Two non-heme iron-nitrosyl species, [Fe2(N-Et-HPTB)(O2CPh)(NO)2](BF4)2 (1a) and [Fe2(N-Et-HPTB)(DMF)2(NO)(OH)](BF4)3 (2a), are characterized by FTIR and resonance Raman spectroscopy. Binding of NO is reversible in both complexes, which are prone to NO photolysis under visible light illumination. Photoproduction of N2O occurs in high yield for 1a but not 2a. Low-temperature FTIR photolysis experiments with 1a in acetonitrile do not reveal any intermediate species, but in THF at room temperature, a new {FeNO}(7) species quickly forms under illumination and exhibits a ν(NO) vibration indicative of nitroxyl-like character. This metastable species reacts further under illumination to produce N2O. A reaction mechanism is proposed, and implications for NO reduction in flavodiiron proteins are discussed.
Two non-hemeiron-nitrosyl species, [Fe2(N-Et-HPTB)(O2CPh)(NO)2](BF4)2 (1a) and [Fe2(N-Et-HPTB)(DMF)2(NO)(OH)](BF4)3 (2a), are characterized by FTIR and resonance Raman spectroscopy. Binding of NO is reversible in both complexes, which are prone to NO photolysis under visible light illumination. Photoproduction of N2O occurs in high yield for 1a but not 2a. Low-temperature FTIR photolysis experiments with 1a in acetonitrile do not reveal any intermediate species, but in THF at room temperature, a new {FeNO}(7) species quickly forms under illumination and exhibits a ν(NO) vibration indicative of nitroxyl-like character. This metastable species reacts further under illumination to produce N2O. A reaction mechanism is proposed, and implications for NO reduction in flavodiiron proteins are discussed.
Nitric oxide (NO) plays an important
role in cellular signaling in a wide range of biological processes.
NO can also be toxic when present at high concentration, and it participates
as a key immune defense agent against invading pathogens. Accordingly,
a variety of detoxifying enzymes have evolved in pathogens, and understanding
their microbial NO defense mechanisms may provide new strategies for
controlling infections.[1−7] In anaerobic environments, NO detoxification occurs via the two-electron
reduction of NO to form nitrous oxide (N2O). Flavodiiron
proteins (FDPs) are flavin-containing, NO-detoxifying enzymes with
an active site containing a non-hemediiron cluster (see Chart 1).[4] In most FDPs,[8] each metal ion is coordinated by two His ligands
and one terminal monodentate carboxylate group from either Asp or
Glu; a bridging bidentate Asp and a water-derived ligand (oxo or hydroxo)
complete the coordination sphere. An open coordination site remains
on each Fe(II). Both mono- ({FeNO}7) and dinitrosyl ([{FeNO}7]2) FDP adducts have been characterized.[9,10] Experiments with a flavin-free form of the enzyme reveal that N2O production can occur without the flavin mononucleotide (FMN)
cofactor.[10] An exceptionally low frequency
ν(NO) band at 1681 cm–1 was detected in mononitrosyl
complexes of FMN-free and FMN-containing enzymes, which suggests a
nitroxyl-like configuration of the {FeNO}7 unit.[9] Electrostatic interaction of thisnitroxyl-like
group with the adjacent FeII center could prime the mononitrosyl
complex for electrophilic attack by a second NO.[9] In contrast, the [{FeNO}7]2 adduct
persists in the FMN-free enzyme, suggesting that it either corresponds
to an inactive state[10] or may be poised
for reduction by FMN in the flavinated enzyme.[4]
Chart 1
Structural Comparison
of Complexes 1, 1a, 2, 2a, 3a, and the Active
Site of FDP
Non-hemeiron synthetic models provide insight into the catalytic
mechanism of FDP proteins. The first report of a non-hemediiron–dinitrosyl
compound, [Fe2(N-Et-HPTB)(O2CPh)(NO)2](BF4)2 (1a, N-Et-HPTB = N,N,N′,N′-tetrakis(2-(1-ethylbenzimidazolyl))-2-hydroxy-1,3-diaminopropane),
detailed a full characterization of the model complex by single-crystal
X-ray diffraction, UV/vis, IR, and Mössbauer spectroscopy,
and magnetic susceptibility measurements. It also revealed 1a to be stable in an acetonitrile solution for over a day at room
temperature.[11]A mixed-valent diiron–mononitrosyl
complex, [Fe2(N-Et-HPTB)(OH)(NO)(DMF)2](BF4)3 (2a), with
the N-Et-HPTB ligand was also isolated.[12] Recently, an iron–nitrosyl dimer,
[Fe2(BPMP)(OPr)(NO)2](BPh4)2 (3a, BPMP = 2,6-bis[(bis(2-pyridylmethyl)amino)methyl]-4-methylphenolate),
was structurally characterized and shown to produce N2O
upon either chemical or electrochemical reduction.[13] This latter example supports the notion that FMN could
reduce the [{FeNO}7]2 complex in FDP and thus
allow catalytic turnover without redox cycling of the Fe(II) centers.
