Raman diagnosis of nucleic acid structure: sugar-puckering and glycosidic conformation in the guanosine moiety.

Observations of Raman spectra of various nucleic acids indicate that the guanine ring breathing frequency is sensitive to the internal rotation angle around the glycosidic bond and to the conformation of the five-membered ring of the ribose residue that is directly connected with the guanine residue in question. It is found that 682 cm-1 for C2'-endo-anti, at 665 cm-1 for C3'-endo-anti, and at 625 cm-1 for C3'-endo-syn. A DNA octamer d(GpGpApApTpTpCpC) shows, in its aqueous solution, a broad Raman band at 680 cm-1 with a tail at 670 cm-1. This fact suggests that the guanosine residues in this oligomer take primarily C2'-endo-anti conformation but an appreciable amount of fluctuation of the ribose ring structure towards C3'-endo is involved.     

Salt induced conformational transition between A and Z forms of r(CGCGCG) as revealed by a Raman spectroscopic study

Solution conformation in different conditions of r(CGCGCG) has been studied by a Raman spectroscopic method. In NaCl solution, r (CGCGCG) takes only an A-form duplex in which guanosine and cytidine have C3'endo-anti conformation even at 5M salt concentration. In much higher ionic strength condition (5M NaCl plus 1M MgCl2 or 6M NaClO4), it undergoes a transition to a left-handed Z-form. The Raman spectrum of the Z-form RNA was found to be very similar to that of Z-form DNA, suggesting that Z-RNA involves a C3'endo-syn guanosine and an in between form of C2'endo-Cl'exo-anti cytidine.     

Salt induced B----A transition of poly(dG).poly(dC) and the stabilization of A form by its methylation.

Raman spectra of poly(dG).poly(dC) have been observed in aqueous solutions at various ionic strengths, [NaCl] = 0.03 to 4 M, and at different temperatures, 10 to 60 degrees C. At 30 degrees C, and at [NaCl] = 0.03 M, it was found to have a B-form (with O4'endo-anti guanosine and C2'endo-anti cytidine), whereas, at [NaCl] = 4 M, an A form (with C3'endo-anti guanosine and C3'endo-anti cytidine). At 30 degrees C and [NaCl] = 1 M, namely at an intermediate state, a fraction of this molecules was considered to have a "heteronomous A" form (with O4'endo-anti guanosine and C3' endo-anti cytidine). At 60 degrees C and [NaCl] = 1 M, it assumes the B form, and at 10 degrees C and [NaCl] = 1 M, the A form. Cytosine-5-methylation was found to cause a marked stabilization of the A form. Even at [NaCl] = 0.1 M (at 30 degrees C), a substantial portion of poly(dG).poly(dm5C) was found to have a heteronomous form, in which the dG atrand is in the B form and the dC an A form; it never assumes a complete B form.     

The resonance Raman frequencies of the Fe-CO stretching and bending modes in the CO complex of cytochrome P-450cam

Resonance Raman spectra of the ferrous CO complex of cytochrome P-450cam have been observed both in its camphor-bound and free states. Upon excitation at 457.9 nm, near the absorption maximum of the Soret band, the ferrous CO complex of the camphor-bound enzyme showed an anomalously intense Raman line at 481 cm-1 besides the strong Raman lines at 1366 and 674 cm-1 for the porphyrin vibrations. The Raman line at 481 cm-1 (of the 12C16O complex) shifted to 478 cm-1 upon the substitution by 13C16O and to 473 cm-1 by 12C18O without any detectable shift in porphyrin Raman lines. This shows that the line at 481 cm-1 is assignable to Fe-CO stretching vibration. By the excitation at 457.9 nm, a weak Raman line was also observed at 558 cm-1, which was assigned to the Fe-C-O bending vibration, because it was found to shift by -14 cm-1 on 13C16O substitution while only -3 cm-1 on 12C18O substitution. These stretching and bending vibrations of the Fe-CO bond were not detected with the excitation at 413.1 nm, though the porphyrin Raman lines at 1366 and 674 cm-1 were clearly observed. When the substrate, camphor, was removed from the enzyme, the Fe-CO stretching vibration was found to shift to 464 cm-1 from 481 cm-1, while no detectable changes were found in porphyrin Raman lines. This means that the bound substrate interacts predominantly with the Fe-CO portion of the enzyme molecule.     

