Iron-ligand Bond Research Articles

Influence of the Fe(II) Spin State on Iron-Ligand Bonds in Heme Model Iron-Porphyrin Complexes with 4, 5 and 6 Ligands.

In this work heme models with four [Fe(II)(P)], five [Fe(II)(P)Im], [Fe(II)(P)O2] and six ligands [Fe(II)(P)(Im)O2], where P=porphyrin, with different spin states (ms=5, 3 and 1) of the iron atom were investigated using relativistic-corrected quantum chemistry methods (PW6B95-D3-DKH/jorge-TZP-DKH). Dependence of the iron-ligand bond properties on (i) spin state and (ii) number of ligands were analyzed using natural bond orbital analysis, electron density topology, electrostatic potential and electron localization function. It is shown that reversible binding of O2 is possible in case of formation of semicoordination bond between Fe(II) and imidazole. Binding of the fifth and sixth ligand from the energetic and orbital points of view is more favorable for the triplet Fe(II) state. At the same time for the six-coordinated complex [Fe(II)(P)(Im)O2] interconversion of Fe(II) electrons of valent 3d orbital from quintet to triplet and vice versa is possible under thermal fluctuations (energy barriers less than 2 kcal/mol).

Single-Molecule Force Spectroscopy Reveals that Iron-Ligand Bonds Modulate Proteins in Different Modes.

The iron-amino acid interactions Fe-O(Glu/Asp), Fe-N(His), and Fe-S(Cys) are the three major iron-ligand bonds in proteins. To compare their properties in proteins, we used atomic force microscopy (AFM)-based single-molecule force spectroscopy to investigate a superoxide reductase (Fe(III)-SOR) with all three types of bonds forming an Fe(His)4CysGlu center. We first found that Apo-SOR without bound iron showed multiple unfolding pathways only from the β-barrel core. Then, using Holo-SOR with a ferric ion, we found that a single Fe-O(Glu) bond can tightly connect the flexible N-terminal fragment to the β-barrel and stabilize the whole protein, showing a complete protein unfolding scenario, while the single Fe-N(His) bond was weak and unable to provide such a stabilization. Moreover, when multiple Fe-N bonds are present, a similar stabilization effect can be achieved. Our results showed that the iron-ligand bond modulates protein structure and stability in different modes at the single-bond level.

Synthesis and Characterization of a Bis(imino)-N-heterocyclic Carbene Analogue to Bis(imino)pyridine Iron Complexes

New bis(imino)-N-heterocyclic carbene ligands have been synthesized, and the corresponding iron complexes have been isolated and characterized. Whereas imidazole-derived complexes exhibited exclusively bidentate binding modes, 4,5,6-trihydropyrimidylidene-based ligands adopted a tridentate pincer conformation analogous to complexes of 2,6-bis(imino)pyridines. Bonding in the five-coordinate bis(imino)-N-heterocyclic carbene complex displayed considerably contracted iron–ligand bond distances in comparison to those in the analogous bis(imino)pyridine iron complex. Of particular note was an extraordinarily short iron–carbene carbon bond distance (1.812(2) A). In addition to demonstrating differences in bonding, the isoelectronic structures have different electrochemical properties that reflect the ability of the carbene to stabilize both oxidized and reduced forms of the parent organometallic species.

Photomagnetic Switching of the Complex [Nd(dmf)4(H2O)3(μ‐CN)Fe(CN)5]⋅H2O Analyzed by Single‐Crystal X‐Ray Diffraction

X-ray vision: Single-crystal XRD experiments (see picture) reveal the excited-state structure of the photomagnetic heterobimetallic title complex. The system shows a decrease in all the iron-ligand bond lengths, suggesting that photoexcitation involves a ligand-to-metal charge transfer or a change in the superexchange coupling between the metal centers.

