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The heme-pocket dynamics subsequent to carbon monoxide photolysis from human hemoglobin have been monitored as a function of glycerol-water solvent composition with time-resolved resonance Raman spectroscopy. Prompt (geminate) ligand recombination rates and the transient heme-pocket geometry established within 10 ns after photolysis appear to be largely independent of solvent composition. The rate of relaxation of the transient geometry to an equilibrium deoxy configuration is, however, quite sensitive to solvent composition. These observations suggest that the former processes result from local, internal motions of the protein, while the relaxation dynamics of the proximal heme pocket are predicated upon more global protein motions that are dependent upon solvent viscosity.

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The structure, ligand binding kinetics, and thermodynamics of hemoglobin have been the subject of a great deal of investigation. However, the exact pathway(s) by which cooperative energetics are communicated within the protein remain undefined. The effects of interspecies variations in quaternary and tertiary structure, oxygen affinity, cooperativity, and ligand binding kinetics upon the overall ligand binding process are, therefore, of great importance in understanding and solving these problems. The demonstrated sensitivity of resonance Raman spectroscopy to heme structure and environment make it an ideal probe of ligand binding dynamics. It is possible to examine how specific vibrational modes change with time and correlate this with solution conditions and protein structural and conformational differences. Those modes which exhibit the greatest change with ligand photolysis are also indicative of possible paths of cooperative energy dissipation within the protein. The changes which occur in the vibrational modes of the heme within 10 ns of CO photolysis have been determined for a wide variety of mammalian and reptilian hemoglobins. The modes most affected by this process are, without exception, nu(Fe-His), nu4, and the substituent bending modes, delta(cb - s) and delta(cb - c alpha - c beta). Furthermore, a direct correlation exists between the shift in porphyrin pi electron density upon CO photolysis (as indicated by the transient changes in nu 4) and the Hill coefficient of cooperativity. The implications of those results concerning ligand binding cooperativity in hemoglobins are discussed.

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Resonance Raman and electron paramagnetic resonance spectroscopy have been utilized to identify histidine as an axial heme ligand in a high spin, heme c-containing protein isolated from the photosynthetic purple sulfur bacterium Chromatium vinosum. Resonance Raman spectroscopy has also been used to characterize the CO adduct of the C. vinosum hemoprotein. Resonance Raman spectra of the heme site obtained within 10 ns of CO photolysis from the ferrous hemoprotein are virtually identical to those of the unligated protein, indicating that there is little or no rearrangement of the heme pocket in response to ligand photolysis. The equilibrium constant for CO binding to the ferrous hemeprotein was measured to be 1.7 X 10(-5) M-1 and the CO association rate constant determined to be 5.4 X 10(3) M-1 S-1. The quantum efficiency for photodissociation of the hemoprotein X CO complex was greater than or equal to 0.9.

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The effects of protein dehydration upon the equilibrium and dynamic properties of the heme active site in human hemoglobin (HbA) have been probed by resonance Raman scattering. Spectra of equilibrium carbonmonoxy-HbA and the photolytic heme transient species generated within 10 ns of ligand photolysis have been obtained from thin films of protein in various stages of dehydration. These data provide detailed information concerning the response of the heme and its bonding interactions with both the proximal histidine and carbon monoxide as a function of protein hydration. For protein hydration levels of 0.4-1.0 g of H2O/g of protein, our results indicate that the C = O stretching mode of carbonmonoxy-HbA is dramatically affected by protein hydration levels, thus corroborating the infrared results of Brown et al. [Brown, W. E., Sutcliffe, J. W., & Pulsinelli, P. D. (1983) Biochemistry 22, 2914-2923]. However, we find that both heme skeletal modes and the Fe-C bond strength are largely insensitive to dehydration. Moreover, the proximal pocket geometry (as reflected in the behavior of the Fe-proximal histidine stretching mode) immediately following ligand photolysis was found to be very similar to that of R-state solution hemoglobin. At protein hydration levels below the theoretical monolayer limit, small changes in the resonance Raman spectra of both equilibrium HbCO and the transient heme species generated subsequent to ligand photolysis are detected. These include broadening of the Fe-C stretching mode in equilibrium HbCO and a small shift to lower frequency of the Fe-His mode in the photolytic transient species.(ABSTRACT TRUNCATED AT 250 WORDS)

