared and raman spectroscopy

The Raman and i.r. spectra in the CH- and CD-stretching region of D-glucose and five selectively deuterated derivatives in the solid state have been recorded. The CH (CD) bonds have different force constants depending on their position and conformation in the pyranose ring and on the dihedral angle HCOH (DCOH). Calculations of the intensities of the i.r. bands confirm these conclusions. Modifications of the force field are proposed that account for the changes in the spectra for solutions in D₂O, which are useful for the interpretation of vibrational c.d. spectra.     

Vibrational analysis and spectra of orotic acid

The IR and Raman spectra of polycrystalline anhydrous orotic acid and its N1, N3, and O12 trideuterated isotopomer are recorded in the 4000-40 cm(-1) spectral interval as part of a series of vibrational analyses of nucleosides, nucleotides, and related compounds carried out in our laboratory. The frequencies of the fundamental transitions and the potential energy distributions of the 39 normal modes of orotic acid and its isotopomer are calculated by an ab initio density functional theory Becke3P86/6-311G** treatment. Assignments of the vibrational modes are proposed that consider the results of these calculations and the observed spectra. The results of the ab initio treatment are related to crystallographic and spectral data, and they are compared with previous assignments for similar molecules.     

Raman spectroscopic study of the conformational changes of thyroxine induced by interactions with phospholipid

Comparison of the Raman spectra of thyroxine ( L-3,3',5,5'-tetraiodothyronine) in the pure state and in a 1:5 mixture with phosphatidylcholine reveals spectral differences that reflect structural changes of thyroxine induced by interactions with the phospholipid. These structural changes could be localized in specific parts of the thyroxine molecule on the basis of a vibrational analysis that was carried out by density functional calculations with the B3LYP hybrid functional applying the SDD effective core potential basis set. The calculated (and subsequently scaled) frequencies reveal a good agreement with the experimental data, which together with calculated IR and Raman intensities allow a plausible assignment of most of the IR and Raman bands. Thus, it is found that modes localized in the aromatic beta-ring and in the ether group as well as the C-I stretching modes of ring alpha are affected upon lipid interactions, indicating that thyroxine interacts with the phosphatidylcholine bilayer via penetration of the hydrophobic part of the molecule.     

Ab initio Hartree-Fock/6-31G** calculation on 9-beta-D-arabinofuranosyladenine-5'-monophosphate molecule: application to the analysis of its IR and Raman spectra

9-beta-D-arabinofuranosyaldenine-5'-monophosphate (5'-ara-AMP) is an arabinonucleotide that has antiviral and antitumor activity. The accurate knowledge of the nature of its vibrational modes is a valuable step for the forthcoming elucidation of drug-nucleotide and drug-enzyme interactions. The FTIR and FT Raman spectra (4000-30 cm(-1)) of 5'ara-AMP and two deuterated derivatives ara-AMP-d(C8) (deuteration in C8) and ara-AMP-d7 (deuteration in C8, amino and hydroxyl groups) are reported. Theoretical vibrational calculations were performed using the Hartree-Fock/6-31G** method. An assignment of the observed spectra is proposed considering the scaled potential energy distribution of the vibrational modes of the 5'ara-AMP molecule and the observed band shifts by deuteration. The scaled ab initio frequencies are in good agreement with the experimental data (<3 cm(-1) SD).     

A Multiscale Vibrational Spectroscopic Approach for Identification and Biochemical Characterization of Pollen

Background

Analysis of pollen grains reveals valuable information on biology, ecology, forensics, climate change, insect migration, food sources and aeroallergens. Vibrational (infrared and Raman) spectroscopies offer chemical characterization of pollen via identifiable spectral features without any sample pretreatment. We have compared the level of chemical information that can be obtained by different multiscale vibrational spectroscopic techniques.

Methodology

Pollen from 15 different species of Pinales (conifers) were measured by seven infrared and Raman methodologies. In order to obtain infrared spectra, both reflectance and transmission measurements were performed on ground and intact pollen grains (bulk measurements), in addition, infrared spectra were obtained by microspectroscopy of multigrain and single pollen grain measurements. For Raman microspectroscopy measurements, spectra were obtained from the same pollen grains by focusing two different substructures of pollen grain. The spectral data from the seven methodologies were integrated into one data model by the Consensus Principal Component Analysis, in order to obtain the relations between the molecular signatures traced by different techniques.