Subpicosecond oxygen trapping in the heme pocket of the oxygen sensor FixL observed by time-resolved resonance Raman spectroscopy

Dissociation of oxygen from the heme domain of the bacterial oxygen sensor protein FixL constitutes the first step in hypoxia-induced signaling. In the present study, the photodissociation of the heme-O2 bond was used to synchronize this event, and time-resolved resonance Raman (TR(3)) spectroscopy with subpicosecond time resolution was implemented to characterize the heme configuration of the primary photoproduct. TR(3) measurements on heme-oxycomplexes are highly challenging and have not yet been reported. Whereas in all other known six-coordinated heme protein complexes with diatomic ligands, including the oxymyoglobin reported here, heme iron out-of-plane motion (doming) occurs faster than 1 ps after iron-ligand bond breaking; surprisingly, no sizeable doming is observed in the oxycomplex of the Bradyrhizobium japonicum FixL sensor domain (FixLH). This assessment is deduced from the absence of the iron-histidine band around 217 cm(-1) as early as 0.5 ps. We suggest that efficient ultrafast oxygen rebinding to the heme occurs on the femtosecond time scale, thus hindering heme doming. Comparing WT oxy-FixLH, mutant proteins FixLH-R220H and FixLH-R220Q, the respective carbonmonoxy-complexes, and oxymyoglobin, we show that a hydrogen bond of the terminal oxygen atom with the residue in position 220 is responsible for the observed behavior; in WT FixL this residue is arginine, crucially implicated in signal transmission. We propose that the rigid O2 configuration imposed by this residue, in combination with the hydrophobic and constrained properties of the distal cavity, keep dissociated oxygen in place. These results uncover the origin of the "oxygen cage" properties of this oxygen sensor protein.

Transient ligand docking sites in Cerebratulus lacteus mini-hemoglobin

The monomeric hemoglobin of the nemertean worm Cerebratulus lacteus functions as an oxygen storage protein to maintain neural activity under hypoxic conditions. It shares a large, apolar matrix tunnel with other small hemoglobins, which has been implicated as a potential ligand migration pathway. Here we explore ligand migration and binding within the distal heme pocket, to which the tunnel provides access to ligands from the outside. FTIR/TDS experiments performed at cryogenic temperatures reveal the presence of three transient ligand docking sites within the distal pocket, the primary docking site B on top of pyrrole C and secondary sites C and D. Site C is assigned to a cavity adjacent to the distal portion of the heme pocket, surrounded by the B and E helices. It has an opening to the apolar tunnel and is expected to be on the pathway for ligand entry and exit, whereas site D, circumscribed by TyrB10, GlnE7, and the CD corner, most likely is located on a side pathway of ligand migration. Flash photolysis experiments at ambient temperatures indicate that the rate-limiting step for ligand binding to CerHb is migration through the apolar channel to site C. Movement from C to B and iron-ligand bond formation involve low energy barriers and thus are very rapid processes in the wt protein.

Extended subnanosecond structural dynamics of myoglobin revealed by Laue crystallography.

Work carried out over the last 30 years unveiled the role of structural dynamics in controlling protein function. Cavity networks modulate structural dynamics trajectories and are functionally relevant; in globins they have been assigned a role in ligand migration and docking. These findings raised renewed interest for time-resolved structural investigations of myoglobin (Mb), a simple heme protein displaying a photosensitive iron-ligand bond. Photodissociation of MbCO generates a nonequilibrium population of protein structures relaxing over a time range extending from picoseconds to milliseconds. This process triggers ligand migration to matrix cavities with clear-cut effects on the rate and yield of geminate rebinding. Here, we report subnanosecond time-resolved Laue diffraction data on the triple mutant YQR-Mb [Leu-29(B10)Tyr, His-64(E7)Gln, Thr-67(E10)Arg] that depict the sequence of structural events associated with heme and protein relaxation from 100 ps to 316 ns and above. The photodissociated ligand rapidly (<0.1 ns) populates the Xe-binding cavity distal to the heme. Moreover, the heme relaxation toward the deoxy configuration is heterogeneous, with a slower phase ( approximately ns) evident in these experiments. Damping of the heme response appears to result from a strain exerted by the E-helix via the CD-turn; Phe-43(CD1), in close contact with heme, opposes tilt until the strain is relieved. A comparison with crystallographic data on wild-type Mb and mutants Leu(29)Phe or Leu(29)Trp suggests that the internal structure controls the rate and amplitude of the relaxation events. A correlation between structural dynamics as unveiled by Laue crystallography and functional properties of Mb is presented.

