3 research outputs found

    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

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    The interaction of imidazole with a [Cu­(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 [Cu­(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 [Cu­(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 ([Cu­(acac)<sub>2</sub>], [Cu­(acac)<sub>2</sub>Im<sub><i>n</i>=1</sub>], and [Cu­(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 [Cu­(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 [Cu­(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 [Cu­(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 [Cu­(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

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    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
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