Metallocytochromes c: characterization of electronic absorption and emission spectra of Sn4+ and Zn2+ cytochromes c.

Tin (Sn4+) and zinc (Zn2+) derivatives of horse heart cytochrome c have been prepared and their optical spectra have been characterized. Zinc cytochrome c has visible absorption maxima at 549 and 585 nm and Soret absorption at 423 nm. Tin cytochrome c shows visible absorption maxima at 536 and 574 nm and Soret absorption at 410 nm. Unlike iron cytochrome c in which the emission spectrum of the porphyrin is almost completely quenched by the central metal, the zinc and tin derivatives of cytochrome c are both fluorescent and phosphorescent. The fluorescence maxima of zinc cytochrome c are at 590 and 640 nm and the fluorescence lifetime is 3.2 ns. The fluorescence maxima of Sn cytochrome are at 580 and 636 nm and the fluorescence lifetime is under 1 ns. The quantum yield of fluorescence is Zn greater than Sn while the quantum yield of phosphorescence is Sn greater than Zn. at 77 K the fluorescence and phosphorescence emission spectra of Sn and Zn cytochrome c show evidence of resolution into vibrational bands. The best resolved bands occur at frequency differences 750 cm-1 and 1540--1550 cm-1 from the O-O transition. These frequencies correspond with those obtained by resonance Raman spectroscopy for in-plane deformations of the porphyrin macrocycle.     

Resonance Raman evidence for an unusually strong exogenous ligand-metal bond in a monomeric nitrosyl manganese hemoglobin

Resonance Raman spectroscopy has been employed to determine the vibrational modes of monomeric nitrosyl manganese Chironomus thummi thummi hemoglobin (CTT IV). This insect hemoglobin has no distal histidine. By applying various isotope-labeled nitric oxides (14N16O, 15N16O, 14N18O), we have identified the Mn11-NO stretching model at 628 cm-1, the Mn11-N-O bending mode at 574 cm-1 and the N-O stretching mode at 1735 cm-1. The results suggest a strong Mn11-NO bond and a weak N-O bond. The vinyl group substitution does not influence the nu (Mn11-NO), delta (Mn11-N-O) and nu (N-O) vibrations. The Mn11-NO stretching frequency is insensitive to distal histidine interactions with NO, whereas the N-O stretching frequency is sensitive. Nitric oxide also binds to Met manganese CTT IV to form an Mn111. NO complex which undergoes a slow but complete autoreduction resulting in the Mn11.NO species. In manganese meso-IX CTT IV, the Mn111. NO Mn11. NO conversion alters the intensities of the porphyrin ring modes at 342, 360, 1587 and 1598 cm-1, but shifts the frequencies at 1504 and 1633 cm-1 (in Mn111.NO) to 1497 and 1630 cm-1 (in Mn11. NO), respectively. The unshifted marker line at 1378 cm-1 reflects the fact that the pi electron densities of the porphyrin ring are the same in the two complexes.     

Localization of repetitive and unique DNA sequences neighbouring the rabbit beta-globin gene

The structure of oxymyoglobin has been refined at 1·6 Å resolution, using diffractometer data collected at ?12 °C. The crystallographic R factor is 0·159, and the atomic positions are known to 0·1 Å accuracy in internal segments of the molecule.The iron atom lies 0·22(3) Å from the plane of the porphyrin, 0·25 Å closer than in deoxymyoglobin, and the F helix has moved by a similar amount. Oxygen binds to the iron in a bent, end-on arrangement, with FeOO = 115(5) ° and FeO = 1·83(6) Å. The mean FeN(porphyrin) bond length is 1·95(6) Å, 0·08 Å shorter than in deoxymyoglobin, but the difference is not significant compared to the experimental error. FeN_ε(His8F) is 2·07(6) Å, the same as in model compounds. Movements of the haem, iron, F helix and FG corner on oxygenation are similar to those found in the T-R state transition in haemoglobin, but are smaller in magnitude.     

Conformational transitions and vibronic couplings in acid ferricytochrome c: a resonance Raman study.

