Relativistic DFT Calculations of the Paramagnetic Intermediates of [NiFe] Hydrogenase. Implications for the Enzymatic Mechanism Matthias Stein, Erik van Lenthe, Evert Jan Baerends, and Wolfgang Lubitz* Max-Volmer-Institut fu ¨ r Biophysikalische Chemie und Biochemie, Technische UniVersita ¨ t Berlin Strasse des 17. Juni 135, 10623 Berlin, Germany ReceiVed NoVember 20, 2000 ReVised Manuscript ReceiVed February 26, 2001 Hydrogenases are enzymes that catalyze the reversible hetero- lytic dissociation of molecular hydrogen H 2 a H + + H - . The largest class of hydrogenases contains a NiFe center that is believed to be the catalytic site for hydrogen activation. 1 Recent insight into the structure of the active site has come from X-ray structure analyses of single crystals of the [NiFe] hydrogenases from DesulfoVibrio (D.) gigas 2 and D. Vulgaris Miyazaki F. 3 The active site (Figure 1) comprises a heterobimetallic cluster of Ni and Fe atoms. The bridging ligand X was proposed to be an oxygen or sulfur species in the oxidized states of D. gigas and D. Vulgaris, respectively; X was found to be absent in the crystal structure of the reduced state of two enzymes. 4 Three nonprotein diatomics (2 CN and 1 CO) ligate the Fe atom. 5 The “as-isolated” oxidized state of the [NiFe] hydrogenase is a mixture of two paramagnetic forms (Ni-A and Ni-B) with slightly different g-values. 1 Ni-B (or “ready”) is reduced within minutes under an H 2 atmosphere while Ni-A (or “unready”) requires incubation for several hours. An EPR-silent state (Ni- Si) is passed before a third paramagnetic state (Ni-C) and the fully reduced state (Ni-R) is obtained. Ni-C is believed to be an intermediate in the catalytic cycle. Upon illumination, the Ni-C state is converted into a fourth paramagnetic state (Ni- L). Carbon monoxide is an inhibitor of the enzyme yielding a paramagnetic CO-bound state (Ni-CO). All paramagnetic states are S ) 1 / 2 . Previous quantum mechanical studies have addressed the question of H 2 activation by [NiFe] hydrogenases 6 and were mainly used to calculate IR transitions. 7 Here, we present the first relativistic 8 description and calculation of magnetic resonance parameters (g-tensors) of a transition metal containing enzyme 9 and show that these values can be correlated with structural parameters. This approach allows us to propose a reaction mechanism for the [NiFe] hydrogenases. Ni-B/Ni-A: The g-tensor magnitudes and orientations of the oxidized states were determined from EPR investigations of single crystals. 10 From the similarities of the g-values of Ni-A (2.32, 2.24, 2.01) and Ni-B (2.33, 2.16, 2.01), a drastic change in the electronic structure of the active site in the Ni-A state compared to Ni-B is unlikely. The g-tensor orientation was found to be very similar for Ni-B and Ni-A. 10 In the calculations, first the possibility of a sulfur species 3 (i.e. S 2- , SH - , or H 2 S) as bridging ligand X (Figure 1) was considered but did not lead to satisfying results. 11 Next, an oxygenic species was considered as X. 12 Such a species was postulated to occupy the position of the bridging ligand in D. gigas 2b and A. Vinosum. 13 The g-tensor orientation and the principal values of Ni-B were confirmed by our calculations when a OH - ligand occupies the position of the bridging ligand (Table 1). 14 The calculated Ni-Fe distance is 3.00 Å, in reasonable agreement with the value obtained from the X-ray analysis of D. gigas (2.9 Å). ZORA calculations with a depro- tonated bridging ligand, i.e., a O 2- bridge, gave g-values of 2.36, 1.95, 1.84. It was investigated whether the unrealistic values below g e result from the spin-restricted nature of the wave function. 15,16 The consideration of spin-polarization drastically improved the description. Thus a µ-oxo bridge was assigned to Ni-A. This is supported by the absence of D 2 O exchangeable protons in the active center of the Ni-A state 17 and the required prolonged exposure to H 2 to be activated compared to Ni-B (see below). Protonation of a terminal cysteine as proposed in ref 7b did not yield satisfying g-values. 