The Position 68(E11) Side Chain in Myoglobin Regulates Ligand Capture, Bond Formation with Heme Iron, and Internal Movement into the Xenon Cavities

After photodissociation, ligand rebinding to myoglobin exhibits complex kinetic patterns associated with multiple first-order geminate recombination processes occurring within the protein and a simpler bimolecular phase representing second-order ligand rebinding from the solvent. A smooth transition from cryogenic-like to solution phase properties can be obtained by using a combination of sol-gel encapsulation, addition of glycerol as a bathing medium, and temperature tuning (-15 --> 65 degrees C). This approach was applied to a series of double mutants, myoglobin CO (H64L/V68X, where X = Ala, Val, Leu, Asn, and Phe), which were designed to examine the contributions of the position 68(E11) side chain to the appearance and disappearance of internal rebinding phases in the absence of steric and polar interactions with the distal histidine. Based on the effects of viscosity, temperature, and the stereochemistry of the E11 side chain, the three major phases, B --> A, C --> A, and D --> A, can be assigned, respectively, to ligand rebinding from the following: (i) the distal heme pocket, (ii) the xenon cavities prior to large amplitude side chain conformational relaxation, and (iii) the xenon cavities after significant conformational relaxation of the position 68(E11) side chain. The relative amplitudes of the B --> A and C --> A phases depend markedly on the size and shape of the E11 side chain, which regulates sterically both ligand return to the heme iron atom and ligand migration to the xenon cavities. The internal xenon cavities provide a transient docking site that allows side chain relaxations and the entry of water into the vacated distal pocket, which in turn slows ligand recombination markedly.

Complex landscape of protein structural dynamics unveiled by nanosecond Laue crystallography.

Although conformational changes are essential for the function of proteins, little is known about their structural dynamics at atomic level resolution. Myoglobin (Mb) is the paradigm to investigate conformational dynamics because it is a simple globular heme protein displaying a photosensitivity of the iron-ligand bond. Upon laser photodissociation of carboxymyoglobin Mb a nonequilibrium population of protein structures is generated that relaxes over a broad time range extending from picoseconds to milliseconds. This process is associated with migration of the ligand to cavities in the matrix and with a reduction in the geminate rebinding rate by several orders of magnitude. Here we report nanosecond time-resolved Laue diffraction data to 1.55-A resolution on a Mb mutant, which depicts the sequence of structural events associated with this extended relaxation. Motions of the distal E-helix, including the mutated residue Gln-64(E7), and of the CD-turn are found to lag significantly (100-300 ns) behind local rearrangements around the heme such as heme tilting, iron motion out of the heme plane, and swinging of the mutated residue Tyr-29(B10), all of which occur promptly (< or =3 ns). Over the same delayed time range, CO is observed to migrate from a cavity distal to the heme known to bind xenon (called Xe4) to another such cavity proximal to the heme (Xe1). We propose that the extended relaxation of the globin moiety reflects reequilibration among conformational substates known to play an essential role in controlling protein function.

Measurement and simulation of nuclear inelastic-scattering spectra of molecular crystals

A procedure is presented that allows us to simulate from first principles the normalized spectra of nuclear inelastic scattering (NIS) of synchrotron radiation by molecular crystals containing a M\ossbauer isotope. Neglecting intermolecular vibrations the NIS spectrum is derived from the normal modes of the free molecule, that are calculated with the density-functional method B3LYP. At low temperatures the inelastic part of the calculated NIS spectrum is a superposition of peaks that correspond to the individual vibrational modes of the molecule. The area of each peak is proportional to that part of the mean-square displacement of the M\ossbauer isotope that is due to the corresponding vibrational mode. Angular-dependent NIS spectra have been recorded for a guanidinium nitroprusside single crystal and temperature-dependent NIS spectra for the spin-crossover system $[\mathrm{Fe}(\mathrm{tpa})(\mathrm{NCS}{)}_{2}]$ [tpa=tris(2-pyridylmethyl)amine]. Qualitative agreement is achieved between measured and simulated spectra for different crystal orientations of guanidinium nitroprusside. A remarkable increase of the iron-ligand bond stretching upon spin crossover has unambiguously been identified by comparing the measured NIS spectra of $[\mathrm{Fe}(\mathrm{tpa})(\mathrm{NCS}{)}_{2}]$ with the theoretical simulations.

