In situ analysis of mineral content and crystallinity in bone using infrared micro-spectroscopy of the nu(4) PO(4)(3-) vibration.

Measurements of bone mineral content and composition in situ provide insight into the chemistry of bone mineral deposition. Infrared (IR) micro-spectroscopy is well suited for this purpose. To date, IR microscopic (including imaging) analyses of bone apatite have centered on the nu(1),nu(3) PO(4)(3-) contour. The nu(4) PO(4)(3-) contour (500-650 cm(-1)), which has been extensively used to monitor the crystallinity of hydroxyapatite in homogenized bone samples, falls in a frequency region below the cutoff of the mercury-cadmium-telluride detectors used in commercial IR microscopes, thereby rendering this vibration inaccessible for imaging studies. The current study reports the first IR micro-spectroscopy spectra of human iliac crest cross sections in the nu(4) PO(4)(3-) spectral regions, obtained with a synchrotron radiation source and a Cu-doped Ge detector coupled to an IR microscope. The acid phosphate (HPO(4)(2-)) content and mineral crystallite perfection (crystallinity) of a human osteon were mapped. To develop spectra-structure correlations, a combination of X-ray powder diffraction data and conventional Fourier transform IR spectra have been obtained from a series of synthetic hydroxyapatite crystals and natural bone powders of various species and ages. X-ray powder diffraction data demonstrate that there is an increase in average crystal size as bone matures, which correlates with an increase in the nu(4) PO(4)(3-) FTIR absorption peak ratio of two peaks (603/563 cm(-1)) within the nu(4) PO(4)(3-) contour. Additionally, the IR results reveal that a band near 540 cm(-1) may be assigned to acid phosphate. This band is present at high concentrations in new bone, and decreases as bone matures. Correlation of the nu(4) PO(4)(3-) contour with the nu(2) CO (3)(2-) contour also reveals that when acid phosphate content is high, type A carbonate content (i.e., carbonate occupying OH(-) sites in the hydroxyapatite lattice) is high. As crystallinity increases and acid phosphate content decreases, carbonate substitution shifts toward occupation of PO(4)(3-) sites in the hydroxyapatite lattice. Thus, IR microscopic analysis of the nu(4) PO(4)(3-) contour provides a straightforward index of both relative mineral crystallinity and acid phosphate concentration that can be applied to in situ IR micro-spectroscopic analysis of bone samples, which are of interest for understanding the chemical mechanisms of bone deposition in normal and pathological states.     

FTIR spectra of solid poly-l-lysine in the stretching NH mode range

Three bands at 3270 cm(-1), 3200 cm(-1) and 3030 cm(-1) are found in the IR stretching proton (nu(1)) mode spectral range in spectra of solid poly-l-lysine (PLL). Strong quantitative changes of these bands are observed in samples dried from water solutions with different pH. The narrow band at 3270 cm(-1), which is strong in the spectrum of PLL precipitated from pH=12 alkaline medium, is assigned to the nu(1) peptide proton mode of NH-CO (amide A) of the beta-sheet structure type. The band at 3200 cm(-1), which is intensified in PLL precipitated from pH=1 acidic medium, relates to the nu(1) peptide mode in the random coil structure. The band at 3030 cm(-1), whose peak intensity increases two-fold in going from alkaline to acidic medium, is assigned to the nu(1) modes of protonated NH(3)(+) side chain groups. The frequencies of all bands were used for estimating H-bond energy relying on an empirical correlation between this property and the red shift of the nu(1) band. The enthalpy of the secondary structure transition from beta-sheet to the random coil, which is observed in PLL at the change of pH from 11 to 1 amounts to 4.7 kJ mol(-1).     

Redox infrared markers of the heme and axial ligands in microperoxidase: bases for the analysis of c-type cytochromes