Results

The vibrational spectroscopy enabled biochemical characterization of pollen and detection of phylogenetic variation. The spectral differences were clearly connected to specific chemical constituents, such as lipids, carbohydrates, carotenoids and sporopollenins. The extensive differences between pollen of Cedrus and the rest of Pinaceae family were unambiguously connected with molecular composition of sporopollenins in pollen grain wall, while pollen of Picea has apparently higher concentration of carotenoids than the rest of the family. It is shown that vibrational methodologies have great potential for systematic collection of data on ecosystems and that the obtained phylogenetic variation can be well explained by the biochemical composition of pollen. Out of the seven tested methodologies, the best taxonomical differentiation of pollen was obtained by infrared measurements on bulk samples, as well as by Raman microspectroscopy measurements of the corpus region of the pollen grain. Raman microspectroscopy measurements indicate that measurement area, as well as the depth of focus, can have crucial influence on the obtained data.     

A systematic approach toward the analysis of drug-DNA interactions using Raman spectroscopy: the binding of metal-free bleomycins A(2) and B(2) to calf thymus DNA

Bleomycins A(2) and B(2) are the two active components in the antineoplastic drug Blenoxane. DNA is targeted by this drug in cancer cells and the mode of action of this drug involves DNA binding. Ambiguity exists as to the way in which bleomycin binds to DNA. Raman spectroscopy was used to examine both calf thymus DNA and a bleomycin/DNA complex at two temperatures. A curvefitting technique was applied to these spectra for a spectral region obscured by many overlapping bands associated with the nucleotide bases in order to derive information about frequencies, bandwidths, and intensities of the vibrational modes in this region. This allowed identification and analysis of bands associated with specific assigned nucleotide base residues. Upon binding of bleomycin, several significant changes in bandwidth, intensities, and frequencies relative to uncomplexed DNA were observed consistently at both higher (30 degrees C) and lower (19 degrees C) temperature. The data presented here support at least a partial intercalation mode of binding for bleomycin that is temperature dependent and more pronounced at the more physiologically relevant temperature of 30 degrees C.     

Low-Temperature conformation of Mg2+-Poly(U) in D2O as revealed by IR and Raman Spectroscopy and by normal-mode analysis treatment

Infrared and Raman spectra of the Mg²⁺ salt of poly(U) in D₂O were recorded in the 1600-1800 cm^?1 region and between 1 and 20C. The ir spectra showed a melting curve similar to the uv melting curves with a temperature of transition of about 6.5°C. This spectral change is assumed to be associated with the formation of the secondary structure of Mg²⁺-poly(U) in D₂O at this temperature. Three double-helical and two triple-helical structures were used as inputs to compute the normal modes of vibration. A double-helical structure was found to give the best agreement with the observations. Knowledge of the C=0 eigenvectors, and of the expression for transition probability from quantum mechanics, was used to explain the so far unanswered question of H. T. Miles [(1964) Proc. Natl. Acad. Sci. USA 51, 1104–1109; (1980) Biomolecular Structure, Conformation, Function and Evolution, Pergamon, Oxford, pp. 251–264] as to why there is an increase in the ir vibrational wave number of a carbonyl band when that group is H-bonded to another polynucleotide chain in a helix. Such considerations also explain why a predicted band at about 1648 cm^?1 is not to be seen in the ir spectra but is present in the Raman spectra. The model incorporating the C?O transition dipole-dipole coupling interaction is able to explain also the observed higher intensity of the higher wave-number ir band. The experimental results demonstrate that the complete picture of vibrational dynamics of Mg²⁺-poly(U) in D₂O is obtained only by looking simultaneously at ir and Raman spectra and not at only one of them. Weak ir bands were found to be as useful as the strong ones in understanding structure and vibrational dynamics. On the bases of our ir and Raman spectra, of the normal-mode analyses, and of the literature data, it is concluded that Mg²⁺-poly(U) in D₂O is present in a double-helical structure at temperatures below the temperature of transition, whereby the uracil residues are paired according to arrangement (a) (see Fig. 1). This structure is rodlike and arises by refolding of one poly(U) chain. The computations show that no normal mode is associated with a single C?O group vibration; all C?O group vibrations are heavily mixed motions of various C?O groups.     