Nevertheless, activating the {FeNO}7 unit for attack by
a second NO to produce a transient hyponitrite remains a valid alternative
for the reduction of NO to N2O.Here we report that
production of N2O by 1a can proceed under
illumination with white light at room temperature
and at 15 K. We also show that this process is preceded by simple
photodissociation of NO from the iron–nitrosyl
dimer. In the case of 2a, photodissociation also
occurs, but the resulting NO does not react further.The chromophoric
{FeNO}7 units in 1a and 2a display
distinctive nitrosyl-to-iron ligand-to-metal charge-transfer
absorption bands, and these NO adducts in acetonitrile solutions easily
revert to diiron(II) compounds after the sample is purged with Ar
(Figure 1). The resonance Raman (RR) spectrum
of 1a obtained with 458 nm laser excitation shows a ν(FeNO)
band at 492 cm–1 with unlabeled NO that shifts to
486 cm–1 with 15NO and to 478 cm–1 with 15N18O (Figure 2). Nearly identical ν(FeNO) frequencies are
observed in the RR spectrum of 2a, which is consistent
with the structural similarity of these [FeNO] units observed by crystallography.[11,12] Additional vibrations in the low-frequency region of the RR spectrum
of 2a cannot be assigned with certainty at this time,
but these modes do not shift with NO labeling or with the addition
of 20% D2O to the acetonitrile solutions and are therefore
unrelated to the nitrosyl or hydroxy ligands.
Figure 1
Electronic spectra of 1 and 1a (left
panel) and 2 and 2a (right panel) in acetonitrile
at room temperature. Also shown are the effects of purging solutions
of 1a and 2a with Ar for 3 min (dashed lines)
before repeated exposure to NO.
Figure 2
Resonance Raman spectra of 1 and 1a (left
panel) and 2 and 2a (right panel) at room
temperature (λexc = 458 nm, [1], [1a] = 2 mM, [2], [2a] = 2.5 mM).
Electronic spectra of 1 and 1a (left
panel) and 2 and 2a (right panel) in acetonitrile
at room temperature. Also shown are the effects of purging solutions
of 1a and 2a with Ar for 3 min (dashed lines)
before repeated exposure to NO.Resonance Raman spectra of 1 and 1a (left
panel) and 2 and 2a (right panel) at room
temperature (λexc = 458 nm, [1], [1a] = 2 mM, [2], [2a] = 2.5 mM).Room-temperature FTIR spectra
of 1a and 2a in acetonitrile show ν(NO)
modes at 1784 and 1810 cm–1, respectively, with
the expected down-shifts with 15NO
and 15N18O (Figure 3).
These ν(NO) values are consistent with earlier reports[11,12] and with the S = 3/2 {FeNO}7 description
of non-heme [FeNO] units.[14] As reported
previously, 1a is composed of two {FeNO}7 units,
which have identical coordination environments and exhibit the same
set of vibrational frequencies. The ν(NO) band in 2a is up-shifted by 26 cm–1 relative to that in 1a and is significantly broadened, presumably because of the
heterogeneity in the binding geometry and environment of the nitrosyl
group in 2a. The up-shift of the ν(NO) may result
from substitution of the bridging benzoate in 1a by two
DMF ligands in 2a. Amide-like vibrations from DMF are
observed for 2a at 1654 and 1677 cm–1. The latter frequency matches that of free DMF in acetonitrile,
whereas the lower frequency at 1654 cm–1 is consistent
with a lengthening of the C=O bond upon coordination of DMF
to metal ions.
Figure 3
Room-temperature FTIR spectra of 1a (left
panel) and 2a (right panel) at room temperature ([1a] =
18 mM, [2a] = 20 mM).