Structural changes accompanying the change in the redox state of microperoxidase-8 (MP8), the heme-octapeptide obtained from cytochrome c, and its complexes with (methyl)imidazole ligands were studied by electrochemically induced Fourier transform IR (FTIR) difference spectroscopy. To correlate with confidence IR modes with a specific electronic state of the iron, we used UV-vis and electron paramagnetic resonance spectroscopy to define precisely the heme spin state in the samples at the millimolar concentration of MP8 required for FTIR difference spectroscopy. We identified four intense redox-sensitive IR heme markers, nu38 at 1,569 cm(-1) (ox)/1,554 cm(-1) (red), nu42 at 1,264 cm(-1) (ox)/1,242 cm(-1) (red), nu43 at 1,146 cm(-1) (ox), and nu44 at 1,124-1,128 cm(-1) (ox). The intensity of nu42 and nu43 was clearly enhanced for low-spin imidazole-MP8 complexes, while that of nu44 increased for high-spin MP8. These modes can thus be used as IR markers of the iron spin state in MP8 and related c-type cytochromes. Moreover, one redox-sensitive band at 1,044 cm(-1) (red) is attributed to an IR marker specific of c-type hemes, possibly the delta(CbH3)(2,4) heme mode. Other redox-sensitive IR bands were assigned to the MP8 peptide backbone and to the fifth and sixth axial heme ligands. The distinct IR frequencies for imidazole (1,075 cm(-1)) and histidine (1,105 cm(-1)) side chains in the imidazole-MP8 complex allowed us to provide the first direct determination of their pKa at pH 9 and 12, respectively.     

Micro-Raman characterisation of the R to T state transition of haemoglobin within a single living erythrocyte

We present the first recorded Raman spectra of haemoglobin in both the R and T states from within a single living erythrocyte using 632.8 nm excitation. Bands characteristic of low spin haems are observed in oxygenated and carboxylated erythrocytes at approx. 1636 (nu(10)), 1562-1565 (nu(2)), 1250-1245 cm(-1) (nu(13)) and 1226-1224 cm(-1) (nu(5)+nu(8)). The spectra of deoxygenated and methaemoglobin erythrocytes have characteristic high spin bands at approx. 1610-1606 cm(-1) (nu(10)), 1582-1580 (nu(37)), 1547-1544 (nu(11)), 1230-1220 cm(-1) (nu(13)) and 1215-1210 cm(-1) (nu(5)+nu(8)). Bands at 1172 (nu(30)), 976 (nu(45)) and 672 (nu(7)) cm(-1) appear to be enhanced at 632.8 nm in low spin haems. The oxidation state marker band (nu(4)) at 1364-1366 cm(-1) appeared invariant within this domain in all single cells and conditions investigated contrary to other resonance Raman studies on haem isolates. The information gained by in vivo single erythrocyte molecular analysis has important ramifications to the understanding of fundamental physiological processes and may have applications in the diagnosis and treatment of red blood cell disorders.     

IR and Raman study on the interactions of the 5′-GMP and 5′-CMP phosphate groups with Mg(II), Ca(II), Sr(II), Ba(II), Cr(III), Co(II), Cu(II), Zn(II), Cd(II), Al(III) and Ga(III)

The chief motive behind this research is the interest provoked by the presence of metal ions as necessary stabilizers of the negative charges of phosphate groups in nucleic acids. The effect that the presence of different metal ions produces on the band principally assigned to the nu(s) PO(3)(2-) mode has been studied using FT-IR and FT-Raman spectroscopy. The results obtained reveal the diagnostic capacity of these techniques in determining the type of metal ion interaction with respect to the mononucleotides that form DNA and RNA, providing a tool for improving the knowledge of the stabilizing or destabilizing effects of these ions on such macromolecules. The metal complexes of the ribonucleotides 5'-CMP and 5'-GMP with Mg(II), Ca(II), Sr(II), Ba(II), Cr(III), Co(II), Cu(II), Zn(II), Cd(II), Al(III) and Ga(III) were obtained in this study. After studying and analyzing the IR and Raman spectra of all these complexes and comparing them with the spectra of the corresponding disodium salts, it was verified that, independently of the type of nucleotide involved, the presence of the metal in the vicinity of the phosphate group produces an alteration in the aforementioned nu(s) PO(3)(2-) band. This effect is related to the type of interaction that the phosphate group has with the metal. Three components are observed: (1) one near 983-975 cm(-1) (detectable in IR and Raman), associated with phosphate groups in an electrostatic type of interaction with the metal ion, separated by two or more water molecules; (2) another near 989-985 cm(-1) (only in IR), associated with phosphate groups in indirect interaction through the water molecules of the coordination sphere of the metal ions; and (3) the IR and Raman bands near 1014-1001 cm(-1), which represent phosphate groups directly bonded to the metal ion. These results are supported by the behavior of 5'-CMP in aqueous solution in the presence of Mg(II) ions.     

