Low-frequency vibrations in resonance Raman spectra of horse heart myoglobin. Iron-ligand and iron-nitrogen vibrational modes.

The low-frequency regions (150--700 cm-1) of resonance Raman (RR) spectra of various complexes of oxidized and reduced horse heart myoglobin were examined by use of 441.6-nm excitation. In this frequency range, RR spectra show 10 bands common to all myoglobin derivatives (numbered here for convenience from I to X). Relative intensities of bands IV, V, and X constitute good indicators of the doming state of the heme and, consequently, of the spin state of the iron atom. An additional band is present for several complexes (fluorometmyoglobin, hydroxymetmyoglobin, azidometmyoglobin, and oxymyoglobin). Isotopic substitutions on the exogenous ligands and of the iron atom (56Fe leads to 54Fe) allow us to assign these additional lines to the stretching vibrations of the Fe-sixth ligand bond. Similarly, bands II are assigned to stretching vibrations of the Fe-N-(pyrrole) bonds. An assignment of bands VI to stretching vibrations of the Fe-Nepsilon(proximal histidine) bonds is also proposed. Mechanisms for the resonance enhancement of the main low-frequency bands are discussed on the basis of the excitation profiles and of the dispersion curves for depolarization ratios obtained for fluorometmyoglobin and hydroxymetmyoglobin.     

Resonance Raman studies of Escherichia coli sulfite reductase hemoprotein. 1. Siroheme vibrational modes

Resonance Raman (RR) spectra are reported for the hemoprotein subunit (SiR-HP) of Escherichia coli NADPH-sulfite reductase (EC 1.8.1.2) in various ligation and redox states. Comparison of the RR spectra of extracted siroheme and the mu-oxo FeIII dimer of octaethylisobacteriochlorin with those of mu-oxo FeIII octaethylchlorin dimer and mu-oxo FeIII octaethylporphyrin dimer demonstrates that many siroheme bands can be correlated with established porphyrin skeletal modes. Depolarization measurements are a powerful tool in this correlation, since the 45 degrees rotation of the C2 symmetry axis of the isobacteriochlorin ring relative to the chlorin system results in reversal of the polarization properties (polarized vs anomalously polarized) of bands correlating with B1g and B2g modes of porphyrin. Various SiR-HP adducts (CO, NO, CN-, SO3(2-] show upshifted high-frequency bands, characteristic of the low-spin state and consistent with the expected core size sensitivity of the skeletal modes. Fully reduced unliganded SiR-HP (both siroheme and Fe4S4 cluster reduced) in liquid solution displays RR features comparable to those of high-spin ferrous porphyrins; on freezing, the RR spectrum changes, reflecting an apparent mixture of siroheme spin states. At intermediate reduction levels in solution a RR species is observed whose high-frequency bands are upshifted relative to oxidized and fully reduced SiR-HP. This spectrum, thought to arise from the "one-electron" state of SiR-HP (siroheme reduced, cluster oxidized), may be due to S = 1 FeII siroheme.     

Resonance Raman studies of Escherichia coli sulfite reductase hemoprotein. 3. Bound ligand vibrational modes

The vibrations of the bound diatomic heme ligands CO, CN-, and NO are investigated by resonance Raman spectroscopy in various redox states of Escherichia coli sulfite reductase hemoprotein, and assignments are generated by use of isotopically labeled ligands. For the fully reduced CO complex (ferrous siroheme, reduced Fe4S4 cluster) at room temperature, nu CO is observed at 1904 cm-1, shifting to 1920 cm-1 upon oxidation of the cluster. The corresponding delta FeCO modes are identified at 574 and 566 cm-1, respectively, by virtue of the zigzag pattern of their isotopic shifts. In frozen solution, two species are observed for the cluster-oxidized state, with nu CO at 1910 and 1936 cm-1 and nu FeC at 532 and 504 cm-1, respectively; nu FeC for the fully reduced species is identified at 526 cm-1 in the frozen state. For the ferrous siroheme-NO complex (cluster oxidized), nu NO is identified at 1555 cm-1 in frozen solution and a low-frequency mode is identified at 558 cm-1; this stretching mode is significantly lower than that observed in Mb-NO. For the ferric siroheme cyanide complexes evidence of two ligand-bonding forms is observed, with modes at 451/390 and 451/352 cm-1; they are distinguished by a reversal of the isotopic shift patterns of the upper and lower modes and could arise from a linear and a bent Fe-C unit, respectively. For the ferrous siroheme cyanide complex isotope-sensitive modes observed at 495 and 452 cm-1 are assigned to the FeCN- bending and FeC stretching vibrations, respectively.(ABSTRACT TRUNCATED AT 250 WORDS)     

