19 research outputs found
Legislative Documents
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Model of the Oxygen Evolving Complex Which Is Highly Predisposed to O–O Bond Formation
Light-driven water
oxidation is a fundamental reaction in the biosphere.
The Mn<sub>4</sub>Ca cluster of photosystem II cycles through five
redox states termed S<sub>0</sub>–S<sub>4</sub>, after which
oxygen is evolved. Critically, the timing of O–O bond formation
within the Kok cycle remains unknown. By combining recent crystallographic,
spectroscopic, and DFT results, we demonstrate an atomistic S<sub>3</sub> state model with the possibility of a low barrier to O–O
bond formation prior to the final oxidation step. Furthermore, the
associated one electron oxidized S<sub>4</sub> state does not provide
more advantages in terms of spin alignment or the energy of O–O
bond formation. We propose that a high energy peroxide isoform of
the S<sub>3</sub> state can preferentially be oxidized by Tyr<sub><i>z</i></sub><sup>ox</sup> in the course of final electron
transfer leading to O<sub>2</sub> evolution. Such a mechanism may
explain the peculiar kinetic behavior of O<sub>2</sub> evolution as
well as serve as an evolutionary adaptation to avoid release of the
harmful peroxides
Model of the Oxygen Evolving Complex Which Is Highly Predisposed to O–O Bond Formation
Light-driven water
oxidation is a fundamental reaction in the biosphere.
The Mn<sub>4</sub>Ca cluster of photosystem II cycles through five
redox states termed S<sub>0</sub>–S<sub>4</sub>, after which
oxygen is evolved. Critically, the timing of O–O bond formation
within the Kok cycle remains unknown. By combining recent crystallographic,
spectroscopic, and DFT results, we demonstrate an atomistic S<sub>3</sub> state model with the possibility of a low barrier to O–O
bond formation prior to the final oxidation step. Furthermore, the
associated one electron oxidized S<sub>4</sub> state does not provide
more advantages in terms of spin alignment or the energy of O–O
bond formation. We propose that a high energy peroxide isoform of
the S<sub>3</sub> state can preferentially be oxidized by Tyr<sub><i>z</i></sub><sup>ox</sup> in the course of final electron
transfer leading to O<sub>2</sub> evolution. Such a mechanism may
explain the peculiar kinetic behavior of O<sub>2</sub> evolution as
well as serve as an evolutionary adaptation to avoid release of the
harmful peroxides
Model of the Oxygen Evolving Complex Which Is Highly Predisposed to O–O Bond Formation
Light-driven water
oxidation is a fundamental reaction in the biosphere.
The Mn<sub>4</sub>Ca cluster of photosystem II cycles through five
redox states termed S<sub>0</sub>–S<sub>4</sub>, after which
oxygen is evolved. Critically, the timing of O–O bond formation
within the Kok cycle remains unknown. By combining recent crystallographic,
spectroscopic, and DFT results, we demonstrate an atomistic S<sub>3</sub> state model with the possibility of a low barrier to O–O
bond formation prior to the final oxidation step. Furthermore, the
associated one electron oxidized S<sub>4</sub> state does not provide
more advantages in terms of spin alignment or the energy of O–O
bond formation. We propose that a high energy peroxide isoform of
the S<sub>3</sub> state can preferentially be oxidized by Tyr<sub><i>z</i></sub><sup>ox</sup> in the course of final electron
transfer leading to O<sub>2</sub> evolution. Such a mechanism may
explain the peculiar kinetic behavior of O<sub>2</sub> evolution as
well as serve as an evolutionary adaptation to avoid release of the
harmful peroxides
Model of the Oxygen Evolving Complex Which Is Highly Predisposed to O–O Bond Formation
Light-driven water
oxidation is a fundamental reaction in the biosphere.
The Mn<sub>4</sub>Ca cluster of photosystem II cycles through five
redox states termed S<sub>0</sub>–S<sub>4</sub>, after which
oxygen is evolved. Critically, the timing of O–O bond formation
within the Kok cycle remains unknown. By combining recent crystallographic,
spectroscopic, and DFT results, we demonstrate an atomistic S<sub>3</sub> state model with the possibility of a low barrier to O–O
bond formation prior to the final oxidation step. Furthermore, the
associated one electron oxidized S<sub>4</sub> state does not provide
more advantages in terms of spin alignment or the energy of O–O
bond formation. We propose that a high energy peroxide isoform of
the S<sub>3</sub> state can preferentially be oxidized by Tyr<sub><i>z</i></sub><sup>ox</sup> in the course of final electron
transfer leading to O<sub>2</sub> evolution. Such a mechanism may
explain the peculiar kinetic behavior of O<sub>2</sub> evolution as
well as serve as an evolutionary adaptation to avoid release of the
harmful peroxides
Spectroscopic Analysis of Catalytic Water Oxidation by [Ru<sup>II</sup>(bpy)(tpy)H<sub>2</sub>O]<sup>2+</sup> Suggests That Ru<sup>V</sup>O Is Not a Rate-Limiting Intermediate
Modern chemistry’s grand challenge
is to significantly improve
catalysts for water splitting. Further progress requires detailed
spectroscopic and computational characterization of catalytic mechanisms.
