The Fe(2+)-His(F8) Raman band shape of deoxymyoglobin reveals taxonomic conformational substates of the proximal linkage

NRVS and DFT of MitoNEET: Understanding the Special Vibrational Structure of a [2Fe-2S] Cluster with (Cys)3(His)1 Ligation

The human mitochondrial protein, mitoNEET (mNT), belongs to the family of small [2Fe-2S] NEET proteins that bind their iron-sulfur clusters with a novel and characteristic 3Cys:1His coordination motif. mNT has been implicated in the regulation of lipid and glucose metabolisms, iron/reactive oxygen species homeostasis, cancer, and possibly Parkinson's disease. The geometric structure of mNT as a function of redox state and pH is critical for its function. In this study, we combine ⁵⁷Fe nuclear resonance vibrational spectroscopy with density functional theory calculations to understand the novel properties of this important protein.

Vibrational coherence spectroscopy of the heme domain in the CO-sensing transcriptional activator CooA

Femtosecond vibrational coherence spectroscopy was used to investigate the low-frequency vibrational dynamics of the heme in the carbon monoxide oxidation activator protein (CooA) from the thermophilic anaerobic bacterium Carboxydothermus hydrogenoformans (Ch-CooA). Low frequency vibrational modes are important because they are excited by the ambient thermal bath (k(B)T = 200 cm(-1)) and participate in thermally activated barrier crossing events. However, such modes are nearly impossible to detect in the aqueous phase using traditional spectroscopic methods. Here, we present the low frequency coherence spectra of the ferric, ferrous, and CO-bound forms of Ch-CooA in order to compare the protein-induced heme distortions in its active and inactive states. Distortions take place predominantly along the coordinates of low-frequency modes because of their weak force constants, and such distortions are reflected in the intensity of the vibrational coherence signals. A strong mode near ~90 cm(-1) in the ferrous form of Ch-CooA is suggested to contain a large component of heme ruffling, consistent with the imidazole-bound ferrous heme crystal structure, which shows a significant protein-induced heme distortion along this coordinate. A mode observed at ~228 cm(-1) in the six-coordinate ferrous state is proposed to be the ν(Fe-His) stretching vibration. The observation of the Fe-His mode indicates that photolysis of the N-terminal α-amino axial ligand takes place. This is followed by a rapid (~8.5 ps) transient absorption recovery, analogous to methionine rebinding in photolyzed ferrous cytochrome c. We have also studied CO photolysis in CooA, which revealed very strong photoproduct state coherent oscillations. The observation of heme-CO photoproduct oscillations is unusual because most other heme systems have CO rebinding kinetics that are too slow to make the measurement possible. The low frequency coherence spectrum of the CO-bound form of Ch-CooA shows a strong vibration at ~230 cm(-1) that is broadened and up-shifted compared to the ν(Fe-His) of Rr-CooA (216 cm(-1)). We propose that the stronger Fe-His bond is related to the enhanced thermal stability of Ch-CooA and that there is a smaller (time dependent) tilt of the histidine ring with respect to the heme plane in Ch-CooA. The appearance of strong modes at ~48 cm(-1) in both the ferrous and CO-bound forms of Ch-CooA is consistent with coupling of the heme doming distortion to the photolysis reaction in both samples. Upon CO binding and protein activation, a heme mode near 112 ± 5 cm(-1) disappears, probably indicating a decreased heme saddling distortion. This reflects changes in the heme environment and geometry that must be associated with the conformational transition activating the DNA-binding domain. Protein-specific DNA binding to the CO-bound form of Ch-CooA was also investigated, and although the CO rebinding kinetics are significantly perturbed, there are negligible changes in the low-frequency vibrational spectrum of the heme.