A weak Fe-O bond in the oxygenated complex of the nitric-oxide synthase of Staphylococcus aureus

Little is known about the intermediates formed during catalysis by nitric-oxide synthase (NOS). We report here the characterization by resonance Raman spectroscopy of the oxygenated complex of the NOS from Staphylococcus aureus (saNOS) as well as the kinetics of formation and decay of the complex. An oxygenated complex transiently formed after mixing reduced saNOS with oxygen and decayed to the ferric enzyme with kinetics that were dependent on the substrate L-arginine and the cofactor H(4)B. The oxygenated complex displayed a Soret absorption band centered at 430 nm. Resonance Raman spectroscopy revealed that it can be described as a ferric superoxide form (Fe(III)O(2)(-)) with a single nu(O-O) mode at 1135 cm(-1). In the presence of L-arginine, an additional nu(O-O) mode at 1123 cm(-1) was observed, indicating an increased pi back-bonding electron donation to the bound oxygen induced by the substrate. With saNOS, this is the first time that the nu(Fe-O) mode of a NOS has been observed. The low frequency of this mode, at 517 cm(-1), points to an oxygenated complex that differs from that of P450(cam). The electronic structure of the oxygenated complex and the effect of L-arginine are discussed in relation to the kinetic properties of saNOS and other NOS.     

Structural heterogeneity of wheat arabinoxylans revealed by Raman spectroscopy

A set of arabinoxylan samples differing in their arabinose composition and various samples of arabino-xylo-oligosaccharide samples were analysed by Raman spectroscopy. Specific signatures for arabinose substitution were found in several spectral regions, that is, 400-600, 800-950 and 1030-1100 cm(-1). A linear relationship was observed between the peak ratio 855/895 cm(-1) of the second derivative spectra and the A/X ratio determined by chemical analysis. Moreover, spectral changes were observed in the 400-600 cm(-1) region assigned to the coupled vibrations mode in the skeleton: while the intensity of the band at 570 cm(-1) increased with the degree of substitution, that at 494 cm(-1) decreased. Similarly, a linear relationship was observed between the peak intensity ratio 570/494 cm(-1) calculated on the second derivative spectra and the composition data. Analysis of Raman spectra of arabino-xylo-oligosaccharides allowed to identify specific spectral features of disubstitution.     

Time-resolved resonance Raman and time-resolved step-scan FTIR studies of nitric oxide reductase from Paracoccus denitrificans: comparison of the heme b3-FeB site to that of the heme-CuB in oxidases

Time-resolved resonance Raman (TR(3)) and time-resolved step-scan (TRS(2)) FTIR spectroscopies have been used to probe the structural dynamics at the heme b(3) proximal and distal sites after carbon monoxide photolysis from fully reduced CO-bound nitric oxide reductase. The Raman spectra of the transient species exhibit structural differences relative to the equilibrium geometry of heme b(3). The most significant of these is a shift of 8 cm(-1) to higher frequency of the 207 cm(-1) mode, and a shift of 7 cm(-1) to lower frequency of the nu(4) mode. Our results indicate that the 207 cm(-1) mode observed in the equilibrium-reduced heme b(3) originates from nu(Fe-His). Its behavior in the photolytic transients indicates that the relaxed Fe-His state is not significantly populated. We suggest that relaxation along the tilt angle (theta) of the proximal histidine with respect to the heme plane and the out-of-plane displacement of the Fe (q) are coupled, and ligand binding and dissociation are accompanied by significant changes in the angular orientation of the His ligand. The results are compared to those obtained for the aa(3)-cytochrome c oxidase from Paracoccus denitrificans. The results are compared to those obtained for the aa(3)-cytochrome c oxidase from P. denitrificans. The TR(3) and TRS(2) FTIR data demonstrate significant alterations in the nature of the heme-protein dynamics between nitric oxide reductase and heme-copper oxidases resulting from specific structural differences in their respective hemepockets.     

