Inter- and intramolecular disulfide bond formation and related structural changes in the lens proteins. A Raman spectroscopic study in vivo of lens aging

Raman spectra have been measured for intact rat lens nuclei at various stages of aging in an attempt to gain further insight into age-related structural changes in the lens proteins, especially changes concerning protein sulfhydryl groups. Two Raman bands at 2579 and 2561 cm-1 were observed to be assignable to SH stretching modes of the cysteine residues. These bands have been attributed to "exposed" and "buried" sulfhydryl groups of the lens proteins, respectively, on the basis of a model compound study. The relative intensities of both SH stretching modes decreased with lens aging, and concurrently the intensity of a S-S stretching mode at 509 cm-1 due to disulfide bridges increased, suggesting that not only exposed but also buried protein sulfhydryl groups are converted to disulfide groups as a result of aging. The rate of the intensity decrease in the 2561 cm-1 band was similar to that in the 2579 cm-1 band. Therefore, it seems likely that the sulfhydryl groups in the two distinct environments are nearly equally subjected to the oxidation. Cysteine and cystine residues of the lens proteins gave their C-S stretching modes at 708 cm-1, indicating that they predominantly assume PC and/or PN conformers. The intensity ratio of a tyrosine doublet near 840 cm-1 (I832/I855) changed from approximately 0.86 to approximately 0.81 with the aging of the rat lens. This result implies that some tyrosine residues undergo a change in their hydrogen bonding environments during the course of aging. Of particular importance is that the relative intensity change of the tyrosine doublet with normal aging and that with cataract formation are in opposite directions.     

Observation of the FeIV=O stretching Raman band for a thiolate-ligated heme protein. Compound I of chloroperoxidase.

The FeIV=O stretching vibration has never been identified for a cysteine-coordinated heme enzyme. In this study, resonance Raman and visible absorption spectra were observed simultaneously for transient species in the catalytic reaction of chloroperoxidase with hydrogen peroxide by using our original apparatus for mixed-flow and Raman/absorption simultaneous measurements. For the first intermediate, the FeIV=O stretching Raman band was observed at 790 cm-1, which shifted to 756 cm-1 with the 18O derivative, but the v4 band was too weak to be identified. This suggested the formation of an oxoferryl porphyrin pi cation radical. The second intermediate gave an intense v4 band at 1,372 cm-1 but no oxygen isotope-sensitive Raman band, suggesting oxygen exchange with bulk water.     

Unusually strong H-bonding to the heme ligand and fast geminate recombination dynamics of the carbon monoxide complex of Bacillus subtilis truncated hemoglobin

The active site of the oxygen-avid truncated hemoglobin from Bacillus subtilis has been characterized by infrared absorption and resonance Raman spectroscopies, and the dynamics of CO rebinding after photolysis has been investigated by picosecond transient absorption spectroscopy. Resonance Raman experiments on the CO bound adduct revealed the presence of two Fe-CO stretching bands at 545 and 520 cm-1, respectively. Accordingly, two C-O stretching bands at 1924 and 1888 cm-1 were observed in infrared absorption and resonance Raman measurements. The very low C-O stretching frequency at 1888 cm-1 (corresponding to the extremely high RR stretching frequency at 545 cm-1) indicates unusually strong hydrogen bonding between CO and distal residues. On the basis of a comparison with other truncated hemoglobin it is envisaged that the two CO conformers are determined by specific interactions with the TrpG8 and TyrB10 residues. Mutation of TrpG8 to Leu deeply alters the hydrogen-bonding network giving rise mainly to a CO conformer characterized by a Fe-CO stretching band at 489 cm-1 and a CO stretching band at 1958 cm-1. Picosecond laser photolysis experiments carried out on the CO bound adduct revealed dynamical processes that take place within a few nanoseconds after photolysis. Picosecond dynamics is largely dominated by CO geminate rebinding and is consistent with strong H-bonding contributions of TyrB10 and TrpG8 to ligand stabilization.     

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.     