We analyzed one of the most studied homogeneous single-site Ru catalysts,
[Ru<sup>II</sup>(bpy)(tpy)H<sub>2</sub>O]<sup>2+</sup> (where bpy
= 2,2′-bipyridine, tpy = 2,2′;6′,2″-terpyridine).
Our results reveal that the [Ru<sup>V</sup>(bpy)(tpy)O]<sup>3+</sup> intermediate, reportedly detected in catalytic mixtures
as a rate-limiting intermediate in water activation, is not present
as such. Using a combination of electron paramagnetic resonance (EPR)
and X-ray absorption spectroscopy, we demonstrate that 95% of the
Ru complex in the catalytic steady state is of the form [Ru<sup>IV</sup>(bpy)(tpy)O]<sup>2+</sup>. [Ru<sup>V</sup>(bpy)(tpy)O]<sup>3+</sup> was not observed, and according to density functional theory
(DFT) analysis, it might be thermodynamically inaccessible at our
experimental conditions. A reaction product with unique EPR spectrum
was detected in reaction mixtures at about 5% and assigned to Ru<sup>III</sup>-peroxo species with (−OOH or −OO–
ligands). We also analyzed the [Ru<sup>II</sup>(bpy)(tpy)Cl]<sup>+</sup> catalyst precursor and confirmed that this molecule is not a catalyst
and its oxidation past Ru<sup>III</sup> state is impeded by a lack
of proton-coupled electron transfer. Ru–Cl exchange with water
is required to form active catalysts with the Ru–H<sub>2</sub>O fragment. [Ru<sup>II</sup>(bpy)(tpy)H<sub>2</sub>O]<sup>2+</sup> is the simplest representative of a larger class of water oxidation
catalysts with neutral, nitrogen containing heterocycles. We expect
this class of catalysts to work mechanistically in a similar fashion
via [Ru<sup>IV</sup>(bpy)(tpy)O]<sup>2+</sup> intermediate
unless more electronegative (oxygen containing) ligands are introduced
in the Ru coordination sphere, allowing the formation of more oxidized
Ru<sup>V</sup> intermediate
Triplet Excited State Energies and Phosphorescence Spectra of (Bacterio)Chlorophylls
(Bacterio)Chlorophyll
((B)Chl) molecules play a major role in photosynthetic
light-harvesting proteins, and the knowledge of their triplet state
energies is essential to understand the mechanisms of photodamage
and photoprotection, as the triplet excitation energy of (B)Chl molecules
can readily generate highly reactive singlet oxygen. The triplet state
energies of 10 natural chlorophyll (Chl <i>a</i>, <i>b</i>, <i>c</i><sub>2</sub>, <i>d</i>) and
bacteriochlorophyll (BChl <i>a</i>, <i>b</i>, <i>c</i>, <i>d</i>, <i>e</i>, <i>g</i>) molecules and one bacteriopheophytin (BPheo <i>g</i>)
have been directly determined via their phosphorescence spectra. Phosphorescence
of four molecules (Chl <i>c</i><sub>2</sub>, BChl <i>e</i> and <i>g</i>, BPheo <i>g</i>) was
characterized for the first time. Additionally, the relative phosphorescence
to fluorescence quantum yield for each molecule was determined. The
measurements were performed at 77K using solvents providing a six-coordinate
environment of the Mg<sup>2+</sup> ion, which allows direct comparison
of these (B)Chls. Density functional calculations of the triplet state
energies show good correlation with the experimentally determined
energies. The correlation determined computationally was used to predict
the triplet energies of three additional (B)Chl molecules: Chl <i>c</i><sub>1</sub>, Chl <i>f</i>, and BChl <i>f</i>
The Key Ru<sup>V</sup>=O Intermediate of Site-Isolated Mononuclear Water Oxidation Catalyst Detected by <i>in Situ</i> X‑ray Absorption Spectroscopy
Improvement of the oxygen evolution
reaction (OER) is a challenging
step toward the development of sustainable energy technologies. Enhancing
the OER rate and efficiency relies on understanding the water oxidation
mechanism, which entails the characterization of the reaction intermediates.
Very active Ru-bda type (bda is 2,2′-bipyridine-6,6′-dicarboxylate)
molecular OER catalysts are proposed to operate via a transient 7-coordinate
Ru<sup>V</sup>O intermediate, which so far has never been
detected due to its high reactivity. Here we prepare and characterize
a well-defined supported Ru(bda) catalyst on porous indium tin oxide
(ITO) electrode. Site isolation of the catalyst molecules on the electrode
surface allows trapping of the key 7-coordinate Ru<sup>V</sup>O
intermediate at potentials above 1.34 V vs NHE at pH 1, which is characterized
by electron paramagnetic resonance and <i>in situ</i> X-ray
absorption spectroscopies. The <i>in situ</i> extended X-ray
absorption fine structure analysis shows a RuO bond distance
of 1.75 ± 0.02 Å, consistent with computational results.
