Resonance Raman spectroscopy of polynucleotides

Resonance Raman Spectroscopy allows a selective study of the bases of DNA and therefore of the interactions of these bases with ligands. This technique is also sensitive to structural modifications. We show here that, first, the structures of native poly(dA-dT).poly(dA-dT) and poly(dA).poly(dT) are not the same and that, secondly, it is possible to characterize the B----Z transition of poly(dG-dC).poly(dG-dC). The study of the Raman hypochromism during the thermal denaturation of the polynucleotides reveals that the stacking of the adenines in poly(dA).poly(dT) is near that observed in poly(rA) but differs of this stacking in poly(dA-dT).poly(dA-dT). The enhancement of the intensity of the guanine line at 1193 cm-1 and of the cytosine lines at 780 cm-1, 1 242 cm-1 and 1268 cm-1 as well as the shift of the guanine line at low frequency should allow to characterize a small proportion of base pairs in Z form in any DNA.     

Resonance Raman spectroscopy of pyridoxal Schiff bases

Resonance Raman (RR) spectra are reported for amino acid and amine adducts of pyridoxal 5'-phosphate (PLP) and 5'-deoxypyridoxal (5'-dPL) in aqueous solution. For the valine adducts, a detailed study has been carried out on solutions at pH and pD 5, 9, and 13, values at which the pyridine and imine protons are successively ionized, and on the adducts formed from 15N-valine, alpha-deuterovaline, and N-methyl-PLP. Good quality spectra were obtained, despite the strong fluorescence of pyridoxal Schiff bases, by adding KI as a quencher, and by exciting the molecules on the blue side of their absorption bands: 406.7 nm (cw Kr+ laser) for the pH 5 and 9 species (lambda max = 409 and 414 nm), and 354.7 nm (pulsed YAG laser, third harmonic) for the pH 13 species (lambda max = 360 nm). A prominent band at 1646 cm-1 is assigned to the imine C=N stretch via its 13 cm-1 15N shift. A 12 cm-1 down-shift of the band in D2O confirms that the Schiff base linkage is protonated at pH 9. Deprotonation at pH 13 shifts VC = N from 1646 to 1629 cm-1, values typical of conjugated Schiff bases. The strongest band in the spectrum, at 1338 cm-1, shifts to 1347 cm-1 upon pyridine protonation at pH 5, and is assigned to a ring mode with a large component of phenolate C-O stretch. A shoulder on its low-frequency side is assigned to the C4-C4' stretch. Large enhancements of these modes can be understood qualitatively in terms of the dominant resonance structures contributing to the ground and resonant excited states. A number of weaker bands are observed, and assigned to pyridine ring modes. These modes gain significantly in intensity, while the exocyclic modes diminish, when the spectra are excited at 266 nm (YAG laser, fourth harmonic) in resonance with ring-localized electronic transitions.     

Resonance Raman spectroscopy of cytochrome c oxidase and electron transport particles with excitation near the Soret band

We report the resonance Raman spectra of cytochrome $\text{c}$ oxidase, both solubilized and in electron transport particles using laser excitation near the Soret band. As in the spectra of other hemoproteins, such as cytochrome $\text{c}$, the shape and intensity of a number of bands change when the oxidation state is varied. However, one of the hemes of solubilized cytochrome $\text{c}$ oxidase shows redox behavior which is anomalous. Spectra of electron transport particles are dominated by cytochrome $\text{c}$ oxidase. There are, however, definite differences between spectra of solubilized cytochrome $\text{c}$ oxidase and electron transport particles in the oxidized states.     

Resonance Raman spectroscopy of iron-oxygen vibrations in hemerythrin

Resonance Raman spectra are reported for oxyhemerythrin and 15 anionic adducts of methemerythrin. All methemerythrin derivatives except sulfidomethemerythrin contain a Raman band near 510 cm^?1 which is assigned to an iron-oxygen stretching vibration. The effect of H₂¹⁸O on the frequency of this vibration was studied extensively. On the basis of the exchange results, the vibration is assigned to OH^?, H₂O, or a μ-oxo bridge between the irons.     