Interaction of ferricytochrome c with zwitterionic phospholipid bilayers: a Raman spectroscopic study

The vibrational Raman spectra of both pure L-alpha-dipalmitoylphosphatidylcholine (DPPC) liposomes and DPPC multilayers reconstituted with ferricytochrome c under varying conditions of pH and ionic strength are reported as a function of temperature. Total integrated band intensities and relative peak height intensity ratios, two spectral scattering parameters used to determine bilayer disorder, are invariant to changes in pH and ionic strength but exhibit a sensitivity to the bilayer concentration of the ferricytochrome c. Protein concentrations were estimated by comparing the 1636 cm-1 resonance Raman line of known ferricytochrome c solutions to intensity values for the reconstituted multilayer samples. Temperature-dependent profiles of the 3100-2800 cm-1 C-H stretching, 1150-1000 cm-1 C-C stretching, 1440 cm-1 CH2 deformation, and 1295 cm-1 CH2 twisting mode regions characteristic of acyl chain vibrations reflect bilayer perturbations due to the weak interactions of ferricytochrome c. The DPPC multilamellar gel to liquid-crystalline phase transition temperature, TM, defined by either the C-H stretching mode I2935/I2880 or the C-C stretching mode I1061/I1090 peak height intensity ratios, is decreased by approximately 4 degrees C for the approximately 10(-4) M ferricytochrome c reconstituted DPPC liposomes. Other spectral features, such as the increase in the 2935 cm-1 C-H stretching mode region and the enhancement of higher frequency CH2 twisting modes, which arise in bilayers containing approximately 10(-4) M protein, are interpreted in terms of protein penetration into the hydrophobic region of the bilayer.     

Laser Raman investigations of intact single muscle fibers. Protein conformations

Raman spectra, in the frequency region of the protein vibrations, of intact single muscle fibers of the giant barnacle are presented. Strong bands at 1521 and 1156 cm-1 in the spectra are attributed to resonance-enhanced Raman bands of membrane-bound beta-carotene. Many bands of the myofibrillar proteins are also observed, and at least three spectral features confirm that these proteins adopt a predominantly alpha-helical structure: (1) the amide I band at 1648 cm-1, (2) the weak scattering in the amide III region, and (3) a strong skeletal C-C stretching band at 939 cm-1. Deuterated fibers have also been examined in order to find the exact shape of the amide III band. The presence in the fibers of paramyosin, which is only found in catch muscles, is also apparent from the spectra.     

Conformation of oxytocin studied by laser Raman spectroscopy

The peptide backbone conformation and salient structural details of oxytocin were examined by laser Raman spectroscopy. Spectra were obtained in the solid phase, water, 2H2O, and dimethyl sulfoxide solutions. A distinct Amide I band was obtained at 1663 cm-1 for aqueous and deuterated samples and 1666 cm-1 for the solid sample. A relatively high frequency Amide III band at 1260 cm-1 was obtained. It is concluded that these Amide I and III bands arise from the "beta-turn"-like conformation of oxytocin. The tyrosine side chain, according to the I850 cm-1/I830 cm-1 intensity ratio, is exposed to the solvent. The S-S stretching vibration at 512 cm-1 indicates the conformation of C-C-S-S-C-C in the disulfide bridge of oxytocin in the ring is gauche-gauche-gauche.     

Structure of the retinal chromophore in the hR578 form of halorhodopsin

Halorhodopsin is a retinal-containing pigment that is thought to function as a light-driven chloride ion pump in the cell membrane of Halobacterium halobium. To address the role of the retinal chromophore in chloride ion transport, resonance Raman spectra have been obtained of the hR578 form of chromatographically purified halorhodopsin (hR). The close similarity of the frequencies and intensities of the hR578 Raman bands with those of light-adapted bacteriorhodopsin (bR568) shows that the chromophore in hR578 has an all-trans configuration and that the protein environment around the chromophore in these two pigments is very similar. In addition, hR578 exhibits a Raman line at 1633 cm-1 which is assigned as the stretching vibration of a protonated Schiff base linkage to the protein based on its shift to 1627 cm-1 in D2O. The reduced frequency of the Schiff base stretching vibration compared with bR568 (1640 cm-1) is shown to result from a reduction of its coupling with the NH in-plane rock. This may be due to a reduction in hydrogen-bonding between the Schiff base proton and an electronegative counterion in halorhodopsin.     

