Protein conformational relaxation following photodissociation of CO from carbonmonoxymyoglobin: picosecond circular dichroism and absorption studies

Picosecond time-resolved polarization spectroscopy is used to study relaxation dynamics in myoglobin following photoelimination of CO from carbonmonoxymyoglobin. Evolution of the transient circular dichroism signal of the N band of myoglobin (probed at 355 nm) to that characteristic of equilibrium myoglobin requires approximately 300 ps. This time scale is significantly longer than that corresponding to the photoinitiated bond cleavage. Transient linear dichroism of the Soret band and picosecond time-resolved magnetic circular dichroism measurements of the Q band demonstrate that the circular dichroism kinetics do not result from either time-dependent changes in the orientation of the transition moments of the heme ring or the doming of the heme that accompanies the out-of-plane motion of the iron. Finally, transient absorption data of the near-IR optical transition of photogenerated myoglobin suggest that the circular dichroism data are not a measure of the tilting of the proximal histidine. The circular dichroism data are discussed in terms of a relaxation in the tertiary structure of the protein following dissociation.     

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.     

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.     

Investigations of optical line shapes and kinetic hole burning in myoglobin.

We present the results of an extensive investigation of the optical line shapes of deoxymyoglobin (Mb), the ligand-bound form (MbCO), and the low-temperature photoproduct (Mb*). The thermal properties and the pH dependence of the Soret band and the near infrared band III (approximately 760 nm) are analyzed, taking into account the underlying vibrational properties of the absorption bands. The strong temperature dependence associated with the Soret band of MbCO and band III of Mb indicates significant coupling to low-frequency modes that may not be directly observed in the resonance Raman spectra. On the basis of analogous line-shape studies in a variety of heme systems, we assign the low-frequency coupling in MbCO to torsional motions of the CO molecule. The low-frequency mode coupled to band III (approximately 70 cm-1) is found to lie quite close to the value for the heme-doming motion (approximately 50 cm-1) calculated by using the kinetically determined value of the force constant (17 N/m). Significant inhomogeneous broadening in the Soret region of Mb and Mb* is found to be due to a "nonkinetic" coordinate that we associate with the orientation of the proximal histidine. A "kinetic" coordinate, associated with the equilibrium displacement of the iron atom from the porphyrin plane (a) is found to contribute to the inhomogeneous broadening of both the Soret band and band III. The relaxation of the heme as the system evolves from from Mb* to Mb is followed optically as a function of temperature, and a sharp transition temperature is found at 185 K. The blue shifts of the Soret band and band III as Mb* evolves to Mb are found to be nearly identical (delta v*ABS approximately 140 cm-1) and attributed to changes in the mean value of a between Mb* (a*0) and Mb (a0 = 0.45 A). A simple quadratic model for the coordinate coupling that simultaneously accounts for the observed shift, delta v*ABS, the low-temperature kinetics and the kinetic hole burning predicts a*0 = 0.2 +/- 0.05 A and EA = 16 +/- 2 kJ/mol for the room temperature Arrhenius barrier height at the heme. A simple quantitative method for the analysis of kinetic hole-burning experiments is also developed and applied to recent studies involving quaternary and subunit-specific hemoglobin structures.     

Resonance Raman investigations of chloroperoxidase, horseradish peroxidase, and cytochrome c using Soret band laser excitation.

Resonance Raman spectra of the heme protein chloroperoxidase in its native and reduced forms and complexed with various small ions are obtained by using laser excitation in the Soret region (350-450 nm). Additionally, Raman spectra of horseradish peroxidase, cytochrome P-450cam, and cytochrome c, taken with Soret excitation, are presented and discussed. The data support previous findings that indicate a strong analogy between the active site environments of chloroperoxidase and cytochrome P-450cam. The Raman spectra of native chloroperoxidase are found to be sensitive to temperature and imply that a high leads to low spin transition of the heme iron atom takes place as the temperature is lowered. Unusual peak positions are also found for native and reduced chloroperoxidase and indicate a weakening of porphyrin ring bond strengths due to the presence of a strongly electron-donating axial ligand. Enormous selective enhancements of vibrational modes at 1360 and 674 cm-1 are also observed in some low-spin ferrous forms of the enzyme. These vibrational frequencies are assigned to primary normal modes of expansion of the prophyrin macrocycle upon electronic excitation.     