Resonance Raman studies of iron spin and axial coordination in distal pocket mutants of ferric myoglobin

We have used resonance Raman spectroscopy to study 11 distal pocket mutants and the "wild type" and native ferric sperm whale myoglobin. The characteristic Raman core-size markers v4, v3, v2, and v10 are utilized to assign the spin and coordination state of each sample. It is demonstrated that replacements of the distal and proximal histidines can discriminate against H2O as a sixth ligand and favor a pentacoordinate Fe3+ atom. Soret absorption band blueshifts are correlated with the pentacoordinate heme environment. One E7 replacement (Arg) leads to an iron spin state change and produces a low spin species. The Glu and Ala mutations at position E11 leave the protein's spin and coordination unaltered. A laser-induced photoreduction effect is observed in all pentacoordinate mutants and seems to be correlated with the loss of the heme-bound water molecule.     

Resonance Raman studies of Escherichia coli sulfite reductase hemoprotein. 2. Fe4S4 cluster vibrational modes

Resonance Raman (RR) spectra from the hemoprotein subunit of Escherichia coli sulfite reductase (SiR-HP) are examined in the low-frequency (200-500 cm-1) region where Fe-S stretching modes are expected. In spectra obtained with excitation in the siroheme Soret or Q bands, this region is dominated by siroheme modes. Modes assignable to the Fe4S4 cluster are selectively enhanced, however, with excitation at 488.0 or 457.9 nm. The assignments are confirmed by observation of the expected frequency shifts in SiR-HP extracted from E. coli grown on 34S-labeled sulfate. The mode frequencies and isotopic shifts resemble those seen in RR spectra of other Fe4S4 proteins and analogues, but the breathing mode of the cluster at 342 cm-1 is higher than that observed in the other species. Spectra of various ligand complexes of SiR-HP reveal only slight sensitivity of the cluster terminal ligand modes to the presence of exogenous heme ligands, at variance with a model of ligand binding in a bridged mode between heme and cluster. Close examination of RR spectra obtained with siroheme Soret-band excitation reveals additional 34S-sensitive features at 352 and 393 cm-1. These may be attributed to a bridging thiolate ligand.     

Resonance Raman investigation of an enzyme-inhibitor complex.

The resonance Raman spectrum has been recorded for two different binary complexes formed between 2-carboxy-2'-hydroxy-5'-sulfoformazylbenzene (zincon) and liver alcohol dehydrogenase. The shifts in the zincon spectrum upon complexation with enzyme in one complex are similar to those in model compounds containing azo or formazyl linkages upon complexation of these with zinc. The results are interpreted in terms of complexation of zincon to a zinc atom at the enzyme active site. Since zincon is a coenzyme competitive inhibitor, it is probably bound at or near the coenzyme binding site; the results of this study, therefore, are useful in understanding the chemistry of zinc at the enzyme active site.     

