3 research outputs found

    Nanostructured SnO<sub>2</sub>ā€“ZnO Heterojunction Photocatalysts Showing Enhanced Photocatalytic Activity for the Degradation of Organic Dyes

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    Nanoporous SnO<sub>2</sub>ā€“ZnO heterojunction nanocatalyst was prepared by a straightforward two-step procedure involving, first, the synthesis of nanosized SnO<sub>2</sub> particles by homogeneous precipitation combined with a hydrothermal treatment and, second, the reaction of the as-prepared SnO<sub>2</sub> particles with zinc acetate followed by calcination at 500 Ā°C. The resulting nanocatalysts were characterized by X-ray diffraction (XRD), FTIR, Raman, X-ray photoelectron spectroscopy (XPS), nitrogen adsorptionā€“desorption analyses, transmission electron microscopy (TEM), and UVā€“vis diffuse reflectance spectroscopy. The SnO<sub>2</sub>ā€“ZnO photocatalyst was made of a mesoporous network of aggregated wurtzite ZnO and cassiterite SnO<sub>2</sub> nanocrystallites, the size of which was estimated to be 27 and 4.5 nm, respectively, after calcination. According to UVā€“visible diffuse reflectance spectroscopy, the evident energy band gap value of the SnO<sub>2</sub>ā€“ZnO photocatalyst was estimated to be 3.23 eV to be compared with those of pure SnO<sub>2</sub>, that is, 3.7 eV, and ZnO, that is, 3.2 eV, analogues. The energy band diagram of the SnO<sub>2</sub>ā€“ZnO heterostructure was directly determined by combining XPS and the energy band gap values. The valence band and conduction band offsets were calculated to be 0.70 Ā± 0.05 eV and 0.20 Ā± 0.05 eV, respectively, which revealed a type-II band alignment. Moreover, the heterostructure SnO<sub>2</sub>ā€“ZnO photocatalyst showed much higher photocatalytic activities for the degradation of methylene blue than those of individual SnO<sub>2</sub> and ZnO nanomaterials. This behavior was rationalized in terms of better charge separation and the suppression of charge recombination in the SnO<sub>2</sub>ā€“ZnO photocatalyst because of the energy difference between the conduction band edges of SnO<sub>2</sub> and ZnO as evidenced by the band alignment determination. Finally, this mesoporous SnO<sub>2</sub>ā€“ZnO heterojunction nanocatalyst was stable and could be easily recycled several times opening new avenues for potential industrial applications

    Preparation of RuO<sub>2</sub>/TiO<sub>2</sub> Mesoporous Heterostructures and Rationalization of Their Enhanced Photocatalytic Properties by Band Alignment Investigations

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    Nanoporous RuO<sub>2</sub>/TiO<sub>2</sub> heterostructures, in which ruthenium oxide acts as a quasi-metallic contact material enhancing charge separation under illumination, were prepared by impregnation of anatase TiO<sub>2</sub> nanoparticles in a rutheniumĀ­(III) acetylacetonate solution followed by thermal annealing at 400 Ā°C. Regardless of the RuO<sub>2</sub> amount (0.5ā€“5 wt %), the as-prepared nanocatalyst was made of a mesoporous network of aggregated 18 nm anatase TiO<sub>2</sub> nanocrystallites modified with RuO<sub>2</sub> according to N<sub>2</sub> sorption, TEM, and XRD analyses. Furthermore, a careful attention has been paid to determine the energy band alignment diagram by XPS and UPS in order to rationalize charge separation at the interface of RuO<sub>2</sub>/TiO<sub>2</sub> heterojunction. At first, a model experiment involving stepwise deposition of RuO<sub>2</sub> on the TiO<sub>2</sub> film and an <i>in situ</i> XPS measurement showed a shift of Ti 2p<sub>3/2</sub> core level spectra toward lower binding energy of 1.22 eV which was ascribed to upward band bending at the interface of RuO<sub>2</sub>/TiO<sub>2</sub> heterojunction. The band bending for the heterostructure RuO<sub>2</sub>/TiO<sub>2</sub> nanocomposites was then found to be 0.2 Ā± 0.05 eV. Photocatalytic decomposition of methylene blue (MB) in solution under UV light irradiation revealed that the 1 wt % RuO<sub>2</sub>/TiO<sub>2</sub> nanocatalyst led to twice higher activities than pure anatase TiO<sub>2</sub> and reference commercial TiO<sub>2</sub> P25 nanoparticles. This higher photocatalytic activity for the decomposition of organic dyes was related to the higher charge separation resulting from built-in potential developed at the interface of RuO<sub>2</sub>/TiO<sub>2</sub> heterojunction. Finally, these mesoporous RuO<sub>2</sub>ā€“TiO<sub>2</sub> heterojunction nanocatalysts were stable and could be recycled several times without any appreciable change in degradation rate constant that opens new avenues toward potential industrial applications

    New Insights into the Photocatalytic Properties of RuO<sub>2</sub>/TiO<sub>2</sub> Mesoporous Heterostructures for Hydrogen Production and Organic Pollutant Photodecomposition

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    Photocatalytic activities of mesoporous RuO<sub>2</sub>/TiO<sub>2</sub> heterojunction nanocomposites for organic dye decomposition and H<sub>2</sub> production by methanol photoreforming have been studied as a function of the RuO<sub>2</sub> loading in the 1ā€“10 wt % range. An optimum RuO<sub>2</sub> loading was evidenced for both kinds of reaction, the corresponding nanocomposites showing much higher activities than pure TiO<sub>2</sub> and commercial reference P25. Thus, 1 wt % RuO<sub>2</sub>/TiO<sub>2</sub> photocatalyst led to the highest rates for the degradation of cationic (methylene blue) and anionic (methyl orange) dyes under UV light illumination. To get a better understanding of the mechanisms involved, a comprehensive investigation on the photogenerated charge carriers, detected by electron spin resonance (ESR) spectroscopy in the form of O<sup>ā€“</sup>, Ti<sup>3+</sup>, and O<sub>2</sub><sup>ā€“</sup> trapping centers, was performed. Along with the key role of superoxide paramagnetic species in the photodecomposition of organic dyes, ESR measurements revealed a higher amount of trapped holes in the case of the 1 wt % RuO<sub>2</sub>/TiO<sub>2</sub> photocatalyst that allowed rationalizing the trends observed. On the other hand, a maximum average hydrogen production rate of 618 Ī¼mol h<sup>ā€“1</sup> was reached with 5 wt % RuO<sub>2</sub>/TiO<sub>2</sub> photocatalyst to be compared with 29 Ī¼mol h<sup>ā€“1</sup> found without RuO<sub>2</sub>. Favorable band bending at the RuO<sub>2</sub>/TiO<sub>2</sub> interface and the key role of photogenerated holes have been proposed to explain the highest activity of the RuO<sub>2</sub>/TiO<sub>2</sub> photocatalysts for hydrogen production. These findings open new avenues for further design of RuO<sub>2</sub>/TiO<sub>2</sub> nanostructures with a fine-tuning of the RuO<sub>2</sub> nanoparticle distribution in order to reach optimized vectorial charge distribution and enhanced photocatalytic hydrogen production rates
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