Contribution of the resonance Raman spectroscopy to the identification of Z DNA

Poly(dG-dC).poly(dG-dC) at low salt concentration (0.1 M NaCl) and at high salt concentration (4.5 M NaCl) has been studied by Raman resonance spectroscopy using two excitation wavelengths: 257 nm and 295 nm. As resonance enhances the intensity of the lines in a proportion corresponding to the square of the molar absorption coefficient, the intensities of the lines with 295 nm wavelength excitation are enhanced about sevenfold during the B to Z transition. With 257 nm excitation wavelength the 1580 cm-1 line of guanosine is greatly enhanced in the Z form whereas with 295 nm excitation several lines are sensitive to the modifications of the conformation: the guanine band around 650 cm-1 and at 1193 cm-1 and the bands of the cytosines at 780 cm-1, 1242 cm-1 and 1268 cm-1. By comparison with the U.V. resonance Raman spectra of DNA, we conclude that resonance Raman spectroscopy allows one to characterize the B to Z transition from one line with 257 nm excitation wavelength and from three lines with 295 nm excitation. The conjoined study of these four lines should permit to observe a few base pairs being in Z form in a DNA.     

Raman spectroscopic investigations of sarcoplasmic reticulum membranes.

Raman spectra are presented for sarcoplasmic reticulum membranes. Interpretation of the 1000-1130 cm-1 region of the spectrum indicates that the sarcoplasmic reticulum membrane may be more fluid than erythrocyte membranes that have been examined by the I portion of the membrane spectrum with a strong 1658 cm-1 band characteristic of C=C stretching in hydrocarbon side chains exhibiting cis conformation. This band is unaltered in intensity and position in H2O and in 2H2O thus obscuring amide I protein conformation. Of particular interest is the appearance of strong, resonantly enhanced bands at 1160 and 1527 cm-1 attributable to membrane-associated carotenoids.     

The occurence of the syn-C3' endo conformation and the distorted backbone conformations for C4'-C5' and P-O5' in oligo and polynucleotides.

The nucleoside constituents of nucleic acids prefer the anti conformation (1). When the sugar pucker is taken into account the nucleosides prefer the C2'endo-anti conformation. Of the nearly 300 nucleosides known, about 250 are in the anti conformation and 50 are in the syn-conformation, i.e., anti to syn conformation is 5:1. The nucleotide building blocks of nucleic acids show the same trend as nucleosides. Both the deoxy-guanosine and riboguanosine residues in nucleosides and nucleotides prefer the syn-C2'endo conformation with an intra-molecular hydrogen bond (for nucleosides) between the O5'-H and the N3 of the base and, a few syn-C3'endo conformations are also observed. Evidence is presented for the occurrence of the C3'endo-syn conformation for guanines in mis-paired double helical right-handed structures with the distorted sugar phosphate C4'-C5' and P-O5' bonds respectively, from g+ (gg) and g- to trans. Evidence is also provided for guanosine nucleotides in left-handed double-helical (Z-DNA) oligo and polynucleotides which has the same syn-C3'endo conformation and the distorted backbone sugar-phosphate bonds (C4'-C5' and P-O5') as in the earlier right-handed case.     