Resonance Raman investigations of cytochrome c conformational change upon interaction with the membranes of intact and Ca2+-exposed mitochondria

The conformational states of cytochrome c inside intact and Ca(2+)-exposed mitochondria have been investigated using resonance Raman spectroscopy. Intact and swelling bovine heart and rat liver mitochondria were examined with an excitation wavelength (413.1 nm) in resonance with the Soret transition of ferrous cytochrome c. The different b- to c-type cytochrome concentration ratio in mitochondria from two different tissues was used to help assign the Raman spectral components. Resonance Raman spectra were also recorded for mitochondria fractions (supernatants and pellets) obtained from swollen (Ca(2+)-exposed) mitochondria after differential centrifugation. The results illustrate that cytochrome c has an altered vibrational spectrum in solution, in intact, and in swollen mitochondria. When cytochrome c is released from mitochondria, its Raman spectrum becomes identical to that of ferrous cytochrome c in solution. The spectra of mitochondrial pellets indicate that a small amount of structurally modified cytochrome c remains associated with the heavy membrane fraction. Indeed, spectroscopic shifts in the low-frequency fingerprint and the high-frequency marker-band regions suggest that membrane binding leads to a partial opening of the heme pocket and an alteration of the heme thioether bonds. The results support the conclusion that most cytochrome c molecules in mitochondria are membrane-bound and that the cytochrome c structure changes upon binding. Furthermore, changes in the resonance Raman active mode located at 675 cm(-)(1) in the spectra of intact, swollen, and fractionated mitochondria indicate that b-type cytochromes may also undergo structural alterations during mitochondrial swelling and disruption.     

Synthesis of 18O-Labelled chlorophyll derivatives at carbonyl oxygen atoms by acidic hydrolysis of the ethylene ketal and acetal

The ethylene ketal of pyropheophorbides, chlorophylls possessing the 13-keto carbonyl group and lacking the 13(2)-methoxycarbonyl group, reacted with H(2)(18)O (ca. 95% 18O atom) by acidic hydrolysis to give efficiently and regioselectively 13(1)-18O-oxo-labelled compounds (ca. 92% 18O). The resulting 18O-labelled chlorin was modified by several chemical reactions to afford some derivatives with little loss of the 18O atom. Following the same procedures, 3(1),13(1)-doubly-18O-labelled pyrochlorophyll derivatives were also prepared. All the synthetic 18O-labelled compounds were identified by FAB-mass and vibrational spectra. Especially, in the vibrational spectroscopic results including IR and resonance Raman spectra, an about 30 cm(-1) wavenumber down-shift of the 3- and/or 13-C[double bond]O stretching vibrational bands was observed by exchanging 3(1)- or 13(1)-oxo-oxygen atom from 16O to 18O.     

Nanosecond retinal structure changes in K-590 during the room-temperature bacteriorhodopsin photocycle: picosecond time-resolved coherent anti-stokes Raman spectroscopy.

Time-resolved vibrational spectra are used to elucidate the structural changes in the retinal chromophore within the K-590 intermediate that precedes the formation of the L-550 intermediate in the room-temperature (RT) bacteriorhodopsin (BR) photocycle. Measured by picosecond time-resolved coherent anti-Stokes Raman scattering (PTR/CARS), these vibrational data are recorded within the 750 cm-1 to 1720 cm-1 spectral region and with time delays of 50-260 ns after the RT/BR photocycle is optically initiated by pulsed (< 3 ps, 1.75 nJ) excitation. Although K-590 remains structurally unchanged throughout the 50-ps to 1-ns time interval, distinct structural changes do appear over the 1-ns to 260-ns period. Specifically, comparisons of the 50-ps PTR/CARS spectra with those recorded with time delays of 1 ns to 260 ns reveal 1) three types of changes in the hydrogen-out-of-plane (HOOP) region: the appearance of a strong, new feature at 984 cm-1; intensity decreases for the bands at 957 cm-1, 952 cm-1, and 939 cm-1; and small changes intensity and/or frequency of bands at 855 cm-1 and 805 cm-1; and 2) two types of changes in the C-C stretching region: the intensity increase in the band at 1196 cm-1 and small intensity changes and/or frequency shifts for bands at 1300 cm-1 and 1362 cm-1. No changes are observed in the C = C stretching region, and no bands assignable to the Schiff base stretching mode (C = NH+) mode are found in any of the PTR/CARS spectra assignable to K-590. These PTR/CARS data are used, together with vibrational mode assignments derived from previous work, to characterize the retinal structural changes in K-590 as it evolves from its 3.5-ps formation (ps/K-590) through the nanosecond time regime (ns/K-590) that precedes the formation of L-550. The PTR/CARS data suggest that changes in the torsional modes near the C14-C15 = N bonds are directly associated with the appearance of ns/K-590, and perhaps with the KL intermediate proposed in earlier studies. These vibrational data can be primarily interpreted in terms of the degree of twisting of the C14-C15 retinal bond. Such twisting may be accompanied by changes in the adjacent protein. Other smaller, but nonetheless clear, spectral changes indicate that alterations along the retinal polyene chain also occur. The changes in the retinal structure are preliminary to the deprotonation of the Schiff base nitrogen during the formation of M-412. The time constant for the ps/ns K-590 transformation is estimated from the amplitude change of four vibrational bands in the HOOP region to be 40-70 ns.     

