Abdelkrim Benabbas

Ultrafast dynamics of diatomic ligand binding to nitrophorin 4

Nitrophorin 4 (NP4) is a heme protein that stores and delivers nitric oxide (NO) through pH-sensitive conformational change. This protein uses the ferric state of a highly ruffled heme to bind NO tightly at low pH and release it at high pH. In this work, the rebinding kinetics of NO and CO to NP4 are investigated as a function of iron oxidation state and the acidity of the environment. The geminate recombination process of NO to ferrous NP4 at both pH 5 and pH 7 is dominated by a single approximately 7 ps kinetic phase that we attribute to the rebinding of NO directly from the distal pocket. The lack of pH dependence explains in part why NP4 cannot use the ferrous state to fulfill its function. The kinetic response of ferric NP4NO shows two distinct phases. The relative geminate amplitude of the slower phase increases dramatically as the pH is raised from 5 to 8. We assign the fast phase of NO rebinding to a conformation of the ferric protein with a closed hydrophobic pocket. The slow phase is assigned to the protein in an open conformation with a more hydrophilic heme pocket environment. Analysis of the ultrafast kinetics finds the equilibrium off-rate of NO to be proportional to the open state population as well as the pH-dependent amplitude of escape from the open pocket. When both factors are considered, the off-rate increases by more than an order of magnitude as the pH changes from 5 to 8. The recombination of CO to ferrous NP4 is observed to have a large nonexponential geminate amplitude with rebinding time scales of approximately 10(-11)-10(-9) s at pH 5 and approximately 10(-10)-10(-8) s at pH 7. The nonexponential CO rebinding kinetics at both pH 5 and pH 7 are accounted for using a simple model that has proven effective for understanding CO binding in a variety of other heme systems (Ye, X.; et al. Proc. Natl. Acad. Sci. U.S.A. 2007, 104, 14682).

Investigations of heme distortion, low-frequency vibrational excitations, and electron transfer in cytochrome c.

Significance To probe the effect of heme ruffling on electron transport, we studied three cytochromes that display wide variation in the heme ruffling distortion. Ruffling is characterized by a low-frequency heme mode in the region 45–60 cm−1 and by a photoreduction cross-section that displays strong variation as a function of the magnitude of the distortion. Given the similarity in the distance between the heme and the nearest aromatic amino acid for all three proteins, the order-of-magnitude changes in photoreduction rate demonstrate that the ruffling coordinate can serve as a control mechanism for electron transport in heme proteins. Major differences in heme ruffling are noted for cytochrome c when bound to the mitochondrial membrane compared with its solution structure. Cytochrome (cyt) c is an important electron transfer protein. The ruffling deformation of its heme cofactor has been suggested to relate to its electron transfer rate. However, there is no direct experimental evidence demonstrating this correlation. In this work, we studied Pseudomonas aeruginosa cytochrome c551 and its F7A mutant. These two proteins, although similar in their X-ray crystal structure, display a significant difference in their heme out-of-plane deformations, mainly along the ruffling coordinate. Resonance Raman and vibrational coherence measurements also indicate significant differences in ruffling-sensitive modes, particularly the low-frequency γa mode found between ∼50–60 cm−1. This supports previous assignments of γa as having a large ruffling content. Measurement of the photoreduction kinetics finds an order of magnitude decrease of the photoreduction cross-section in the F7A mutant, which has nearly twice the ruffling deformation as the WT. Additional measurements on cytochrome c demonstrate that heme ruffling is correlated exponentially with the electron transfer rates and suggest that ruffling could play an important role in redox control. A major relaxation of heme ruffling in cytochrome c, upon binding to the mitochondrial membrane, is discussed in this context.

Temperature-dependent heme kinetics with nonexponential binding and barrier relaxation in the absence of protein conformational substates

We present temperature-dependent kinetic measurements of ultrafast diatomic ligand binding to the “bare” protoheme (L1-FePPIX-L2, where L1 = H2O or 2-methyl imidazole and L2 = CO or NO). We found that the binding of CO is temperature-dependent and nonexponential over many decades in time, whereas the binding of NO is exponential and temperature-independent. The nonexponential nature of CO binding to protoheme, as well as its relaxation above the solvent glass transition, mimics the kinetics of CO binding to myoglobin (Mb) but on faster time scales. This demonstrates that the nonexponential kinetic response observed for Mb is not necessarily due to the presence of protein conformational substates but rather is an inherent property of the solvated heme. The nonexponential kinetic data were analyzed by using a linear coupling model with a distribution of enthalpic barriers that fluctuate on slower time scales than the heme–CO recombination time. Below the solvent glass transition (Tg ≈ 180 K), the average enthalpic rebinding barrier for H2O-PPIX-CO was found to be ≈1 kJ/mol. Above Tg, the barrier relaxes and is ≈6 kJ/mol at 290 K. Values for the first two moments of the heme doming coordinate distribution extracted from the kinetic data suggest significant anharmonicity above Tg. In contrast to Mb, the protoheme shows no indication of the presence of “distal” enthalpic barriers. Moreover, the wide range of Arrhenius prefactors (109 to 1011 s−1) observed for CO binding to heme under differing conditions suggests that entropic barriers may be an important source of control in this class of biochemical reactions.