Resonance Raman analysis of the Pr and Pfr forms of phytochrome

Resonance Raman vibrational spectra of the Pr and Pfr forms of oat phytochrome have been obtained at room temperature. When Pr is converted to Pfr, new bands appear in the C = C and C = N stretching region at 1622, 1599, and 1552 cm-1, indicating that a major structural change of the chromophore has occurred. The Pr to Pfr conversion results in an 11 cm-1 lowering of the N-H rocking band from 1323 to 1312 cm-1. Normal mode calculations correlate this frequency drop with a Z----E isomerization about the C15 = C16 bond. A line at 803 cm-1 in Pr is replaced by an unusually intense mode at 814 cm-1 in Pfr. Calculations on model tetrapyrrole chromophores suggest that these low-wavenumber modes are hydrogen out-of-plane (HOOP) wagging vibrations of the bridging C15 methine hydrogen and that both the intensity and frequency of the C15 HOOP mode are sensitive to the geometry around the C14-C15 and C15 = C16 bonds. The large intensity of the 814-cm-1 mode in Pfr indicates that the chromophore is highly distorted from planarity around the C15 methine bridge. If the Pr----Pfr conversion does involve a C15 = C16 Z----E isomerization, then the intensity of the C15 HOOP mode in Pfr argues that the chromophore has an E,anti conformation. On the basis of a comparison with the vibrational calculations, the low frequency (803 cm-1) and the reduced intensity of the C15 HOOP mode in Pr suggest that the chromophore in Pr adopts the C15-Z,syn conformation.     

Beta-sheet and associated turn signatures in vibrational Raman optical activity spectra of proteins.

We have measured the aqueous solution vibrational Raman optical activity (ROA) spectra of concanavalin A, alpha-chymotrypsin, and beta-lactoglobulin, all of which are rich in beta-sheet, together with that of the model beta-turn peptide L-pro-L-leu-gly-NH2. Possible ROA signatures of antiparallel beta-sheet include a strong sharp positive band at approximately 1,313 cm-1 associated with backbone amide III C alpha H and NH deformations, and an amide I couplet, negative at low wavenumber and positive at high, centered at approximately 1,658 cm-1. Negative ROA bands in the range approximately 1,340-1,380 cm-1, which might originate in glycine CH2 deformations, appear to be characteristic of beta-turns. Our results provide further evidence that ROA is a more incisive probe of protein conformation than conventional vibrational spectroscopy, infrared, or Raman, because only those few vibrational coordinates within a given normal mode that sample the skeletal chirality directly contribute to the corresponding ROA band intensity.     

Raman spectroscopy of cytoplasmic muscle fiber proteins. Orientational order.

The polarized Raman spectra of glycerinated and intact single muscle fibers of the giant barnacle were obtained. These spectra show that the conformation-sensitive amide I, amide III, and C-C stretching vibrations give Raman bands that are stronger when the electric field of both the incident and scattered radiation is parallel to the fiber axis (Izz). The detailed analysis of the amide I band by curve fitting shows that approximately 50% of the alpha-helical segments of the contractile proteins are oriented along the fiber axis, which is in good agreement with the conformation and composition of muscle fiber proteins. Difference Raman spectroscopy was also used to highlight the Raman bands attributed to the oriented segments of the alpha-helical proteins. The difference spectrum, which is very similar to the spectrum of tropomyosin, displays amide I and amide III bands at 1,645 and 1,310 cm-1, respectively, the bandwidth of the amide I line being characteristic of a highly alpha-helical biopolymer with a small dispersion of dihedral angles. A small dichroic effect was also observed for the band due to the CH2 bending mode at 1,450 cm-1 and on the 1,340 cm-1 band. In the C-C stretching mode region, two bands were detected at 902 and 938 cm-1 and are both assigned to the alpha-helical conformation.     

Effect of the G.T mismatch on backbone and sugar conformations of Z-DNA and B-DNA: analysis by Raman spectroscopy of crystal and solution structures of d(CGCGTG) and d(CGCGCG)