Tyrosine Raman signatures of the filamentous virus Ff are diagnostic of non-hydrogen-bonded phenoxyls: demonstration by Raman and infrared spectroscopy of p-cresol vapor

p-Cresol is a simple molecular model for the para phenolic side chain of tyrosine. Previously, Siamwiza and co-workers [(1975) Biochemistry 14, 4870-4876] investigated p-cresol solutions to identify Raman spectroscopic signatures for different hydrogen-bonding states of the tyrosine phenoxyl group in proteins. They found that the phenolic moiety exhibits an intense Raman doublet in the spectral interval 820-860 cm(-1) and that the doublet intensity ratio (I2/I1, where I2 and I1 are Raman peak intensities of the higher- and lower-wavenumber members of the doublet) is diagnostic of specific donor and acceptor roles of the phenoxyl OH group. The range of the doublet intensity ratio in proteins (0.30 < I2/I1 < 2.5) was shown to be governed by Fermi coupling between the phenolic ring-stretching fundamental nu1 and the first overtone of the phenolic ring-deformation mode nu(16a), such that when the tyrosine phenoxyl proton is a strong hydrogen-bond donor, I2/I1 = 0.30, and when the tyrosine phenoxyl oxygen is a strong hydrogen-bond acceptor, I2/I1 = 2.5. Here, we interpret the Raman and infrared spectra of p-cresol vapor and extend the previous correlation to the non-hydrogen-bonded state of the tyrosine phenoxyl group. In the absence of hydrogen bonding, the Raman intensity of the higher-wavenumber component of the canonical Fermi doublet is greatly enhanced such that I2/I1 = 6.7. Thus, for the non-hydrogen-bonded phenoxyl, the lower-wavenumber member of the Fermi doublet loses most of its Raman intensity. This finding provides a basis for understanding the anomalous Raman singlet signature (approximately 854 cm(-1)) observed for tyrosine in coat protein subunits of filamentous viruses Ff and Pf1 [Overman, S. A., et al. (1994) Biochemistry 33, 1037-1042; Wen, Z. Q., et al. (1999) Biochemistry 38, 3148-3156]. The implications of the present results for Raman analysis of tyrosine hydrogen-bonding states in other proteins are considered.     

Heme structures of five variants of hemoglobin M probed by resonance Raman spectroscopy

The alpha-abnormal hemoglobin (Hb) M variants show physiological properties different from the beta-abnormal Hb M variants, that is, extremely low oxygen affinity of the normal subunit and extraordinary resistance to both enzymatic and chemical reduction of the abnormal met-subunit. To get insight into the contribution of heme structures to these differences among Hb M's, we examined the 406.7-nm excited resonance Raman (RR) spectra of five Hb M's in the frequency region from 1700 to 200 cm(-1). In the high-frequency region, profound differences between met-alpha and met-beta abnormal subunits were observed for the in-plane skeletal modes (the nu(C=C), nu(37), nu(2), nu(11), and nu(38) bands), probably reflecting different distortions of heme structure caused by the out-of-plane displacement of the heme iron due to tyrosine coordination. Below 900 cm(-1), Hb M Iwate [alpha(F8)His --> Tyr] exhibited a distinct spectral pattern for nu(15), gamma(11), delta(C(beta)C(a)C(b))(2,4), and delta(C(beta)C(c)C(d))(6,7) compared to that of Hb M Boston [alpha(E7)His --> Tyr], although both heme irons are coordinated by Tyr. The beta-abnormal Hb M variants, namely, Hb M Hyde Park [beta(F8)His --> Tyr], Hb M Saskatoon [beta(E7)His --> Tyr], and Hb M Milwaukee [beta(E11)Val --> Glu], displayed RR band patterns similar to that of metHb A, but with some minor individual differences. The RR bands characteristic of the met-subunits of Hb M's totally disappeared by chemical reduction, and the ferrous heme of abnormal subunits was no longer bonded with Tyr or Glu. They were bonded to the distal (E7) or proximal (F8) His, and this was confirmed by the presence of the nu(Fe-His) mode at 215 cm(-1) in the 441.6-nm excited RR spectra. A possible involvement of heme distortion in differences of reducibility of abnormal subunits and oxygen affinity of normal subunits is discussed.     

On-line monitoring of Phaffia rhodozyma fed-batch process with in situ dispersive Raman spectroscopy

Since the yeast Phaffia rhodozyma was first described some 35 years ago, there has been significant interest in the development of commercial processes to exploit its ability to produce carotenoids (approximately 80% astaxanthin). However, the optimal conditions for carotenoid production are not well understood. A key limitation has been the lack of an appropriate sensor for on-line carotenoid quantification. In this study, an in situ Raman spectroscopy probe was used to monitor intracellular carotenoid production for three consecutive P. rhodozyma fed-batch experiments. Raman spectroscopy is particularly well suited to the study of carotenoids due to a resonance effect, which greatly enhances the intensity of the three fundamental carotenoid bands, nu(1) (1513 cm(-1), C(-) (-)C stretch), nu(2) (1154 cm(-1), C-C stretch), and nu(3) (1003 cm(-1), CH(3) rock). For all three cultures, the peak height of these bands was linearly correlated with intracellular carotenoid content (1 to 45 mg/L) to a precision of better than 5%, and the correlation from one experiment was directly applicable to others.     