Resonance Raman spectral changes in ferricytochrome c as a function of pH between 6.7 and 1.0 are reported and the structural implication is discussed in terms of the "core-expansion" model advanced by L. D. Spaulding et al. [(1975) J. Am. Chem. Soc. 97, 2517]. The data are interpreted as indicating the iron in high-spin ferricytochrome c (at pH 2.0) with two water molecules as axial ligands lies in the plane of the porphyrin ring. At pH 1.0 there is a different high-spin form of cytochrome c which has an estimated iron out-of-plane distance of approximately 0.46 A. The effect of a monovalent anion at pH 2.0 is to produce a thermal spin mixture with predominant low-spin species. Excitation at approximately 620 nm in acid cytochrome c (pH 2.0) enhances only three depolarized ring vibrations at 1623, 1555, and 764 cm-1. Marked enhancement of depolarized modes relative to polarized and anomalously polarized modes is attributed to the vibronic coupling between porphyrin pi leads to pi and porphyrin pi leads to iron (dpi) charge-transfer states.     

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.     

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.     

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.     

Electron structure of the heme of reduced cytochrome P450 and P420 from the data of low-temperature magnetic circular dichroism

Magnetic circular dichroism spectra (MCD) of reduced cytochromes P450 and P420 from rabbit liver microsomes have been recorded and analyzed for the 350-600 nm spectral region in the temperature interval from 2 to 290 K. The shape, intensity and temperature dependence of the MCD of reduced P450 in the Soret region are quite different from that of other high-spin ferrous hemoproteins, whose heme iron is coordinated to the imidazole of histidine (deoxymyoglobin, deoxyhemoglobin, reduced peroxidase and cytochrome c oxidase). Assuming that in the reduced P450 as well as in its CO-complex the protein-derived ligand is mercaptide (RS-) the differences can be explained by the existence of two electronic transitions in the Soret region: the common for hemoproteins pi----pi porphyrin transition and sulfur to porphyrin charge-transfer transition, p+(Sp)----eg (pi). The unusual spectral characteristics of the CO-complex of P450 have been ascribed earlier to strong configurational interaction of these two transitions. From the similarities of the Soret MCD and their temperature dependences for the reduced P420 and for other high-spin ferrous hemoproteins one can conclude that heme iron of the reduced P420 is high-spin and is coordinated to the imidazole of histidine. The zero-field splitting parameter D of the spin Hamiltonian has been estimated from the MCD temperature dependences. The obtained splitting of approximately 30 cm-1 for P450 and of approximately 10 cm-1 for P420 exceeds that for myoglobin and hemoglobin (approximately 5 cm-1).     

Molecular changes following oxidoreduction of cytochrome b559 characterized by Fourier transform infrared difference spectroscopy and electron paramagnetic resonance: photooxidation in photosystem II and electrochemistry of isolated cytochrome b559 and iron protoporphyrin IX-bisimidazole model compounds.

The vibrational infrared absorption changes associated with the oxidation of cytochrome b559 (Cyt b559) have been characterized. In photosystem II (PS II) enriched membranes, low-potential (LP) and high-potential (HP) Cyt b559 were investigated by light-induced FTIR difference spectroscopy. The redox transition of isolated Cyt b559 is characterized by protein electrochemistry. On the basis of a model of the assembly of Cyt b559 with the two axial Fe ligands being histidine residues of two distinct polypeptides, each forming a transmembrane alpha-helix [Cramer, W.A., Theg, S.M., & Widger, W.R. (1986) Photosynth. Res. 10, 393-403], the bisimidazole and bismethylimidazole complexes of Fe protoporphyrin IX were electrochemically oxidized and reduced to detect the IR oxidation markers of the heme and its two axial ligands. Major bands at 1674/1553, 1535, and 1240 cm-1 are tentatively assigned to nu 37 (CaCm), nu 38-(CbCb) and delta (CmH) modes, respectively; other bands at 1626, 1613, 1455, 1415, and 1337 cm-1 are assigned to porphyrin skeletal and vinyl modes. Modes at 1103 and 1075/1066 cm-1 are assigned to the 4-methylimidazole and imidazole ligands, respectively. For the isolated Cyt b559, it is shown that both the heme (at 1556-1535, 1337, and 1239 cm-1), the histidine ligands at 1104 cm-1 and the protein (between 1600 and 1700 cm-1 and at 1545 cm-1) are affected by the charge stabilization. The excellent agreement between model compounds and isolated Cyt b559 reinforces the validity of the model of a heme iron coordinated to two histidine residues for Cyt b559. A differential signal at 1656/1641 cm-1 is assigned to peptide C = O mode(s). We speculate that this signal reflects the change in strength of a hydrogen bond formed between the histidine ligand(s) and the polypeptide backbone upon oxidoreduction of the cytochrome. In PS II membranes, the signals characteristic of Cyt b559 photooxidation are found at 1660/1652 and 1625 cm-1, for both the high- and low-potential forms. The differences observed in the amplitude of the 1660/1652-cm-1 band, at 1700 and 1530-1510 cm-1 in the light-induced FTIR difference spectra of Cyt b559 HP and LP, show that the mechanisms of heme oxidation in vivo imply different molecular processes for the two forms Cyt b559 HP and LP.     