Picosecond study of the near infrared absorption band of hemoglobin after photolysis of carbonmonoxyhemoglobin.

Picosecond absorption spectroscopy is used to examine the position and band shape of the near infrared absorption band of hemoglobin as a function of time after the photodissociation of CO from carbonmonoxyhemoglobin. For the earliest delay time probed, 35 ps, the peak of the transient spectrum is at 765 nm, red shifted by 6 nm from that characteristic of equilibrium deoxyhemoglobin. No evolution in either the peak position or band shape is observed for time delays up to 60 ns. In addition, the position and shape of the spectrum are independent of photolysis energies ranging from 15 microJ/pulse to 150 microJ/pulse, spanning conditions under which the photon/heme ratio is varied from 0.01 to 2.0. This indicates that the geometry in the heme group is unrelaxed and that equilibration of the surrounding protein structure occurs on a time scale longer than 60 ns.     

An ultrafast time-resolved anisotropy study of bacteriochlorophyll a in pyridine

The transient absorption anisotropy spectrum of bacteriochlorophyll a (BChl a) in pyridine was measured in the wavelength interval 550-850 nm, 1 ps after optical excitation with a 792-nm femtosecond light pulse. In the wavelength region of Q(y) absorption and stimulated emission (775-825 nm), the anisotropy was found to be close to the theoretically expected value (0.4) for a two-level system. In the wavelength region 650-750 nm, where the transient absorption signal is dominated by excited state absorption, the anisotropy is reduced to approximately 0.18. Anisotropy kinetics were measured at several wavelengths and found to be constant within the time window 0-5 ps, showing that no internal dynamics of the BChl a molecule change the anisotropy on the time scale of tens of picoseconds.     

FT-Infrared spectroscopic studies of the iron ligand CO stretch mode of iNOS oxygenase domain: effect of arginine and tetrahydrobiopterin

The iron ligand CO stretch vibration mode of the inducible nitric oxide synthase oxygenase domain (iNOSox) has been studied from 20 to 298 K. iNOSox in the absence of arginine reveals a temperature-dependent equilibrium of two major conformational substates with CO stretch bands centered at about 1945 and 1954 cm(-)(1). This behavior is not qualitatively changed when tetrahydrobiopterin (H(4)B) is bound. Arginine binding changes significantly the spectrum by formation of a sharp CO stretch mode band at about 1905 cm(-)(1) and indicates the formation of a hydrogen bond to the CO ligand. For temperatures lower than 250 K, the stretch vibration frequency decreases almost linearly with decreasing temperature and indicates that the coupling between the CO ligand and the arginine/protein in the active site via the hydrogen bond is very strong. Flashphotolysis of the CO ligand carried out at 25 K revealed the CO stretch mode of the photodissociated CO ligand trapped in the heme pocket. There is a negative linear relation between the stretch vibration frequencies of the photodissociated and the iron-bound CO indicating that the photodissociated ligand stays near the heme.     

Folding character of cytochrome c studied by o-nitrobenzyl modification of methionine 65 and subsequent ultraviolet light irradiation

The protein folding character of cyt c was studied with the use of a photocleavable o-nitrobenzyl derivative of Met65 (NBz-Met65). For the NBz-Met65 cyt c, the Soret absorption band slightly blue shifted compared with the unlabeled cyt c, the 695 nm absorption band related to the Met80 sulfur ligation to the heme iron disappeared, and its resonance Raman spectrum was characteristic of a six-coordinate low-spin species, all characters demonstrating coordination of a non-native ligand, probably a histidine, instead of Met80 to the heme iron. The far-UV circular dichroism (CD) spectrum of cyt c was altered, and the transition midpoint concentration value of guanidine hydrochloride (GdnHCl) for unfolding the protein decreased by 0.9 M by the modification, which showed perturbation of the structure and decrease in protein stability, respectively. With irradiation of 308 nm laser pulses on the NBz-Met65 cyt c, the Soret absorption band slightly red shifted, the 695 nm absorption band appeared, and the CD spectrum shifted toward that of the native protein, which demonstrated recovery of the methionine heme coordination and the native protein structure, due to reconversion of NBz-Met65 to unlabeled methionine. A fast phase was detected as a change in Soret absorbance with a rate constant of 21 000 +/- 4000 s(-)(1) during refolding of cyt c initiated by irradiation of a 308 nm pulse on the NBz-Met65 cyt c in the presence of 2 M GdnHCl. The observed rate constant corresponded well with that reported by the tryptophan fluorescence study [Shastry, M. C. R. S., and Roder, H. (1998) Nat. Struct. Biol. 5, 385-392]. The intermediate decayed with a rate constant of 90 +/- 15, followed by another phase with a rate constant of 13 +/- 3 s(-)(1), and was not seen in the absence of GdnHCl.     