Raman spectroscopy investigation of various saturated monoacid triglycerides

A study of the vibrational behavior of five saturated monoacid triacylglycerides is performed by Raman spectroscopy at room temperature in the 3100-500 cm(-1) spectral range. The splitting of the CO stretching mode leads to conclude on the existence of two or three geometries of CO in the "knot" group OCO. The CO stretching mode seems to be a good tool for distinguishing the polymorphic forms of the studied triglycerides. The assignments of the different CH stretching modes are performed in the 1500-500 cm(-1) spectral range. The I(2845)/I(2880) (in the CH stretching spectral region) and I(1445)/I(1296) intensity ratios (between the maximal intensity I(1445) of the CH(2) scissoring mode and the maximal intensity I(1296) of the skeletal vibration of (CH(2))(n) in-phase twist) seem to depend on the type of polymorphic forms of these molecules.     

Vibrational spectroscopy to study the properties of redox-active tyrosines in photosystem II and other proteins

Tyrosine radicals play catalytic roles in essential metalloenzymes. Their properties--midpoint potential, stability...--or environment varies considerably from one enzyme to the other. To understand the origin of these properties, the redox tyrosines are studied by a number of spectroscopic techniques, including Fourier transform infrared (FTIR) and resonance Raman (RR) spectroscopy. An increasing number of vibrational data are reported for the (modified-) redox active tyrosines in ribonucleotide reductases, photosystem II, heme catalase and peroxidases, galactose and glyoxal oxidases, and cytochrome oxidase. The spectral markers for the tyrosinyl radicals have been recorded on models of (substituted) phenoxyl radicals, free or coordinated to metals. We review these vibrational data and present the correlations existing between the vibrational modes of the radicals and their properties and interactions formed with their environment: we present that the nu7a(C-O) mode of the radical, observed both by RR and FTIR spectroscopy at 1480-1515 cm(-1), is a sensitive marker of the hydrogen bonding status of (substituted)-phenoxyl and Tyr*, while the nu8a(C-C) mode may probe coordination of the Tyr* to a metal. For photosystem II, the information obtained by light-induced FTIR difference spectroscopy for the two redox tyrosines TyrD and TyrZ and their hydrogen bonding partners is discussed in comparison with those obtained by other spectroscopic methods.     

Resonance Raman spectra of riboflavin and its derivatives in the bound state with egg riboflavin binding proteins

The resonance Raman spectra of riboflavin (RF) and its derivatives, including 3-deuterated (3-D RF), 3-methyl (3-CH3 RF), 3-carboxymethyl (3-CH2COOH RF), and 7,8-dichlororiboflavins (7,8-Cl RF), in H2O and D2O were observed in the 700-1700 cm-1 region. The fluorescence problem of riboflavin was overcome by complex formation of riboflavin with riboflavin binding proteins. The observed frequencies of Raman lines of RF are in good agreement with those of glucose oxidase obtained by Spiro et al. by the resonance CARS method, although the present spectral range is extended to much lower frequency with a higher signal-to-noise ratio than that for glucose oxidase. The observed Raman lines were assigned to the individual ring modes of isoalloxazine on the basis of the Raman spectra of appropriate model compounds such as uracil, pyrazine, and o-xylene. The 1253 cm-1 line of RF was shifted to ca. 1300 cm-1 for 3-D RF, 3-CH3 RF, and 3-CH2COOH RF, and accordingly can be assigned to the CN stretching mode of Ring III. The 1632 cm-1 line of RF was shifted for 7,8-Cl RF and was assigned to a Ring I mode. No Raman line mainly due to C = O stretching mode was observed in the present resonance Raman spectra.     