The effects of heme modification on reactivity, ligand binding properties and iron-coordination structures of cytochrome P450nor

Artificial cytochrome P450nors (nitric oxide reductase) were prepared by replacing the native protoheme with various 2,4-substituted hemes: meso-, deutero-, and diacetyldeutero-hemes. For these samples, the ratio of low spin/high spin states of the ferric resting enzyme were varied, indicating that the coordination of the water molecule at the iron sixth site was affected by the electron withdrawing capacities of the heme 2,4-substituents. The binding of the water molecule reduces the rate of binding of nitric oxide (NO) to the ferric iron. In addition, the reduction reaction of the ferric–NO complex with NADH, which constitutes the second step in the NO reduction, was facilitated by the electron withdrawing capacity of 2,4-substituents. Consequently, proto- (native-) P450nor exhibited the highest overall enzymatic activity (NO reduction activity), while the enzymes containing diacetyl-, deutero-, and meso-hemes had considerably lower activities, since the NO reduction activity is determined by a balance of the reaction rates of the above two steps. The optical absorption spectra of the ferric–NO and the ferrous–CO complexes of the reconstituted enzymes show that the electron density on the heme in both states was modulated by the substituent groups. However, the resonance Raman spectral measurements showed that the Fe–NO and N–O stretching frequencies in the ferric–NO complex were insensitive to the electron density of the heme while the Fe–CO and C–O stretching frequencies in the ferrous–CO complex were sensitively varied by the electron withdrawing capacity of the 2,4-substituent. The differences are discussed in terms of the difference in the iron-ligand bond characters between the ferric–NO and the ferrous–CO complexes.

Direct evidence for the role of haem doming as the primary event in the cooperative transition of haemoglobin

The study of cooperative ligand binding among the four subunits of haemoglobin has played a central role in the understanding of allosteric transitions in a large number of enzymes. Haem iron out-of-plane motion has been suggested to be the trigger for the cooperative transition of haemoglobin. To function as a trigger in a dynamic sense, haem-iron doming must be the first conformational change to occur following ligand dissociation. Here we present the first direct demonstration that haem-iron doming occurs on the same time scale as the breaking of the iron-ligand bond, thus establishing haem-iron doming as the primary event which lead to the R-->T transition in haemoglobin.

Pressure effects on carbon monoxide rebinding to the isolated .alpha. and .beta. chains of human hemoglobin

The effects of pressure on the recombination kinetics of carbon monoxide binding to the isolated alpha and beta chains of human adult hemoglobin at pH 7, approximately 20 degrees C, were studied by the use of millisecond and nanosecond laser photolyses. The kinetic data were analyzed on the basis of a simple three-species model, which assumes two elementary reaction processes of bond formation and ligand migration steps. The activation volume for each elementary step was obtained from the pressure dependence of the rate constants. A pressure-dependent activation volume change from negative to positive values in the bimolecular carbon monoxide association reaction was observed for both of the isolated chains. This finding is attributed to a change of the rate-limiting step from the bond formation step to the ligand migration step. For both of the isolated chains, the activation volumes for ligand migration into and from the protein were estimated as +12-16 and +7-11 cm3 mol-1, respectively. These positive activation volumes for the ligand migration process may be caused by conformational fluctuations of proteins, that is, the conformational changes from "closed" to "open" structure. In the iron-ligand bond formation process, the activation volumes are -15 to -22 cm3 mol-1, which are almost identical to that for the model heme complexes [Taube, D. J., Projahn, H.-D., van Eldik, R., Magde, D., & Traylor, T. G. (1990) J. Am. Chem. Soc. 112, 6880-6886]. Accordingly, the surrounding protein contributions to the activation volumes for the bond formation process could be small.(ABSTRACT TRUNCATED AT 250 WORDS)

High-pressure laser photolysis study of hemoproteins. Effects of pressure on carbon monoxide binding dynamics for R- and T-state hemoglobins

The bimolecular association reaction of carbon monoxide to human adult hemoglobin at pH 7, 20 degrees C, was examined as a function of pressure up to 1500 bar by means of high-pressure laser photolysis. The apparent quantum yield for a millisecond recombination reaction decreased with pressure, which was attributed to an increase in the fraction of nanosecond geminate recombination reaction. On the basis of the pressure dependence of the recombination rate, the activation volumes at normal pressure for the binding of carbon monoxide to the R- and T-state hemoglobins were determined as -9.0 +/- 0.7 and -31.7 +/- 2.4 cm3 mol-1, respectively. Since the activation volumes for the overall CO association reaction were negative, it seems that the iron-ligand bond formation process mainly contributes to the rate-limiting step for both quaternary structures. The characteristic pressure dependence of the activation volume was observed for the R-state Hb but not for the T-state Hb. At 1000 bar, the activation volume for the R-state Hb was reduced to nearly zero, probably resulting from the contribution of the ligand migration process to the rate-limiting step. The effect of pressure on the activation enthalpy and entropy was also extracted from the data.

