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.
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A.; Frey, M.; Fontecilla-Camps, J.-C. Structure 1999, 7, 557-566.
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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,
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H. J. Am. Chem. Soc. 1998, 120, 548-555. (b) DeGioia, L.; Fantucci, P.;
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J. Quantum Chem. 1999, 73, 187-195.
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J. J. Am. Chem. Soc. 1999, 121, 4468-4477.
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(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