Stimulation of bull seminal Ca2+, Mg2+-dependent endonuclease by various DNA-binding proteins

We have measured ΔA transient absorption spectra in the Soret region and kinetics of photodissociation of oxymyoglobin (MbO₂) solutions following excitation by pulses of duration 350 fsec and 10 μJ energy at 307 nm. We observed an instantaneous bleaching of the absorbance at 414 nm and the appearance of a broad, red-shifted absorption band in the 438–470 nm region with a time constant of 250 fsec indicative of the formation of a short-lived deliganded Mb^★ species which relaxes to the stable Mb with a constant of 3.5 psec. Following this early relaxation, changes in absorption kinetics indicate also a geminate recombination process of constant τ = 100 psec. These data demonstrate that the well established low quantum yield (φ = 0.03) of photodissociation in MbO₂ is related both to the relaxation of an excited Mb^★ state and to a fast geminate recombination process.     

Reconstitution of myoglobin from apoprotein and heme, monitored by stopped-flow absorption, fluorescence and circular dichroism

The reconstitution reaction of ferric cyanomyoglobin from apomyoglobin and hemin dicyanide was investigated with a stopped-flow apparatus by the use of five kinds of probes; (a) Soret absorption, (b) fluorescence quenching of tryptophan, (c) far-ultraviolet CD, (d) near-ultraviolet CD, and (e) Soret CD. After mixing of apomyoglobulin with equimolar amounts of hemin dicyanide, the Soret absorption band was shifted to longer wavelengths within 10 ms. The shifted band kept its shape for a few seconds, and then gradually shifted to shorter wavelengths. A rate constant of the slow reaction was 1.1 x 10(-2) s-1. Time courses of fluorescence quenching followed a second-order reaction with a rate constant of 9 x 10(7) M-1 s-1. Far-ultraviolet CD recovered to the level of native state within the response time of an apparatus (= 64 ms). Near-ultraviolet CD and Soret CD changed with first-order rate constants of 5-30 s-1 and 5 x 10(-3) s-1 respectively. On the basis of the kinetic results we propose the following reconstitution pathway of myoglobin. Apomyoglobin has essentially a highly folded structure similar to myoglobin, but there are some differences in the secondary structure between them. In the first step, heme enters the pocket-like site of apomyoglobin and interacts with surrounding hydrophobic residues in the pocket, and then the interaction may give a complete ordered structure to the protein. Second, the tertiary structure of the heme pocket is partly constructed. Third, the iron-proximal His bond occurs, followed by the attainment of the final conformation. This sequence of the events shows that the polypeptide chain is entirely folded before the completion of three-dimensional structure of the heme pocket. The reconstitution pathway is fairly different from that of the alpha subunit of hemoglobin reported by Leutzinger and Beychok [Proc. Natl Acad. Sci. USA (1981) 78, 780-784], which described how a drastic recovery in helicity was observed on the heme-binding, and that the recovery is introduced by the formation of the heme pocket structure. The difference in the results found for the alpha subunit and myoglobin suggests a difference in conformation: in apomyoglobin most of the helices are arranged and folded around a helix core to form a compact structure as a whole, while in apo-alpha subunit some helices are not folded around the helix core. Helix D, which is absent in the alpha subunit, may play an important role in folding of the helices.     

Resonance Raman investigation of the effects of copper binding to iron-mesoporphyrin.histidine-rich glycoprotein complexes.