The Z-DNA crystal structures of d(CGCGTG) and d(CGCGCG) are compared by laser Raman spectroscopy. Raman bands originating from vibrations of the phosphodiester groups and sensitive to the DNA backbone conformation are similar for the two structures, indicating no significant perturbation to the Z-DNA backbone as a result of the incorporation of G.T mismatches. Both Z structures also exhibit Raman markers at 625 and 670 cm-1, assigned respectively to C3'-endo/syn-dG (internal) and C2'-endo/syn-dG conformers (3' terminus). Additional Raman intensity near 620 and 670 cm-1 in the spectrum of the d(CGCGTG) crystal is assigned to C4'-exo/syn-dG conformers at the mismatch sites (penultimate from the 5' terminus). A Raman band at 1680 cm-1, detected only in the d(CGCGTG) crystal, is assigned to the hydrogen-bonded dT residues and is proposed as a definitive marker of the Z-DNA wobble G.T pair. For aqueous solutions, the Raman spectra of d(CGCGTG) and d(CGCGCG) are those of B-DNA, but with significant differences between them. For example, the usual B-form marker band at 832 cm-1 in the spectrum of d(CGCGTG) is about 40% less intense than the corresponding band in the spectrum of d(CGCGCG), and the former structure exhibits a companion band at 864 cm-1 not observed for d(CGCGCG). The simplest interpretation of these results is that the conventional B-form OPO geometry occurs for only 6 of the 10 OPO groups of d(CGCGTG). The remaining four OPO groups, believed to be those at or near the mismatch site, are in an "unusual B" conformation which generates the 864 cm-1 band.(ABSTRACT TRUNCATED AT 250 WORDS)     

The study of microviscosity of plasma membranes of Nitella cells during rest and excitation

Changes in the microviscosity of excitable membranes was investigated using resonance Raman spectroscopy of carotenoids. The Raman resonance spectra of carotenoids in Nitella cells were excited by 514.5 nm line of an argon ion laser. The bands at 1525 cm-1, 1160 cm-1 and 1008 cm-1 were observed and they were assigned to C=C, C-C and C-CH vibrations, respectively. The rhythmic excitation of cell reduced the intensity and increased the ratios of intensity of major carotenoid bands with no noticeable shift in the position of peaks. The Arrhenius plot of relative intensity ratios of 1525 cm-1 and 1160 cm-1 bands versus reciprocal temperature showed a change of the slope in the range of 13-18 degrees C. This indicates a membrane phase transitions in which a reorientation of carotenoids species takes place. The interpretation was supported by parallel microcalorimetric and EPR measurements. The decrease of microviscosity with increasing temperature is probably caused by changes in polyene chain conformation. It is suggested that membrane microviscosity during NH4(+)-stimulated rhythmic excitation of algal cells increases, and membrane-associated carotenoids act as microviscosity-sensitive "potential sensor" for the channel.     

Flexibility of DNA and RNA upon binding to different metal cations. An investigation of the B to A to Z conformational transition by Fourier transform infrared spectroscopy

The interaction of DNA and RNA with Cu(II), Mg(II), [Co(NH3)6]3+ [Co(NH3)5Cl]2+ chlorides and, cis- and trans-Pt(NH3)2Cl2 (CIS-DDP, trans-DDP) has been studied by Fourier Transform Infrared (FT-IR) spectroscopy and a correlation between metal-base binding and conformational transitions in the sugar pucker has been established. It has been found that RNA did not change from A-form on complexation with metals, whereas DNA exhibited a B to Z transition. The marker bands for the A-form (C3'-endo-anti conformation) were found to be near 810-816 cm-1, while the bands at 825 and 690 cm-1 are marker bands for the B-conformation (C2'-endo, anti). The B to Z (C3'-endo. syn conformation) transition is characterized by the shift of the band at 825 cm-1 to 810-816 cm-1 and the shift of the guanine band at 690 cm-1 to about 600-624 cm-1.     