Electron-Transfer Thermodynamics, Valence-Electron Hybridization, and Bonding for Iron Compounds

Abstract The electron-transfer thermodynamics (a) for iron compounds (FeXm) and complexes (FeLn) and (b) for their heteroatoms (X/X−) and ligands (L/L−) in combination with other physical data provide insight into the valence-electron hybridization and bonding of the iron center. The basic conclusions are: (a) the chemical bonding of iron in its compounds and complexes is covalent and similar to that of carbon. (b) the electron-transfer processes of iron complexes are ligand-centered, and (c) the iron-ligand covalent bond energies can be evaluated from the electrochemically determined redox thermodynamics.

A comparison of the geminate recombination kinetics of several monomeric heme proteins.

The geminate rate constants for CO, O2, NO, methyl, ethyl, n-propyl, and n-butyl isocyanide rebinding to soybean leghemoglobin and monomeric component II of Glycera dibranchiata hemoglobin were measured at pH 7, 20 degrees C using a dye laser with a 30-ns square-wave pulse. The results were compared to the corresponding parameters for sperm whale myoglobin and the isolated alpha and beta subunits of human hemoglobin (Olson, J.S., Rohlfs, R.J., and Gibson, Q.H. (1987) J. Biol. Chem., 262, 12930-12938). The rate-limiting step for O2, NO, and isonitrile binding to all five proteins is ligand migration up to the initial geminate state, and the rate of this process determines the overall bimolecular association rate constant for these ligands. In contrast, iron-ligand bond formation limits the overall bimolecular rate for CO binding. The distal pockets in leghemoglobin and in Glycera HbII are approximately 10 times more accessible kinetically to diatomic ligands than that in sperm whale myoglobin. This difference accounts for the much larger association rate constants (1-2 x 10(8) M-1 s-1) that are observed for O2 and NO binding to leghemoglobin and Glycera HbII. The rates of isonitrile migration through leghemoglobin are also very large and indicate a very fluid or open distal structure near the sixth coordination position. In contrast, there is a marked decrease in the rate of migration up to and away from the sixth coordination position in Glycera HbII with increasing ligand size. These results were also used to interpret previously published rate constants and quantum yields for the high (R) and low (T) affinity states of human hemoglobin. In contrast to the differences between the monomeric proteins, the differences between the CO-, O2-, and NO-binding parameters for R and T state hemoglobin appear to be due to a decrease in the geminate reactivity of the heme iron atom, with little or no change in the accessibility of the distal pocket.

Ligand recombination to the alpha and beta subunits of human hemoglobin.

The rebinding of CO, O2, NO, methyl, ethyl, n-propyl, and n-butyl isocyanide to isolated alpha and beta chains and intact hemoglobin at pH 7, 20 degrees C was examined both during and after a 30-ns dye laser pulse. The resultant absorbance changes were analyzed in terms of a linear three-step reaction scheme: Hb + X in equilibrium with C in equilibrium with B in equilibrium with A or HbX, where A is the final bound state, and C and B are geminate states. Rate constants were assigned for each of the transitions in this mechanism using fitting procedures described previously for analyzing ligand rebinding to sperm whale myoglobin at room temperature (Gibson, Q. H., Olson, J. S., McKinnie, R. E., and Rohlfs, R. J. (1986) J. Biol. Chem. 261, 10228-10239). Five major conclusions were obtained. First, initial geminate recombination phases for the NO and O2 complexes of hemoglobin and its isolated subunits exhibit half-times equal to approximately 12 and approximately 440 ps, respectively. These values are in excellent agreement with more direct, picosecond measurements of the geminate recombination of HbNO (Cornelius, P. A., Hochstrasser, R. M., and Steele, A. W. (1983) J. Mol. Biol. 163, 119-128) and HbO2 (Friedman, J. M., Scott, T. W., Fisanick, G. J., Simon, S. R., Findsen, E. W., Ondrias, M. R., and MacDonald, V. W. (1985) Science 229, 187-229) following extremely short laser pulses. Second, the correspondence between our nanosecond measurements and the published picosecond data suggests strongly that the intrinsic photochemical yield of all ferrous, hexacoordinate heme complexes approaches one. Third, the major differences between the isolated alpha and beta chains involve the rate of ligand migration to the solvent, kC----X and the extent of recombination from the second geminate state, C, as measured by the ratio kC----B/kC----X. Fourth, for both isolated chains and intact hemoglobin, the rate and equilibrium constants for the formation of the initial O2 geminate state starting from ligand in the solvent (i.e. kX----B and KX----B) are 5-10 times greater than the corresponding parameters for the formation of the first CO geminate state. Fifth, the rate-limiting step for NO, O2, and isonitrile binding to hemoglobin and its isolated subunits is ligand migration up to the initial geminate state (i.e. kX----B). In the case of CO binding, both migration to state B and iron-ligand bond formation (kB----A) affect the overall, bimolecular association rate constant.