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.     

Resonance Raman examination of axial ligand bonding and spin-state equilibria in metmyoglobin hydroxide and other heme derivatives

Resonance Raman spectra and excitation profiles have been obtained within the 5700-6300-A absorption band of purified sperm whale metmyoglobin hydroxide (MbIIIOH) solutions. A large enhancement occurs for a Raman peak at 490 cm-1 which is shown by isotopic substitution of 18O for 16O to be almost purely an Fe-O stretch. The Fe-O vibration in MbIIIOH occurs 5 cm-1 to lower energy than the corresponding vibration at 495 cm-1 in human methemoglobin hydroxide (HbIIIOH) [Asher, S., Vickery, L., Schuster, T., & Sauer, K. (1977) Biochemistry 16, 5849], reflecting differences in ligand bonding between Mb(III) and Hb(III). A larger frequency difference (10 cm-1) exists between MbIIIF and HbIIIF for the Fe-F stretch. We do not observe separate Fe-O or Fe-F stretches from the alpha and beta chains of either HbIIIOH or HbIIIF. Excitation profile measurements for MbIIOH indicate that the 5700-6300-A absorption band is composed of two separate absorption bands which result from a high- and a low-spin form of MbIIIOH. The spin-state-sensitive Raman band at 1608 cm-1 reflects the high-spin species and has an excitation profile maximum at about 6000 A while the low-spin Raman band occurs at 1644 cm-1 and shows an excitation profile maximum at 5800 A. The Fe-O stretch at 490 cm-1 has an excitation profile maximum at about 6000 A. The differences in frequency and Raman cross section between the Fe-X vibrations in MbIIIX and HbIIIX (X = OH-, F-) can be related to increases in the out-of-plane iron distance for the high-spin species of MbIIIX. The shift in the 1644-cm-1 MbIIIOH low-spin state Raman band indicative of the heme core size to 1636 cm-1 in HbIIIOH indicates a larger heme core size in HbIIIOH. Raman frequency shifts are used to estimate differences in bond strain energies between MbIIIX and HbIIIX (X = OH-, F-). Previous resonance Raman excitation profile data can be interpreted in terms of separate contributions from different spin-state species.     

Identification of structural markers for vitamin B12 and other corrinoid derivatives in solution using FTIR spectroscopy

The identification of structural markers for B12/protein interactions is crucial to a complete understanding of vitamin B12 transport and metabolic reaction mechanisms of B12 coenzymes. Fourier transform infrared spectroscopy can provide direct measurements of changes in the side chains and corrin ring resulting from B12/protein interactions. Using FTIR spectroscopy in various solvent systems, we have identified structural markers for corrinoids in the physiological state. We assign the major band (denoted B), which occurs at ca. 1630 cm-1 in D2O and ca. 1675 cm-1 in ethanol, to the amide I C=O stretching mode of the propionamide side chains of the corrin ring. The lower frequency of band B in D2O versus ethanol is due to the greater hydrogen-bonding properties of D2O that stabilize the charged amide resonance form. Since the propionamides are known to be important in protein binding, band B is a suitable marker for monitoring the interaction of these side chains with proteins. We assign bands at ca. 1575 and 1545 cm-1 (denoted C and D) as breathing modes of the corrin ring on the basis of the bands' solvent independence and their sensitivity to changes in axial ligation. As the sigma-donating strength of the axial ligands increases, the frequencies of bands C and D decrease, possibly indicating a lengthening of the corrin conjugated system. Band A, the known cyanide stretching frequency at ca. 2130 cm-1, probes the cobalt-carbon distance in cyanocorrinoids. As the frequency of band A increases, the cobalt-carbon bond strength should decrease.     