Effects of a thiolate axial ligand on the π→π* electronic states of oxoferryl porphyrins: a study of the optical and resonance Raman spectra of compounds I and II of chloroperoxidase

Optical absorption and resonance Raman spectra have been investigated for enzymatic intermediates, compounds I and II, of chloroperoxidase (CPO) which contains a thiolate-ligated iron porphyrin. Compound I of CPO (CPO-I), an oxoferryl porphyrin pi cation radical, gave an apparently asymmetric single-peaked Soret band at 367 nm, for which band fitting analyses revealed the presence of two transition bands around 365 and 415 nm. Compound II of CPO (CPO-II), an oxoferryl neutral porphyrin, gave a split Soret spectrum with two bands (blue and red Soret bands) at 373 and 436 nm. Thus both CPO-I and CPO-II can be categorized as hyperporphyrins. The maximum extinction coefficients (epsilon(b) and epsilon(r)) and energies (Eb and Er) of the blue and red Soret bands of CPO-II were found to fall on an epsilon(b)/epsilon(r) versus Eb-Er correlation line derived from data reported for six-coordinate ferrous derivatives of cytochrome P450 and CPO. Corresponding data for CPO-I did not fall on the correlation line. Resonance enhancement of the FeIV=O stretching (vFeO) Raman band was found for CPO-I when Raman scattering was excited at wavelengths within both transition bands around 365 and 415 nm, while the vFeO Raman band was not identified for CPO-II at any of the excitation wavelengths examined here. These findings suggest that the thiolate axial ligand causes Soret band splitting of CPO-II through configuration interaction between the sulfur-->porphyrin e(g)* charge transfer and porphyrin a1u,a2u-->e(g)* transitions, while the FeO portion is important in determining the shape of the Soret band of CPO-I.     

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.     

Direct detection of Fe(IV)[double bond]O intermediates in the cytochrome aa3 oxidase from Paracoccus denitrificans/H2O2 reaction

We report the first evidence for the formation of the "607- and 580-nm forms" in the cytochrome oxidase aa3/H2O2 reaction without the involvement of tyrosine 280. The pKa of the 607-580-nm transition is 7.5. The 607-nm form is also formed in the mixed valence cytochrome oxidase/O2 reaction in the absence of tyrosine 280. Steady-state resonance Raman characterization of the reaction products of both the wild-type and Y280H cytochrome aa3 from Paracoccus denitrificans indicate the formation of six-coordinate low spin species, and do not support, in contrast to previous reports, the formation of a porphyrin pi-cation radical. We observe three oxygen isotope-sensitive Raman bands in the oxidized wild-type aa3/H2O2 reaction at 804, 790, and 358 cm-1. The former two are assigned to the Fe(IV)[double bond]O stretching mode of the 607- and 580-nm forms, respectively. The 14 cm-1 frequency difference between the oxoferryl species is attributed to variations in the basicity of the proximal to heme a3 His-411, induced by the oxoferryl conformations of the heme a3-CuB pocket during the 607-580-nm transition. We suggest that the 804-790 cm-1 oxoferryl transition triggers distal conformational changes that are subsequently communicated to the proximal His-411 heme a3 site. The 358 cm-1 mode has been found for the first time to accumulate with the 804 cm-1 mode in the peroxide reaction. These results indicate that the mechanism of oxygen reduction must be reexamined.     