Room-temperature FTIR spectra of 1a (left
panel) and 2a (right panel) at room temperature ([1a] =
18 mM, [2a] = 20 mM).Low-temperature FTIR spectra of 1a reproduce
the ν(NO)
values observed at room temperature, but those of 2a display
a significant decrease in the intensity of the ν(NO) modes that
is indicative of a diminished NO binding affinity at cryogenic temperatures
(Figure S1). Previous differential FTIR
photolysis experiments indicate that, at least within the active sites
of metalloproteins, non-hemeiron–nitrosyl complexes
can be trapped as photodissociated states following illumination
with white light at cryogenic temperatures.[9,10,15,16] Based on these
findings, “dark” minus “illuminated” FTIR
difference spectra can be used to isolate ν(NO) bands emanating
from {FeNO}7 species as positive features in the 1700 cm–1 region, whereas the photolyzed NO group is detected
as a weak negative band near 1870 cm–1. Typically,
the buildup of the photolyzed population occurs during the first few
minutes of white-light illumination, and further illumination does
not produce any additional spectral changes. Geminate rebinding of
the photolyzed ligand requires a slight increase in sample temperature
(to ∼40–80 K), and repeating the photolysis procedure
at 15 K confirms the complete reversibility of these processes. Reversible
photorelease of NO from a non-heme {FeNO}7 synthetic
complex at room temperature was also reported recently.[17]Low-temperature FTIR photolysis experiments
with 2a reproduce the behavior displayed previously by
non-heme protein
NO adducts (Figure 4). Specifically, the spectra
show that the {FeNO}7 species in 2a is photolabile
and that further illumination does not produce any additional changes.
In contrast, 1a reveals unique photoreactivity.
The light-induced FTIR difference spectrum of 1a at 15
K exhibits a positive band at 1787 cm–1 and a weak
negative band at 1867 cm–1 which, based on 15NO-isotope shifts, are assigned to the ν(NO) of {FeNO}7 and free NO, respectively (Figure 4). Further illumination at 15 K produces additional spectral changes,
including the appearance of a negative signal at 2239 cm–1 that shifts to 2168 and 2162 cm–1 with 15NO and 15N18O, respectively. (Figures 4 and S2). The 2239 cm–1 signal and its accompanying isotope shifts are characteristic
of the ν(NN) mode of N2O. This process is irreversible
and can result in the complete consumption of 1a after
prolonged illumination at 15 K (Figure S3). FTIR samples prepared by exposing 1 to substochiometric
levels of NO produce light-induced difference spectra equivalent to
those obtained with 1a, indicating that two NO molecules
bind in a cooperative fashion to 1 without significant
buildup of a mononitrosyl species (Figure
S4). Comparing the integration of the ν(NN) signal generated
from 1a after illumination at 15 K with titration curves
generated using N2O-saturated acetonitrile suggests that
the formation of N2O proceeds with a high yield (∼90%
at 15 K, Figure S5). These FTIR experiments
indicate that white-light illumination of 1a initially
produces a population of caged-in dissociated NO that can react with
the diiron complex to subsequently generate N2O under further
illumination. Because this reaction occurs at 15 K, an intermolecular
process between two or more 1a diiron complexes can be
ruled out. In addition, decreasing the concentration of 1a does not significantly affect the illumination time required for
the formation of N2O (data not shown).
Figure 4
Light-induced FTIR difference
spectra of 1a (left
panel, difference spectra for 1 and 7 min illuminations) and 2a (right panel, difference spectra after completion of the
photoprocess) at 15 K ([1a] = 18 mM, [2a] = 20 mM).
Light-induced FTIR difference
spectra of 1a (left
panel, difference spectra for 1 and 7 min illuminations) and 2a (right panel, difference spectra after completion of the
photoprocess) at 15 K ([1a] = 18 mM, [2a] = 20 mM).Because the reduction
of two NO molecules to N2O requires
two electrons, the other product of the photoreaction is likely
to be a diiron(III) complex. EPR spectra of 1a obtained
after illumination at 15 K showed no signal that could be assigned
as Fe(III) centers (data not shown), suggesting antiferromagnetic
coupling between the two Fe(III) centers. RR spectroscopy was used
to determine whether a (μ-oxo)diiron(III) product is formed
after the release of N2O, but the results were inconclusive.Production of N2O from 1a under illumination
is also observed at room temperature in acetonitrile and THF, although
with reduced yields compared to those at low temperature (15% and
26%, respectively). FTIR spectra of 1a in THF collected
in the dark and after consecutive 1 min illuminations reveal a loss
of the ν(NO) at 1781 cm–1 in favor of a signal
at 1695 cm–1 that shifts to 1665 cm–1 with 15NO, and a minor intensity gain in the ν(NN)
of N2O at 2223 cm–1 (Figure 5, top traces). After the first
2 min of irradiation, subsequent illuminations lead to growth of the
ν(NN) signal and concurrent decreases in ν(NO) and the
peak at 1695 cm–1 (Figure 5, lower traces). Differential FTIR spectra for the initial and later
phases of the photoprocess also help isolate light-induced features
below 1600 cm–1 that are insensitive to NO-isotope
substitution and are likely to reflect minor perturbations of vibrational
modes from the N-Et-HPTB ligand and
the benzoate bridge (Figure S6).