Resonance Raman spectroscopy of octopus rhodopsin and its photoproducts

We report here the resonance Raman spectra of octopus rhodopsin and its photoproducts, bathorhodopsin and acid metarhodopsin. These studies were undertaken in order to make comparisons with the well-studied bovine pigments, so as to understand the similarities and the differences in pigment structure and photochemical processes between vertebrates and invertebrates. The flow method was used to obtain the Raman spectrum of rhodopsin at 13 degrees C. The bathorhodopsin spectrum was obtained by computer subtraction of the spectra containing different photostationary mixtures of rhodopsin, isorhodopsin, hypsorhodopsin, and bathorhodopsin, obtained at 12 K using the pump-probe technique and from measurements at 80 K. Like their bovine counterparts, the Schiff base vibrational mode appears at approximately 1660 cm-1 in octopus rhodopsin and the photoproducts, bathorhodopsin and acid metarhodopsin, suggesting a protonated Schiff base linkage between the chromophore and the protein. Differences between the Raman spectra of octopus rhodopsin and bathorhodopsin indicate that the formation of bathorhodopsin is associated with chromophore isomerization. This inference is substantiated by the chromophore chemical extraction data which show that, like the bovine system, octopus rhodopsin is an 11-cis pigment, while the photoproducts contain an all-trans pigment, in agreement with previous work. The octopus rhodopsin and bathorhodopsin spectra show marked differences from their bovine counterparts in other respects, however. The differences are most dramatic in the structure-sensitive fingerprint and the HOOP regions. Thus, it appears that although the two species differ in the specific nature of the chromophore-protein interactions, the general process of visual transduction is the same.     

Femtosecond coherent Raman spectroscopy and its application to porphyrins

The results on femtosecond time-resolved coherent anti-Stokes Raman scattering (CARS) experiments for the analysis and control of ground state vibrational dynamics of porphyrin systems are briefly reviewed. By detecting the spectrum of the transient CARS signal, a detailed mapping of the dynamics initiated by the stimulated Raman pump process is achieved. The method yields the dephasing behavior and spectral information of the investigated system at the same time. The different contributions to the ground state vibrational dynamics are selected by changing the direction of the CARS signal analyzer in the polarization arrangement used.     

Resonance Raman spectroscopy of carotenoids in Photosystem I particles

Low-temperature resonance Raman (RR) spectroscopy was used for the first time to study the spectral properties, binding sites and composition of major carotenoids in spinach Photosystem I (PSI) particles. Excitation was provided by an argon ion laser at 457.9, 476.5, 488, 496.5, 502 and 514.5 nm. Raman spectra contained the four known groups of bands characteristic for carotenoids (called from nu(1) to nu4). Upon 514.5, 496.5 and 476.5 nm excitations, the nu(1)-nu(3) frequencies coincided with those established for lutein. Spectrum upon 502-nm excitation could be assigned to originate from violaxanthin, at 488 nm to 9-cis neoxanthin, and at 457.9 nm to beta-carotene and 9-cis neoxanthin. The overall configuration and composition of these bound carotenoid molecules in Photosystem I particles were compared with the composition of pigment extracts from the same PSI particles dissolved in pyridine, as well as to configuration in the main chlorophyll a/b light-harvesting protein complex of photosystem II. The absorption transitions for lutein, violaxanthin and 9-cis neoxanthin in spinach photosystem I particles are characterized, and the binding sites of lutein and neoxanthin are discussed. Resonance Raman data suggest that beta-carotene molecules are also present in all-trans and, probably, in 9-cis configurations.     

Resonance Raman spectroscopy of sensory rhodopsin II from Natronobacterium pharaonis

Sensory rhodopsin II (pSRII), the photophobic receptor from Natronobacterium pharaonis, has been studied by time-resolved resonance Raman (RR) spectroscopy using the rotating cell technique. Upon excitation with low laser power, the RR spectra largely reflect the parent state pSRII(500) whereas an increase of the laser power leads to a substantial accumulation of long-lived intermediates contributing to the RR spectra. All RR spectra could consistently be analysed in terms of four component spectra which were assigned to the parent state pSRII(500) and the long-lived intermediates M(400), N(485) and O(535) based on the correlation between the C = C stretching frequency and the absorption maximum. The parent state and the intermediates N(485) and O(535) exhibit a protonated Schiff base. The C = N stretching frequencies and the H/D isotopic shifts indicate strong hydrogen bonding interactions of the Schiff base in pSRII(500) and O(535) whereas these interactions are most likely very weak in N(485).     

Resonance Raman spectroscopy of carotenoids in Photosystem II core complexes

Resonance Raman (RR) spectroscopy has been used to examine the configuration of the carotenoids bound to Synechocystis PCC 6803 Photosystem II (PS II) core complexes. The excitation wavelengths used (514.5, 488.0, 476.5 and 457.9 nm) span the absorption bands of all of the ~12–17 neutral carotenoids in the PS II core complex. The RR spectra of the two carotenoids associated with the D1–D2 polypeptides (Car₅₀₇ and Car₄₈₉) of the reaction center are extracted via light versus dark difference experiments measured at 20 K. The RR results are consistent with all-trans configurations for both Car₅₀₇ and Car₄₈₉ and indicate that majority of the other carotenoids in the PS II core complex must also be in the all-trans configuration. The configuration of β-carotene is relevant to its proposed function as a molecular wire in the secondary electron-transfer reactions of PS II.     