M?ssbauer, EPR, and optical studies of the P-460 center of hydroxylamine oxidoreductase from Nitrosomonas. A ferrous heme with an unusually large quadrupole splitting

Hydroxylamine oxidoreductase from Nitrosomonas europeae catalyzes the oxidative conversion of NH2OH to NO-2. The enzyme, Mr = 220,000, has an (alpha beta)3 subunit structure with each alpha beta subunit containing 7-8 c-type hemes and one unusual prosthetic group, termed P-460. The P-460 is also found in a Mr approximately equal to 17,000 protein (P-460 fragment). M?ssbauer spectra of the reduced P-460 groups, in hydroxylamine oxidoreductase and the fragment, exhibit nearly identical quadrupole doublets with an unusually large splitting, delta EQ = 4.21 mm/s (no ferrous heme protein is known with delta EQ greater than 2.75 mm/s). The observed isomer shift, delta = 0.96 mm/s at 4.2 K, shows that the P-460 iron is high spin ferrous. Treatment of oxidized hydroxylamine oxidoreductase with H2O2 followed by reduction or exposure of the native sample to CO led to the disappearance of both the characteristic 460 nm absorption band (epsilon = 89 mM-1 cm-1) and the delta EQ = 4.21 mm/s doublet. The iron of the oxidized P-460 fragment is high spin ferric, with M?ssbauer and EPR parameters very similar to those of metmyoglobin. Optical spectra of the reduced P-460 fragment show long wavelength bands at 650 and 688 nm which are sensitive to treatment of the fragment with reagents which react with P-460. These bands were, however, not detected in hydroxylamine oxidoreductase. The spectroscopic and chemical evidence obtained to date suggests strongly that the P-460 iron resides in a heme-like macrocycle although the presumed porphyrin must have some unusual features.     

Resonance Raman study of cytochrome aa3 from Sulfolobus acidocaldarius.

The single subunit terminal oxidase of Sulfolobus acidocaldarius, cytochrome aa3, was studied by resonance Raman spectroscopy. Results on the fully oxidized, the fully reduced, and the reduced carbon monoxide complex are reported and compared with those of eucaryotic cytochrome oxidase. It is shown that in both redox states the hemes a and a3 are in the six-coordinated low-spin and six-coordinated high-spin configuration, respectively. The resonance Raman spectra reveal far-reaching similarities of this archaebacterial with mammalian or plant enzymes except for the reduced form of heme a. The formyl substituent of this heme appears above 1640 cm-1, ruling out significant hydrogen bonding interactions which is in sharp contrast to beef heart cytochrome oxidase. In addition, frequency upshifts of the marker bands v4 and v2 are noted indicating differences in the electron density distribution within the molecular orbitals of the porphyrin.     

Influence of heme-surrounding amino acid residues on the manganese (V)-nitrido bond in manganese-substituted hemoproteins: resonance Raman evidence for porphyrin core expansion and reduction of the manganese(V)-nitrido stretching force constant

Nitridomanganese(V) protoporphyrin IX was prepared by hypochlorite oxidation of the corresponding manganese(III) protoporphyrin IX derivative in the presence of ammonium ion and by photolysis of the corresponding azidomanganese(III) complex. Myoglobin and horseradish peroxidase containing this novel protoporphyrin derivative were prepared for the first time. These remarkably stable species were examined by electronic absorption, electron paramagnetic resonance, and resonance Raman spectroscopies. The MnV-N stretching modes of the nitridomanganese(V)-substituted myoglobin and horseradish peroxidase were observed at 1010 and 1003 cm-1, respectively, by resonance Raman spectroscopy, while the MnV-N stretching frequency for nitridomanganese(V) protoporphyrin IX in 0.1 N aqueous NaOH was found at 1046 cm-1. The equilibrium dissociation energies of MnV-N bonds in these complexes were estimated from vibrational overtone spacings by introducing the Morse potential energy function, were found to be around 4.5 eV, and seemed independent of the surroundings of the manganese porphyrin, although its force constant decreased from 7.3 to 6.7 mdyn/A upon incorporation into apoprotein. The porphyrin ring modes of these nitridomanganese(V) derivatives were influenced greatly upon incorporation into apoproteins, suggestive of the occurrence of porphyrin core expansion. Upon this core expansion the MnV center moves into the mean plane of porphyrin plane, but the access of nitrido (N) toward MnV is restricted due to a steric hindrance from porphyrin pyrrole nitrogens. The resulting stretched MnV-N bond might cause lowering of the MnV-N stretching frequency upon incorporation into apoprotein.     