On the structures of flavoprotein D-amino acid oxidase purple intermediates. A resonance Raman study

Resonance Raman (RR) spectra were obtained in H2O or D2O solution for the purple intermediates of D-amino acid oxidase (DAO) with isotopically labeled substrates, i.e., [1-13C]-, [2-13C]-, [3-13C]-, [15N]-, and [3,3,3-D3]alanine; [carboxyl-13C]- and [15N]proline. RR spectra were also measured for the intermediates of DAO reconstituted with isotopically labeled FAD's, i.e., [4a-13C]-, [4,10a-13C2]-, [2-13C]-, [5-15N]-, and [1,3-15N2]FAD in D2O. The isotopic shift of the 1692 cm-1 band upon [15N]- or [2-13C]-substitution of alanine indicates that the band is due to the C = N stretching mode of an imino acid derived from D-alanine, i.e., alpha-iminopropionate. The 1658 cm-1 band with D-proline was also assigned to the C = N stretching mode of an imino acid derived from D-proline, i.e., delta 1-pyrrolidine-2-carboxylate, since the band shifts to 1633 cm-1 upon [15N]-substitution and its stretching frequency is generally found in this frequency region. Since the band shifts to low frequency in D2O, the imino acid should have a protonated imino group such as the C = N+1H form. The intense band at 1363 cm-1 with D-alanine was assigned to a mixing of the CO2- symmetric stretching and CH3 symmetric deformation modes in alpha-iminopropionate, based on the isotope effects. The 1359 cm-1 band with D-proline has probably contributions of CO2- symmetric stretching and CH2 wagging, considering the isotope effects with [carboxyl-13C]proline. The 1359 cm-1 band with D-proline was split into 1371 cm-1 and 1334 cm-1 bands in D2O. As this splitting of the 1359 cm-1 band with D-proline in D2O can not be interpreted only by the replacement of the C = N+1-H proton by deuterium, the carboxylate of the imino acid probably interacts with the enzyme through some proton(s) exchangeable by deuterium(s) in D2O. The bands around 1605 cm-1 which shift upon [4a-13C]- and [4,10a-13C2]-labeling of FAD are derived from a fully reduced flavin, because the isotopic shifts of the band are very different from those of the bands of oxidized or semiquinoid flavin observed near 1605 cm-1.(ABSTRACT TRUNCATED AT 400 WORDS)     

Heme pocket interactions in cytochrome c peroxidase studied by site-directed mutagenesis and resonance Raman spectroscopy

Resonance Raman spectra are reported for FeII and FeIII forms of cytochrome c peroxidase (CCP) mutants prepared by site-directed mutagenesis and cloning in Escherichia coli. These include the bacterial "wild type", CCP(MI), and mutations involving groups on the proximal (Asp-235----Asn, Trp-191----Phe) and distal (Trp-51----Phe, Arg-48----Leu and Lys) side of the heme. These spectra are used to assess the spin and ligation states of the heme, via the porphyrin marker band frequencies, especially v3, near 1500 cm-1, and, for the FeII forms, the status of the Fe-proximal histidine bond via its stretching frequency. The FeII-His frequency is elevated to approximately 240 cm-1 in CCP(MI) and in all of the distal mutants, due to hydrogen-bonding interactions between the proximal His-175 N delta and the carboxylate acceptor group on Asp-235. The FeII-His RR band has two components, at 233 and 246 cm-1, which are suggested to arise from populations having H-bonded and deprotonated imidazole; these can be viewed in terms of a double-well potential involving proton transfer coupled to protein conformation. The populations shift with changing pH, possibly reflecting structure changes associated with protonation of key histidine residues, and are influenced by the Leu-48 and Phe-191 mutations. A low-spin FeII form is seen at high pH for the Lys-48, Leu-48, Phe-191, and Phe-51 mutants; for the last three species, coordination of the distal His-52 is suggested by a approximately 200-cm-1 RR band assignable to Fe(imidazole)2 stretching.(ABSTRACT TRUNCATED AT 250 WORDS)     

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.     

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.     

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.     

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.     