Investigations of heme ligation and ligand switching in cytochromes P450 and P420

It is generally accepted that the inactive P420 form of cytochrome P450 (CYP) involves the protonation of the native cysteine thiolate to form a neutral thiol heme ligand. On the other hand, it has also been suggested that recruitment of a histidine to replace the native cysteine thiolate ligand might underlie the P450 → P420 transition. Here, we discuss resonance Raman investigations of the H93G myoglobin (Mb) mutant in the presence of tetrahydrothiophene (THT) or cyclopentathiol (CPSH), and on pressure-induced cytochrome P420cam (CYP101), that show a histidine becomes the heme ligand upon CO binding. The Raman mode near 220 cm⁻¹, normally associated with the Fe-histidine vibration in heme proteins, is not observed in either reduced P420cam or the reduced H93G Mb samples, indicating that histidine is not the ligand in the reduced state. The absence of a mode near 220 cm⁻¹ is also inconsistent with a generalization of the suggestion that the 221 cm⁻¹ Raman mode, observed in the P420-CO photoproduct of inducible nitric oxide synthase (iNOS), arises from a thiol-bound ferrous heme. This leads us to assign the 218 cm⁻¹ mode observed in the 10 ns P420cam-CO photoproduct Raman spectrum to a Fe-histidine vibration, in analogy to many other histidine-bound heme systems. Additionally, the inverse correlation plots of the νFe-His and νCO frequencies for the CO adducts of P420cam and the H93G analogs provide supporting evidence that histidine is the heme ligand in the P420-CO-bound state. We conclude that, when CO binds to the ferrous P420 state, a histidine ligand is recruited as the heme ligand. The common existence of an HXC-Fe motif in many CYP systems allows the C → H ligand switch to occur with only minor conformational changes. One suggested conformation of P420-CO involves the addition of another turn in the proximal L helix so that, when the protonated Cys ligand is dissociated from the heme, it can become part of the helix, and the heme is ligated by the His residue from the adjoining loop region. In other systems, such as iNOS and CYP3A4 (where the HXC-Fe motif is not found), a somewhat larger conformational change would be necessary to recuit a nearby histidine.

Effect of DNA Binding on Geminate CO Recombination Kinetics in CO-sensing Transcription Factor CooA

Background: CooA proteins are CO-sensing transcription factors. Results: DNA binding to CooA-CO speeds up geminate rebinding of CO. Conclusion: DNA binding reduces heme heterogeneity and CO rebinding barrier. This along with distal pocket trapping maintains the “on” state long enough for transcription to take place. Significance: This work provides a deeper understanding of the allosteric transition in CooA proteins. Carbon monoxide oxidation activator (CooA) proteins are heme-based CO-sensing transcription factors. Here we study the ultrafast dynamics of geminate CO rebinding in two CooA homologues, Rhodospirillum rubrum (RrCooA) and Carboxydothermus hydrogenoformans (ChCooA). The effects of DNA binding and the truncation of the DNA-binding domain on the CO geminate recombination kinetics were specifically investigated. The CO rebinding kinetics in these CooA complexes take place on ultrafast time scales but remain non-exponential over many decades in time. We show that this non-exponential kinetic response is due to a quenched enthalpic barrier distribution resulting from a distribution of heme geometries that is frozen or slowly evolving on the time scale of CO rebinding. We also show that, upon CO binding, the distal pocket of the heme in the CooA proteins relaxes to form a very efficient hydrophobic trap for CO. DNA binding further tightens the narrow distal pocket and slightly weakens the iron-proximal histidine bond. Comparison of the CO rebinding kinetics of RrCooA, truncated RrCooA, and DNA-bound RrCooA proteins reveals that the uncomplexed and inherently flexible DNA-binding domain adds additional structural heterogeneity to the heme doming coordinate. When CooA forms a complex with DNA, the flexibility of the DNA-binding domain decreases, and the distribution of the conformations available in the heme domain becomes restricted. The kinetic studies also offer insights into how the architecture of the heme environment can tune entropic barriers in order to control the geminate recombination of CO in heme proteins, whereas spin selection rules play a minor or non-existent role.

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.