Photoreduction of methemoglobin by irradiation in the near-ultraviolet region

Ferric metHb can be photoreduced to the ferrous state by direct photoexcitation in the near-ultraviolet region. In this research, we studied the mechanism and facilitating conditions for the photoreduction and the resulting restoration of O(2) binding. MetHb in phosphate-buffered saline or pure water in a CO atmosphere was photoreduced to form HbCO by illuminating the N band (365 nm), one of the porphyrin pi --> pi transitions, whereas the photoreduction did not occur in Ar, N(2), or O(2). The transient absorption spectrum exhibited the generation of deoxyHb within 30 ns in both the CO and Ar atmospheres; however, only in CO did the subsequent CO binding inhibit the back reaction. The photoreduction rate was dependent on the pH and ligand anions, showing that aquametHb in the high-spin state was predominant for the photoreduction. Axial ligand-to-metal charge-transfer (LMCT) bands overlap with the Soret and Q bands in metHb; however, the excitation of these bands showed little photoreduction, indicating that the contribution of these LMCT bands is minimal. Excitation of the N band significantly contributes to the photoreduction, and this is facilitated by the external addition of mannitol, hyaluronic acid, Trp, Tyr, etc. Especially, Trp allowed the photoreduction even in an Ar atmosphere, and the reduced Hb can be converted to HbO(2) by O(2) bubbling. One mechanism of the metHb photoreduction that is proposed on the basis of these results consists of a charge transfer from the porphyrin ring to the central ferric iron to form the porphyrin pi cation radical and ferrous iron by the N band excitation, and the contribution of the amino acid residues in the globin chain as an electron donor or an electron pathway.     

Observation of an isotope-sensitive low-frequency Raman band specific to metmyoglobin

A resonance Raman band involving significantly the iron(III)-histidine stretching (upsilonFe-His) character is identified for metmyoglobin (metMb) through isotope sensitivity of its low-frequency resonance Raman bands, but the identification was not successful for methemoglobin (metHb) and its isolated alpha and beta subunits. A band at 218 cm-1 of natural abundance metMb exhibited a low-frequency shift for 15N-His-labeled metMb (-1.4 cm-1 shift), while the strong porphyrin bands at 248 and 271 cm-1 did not shift significantly. The frequency of the 218-cm-1 band of metMb decreased by 1.6 cm-1 in D2O, probably due to Ndelta-deuteration of the proximal His, in a similar manner to that of the upsilonFe-His band of deoxyMb in D2O. This 218-cm-1 band shifted slightly to a lower frequency in H2(18)O, whereas it did little upon 54Fe isotopic substitution (<0.3 cm-1), presumably because of the six-coordinate structure. The lack of the 54Fe-isotope shift shows that the 218-cm-1 band is specific to metMb and not due to the deoxy species. The intensity of this band decreased for hydroxymetMb and was indiscernible for cyanometMb. For metHb and its alpha and beta subunits, however, the frequencies of the band around 220 cm-1 were not D2O sensitive. These results suggest an assignment of the band around 220 cm-1 to a pyrrole tilting mode, which significantly contains the Fe-His stretching character for metMb but scarcely for metHb and its subunits. The differences in the isotope sensitivity of this band in different proteins are considered to reflect the heme distortion from the planarity and the Fe-His geometry specific to individual proteins.     