Density functional theory and ab initio studies of vibrational spectra of 2-bis (2-chloroethyl) aminoperhydro-1,3,2-oxazaphosphorinane-2-oxide

The Fourier transform Raman (FTR) and Fourier transform infrared (FTIR) spectra of 2-bis (2-chloroethyl) aminoperhydro-1,3,2-oxazaphosphorinane-2-oxide were recorded in the regions 4000–100 cm^? 1 and 4000–400 cm¹, respectively, in the solid phase. Molecular electronic energy, geometrical structure, harmonic vibrational spectra, infrared intensities and Raman scattering activities, highest occupied molecular orbital, lowest unoccupied molecular orbital energy, energy gaps and thermodynamical properties such as zero-point vibrational energies, rotational constants, entropies and dipole moment were computed at the Hartree–Fock/6-31G(d,p) and three parameter hybrid functional Lee–Yang–Parr/6-31G(d,p) levels of theory. The vibrational studies were interpreted in terms of potential energy distribution. The results were compared with experimental values with the help of scaling procedures. The observed wave number in FTIR and FTR spectra was analysed and assigned to different normal modes of the molecule. Most of the modes have wave numbers in the expected range and are in good agreement with computed values.     

Protonation state and structural changes of the tetrapyrrole chromophore during the Pr --> Pfr phototransformation of phytochrome: a resonance Raman spectroscopic study

The photoconversion of phytochrome (phytochrome A from Avena satina) from the inactive (Pr) to the physiologically active form (Pfr) was studied by near-infrared Fourier transform resonance Raman spectroscopy at cryogenic temperatures, which allow us to trap the intermediate states. Nondeuterated and deuterated buffer solutions were used to determine the effect of H/D exchange on the resonance Raman spectra. For the first time, reliable spectra of the "bleached" intermediates meta-R(A) and meta-R(C) were obtained. The vibrational bands in the region 1300-1700 cm(-)(1), which is particularly indicative of structural changes in tetrapyrroles, were assigned on the basis of recent calculations of the Raman spectra of the chromophore in C-phycocyanin and model compounds [Kneip, C., Hildebrandt, P., Németh, K., Mark, F., Schaffner, K. (1999) Chem. Phys. Lett. 311, 479-485]. The experimental resonance Raman spectra Pr are compatible with the Raman spectra calculated for the protonated ZZZasa configuration, which hence is suggested to be the chromophore structure in this parent state of phytochrome. Furthermore, marker bands could be identified that are of high diagnostic value for monitoring structural changes in individual parts of the chromophore. Specifically, it could be shown that not only in the parent states Pr and Pfr but also in all intermediates the chromophore is protonated at the pyrroleninic nitrogen. The spectral changes observed for lumi-R confirm the view that the photoreaction of Pr is a Z --> E isomerization of the CD methine bridge. The subsequent thermal decay reaction to meta-R(A) includes relaxations of the CD methine bridge double bond, whereas the formation of meta-R(C) is accompanied by structural adaptations of the pyrrole rings B and C in the protein pocket. The far-reaching similarities between the chromophores of meta-R(A) and Pfr suggest that in the step meta-R(A) --> Pfr the ultimate structural changes of the protein matrix occur.     

