8 research outputs found
Preparation of Single-Crystalline AgIn<sub>5</sub>S<sub>8</sub> Octahedrons with Exposed {111} Facets and Its Visible-Light-Responsive Photocatalytic H<sub>2</sub> Production Activity
Although AgIn<sub>5</sub>S<sub>8</sub> as one kind of ternary chalcogenides has been
extensively investigated due to its band-edge positions meeting the
thermodynamic requirement for water photosplitting, very little attention
has been focused on the crystallinity and facet effects of AgIn<sub>5</sub>S<sub>8</sub> on its photocatalytic activity. Herein, a facile
hydrothermal route was developed to fabricate regular single-crystalline
AgIn<sub>5</sub>S<sub>8</sub> octahedrons with only {111} facets exposed.
Also, the effects of the hydrothermal reaction conditions on the composition,
crystal phase, crystallinity, and morphology of the obtained Ag<sub><i>x</i></sub>In<sub><i>y</i></sub>S<sub>(<i>x</i>+3<i>y</i>/2)</sub> products (hereafter denoted
as AIS-<i>x</i>, where <i>x</i> represents the
pH value of the reaction solution) were investigated, and it was found
that the accurately released S<sup>2ā</sup> ions from the thermal
decomposition of thioacetamide (TAA) is the central factor for the
nucleation and growth of the AgIn<sub>5</sub>S<sub>8</sub> octahedrons.
The experimental results indicate that the resultant regular AgIn<sub>5</sub>S<sub>8</sub> octahedrons (AIS-10.6) exhibit the best photocatalytic
activity for H<sub>2</sub> production among those Ag<sub><i>x</i></sub>In<sub><i>y</i></sub>S<sub>(<i>x</i>+3<i>y</i>/2)</sub> products, and the higher crystallinity and fewer
defects of the AgIn<sub>5</sub>S<sub>8</sub> octahedrons compared
to the other Ag<sub><i>x</i></sub>In<sub><i>y</i></sub>S<sub>(<i>x</i>+3<i>y</i>/2)</sub> products
can retard the photogenerated charge recombination, while those indium
atoms with higher density in the exposed {111} facets might be beneficial
for the photocatalytic H<sub>2</sub> production reaction by acting
as active sites to promote the charge separation and transfer processes.
The results presented here provide new insights into the significance
of crystallinity and exposed facets in the visible-light-responsive
activity of AgIn<sub>5</sub>S<sub>8</sub>, thus paving new ways into
the design and synthesis of high-performance, cost-effective AgIn<sub>5</sub>S<sub>8</sub> photocatalysts for H<sub>2</sub> production
Controllable Fabrication of Regular Hexagon-Shaped SnS<sub>2</sub> Nanoplates and Their Enhanced Visible-Light-Driven H<sub>2</sub> Production Activity
SnS<sub>2</sub> nanoplate-like products were fabricated via a facile
hydrothermal process of a mixed solution containing SnCl<sub>4</sub> and thiourea (SCĀ(NH<sub>2</sub>)<sub>2</sub>) without organic capping
agent, and their composition, crystallinity, and morphology can be
adjusted by varying the SCĀ(NH<sub>2</sub>)<sub>2</sub>/SnCl<sub>4</sub> molar ratio. In particular, regular hexagon-shaped SnS<sub>2</sub> nanoplates with an average size of ā¼275 nm and thickness
of ā¼56 nm were attained when the SCĀ(NH<sub>2</sub>)<sub>2</sub>/(SnCl<sub>4</sub>) molar ratio is 6:1. The obtained SnS<sub>2</sub> nanoplates exhibit layered structures with exposed {001} facets
and a single-crystalline feature, and its growth mechanism was proposed
according to the hydrothermal time-dependent experimental results.
The regular hexagon-shaped SnS<sub>2</sub> nanoplates achieve high
photocatalytic H<sub>2</sub> production activity of 356 Ī¼mol
h<sup>ā1</sup> under visible light (Ī» ā„ 420 nm)
irradiation, much better than that of the irregular nanoplate-like
products. The higher crystallinity and fewer defects of the regular
hexagon-shaped SnS<sub>2</sub> nanoplates compared to the irregular
ones can more efficiently retard the photogenerated charge recombination,
while the S atoms with higher density in the exposed {001} facets
might be beneficial for the formation of H bonds with H<sub>2</sub>O molecules, which then cause good dispersity and photocatalytic
activity for H<sub>2</sub> production of the SnS<sub>2</sub> nanoplates.