Characterization of the heme environmental structure of cytoglobin,a fourth globin in humans

Cytoglobin (Cgb) represents a fourth member of the globin superfamily in mammals, but its function is unknown. Site-directed mutagenesis, in which six histidine residues were replaced with alanine, was carried out, and the results indicate that the imidazoles of His81 (E7) and His113 (F8) bind to the heme iron as axial ligands in the hexacoordinate and the low-spin state. The optical absorption, resonance Raman, and IR spectral results are consistent with this conclusion. The redox potential measurements revealed an E' of 20 mV (vs NHE) in the ferric/ferrous couple, indicating that the imidazole ligands of His81 and His113 are electronically neutral. On the basis of the nu(Fe-CO) and nu(C-O) values in the resonance Raman and infrared spectra of the ferrous-CO complexes of Cgb and its mutants, it was found that CO binds to the ferrous iron after the His81 imidazole is dissociated, and three conformers are present in the resultant CO coordination structure. Two are in closed conformations of the heme pocket, in which the bound CO ligand interacts with the dissociated His81 imidazole, while the third is in an open conformation. The nu(Fe-O2) in the resonance Raman spectra of oxy Cgb can be observed at 572 cm(-1), suggesting a polar heme environment. These structural properties of the heme pocket of Cgb are discussed with respect to its proposed in vivo oxygen storage function.     

Observation of the Fe4+ = O stretching Raman band for cytochrome oxidase compound B at ambient temperature

Resonance Raman and visible absorption spectra were simultaneously observed for cytochrome oxidase reaction intermediates at 5 degrees C by using the artificial cardiovascular system (Ogura, T., Yoshikawa, S., and Kitagawa, T. (1989) Biochemistry 28, 8022-8027) and a device for Raman/absorption simultaneous measurements (Ogura, T., and Kitagawa, T. (1988) Rev. Sci. Instrum. 59, 1316-1320). The Fe4+ = O stretching (nu FeO) Raman band was observed at 788 cm-1 for compound B for the first time. This band showed the 16O/18O isotopic frequency shift (delta nu FeO) by 40 cm-1, in agreement with that for horseradish peroxidase compound II (nu FeO = 787 cm-1 and delta nu FeO = 34 cm-1). In the time region when the FeII-O2 stretching band for compound A and the nu FeO band for compound B were coexistent, a Raman band assignable to the Fe3+-O-O-Cu2+ linkage was not recognized.     

Characterization of the CuA center in the cytochrome c oxidase from Thermus thermophilus for the spectral range 1800-500 cm-1 with a combined electrochemical and Fourier transform infrared spectroscopic setup

In this study we present the electrochemically induced Fourier transform infrared (FTIR) difference spectra of the Cu(A) center derived from the ba(3)-type cytochrome c oxidase of Thermus thermophilus in the spectral range from 1800 to 500 cm(-1). The mid infrared is dominated by the nu(C[double bond]O) vibrations of the amide I modes at 1688, 1660, and 1635 cm(-1), reflecting the redox-induced perturbation of the predominantly beta-sheet type structure. The corresponding amide II signal is found at 1528 cm(-1). In the lower frequency range below 800 cm(-1), modes from amino acids liganding the Cu(A) center are expected. On the basis of the absorbance spectrum of the isolated amino acids, methionine is identified as an important residue, displaying C-S vibrations at these frequencies. This spectral range was previously disregarded by protein IR spectroscopists, mainly due to the strong absorbance of the solvent, H(2)O. With an optimized setup, however, IR is found suitable for structure/function studies on proteins.     

Resonance raman studies of oxo intermediates in the reaction of pulsed cytochrome bo with hydrogen peroxide

Cytochrome bo from Escherichia coli, a member of the heme-copper terminal oxidase superfamily, physiologically catalyzes reduction of O(2) by quinols and simultaneously translocates protons across the cytoplasmic membrane. The reaction of its ferric pulsed form with hydrogen peroxide was investigated with steady-state resonance Raman spectroscopy using a homemade microcirculating system. Three oxygen-isotope-sensitive Raman bands were observed at 805/X, 783/753, and (767)/730 cm(-)(1) for intermediates derived from H(2)(16)O(2)/H(2)(18)O(2). The experiments using H(2)(16)O(18)O yielded no new bands, indicating that all the bands arose from the Fe=O stretching (nu(Fe)(=)(O)) mode. Among them, the intensity of the 805/X cm(-)(1) pair increased at higher pH, and the species giving rise to this band seemed to correspond to the P intermediate of bovine cytochrome c oxidase (CcO) on the basis of the reported fact that the P intermediate of cytochrome bo appeared prior to the formation of the F species at higher pH. For this intermediate, a Raman band assignable to the C-O stretching mode of a tyrosyl radical was deduced at 1489 cm(-)(1) from difference spectra. This suggests that the P intermediate of cytochrome bo contains an Fe(IV)=O heme and a tyrosyl radical like compound I of prostaglandin H synthase. The 783/753 cm(-)(1) pair, which was dominant at neutral pH and close to the nu(Fe)(=)(O) frequency of the oxoferryl intermediate of CcO, presumably arises from the F intermediate. On the contrary, the (767)/730 cm(-)(1) species has no counterpart in CcO. Its presence may support the branched reaction scheme proposed previously for O(2) reduction by cytochrome bo.     