18 The postulated protonation of the O 2- bridge in the Ni-B form would not be detectable in the X-ray structure due to the limited resolution of 2.5 Å. 2b Theoretical Chemistry, Vrije Universiteit, De Boelelaan 1083, 1081 HV Amsterdam, The Netherlands. (1) Albracht, S. P. J. Biochim. Biophys. Acta 1994, 1188, 167-204. (2) (a) Volbeda, A.; Charon, M.-H.; Piras, C.; Hatchikian, E. C.; Frey, M.; Fontecilla-Camps, J.-C. Nature 1995, 373, 580-587. (b) Volbeda, A.; Garcin, E.; Piras, C.; de Lacey, A. L.; Fernandez, V. M.; Hatchikian, E. C.; Frey, M.; Fontecilla-Camps, J. C. J. Am. Chem. Soc. 1996, 118, 12989-12996. (3) Higuchi, Y.; Yagi, T.; Yasuoka, N. Structure 1997, 5, 1671-1680. (4) (a) Higuchi, Y.; Ogata, H.; Miki, K.; Yasuoka, N.; Yagi, T. Structure 1999, 7, 549-556. (b) Garcin, E.; Vernede, X.; Hatchikian, E. C.; Volbeda, A.; Frey, M.; Fontecilla-Camps, J.-C. Structure 1999, 7, 557-566. (5) (a) Happe, R. P.; Roseboom, W.; Pierik, A. J.; Albracht, S. P. J. Nature 1997, 385, 126. (b) De Lacey, A. L.; Hatchikian, E. C.; Volbeda, A.; Frey, M.; Fontecilla-Camps, J.-C.; Fernandez, V. M. J. Am. Chem. Soc. 1997, 119, 7181-7189. (6) (a) Pavlov, M.; Siegbahn, P. E. M.; Blomberg, M. R. A.; Crabtree, R. H. J. Am. Chem. Soc. 1998, 120, 548-555. (b) DeGioia, L.; Fantucci, P.; Guigliarelli, B.; Bertrand, P. Inorg. Chem. 1999, 38, 2658-2662. (c) Pavlov, M.; Blomberg, M. R. A.; Siegbahn, P. E. M. Int. J. Quantum Chem. 1999, 73, 197-207. (d) DeGioia, L.; Fantucci, P.; Guigliarelli, B.; Bertrand, P. Int. J. Quantum Chem. 1999, 73, 187-195. (7) (a) Niu, S.; Thomson, L. M.; Hall, M. B. J. Am. Chem. Soc. 1999, 121, 4000-4007. (b) Amara, P.; Volbeda, A.; Fontecilla-Camps, J.-C.; Field, M. J. J. Am. Chem. Soc. 1999, 121, 4468-4477. (8) (a) van Lenthe, E.; Wormer, P. E. S.; van der Avoird, A. J. Chem. Phys. 1997, 107, 2488-2498. (b) van Lenthe, E.; van der Avoird, A.; Wormer, P. E. S. J. Chem. Phys. 1998, 108, 4783-4796. (9) Computational details: The ZORA formalism as implemented in the Amsterdam Density Functional (ADF) package was used. The calculations are single-point calculations at nonrelativistic geometry-optimized structures using the BP86 exchange-correlation functional. Cysteines were modeled as CH3-CH2-S - groups. No constraints were imposed on the structures. A double-Slater-type basis set with polarization functions (basis II in ADF nomenclature) was used. A triple-basis set is used for the 3d shells of the first transition metals. The following orbitals were frozen during geometry optimizations: C 1s, N 1s, O 1s, S up to 2p, Ni up to 2p, Fe up to 2p. The calculations of magnetic resonance parameters were performed in an all- electron basis. (10) (a) Gessner, C.; Trofanchuk, O.; Kawagoe, K.; Higuchi, Y.; Yasuoka, Y.; Lubitz, W. Chem. Phys. Lett. 1996, 256, 518-524. (b) Trofanchuk, O.; Stein, M.; Gessner, C.; Lendzian, F.; Higuchi, Y.; Lubitz, W. J. Biol. Inorg. Chem. 2000, 5, 36-44. (11) After complete geometry optimizations the Ni-Fe distances are 3.15 Å for H2S, 3.11 Å for SH - , and 3.19 Å for S 2- , whereas the X-ray structures yield 2.55 Å for D. Vulgaris Miyazaki F and 2.90 Å for D. gigas. The calculated g-values (gx, gy, gz) are 2.19, 2.06, 2.01 for a H2S, 2.19, 2.15, 1.99 for a SH - , and 2.31, 2.07, 1.91 for an S 2- ligand. These are not in good agreement with experimental values. (12) Comparison of structural data from X-ray analysis and geometry optimizations are available as Supporting Information. (13) Van der Zwaan, J. W.; Coremans, J. M. C. C.; Bouwens, E. C. M.; Albracht, S. P. J. Biochim. Biophys. Acta 1990, 1041, 101-110. (14) The deviation of the calculated gx-value from the experimental value is not unusual for the ZORA approach (Stein, M.; van Lenthe, E.; Baerends, E. J.; Lubitz, W. J. Phys. Chem. A 2001, 105, 416-425). Figure 1. Active site of [NiFe] hydrogenase from D. gigas (predomi- nantely in the Ni-A oxidation state) 2 , Cys ) cysteine. 5839 J. Am. Chem. Soc. 2001, 123, 5839-5840 10.1021/ja005808y CCC: $20.00 © 2001 American Chemical Society Published on Web 05/26/2001