A holistic approach to protein secondary structure characterization using amide I band Raman spectroscopy

We have developed a holistic protein structure estimation technique using amide I band Raman spectroscopy. This technique combines the superposition of reference spectra for pure secondary structure elements with simultaneous aromatic, fluorescence, and solvent background subtraction, and is applicable to solution, suspension, and solid protein samples. A key component of this technique was the calculation of the reference spectra for ordered helix, unordered helix, and sheet, turns, and unordered structures from a series of well-characterized reference proteins. We accurately account for the overlap between the amide I and non-amide I regions and allow for different scattering efficiencies for different secondary structures. For hydrated samples, we allowed for the possibility that bound water spectra differ from the bulk water spectra. Our computed reference spectra compare well with previous experimental and theoretical results in the literature. We have demonstrated the use of these reference spectra for the estimation of secondary structures of proteins in solution, suspension, and dry solid forms. The agreement between our structure estimates and the corresponding determinations from X-ray crystallography is good.     

Resonance Raman spectroscopy of chemically modified retinals: Assigning the carbon-methyl vibrations in the resonance Raman spectrum of rhodopsin

To assign the observed vibrationsl modes in the resonance Raman spectrum of the retinylidene chromophore of rhodopsin, we have studied chemically modified retinals. The series of analogs investigated are the n-butyl retinals substituted at C₉ and C₁₃. The results obtained for the 11-cis isomer have clearly assigned the CCH₃ vibrational frequencies observed in the spectrum of the retinylidene chromophore. The data show that the C₍₉₎CH₃ stretching vibration can be assigned to the vibrational mode observed in the 1017 cm^?1 region, and the vibration detected at 997 cm^?1 can be assigned to the C₍₁₃CH₃ vibration. The C₍₅₎CH₃ stretching mode does not contribute to the vibrations observed in this region. The splitting in the C_(n)CH₃ (n = 9, 13) vibration is characteristic of the 11-cis conformation. The results on the modified retinals do not support the hypothesis that the splitting arises from equilibrium mixtures of 11-cis, 12-s-cis and 11-cis, 12-s-trans in solution. Thus, this splitting cannot be used to determine whether the chromophore in rhodopsin is in a 12-s-cis or 12-s-trans conformation. However, our results demonstrate that there are other vibrational modes in the spectra which are sensitive to this conformational equilibrium and we use the presence of a strong ~ 1271 cm^?1 mode in bovine and squid rhodopsin spectra as an indication that the chromophore in these pigments is 11-cis, 12-s-trans.     

Resonance Raman spectroscopy shows different temperature-dependent coordination equilibria for native horseradish and cytochrome c peroxidase

Resonance Raman spectra are reported for native horseradish peroxidase (HRP) and cytochrome c peroxidase (CCP) at 290, 77 and 9 K, using 406.7 nm excitation, in resonance with the Soret electronic transition. The spectra reveal temperature-dependent equilibria involving changes in coordination or spin state. At 290 K and pH 6.5, CCP contains a mixture of 5- and 6-coordinate high-spin Fe^III heme while at 9 K the equilibrium is shifted entirely to the 6-coordinate species. The spectra indicate weak binding of H₂O to the heme Pe, consistent with the long distance, 2.4 Å, seen in the crystal structure. At 290 K HRP also contains a mixture of high-spin Fe^III hemes with the 5-coordinate form predominant. At low temperature, a small 6-coordinate high-spin component remains but the 5-coordinate high-spin spectrum is replaced by another which is characteristic either of 6-coordinate low-spin or 5-coordinate intermediate spin heme. The latter species is definitely indicated by previous EPR studies at low temperature. This behavior implies that, in contrast to CCP, the distal coordination site of HRP is only partially occupied by H₂O at any temperature and that lowering the temperature significantly weakens the Fe-proximal imidazole bond. Consistent with this inference, the 77 K spectrum of reduced HRP shows an appreciable fraction of molecules having an Fe-imidazole stretching frequency of 222 cm⁻¹, a value indicating weakened H-bonding of the proximal imidazole.Resonance Roman spectroscopyHorseradish peroxidaseCytochrome c peroxidaseCoordination equilibrium     

Resonance Raman spectroscopy of xanthophylls in pigment mutant thylakoid membranes of pea

Low-temperature resonance Raman spectroscopy was used to study the changes in the molecular structure and configuration of the major xanthophylls in thylakoid membranes isolated from mutants of pea with modified pigment content and altered structural organization of their pigment-protein complexes. The Raman spectra contained four known groups of bands, nu(1)-nu(4), which could be assigned to originate mainly from the long wavelength absorbing lutein and neoxanthin upon 514.5 nm and at 488 nm excitations, respectively. The overall configuration of these bound xanthophyll molecules in the mutants appeared to be similar to the wild type, and the configuration in the wild type was almost identical with that in the isolated main chlorophyll a/b light harvesting protein complex of photosystem II (LHCII). Significant differences were found mainly in the region of nu(4) (around 960 cm(-1)), which suggest that the macroorganization of PS II-LHCII supercomplexes and/or of the LHCII-only domains are modified in the mutants compared to the wild type.     