These results demonstrate the potential application of SnS<sub>2</sub> nanoplates in the photocatalytic H<sub>2</sub> production field,
and might provide guidance to the controllable syntheses of the family
of MS<sub>2</sub> photocatalysts with a highly efficient H<sub>2</sub> production property
Controllable Preparation of Rutile TiO<sub>2</sub> Nanorod Array for Enhanced Photovoltaic Performance of Perovskite Solar Cells
A vertically oriented
rutile TiO<sub>2</sub> nanorod (NR) array,
as an efficient electron transport layer (ETL), has been used in the
perovskite solar cells (PSCs), and its microstructure has a great
impact on the corresponding photovoltaic conversion efficiency (PCE).
Here we employ a facile control strategy to modulate the microstructures
of rutile TiO<sub>2</sub> NR arrays hydrothermally grown on the fluorine
tin oxide (FTO) glass from a waterāHCl solution of titanium <i>n</i>-butoxide (TBOT). It was found that introducing commercial
TiO<sub>2</sub> nanoparticles (P25, Degussa) into the hydrothermal
reaction system can efficiently slow down the growth rate of rutile
TiO<sub>2</sub> NRs, thus causing the controllable preparation of
an NR array on the FTO substrate. The device fabricated with an optimized
NR array derived from the hydrothermal reaction solution containing
P25 exhibits an improvement of 26.5% in PCE compared with the device
fabricated with the NR array from the hydrothermal solution without
P25, which is mainly attributed to the reduced charge recombination
and the enhanced fill factor stemming from the better contact at the
NRs array/perovskite interface. This successful finding demonstrates
that the introduction of TiO<sub>2</sub> nanoparticles into the hydrothermal
reaction solution of TBOT slows down the growth rate and the electron
recombination process of the rutile TiO<sub>2</sub> NRs array, and
thus acts as a facile control strategy for improving the photovoltaic
performance of the rutile TiO<sub>2</sub> NRs array film-based PSCs
Asymmetric Zinc Porphyrin Derivative-Sensitized Graphitic Carbon Nitride for Efficient Visible-Light-Driven H<sub>2</sub> Production
An
asymmetric zinc porphyrin (ZnPy) derivative bearing one benzoic
acid and three 3-pyridines as <i>meso</i>-position substituents
(zinc-5-(4-carboxyphenyl)-10,15,20-triĀ(3-pridyl)Āporphyrin, ZnMT3PyP)
was used to sensitize graphitic carbon nitride (g-C<sub>3</sub>N<sub>4</sub>) for visible-light-driven photocatalytic H<sub>2</sub> production.
It was found that ZnMT3PyP exhibits more excellent photosensitization
and stability on g-C<sub>3</sub>N<sub>4</sub> than its counterpart
bearing one benzoic acid and three phenyls (zinc-5-(4-carboxyphenyl)-10,15,20-triphenylporphrin,
ZnMTPP) under visible light (Ī» > 420 nm) irradiation even
though
they have very similar physicochemical properties such as optical
absorption capacities and energy band structures. Especially, ZnMT3PyP-Pt/g-C<sub>3</sub>N<sub>4</sub> gives an apparent quantum yield (AQY) up to
25.1% at Ī» = 420 nm light illumination, greater than that (11.6%)
of ZnMTPP-Pt/g-C<sub>3</sub>N<sub>4</sub>. The differences in photosensitization
and stability between ZnMT3PyP and ZnMTPP are mainly due to the substitution
of 3-pyridine for the phenyls in ZnMTPP, which leads to the electron
transfers between ZnMT3PyP and g-C<sub>3</sub>N<sub>4</sub> faster
than that between ZnMTPP and g-C<sub>3</sub>N<sub>4</sub>. The present
results provide a new insight applying porphyrin derivatives to the
photocatalytic H<sub>2</sub> production and open up a new path for
further improving the conversion efficiency of solar energy to hydrogen
energy through molecular designing
Highly Asymmetric Phthalocyanine as a Sensitizer of Graphitic Carbon Nitride for Extremely Efficient Photocatalytic H<sub>2</sub> Production under Near-Infrared Light
Highly asymmetric zinc phthalocyanine derivative (Zn-<i>tri</i>-PcNc) with intense near-IR light (650ā800 nm) absorption
is utilized as a sensitizer to extend the spectral response region
of graphitic carbon nitride (g-C<sub>3</sub>N<sub>4</sub>) from ā¼450
nm to more than 800 nm. Ultravioletāvisible light (UV-vis)
diffuse reflectance absorption spectra (DRS), photoluminescence (PL)
spectra, time-resolved photoluminescence spectra (TRPS), and energy
band structure analyses are adopted to investigate the photogenerated
electron transfer process between Zn-<i>tri</i>-PcNc and
g-C<sub>3</sub>N<sub>4</sub> on both thermodynamics and dynamics aspects.