Demonstration by ultraviolet resonance Raman spectroscopy of differences in DNA organization and interactions in filamentous viruses Pf1 and fd

Pf1, a class II filamentous virus, has been investigated by ultraviolet resonance Raman (UVRR) spectroscopy with excitation wavelengths of 257, 244, 238, and 229 nm. The 257-nm UVRR spectrum is rich in Raman bands of the packaged single-stranded DNA (ssDNA) genome, despite the low DNA mass (6%) of the virion. Conversely, the 229-nm UVRR spectrum is dominated by tyrosines (Tyr 25 and Tyr 40) of the 46-residue alpha-helical coat subunit. UVRR spectra excited at 244 and 238 nm exhibit Raman bands diagnostic of both viral DNA and coat protein tyrosines. Raman markers of packaged Pf1 DNA contrast sharply with those of the DNA packaged in the class I filamentous virus fd [Wen, Z. Q., Overman, S. A., and Thomas, G. J., Jr. (1997) Biochemistry 36, 7810-7820]. Interestingly, deoxynucleotides of Pf1 DNA exhibit sugars in the C2'-endo/anti conformation and bases that are largely unstacked, compared with C3'-endo/anti conformers and very strong base stacking in fd DNA; hydrogen-bonding interactions of thymine carbonyls are also different in Pf1 and fd. On the other hand, coat protein tyrosines of Pf1 exhibit Raman markers of ring environment identical to those of fd, including an anomalous singlet at 853 cm-1 in lieu of the canonical Fermi doublet (850/830 cm-1) found in globular proteins. The results indicate markedly different modes of organization of ssDNA in Pf1 and fd virions, despite similar environments for coat protein tyrosines, and suggest strong hydrogen-bonding interactions between DNA bases and coat subunits of Pf1 but not between those of fd. We propose that structural relationships between the protein coat and encapsidated ssDNA genome are also fundamentally different in the two assemblies.     

Protein influences on porphyrin structure in cytochrome c: evidence from Raman difference spectroscopy

To probe the details of protein heme interactions, we have developed a Raman difference spectroscopic technique, which allows reliable detection of very small, approximately equal to 0.01 cm-1, frequency differences. When this technique is applied to heme proteins, structural differences in the protein which perturb the porphyrin macrocycle may be examined by obtaining Raman difference data on the porphyrin vibrational modes which are strongly enhanced in the Raman spectrum produced with visible laser excitation. We report here Raman difference spectroscopic data on cytochromes c from 24 species. The differences in the Raman spectrum of the porphyrin between the cytochromes c of any two species are small, confirming that all of the cytochromes we have examined have the same "cytochrome fold". However, many small (0.02-2 cm-1) but systematic differences were detected which indicate structural differences among these proteins. These differences could be classified into three different groups and interpreted in terms of different types of structural variations resulting from specific differences in the amino acid sequences. First, direct interactions between near-heme residues and the porphyrin influence the electron density in the pi orbitals of the porphyrin macrocycle. Second, variation in the residue at position 92, far removed from the heme, affects the frequency of the core-size marker line at 1584 cm-1. Third, the conformation near cysteine 14 affects the shape of the Raman mode which is sensitive to the pyrrole ring substituents (approximately 1313 cm-1). From these data we conclude that there are several ways in which the protein amino acid sequence may regulate the oxidation-reduction potential and several ways in which the sequence can modify the binding site between cytochrome c and its redox partners.     

Z form of poly d(A-C).poly d(G-T) in solution studied by Raman spectroscopy.

Poly d(A-C).poly d(G-T) structures have been studied in solution by Raman spectroscopy, in presence of Na+, Mn2+ and Ni2+ counterions. Increase of the Na+ concentration or addition of Mn2+ ions up to 1M MnCl2 does not modify the B geometry of the polynucleotide. On the contrary, in conditions of low water activity (4M NaCl), the presence of small amounts of nickel ions (65 mM) induces a left-handed geometry of the DNA. The shift of the guanine line located at 682 cm-1 in B form to 622 cm-1 reflects unambiguously the C2'-endo/anti-greater than C3'-endo/syn reorientation of the deoxyribose-purine entities. Moreover modifications in the phosphate backbone lines indicate that the polymer is in a Z conformation. New or displaced lines corresponding to adenosine vibrations are correlated with the left-handed structure. An interaction of the Ni2+ ions specifically with the N7 site of purines, combined with a low water activity is necessary to promote the B-greater than Z transition.     