Electron-oscillatory spectra of pyrimidine bases of nucleic acids in argon matrices

The studies on the oscillatory structure of adsorption spectra of pyrimidine bases of nucleic acids isolated in Ar matrix at 11 K are described. To clear up the importance of molecule isolation in the matrix, amorphous films of the materials studied were investigated experimentally at 11 and 77 K. The work was carried out using the low temperature optic attachment developed by the authors. The long wavelength band of cytosine and deuterocytosine in the matrix is shown to consist of two bands: 1) lambda max = 267 nm with oscillatory progressions of 500 and 400 cm-1, respectively, and 2) lambda max = 280 nm with progression approximately 800 cm-1. The first pi pi*-absorption band of 1-methylcytosine has a single oscillatory progression 470 cm-1. Thymine and uracil in Ar matrices form diffuse structural spectra of 630 and 660 cm-1, respectively. The oscillatory progressions are attributed to the oscillatory frequencies of the pyrimidine molecule ring oscillations in the excited state. The annealing of the matrix results for all the materials in smearing the oscillatory molecule structure up to its complete vanishing. In film samples the oscillatory structure is not seen at low temperatures.     

Infrared magnetic circular dichroism of myoglobin derivatives.

By use of a newly constructed CD instrument, infrared magnetic circular dichroism (MCD) spectra were observed for various myoglobin derivatives. The ferric high spin myoglobin derivatives such as fluoride, water and hydroxide complexes, commonly exhibited the MCD spectra consisting of positive A terms. Therefore, the results reinforced the assignment that the infrared band is the charge transfer transition to the degenerate excited state (eg (dpi)). Since the fraction of A term estimated was approximately 80% for myoglobin fluoride and approximately 35% for myoglobin water, the effective symmetry for myoglobin fluoride is determined to be as close as D4h, while that for myoglobin water seems to have lower symmetry components. The ferric low spin derivatives such as myoglobin cyanide, myoglobin imidazole and myoglobin azide showed positive MCD spectra which are very similar to the electronic absorption spectra. These MCD spectra were assigned to the charge transfer transitions from porphyrin pi to iron d orbitals on the ground that they were observed only for the ferric low spin groups and insensitive to the axial ligands. The lack of temperature dependence in the MCD magnitude indicated that the MCD spectra are attributable to the Faraday B terms. Deoxymyoglobin, the ferrous high spin derivative, had fairly strong positive MCD around 760 nm with an anisotropy factor (delta epsilon/epsilon) of 1.4-10(-4). It shows some small MCD bands from 800 to 1800 nm. Among the ferrous low spin derivatives, carbonmonoxymyoglobin did not give any observable MCD in the infrared region while oxymyoglobin seemed to have significant MCD in the range from 700 to 1000 nm.     

Resonance Raman enhancement of phenyl ring vibrational modes in phenyl iron complex of myoglobin.

Resonance Raman spectra are reported for the organometallic phenyl-FeIII complexes of horse heart myoglobin. We observed the resonance enhancement of the ring vibrational modes of the bound phenyl group. They were identified at 642, 996, 1,009, and 1,048 cm-1, which shift to 619, 961, 972, and 1,030 cm-1, respectively, upon phenyl 13C substitution. The lines at 642 and 996 cm-1 are assigned, respectively, as in-plane phenyl ring deformation mode (derived from benzene vibration No. 6a at 606 cm-1) and out-of-plane CH deformation (derived from benzene vibration No. 5 at 995 cm-1). The frequencies of the ring "breathing" modes at 1,009 and 1,048 cm-1 are higher than the corresponding ones in phenylalanine (at 1,004 and 1,033 cm-1) and benzene (at 992 and 1,010 cm-1), indicating that the ring C--C bonds are strengthened (or shortened) when coordinated to the heme iron. The excitation profiles of these phenyl ring modes and a porphyrin ring vibrational mode at 674 cm-1 exhibit peaks near its Soret absorption maximum at 431 nm. This appears to indicate that these phenyl ring modes may be enhanced via resonance with the Soret pi-pi transition. The FeIII--C bond stretching vibration has not been detected with excitation wavelengths in the 406.7-457.9-nm region.