Measurement of hemoglobin oxygen saturation using Raman microspectroscopy and 532-nm excitation.

The resonant Raman enhancement of hemoglobin (Hb) in the Q band region allows simultaneous identification of oxy- and deoxy-Hb. The heme vibrational bands are well known at 532 nm, but the technique has never been used to determine microvascular Hb oxygen saturation (So(2)) in vivo. We implemented a system for in vivo noninvasive measurements of So(2). A laser light was focused onto areas of 15-30 microm in diameter. Using a microscope coupled to a spectrometer and a cooled detector, Raman spectra were obtained in backscattering geometry. Calibration was performed in vitro using blood at several Hb concentrations, equilibrated at various oxygen tensions. So(2) was estimated by measuring the intensity of Raman signals (peaks) in the 1,355- to 1,380-cm(-1) range (oxidation state marker band nu(4)), as well as from the nu(19) and nu(10) bands (1,500- to 1,650-cm(-1) range). In vivo observations were made in microvessels of anesthetized rats. Glass capillary path length and Hb concentration did not affect So(2) estimations from Raman spectra. The Hb Raman peaks observed in blood were consistent with earlier Raman studies using Hb solutions and isolated cells. The correlation between Raman-based So(2) estimations and So(2) measured by CO-oximetry was highly significant for nu(4), nu(10), and nu(19) bands. The method allowed So(2) determinations in all microvessel types, while diameter and erythrocyte velocity could be measured in the same vessels. Raman microspectroscopy has advantages over other techniques by providing noninvasive and reliable in vivo So(2) determinations in thin tissues, as well as in solid organs and tissues in which transillumination is not possible.     

Resonance Raman studies indicate a unique heme active site in prostaglandin H synthase

Prostaglandin H synthase isoforms 1 and 2 (PGHS-1 and -2) catalyze the first two steps in the biosynthesis of prostaglandins. Resonance Raman spectroscopy was used to characterize the PGHS heme active site and its immediate environment. Ferric PGHS-1 has a predominant six-coordinate high-spin heme at room temperature, with water as the sixth ligand. The proximal histidine ligand (or the distal water ligand) of this hexacoordinate high-spin heme species was reversibly photolabile, leading to a pentacoordinate high-spin ferric heme iron. Ferrous PGHS-1 has a single species of five-coordinate high-spin heme, as evident from nu(2) at 1558 cm(-1) and nu(3) at 1471 cm(-1). nu(4) at 1359 cm(-1) indicates that histidine is the proximal ligand. A weak band at 226-228 cm(-1) was tentatively assigned as the Fe-His stretching vibration. Cyanoferric PGHS-1 exhibited a nu(Fe)(-)(CN) line at 446 cm(-1) and delta(Fe)(-)(C)(-)(N) at 410 cm(-1), indicating a "linear" Fe-C-N binding conformation with the proximal histidine. This linkage agrees well with the open distal heme pocket in PGHS-1. The ferrous PGHS-1 CO complex exhibited three important marker lines: nu(Fe)(-)(CO) (531 cm(-1)), delta(Fe)(-)(C)(-)(O) (567 cm(-1)), and nu(C)(-)(O) (1954 cm(-1)). No hydrogen bonding was detected for the heme-bound CO in PGHS-1. These frequencies markedly deviated from the nu(Fe)(-)(CO)/nu(C)(-)(O) correlation curve for heme proteins and porphyrins with a proximal histidine or imidazolate, suggesting an extremely weak bond between the heme iron and the proximal histidine in PGHS-1. At alkaline pH, PGHS-1 is converted to a second CO binding conformation (nu(Fe)(-)(CO): 496 cm(-1)) where disruption of the hydrogen bonding interactions to the proximal histidine may occur.