Mechanism of the control of dioxygen binding in a dimeric cobalt-substituted insect hemoglobin. Resonance Raman evidence for cobalt-axial-ligand bond changes

Resonance Raman spectroscopy has been used to investigate the allosteric control mechanism for O2 binding in a cobalt-substituted dimeric insect hemoglobin (CTT II), which exhibits a large Bohr effect due to a pH-induced transition between two ligand affinity states. Substitution of cobalt for iron in CTT II does not modify the Bohr effect, but permits the resonance enhancement (hence the detection) of Raman lines corresponding to the vibrations of the axial ligand-cobalt bonds. Using 16O2/18O2 isotope substitution the O-O and Co-O2 stretching and the Co-O-O bending mode have been assigned to the two affinity states of this hemoglobin: v (O-O) changes from 1152 cm-1 (pH 5.5; t conformation) to about 1125 cm-1 (pH 9.5, r conformation), v (Co-O2) from 512 cm-1 (pH 5.5) to 537 cm-1 (pH 9.5) and delta (Co-O-O) from 378 cm-1 (pH 5.5) to 390 cm-1 (pH 9.5). The Co-N epsilon (His) stretching mode has also been detected changing from 313 cm-1 (pH 5.5) to 307 cm-1 (pH 9.5). For the first time, reciprocal behaviour between the Co-N epsilon and Co-O2 bonds and between the Co-O2 and the O-O bonds in an allosteric hemoglobin are demonstrated. Furthermore, the pH sensitivity of a vinyl bending mode in the range of 411-415 cm-1 has been investigated and shown also to reflect the t in equilibrium with r conformation transition.     

Conformation of d(GGGATCCC)2 in crystals and in solution studied by X-ray diffraction, Raman spectroscopy and molecular modelling.

In the crystal, d(GGGATCCC)2 forms an A-DNA double helix as known from a single crystal X-ray diffraction study. Accordingly, in the Raman spectra of crystals the A-family marker bands at 664, 705, 807 and 1101 cm-1 and the spectral characteristics in the region 1200 to 1500 cm-1 clearly demonstrate the A-form as the dominant conformation. Bands at 691, 850, and 1080 cm-1, however, indicate that a minor fraction of the octamer molecules in the crystal is in an unusual, still not unequivocally identified conformation possibly belonging to the B-family. In solution, the octamer is in B-like conformation as shown by the presence of B-DNA Raman marker bands at 685, 837, 1094 and 1421 cm-1. Molecular modelling techniques lead to three structures with slightly different B-form geometries as the lowest energies models when a sigmoidal dielectric function with the bulk dielectric constant epsilon = 78 and the value q = -0.5e for the effective phosphate charges was used in the calculations. An A-form structure bearing a strong resemblance to the experimentally determined crystal structure becomes the lowest energy model structure when the electrostatic parameters are changed to epsilon = 30 and q = -0.25e, respectively.     

A Raman scattering study of the helix-destabilizing gene-5 protein with adenine-containing nucleotides.

Raman spectra of gp5 and complexes of gp5 with poly(rA) and poly(dA) have been determined and analysed. From a fit of the amide I-band with model spectra it follows that the secondary structure of gp5 contains 52% beta-sheet, 28% undefined conformation and 19% alpha-helix. The band at 1032 cm-1 due to phenylalanine has an anomalous intensity both in the spectra of the complexes and the free protein. This possibly indicates a stacked structure present in the protein. Binding of gp5 to poly(rA) and poly(dA) influences the intensity of bands near 1338 and 1480 cm-1 which are considered to be marker-bands for the phosphate-sugar-base conformer. A change in conformation of the nucleotides is also reflected by vibrations originating in the phosphate- and sugar-residues of the backbone. In the spectrum of complexed poly(rA) the intensity of the conformation sensitive band at 813 cm-1, which is due to the phosphodiester group, is zero. It seems that gp5 forces poly(rA) and poly(dA) to a similar conformation. A marker band for stacking interaction in poly(rA) indicates that stacking interactions in the complex have increased.