Effects of cholesterol analogues and inhibitors on the heme moiety of cytochrome P-450scc: a resonance Raman study

Interactions of cholesterol analogues and inhibitors with the heme moiety of cytochrome P-450scc were examined by resonance Raman spectroscopy. The Raman spectra of ferric cytochrome P-450scc complexed with inhibitors such as cyanide, phenyl isocyanide, aminoglutethimide, and metyrapone were characteristic of low-spin state and were very similar. However, the effect of exchange of the sixth ligand from the oxygen atom (ferric low-spin state) to the nitrogen atom upon aminoglutethimide and metyrapone binding was seen as down-frequency shifts of the v3 band from 1503 to 1501 and 1502 cm-1, respectively, while cyanide and phenyl isocyanide binding caused an up-frequency shift of the v3 band to 1505 cm-1. The effects of cholesterol analogues [22(R)-hydroxycholesterol, 22(S)-hydroxycholesterol, 22-ketocholesterol, 20(S)-hydroxycholesterol, and 25-hydroxycholesterol] on a Fe2+-CO stretching frequency of cytochrome P-450scc in ferrous CO form were examined. The 22(R)-hydroxycholesterol complex could not give a clear Fe2+-CO stretching Raman band due to a strong photodissociability. 22(S)-Hydroxycholesterol and 25-hydroxycholesterol complexes gave the Raman bands at 487 and 483 cm-1, respectively, whereas 20(S)-hydroxycholesterol and 22-ketocholesterol complexes gave Fe2+-CO stretching frequencies (478 cm-1) almost identical with that without substrate (477 cm-1). These findings suggest the existence of the following physiologically important natures of the cytochrome P-450scc active site: (1) there is a strong steric interaction between heme-bound carbon monoxide and the 22(R)-hydroxyl group or the 22(R)-hydrogen of the steroid side chain and (2) the hydroxylation at the 20S position may cause a conformational change of the side-chain group relative to the heme.     

Rhodopsin-lumirhodopsin phototransition of bovine rhodopsin investigated by Fourier transform infrared difference spectroscopy

The rhodopsin-lumirhodopsin transition has been investigated by Fourier transform infrared difference spectroscopy using isotope-labeled retinals. In the transition, two protonated carboxyl groups are involved. Another carbonyl band, located at 1725 cm-1 in rhodopsin, is shifted to 1731.5 cm-1 in lumirhodopsin. This line is tentatively assigned to a carbonyl stretching vibration of a peptide bond adjacent to the nitrogen of a proline residue. The C=N stretching vibration of rhodopsin could unequivocally be assigned to a band at 1659 cm-1. In contrast to rhodopsin and bathorhodopsin, the C=N stretching vibration of lumirhodopsin is at a low position, i.e., at 1635 cm-1, and exhibits only a downshift of 4 cm-1 upon deuteriation of the nitrogen. The C15-H rocking vibration of rhodopsin is assigned to the unusual high position of 1456 cm-1 and shifts into the normal region upon formation of lumirhodopsin. From these results, it is concluded that, whereas the environment of the Schiff base in rhodopsin, bathorhodopsin, and isorhodopsin is approximately the same, large changes occur with the formation of lumirhodopsin. From the assignment of the C10-C11 stretching vibration in bathorhodopsin and lumirhodopsin, a 10-s-cis geometry of lumirhodopsin can be excluded.     

The cobalt-nitrosyl stretching vibration as a sensitive resonance Raman probe for distal histidine-nitrosyl interaction in monomeric hemoglobins

The Co-NO stretching vibration has been assigned in the resonance Raman spectra of various cobalt-substituted monomeric hemoglobins by employing isotope-labeling of nitrosyl (14N16O, 15N16O, 14N18O). Monomeric hemoglobins with a distal histidine (sperm whale myoglobin and leghemoglobin) exhibit this vibration at 573-575 cm-1, whereas hemoglobins without distal histidine (elephant myoglobin and insect hemoglobin from Chironomus thummi thummi, CTT III) show this vibration in the range of 553-558 cm-1. The Fe-NO stretching vibration which occurs in the range of 554-556 cm-1 does not reflect the distal histidine-ligand interaction. Therefore, the Co-NO moiety which is isoelectronic with the Fe-O2 moiety is a good monitor for distal effects on the exogenous ligand of hemoglobins, especially due to the fact that in hemoglobins with distal histidine the Fe-O2 stretching vibration (567-572 cm-1) is similar to the Co-NO stretching vibration.