3 research outputs found
Nanostructured SnO<sub>2</sub>āZnO Heterojunction Photocatalysts Showing Enhanced Photocatalytic Activity for the Degradation of Organic Dyes
Nanoporous SnO<sub>2</sub>āZnO 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 adsorptionādesorption
analyses, transmission electron microscopy (TEM), and UVāvis
diffuse reflectance spectroscopy. The SnO<sub>2</sub>āZnO 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
UVāvisible diffuse reflectance spectroscopy, the evident energy
band gap value of the SnO<sub>2</sub>āZnO 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>āZnO 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>āZnO 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>āZnO 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>āZnO 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
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 (0.5ā5 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>āTiO<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
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 1ā10
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>ā1</sup> was reached
with 5 wt % RuO<sub>2</sub>/TiO<sub>2</sub> photocatalyst to be compared
with 29 Ī¼mol h<sup>ā1</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