EPR and ENDOR studies of Fe(II) hemoproteins reduced and oxidized at 77 K

gamma-irradiation of frozen solutions of Fe(II) hemoproteins at 77 K generates both electron paramagnetic resonance (EPR) active singly reduced and oxidized heme centers trapped in the conformation of the Fe(II) precursors. The reduction products of pentacoordinate (S = 2) Fe(II) globins, peroxidases and cytochrome P450cam show EPR and electron-nuclear double resonance (ENDOR) spectra characteristic of (3d 7) Fe(I) species. In addition, cryoreduced Fe(II) alpha-chains of hemoglobin and myoglobin exhibit an S = 3/2 spin state produced by antiferromagnetic coupling between a porphyrin anion radical and pentacoordinate (S = 2) Fe(II). The spectra of cryoreduced forms of Fe(II) hemoglobin alpha-chains and deoxymyoglobin reveal that the Fe(II) precursors adopt multiple conformational substates. Reduction of hexacoordinate Fe(II) cytochrome c and cytochrome b5 as well as carboxy complexes of deoxyglobins produces only Fe(II) porphyrin pi-anion radical species. The low-valent hemoprotein intermediates produced by cryoreduction convert to the Fe(II) states at T > 200 K. Cryogenerated Fe(III) cytochrome c and cytochrome b5 have spectra similar to these for the resting Fe(III) states, whereas the spectra of the products of cryooxidation of pentacoordinate Fe(II) globins and peroxidases are different. Cryooxidation of CO-Fe(II) globins generates Fe(III) hemes with quantum-mechanically admixed S = 3/2, 5/2 ground states. The trapped Fe(III) species relax to the equilibrium ferric states upon annealing at T > 190 K. Both cryooxidized and reduced centers provide very sensitive EPR/ENDOR structure probes of the EPR-silent Fe(II) state.

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.

Resonance Raman spectroscopy study of change of iron spin state in horseradish peroxidase C induced by removal of calcium

Resonance Raman spectroscopy is used to probe the effect of calcium depletion on the heme group of horseradish peroxidase C at pH 8. Polarized Raman spectra are recorded with an argon ion laser at eight different wavelengths to provide a sound database for a reliable spectral decomposition. Upon calcium depletion, the spectrum is indicative of a predominantly pentacoordinated high spin state of the heme iron coexisting with small fractions of hexacoordinated high and low spin states. The dominant quantum mixed spin state of native ferric horseradish peroxidase, which is characteristic for class III peroxidases, is not detectable in the spectrum of the enzyme with partial distal Ca(2+) depletion. The quenching of the quantum mixed spin state and the predominance of the pentacoordinated high spin state are likely to arise from distortions induced by distal calcium depletion, which translates into a weaker Fe-N(epsilon)(His) bond and a more tilted imidazole. A correlation is proposed between the lower enzyme activity and the elimination of the pentacoordinated quantum mixed state upon Ca(2+) depletion.

An electrostatic model for the frequency shifts in the carbonmonoxy stretching band of myoglobin: correlation of hydrogen bonding and the stark tuning rate

The effect of internal and applied external electric fields on the vibrational stretching frequency for bound CO (nu(CO)) in myoglobin mutants was studied using density functional theory. Geometry optimization and frequency calculations were carried out for an imidazole-iron-porphine-carbonmonoxy adduct with various small molecule hydrogen-bonding groups. Over 70 vibrational frequency calculations of different model geometries and hydrogen-bonding groups were compared to derive overall trends in the C-O stretching frequency (nu(CO)) in terms of the C-O bond length and Mulliken charge. Simple linear functions were derived to predict the Stark tuning rate using an approach analogous to the vibronic theory of activation.(1) Potential energy calculations show that the strongest interaction occurs for C-H or N-H hydrogen bonding nearly perpendicular to the Fe-C-O bond axis. The calculated frequencies are compared to the structural data available from 18 myoglobin crystal structures, supporting the hypothesis that the vast majority of hydrogen-bonding interactions with CO occur from the side, rather than the end, of the bound CO ligand. The nu(CO) frequency shifts agree well with experimental frequency shifts for multiple bands, known as A states, and site-directed mutations in the distal pocket of myoglobin. The model calculations quantitatively explain electrostatic effects in terms of specific hydrogen-bonding interactions with bound CO in heme proteins.