3 research outputs found
Efficiency of Solar-Light-Driven TiO<sub>2</sub> Photocatalysis at Different Latitudes and Seasons. Where and When Does TiO<sub>2</sub> Really Work?
Efficiency
of Solar-Light-Driven TiO<sub>2</sub> Photocatalysis
at Different Latitudes and Seasons. Where and When Does TiO<sub>2</sub> Really Work
Understanding the Coordination Modes of [Cu(acac)<sub>2</sub>(imidazole)<sub><i>n</i>=1,2</sub>] Adducts by EPR, ENDOR, HYSCORE, and DFT Analysis
The interaction of
imidazole with a [CuÂ(acac)<sub>2</sub>] complex was studied using
electron paramagnetic resonance (EPR), electron nuclear double resonance
(ENDOR), hyperfine sublevel correlation spectroscopy (HYSCORE), and
density functional theory (DFT). At low Im ratios (Cu:Im 1:10), a
5-coordinate [CuÂ(acac)<sub>2</sub>Im<sub><i>n</i>=1</sub>] monoadduct is formed in frozen solution with the spin Hamiltonian
parameters <i>g</i><sub>1</sub> = 2.063, <i>g</i><sub>2</sub> = 2.063, <i>g</i><sub>3</sub> = 2.307, <i>A</i><sub>1</sub> = 26, <i>A</i><sub>2</sub> = 15,
and <i>A</i><sub>3</sub> = 472 MHz with Im coordinating
along the axial direction. At higher Im concentrations (Cu:Im 1:50),
a 6-coordinate [CuÂ(acac)<sub>2</sub>Im<sub><i>n</i>=2</sub>] bis-adduct is formed with the spin Hamiltonian parameters <i>g</i><sub>1</sub> = 2.059, <i>g</i><sub>2</sub> =
2.059, <i>g</i><sub>3</sub> = 2.288, <i>A</i><sub>1</sub> = 30, <i>A</i><sub>2</sub> = 30, and <i>A</i><sub>3</sub> = 498 MHz with a poorly resolved <sup>14</sup>N superhyperfine
pattern. The isotropic EPR spectra revealed a distribution of species
([CuÂ(acac)<sub>2</sub>], [CuÂ(acac)<sub>2</sub>Im<sub><i>n</i>=1</sub>], and [CuÂ(acac)<sub>2</sub>Im<sub><i>n</i>=2</sub>]) at Cu:Im ratios of 1:0, 1:10, and 1:50. The superhyperfine pattern
originates from two strongly coordinating N<sup>3</sup> imino nitrogens
of the Im ring. Angular selective <sup>14</sup>N ENDOR analysis revealed
the <sup>N</sup><i>A</i> tensor of [34.8, 43.5, 34.0] MHz,
with e<sup>2</sup><i>qQ</i>/<i>h</i> = 2.2 MHz
and η = 0.2 for N<sup>3</sup>. The hyperfine and quadrupole
values for the remote N<sup>1</sup> amine nitrogens (from HYSCORE)
were found to be [1.5, 1.4, 2.5] MHz with e<sup>2</sup><i>qQ</i>/<i>h</i> = 1.4 MHz and η = 0.9. <sup>1</sup>H ENDOR
also revealed three sets of <sup>H</sup><i>A</i> tensors
corresponding to the nearly equivalent H<sup>2</sup>/H<sup>4</sup> protons in addition to the H<sup>5</sup> and H<sup>1</sup> protons
of the Im ring. The spin Hamiltonian parameters for the geometry optimized
structures of [CuÂ(acac)<sub>2</sub>Im<sub><i>n</i>=2</sub>], including <i>cis</i>-mixed plane, <i>trans</i>-axial, and <i>trans</i>-equatorial, were calculated. The
best agreement between theory and experiment indicated the preferred
coordination is <i>trans</i>-equatorial [CuÂ(acac)<sub>2</sub>Im<sub><i>n</i>=2</sub>]. A number of other Im derivatives
were also investigated. 4(5)-methyl-imidazole forms a [CuÂ(acac)<sub>2</sub>(Im-<b>3</b>)<sub><i>n</i>=2</sub>] <i>trans</i>-equatorial adduct, whereas the bulkier 2-methyl-imidazole
(Im-<b>2</b>) and benzimidazole (Im-<b>4</b>) form the
[CuÂ(acac)<sub>2</sub>(Im-<b>2,4</b>)<sub><i>n</i>=1</sub>] monoadduct only. Our data therefore show that subtle changes in
the substrate structure lead to controllable changes in coordination
behavior, which could in turn lead to rational design of complexes
for use in catalysis, imaging, and medicine
Improving the Selectivity of Photocatalytic NO<i><sub>x</sub></i> Abatement through Improved O<sub>2</sub> Reduction Pathways Using Ti<sub>0.909</sub>W<sub>0.091</sub>O<sub>2</sub>N<sub><i>x</i></sub> Semiconductor Nanoparticles: From Characterization to Photocatalytic Performance
In
this paper, we provide detailed insight into the electronic–crystallographic–structural
relationship for Ti<sub>0.909</sub>W<sub>0.091</sub>O<sub>2</sub>N<sub><i>x</i></sub> semiconductor nanoparticles, explaining
the mutual electronic and magnetic influence of the photoinduced stable
N- and W-based paramagnetic centers, their involvement in the photoinduced
charge-carrier trapping, and their role in improving the nitrate selectivity
of the photocatalytic oxidation of NO<sub><i>x</i></sub> to nitrates. In particular, reduced tungsten species in various
crystallographic environments within the anatase host lattice were
observed as playing a fundamental role in the storage and stabilization
of photogenerated electrons. Here, we show how these reduced centers
can catalyze multielectron transfer events without the need for rare
and expensive platinum-group metals (PGMs). This allows for the versatile
and elegant configuration of redox potentials. As a result, electron-transfer
processes that are kinetically inaccessible with metal oxides such
as TiO<sub>2</sub> can now be accessed, enabling dramatic improvements
in reaction selectivity. The photocatalytic abatement of NO<sub><i>x</i></sub> toward nontoxic products is exemplified here and
is shown to pivot on multiple routes for molecular oxygen reduction.
The same rationale can furthermore be applied to other photocatalytic
processes. The observations described in this work could open new
and exciting avenues in semiconductor photocatalysis for environmental
remediation technologies in which the optimization of molecular oxygen
reduction, together with the pollutant species to be oxidized, becomes
a central element of the catalyst design without relying on the use
of rare and expensive PGMs