Figure 5
Room-temperature
FTIR spectra of 1a prepared in THF
with 14NO (top traces) or 15NO (lower traces).
Spectra were collected in the dark and after illumination periods
of 1, 2, 3, 7, and 15 min.
Room-temperature
FTIR spectra of 1a prepared in THF
with 14NO (top traces) or 15NO (lower traces).
Spectra were collected in the dark and after illumination periods
of 1, 2, 3, 7, and 15 min.Time-dependent traces for the decay of the 1781 cm–1 ν(NO) band from 1a and the growth of the 2223
cm–1 ν(NN) band from N2O are shown
in Figure 6. The intensity gain at 2223 cm–1 fits a single-exponential rate of 0.2 min–1. The time trace for the intensity loss of the ν(NO) of 1a requires a biexponential fit with rate constants of 1.1
and 0.1 min–1. The fast phase represents 26% of
the overall amplitude of the signal change and matches the yield of
N2O; presumably, the slower phase reflects side reactions
that do not produce N2O. Analyzing the time progression
of the 1695 cm–1 signal is less reliable because
of its weak intensity and because expected diiron(III) products are
likely to give weak signals below 1700 cm–1. Nevertheless,
it is worthwhile to compare the progression of this signal by means
of a simulation curve for an intermediate species with formation and
decay rates that correspond to the 1.1 min–1 decay
of 1a and the 0.2 min–1 formation of
N2O (Figure 6).
Figure 6
Progression of the FTIR
intensity for ν(NO) of 1a (black squares) and ν(NN)
of N2O (red circles)
and for the 1695 cm–1 signal (open blue squares)
(see Supporting Information for details).
Progression of the FTIR
intensity for ν(NO) of 1a (black squares) and ν(NN)
of N2O (red circles)
and for the 1695 cm–1 signal (open blue squares)
(see Supporting Information for details).The 1695 cm–1 FTIR signal and its 30 cm–1 down-shift with 15NO are consistent with a ν(NO)
from an iron–nitrosyl complex with [FeIII–NO–] nitroxyl-like character. However,
this ν(NO) frequency is unusually low for a non-heme {FeNO}7 species and is reminiscent of the 1681 cm–1 band seen in the FTIR spectra of the mononitrosyl adducts
of the FDP from Thermotoga maritima, which also shows
a 30 cm–1 down-shift with 15NO. Such
nitrosyl-like character may result from semi-bridging interactions
of the NO group that render these mononitrosyl complexes susceptible
to side-on electrophilic attack by a second NO to produce transient
hyponitrite complexes that subsequently decay to form N2O. Theoretical analyses of NO reduction in FDPs favor a mechanism
where the formation of a partially reduced NO group in a diiron–mononitrosyl
complex allows for attack by a second NO to form the N–N bond.[18]From these data, we propose that the metastable
nitroxyl-like mononitrosyl
complex observed in THF at room temperature is a competent intermediate
in the light-induced formation of N2O via electrophilic
attack by a second NO molecule (Scheme 1). Although light activation is not required for catalytic activity
in FDPs, and a recent pre-steady-state study of FDP favors a diferrous–dinitrosyl
intermediate as the precursor to N–N bond formation,[20] characterizing non-equilibrium states in synthetic
models provides insight into possible reaction mechanisms and transition
states that enzymes may stabilize to optimize their catalytic activity.
Efforts are underway in our laboratories to further characterize this
chemistry using monochromatic laser illumination as a possible way
to better control the formation and decay of the 1695 cm–1 species. We will also explore the possible role of protons in the
reduction of NO as we did previously for the dioxygen activation reaction
of these diiron models.[21]
Scheme 1
Possible
Mechanistic Steps for the Light-Induced Production of N2O from 1a(19)
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