Resonance Raman spectroscopic studies of hydroperoxo derivatives of cobalt-substituted myoglobin

Recent progress in generating and stabilizing reactive heme protein enzymatic intermediates by cryoradiolytic reduction has prompted application of a range of spectroscopic approaches to effectively interrogate these species. The impressive potential of resonance Raman spectroscopy for characterizing such samples has been recently demonstrated in a number of studies of peroxo- and hydroperoxo-intermediates. While it is anticipated that this approach can be productively applied to the wide range of heme proteins whose reaction cycles naturally involve these peroxo- and hydroperoxo-intermediates, one limitation that sometimes arises is the lack of enhancement of the key intraligand ν(O-O) stretching mode in the native systems. The present work was undertaken to explore the utility of cobalt substitution to enhance both the ν(Co-O) and ν(O-O) modes of the CoOOH fragments of hydroperoxo forms of heme proteins bearing a trans-axial histidine linkage. Thus, having recently completed RR studies of hydroperoxo myoglobin, attention is now turned to its cobalt-substituted analogue. Spectra are acquired for samples prepared with ¹⁶O₂ and ¹⁸O₂ to reveal the ν(M-O) and ν(O-O) modes, the latter indeed being observed only for the cobalt-substituted proteins. In addition, spectra of samples prepared in deuterated solvents were also acquired, providing definitive evidence for the presence of the hydroperoxo-species.     

Resonance Raman assignment and evidence for noncoupling of individual 2- and 4-vinyl vibrational modes in a monomeric cyanomethemoglobin

We have investigated the resonance Raman spectra of monomeric insect cyanomethemoglobins (CTT III and CTT IV) reconstituted with (1) protohemes IX selectively deuterated at the 4-vinyl as well as the 2,4-divinyls, (2) monovinyl-truncated hemes such as pemptoheme (2-hydrogen, 4-vinyl) and isopemptoheme (2-vinyl, 4-hydrogen), (3) symmetric hemes such as protoheme III (with 2- and 3-vinyls) and protoheme XIII (with 1- and 4-vinyls), and (4) hemes without 2- and 4-vinyls such as mesoheme IX, deuteroheme IX, 2,4-dimethyldeuteroheme IX, and 2,4-dibromodeuteroheme IX. Evidence is presented that the highly localized vinyl C = C stretching vibrations at the 2- and 4-positions of the heme in these cyanomet CTT hemoglobins are noncoupled and inequivalent; i.e., the 1631- and 1624-cm-1 lines have been assigned to 2-vinyl and 4-vinyl, respectively. The elimination of the 2-vinyl (in pemptoheme) or the 4-vinyl (in isopemptoheme) does not affect the C = C stretching frequency of the remaining vinyl. Furthermore, two low-frequency vinyl bending modes at 412 and 591 cm-1 exhibit greatly different resonance Raman intensities between 2-vinyl and 4-vinyl. The observed intensity at 412 cm-1 is primarily derived from 4-vinyl, whereas the 591-cm-1 line results exclusively from the 2-vinyl. Again, there is no significant coupling between 2-vinyl and 4-vinyl for these two bending modes.     

Resonance Raman enhancement of FeIV=O stretch in high-valent iron porphyrins: an insight from TD-DFT calculations

Density functional theory (DFT) has been applied to explain the origin of resonance Raman enhancement associated with the Fe(IV)=O stretch observed in iron(IV)oxo porphyrins. To accomplish this electronic excitations of the Im-(Por)Fe(IV)=O model were computed in the 1.5-4.0 eV spectral range using time-dependent DFT (TD-DFT). All electronic transitions having dominant pi-->pi* character were analyzed and assigned in terms of one-electron excitations. It was found that the most intense Soret band has a multi-component character, but the pi (a(2u))-->pi*(d(xz),d(yz)) and pi (a(1u))-->pi*(d(xz),d(yz)) electronic excitations are primarily responsible for observed resonance enhancement of the Fe(IV)=O stretch.     

Resonance Raman studies and structure of a sulfide complex of methemerythrin.

The complex of sulfide and methemerythrin has been characterized by resonance Raman spectroscopy. At pH 8.0 the complex contains two irons and one S2- at the active site. The resonance Raman spectrum of the sulfidomethemerythrin complex contains only one vibration, at 444 cm-1. This vibration is assigned to an iron-sulfide stretch. The possibility that sulfidomethemerythrin contains a mu-sulfido bridge. FeIII-S2-FeIII, analogous to the proposed mu-oxo bridge in azidomethemerythrin is discussed.     