Resonance Raman spectroscopy of methylamine dehydrogenase from bacterium W3A1

Resonance Raman spectroscopy has been used to probe the structure of the covalently bound quinone cofactor in methylamine dehydrogenase from the bacterium W3A1. Spectra were obtained on the phenylhydrazine and 2-pyridylhydrazine derivatives of the native enzyme, on the quinone-containing subunit labeled with phenylhydrazine, and on an active-site peptide also labeled with phenylhydrazine. Comparisons of these spectra to the corresponding spectra of copper-containing amine oxidase derivatives indicate that the quinones in these two classes of quinoproteins are not identical. The resonance Raman spectra of the native enzyme and small subunit have also been measured. 16O/18O exchange permitted the carbonyl modes of the quinone to be identified in the resonance Raman spectrum of oxidized methylamine dehydrogenase: a band at 1614 cm-1, together with a shoulder at 1630 cm-1, are assigned as modes containing substantial C = O stretching character. D2O/H2O exchange has pronounced effects on the resonance Raman spectrum of the oxidized enzyme, suggesting that the quinone may have numerous hydrogen bonds to the protein or that it is unusually sensitive to the local environment. Resonance Raman spectra of the isolated small subunit, and its phenylhydrazine derivative, are considerably different from the corresponding spectra of the intact protein. An attractive explanation for these observations is that the quinone cofactor in methylamine dehydrogenase from W3A1 is located at the interface between the large and small subunits, as found for the enzyme from Thiobacillus versutus [Vellieux, F. M. D., Huitema, F., Groendijk, H., Kalk, K. H., Frank, J. Jzn., Jongejan, J. A., & Duine, J. A. (1989) EMBO J. 8, 2171-2178].(ABSTRACT TRUNCATED AT 250 WORDS)     

Resonance Raman kinetic spectroscopy of bacteriorhodopsin on the microsecond time scale.

Using a rotating disk with a slit of variable width, a continuous wave argon ion laser, and an Optical Multichannel Analyzer for detection, a new technique is reported which should, in principle, be capable of recording resonance Raman spectra with time resolution of 100 ns. The resonance Raman spectra of the intermediates of the photosynthetic cycle of bacteriorhodopsin are recorded on the microsecond time scale. Both the kinetic results and the resonance enhancement profile suggest that deprotonation results in an intermediate preceding bM412 that has an optical absorption maximum at a wavelength longer than that of bM412.     

Resonance Raman spectroscopy of amicyanin, a blue copper protein from Paracoccus denitrificans

The copper binding site of amicyanin from Paracoccus denitrificans has been examined by resonance Raman spectroscopy. The pattern of vibrational modes is clearly similar to those of the blue copper proteins azurin and plastocyanin. Intense resonance-enhanced peaks are observed at 377, 392, and 430 cm-1 as well as weaker overtones and combination bands in the high frequency region. Most of the peaks below 500 cm-1 shift 0.5-1.5 cm-1 to lower energy when the protein is exposed to D2O. Based on the pattern of conserved amino acids, the axial type EPR spectrum, and the resonance Raman spectrum, it is proposed that the copper binding site in amicyanin contains a Cu(II) ion in a distorted trigonal planar geometry with one cysteine and two histidine ligands and an axial methionine ligand at a considerably longer distance. Furthermore, the presence of multiple intense Raman peaks in the 400 cm-1 region which are sensitive to deuterium substitution leads to the conclusion that the Cu-S stretch is coupled with internal ligand vibrational modes and that the sulfur of the cysteine ligand is likely to be hydrogen-bonded to the polypeptide backbone.     

Resonance Raman spectroscopy and enhanced photoreducibility for the 420 nm pulsed form of cytochrome oxidase

Resonance Raman (RR) spectra, with 413.1 nm Kr+ laser excitation, are reported for cytochrome oxidase in resting, reduced, and 428 nm (oxygenated) forms, and for the first time, in the 420 nm (pulsed) forms [(1984) J. Biol. Chem. 259, 2073-2076]. The differences between the resting, 420 nm, and 428 nm forms' RR spectra are small. All these forms contain FeIII only, as indicated by single v4 bands at approximately 1371 cm-1, and the reoxidized forms show partial conversion from high- to intermediate- or low-spin heme a3 (intensity shift from 1575 to 1588 cm-1 for v2). The 420 nm form differs strikingly from both the 428 nm and resting forms, however, in being much more readily photoreduced by the laser illumination. This property is linked to the protein conformational change believed to be responsible for the greater accessibility to exogenous ligands of the heme a3 in the 420 nm form.