Histidine-rich glycoprotein (HRG) binds both hemes and metal ions simultaneously with evidence for interaction between the two. This study uses resonance Raman and optical absorption spectroscopies to examine the heme environment of the 1:1 iron-mesoporphyrin.HRG complex in its oxidized, reduced and CO-bound forms in the absence and presence of copper. Significant perturbation of Fe(3+)-mesoporphyrin.HRG is induced by Cu2+ binding to the protein. Specifically, high frequency heme resonance Raman bands indicative of low-spin, six-coordinate iron before Cu2+ binding exhibit monotonic intensity shifts to bands representing high-spin, five-coordinate iron. The latter coordination is in contrast to that found in hemoglobin and myoglobin, and explains the Cu(2+)-induced decrease and broadening of the Fe(3+)-mesoporphyrin.HRG Soret band concomitant with the increase in the high-spin marker band at 620 nm. After dithionite reduction, the Fe(2+)-mesoporphyrin.HRG complex displays high frequency resonance Raman bands characteristic of low-spin heme and no iron-histidine stretch, which together suggest six-coordinate iron. Furthermore, the local heme environment of the complex is not altered by the binding of Cu1+. CO-bound Fe(2+)-mesoporphyrin.HRG exhibits bands in the high and low frequency regions similar to those of other CO-bound heme proteins except that the iron-CO stretch at 505 cm-1 is unusually broad with delta nu approximately 30 cm-1. The dynamics of CO photolysis and rebinding to Fe(2+)-mesoporphyrin.HRG are also distinctive. The net quantum yield for photolysis at 10 ns is low relative to most heme proteins, which may be attributed to very rapid geminate recombination. A similar low net quantum yield and broad iron-CO stretch have so far only been observed in a dimeric cytochrome c' from Chromatium vinosum. Furthermore, the photolytic transient of Fe(2+)-mesoporphyrin.HRG lacks bands corresponding to high-spin, five-coordinate iron as is found in hemoglobin and myoglobin under similar experimental conditions, suggesting iron hexacoordination before CO recombination. These data are consistent with a closely packed distal heme pocket that hinders ligand diffusion into the surrounding solvent.     

Correct interpretation of heme protein spectra allows distinguishing between the heme and the protein dynamics

It is shown by using the vibronic approach that the iron displacement out of the porphyrin plane in deoxyheme proteins intermixes the porphyrin pi and axial iron-histidine sigma electronic subsystems. This intermixing explains the substantial coupling of the iron-histidine vibration to the heme Soret excitation, the appearance of the iron-histidine band in the corresponding resonance Raman spectra, and a number of other experimental data, including the dependence of the iron-histidine vibrational frequency on the extent of the iron displacement out of the porphyrin plane. This dependence implies that there is an anharmonic coupling between the corresponding vibrations, which is shown to be the cause of the specific temperature dependence of the iron-histidine band. The anharmonic coupling and the dependence of the dipole transition moment of the charge transfer optical absorption band III on the iron-porphyrin distance cause the anomalous temperature and pressure dependencies of this band. It is shown that the change in both the magnitude and the distribution of the iron-porphyrin distance is expected to affect the band III intensity. Consequently, the stationarity of the band III intensity can be considered as a signature of the stationarity of the iron-porphyrin distance and its distribution in deoxyheme proteins, whereas the band III position and width could be also affected by the change in the protein electric field, caused by the protein globule dynamics.     

Sequential photoisomerisation dynamics of the push-pull azobenzene Disperse Red 1