Time-resolved resonance Raman study on ultrafast structural relaxation and vibrational cooling of photodissociated carbonmonoxy myoglobin

A localized small structural change is converted to a higher order conformational change of protein and extends to a mesoscopic scale to induce a physiological function. To understand such features of protein, ultrafast dynamics of myoglobin (Mb) following photolysis of carbon monoxide were investigated. Recent results are summarized here with a stress on structural and vibrational energy relaxation. The core expansion of heme takes place within 2 ps but the out of plane displacement of the heme iron and the accompanying protein conformational change occur in 10 and 100 s of the picosecond regimes, respectively. Unexpectedly, it was found from UV resonance Raman spectra that Trp7 in the N-terminal region and Tyr151 in the C-terminal region undergo appreciable structural changes upon ligand binding-dissociation while Tyr104, Tyr146, and Trp14 do not. Because of the communication between the movements of these surface residues and the heme iron, the rate of spectral change of the iron-histidine (Fe- His) stretching band after CO photodissociation is influenced by the viscosity of solvent. Temporal changes of the anti-Stokes Raman intensity demonstrated immediate generation of vibrationally excited heme upon photodissociation and its decay with a time constant of 1-2 ps.     

Resonance Raman interrogation of the consequences of heme rotational disorder in myoglobin and its ligated derivatives

Resonance Raman spectroscopy is employed to characterize heme site structural changes arising from conformational heterogeneity in deoxyMb and ligated derivatives, i.e., the ferrous CO (MbCO) and ferric cyanide (MbCN) complexes. The spectra for the reversed forms of these derivatives have been extracted from the spectra of reconstituted samples. Dramatic changes in the low-frequency spectra are observed, where newly observed RR modes of the reversed forms are assigned using protohemes that are selectively deuterated at the four methyl groups or at the four methine carbons. Interestingly, while substantial changes in the disposition of the peripheral vinyl and propionate groups can be inferred from the dramatic spectral shifts, the bonds to the internal histidyl imidazole ligand and those of the Fe-CO and Fe-CN fragments are not significantly affected by the heme rotation, as judged by lack of significant shifts in the nu(Fe-N(His)), nu(Fe-C), and nu(C-O) modes. In fact, the apparent lack of an effect on these key vibrational parameters of the Fe-N(His), Fe-CO, and Fe-CN fragments is entirely consistent with previously reported equilibrium and kinetic studies that document virtually identical functional properties for the native and reversed forms.     

Resonance Raman evidence of chloride binding to the heme iron in myeloperoxidase

The resonance Raman spectra of ferric derivatives of myeloperoxidase at pH 8 show ligand-dependent differences. The data are consistent with the resting enzyme and the chloride and fluoride derivatives all having 6-coordinated high-spin configurations. At pH 4 we find that the resting enzyme is susceptible to photodegradation from our low power incident laser beam. Chloride binding inhibits this denaturation. Our data support direct binding of chloride to the enzyme under physiological conditions.     

Resonance Raman studies of the HOOP modes in octopus bathorhodopsin with deuterium-labeled retinal chromophores

Resonance Raman spectra of the hydrogen out-of-plane (HOOP) vibrational modes in the retinal chromophore of octopus bathorhodopsin with deuterium label(s) along the polyene chain have been obtained. In clear contrast with bovine bathorhodopsin's HOOP modes, there are only two major HOOP bands at 887 and 940 cm-1 for octopus bathorhodopsin. On the basis of their isotopic shifts upon deuterium labeling, we have assigned the band at 887 cm-1 to C10H and C14H HOOP modes, and the band at 940 cm-1 to C11H = C12H Au-like HOOP mode. Except for a 26 cm-1 downward shift, the C11H = C12H Au-like wag appears to be little disturbed in octopus bathorhodopsin from the chromophore in solution since its changes upon deuterium labeling are close to those found in solution model-compound studies. We found also that the C10H and C14H HOOP wags are also similar to those in the model-compound studies. However, we have found that the interaction between the C7H and C8H HOOP internal coordinates of the chromophore in octopus bathorhodopsin is different from that of the chromophore in solution. The intensity of the C11H = C12H and the other HOOP modes suggests that the chromophore of octopus bathorhodopsin is somewhat torsionally distorted from a planar trans geometry. Importantly, a twist about C11 = C12 double bond is inferred. Such a twist breaks the local symmetry, resulting in the observation of the normally Raman-forbidden C11H = C12H Au-like HOOP mode. The twisted nature of the chromophore, semiquantitatively discussed here, likely affects the lambda max of the chromophore and its enthalpy.(ABSTRACT TRUNCATED AT 250 WORDS)     