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Picosecond time-resolved Raman spectra of hemoglobin generated with blue pulses (20 to 30 picoseconds) that were resonant with the Soret band and of sufficient intensity to completely photodissociate the starting liganded sample are reported. For both R- and T-state liganded hemoglobins, the peak frequencies in the spectrum of the deoxy transient were the same at approximately 25 picoseconds as those observed at 10 nanoseconds subsequent to photodissociation. In particular, the large R-T differences in the frequency of the stretching mode for the iron-proximal histidine bond (VFe-His) detected in previously reported nanosecond-resolved spectra were also evident in the picosecond-resolved spectra. The implications of this finding with respect to the distribution of strain energy in the liganded protein and the origin of the time course for geminate recombination are discussed. On the basis of these results, a microscopic model is proposed in which delocalization of strain energy is strongly coupled to the coordinate of the iron. The model is used to explain the origin of the R-T differences in the rates of ligand dissociation.

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The picosecond geminate rebinding of molecular oxygen was monitored in a variety of different human, reptilian, and fish hemoglobins. The fast (100 to 200 picoseconds) component of the rebinding is highly sensitive to protein structure. Both proximal and distal perturbations of the heme affect this rebinding process. The rebinding yield for the fast process correlates with the frequency of the stretching motion of the iron-proximal histidine mode (VFe-His) observed in the transient Raman spectra of photodissociated ligated hemoglobins. The high-affinity R-state species exhibit the highest values for VFe-His and the highest yields for fast rebinding, whereas low affinity R-state species and T-state species exhibit lower values of VFe-His and correspondingly reduced yields for this geminate process. These findings link protein control of ligand binding with events at the heme.

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Resonance Raman spectroscopy was employed to characterize the local heme environment of a high-spin, ligand-binding heme protein from Chromatium vinosum (Chromatium high-spin hemoprotein). High-frequency spectra obtained with both B- and Q-band excitation were found to resemble qualitatively those of deoxyhemoglobin (HbA). Differences between HbA and Chromatium high-spin hemoprotein spectra can be assigned to either the effects of a covalent linkage of the heme vinyls to the protein matrix or alterations in the heme-proximal ligand bonding interaction. Both kinematic and electronic effects were evident. The behavior of heme core-size sensitive modes and low-frequency modes in Chromatium high-spin hemoprotein may be an indication of distortions in the heme geometry of Chromatium high-spin hemoprotein relative to HbA. The effects of covalent bonding of the heme peripheral vinyls upon the vibrational, electronic, and geometric characteristics of the heme active site in Chromatium high-spin hemoprotein are discussed.

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Resonance Raman spectra with both Soret and visible excitation have been obtained for Chromatium flavocytochrome c552 and its isolated diheme subunit under varying conditions of pH and inhibitor binding. The spectra are generally consistent with previously established classification schemes for porphyrin ring vibrations. The presence of covalently bound flavin in the protein was apparent in the fluorescent background it produced and in flavin-mediated photoeffects observed in heme Raman spectra obtained at high laser power. No flavin modes were present in the Raman spectra, nor was any evidence of direct heme-flavin interaction found by using this technique; however, a systematic perturbation of heme B1g vibrational frequencies was found in the oxidized holoprotein. The heme vibrational frequencies of c552 are compared to those of the diheme peptide and of other c-type cytochromes. They are consistent with an interpretation that involves pH-dependent changes in axial ligation and treats the hemes and flavin as isolated chromphores communicating via protein-mediated interactions.

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