The ultrafast dynamics of the push-pull azobenzene Disperse Red 1 following photoexcitation at λ(pump) = 475 nm in solution in 2-fluorotoluene have been probed by broadband transient absorption spectroscopy and fluorescence up-conversion spectroscopy. The measured two-dimensional spectro-temporal absorption map features a remarkable "fast" excited-state absorption (ESA) band at λ ≈ 570 nm appearing directly with the excitation laser pulse and showing a sub-100 fs lifetime with a rapid spectral blue-shift. Moreover, its ultrafast decay is paralleled by rising distinctive ESA at other wavelengths. Global fits to the absorption-time profiles using a consecutive kinetic model yielded three time constants, τ(1) = 0.08 ± 0.03 ps, τ(2) = 0.99 ± 0.02 ps, and τ(3) = 6.0 ± 0.1 ps. Fluorescence-time profiles were biexponential with time constants τ(1)' = 0.12 ± 0.06 ps and τ(2)' = 0.70 ± 0.10 ps, close to the absorption results. Based on the temporal evolution of the transient spectra, especially the "fast" excited-state absorption band at λ ≈ 570 nm, and on the global kinetic analysis of the time profiles, τ(1) is assigned to an ultrafast transformation of the optically excited ππ* state to an intermediate state, which may be the nπ* state, τ(2) to the subsequent isomerisation and radiationless deactivation time to the S(0) electronic ground state, and τ(3) to the eventual vibrational cooling of the internally "hot" S(0) molecules.     

Role of distal arginine in early sensing intermediates in the heme domain of the oxygen sensor FixL

FixL is a bacterial heme-based oxygen sensor, in which release of oxygen from the sensing PAS domain leads to activation of an associated kinase domain. Static structural studies have suggested an important role of the conserved residue arginine 220 in signal transmission at the level of the heme domain. To assess the role of this residue in the dynamics and properties of the initial intermediates in ligand release, we have investigated the effects of R220X (X = I, Q, E, H, or A) mutations in the FixLH heme domain on the dynamics and spectral properties of the heme upon photolysis of O(2), NO, and CO using femtosecond transient absorption spectroscopy. Comparison of transient spectra for CO and NO dissociation with steady-state spectra indicated less strain on the heme in the ligand dissociation species for all mutants compared to the wild type (WT). For CO and NO, the kinetics were similar to those of the wild type, with the exception of (1) a relatively low yield of picosecond NO rebinding to R220A, presumably related to the increase in the free volume of the heme pocket, and (2) substantial pH-dependent picosecond to nanosecond rebinding of CO to R220H, related to formation of a hydrogen bond between CO and histidine 220. Upon excitation of the complex bound with the physiological sensor ligand O(2), a 5-8 ps decay phase and a nondecaying (>4 ns) phase were observed for WT and all mutants. The strong distortion of the spectrum associated with the decay phase in WT is substantially diminished in all mutant proteins, indicating an R220-induced role of the heme in the primary intermediate in signal transmission. Furthermore, the yield of dissociated oxygen after this phase ( approximately 10% in WT) is increased in all mutants, up to almost unity in R220A, indicating a key role of R220 in caging the oxygen near the heme through hydrogen bonding. Molecular dynamics simulations corroborate these findings and suggest motions of O(2) and arginine 220 away from the heme pocket as a second step in the signal pathway on the 50 ps time scale.     

Interaction of bd-type quinol oxidase from Escherichia coli and carbon monoxide: Heme d binds CO with high affinity

Comparative studies on the interaction of the membrane-bound and detergent-solubilized forms of the enzyme in the fully reduced state with carbon monoxide at room temperature have been carried out. CO brings about a bathochromic shift of the heme d band with a maximum at 644 nm and a minimum at 624 nm, and a peak at 540 nm. In the Soret band, CO binding to cytochrome bd results in absorption decrease and minima at 430 and 445 nm. Absorption perturbations in the Soret band and at 540 nm occur in parallel with the changes at 630 nm and reach saturation at 3-5 microM CO. The peak at 540 nm is probably either beta-band of the heme d-CO complex or part of its split alpha-band. In both forms of cytochrome bd, CO reacts predominantly with heme d. Addition of high CO concentrations to the solubilized cytochrome bd results in additional spectral changes in the gamma-band attributable to the reaction of the ligand with 10-15% of low-spin heme b558. High-spin heme b595 does not bind CO even at high concentrations of the ligand. The apparent dissociation constant values for the heme d-CO complex of the membrane-bound and detergent-solubilized forms of the fully reduced enzyme are about 70 and 80 nM, respectively.     

Probing protein-cofactor interactions in the terminal oxidases by second derivative spectroscopy: study of bacterial enzymes with cofactor substitutions and heme A model compounds.