Resonance Raman study on the role of the iron-ligand bond for functional activity of heme proteins

Abstract

A kinetic description of ligand binding to sperm whale myoglobin.

Nanosecond recombination time courses were measured by photolyzing O2, NO, CO, methyl, ethyl, n-propyl, n-butyl, and tert-butyl isocyanide complexes of sperm whale myoglobin with a 30-ns laser pulse at pH 7, 20 degrees C. Absorbance was measured both during and after the excitation pulse and as a function of laser light intensity. The results were analyzed quantitatively in terms of a three-step reaction scheme, MbX in equilibrium B in equilibrium C in equilibrium Mb + X, where Mb is myoglobin, B represents a geminate state in which the ligand is present in the distal pocket but not covalently bound to the iron atom, and C, a state in which the ligand is still embedded in the protein but further away from the heme group. The fitted rate parameters were required to be consistent with the observed overall quantum yield, Q, which had been measured independently using much longer (approximately 0.5 ms) xenon flash pulses. Three major conclusions were derived from these analyses. First, the overall quantum yield of the ligand complex is determined primarily by the competition between the rate of iron-ligand bond formation from the initial photoproduct, kB----MbX, and the rate of migration away from state B, kB----C. For example, kB----C approximately equal to 30-100 microseconds-1 for all three gaseous ligands, whereas both Q and kB----MbX vary over 3 orders of magnitude (i.e. NO, Q = 0.001, kB----MbX approximately equal to 16,000 microseconds-1; O2, Q = 0.1, kB----MbX approximately equal to 500 microseconds-1; CO, Q = 1.0, kB----MbX approximately equal to 2 microseconds-1). Second, for NO, O2, and the isonitriles, the rate-limiting step in the overall association reaction starting from ligand in solution is the formation of state B. The rate constant for this process varies from 2 X 10(7) M-1 s-1 for the gaseous ligands to 0.02-1.4 X 10(5) M-1 s-1 for the isonitriles. In contrast, the B to MbX transition is limiting for CO binding. Third, for all the ligands except CO, the overall rate of dissociation is limited significantly both by the rate of thermal bond disruption, kMbX----B, and the competition between geminate recombination and migration away from the distal pocket (i.e. kB----C/(kB----MbX + kB----C]. In the case of CO, the rate of bond disruption is equal to the observed dissociation rate constant.

Resonance raman spectra of some ferric and cupric thiolate complexes

Resonance Raman (RR) spectra of intensely absorbing (at ∼600 nm) transient ferric thiolate species obtained by mixing iron(III) salts with l-cysteine, d-penicillamine, N-acetyl- d-penicillamine, and α-mercaptopropionic acid were measured between 250 and 500 cm −1. RR spectra of a red ferric d-penicillamine complex showing band maxima at 500 and 550 nm and of oxidized spinach ferredoxin are also reported. Vibrational bands in the low-frequency region are associated with ν(FeS) and ν(FeO) modes, resonance-enhanced with excitation into an iron-sulfur charge transfer electronic transition. Iron-ligand bond strength and possible structure-stability correlations are suggested. In addition, the RR spectrum of the violet Cu IIN 2S 2 core-containing copper d-penicillamine cluster complex was obtained. Comparisons with RR spectra of “blue” copper proteins and reinterpretation of the latter spectra are made. Use of Franck-Condon factors in interpreting resonance-enhancement of particular modes of vibration is discussed with regard to metal-ligand vibrations and charge transfer electronic transitions.