Vibrational mode analysis of 2-aminoadenine and its deuterated species from Raman and ultraviolet resonance Raman data

Resonance Raman spectroscopy data of 2-aminoadenine and its deuterated species (C8-deuterated, N-deuterated and C8-, N-deuterated derivatives) in aqueous solution have been collected in the spectral region between 400 and 1800 cm^–1, by using ultraviolet excitation wavelengths (_exc = 222, 257 and 281 nm) located in the three main UV absorption bands corresponding to the strongly allowed electronic transitions of the molecule of interest. Moreover, a Raman spectrum has been recorded under off-resonance conditions with a visible excitation (_exc= 488 nm). In order to assign the 2-aminoadenine in-plane vibrational bands displayed in the RRS spectra, a normal coordinate analysis has been performed by means of an empirical internal valence force field. These calculations are based on our recent normal mode analysis of adenine and guanine nucleic bases and their deuterated species, which was based on the joint use of resonance Raman spectroscopy and neutron inelastic scattering data. In the 2-aminoadenine force field proposed here, the diagonal force constants have been directly transferred from those recently obtained for adenine (and from guanine as concerns the 2-amino group), the interaction force constants (off-diagonal) then being adjusted on the basis of the actual experimental data from 2-aminoadenine and its deuterated species. The current force field is also able to assign infrared and Raman data obtained by other authors from polycrystalline samples of the pure species. Correspondence to: M. Ghomi     

Resonance raman spectroscopy of chemically modified and isotopically labelled purple membranes. II. Kinetic studies

Kinetic resonance Raman spectra of native and isotopically labelled purple membranes are compared. Using these data and the assignments of the previous paper in this sequence, we have confirmed that the Schiff base is deprotonated at times that are short in comparison to M₄₁₂ evolution. In addition, by monitoring the kinetic resonance Raman spectra in ²H₂O with 488.0 nm excitation we have been able to characterize in more detail the vibrational features associated with this unprotonated intermediate that precedes M₄₁₂. Furthermore, the kinetic spectra of fully deuterated purple membranes in H₂O have allowed us to assign the 1465 cm⁻¹ band in these spectra to the C=C stretching frequency of BR₅₇₀ and the 1512 cm⁻¹ band to the C=C stretching frequency of M₄₁₂. These spectra have also provided an indication of a Raman spectral feature associated with O₆₄₀ and, finally, our kinetic spectra have provided evidence that there is a significant alteration in the rate constants for the evolution of the various intermediates when the non-exchangeable protons on the membrane are replaced by deuterons.     

Partial B-to-A DNA transition upon minor groove binding of protein Sac7d monitored by Raman spectroscopy

Members of the Sso7d/Sac7d protein family and other related proteins are believed to play an important role in DNA packaging and maintenance in archeons. Sso7d/Sac7d are small, abundant, basic, and nonspecific DNA-binding proteins of the hyperthermophilic archeon Sulfolobus. Structures of several complexes of Sso7d/Sac7d with DNA octamers are known. These structures are characterized by sequence unspecific minor groove binding of the proteins and sharp kinking of the double helix. Corresponding Raman vibrational signatures have been identified in this study. A Raman spectroscopic analysis of Sac7d binding to the oligonucleotide decamer d(GAGGCGCCTC)(2) reveals large conformational perturbations in the DNA structure upon complex formation. Perturbed Raman bands are associated with the vibrational modes of the sugar phosphate backbone and frequency shifts of bands assigned to nucleoside vibrations. Large changes in the DNA backbone and partial B- to A-form DNA transitions are indicated that are closely associated with C2'-endo/anti to C3'-endo/anti conversion of the deoxyadenosyl moiety upon Sac7d binding. The major spectral feature of Sac7d binding is kinking of the DNA. Raman markers of minor groove binding do not largely contribute to spectral differences; however, clear indications for minor groove binding come from G-N2 and G-N3 signals that are supported by Trp24 features. Trp24 is the only tryptophan present in Sac7d and binds to guanine N3, as has been demonstrated clearly in X-ray structures of Sac7d-DNA complexes. No changes of the Sac7d secondary structure have been detected upon DNA binding.