Electrochemical studies and density functional theory calculations
suggest that the water nucleophilic attack on the surface-bound Ru<sup>V</sup>O intermediate (O–O bond formation) is the
rate limiting step for OER catalysis at low
pH
Uncovering the Role of Oxygen Atom Transfer in Ru-Based Catalytic Water Oxidation
The realization of artificial photosynthesis
carries the promise
of cheap and abundant energy, however, significant advances in the
rational design of water oxidation catalysts are required. Detailed
information on the structure of the catalyst under reaction conditions
and mechanisms of O–O bond formation should be obtained. Here,
we used a combination of electron paramagnetic resonance (EPR), stopped
flow freeze quench on a millisecond–second time scale, X-ray
absorption (XAS), resonance Raman (RR) spectroscopy, and density functional
theory (DFT) to follow the dynamics of the Ru-based single site catalyst,
[Ru<sup>II</sup>(NPM)(4-pic)<sub>2</sub>(H<sub>2</sub>O)]<sup>2+</sup> (NPM = 4-<i>t</i>-butyl-2,6-di(1′,8′-naphthyrid-2′-yl)pyridine,
pic = 4-picoline), under the water oxidation conditions. We report
a unique EPR signal with g-tensor, g<sub><i>x</i></sub> =
2.30, g<sub><i>y</i></sub> = 2.18, and g<sub><i>z</i></sub> = 1.83 which allowed us to observe fast dynamics of oxygen
atom transfer from the Ru<sup>IV</sup>O oxo species to the
uncoordinated nitrogen of the NPM ligand. In few seconds, the NPM
ligand modification results in [Ru<sup>III</sup>(NPM-NO)(4-pic)<sub>2</sub>(H<sub>2</sub>O)]<sup>3+</sup> and [Ru<sup>III</sup>(NPM-NO,NO)(4-pic)<sub>2</sub>]<sup>3+</sup> complexes. A proposed [Ru<sup>V</sup>(NPM)(4-pic)<sub>2</sub>O]<sup>3+</sup> intermediate was not detected under
the tested conditions. We demonstrate that while the proximal base
might be beneficial in O–O bond formation via nucleophilic
water attack on an oxo species as shown by DFT, the noncoordinating
nitrogen is impractical as a base in water oxidation catalysts due
to its facile conversion to the N–O group. This study opens
new horizons for understanding the real structure of Ru catalysts
under water oxidation conditions and points toward the need to further
investigate the role of the N–O ligand in promoting water oxidation
catalysis
Structure and Electronic Configurations of the Intermediates of Water Oxidation in Blue Ruthenium Dimer Catalysis
Catalytic O<sub>2</sub> evolution with <i>cis</i>,<i>cis</i>-[(bpy)<sub>2</sub>(H<sub>2</sub>O)Ru<sup>III</sup>ORu<sup>III</sup>(OH<sub>2</sub>)(bpy)<sub>2</sub>]<sup>4+</sup> (bpy
is
2,2-bipyridine), the so-called blue dimer, the first designed water
oxidation catalyst, was monitored by UV–vis, EPR, and X-ray
absorption spectroscopy (XAS) with ms time resolution. Two processes
were identified, one of which occurs on a time scale of 100 ms to
a few seconds and results in oxidation of the catalyst with the formation
of an intermediate, here termed [3,4]′. A slower process occurring
on the time scale of minutes results in the decay of this intermediate
and O<sub>2</sub> evolution. Spectroscopic data suggest that within
the fast process there is a short-lived transient intermediate, which
is a precursor of [3,4]′. When excess oxidant was used, a highly
oxidized form of the blue dimer [4,5] was spectroscopically resolved
within the time frame of the fast process. Its structure and electronic
state were confirmed by EPR and XAS. As reported earlier, the [3,4]′
intermediate likely results from reaction of [4,5] with water. While
it is generated under strongly oxidizing conditions, it does not display
oxidation of the Ru centers past [3,4] according to EPR and XAS. EXAFS
analysis demonstrates a considerably modified ligand environment in
[3,4]′. Raman measurements confirmed the presence of the O–O
fragment by detecting a new vibration band in [3,4]′ that undergoes
a 46 cm<sup>–1</sup> shift to lower energy upon <sup>16</sup>O/<sup>18</sup>O exchange. Under the conditions of the experiment
at pH 1, the [3,4]′ intermediate is the catalytic steady state
form of the blue dimer catalyst, suggesting that its oxidation is
the rate-limiting step