Resonance Raman spectra of bovine liver catalase: enhancement of proximal tyrosinate vibrations

Resonance Raman spectra of native bovine liver ferri-catalase have been obtained in the 200-1800 cm-1 region. Excitation at a series of wavelengths ranging from 406.7 to 514.5 nm has been used and gives rise to distinct sets of resonance Raman bands. Excitation within the Soret and Q-bands of the heme group produces the expected set of polarized and nonpolarized porphyrin modes, respectively. The frequencies of the porphyrin skeletal stretching bands in the 1450-1700 cm-1 region indicate that catalase contains only five-coordinate, high-spin heme groups. In addition to the porphyrin modes, bovine liver catalase exhibits bands near 1612 and 1520 cm-1 that are attributable to ring vibrations of the proximal tyrosinate that are enhanced via resonance with a proximal tyrosinate----Fe(III) change transfer transition centered near 490 nm. Similar bands have been observed in mutant hemoglobins that have tyrosinate axial ligands and in other Fe(III)-tyrosinate proteins. No resonance Raman bands have been observed that can be attributed to degraded hemes. The spectra are relatively insensitive to pH over the range of 5-10, and the same spectra are observed for catalase samples that do and do not contain tightly bound NADPH. Resonance Raman spectra of the fluoride complex exhibit porphyrin skeletal stretching modes that show it to be six coordinate, high spin, while the cyanide complex is six coordinate, low spin. Both the azide and thiocyanate complexes, however, are spin-state mixtures with the high-spin form predominant.     

Resonance Raman studies of ETE dehydrogenase (an iron sulfur flavoprotein)

ETF Dehydrogenase is an iron sulfur flavoprotein responsible for the transfer of electrons between electron transfer flavoprotein (ETF) and CoQ of the electron transport chain. We have determined the resonance Raman spectrum of this enzyme observing in the process at least seven of thirteen flavin bands in the 1100cm-1-1600 cm-1 region of the Raman spectrum. The positions of three of these bands, II, IX, and X (see Figure I and Table I for band numbering system) in ETF dehydrogenase is very similar to their positions in aqueous solution of flavins in which water is hydrogen bonded to N-1, N-5, C=0(2), C=0(4), and N-H(3) of flavin. Conversely the positions of the flavin Raman bands are considerably shifted from those of flavin in nonhydrogen bonding solvent. The positions of bands II, IX, and X are nearly identical to those in the flavoprotein glutathione reductase; x-ray structural investigations on this enzyme indicate that there is extensive hydrogen bonding between FAD and protein in this molecule. A previous study in our laboratory has demonstrated that metal complexation at N-5 and C=0(4) with either Ru or Ag produces large shifts in the positions of Raman bands II, VI, IX, and X. None of these shifts are observed in ETF dehydrogenase indicating that there is no direct inner sphere coordination of Fe to flavin. In addition to the Raman bands of flavin observed in our spectrum, we also observe one band that is in the Fe-S stretching region observed for a variety of Fe-S proteins. This band is located at 331 cm-1. The frequency of the band corresponds to the 335 cm-1 band associated with the strongest Fe-S stretching mode in the 4Fe-4S protein ferrodoxin from C. pasterianum. The observed frequency is quite different from that of the 3Fe-3S proteins such as ferrodoxin(II) from D. gigas. Finally, ETF dehydrogenase shows no loss of activity or visual evidence of photodegradation in the laser beam as most other FeS proteins do.