Investigations of Ferric Heme Cyanide Photodissociation in Myoglobin and Horseradish Peroxidase

The photodissociation of cyanide from ferric myoglobin (MbCN) and horseradish peroxidase (HRPCN) has definitively been observed. This has implications for the interpretation of ultrafast IR (Helbing et al. Biophys. J. 2004, 87, 1881-1891) and optical (Gruia et al. Biophys. J. 2008, 94, 2252-2268) studies that had previously suggested the Fe-CN bond was photostable in MbCN. The photolysis of ferric MbCN takes place with a quantum yield of ~75%, and the resonance Raman spectrum of the photoproduct observed in steady-state experiments as a function of laser power and sample spinning rate is identical to that of ferric Mb (metMb). The data are quantitatively analyzed using a simple model where cyanide is photodissociated and, although geminate rebinding with a rate of kBA ≈ (3.6 ps)(-1) is the dominant process, some CN(-) exits from the distal heme pocket and is replaced by water. Using independently determined values for the CN(-) association rate, we find that the CN(-) escape rate from the ferric myoglobin pocket to the solution at 293 K is kout ≈ (1-2) × 10(7) s(-1). This value is very similar to, but slightly larger than, the histidine gated escape rate of CO from Mb (1.1 × 10(7) s(-1)) under the same conditions. The analysis leads to an escape probability kout/(kout + kBA) ~ 10(-4), which is unobservable in most time domain kinetic measurements. However, the photolysis is surprisingly easy to detect in Mb using cw resonance Raman measurements. This is due to the anomalously slow CN(-) bimolecular association rate (170 M(-1) s(-1)), which arises from the need for water to exchange at the ferric heme binding site of Mb. In contrast, ferric HRP does not have a heme bound water molecule and its CN(-) bimolecular association rate is larger by ~10(3), making the CN(-) photolysis more difficult to observe.

Kinetic Control of O2 Reactivity in H-NOX Domains.

Transient absorption, resonance Raman, and vibrational coherence spectroscopies are used to investigate the mechanisms of NO and O2 binding to WT Tt H-NOX and its P115A mutant. Vibrational coherence spectra of the oxy complexes provide clear evidence for the enhancement of an iron-histidine mode near 217 cm(-1) following photoexcitation, which indicates that O2 can be dissociated in these proteins. However, the quantum yield of O2 photolysis is low, particularly in the wild type (≲3%). Geminate recombination of O2 and NO in both of these proteins is very fast (∼1.4 × 10(11) s(-1)) and highly efficient. We show that the distal heme pocket of the H-NOX system forms an efficient trap that limits the O2 off-rate and determines the overall affinity. The distal pocket hydrogen bond, which appears to be stronger in the P115A mutant, may help retard the O2 ligand from escaping into the solvent following either photoinduced or thermal dissociation. This, along with a strengthening of the Fe-O2 bond that is correlated with the significant heme ruffing and saddling distortions, explains the unusually high O2 affinity of WT Tt H-NOX and the even higher affinity found in the P115A mutant.

Investigations of the low frequency modes of ferric cytochrome c using vibrational coherence spectroscopy.

Femtosecond vibrational coherence spectroscopy is used to investigate the low frequency vibrational dynamics of the electron transfer heme protein, cytochrome c (cyt c). The vibrational coherence spectra of ferric cyt c have been measured as a function of excitation wavelength within the Soret band. Vibrational coherence spectra obtained with excitation between 412 and 421 nm display a strong mode at ∼44 cm–1 that has been assigned to have a significant contribution from heme ruffling motion in the electronic ground state. This assignment is based partially on the presence of a large heme ruffling distortion in the normal coordinate structural decomposition (NSD) analysis of the X-ray crystal structures. When the excitation wavelength is moved into the ∼421–435 nm region, the transient absorption increases along with the relative intensity of two modes near ∼55 and 30 cm–1. The intensity of the mode near 44 cm–1 appears to minimize in this region and then recover (but with an opposite phase compared to the blue excitation) when the laser is tuned to 443 nm. These observations are consistent with the superposition of both ground and excited state coherence in the 421–435 nm region due to the excitation of a weak porphyrin-to-iron charge transfer (CT) state, which has a lifetime long enough to observe vibrational coherence. The mode near 55 cm–1 is suggested to arise from ruffling in a transient CT state that has a less ruffled heme due to its iron d6 configuration.

Peptide-Decorated Tunable-Fluorescence Graphene Quantum Dots

We report here the synthesis of graphene quantum dots with tunable size, surface chemistry, and fluorescence properties. In the size regime 15-35 nm, these quantum dots maintain strong visible light fluorescence (mean quantum yield of 0.64) and a high two-photon absorption (TPA) cross section (6500 Göppert-Mayer units). Furthermore, through noncovalent tailoring of the chemistry of these quantum dots, we obtain water-stable quantum dots. For example, quantum dots with lysine groups bind strongly to DNA in solution and inhibit polymerase-based DNA strand synthesis. Finally, by virtue of their mesoscopic size, the quantum dots exhibit good cell permeability into living epithelial cells, but they do not enter the cell nucleus.