Second derivative absorption spectra are reported for the aa3-cytochrome c oxidase from bovine cardiac mitochondria, the aa3-600 ubiquinol oxidase from Bacillus subtilis, the ba3-cytochrome c oxidase from Thermus thermophilis, and the aco-cytochrome c oxidase from Bacillus YN-2000. Together these enzymes provide a range of cofactor combinations that allow us to unequivocally identify the origin of the 450-nm absorption band of the terminal oxidases as the 6-coordinate low-spin heme, cytochrome a. The spectrum of the aco-cytochrome c oxidase further establishes that the split Soret band of cytochrome a, with features at 443 and 450 nm, is common to all forms of the enzyme containing ferrocytochrome a and does not depend on ligand occupancy at the other heme cofactor as previously suggested. To test the universality of this Soret band splitting for 6-coordinate low-spin heme A systems, we have reconstituted purified heme A with the apo forms of the heme binding proteins, hemopexin, histidine-proline-rich glycoprotein and the H64V/V68H double mutant of human myoglobin. All 3 proteins bound the heme A as a (bis)histidine complex, as judged by optical and resonance Raman spectroscopy. In the ferroheme A forms, none of these proteins displayed evidence of Soret band splitting. Heme A-(bis)imidazole in aqueous detergent solution likewise failed to display Soret band splitting. When the cyanide-inhibited mixed-valence form of the bovine enzyme was partially denatured by chemical or thermal means, the split Soret transition of cytochrome a collapsed into a single band at 443 nm.(ABSTRACT TRUNCATED AT 250 WORDS)     

Compressibility and uncoupling of cytochrome P450cam: high pressure FTIR and activity studies

The effect of the hydrostatic pressure on the CO ligand stretch vibration in cytochrome P450cam-CO bound with various substrates is studied by FTIR. The vibration frequency is linearily shifted to lower values with increasing pressure. The slope of the shift gives the isothermal compressibility of the heme pocket and is found to be related to the high-spin state content in an opposite direction to that previously observed from the pressure-induced shift of the Soret band. This opposite behaviour is explained by the dual effect of heme pocket water molecules both on the CO ligand and on electrostatic potentials produced by the protein at the distal side. The latter effect disturbs ligand-distal side contacts which are needed for a specific proton transfer in oxygen activation when dioxygen is the ligand. Their loss results in uncoupled H(2)O(2) formation.     

Carboxy Mb at pH 3. Time-resolved resonance Raman study at cryogenic temperatures.

Cryogenic samples of MbCO at pH3 are studied using nanosecond and picosecond time-resolved resonance Raman spectroscopy. It is observed that under excitation conditions sufficient to completely photodissociate MbCO at pH7, the pH3 sample at 10 ns remains substantially unphotolyzed even at 15 K. The similarity in the optical and resonance Raman spectra of MbCO at pH3 with that of pH7 indicates that at pH3 the iron remains six-coordinate and low-spin. The Fe-CO stretch frequency is consistent with a more upright CO orientation. The absence of the v(Fe-His) band in the 30 ps photoproduct Raman spectrum suggests that the Fe-His(F8) bond is broken within 30 ps of photodissociation. Other Raman bands, though, are not consistent with a normal four-coordinate heme for the photoproduct, Mb*. Suggested possible interpretations include a four-coordinate heme highly perturbed by the close lying protonated proximal histidine or a five-coordinate heme with the Fe-His bond significantly weakened. The partial photolysis monitored at 30 ps and 100 K indicates either a significant amount of geminate recombination within 30 ps or low quantum yield or photolysis. The time course for CO recombination is monitored via the Raman spectra from 30 ps to 3 ns at 100 K and 160 K. Of the fraction of protein-ligand pairs that remain photodissociated at 30 ps, 50% recombine by approximately 250 ps at 100 K and 160 K, supporting the flash photolysis rebinding data of Cowen et al. (Cowen, B. R. 1990. Ph. D. thesis. University of Illinois at Urbana-Champaign; Cowen, B. R., D. Braunstein, H. Frauenfelder, P. J. Steinbach, and R. D. Young. 1989. Biophys. J. 55:55a. [Abstr.].) The conclusions from these resonance Raman studies are extended to solution phase studies at ambient temperatures.