After optimizing the photocatalytic condition and adding chenodeoxycholic
acid (CDCA) as coadsorbent, Zn-<i>tri</i>-PcNc sensitized
g-C<sub>3</sub>N<sub>4</sub> photocatalyst shows a H<sub>2</sub> production
efficiency of 125.2 Ī¼mol h<sup>ā1</sup> under visible/near-IR-light
(Ī» ā„ 500 nm) irradiation, corresponding to a turnover
number (TON) of 5008 h<sup>ā1</sup> with an extremely high
apparent quantum yield (AQY) of 1.85% at 700 nm monochromatic light
irradiation. The present work should be the rarely fundamental investigation
on the utilization of near-IR light of solar radiation for the photocatalytic
H<sub>2</sub> production from water splitting over a dye-sensitized
semiconductor
Two Different Roles of Metallic Ag on Ag/AgX/BiOX (X = Cl, Br) Visible Light Photocatalysts: Surface Plasmon Resonance and Z-Scheme Bridge
Ag/AgX/BiOX (X = Cl, Br) three-component visible-light-driven
(VLD)
photocatalysts were synthesized by a low-temperature chemical bath
method and characterized by X-ray diffraction patterns, X-ray photoelectron
spectroscopy, field emission scanning electron microscopy, transmission
electron microscopy, high-resolution transmission electron microscopy,
and UVāvis diffuse reflectance spectra. The Ag/AgX/BiOX composites
showed enhanced VLD photocatalytic activity for the degradation of
rhodamine B, which was much higher than Ag/AgX and BiOX. The photocatalytic
mechanisms were analyzed by active species trapping and superoxide
radical quantification experiments. It revealed that metallic Ag played
a different role for Ag/AgX/BiOX VLD photocatalysts, surface plasmon
resonance for Ag/AgCl/BiOCl, and the Z-scheme bridge for Ag/AgBr/BiOBr
Attempt to Improve the Performance of Pyrrole-Containing Dyes in Dye Sensitized Solar Cells by Adjusting Isolation Groups
Four new pyrrole-based organic sensitizers
with different isolation groups were conveniently synthesized and
applied to dye sensitized solar cells (DSCs). The introduction of
isolation group in the side chain could both suppress the formation
of dye aggregates and electron recombination. Especially, when two
pieces of D-Ļ-A chromophore moieties shared one isolation group
to construct the āHā type dye, the performance was further
improved. Consequently, in the corresponding solar cell of <b>LI-57</b>, a short-circuit photocurrent density (<i>J</i><sub>sc</sub>) was tested to be 13.85 mA cm<sup>ā2</sup>, while 0.72 V
for the open-circuit photovoltage (<i>V</i><sub>oc</sub>), 0.64 for the fill factor (FF), and 6.43% for the overall conversion
efficiency (Ī·), exceeding its analogue <b>LI-55</b> (5.94%)
with the same isolation group. The results demonstrated that both
the size (bulk and shape) and the linkage mode between the D-Ļ-A
chromophores and the isolation groups, could affect the performance
of sensitizers in DSCs in a large degree, providing a new approach
to optimize the chemical structure of dyes to achieve high conversion
efficiencies
Organic Sensitizers Featuring 9,10-Diaryl-Substituted Anthracene Unit
A series of anthracene-based dyes
were designed and employed in
dye-sensitized solar cells in which different 9,10-diaryl-substituted
anthracene groups acted as a Ļ-bridge with 2,6-linkage mode.
The <i>tert</i>-butylphenyl and hexyloxyphenyl groups in
the 9 and 10 positions of the anthracene unit were almost perpendicular
to the conjugated plane, which would be beneficial to suppressing
the possible ĻāĻ stacking and retarding the charge
recombination. Their photophysical properties and photovoltaic performance
could be tuned by the modification of the substituted groups to the
anthracene ring in some degree. Consequently, dye <b>LI-59</b>-based solar cells gave the best performance, with a <i>J</i><sub>sc</sub> (short circuit current) of 13.42 mA cm<sup>ā2</sup>, <i>V</i><sub>oc</sub> (open circuit voltage) of 722 mV,
and FF (fill factor) of 0.66, corresponding to an overall conversion
efficiency of 6.42% without the presence of CDCA